AMA | March 2025

AMA | March 2025

BonusReleased Monday, 10th March 2025
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AMA | March 2025

AMA | March 2025

AMA | March 2025

AMA | March 2025

BonusMonday, 10th March 2025
Good episode? Give it some love!
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everyone, welcome to the March 2025

1:01

Ask Me Anything edition of the

1:03

Mindscape podcast. I'm your host Sean

1:05

Carroll. Before diving in to the

1:07

AMAs, I want to mention two

1:09

announcement kind of things, not really

1:11

announcements, two things, one announcement and

1:13

one reflection, if you want to put

1:15

it that way. The announcement is,

1:17

we have winners for this year's

1:19

Mindscape Big Picture Scholarship. I hope I've

1:22

been flogging this enough, probably I

1:24

haven't, but this has been going

1:26

on for a few years now.

1:28

It's at bold.org, so it's going

1:30

to keep going on. It's

1:32

not ended, so you can

1:34

still contribute. We solicit donations

1:36

from mindscape listeners to help

1:38

undergraduate university students achieve their

1:40

dreams of studying big picture

1:42

ideas down the road. So

1:44

this is hosted by bold.org,

1:46

which has scholarships and all

1:48

kinds of things. If you

1:51

go to bold.org/scholarships slash mindscape,

1:53

you can find hours and

1:55

contribute to it. You can

1:57

just go to our podcast

1:59

homepage. proposterousuniverse.com/podcast. In the right hand

2:01

column, there's a link that says

2:03

Minescape Big Picture Scholarship. Click on

2:05

it and you get all

2:07

the info. So we've been super

2:09

successful. Thank you so much for

2:11

contributing. We've been very successful at

2:14

getting donations so much so that

2:16

each year the current plan

2:18

is we can give two scholarships

2:20

worth $20 ,000 each, which is

2:22

not enough to send someone to

2:24

college entirely, but makes a big

2:26

difference to someone who's just trying

2:28

to pay that tuition for school,

2:30

especially if you're not

2:32

planning to go in some

2:35

area that is super

2:37

financially remunerative down the road.

2:39

And I'm very happy

2:41

to announce this year's winners.

2:43

One winner is Jillian

2:45

Kate from, she's already a

2:47

undergraduate enrolled at Auburn

2:49

University and she's studying biochemistry,

2:51

biophysics, molecular biology with

2:53

the goal of becoming a

2:55

college professor and doing

2:57

research in those areas. And

2:59

one line that caught my eye

3:01

from her application was that she's already

3:03

planning not only to be a

3:05

professor, but what kinds of courses she's

3:07

going to teach as a professor.

3:09

So Jillian says, my goal is to

3:11

one day teach biology in a

3:13

southeastern university. And when I teach introductory

3:15

courses, I hope to intertwine creativity,

3:17

philosophy and art into my lectures and

3:19

course content. That certainly sounds something

3:21

like something we could use more of

3:23

in academia. So I'm all in

3:25

favor of that. Other winner is Miles

3:27

Webb, who is a senior in

3:29

high school and looking at different universities

3:31

to go to wants to study computer

3:33

engineering, material science, chemistry and physics.

3:35

And one of the lines in his

3:38

application was a dream of mine

3:40

is to become the first black Nobel

3:42

Prize winner in physics. Part of

3:44

me says, you know, I hope you're

3:46

not miles because I hope someone

3:48

else is even before you get there.

3:50

But if miles is the first

3:52

black Nobel Prize winner in physics, I

3:54

hope he gives a shout out

3:56

to mindscape listeners in his Nobel Prize

3:58

acceptance speech because because we have

4:00

given them a little bit of

4:02

a boost in paying for that

4:04

college education along the way. Again,

4:06

very many sincere thanks to all

4:08

the listeners because you are the

4:10

ones who contribute and it really

4:13

does make a difference to students,

4:15

especially in times of uncertainty when

4:17

it comes to higher education, scientific

4:19

research, things like that. The other

4:21

announcement, which is not an announcement

4:23

but a little reflection, is that

4:25

in last week's episode, I did

4:27

the theory of cocktails with Kevin

4:29

Peterson, a bit of a

4:31

change of pace, but we're allowed to

4:33

have fun here at the podcast. We

4:35

don't to be serious all the time.

4:37

And the thing we did at

4:39

the end of the podcast, if you'll

4:41

remember, is that we invented on the

4:44

spot, I say we, but it was

4:46

really Kevin, invented a Minescape cocktail, the

4:48

Minescape Petricor Negroni. Petricor is a word

4:50

having to do with that smell

4:52

in the forest after it rains. So

4:54

Kevin came up with a great idea,

4:56

except that it was difficult to pull

4:58

off for the typical home bartender. Negroni,

5:00

for those of you who

5:02

don't know, is one part

5:05

gin, one part something Campari

5:08

-esque, something bitter like that, and amaro,

5:10

I guess, in general. And then

5:12

one part sweet vermouth, red vermouth. So

5:14

the specific ingredients that matter is,

5:16

you know, what kind of gin, what

5:18

kind of vermouth, what kind of

5:20

amaro do you use? And Kevin came

5:22

up with Antica Formula Vermouth, which

5:24

is a very standard, you know, it's

5:26

one of the ones you can

5:28

easily get, typically, in the liquor

5:31

stores. It's what I generally use

5:33

when I'm using that kind of

5:35

vermouth in cocktails. For the amaro,

5:37

he suggested St. George Bruto Americano,

5:39

which I'd never heard of. St.

5:41

George, I knew quite well as

5:43

a gin producer, and I didn't

5:45

know that they made sort of

5:47

a Campari substitute. But now I

5:49

do, and it's amazing. It's really,

5:51

really wonderful. It's a little bit

5:53

smoother than real Campari. Opera roll

5:55

is the other thing that people

5:57

often substitute for Campari. But I

5:59

like the same. Georgia's brutal Americano better than

6:01

either one of them. So that's a

6:04

real discovery. And it does have that

6:06

little bit of herbaceousness in it that

6:08

we were looking for in our cocktail.

6:10

But then for the gin, Kevin's suggestion

6:13

was to distill our own gin from

6:15

vetiver, which is a type of grass

6:17

that is. hard to find. It's in

6:19

Haiti and maybe in India, something like

6:21

that. It's not easy to find a

6:24

vetiver. It's also not easy to distill

6:26

your own gin. So I'm not at

6:28

that level of cocktail wizardry. And I

6:30

asked him for maybe an off-the-shelf replacement

6:33

option. So he suggested moletto. gin, which

6:35

I had not been aware of, and

6:37

now I am. So I actually, when

6:39

we did the podcast and I recorded

6:42

the intro, etc., I hadn't made the

6:44

cocktail, but now I have, and I'm

6:46

here to report to you that it

6:49

was very good. So the issue with

6:51

the mulleto gin is the gimmick that

6:53

they have. You know, gin is sort

6:55

of flavored. Vodka, flavored neutral spirit of

6:58

some sort, and the flavors are supposed

7:00

to be various botanicals, largely juniper, but

7:02

then the individual character of the gin

7:04

comes from exactly which botanicals you use.

7:07

And Moleto uses tomatoes, among other things,

7:09

to flavor their gin. And I got

7:11

a say, I didn't say it to

7:14

Kevin in the moment, but I was

7:16

instantly thinking and was still thinking, that

7:18

sounds terrible. Like, I like tomatoes in

7:20

the right context, but in gin might

7:23

not be that context. And when I

7:25

got it, I managed to, you know,

7:27

shake up a bottle and it arrived

7:29

and indeed, it's not mostly made of

7:31

tomatoes, it's made of some grain, but

7:34

then there's a tomato essence in there

7:36

and you open it up and it

7:38

kind of smells like tomato juice. Like

7:40

it's a very noticeable tomato smell. And

7:42

I was very skeptical about this, but

7:44

I thought, you know, look, he knows

7:46

what he's doing. I bet this is

7:48

one of those things that when you

7:50

put it into the cocktail, it's not

7:52

going to smell to me at all.

7:54

It's going to be mixed in in

7:56

a particular way. And indeed, that's exactly

7:58

what happened. So I don't know. whether

8:00

I would drink Moleto gin straight.

8:02

I haven't tried yet. Maybe it

8:04

would be good in the right

8:07

circumstances with a grilled cheese sandwich,

8:09

perhaps. I really don't know. But

8:11

in the cocktail, it was very

8:13

good. And it did, in fact,

8:15

completely satisfy the requirements of giving

8:18

you that foresty, piney, herbaceous kind

8:20

of feel. In fact, maybe I

8:22

could add a drop of my

8:24

pine. bidders that I got on

8:26

the shelf there. Maybe that could

8:29

like juiced up a little bit.

8:31

Anyway, I can give a positive

8:33

recommendation to the Mindscape Petricor Negroni.

8:35

I think that it works. For

8:37

those of you who are into

8:40

that kind of thing. I would

8:42

hesitate to try to come up

8:44

with a mocktail version, but it

8:46

would definitely involve tomato juice somehow,

8:49

which I don't know whether that

8:51

would be a good thing. Anyway,

8:53

many thanks as always to Mindscape

8:55

listeners, especially patron supporters. The monthly

8:57

AMA is supported by patron supporters,

9:00

if you join on patron.com/Sean M.

9:02

Carroll, then you get ad-free versions

9:04

of the podcast, and you get

9:06

to ask questions for the AMAs,

9:08

and you get my little tiny

9:11

reflections after each episode. As usual,

9:13

too many questions to answer all

9:15

of them, but they're all good.

9:17

Keep asking them. Someone said, like,

9:19

can we keep asking questions even

9:22

if we if we tried once

9:24

and didn't get selected? Can we

9:26

ask the next question the same

9:28

question next time? Absolutely yes. I

9:30

mean, it might even slightly increase

9:33

your chances of getting selected. You

9:35

know, I do. Try to select

9:37

questions that are new to me,

9:39

that have something interesting to say

9:41

about, that are relatively short, that

9:44

I think will be interesting to

9:46

listeners. So there's a lot of

9:48

criteria that go in there, even

9:50

some really good questions I can't

9:52

answer just because of bandwidth reasons.

9:55

But I appreciate your understanding in

9:57

that matter. And with that, let's

9:59

go. Julian

10:07

Mark starts us off with a priority

10:10

question. Remember that priority questions are ones

10:12

that patron supporters are allowed to ask

10:14

once. per their lifetime, at least, you

10:16

know, their initial lifetime here on Earth,

10:19

who knows, with cyclic universe models, and

10:21

I will try my best to answer

10:23

it. So, sometimes that best is okay,

10:25

sometimes it's not, but, you know, that's

10:27

the risk that you run here. The

10:30

question is, if I were floating somewhere

10:32

between our sun and the closest star,

10:34

would I be able to see my

10:36

own hands? In other words, are the

10:38

stars in our galaxy bright enough to

10:41

illuminate any object in interstellar and, if

10:43

you're right? next to it. Well, this

10:45

is a question more about your ability

10:47

to see, or at least as much

10:50

about your ability to see as it

10:52

is about astronomy, so I don't actually

10:54

know the answer. My suspicion is it

10:56

would look pretty dark to you. It's

10:59

not that much different than just saying

11:01

what What do things look like if

11:03

you're outside on a clear moonless night

11:05

in an area where there is no

11:08

artificial illumination, right? You can certainly

11:10

see stars. In fact, you can

11:12

see the Milky Way galaxy surrounding

11:14

you. It would be kind of

11:17

cool, but that's probably not enough

11:19

to reflect light off of your

11:21

hands and see them unless your

11:23

vision just is really, really good,

11:25

I suppose. That's my guess. James

11:27

Heath says, I really enjoyed your solo

11:30

episode on science funding specifically when you

11:32

said that the current administration is not

11:34

thinking seriously about what they're cutting. Do

11:36

you think we need to touch the

11:38

hot stove and suffer consequences to remember

11:40

why government funding of science vaccines, alliances

11:42

with Europe really matter? I want to

11:44

know where this... phrase of touching the

11:46

hot stove came from, like suddenly it's

11:49

everywhere on the internet, like I guess

11:51

I can figure out what it means,

11:53

but it just suddenly appeared in all

11:55

my social media feeds all at once.

11:57

I don't know where it came from. Well,

11:59

you know... Do we need to do

12:01

that? No, we should be smart

12:03

enough to know that funding science

12:05

vaccines and protecting alliances with Europe

12:08

really matter. That should not be

12:10

something we need to... test and

12:12

remember like, oh yes, these things

12:14

actually solved real problems that we

12:16

faced with. All the evidence you

12:18

need that the cutting is not

12:20

being done in any sensible way

12:23

comes from the fact that so

12:25

many things have been cut and

12:27

then uncut. So many people have

12:29

been fired and then rehired right

12:31

away. So much damage has been

12:33

done and to important things with

12:35

respect to health and science and

12:37

national defense and national security that

12:39

they're clearly not. paying attention. The

12:42

most recent one was they put

12:44

up for sale a building that

12:46

is used by the CIA for

12:48

secret operations that was supposed to

12:50

be secret. I mean it's not

12:52

the best secret in the world

12:54

but you know they just listed

12:56

it for for soon being sold

12:58

by the General Services Administration. You

13:00

know, they're very excited about cutting things, but

13:02

they're doing enormous damage. It's like saying, you

13:05

know, you know you have a tumor in

13:07

your body, so I'm just going to start

13:09

cutting things open and taking things out. Eventually

13:12

we'll find that tumor. No sensible person thinks

13:14

that this is the right thing to do.

13:16

And part of it is that... You might

13:18

think, well, if you make a

13:20

mistake, we'll just fix it, but

13:23

some of these things are not

13:25

fixable. The United States is supposed

13:27

to have a reputation as a

13:29

relatively reliable international partner. All that

13:31

talks about tariffs being put on

13:33

and then taken off has done

13:36

irreparable damage to that reputation that

13:38

we've had. People in Europe and

13:40

in Asia and elsewhere are absolutely

13:42

realizing that they cannot rely on

13:44

the United States for protection for

13:47

military support. or anything like that,

13:49

so they're gonna have to beef up

13:51

their own defenses. And there's a certain

13:53

attitude that says, well, they should defend

13:55

themselves, but you know, as far as

13:57

the United States is concerned, it really.

14:00

serves the United States' interest to

14:02

be in charge of all that,

14:04

because they might not always agree

14:06

with decisions that other places make.

14:08

I mean, maybe a multipolar world

14:10

is better in some ways. I

14:12

absolutely could see the argument for

14:14

that. The real, very obvious, huge

14:16

disadvantage to me is that some

14:18

of these other countries are going

14:20

to develop nuclear weapons. And the

14:22

more countries that have nuclear weapons,

14:24

the worse we are. worse we

14:26

all are because the greater chance

14:28

that someone uses them either intentionally

14:30

or by mistake or they lose

14:32

it or whatever. So none of

14:34

this is good. It's all bad

14:36

and it's not something that is

14:38

going to be easy to fix.

14:41

Dennis Cooperberg says, in the big

14:43

picture a crucial claim is made.

14:45

The laws of physics underlying everyday

14:47

life are completely known. This strikes

14:49

me as both highly plausible and

14:51

surprisingly almost never mentioned elsewhere. How

14:53

widely accepted would you say this

14:55

claim is among physicists or more

14:57

generally among those well-versed in modern

14:59

physics? Well, I've said this before,

15:01

but basically, when I explain the

15:03

claim to my fellow physicists, they

15:05

think for about five seconds and

15:07

go, yeah, I guess that's true.

15:10

So I don't think it's something

15:12

that they think about. You know,

15:14

scientists are kind of laser focused

15:16

on pushing beyond what we already

15:18

know into regimes that we don't

15:20

yet understand. So the typical theoretical

15:22

particle physicists spend their time thinking

15:24

about amplitudes or supersymmetry or. brains

15:27

or hidden symmetries in quantum field

15:29

theory or quantum gravity or whatever it

15:31

is, things that we don't understand very

15:33

well. So, and also of course the

15:35

fact that we understand the laws of

15:38

physics well enough doesn't really have a

15:40

huge impact on the higher emergent levels,

15:42

whether it be chemistry or biology or

15:45

whatever. It has some impact because you

15:47

might otherwise... wonder whether you're when you

15:49

know studying a chemical reaction and it

15:51

doesn't happen at the rate that you

15:54

expected it to if you didn't know

15:56

about underlying laws of physics you might say

15:58

well oh maybe there's like a a new particle

16:00

or a new field somehow involved that

16:02

is changing the reaction rates. That is

16:05

not the way to go, given what

16:07

we understand about effective field theory. So

16:09

instead, people look for much more mundane

16:12

chemical reasons for those kinds of things

16:14

and they find them. So I think

16:16

it is something that is not controversial

16:18

in the sense that there's a lot

16:21

of people out there who deny it

16:23

within the physics community, but it's not

16:25

also something that people think about that

16:27

much. And again, as I should always

16:30

add, it's, it could, it might not

16:32

be true, right? That's, I always try

16:34

to phrase it as, given everything we

16:37

know, this is absolutely what is the

16:39

most sensible thing to believe as good

16:41

basians, but who knows, you know, we

16:43

could be missing something deep. in quantum

16:46

mechanics. I don't think that that's a

16:48

very likely place to find anything new,

16:50

but other people disagree about that.

16:52

Radolfo Hansen says, I've heard you

16:55

speak positively about capitalism in the

16:57

past. Given increasing evidence in forcible

16:59

cooperative frameworks, outperform their competitive counterparts,

17:02

would you consider alternatives allow us

17:04

to step away from the negative

17:06

some game we are currently running

17:08

to a positive someone? Well, lot

17:11

to unpack here. I don't know

17:13

what that evidence is that you're

17:15

pointing to the increasing evidence about

17:18

enforceable cooperative frameworks. I'm not exactly

17:20

sure what is meant by enforceable

17:22

cooperative frameworks. I will certainly consider

17:24

alternatives. I'll always consider alternatives, but

17:27

I do think a lot of

17:29

alternatives are sort of influenced by

17:31

wishful thinking or by unrealistic expectations.

17:33

Capitalism, I think, is very very

17:35

effective at certain things, very very

17:37

harmful in other ways, and I'm

17:40

in favor of fixing it and

17:42

ameliorating the bad effects rather than

17:44

trying something completely different until we

17:46

really do get evidence that something

17:48

completely different would be better. Finally,

17:50

I don't quite agree with the

17:53

negative some game versus positive some

17:55

game. Like, there's no reason intrinsically

17:57

why capitalism has to be negative

17:59

some... game. Indeed, I think that

18:01

one could easily make an

18:03

argument that standards of living and

18:06

health and other very basic

18:08

measures have improved over years, even

18:10

for most of the less

18:12

well -off people in capitalist societies.

18:14

Not to undersell any of the

18:16

real problems under capitalism, but

18:18

there's no, again, intrinsic reason why

18:21

it's a negative sum game.

18:23

The whole idea is that you

18:25

incentivize people to be productive

18:27

and productivity makes everybody better off.

18:30

So I think that capitalism

18:32

plus a very strong taxation

18:34

and social safety net system

18:36

would actually be very obviously

18:39

positive sum. This

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-L -p.com/Mindscape. Okay

19:45

we have two questions I'm gonna group

19:47

together. They're both a little vague

19:49

so maybe that's a good reason to

19:51

group them together. One is from

19:53

Yazan al -Hajari who says, Kepler wrote,

19:55

metaphors are my truthful masters. One should

19:58

make good use of them. In

20:00

science, metaphors shape our understanding black

20:02

holes as cosmic sinks, entropy is

20:04

disorder, just as thought experiments stretch

20:06

logic to reveal deep truths. Science

20:08

fiction blends both inspiring real discoveries.

20:10

How do you see the role

20:12

of metaphor and thought experiments in

20:14

science? Are they essential tools for

20:16

discovery? Or should we be cautious

20:18

of their limits? And has any

20:20

metaphor, thought experiment or sci-fi story

20:22

ever influenced the way you think

20:24

about physics? And then Nanou asks...

20:26

When you were learning physics or

20:28

cosmology over the years, did you

20:30

incorporate your imagination? If you did

20:33

and still do when you think

20:35

about those ideas, what images does

20:37

your brain generate? So to take

20:39

the second question first from NANU,

20:41

I mean, yeah, you definitely incorporate

20:43

your imagination. I might hesitate here

20:45

because maybe you mean something different

20:47

by incorporating one's imagination than I

20:49

might mean. imagination is that just

20:51

a supernupor important part of all

20:53

of science because you're trying as

20:56

we just mentioned to push beyond

20:58

what we know to suggest ideas

21:00

for doing better than our current

21:02

theoretical models do and that is

21:04

a fundamentally act. So you say,

21:06

what images does your brain generate,

21:09

implying that imagination is somehow associated

21:11

with images in the brain? That's

21:13

one kind of imagination, but there's

21:15

other kind of imagination. You can

21:17

imagine equations. You can imagine structural

21:20

relations between different parts of the

21:22

physical world or something like that.

21:24

So imagination is absolutely centrally crucial.

21:26

And indeed, we don't understand it.

21:28

very well. We don't really understand

21:31

how it is that the human

21:33

brain comes parts of the physical

21:35

world or something like that. So

21:37

imagination is absolutely centrally crucial and

21:39

indeed we don't understand it very

21:41

well. We don't really understand how

21:43

it is that the human brain

21:45

comes up with hypotheses scientifically and

21:48

this is becoming a more directly relevant

21:50

question in the age of AI where you

21:52

might say, well I'm going to... Imagine building

21:54

an AI that will do science in the

21:56

same way that theoretical physicists do, and we

21:59

don't really know how. don't even really

22:01

have any expectations for whether that's

22:03

easy or hard or whatever so

22:05

it's becoming a very down-to-earth kind

22:07

of question. For Yuzan's question you

22:09

know what is the role of

22:11

metaphor and thought experiments it's super

22:13

crucial as a matter of empirical

22:15

fact so I don't necessarily think

22:17

that it's you need to have

22:19

thought experiments or metaphor. I could

22:21

imagine a kind of science that

22:23

was just much more straightforward and

22:25

literal, but I don't think it

22:27

would be as productive, at least

22:29

for we human beings. We human

22:31

beings definitely think in terms of

22:33

images and metaphors. I mean, one

22:35

that I like to use is

22:37

when I talk about Hilbert space,

22:39

the space of all possible quantum

22:41

states of a system in very...

22:43

commonly thought of examples. Hilbert space

22:45

is a vector space that is

22:47

infinite dimensional. In some very realistic

22:49

examples, it's still very, very big,

22:51

right? Ten to the ten to

22:53

the hundred dimensional or some crazy

22:55

number like that, right? So there's

22:57

no possible way that any human

22:59

being can actually visualize all of

23:01

those dimensions of Hilbert space in

23:03

their head. And yet we visualize

23:05

a little bit and we use

23:07

tools like reducing the number from

23:09

infinity to three. the number of

23:11

dimensions of Hilbert space, and we

23:13

make a little picture of it,

23:15

like a three-dimensional vector space. That's...

23:17

Not really a metaphor, it's just

23:19

a sort of a simplification. It's

23:21

helpful in some ways, and it's

23:23

misleading in other ways because things

23:25

become different when you have a

23:27

very very large dimensional vector space

23:29

compared to a very very small

23:31

dimensional vector space. But it's absolutely

23:33

crucial for most of us. Others,

23:35

maybe it's not crucial. Like maybe

23:37

you just memorize the rules of

23:39

a vector space. You say, oh,

23:41

a vector is helpful in some

23:43

ways. and it's misleading in other

23:46

ways because things become different when

23:48

you have a very very large

23:50

dimensional vector space compared to a

23:52

very very small dimensional vector space.

23:54

But it's absolutely crucial for most

23:56

of us. Others, maybe it's not

23:58

crucial. Like, maybe you just memorize

24:00

the rules of a vector space.

24:02

You say, oh, a vector is

24:04

something you can add to other

24:06

vectors and scale by real numbers

24:08

or complex numbers or something like

24:10

that. Everyone who understands vector spaces

24:12

knows those rules, but what I'm

24:14

saying is maybe someone only knows

24:16

those rules and doesn't ever think

24:18

about vectors as little arrows, right?

24:20

That would be fine. You could

24:22

do it that way. I always

24:24

think that science is something that...

24:26

benefits from a diverse set of

24:28

approaches, because the space of possible

24:30

ideas is very, very large, and

24:32

no matter how brilliant you are,

24:34

if you sort of have your

24:36

particular way of moving forward in

24:38

the space of ideas, you're bound

24:40

to miss some good ones. We're

24:42

all bound to miss some good

24:44

ones, and that's why you need

24:46

lots of people with lots of

24:48

different kinds of ideas, and you

24:50

need to support them, even though

24:52

they're not doing things exactly the

24:54

way that you want to be

24:56

doing them. And that is the

24:58

difficult thing to do. Are there

25:00

any metaphors, thought experiments, ever influencing

25:02

the way I think about physics?

25:04

I mean, sure, but I would

25:06

separate out those three things. Those

25:08

are very different things. Metaphors, thought

25:10

experiments, sci-fi stories. I don't think

25:12

that sci-fi stories have really influenced

25:14

the way I think about physics.

25:16

Maybe the closest is, you know,

25:18

time travel stories that tried to

25:20

make everything completely logically consistent. provide

25:22

a nice way to think about

25:24

that, because I do think that

25:26

if time travel were possible, it

25:28

would be logically consistent. It's not

25:30

a major part of my scientific

25:32

research, though, so most other science

25:34

fiction stories do not talk about

25:37

the kinds of science that I

25:39

personally am invested in. For thought

25:41

experiments, yes, I mean, thought experiments

25:43

are everything. We're always doing sort

25:45

of spherical cows, you know, imagining

25:47

if this is true, then what

25:49

would happen? That's really the bread

25:51

and butter of what theoretical physicistsists

25:53

do for a living. metaphors it's

25:55

harder you know we I'm always

25:57

skeptical of metaphors. You know, many

25:59

of you will know my long-standing

26:01

antipathy for thinking of the universe

26:03

as a balloon being blown up.

26:05

That's a metaphor, right? You know,

26:07

take a balloon, put some dots

26:09

on it with a marker, blow

26:11

it up, and say, oh look,

26:13

it's kind of like the expanding

26:15

universe, and the dots are moving

26:17

apart from each other like galaxies

26:19

are, which is... explaining something correctly,

26:21

but also getting other things very

26:23

very wrong. In that picture of

26:25

the balloon blowing up, not only

26:27

do the dots get further away

26:29

from each other, the individual dots

26:31

get bigger. and individual galaxies don't

26:33

get bigger. When you're blowing the

26:35

balloon up there is an obvious

26:37

inside and outside and in the

26:39

universe there is not. So you

26:41

can use metaphors and they're very

26:43

helpful but they are all so

26:45

dangerous and so you got to

26:47

keep your what's about you understanding

26:49

exactly what the limitations of the

26:51

metaphor are supposed to be. Mark

26:54

Sleight says, how should a layman

26:56

understand the temperature of the cosmic

26:58

microwave background radiation? Is this the

27:00

temperature a thermometer in space would

27:03

show? If it only absorbed the

27:05

microwave background and no other photons

27:07

or particle collisions? Yes, that's exactly

27:09

what it is. I mean, that

27:11

is more or less what we

27:13

measure. We have a telescope. Here

27:15

on Earth, we have a radio

27:18

telescope, right? Like, I mean, the

27:20

original one, it was in New

27:22

Jersey, but now we have more

27:24

advanced telescopes, but it's not that

27:26

hard, if you know what you're

27:28

doing, to go up on the

27:30

top of a building in your

27:32

random urban area in the United

27:35

States and put up a telescope

27:37

that can detect the cosmic microwave

27:39

background. And not only do you

27:41

detect detect photons in the radio

27:43

band coming from the CMB, but

27:45

you can, if you're good, measure

27:47

the spectrum. and the spectrum takes

27:50

the form of a black body

27:52

with a certain temperature. So that's

27:54

the temperature. It really is literally

27:56

what you're doing. Even though there

27:58

are other photons there, you build

28:00

a detector that is not sensitive

28:02

to the other photons, only to

28:04

those in a certain direction and

28:07

in a certain wavelength range, and

28:09

you detect the CMB, and you

28:11

figure out its temperature. It's really

28:13

just gas of photons bumping into

28:15

you. Anonymous says, I think democracy

28:17

only makes sense for groups of

28:19

people who share a common ontology.

28:22

If the primary concern of one

28:24

group is to secure themselves an

28:26

entrance ticket to a type of

28:28

heaven, the other group does not

28:30

believe in. The minority group needlessly

28:32

suffers. A decision between building a

28:34

dam or an airport with a

28:36

limited budget can effectively be guided

28:39

by the outcome of a popular

28:41

vote, whereas a decision on abortion

28:43

rights hinges on whether a fetus

28:45

has a soul. Given that a

28:47

majority of the population is unwilling

28:49

to reassess their ontological commitments, the

28:51

divide often results in a hostage

28:54

situation. What are your thoughts on

28:56

this? Well, I think this is

28:58

a real and very well-known problem

29:00

in democracy. We've discussed it before

29:02

on the podcast, the idea that...

29:04

A democracy is supposed to allow

29:06

for people with different value systems

29:08

to coexist together, but their value

29:11

systems have to overlap enough to

29:13

make democracy work. And in the

29:15

case of abortion or something like

29:17

that... Well, let's just try to

29:19

be the more general principle here.

29:21

In the case where someone, two

29:23

sets of people, have very different

29:26

ideas about the morality, the sort

29:28

of fundamental morality of some kind

29:30

of action, this is where democracy

29:32

is always going to get in

29:34

trouble. It's not that it can't

29:36

work, right? Like, whether it's abortion

29:38

or the death penalty or going

29:40

to war with some other country,

29:43

you can personally say, look, I

29:45

don't believe in the moral correctness

29:47

of this. I do, however, believe

29:49

in the democratic process. So what's

29:51

going to happen is I'm going

29:53

to accept that the democratic process

29:55

has led to an outcome that

29:58

I don't like, and I'm going

30:00

to protest it, and I'm going

30:02

to vote against it, and I'm

30:04

going to try to convince other

30:06

people on the other side to

30:08

come to my side, but that's

30:10

the best I can do, because

30:13

I'm part of the democracy, and

30:15

I'm subject to decisions that democracy

30:17

makes. That is inevitable, and I

30:19

think that we can easily imagine

30:21

groups of people who would not

30:23

work well, who would not function

30:25

in a functioning democracy together. You

30:27

have to imagine that the people

30:30

in the democracy are committed enough

30:32

to the values of democracy. You

30:34

know, there was a... a little

30:36

plot that I just reposted on

30:38

Blue Sky the other day. There

30:40

was a survey of values or

30:42

something like that in political parties

30:45

in the Western world. Not even

30:47

the Western world, in the world,

30:49

I guess. And they plotted them

30:51

on two axes, whether a political

30:53

party was overall liberal or conservative

30:55

in values. And then also their

30:57

importance that a political party put

30:59

on international cooperation. And you know,

31:02

we can debate. where you should

31:04

be on that plot. Are you

31:06

in favor of international cooperation? Are

31:08

you not? Are you liberal or

31:10

conservative? Are you not? That's a

31:12

very... very much up for debate,

31:14

up for grabs, that's fine. What

31:17

was interesting is that, you know,

31:19

they plotted to different countries, the

31:21

United States, the UK, Norway, Italy,

31:23

China, Turkey, Russia, and they plotted

31:25

where there was a functioning democracy,

31:27

they plotted both what the left

31:29

leaning party where they landed on

31:31

this two-dimensional plot and the right

31:34

leaning party. And there's a group

31:36

of countries and parties grouped together

31:38

that roughly speaking is either more

31:40

liberal than conservative or at least

31:42

close to neutral and more interested

31:44

in international cooperation than not or

31:46

close to neutral on that also

31:49

and includes all of the parties

31:51

right and left in countries that

31:53

we know in love as Western

31:55

liberal democracies you know the European

31:57

countries Canada or whatever except for

31:59

the right-wing party in the United

32:01

States, which is off that off

32:03

of the group of Western democracy

32:06

parties right next to China, Turkey,

32:08

and Russia, which are not democracies

32:10

at all. In other words, what

32:12

it's saying is the Republican Party

32:14

in the United States is now

32:16

closer to Russia, China, and Turkey

32:18

in its political values than it

32:21

is to any other party in

32:23

Western liberal democracies. Okay? Now maybe

32:25

there is some... room to argue

32:27

about the particular methodology of

32:29

that Survey that they did

32:31

fine go ahead and do

32:33

that But the point is

32:36

One can imagine a large

32:38

group of people in a

32:40

country abandoning what we think

32:42

of as democratic values, and

32:44

I think that that's more

32:47

the problem than people disagreeing

32:49

about a little bit of

32:51

morality because of their ontological

32:53

differences Stone R. Carroll, no

32:55

relation as far as I know,

32:58

says what are your thoughts on

33:00

the physical foundations of mathematics? It

33:02

is interesting that the universe has

33:05

produced a possibility for us to

33:07

reason about these abstract mathematical objects

33:09

and deduce objective truths about them.

33:12

For example, to me, if Zermelo

33:14

Frankel axioms are true, then one

33:16

plus one equals two is undeniably

33:19

true. Are these truths fundamental, independent

33:21

of the physical reality? Are they

33:23

emergent? What's in your opinion the

33:25

most compelling view? So I am

33:27

not an expert on this stuff.

33:30

I have grappled with it. I

33:32

have tried to get a more

33:34

nuanced understanding, but I am left

33:36

unconvinced in any of the arguments

33:38

either way. But so I can

33:40

tell you my feelings, okay, but

33:42

I'm not going to be held

33:44

to saying, you have to defend

33:46

these feelings because I... feel the

33:48

force of the countervailing arguments. I'm

33:50

not a mathematical realist, okay? I

33:52

don't think that we should think

33:55

of mathematical objects as being real,

33:57

at least not in the same

33:59

sense. as we think about physical

34:01

things as being real. So I

34:03

think that physical things are real,

34:05

or at least the physical world

34:07

is real. We divide it up

34:09

into sub things, and that's our

34:12

move, not the universe's move. And

34:14

it turns out, maybe it didn't

34:16

have to turn out this way,

34:18

but it turns out that there

34:20

are patterns inherent in the sort

34:22

of instantiation of physical reality that

34:24

are describable by what we call

34:26

mathematics. Okay, one plus one equals

34:28

two is one way of saying

34:30

that every time I have one

34:32

coffee cup and another coffee cup,

34:34

now I have two coffee cups

34:36

and et cetera. There's sort of

34:38

a physical understanding of what that

34:40

means. And when you get into

34:43

the more wild areas of mathematics

34:45

with transfinite numbers and things like

34:47

that, maybe there isn't any physical

34:49

instantiation of that, and maybe it

34:51

sort of doesn't matter. So I

34:53

think where it really becomes, we

34:55

had this conversation on the podcast

34:57

not too long ago with Joel

34:59

David Hamkins, so you're welcome to

35:01

check that out. In a previous

35:03

discussion with Justin Clark Doan that

35:05

touched on these things, there

35:08

are, it is a well

35:10

known fact in post 20th century

35:12

mathematics, or I guess post

35:15

19th century mathematics that you can

35:17

easily write down axiom systems

35:19

that are very similar to each

35:21

other, but differ in one

35:23

axiom, and whether or not that

35:25

axiom is there, or the

35:27

opposite of that axiom is there,

35:29

or that axiom is neither

35:31

there nor not there, all of

35:33

those are consistent systems, right?

35:35

Like the continuum hypothesis, the existence

35:37

of infinite numbers that are

35:39

larger than the number of countable

35:41

numbers, the integers, but smaller

35:43

than the number of real numbers.

35:45

Is that true or false?

35:47

Well, you can choose. You can

35:49

pick an axiom to include

35:52

or not to include. And to

35:54

me, that means like clearly

35:56

these things are not objectively real.

35:58

There are ways that we

36:00

are constructing systems ourselves that turn

36:02

out to be super duper... useful

36:04

for discussing physical reality. For what it's worth I do have

36:06

a paper where I express these feelings. It is called reality

36:08

realism. You're welcome to check it out. Yusuf

36:10

says, do you think taking more

36:12

abstract math courses is beneficial for

36:14

a physics student wanting to pursue

36:16

higher education in physics? For example,

36:18

classes like real analysis, topology, and

36:20

abstract algebra. I'm curious if you

36:23

think being trained in upper level

36:25

math courses is beneficial for people

36:27

doing not just theoretical research but

36:29

experimental. Well, I think it's a

36:31

cost-benefit analysis question. All else being

36:33

equal, yes, it is absolutely useful

36:35

to take those courses. It's also

36:37

useful to learn foreign languages and

36:39

to learn programming languages and to

36:41

appreciate the history and philosophy both

36:43

of science and other things. Maybe

36:45

it's beneficial to take classes in

36:47

literature or poetry because it makes

36:49

you a more eloquent explainer of

36:51

your science. So there's lots of

36:54

things that could be beneficial. Whether

36:56

or not taking a class in real

36:58

analysis, for example, for those of you

37:00

who don't know, real analysis is like

37:02

the fancy pants way of saying calculus.

37:05

But it gets very, very fancy, so

37:07

you almost don't recognize it anymore. Like

37:09

once you take seriously the number of

37:11

numbers on the real line, things go

37:14

pretty wild. And a lot of your

37:16

common sensical ways of thinking about math

37:18

break down, so you have to like

37:20

stick with what the axioms are actually

37:23

telling you, and then that's... That's a

37:25

step along the way to becoming

37:27

a more rigorous mathematician. Physicists generally

37:29

don't care about any of that

37:32

stuff. Generally, sometimes they might. But

37:34

generally, you just do an integral.

37:36

You're not worried too much about

37:39

all the higher level details of

37:41

proving that it converges or whatever.

37:43

Some areas in quantum field theory,

37:46

where you really try to prove

37:48

careful theorems, then you need some

37:50

functional analysis, real analysis, real analysis.

37:53

topological considerations and so

37:55

forth. But that's, you know, a

37:57

tiny little subset of physics, even

37:59

theoretical. physics, like most theoretical physicists,

38:01

if you want to calculate the

38:04

scattering amplitude of two electrons into

38:06

two photons or whatever, okay, you

38:08

don't need any of that fancy

38:10

math to do that. I think

38:12

it's good training because it stretches

38:14

your brain. It really is, mathematics

38:16

is the most rigorous I count

38:18

mathematics and sort of logic together

38:20

in a set of things that

38:22

say like here's a set of

38:24

axioms, what can you prove? And

38:26

that way of thinking is really

38:29

good exercise. It's a good calisthenics

38:31

for your brain, okay? But the

38:33

actual substance of what you learn,

38:35

you know, about some theorem, about,

38:37

you know, contractability of a certain

38:39

space or whatever, will be... unlikely

38:41

to be directly useful to you

38:43

in your physics research. And again,

38:45

it could be if you're one

38:47

of those supermathematical physicists, but you're

38:49

asking in general, and I think

38:51

that most physicists learn the math

38:53

they need as they go, rather

38:56

than learning math classes. And the

38:58

other thing is... Mathematicians are doing

39:00

math for different reasons than physicists

39:02

are. Physicists want to get the

39:04

answer and they want to put

39:06

it to work. You know, when

39:08

I was in grad school and

39:10

it dawned on me from taking

39:12

quantum field theory classes, etc. that

39:14

the idea of group theory and

39:16

Lee groups and Lee algebras and

39:18

representations was really important. I sat

39:21

in on a class in the

39:23

math department on the groups and

39:25

the algebras and it was entirely

39:27

a waste of time. It was,

39:29

you know, like theorem lemma proof,

39:31

you know, showing that something could

39:33

be diagonalizable or representation was faithful

39:35

or whatever it was, and as

39:37

a physicist, you would just look

39:39

it up. you just say, oh,

39:41

is this true? Okay, it is.

39:43

All right, I'm going to move

39:45

on, right? And very elaborate methods

39:48

of proving these things. So what

39:50

you want out of these mathematical

39:52

concepts is different as a mathematician,

39:54

and that's fine. But don't think,

39:56

I guess, is the short answer

39:58

that you need to take fancy

40:00

math classes to be a very

40:02

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40:54

restrictions may apply. Astro Nobel says,

40:56

I hear a lot of people,

40:58

scientists and laymen alike, talk with

41:00

confidence about the existence of extraterrestrial

41:02

life and the chances to find

41:05

it in the near future. I

41:07

have the impression that proper Bayesian

41:09

reasoning is not applied most of

41:11

the time, and that expectations are

41:13

often mixed with hope and wishful

41:15

thinking. No matter what we find

41:17

or fail to find, credences are

41:19

never lowered. Why are people so

41:21

reluctant to admit that new results

41:23

indicate that life may not exist

41:25

outside the earth at all? How

41:27

should a good Bayesian reason about

41:30

this? Well, I think that the

41:32

thing about Bayesianism, of which I'm

41:34

a big fan, is the following.

41:36

You admit that you start your

41:38

investigation with prior credences, right? You

41:40

have priors for something being true,

41:42

and then you update them when

41:44

new evidence comes in. And... The

41:46

way that you update them is

41:48

on the basis of what are

41:50

called likelihood functions. Given all the

41:52

different possible theories, under which theory

41:54

would, no, under each theory I

41:57

should say, would the new information

41:59

be probable or improbable? and conditions

42:01

under which the information you're

42:03

getting is probable would increase

42:05

in their credences and that's

42:08

given you your posterior not

42:10

your prior people keep calling it

42:12

a prior even after it's been

42:14

updated but that is you know

42:17

technically not correct so The big

42:19

worry about Bayesian reasoning is what

42:21

if we start with very very

42:23

different priors, which is allowed by

42:26

the rules of Bayesianism, and then

42:28

you require enormous overwhelming evidence in

42:30

the form of likelihood functions to

42:32

converge on a common answer. There

42:35

are theorems that assure us that

42:37

if we get enough evidence, we

42:39

will always converge on the common answer,

42:41

but... You can easily find yourself in

42:44

a situation where, number one, priors are

42:46

very different, and number two, there's just

42:48

not enough evidence to move them very

42:50

much. I think that's the situation we're

42:53

in right now with life on other

42:55

planets. We have the fact that we

42:57

exist. Some people take our existence to

43:00

say you should have a prior that

43:02

life is actually pretty ubiquitous, that it's

43:04

easy to make. You'll keep being told

43:06

that life arose relatively quickly here on

43:09

earth, even though it might have

43:11

been hundreds of millions of years,

43:13

still relatively quickly compared to the

43:15

billions of years that we've been

43:17

around. and therefore the argument goes

43:20

your prior should be large. Other

43:22

people will say, well, I have

43:24

a prior that it's very small,

43:26

I have evidence that we haven't

43:28

met any other civilizations yet, and

43:31

that decreases my prior to an

43:33

even lower number, and that's both

43:35

perfectly fine. There's a lot of

43:37

evidence, and none of it is...

43:39

definitive, I guess. I mean, there's a

43:42

lot of evidence in some sense. What

43:44

I mean is there's a lot of

43:46

different kinds of evidence. There's evidence from

43:48

biochemistry and thinking about the origin of

43:50

life. There's evidence that we've looked for

43:52

a lot of planets, and we found

43:54

a lot of planets, right? So

43:56

whatever your credence is that life on

43:59

other planets exist, based purely on the

44:01

number of planets we found, it's very

44:03

reasonable that it should be higher now

44:05

than it was before. Based on the

44:07

fact that none of them have stood

44:10

up and said, hi, your credence should

44:12

be lower than it was before, and

44:14

there's a battle going on. So I

44:16

just don't think that the evidence is

44:18

strong enough in any way to... really

44:21

be upset if people still have credences

44:23

that are very different than yours. That's

44:25

why I'm very, very open-minded about this

44:27

particular question. The credences are just not

44:30

pinned very close to zero or one.

44:32

Chris Mason says, how do you feel

44:34

about the 76ers season so far? Disappointed

44:36

or as expected. So I'm not sure

44:38

if Chris is teasing me a little

44:41

bit here, but for those of you

44:43

basketball fans out there, my team, the

44:45

Philadelphia 76ers, went into the season with

44:47

enormously high expectations, having two superstars on

44:49

the team, Joelle Embed and Tyres Maxie,

44:52

and getting a third superstar, Paul George,

44:54

as a free agent, and doing a

44:56

pretty good job of building out the

44:58

rest of the roster on very cheap.

45:00

contracts, etc. So expectations were very high

45:03

and it has been a complete unmitigated

45:05

disaster. And it's a weird, like it's

45:07

so disastrous this season that it's almost

45:09

inexplicable. You know, it's not really that

45:11

the team was ill-constructed. You know, the

45:14

obvious thing is there have been injuries,

45:16

especially to Joelle and Bede. If you,

45:18

I follow this too closely, so for

45:20

those of you who care, Joe Allenbeat

45:23

had a knee injury and... There's a

45:25

question of how do you get better

45:27

after the knee injury. He's had a

45:29

lot of injuries over the year, but

45:31

I think people hope and beat has

45:34

been shut down for the year. They're

45:36

gonna try other different strategies for getting

45:38

him better. I still, you know, I

45:40

recognize that I am not the general

45:42

manager of the team. I'm not the

45:45

coach of the team. I'm not a

45:47

player on the team. My job is

45:49

to enjoy the team's success. So I'm

45:51

going to continue to be optimistic that

45:53

next year, everyone's gonna be optimistic. to

45:56

happen. Peter Bamber says, you recently said

45:58

that for the first time you had

46:00

a thought about leaving the USA as

46:02

a consequence of political changes, though you

46:05

have no plans to do so. What

46:07

is the view amongst your friends and

46:09

colleagues on this topic? Well, look, I

46:11

think most people don't really want to

46:13

leave their... houses and their jobs, right?

46:16

Especially in academia, that's super hard to

46:18

do. If you're like a genius superstar,

46:20

then you can call up another university

46:22

and get a job offer, but most

46:24

people, you know, getting a job is

46:27

very difficult and very precious and you

46:29

hang on to it when you have

46:31

it, especially at a moment when funding

46:33

and things like that are very precarious.

46:35

It's super precarious here in the United

46:38

States, obviously. The president of John's... just

46:40

put out an email, which was overall,

46:42

I think, a pretty good email. Ron

46:44

Daniels is the president, and he was

46:46

sort of, he made the point, which

46:49

I hoped he would make, that we

46:51

still stand up for diversity and pluralism

46:53

here at Johns Hopkins, but he also

46:55

said, look, we're getting cut. by an

46:58

enormous amount and it might be a

47:00

devastating set of cuts coming down the

47:02

road, even though they don't know exactly

47:04

what they are yet. As I said,

47:06

because we have no idea what the

47:09

actual funding cuts are going to be,

47:11

so it's very hard to do planning

47:13

for the future. So that kind of

47:15

thing makes people worried, you know. Certainly

47:17

if I were a young person, if

47:20

I were looking at postdocs, and I

47:22

had a chance to go to a

47:24

country that was a little more reliable

47:26

in their funding of science, then I

47:28

would take that very, very seriously. But,

47:31

you know, as an old settled person,

47:33

you know, I'd rather, you know, just

47:35

stick around, and I think that that's...

47:37

basically what people think. I think that

47:40

a lot of young people, you know,

47:42

we're right now, it is early March,

47:44

which means that we're recruiting new grad

47:46

students and things like that. Some major

47:48

universities have already said we're not going

47:51

to accept any new graduate students this

47:53

year. Others have accepted grad students and

47:55

then rescinded the offer to them because

47:57

they just don't have. money. And this

47:59

is, it makes a very difficult time

48:02

of a young person's life even more

48:04

difficult in ways that, you know, my

48:06

heart breaks for them and I really

48:08

feel bad for them. Here at Hopkins,

48:10

we're thinking that we can just stick

48:13

with the number of grad students that

48:15

we've already accepted, so we're recruiting them,

48:17

and in fact, it looks like we're

48:19

going to do much better this year

48:21

at getting people to come to Hopkins

48:24

because we're better than average in terms

48:26

of... assuring the prospective grad students that

48:28

they will get a position when they

48:30

arrive. But if I had an option

48:33

to go somewhere else that, you know,

48:35

things were more reliable and I would

48:37

take that very, very seriously. I don't

48:39

yet know of any senior colleagues who

48:42

are saying, I'm picking up and leaving.

48:44

This is something that takes months or

48:46

years to really sink in to people.

48:49

So I don't think it's like that

48:51

anyone will snap their fingers and suddenly

48:53

will lose 10 percent of our scientists,

48:55

but... there's an accumulated effect that is

48:58

sort of difficult to discern from moment

49:00

to moment and it's many little

49:02

changes in outlook that add up to

49:04

a big effect. So I don't I

49:07

don't see in any exodus from the

49:09

United States right now but I think

49:11

the long-term effects are going to be

49:13

very very noticeable. Paulina Vino

49:15

says, do you think that agents made

49:18

up of conscious agents, for example

49:20

a company or a society, can themselves

49:22

have a conscious experience? What are

49:24

the caveats for this and how would

49:26

we know if say a corporation

49:28

or a country were conscious if we

49:31

can even know this? So I

49:33

think... I don't think it's useful to

49:35

think of countries as being conscious in

49:37

the same way that we human beings

49:40

are being conscious for a number of

49:42

reasons. I should mention that not everyone

49:44

agrees. Eric Schutzkable, who is a previous

49:47

mindscape guest, has written a paper saying

49:49

that if you are materialist about ontology

49:51

and you think that, you know, consciousness

49:53

is just an immersion property, both of

49:55

which are true for me, then you

49:57

should probably think that the United States

49:59

is conscious. which I don't think. But

50:01

my reason for thinking that is

50:03

not thinking that it's impossible in

50:05

principle, but I think that there

50:07

are questions of time scales and

50:09

integration that aren't quite... appreciated in

50:12

most discussions of what consciousness is.

50:14

When we think about consciousness, we

50:16

think about not just a person

50:18

contemplating themselves, we also think about

50:20

their interactions with other people, right?

50:22

And, you know, people just are

50:24

smaller and quicker than countries or

50:26

corporations. They can have a lot

50:28

of thoughts in a very short

50:30

period of time, and those thoughts

50:32

are kind of coherent. You know,

50:34

we know that in the brain

50:36

lots of incoherent things are going

50:38

on, lots of different parts of

50:40

the brain. are bouncing back and

50:42

forth and interacting with each other

50:45

much like a country or a

50:47

corporation. But in physics terms you

50:49

would say that the bouncing around

50:51

is tightly coupled, right? Like there's

50:53

part of your brain that's literally

50:55

right next to the other part

50:57

of your brain and very very

50:59

quickly exchanging information and coming to

51:01

some equilibrium or consensus or whatever

51:03

in ways that doesn't quite happen

51:05

for a country or a corporation.

51:07

So I think that you know

51:09

there are... details about what is

51:11

necessary to say that a group

51:13

is truly conscious that tend to

51:15

be absent in these dilute large-scale

51:17

things like countries or corporations. But

51:20

that's more or less a feeling.

51:22

There's nothing quantitative there. I'm open

51:24

to the possibility. I guess I

51:26

would need some operational. way of

51:28

thinking about it. What is the

51:30

difference that it makes to thinking

51:32

about the behavior of a country

51:34

or corporation to say that it

51:36

is conscious or not? I think

51:38

that when it comes to human

51:40

beings, we invent the concept of

51:42

consciousness because it is explanatory. It

51:44

helps us understand how people are

51:46

behaving. Oh, this person is conscious

51:48

of this happening and that's why

51:50

they did this other thing. Not

51:53

sure that that talk is very

51:55

useful when it comes to countries

51:57

or corporations, but, you know, maybe

51:59

in some circumstances it is. I'm

52:01

open to the possibility. Morrison Chady

52:03

or Chaddy says, when I was

52:05

in high school we were told

52:07

that the 19th century scientists were

52:09

looking for a medium which they

52:11

called ether in which light waves

52:13

would propagate. Eventually, the theory of

52:15

electromagnetism established that there was no

52:17

such medium. Yet I can't help

52:19

but think that the original view

52:21

was vindicated by quantum field theory.

52:23

Isn't the electron field of quantum

52:26

field theory the equivalent of ether?

52:28

No. It is not the equivalent

52:30

of ether. I have answered this

52:32

question or talked about it in

52:34

various times, but it's been a

52:36

while, so let's address it again.

52:38

The fields of quantum field theory

52:40

are just the quantum versions of

52:42

the fields of classical field theory.

52:44

So if you think that classical

52:46

electromagnetism, which is a classical field

52:48

theory, doesn't need ether, then you

52:50

think that quantum fields don't need

52:52

ether either. The point is that

52:54

either was supposed to be, like

52:56

you say, a medium in which

52:58

waves propagate. Whereas in contrast... Field

53:01

theory, classical or quantum, takes the

53:03

fields as the fundamental independent entities.

53:05

The waving electron field or the

53:07

waving electromagnetic field or the waving

53:09

Higgs field or whatever, none of

53:11

these are waves in something other

53:13

than themselves. Okay, so that's the

53:15

ontological difference. And there's also a

53:17

practical difference. The whole point of

53:19

the ether in 19th century physics

53:21

was to allow for there to

53:23

be a rest frame. with respect

53:25

to which you can measure your

53:27

motion, as opposed to the naive

53:29

reading of Maxwell's equations, which say

53:31

there is no universal rest frame.

53:34

So 19th century physicists went to

53:36

great lengths to sort of bend

53:38

over backwards and figure out how

53:40

you could reconcile the existence of

53:42

a rest frame determined by the

53:44

ether with the fact that you

53:46

couldn't observe it in any way

53:48

in Maxwell's equations. And that's how

53:50

they invented things like Lorentz transformations,

53:52

even before relativity came on the

53:54

scene. But in quantum field theory,

53:56

there's no rest frame. There's no

53:58

rest frame. Everything is. perfectly relativistically

54:00

invariant. So the whole point of

54:02

the ether is completely missing in

54:04

quantum field theory. So I don't

54:07

think that's an especially useful way

54:09

of thinking about things. Mark Foske says,

54:11

you have said that it's wrong to

54:13

think of the inside of a nucleon

54:15

as a dynamic place with lots of

54:17

quarks popping into and out of existence.

54:20

To the best of my understanding, it's

54:22

Matt Strassler who popularized that very view.

54:24

Can you think of something about how

54:26

a physicist could arrive at such a

54:28

So it's certainly not Matt who popularized

54:31

that view. That view has been around

54:33

forever. This is a very very common

54:35

way that physicists talk, as if the

54:37

vacuum state or a particular state of

54:39

a proton or neutron is actually

54:42

wildly fluctuating back and forth. And

54:44

I think it's just because people

54:46

don't have what I would call

54:49

the right. philosophical view of how

54:51

to think about quantum states. There's

54:53

a relationship between our classical way

54:56

of thinking and then what happens

54:58

when we quantize it. And people

55:00

kind of are reluctant to let

55:03

go of that classical way of

55:05

thinking. I think that if you

55:08

asked any physicist, is the quantum

55:10

state of a proton in its

55:12

lowest energy state? Is it static?

55:14

Or is it dynamical? Right? So

55:16

as a literal question, you know,

55:18

there's a quantum state, sie, a

55:20

vector in Hilbert space, that represents

55:22

a single proton, alone in the

55:24

universe, in its lowest energy state,

55:26

and just ask them, is that

55:28

static or not? If they thought

55:30

about it carefully, they would tell

55:33

you is static, right? So the

55:35

question is, is that all that is

55:37

going on? If you were somehow... to observe

55:39

what is happening inside the proton over and

55:41

over again. So you make a measurement of

55:43

the proton that excites it because you're interacting

55:45

with it so it's no longer in its

55:47

ground state, but okay, now you let it

55:50

settle back down and you measure it again,

55:52

you let it settle back down and you

55:54

measure it again, or you just measure a

55:56

million protons separately, each in their ground states.

55:58

You would see different answers. Every time you

56:01

measure it, because that's the nature

56:03

of quantum mechanics, and there is

56:05

a really strong impulse when you

56:07

measure something over and over again

56:09

and see it moving around from

56:11

measurement to measurement, to think that

56:13

it's moving around when you're not

56:15

measuring it. But if you take

56:17

the point of view that the

56:19

quantum state is what really exists,

56:21

that's just not true. So I

56:23

think it's a very common view.

56:25

I think that physicists have avoided

56:27

talking to philosophers for a long

56:29

time and haven't thought about this

56:31

very carefully, but I'm going to

56:33

do my part to change their

56:35

minds. Tariq says, would you be

56:37

able to talk about information conservation

56:39

from a few perspectives to try

56:41

to help clarify what information actually

56:43

means in this context, particularly at

56:45

the quantum level, and in the

56:47

context of many worlds and why

56:49

there is such a strong perspective

56:51

that it must be conserved. A

56:54

common example that's given is if

56:56

a book is burned and you

56:58

gathered all the energy, smoke ashes,

57:00

etc. You could in principle reconstruct

57:02

the book in all respects. Binding

57:04

glue all the way down to

57:06

every atom and its state. If

57:08

they were radioactive elements in the

57:10

ink and they were decaying randomly,

57:12

as the book was burned, how

57:14

could all this be unambiguously reversible

57:16

in principle, and I don't expect

57:18

such a machine to be built,

57:20

such that no information is lost?

57:22

Yeah, I mean when you talk

57:24

about information conservation in general in

57:26

physics Let's first be clear about

57:28

what we mean by information because

57:30

lots of different people mean different

57:32

things I'm not going to go

57:34

through all the different definitions, but

57:36

the relevant one here is the

57:38

data that you require to precisely

57:40

specify the physical state of a

57:42

system So in good old classical

57:44

mechanics you imagine you have some

57:47

number of degrees of freedom, maybe

57:49

they're particles points of a field

57:51

in space, and typically the relevant

57:53

parts of information you need to

57:55

specify the state are the position,

57:57

the configuration of those degrees of

57:59

freedom, and the momentum of those

58:01

degrees of freedom, whether it's a

58:03

particle or a field or whatever.

58:05

In quantum mechanics, the state of

58:07

the entire system is generally specified

58:09

by the quantum state, the wave

58:11

function, whatever you want to call

58:13

it, the vector in Hilbert space.

58:15

There's details there about, you know,

58:17

maybe you could think of a

58:19

density operator which indicates a distribution

58:21

over possible quantum states as more

58:23

general, but that's not the point

58:25

right here. We can think of

58:27

everything as just a quantum state.

58:29

So if you give the wave

58:31

function, you've given the information, and

58:33

the statement of information conservation is

58:35

just that the amount of information

58:37

you need to specify the state

58:40

at one moment in time is

58:42

preserved over time. So if I

58:44

give you the equation, the information

58:46

to specify the state at one

58:48

moment, and I use the Schrodinger

58:50

equation to evolve it forward in

58:52

time. I can also go backward.

58:54

The information that was in the

58:56

original state is preserved. It's modified

58:58

by the fact that it's evolving

59:00

under the Schurner equation, but it's

59:02

still there. If you know the

59:04

Schurner equation, you can figure out

59:06

from the future state what the

59:08

past state was. Now, quantum mechanics.

59:10

raises a complication here because there's

59:12

such a thing called measurement. The

59:14

way that we usually talk about

59:16

quantum mechanics is there are two

59:18

different ways that a quantum state

59:20

can evolve. When you're not measuring

59:22

it, it evolves according to unitary

59:24

evolution, which is a fancy way

59:26

of saying it obeys the shorteninger

59:28

equation. But when you measure it,

59:30

the wave function collapses. Of course,

59:32

in many worlds, you interpret that

59:35

measurement event as actually just a

59:37

branching of the wave function. so

59:39

that the wave function as a

59:41

whole just does unitary evolution. But

59:43

inside a branch, which is where

59:45

actually observers live, they do not

59:47

see unitary evolution. They see wave

59:49

functions collapsing when measurement is done.

59:51

But of course, there's a more

59:53

sophisticated notion of what measurement means

59:55

in many worlds. It doesn't actually

59:57

require any conscious being to measure

59:59

it. It just requires... decoherence and

1:00:01

branching of the wave function. So, whether

1:00:03

or not information is conserved just

1:00:05

depends on what kind of evolution

1:00:08

you're talking about. In the overall

1:00:10

unitary evolution of the wave function

1:00:12

in many worlds, information is conserved.

1:00:14

In Copenhagen or objective collapse models,

1:00:16

it would not be. conserved. But

1:00:18

from the perspective of an observer

1:00:21

in a branch, that information is

1:00:23

completely lost because you do not

1:00:25

see the entire wave function of

1:00:27

the universe. So if you burn

1:00:29

a book or burn something else

1:00:31

in a fire and try to

1:00:34

collect all the information about it,

1:00:36

and like you say, in the

1:00:38

process there's some radioactive decay in

1:00:40

the wave function of the universe

1:00:42

branches, then there is no way.

1:00:44

in principle or in practice for

1:00:46

you to accumulate all the information

1:00:48

that was in the book ahead

1:00:50

of time. The statement is that

1:00:52

it's there in the wave function

1:00:54

of the universe, but that's very

1:00:56

different than saying you can actually

1:00:58

recover it somehow. So those kinds

1:01:00

of thoughts experiments are always a

1:01:03

little bit unrealistic and in fact

1:01:05

are super duper unrealistic if you

1:01:07

believe in branching of the wave

1:01:09

function. But it's just a statement

1:01:11

about the unitary evolution part of

1:01:14

quantum mechanics, not a statement about

1:01:16

measurement. Everyone knows that in measurement

1:01:18

information is not conserved. Nicola

1:01:20

Ivanov says, my question is about

1:01:22

possible information loss. See what I

1:01:24

did there? I put these questions

1:01:26

right next to each other because

1:01:28

they make sense together. Possible information

1:01:30

loss for a hypothetical observer when

1:01:33

our universe eventually enters the phase

1:01:35

of the dissiter vacuum. Are degrees

1:01:37

of freedom of the universal wave

1:01:39

function inaccessible hidden behind the dissiter

1:01:41

cosmological horizon for a hypothetical observer?

1:01:43

Or do they remain scrambled at

1:01:45

the cosmological horizon and somehow recoverable

1:01:47

in principle similarly to a black

1:01:49

hole horizon? Yeah, nobody knows that

1:01:51

is not something that is understood

1:01:53

for those of you who are

1:01:56

not familiar with this story You

1:01:58

know our universe is accelerating discovered

1:02:00

in 1998 and we attribute that

1:02:02

to dark energy pushing the universe

1:02:04

apart. We don't know exactly what

1:02:06

the dark energy is, but the

1:02:08

leading candidate is simply a cosmological

1:02:10

constant, a constant amount of energy

1:02:12

density. And if that's true, that

1:02:14

can stay like constant forever and

1:02:16

it will push our universe apart

1:02:19

forever and our universe will settle

1:02:21

down into a... cold, desolate, empty

1:02:23

state called dissiter space with nothing

1:02:25

in it other than the vacuum

1:02:27

energy, the cosmological constant, the dark

1:02:29

energy that is pushing the universe

1:02:31

apart. in that case we will

1:02:33

have a horizon around us, much

1:02:35

like a black hole has a

1:02:37

horizon, but in this case we

1:02:39

are looking at the horizon from

1:02:41

inside, and there's no singularity associated

1:02:43

with it. It's just a horizon

1:02:45

in the sense that if something

1:02:47

goes outside the horizon, then from

1:02:49

our point of view, it can

1:02:51

never come back. It is separated

1:02:53

by faster than speed of light

1:02:55

barrier. in the context of information

1:02:57

conservation, would you, would it be

1:02:59

right to think of things that

1:03:01

are inside our desiter observable universe

1:03:03

as going outside and being lost

1:03:05

forever? Or can they somehow eventually

1:03:08

come back? I think that the

1:03:10

simple understanding is that they're lost

1:03:12

forever. And the real difference with

1:03:14

the black hole case is that

1:03:16

a black, so there's a similarity

1:03:18

first, I should say. Again, for

1:03:20

those of you who aren't familiar,

1:03:22

both a black hole horizon and

1:03:24

a decider horizon have a temperature

1:03:26

and they have an entropy. This

1:03:28

is all very, very similar calculations.

1:03:30

When Hawking and Beckenstein first figured

1:03:32

out the stuff about black holes,

1:03:34

Hawking and Gary Gibbons soon thereafter

1:03:36

showed that the same kind of

1:03:38

thing is true for the horizon

1:03:40

and decider space. So there's a

1:03:42

temperature, there's radiation. The radiation for

1:03:44

our real world would be very,

1:03:46

very, very cold. You know, if

1:03:48

it's about... three degrees Kelvin outside

1:03:50

in the cosmic microwave background right

1:03:52

now. The eventual dissiter temperature would

1:03:54

be something like 10. to the

1:03:57

minus 30 Kelvin very roughly speaking.

1:03:59

So the point is it's much

1:04:01

much much much much lower. But

1:04:03

in principle it's there. So you

1:04:05

might ask can we get that

1:04:07

information back? The difference is black

1:04:09

holes evaporate. Decider space doesn't. as

1:04:11

far as we know. So black

1:04:13

holes don't last forever. Before we

1:04:15

knew about black hole evaporation, Allah

1:04:17

Hawking, people didn't worry that much

1:04:19

about information loss because you say,

1:04:21

well, I've thrown some information into

1:04:23

the black hole, I can't get

1:04:25

it back, but it's still in

1:04:27

there. Right? So I'm not that

1:04:29

worried about it. Whereas once you

1:04:31

know the black hole can evaporate,

1:04:33

now you're like, oh, well, it's,

1:04:35

there's no more black hole after

1:04:37

it's evaporated. There's nowhere for that

1:04:39

information to be. It must have

1:04:41

returned to us in the radiation.

1:04:43

Maybe, maybe not. You know, we

1:04:46

think that that's the nice way

1:04:48

to think about unitary evolution, as

1:04:50

just explained. But of course, we

1:04:52

don't know the ultimate laws of

1:04:54

physics yet. Decider space, however, is

1:04:56

forever. It's the attractor solution. It's

1:04:58

the equilibrium solution. It's the highest

1:05:00

entropy state the universe can be

1:05:02

in. So as far as we

1:05:04

know, that horizon just stays there.

1:05:06

And there's no sense in which

1:05:08

the information that goes beyond the

1:05:10

horizon needs to come back to

1:05:12

our observable universe. That's not to

1:05:14

say it doesn't. You know, we

1:05:16

don't. there is an open question

1:05:18

about whether or not we should

1:05:20

think of dissiter space as a

1:05:22

finite number of degrees of freedom

1:05:24

inside the horizon and an infinite

1:05:26

number outside or as a finite

1:05:28

number of degrees in degrees of

1:05:30

freedom inside the horizon and everything

1:05:32

outside is just sort of a

1:05:35

mirage. Everything that we're thinking about

1:05:37

as being outside the horizon is

1:05:39

actually encoded on the horizon and

1:05:41

there's only a finite number of

1:05:43

degrees of freedom to the whole

1:05:45

shebang. Okay, we don't know because

1:05:47

there's lots of things we don't

1:05:49

know about quantum gravity, holography, things

1:05:51

like that. But I think that

1:05:53

the easy way to think about

1:05:55

it until there's some strong evidence

1:05:57

otherwise is that the information just

1:05:59

leaves us when it crosses the

1:06:01

dissiter horizon and we're never going

1:06:03

to get it back. It's out

1:06:05

there, but we're never going to

1:06:07

be able to see it ourselves.

1:06:09

Water says, if special relativity says

1:06:11

there is no universal now, how

1:06:13

does many worlds know how to

1:06:15

split? Or when to split, sorry.

1:06:17

Many worlds is very smart. It

1:06:19

knows lots of things. I think

1:06:21

that this is an example where

1:06:24

I'm going to invoke the thing

1:06:26

that I often say, which is

1:06:28

that the idea of branching. in

1:06:30

many worlds is made up by

1:06:32

human beings. The laws of physics

1:06:34

are simply that the universe obeys

1:06:36

the Schrodinger equation. The universe is

1:06:38

described mathematically as a wave function

1:06:40

or a vector in Hilbert space,

1:06:42

and it obeys a Schrodinger equation.

1:06:44

There's nowhere in there any mention

1:06:46

in the fundamental... description of what

1:06:48

many worlds is of branches or

1:06:50

splits or anything like that. Those

1:06:52

are higher level emergent phenomena. That's

1:06:54

why David Wallace's book, former Mindscape

1:06:56

guest David Wallace, his famous book

1:06:58

about many worlds, is called the

1:07:00

emergent multiverse. And the thing about

1:07:02

emergent things is we choose to

1:07:04

define them by throwing away information,

1:07:06

right? By coarse graining or whatever,

1:07:08

by making some choices about what

1:07:10

information matters to us and what

1:07:13

doesn't. Typically in emergence and things

1:07:15

like the emergence of a fluid

1:07:17

description from a bunch of molecules,

1:07:19

there's more or less a unique

1:07:21

way. to throw away that information

1:07:23

to do the course graining. In

1:07:25

the case of the branching of

1:07:27

the wave function that's not true.

1:07:29

We can choose to let the

1:07:31

branching happen in all sorts of

1:07:33

different ways. So some people think

1:07:35

that branching should be thought of

1:07:37

as only happening inside a light

1:07:39

cone. I'm not a big fan

1:07:41

of that because I don't think

1:07:43

that light cones are fundamental. I

1:07:45

think that quantum gravity exists and

1:07:47

you should take advantage of that.

1:07:49

So what I like to say

1:07:51

is, you can do the branching

1:07:53

whatever way makes sense to you

1:07:55

as long as compatible with observationalational

1:07:57

with observationalational outcomes. In particular, in

1:07:59

terms of special relativity, saying that

1:08:02

different people are going to choose

1:08:04

different reference frames, that's just a

1:08:06

way of saying that I can

1:08:08

do the branching differently, depending on

1:08:10

what reference frame I'm in. And

1:08:12

the point is, it makes zero

1:08:14

difference to any observational outcome, how

1:08:16

you do the branching. There's no

1:08:18

right way to do it. There's

1:08:20

no implication. If I'm here and

1:08:22

I have a spin and it's

1:08:24

entangled with some spin very far

1:08:26

away, and I'm going to measure

1:08:28

it. I might use a language

1:08:30

that said, oh, the wave function of

1:08:32

the other spin collapses now in my

1:08:35

reference frame. But nobody cares what I

1:08:37

what my now is what reference frame

1:08:39

I'm in because there's no observable effect

1:08:41

at the other spin There eventually will

1:08:43

be when they measure it But that's

1:08:46

true no matter when I do it

1:08:48

or even if I'm working in a

1:08:50

frame where they measure it before me

1:08:52

the answers are all exactly the same

1:08:54

So it's completely a matter of convention

1:08:57

how we choose to describe that branching

1:08:59

process Ken Wolf says, I

1:09:01

recall you saying that you were very

1:09:03

disappointed with the transformation of Twitter into

1:09:05

X. What I have heard is that

1:09:07

under X freedom of speech was protected

1:09:09

all but unconditionally, with protection from unsavility

1:09:11

or downright harassment being almost entirely sacrificed

1:09:13

as a result. Is that your experience

1:09:15

or was there something else at play?

1:09:17

Well I think there's lots going on.

1:09:19

I don't actually spend a lot of

1:09:21

time on X anymore, so I'm not

1:09:24

going to try out a whole bunch

1:09:26

of evidence for what it's like there,

1:09:28

but when I do go there, because

1:09:30

I do post the new podcast every

1:09:32

day, every week when it comes out,

1:09:34

it's just mess. It's just unpleasant. People

1:09:36

are mean, people are jerks to each

1:09:39

other, there's an enormous amount of spam

1:09:41

and bots, and that's just not rewarding

1:09:43

for me. There's a lot of people

1:09:46

who are still there, who are still

1:09:48

there. And I wish that they were

1:09:50

on Blue Sky where I am, but

1:09:52

that's okay. We don't need one single

1:09:55

social media site for everybody. That's fine.

1:09:57

On Blue Sky, I enjoy talking to

1:09:59

people. It reminds me of what

1:10:01

Twitter used to be. There's always

1:10:03

jerks, right? There's always people, but

1:10:06

it's easy to ban people and

1:10:08

easy to block them and move

1:10:10

on. Whereas on Twitter, that's almost

1:10:12

all I do is block people

1:10:14

and very rarely get constructive engagement.

1:10:17

So yeah. So I just moved

1:10:19

over to Blue Sky, and Blue

1:10:21

Sky for various reasons is more...

1:10:23

shielded from potential future capture by

1:10:25

bad actors. We'll see if that's

1:10:28

true or not, but for the

1:10:30

moment that's true right now. Connor

1:10:32

Schaffrin says, I hope this question

1:10:34

isn't too much of a bummer,

1:10:36

but I'm just curious, how bad

1:10:39

do you think things will get

1:10:41

in the next four years? Yeah,

1:10:43

I don't know. I've mentioned before

1:10:45

that my track record for making

1:10:48

political predictions used to be very

1:10:50

good, and then starting in 2016,

1:10:52

it became very bad. So recognizing

1:10:54

my own limitations, I'm not about

1:10:56

making predictions, because my predictions have

1:10:59

been pretty reliably wrong for the

1:11:01

last decade. It could get very

1:11:03

bad. I mean, I guess... It

1:11:05

is useful to understand, even if

1:11:07

you don't want to make a

1:11:10

prediction, the range of possible outcomes,

1:11:12

right? And that includes the best

1:11:14

possible and the worst possible outcomes.

1:11:16

In my own personal view, I

1:11:18

do not think that Donald Trump

1:11:21

is a good president. I think

1:11:23

that the things he is doing

1:11:25

to the United States and to

1:11:27

the world order and to the

1:11:29

progress of science and academia are

1:11:32

terrible and bad. If you think

1:11:34

differently, you will obviously have different

1:11:36

answers to this question, just so

1:11:38

you know that that's where I'm

1:11:41

coming from. So to me, the

1:11:43

best possible outcome is the courts

1:11:45

and the rest of the governmental

1:11:47

system. constrain the Trump administration from

1:11:49

giving into their worst impulses. They

1:11:52

try to preserve most scientific funding,

1:11:54

most freedom of the press and

1:11:56

universities and so forth, all of

1:11:58

which are under threat right now,

1:12:00

to try to mostly, you know,

1:12:03

somehow or another, we don't. do

1:12:05

too much damage to our international

1:12:07

standing and alliances. That would be

1:12:09

the best possible outcome and then

1:12:11

in four years people are tired

1:12:14

of this and they throw the

1:12:16

bums out. That seems like very

1:12:18

very rosy right now. I don't

1:12:20

think it's not going to be

1:12:22

business as usual. It's not it's

1:12:25

already not business as usual. Literally

1:12:27

as I'm recording this they just

1:12:29

announced that they've cut off stipends

1:12:31

to full bright scholars. Full bright

1:12:33

scholars are you know it's a...

1:12:36

for college students who want to

1:12:38

spend a year abroad, sometimes they're

1:12:40

in the United States, but they're

1:12:42

doing something, you know, for a

1:12:45

year, something interesting because they want

1:12:47

a competition and they show that

1:12:49

they're some of the best, most

1:12:51

promising scholars we have and this

1:12:53

is their... tiny salary that they

1:12:56

pay rent on and buy groceries

1:12:58

with and suddenly the government says,

1:13:00

oh, actually we changed our mind,

1:13:02

we're not going to give that

1:13:04

to you. And they might be

1:13:07

stuck in another country or something

1:13:09

like that. This is just unconscionably

1:13:11

bad behavior on the part of

1:13:13

our government. And it's a very

1:13:15

tiny thing compared to other things

1:13:18

that they're doing, but it shows

1:13:20

how little they care about real

1:13:22

human beings and some of the

1:13:24

best human beings that we have.

1:13:26

So the worst side, the worst

1:13:29

case scenario is... that the rest

1:13:31

of the governmental apparatus lets them

1:13:33

get along, go along with their

1:13:35

plans to break everything. We essentially

1:13:38

become pariahs on the international scene

1:13:40

because Canada and Australia and Europe

1:13:42

and Japan and so forth no

1:13:44

longer think of us as reliable

1:13:46

partners and they form their own

1:13:49

organizations that exclude us. The economy

1:13:51

completely collapses because we are... firing

1:13:53

in an enormous number of government

1:13:55

workers which leads to huge amounts

1:13:57

of unemployment and then we cut

1:14:00

taxes for very rich people while

1:14:02

not doing anything for non-rich people

1:14:04

and we cut Social Security and

1:14:06

Medicaid so that very poor people

1:14:08

are worse off and we put

1:14:11

on tariffs that lead to trade

1:14:13

wars so there's enormous inflation that

1:14:15

we're going to have to be

1:14:17

faced with. All of these... are

1:14:19

super plausible. They're happening, right? Like

1:14:22

we're not making this up right

1:14:24

now. And potentially worse than that

1:14:26

is that the political system will

1:14:28

be undermined. You know, there's this

1:14:31

long-standing pattern where people on that

1:14:33

side of things make a joke

1:14:35

about something terrible and then they

1:14:37

actually do it. And right now

1:14:39

they're joking about getting Trump a

1:14:42

third term in 2028. So let's

1:14:44

just to... put the fear of

1:14:46

God into you as it were.

1:14:48

Trump became president in 2017 and

1:14:50

he's become president again now in

1:14:53

2025 and he's the same person

1:14:55

that he was but the amount

1:14:57

of damage and the swiftness that

1:14:59

he's with which he's doing the

1:15:01

damage has been ramped up enormously

1:15:04

now. Back then, he was still

1:15:06

rained in by certain expectations, right?

1:15:08

By having certain ideas of like

1:15:10

having regular old people in the

1:15:12

cabinet or in government organizations. That's

1:15:15

completely gone. Now his cabinet is

1:15:17

full of Fox News hosts and

1:15:19

loyalists who don't know anything about

1:15:21

the agencies that they're leading, but

1:15:23

they're very very loyal to Donald

1:15:26

Trump. So there's an enormous ramping

1:15:28

up of the boldness and brazenness,

1:15:30

right? Okay, keep that in mind.

1:15:32

And then think about the fact

1:15:35

that in 2020, he lost an

1:15:37

election and refused to give up

1:15:39

power. He tried his best to

1:15:41

overturn the election results and eventually

1:15:43

led to January 6th, the riot

1:15:46

taking over the U.S. capital. So

1:15:48

the sensible thing to believe is

1:15:50

that 2024, sorry, five years, three

1:15:52

years from now. So 2028. you

1:15:54

can imagine will be as much

1:15:57

worse than 2020 was as 2025

1:15:59

right now is worse than 2017

1:16:01

was. so much more brazenness, so

1:16:03

much more relying on complete control

1:16:05

of all the leavers of government

1:16:08

and having loyalists in place, you

1:16:10

know, of all the things that

1:16:12

he's done, there's things that, you

1:16:14

know, are very obvious, like tariffs

1:16:16

and things like that, that people

1:16:19

get worked up about, but the

1:16:21

complete purges of independent agency leaders

1:16:23

and... people in inspector generals were

1:16:25

supposed to control corruption and things

1:16:28

like that those people are all

1:16:30

fired right so the number of

1:16:32

things he can get away with

1:16:34

now or in 2028 are enormously

1:16:36

larger than what he could get

1:16:39

away with in 2020. So that's

1:16:41

the worst case scenario. Like, usually

1:16:43

you talk to political scientists when

1:16:45

you get like crazy political ideas

1:16:47

in your head. You talk to

1:16:50

professional political scientists and they talk

1:16:52

you down. Like, oh no, it's

1:16:54

not that bad. If you right

1:16:56

now talk to professional political scientists,

1:16:58

they will tell you, 90% of

1:17:01

them will tell you, it can

1:17:03

be much worse than you think.

1:17:05

Like, whatever crazy dream you have

1:17:07

about democracy collapsing, the Constitution being

1:17:09

overthrown, no more actual elections with

1:17:12

undetermined outcomes ahead of time, all

1:17:14

that could go. That's the worst

1:17:16

case scenario. And I think we

1:17:18

need to take that seriously. People

1:17:21

are certainly talking about that. So

1:17:23

I hope it doesn't go that

1:17:25

bad. And, you know, this is

1:17:27

not even to get into... measles

1:17:29

outbreaks and other disease outbreaks and

1:17:32

universities collapsing. We already see universities

1:17:34

stopping letting new students in because

1:17:36

they can't afford it. New graduate

1:17:38

students at a lot of major

1:17:40

universities. The amount of bad that

1:17:43

it can be is really really

1:17:45

really bad so I think that

1:17:47

even though the range of possibilities

1:17:49

is still broad it's prudent to

1:17:51

plan for the worst and to

1:17:54

see what we can do to

1:17:56

prevent it. Justin Proctor says I

1:17:58

have to fly back to... East

1:18:00

to visit families. as someone who

1:18:02

does a lot of traveling for

1:18:05

work, do you feel as safe

1:18:07

flying now after the recent cuts

1:18:09

to the FAA and increase in

1:18:11

collisions and near collisions as before?

1:18:13

Well, no, certainly not as safe

1:18:16

as before, but still pretty darn

1:18:18

safe. I have no problems flying.

1:18:20

Flying until very recently was actually

1:18:22

super duper safe. You know, congratulations

1:18:25

to the FAA and to the

1:18:27

airline industry, etc. the idea of

1:18:29

taking a giant metal bird and

1:18:31

flinging it across the country seems

1:18:33

a little dicey but we don't

1:18:36

really have air crashes anymore because

1:18:38

we have built in an enormous

1:18:40

amount of safety is much safer

1:18:42

than driving a car or something

1:18:44

like that. But yes, one of

1:18:47

the very bad things that is

1:18:49

going on right now is cutting

1:18:51

people from the FAA. generally degrading

1:18:53

our ability to take care of

1:18:55

these things, shifting from well-established procedures

1:18:58

to letting Elon Musk's company be

1:19:00

in charge of things, it's not

1:19:02

as safe. And I think that

1:19:04

on the one hand, it's kind

1:19:06

of like climate change, right? Like,

1:19:09

you know the climate change is

1:19:11

going to increase the number of

1:19:13

unpredictable bad things happening. But when

1:19:15

you get a specific unpredictable bad

1:19:18

thing, you can't very easily just

1:19:20

say, oh, climate change did it,

1:19:22

right? You can say climate change

1:19:24

increase the chances of that happening,

1:19:26

but it's hard to get it

1:19:29

a very, very specific correlation there,

1:19:31

causal relationship there. Exactly the same

1:19:33

thing with the plane crashes that

1:19:35

we've seen and the close calls

1:19:37

on runways that we've seen. It's

1:19:40

been a little scary for some

1:19:42

people. Some people I know personally

1:19:44

have been in one of these

1:19:46

situations where the plane was landing

1:19:48

and had to actually stop landing

1:19:51

and zoom off because there was

1:19:53

by mistake another plane on the

1:19:55

runway just in the last couple

1:19:57

weeks. It's not, it's very very

1:19:59

difficult to directly associate these. these

1:20:02

events with the degradation of the

1:20:04

Federal Aviation Administration, but it is

1:20:06

not surprising that the rate of

1:20:08

those events has gone up. It's

1:20:10

still pretty low though. If we're

1:20:13

honest about it, it's still pretty

1:20:15

low right now. So I'm still

1:20:17

very willing to hop on a

1:20:19

plane. If it gets worse, then

1:20:22

that could conceivably change. Chris

1:20:24

says at some point a few

1:20:26

episodes back you made an often

1:20:28

comment about how the locality of

1:20:30

physical laws was an astonishing or

1:20:32

least unnecessary property and could be

1:20:34

viewed as a type of fine

1:20:37

tuning. I'm confused how locality can

1:20:39

be viewed as surprising. What would

1:20:41

a universe with non-local interactions look

1:20:43

like? If we'd evolve in such

1:20:45

a universe wouldn't we have a

1:20:47

different notion of distance such that

1:20:49

physical laws appear to respect our

1:20:51

idea of locality? What does distance

1:20:53

even mean if not the metric

1:20:56

that determines which things can interact?

1:20:58

Well, yeah, this is a very

1:21:00

good question. Sorry if I wasn't

1:21:02

clear about it before, but the

1:21:04

important part of this question is,

1:21:06

wouldn't you say, if we devolve

1:21:08

in a universe with non-local interactions,

1:21:10

wouldn't we just have a different

1:21:12

notion of locality, such that the

1:21:14

physical laws appear to respect those

1:21:17

different laws? So the implication there

1:21:19

is that given any set of

1:21:21

interactions, it must be possible to

1:21:23

organize them so that things interact

1:21:25

readily when they're near... nearby under

1:21:27

some definition of locality, but not

1:21:29

when they're far away under some

1:21:31

definition of locality. But the mathematical

1:21:33

fact is there's no reason that

1:21:36

that kind of organization must apply

1:21:38

to hypothetical laws of physics. If

1:21:40

you think about locality as we

1:21:42

have it in the real world,

1:21:44

given that the real world is

1:21:46

governed by quantum field theory to

1:21:48

a good approximation, we can sort

1:21:50

of chop up the world into

1:21:52

regions of space, you know, little...

1:21:54

tiny one cubic nanometer regions, okay,

1:21:57

like little boxes all over the

1:21:59

world. And according to the rules

1:22:01

of quantum field theory, Each little

1:22:03

box will interact directly under the

1:22:05

laws of physics with its nearest

1:22:07

neighbor boxes. Okay? It doesn't interact

1:22:09

directly with boxes far away at

1:22:11

all or even a little bit

1:22:13

away, even one centimeter away. It

1:22:16

only interacts indirectly via the boxes

1:22:18

in between. Okay? That's locality. That's

1:22:20

what locality is. And... I can easily

1:22:22

imagine different laws of physics in

1:22:24

which every box interacts directly and

1:22:26

strongly with every other box. That

1:22:29

would be entirely different than the

1:22:31

laws of physics that we have

1:22:33

right now, and there wouldn't necessarily

1:22:35

be any way to organize some

1:22:38

things such that it looked local.

1:22:40

This is even a proven result.

1:22:42

There's a paper called locality from

1:22:45

the spectrum. by Jordan-Kottler at all,

1:22:47

and they showed that a generic

1:22:49

set of laws of physics isn't

1:22:51

local at all. So it is sort

1:22:54

of a mathematical fact that in the

1:22:56

space of all possible laws, ones that

1:22:58

admit some notion of locality are a

1:23:00

tiny subset. Of course you're right that

1:23:02

the notion of locality isn't given to

1:23:05

you by God ahead of time. If

1:23:07

you do have some laws of physics

1:23:09

that allow for the existence of some

1:23:11

notion of locality, you can go and

1:23:13

find it, right? And then you can

1:23:15

do your best. But it's not at

1:23:18

all something that is necessary under

1:23:20

any possible laws of physics. Pete

1:23:22

Harlan says, I've heard you say

1:23:24

that effective field theories choose a

1:23:26

cutoff for maximum energies in order

1:23:28

not to blow up. Does anyone

1:23:31

think that there actually is a

1:23:33

theoretical limit on maximum energy? Yeah,

1:23:35

sure. Plenty of theories do that.

1:23:37

The sort of most straightforward way

1:23:39

to do that is to really

1:23:41

imagine that there is a smallest

1:23:43

distance, right? That there is some...

1:23:45

minimal length scale in nature. Because

1:23:48

you know that in whenever you

1:23:50

have a field theory, if your

1:23:52

wavelength is shorter, the energy of

1:23:54

the wave that you're thinking about

1:23:57

is higher. So short wavelengths correspond

1:23:59

to high... energies, so if there's

1:24:01

a shortest possible wavelength, there is a

1:24:03

maximum possible energy. And plenty of approaches

1:24:05

to quantum gravity try to do that.

1:24:07

Arguably loop quantum gravity tries to do

1:24:10

that. I think that that way of

1:24:12

doing quantum gravity is not right. It

1:24:14

takes locality too seriously, and it's not

1:24:16

going to be able to... to recover

1:24:18

holography black hole information conservation, things like

1:24:21

that. Now maybe those things aren't true.

1:24:23

So, okay, maybe that does actually work,

1:24:25

but I think that there's good reason

1:24:27

to think that those things are true.

1:24:29

So relying too heavily on locality, I

1:24:32

don't think is the way to go.

1:24:34

But in a very different way, string

1:24:36

theory has a kind of maximum energy

1:24:38

because there's the plank scale or the

1:24:40

string scale. There's a kind of duality,

1:24:43

and this is very vague because it

1:24:45

happens under some circumstances, but not others,

1:24:47

but just to give you an idea,

1:24:49

if you have string theory and there's

1:24:51

an extra dimension in the shape of

1:24:53

a circle, you can imagine wrapping a

1:24:56

string around the circle, right? And you

1:24:58

can imagine wrapping it once or twice

1:25:00

or three times or whatever, or you

1:25:02

can imagine taking a string and not

1:25:04

wrapping it around the circle, but letting

1:25:07

it travel. around the circle with a

1:25:09

certain momentum. It turns out that there's

1:25:11

a duality where you can trade one

1:25:13

for the other. Having a string moving

1:25:15

really fast is kind of like having

1:25:18

it wrapped around in some, there's some

1:25:20

map between those possibilities anyway. So basically,

1:25:22

this is, I'm not doing a very

1:25:24

good job of explaining this, but the

1:25:26

upshot is that if you try to

1:25:29

imagine scattering two strings at super duper

1:25:31

high energy, it turns into the equivalent

1:25:33

of a low energy. interaction in some

1:25:35

other perspective, some other point of view.

1:25:37

It's not quite a hard cutoff on

1:25:39

maximum energy because that probably wouldn't work

1:25:42

anyway, but it's sort of effectively that.

1:25:44

You know, you can't be too naive

1:25:46

about this because energy is not a

1:25:48

larynx invariant concept. The energy that a

1:25:50

particle has depends on the reference frame

1:25:53

in which you're measuring it. So you

1:25:55

have to be a little more subtle

1:25:57

about talking about a theoretical limit on

1:25:59

the... scattering the energy that is exchanged

1:26:01

from one particle to another in the

1:26:04

center of mass frame or something like

1:26:06

that. But yeah, so you can imagine

1:26:08

that. All of this is very far

1:26:10

away from how we use effective field

1:26:12

theories in the real world, because in

1:26:14

the real world, in the real world

1:26:17

in the sense of actual effective field

1:26:19

theories used to make predictions in nuclear

1:26:21

physics or something like that, the cutoffs

1:26:23

that we use are far, far below,

1:26:25

the plank scale or anything to do

1:26:28

with quantum gravity. The

1:26:30

great deceiver says, I haven't heard

1:26:32

you talk too much about the

1:26:34

large-scale structure of the universe, filaments

1:26:36

and super voids and all that

1:26:38

fun stuff. I was wondering if

1:26:40

the galactic clustering, in terms of

1:26:42

these immense filaments, comes out of

1:26:44

GR and its math or even

1:26:46

other theories models like inflation. Yeah,

1:26:48

it basically does, but of course

1:26:50

there are details that are going

1:26:52

to matter. The story is that

1:26:54

we have from inflation or from

1:26:56

some other... theory of initial conditions,

1:26:58

whatever that turns out to be,

1:27:00

the early universe is pretty smooth

1:27:02

but not exactly smooth. So there

1:27:04

are fluctuations with different amounts of

1:27:06

noticeability on different length scales, but

1:27:08

on every length scale there are

1:27:10

some kinds of fluctuations and they're

1:27:12

generally small in the early universe.

1:27:14

One part in 10 to the

1:27:16

5, so a hundred thousandth. So

1:27:18

if there's a region of space

1:27:20

that has a hundred thousand particles,

1:27:22

the region next to it might

1:27:24

have a hundred thousand and one

1:27:26

or 99, nine hundred nine parts.

1:27:28

right? That's the kind of fluctuation

1:27:30

we're talking about. And then over

1:27:32

time, as the universe expands and

1:27:34

dilutes, gravity pulls together matter from

1:27:36

the slightly over-dense regions by pulling

1:27:38

matter out of the slightly under-dense

1:27:40

regions, so the universe becomes more

1:27:43

contrasty and it becomes more lumpy

1:27:45

in some regions, emptier in other

1:27:47

regions. That's exactly what is predicted

1:27:49

by general relativity plus cosmology plus

1:27:51

initial conditions, and that's exactly what

1:27:53

we see. in the universe today.

1:27:55

Now the details happen because you

1:27:57

know you have dark matter and

1:27:59

you have ordinary matter and you

1:28:01

have magnetic fields and you have

1:28:03

light in the universe heating things

1:28:05

up and you have x-rays and

1:28:07

you have supernovae exploding and injecting

1:28:09

energy into the world around them.

1:28:11

So the whole thing is kind

1:28:13

of a mess. It's what is

1:28:15

called gastrophysics by theoretical physicists who

1:28:17

find it a little frustrating. But

1:28:19

having said all that we try

1:28:21

to do our best, we do

1:28:23

pencil and paper, we do simulations,

1:28:25

we collect as much data as

1:28:27

we can. There is right now

1:28:29

a slight mismatch. between what you

1:28:31

predict the clustering of galaxies to

1:28:33

be in the current universe from

1:28:35

what we see at early times,

1:28:37

from the microwave background, etc. You

1:28:39

make a prediction and it's not

1:28:41

quite right. This is called the

1:28:43

S... You may have heard of

1:28:45

the Hubble tension. We talked to

1:28:47

Adam Reese on the podcast some

1:28:49

time ago. If you infer the

1:28:51

current Hubble constant by looking at

1:28:53

the microwave background versus if you

1:28:55

measure the current Hubble constant directly,

1:28:57

you get slightly different answers with

1:28:59

a statistically significant difference. And the

1:29:01

same thing is true for the

1:29:03

amount of clustering. And it's called

1:29:05

S8 because that's just S sub

1:29:07

8 is the number that you

1:29:09

use to have the best constrained

1:29:11

characterization of how much clustering there

1:29:13

is in the current. universe. Maybe

1:29:15

it will go away when data

1:29:17

becomes better. Maybe it's signal that

1:29:19

something really interesting is going on.

1:29:21

That's why we do science because

1:29:23

we don't know ahead of time.

1:29:25

David Maxwell says, your chat with

1:29:27

Blaiseggari Yarkas added to my growing

1:29:29

impression that life at its most

1:29:31

basic is, if not inevitable, highly

1:29:33

likely in any environment that permits

1:29:35

enough complexity. How have your credences

1:29:37

changed over time? Is any Fermi

1:29:39

paradox bottleneck at abiogenesis, multi-cellularity, sentions,

1:29:41

or somewhere else? You know I

1:29:44

do think that Blaze's results increased

1:29:46

my credence that some kind of

1:29:48

life is easier to get started

1:29:50

or more likely to get started

1:29:52

than you might have thought. But

1:29:54

if you might have thought that

1:29:56

that number was incredibly small to

1:29:58

begin with and maybe it didn't

1:30:00

really do a lot to update

1:30:02

your credences. Again, I'm actually pretty

1:30:04

open-minded about this. I do tend

1:30:06

to think that there are not

1:30:08

hyper-advised technological civilizations here in our

1:30:10

Milky Way galaxy for the simple

1:30:12

reason that it would have been

1:30:14

too easy to notice them already

1:30:16

and we haven't. That could be

1:30:18

wrong. There could be some reason

1:30:20

why they're hiding from us. But

1:30:22

it's much easier for me to

1:30:24

imagine that they're just not there,

1:30:26

either because life is rare or

1:30:28

complex life is rare or something

1:30:30

like that. But I'm open to all

1:30:32

those possibilities. Maybe life is ubiquitous, but

1:30:34

it never becomes complex, or just typically

1:30:36

it takes a trillion years to become

1:30:38

complex and the universe hasn't been around

1:30:40

long enough for that to happen. Tim

1:30:43

Converse says, one possible explanation of the

1:30:45

Fermi paradox is that life or intelligent

1:30:48

life is super rare and extremely unlikely

1:30:50

to arise. Maybe I should have, maybe

1:30:52

I thought of grouping these together, but

1:30:54

just didn't pull it off. If this

1:30:56

were true and it turned out that

1:30:58

say we are the only exemplar in

1:31:00

10 to the 23 star systems, would

1:31:03

it undercut a scientific approach to the

1:31:05

origins of life that prefers likely explanations

1:31:07

of what we see? Rarity like that

1:31:09

would seem to open the door to

1:31:11

boltsman brain-like starting events. of RNA occurring

1:31:13

by chance. Could a journal reviewer of

1:31:16

the future say, if you're proposed mechanisms

1:31:18

for the origin of life or intelligent

1:31:20

life or correct, then we would expect

1:31:23

life or intelligent life to be common,

1:31:25

but it is not common so we

1:31:27

recommend rejection? Well... Yes, my general answer

1:31:29

to the question is yes. I'm made

1:31:32

uncomfortable by the invocation of boltsman brain-like

1:31:34

things because boltsman brains are truly truly

1:31:36

truly truly truly truly unlikely You know

1:31:38

there's you got to do the math

1:31:41

here and you got to say that

1:31:43

the actual boltsman brains are just very

1:31:45

very unlikely So I think what you

1:31:47

mean is in order for life to

1:31:49

start did there need to be something

1:31:52

that was simply a random fluctuation that

1:31:54

under ordinary circumstances we would think is

1:31:56

very unlikely but because the universe is

1:31:58

big enough it happened to have occurred. And

1:32:01

yeah, I think that's absolutely a

1:32:03

possible thing to ultimately come out

1:32:05

as true. That's why I don't

1:32:07

put a lot of evidentiary value

1:32:09

on the fact that we exist

1:32:12

here. There is truly an anthropic

1:32:14

consideration. We wouldn't be having this

1:32:16

conversation unless we existed. So the

1:32:18

fact that we exist does count

1:32:21

as evidence that life is possible.

1:32:23

but it really gives zero impact

1:32:25

on how likely life is. It

1:32:27

doesn't help us distinguish between the

1:32:30

hypothesis where life happens on 10%

1:32:32

of habitable worlds in the universe

1:32:34

and the hypothesis where life happens

1:32:36

on 10 to the minus 100

1:32:38

habitable worlds in the universe. They're

1:32:41

both completely consistent with us being

1:32:43

here, so there's no evidence one

1:32:45

way or the other. If we

1:32:47

improve our understanding of biochemistry and

1:32:50

geology and all those things, to

1:32:52

say that under conditions that typically

1:32:54

occur on a planet in our

1:32:56

observable universe, the chance of life

1:32:58

starting is 10 to the minus

1:33:01

100, then indeed any new theory

1:33:03

that implied that the chances were

1:33:05

much greater than that would be...

1:33:07

counter-indicated would be ruled out if

1:33:10

you want to put it that

1:33:12

way, but I don't think it's

1:33:14

anything special about life or Fermi

1:33:16

paradox or anything like that here

1:33:18

It's just saying that if your

1:33:21

theory is making predictions that are

1:33:23

completely violated by the world in

1:33:25

which we live Your theory is

1:33:27

not going to get a lot

1:33:30

of traction Anonymous says, have

1:33:32

you ever had a million dollar

1:33:34

year? I just want to know

1:33:36

that my boy Sean is securing

1:33:38

the bag. I have not been

1:33:40

securing the bag that well. Look,

1:33:42

I'm doing fine. I don't, you

1:33:45

know, we don't go into personal

1:33:47

details here, but I've certainly never

1:33:49

complained compared to many people in

1:33:51

the world about how much money

1:33:53

I'm making or anything like that,

1:33:55

but a million dollars in a

1:33:57

year is not something that I

1:33:59

have ever gotten or I've ever

1:34:01

threatened to get or ever expected

1:34:03

to get in my life. But

1:34:06

that's okay, you know, you can

1:34:08

do pretty well with less than

1:34:10

a million dollars a year. Roland

1:34:12

Weber says, how do we know

1:34:14

that gravity was strong near the

1:34:16

Big Bang? Is that a prediction

1:34:18

from running models of the universe

1:34:20

backwards in time and hitting singularities

1:34:22

or do we have direct evidence?

1:34:24

Is that even a valid distinction

1:34:27

or does everything we can observe

1:34:29

today have to be processed through

1:34:31

models and projected back in time

1:34:33

to tell us about the state

1:34:35

of the universe near the Big

1:34:37

Bang? Well, to say that gravity

1:34:39

is strong, there's two different... possible

1:34:41

construals there. One is that as

1:34:43

a force between two particles, gravity

1:34:45

was stronger near the Big Bang.

1:34:47

And that's false. At least we

1:34:50

have no evidence of that. We

1:34:52

have very good evidence that the

1:34:54

strength of gravity in terms of

1:34:56

Newton's constant was more or less

1:34:58

the same, to within 10% of

1:35:00

its current value a minute after

1:35:02

the Big Bang, during Big Bang

1:35:04

nucleosynthesis. When people, including myself, say

1:35:06

that gravity was strong near the

1:35:08

Big Bang, what you mean is

1:35:11

not... on a particle-by-particle basis, you

1:35:13

just mean that there's a lot

1:35:15

more density of particles. So gravity

1:35:17

is stronger on Jupiter than on

1:35:19

Earth, because Jupiter is more massive,

1:35:21

not because Newton's constant is different.

1:35:23

In the early universe, we have

1:35:25

super-duper practically irrefutable evidence that the

1:35:27

density of matter was very, very

1:35:29

high. So in that sense, gravity

1:35:32

was just strong. You don't need

1:35:34

anything fancy. To say that that's

1:35:36

true, you just need to understand

1:35:38

the fact that the universe is

1:35:40

expanding plus ordinary general relativity. Dario

1:35:42

Kubler says for an isotropic photon,

1:35:44

isotropic photon source, the received signal

1:35:46

intensity at a given distance is

1:35:48

modulated by the mass distribution along

1:35:50

the optical path. This implies that

1:35:53

the perceived brightness of distance sources,

1:35:55

particularly a cosmological distances, may be

1:35:57

influenced by mass distributions beyond our

1:35:59

observable horizon, potentially impacting brightness estimations.

1:36:01

Could this phenomenon introduce systematic errors

1:36:03

in the standardized luminosity of type

1:36:05

1A supernov? thereby affecting cosmological distance

1:36:07

measurements and ultimately our understanding of

1:36:09

the universe is accelerated expansion. In

1:36:11

principle, yes, this is a very

1:36:13

well-known phenomenon. This is gravitational lensing.

1:36:16

There are different regimes in which

1:36:18

gravitational lensing can happen, so there's

1:36:20

weak lensing and strong lensing. Strong

1:36:22

lensing is... roughly speaking, when you

1:36:24

have a gravitating source that is

1:36:26

so strong that it creates multiple

1:36:28

images of a source in the

1:36:30

background. And when you have strong

1:36:32

lensing, the total luminosity that you're

1:36:34

measuring can be dramatically changed by

1:36:37

that event. But strong lensing is

1:36:39

relatively rare. It happens, but astronomers

1:36:41

are very happy when they see

1:36:43

it. It leads to beautiful pictures.

1:36:45

You can just Google strong gravitational

1:36:47

lens, get all these multiple images,

1:36:49

etc. But it's the rarer thing.

1:36:51

The more interesting thing is weak

1:36:53

gravitational lensing, which as you might

1:36:55

expect is weaker, but also more

1:36:58

ubiquitous. It's everywhere. So plenty of

1:37:00

people have done research on asking

1:37:02

the question, what is the effect

1:37:04

of weak gravitational lensing on the

1:37:06

inferred brightness of distant supernovae? The

1:37:08

answer is not that much. It's

1:37:10

weak, right? And you know, overall

1:37:12

balances out. Sometimes you increase the

1:37:14

brightness a little bit, sometimes you

1:37:16

decrease it, but there's very very

1:37:19

strong evidence that for whatever reasons,

1:37:21

once you apply a certain correction

1:37:23

relative to the time it takes

1:37:25

the supernova to increase and then

1:37:27

decrease in brightness, Type 1A supernovae

1:37:29

at fixed red shifts all have

1:37:31

the same brightness. So there can't

1:37:33

be a huge effect of lensing

1:37:35

because sometimes it would increase the

1:37:37

brightness, sometimes it would decrease it,

1:37:39

and that simply is not seen

1:37:42

in the data. And that's consistent

1:37:44

with the theoretical predictions, so I

1:37:46

think that that is pretty much

1:37:48

under control. Reese Johns says, could

1:37:50

Laplace's demon know next? No. I

1:37:52

think maybe this isn't always clear.

1:37:54

Maybe I don't even say it

1:37:56

because it's just so clear to

1:37:58

me that I don't bother. Laplace's

1:38:00

demon doesn't live in the universe.

1:38:03

Even if you imagine, it's just

1:38:05

a thought experiment, it's not true,

1:38:07

but if you imagine the thought

1:38:09

experiment where there is a demon

1:38:11

with a vast intelligence who knows

1:38:13

everything in the universe well enough

1:38:15

to predict what will happen next,

1:38:17

You can't imagine that that demon

1:38:19

is part of the universe, a

1:38:21

subset of the universe, right? Because

1:38:24

it can't have enough storage capacity

1:38:26

in its brain to keep track

1:38:28

of literally everything defining itself plus

1:38:30

everything defining the rest of the world.

1:38:32

So in any construal of what Laplace's

1:38:34

demon is, it has to be outside.

1:38:36

of the universe, it can't be part

1:38:38

of it. So in particular when we

1:38:40

say Laplace's demon knows what's going to

1:38:42

happen next in the universe, that does

1:38:44

not include Laplace's demon itself. Laplace's demon

1:38:46

can't even interact with the universe because

1:38:48

if it could, it would have to

1:38:50

be considered to be part of it

1:38:52

and it wouldn't be able to make

1:38:54

those predictions. EMB asks a

1:38:56

stupid procedural question. Is it okay when you

1:38:58

have these AMAs to re-ask a question that

1:39:01

you didn't pick for a previous EMA? This

1:39:03

is a bit thorny because there's no way

1:39:05

to know if you didn't pick it previously

1:39:07

for time or just because it wasn't a

1:39:10

good question. This of course excludes priority questions.

1:39:12

So I mentioned this in the intro, and

1:39:14

so I hope it's clear. Of course it's

1:39:16

okay. You're welcome to ask whatever questions you

1:39:18

want. Go ahead. And I might even pick

1:39:21

them. But you're right. I do not go

1:39:23

through all the questions that are

1:39:25

not picked and provide explanations as

1:39:28

to why I didn't do it.

1:39:30

But hopefully, you know, through my

1:39:32

explicit instructions, plus abstracting from what

1:39:35

kinds of questions I do pick,

1:39:37

you can kind of get a

1:39:39

feeling for what kind of

1:39:41

questions get answered. You know, it is

1:39:44

a fine line. Like, I don't... answer

1:39:46

too many super personal questions, although I

1:39:48

did the how much money I make

1:39:50

one just as a joke a little

1:39:52

bit there, even though I told the

1:39:54

truth, but it was a very vague

1:39:56

truth. I don't, you know, do a

1:39:58

lot of homeworky type questions. Imagine this

1:40:00

spaceship is going at 0.99% of the

1:40:03

speed of light? Like yeah, no, that's

1:40:05

that's just not interesting to me. Something

1:40:07

that you can get more easily by,

1:40:09

you know, asking chat GPT, I think

1:40:11

is kind of a waste of my

1:40:14

time. I don't. It's a weird quirk

1:40:16

of me and I don't want to

1:40:18

blame anybody else, but I don't love

1:40:20

questions that like ask me about my

1:40:22

favorite X or like the one person

1:40:25

I wanted to meet in history or

1:40:27

you know things like that. Like I

1:40:29

just don't think that way. That's not

1:40:31

how I how I roll. And also

1:40:33

I don't like questions that I think

1:40:36

I've asked been answered many times before

1:40:38

or questions that are too long or

1:40:40

questions that are secretly trying to make

1:40:42

an argument rather than ask a question.

1:40:44

Imagine that you're having a conversation with

1:40:47

me and you want my opinion about

1:40:49

something, or you want a little bit

1:40:51

of clarification that goes beyond what you

1:40:53

could easily find on the internet. Those

1:40:55

are the questions that I think it's

1:40:58

most likely for me to pick. Short

1:41:00

versions of those. Dim Gienizos says, occasionally

1:41:02

an academic discipline originates from a non-rigorous

1:41:04

foundation. For example, Newton's study of derivatives

1:41:06

and infinitesimals were not on a rigorous

1:41:09

mathematical footing for over 100 years until

1:41:11

the advent of real analysis, which we've

1:41:13

already mentioned earlier, in the 1800s. However,

1:41:15

calculus was incredibly useful in the interim.

1:41:18

What are the most promising areas of

1:41:20

science that you believe are worth entertaining

1:41:22

even though they lack agreement with experiment?

1:41:24

Well, what just happened there in the

1:41:26

last sentence of this question? So, the

1:41:29

first part was about a rigorous mathematical

1:41:31

foundation. Then the question at the end

1:41:33

was about agreement with experiment. These are

1:41:35

two very, very different things. I think

1:41:37

that if you were to actually leaf

1:41:40

through almost all of physics and chemistry

1:41:42

and biology, which are all in their

1:41:44

ways highly mathematical, Almost none of them

1:41:46

would reach the level of rigorous mathematical

1:41:48

justification that we have in the best

1:41:51

pure math research. Scientists just like to

1:41:53

get to the answer, right? They like

1:41:55

to zoom ahead without rigorous mathematical justification.

1:41:57

Lacking agreement with experiment is an entirely

1:41:59

different thing. I'm not going to give

1:42:02

you a very good answer to this

1:42:04

because the phrase lack agreement with experiment

1:42:06

is a little bit too loose. Does

1:42:08

that mean... disagreeing with experiment? Does it

1:42:10

mean not yet making testable predictions that

1:42:13

we've been able to measure? Does it

1:42:15

mean just being too vague to even

1:42:17

talk about experiment? Does it mean having

1:42:19

made predictions that we don't have the

1:42:21

technology to test yet? All these are

1:42:24

possible and all these are going to

1:42:26

be very different. But you know, I

1:42:28

think that science is a messy thing

1:42:30

and we make progress by inventing theories.

1:42:32

gradually and trying to confront them with

1:42:35

experiment as best we can. I think

1:42:37

that sometimes people, both inside and outside,

1:42:39

but especially outside of professional science, fetishize,

1:42:41

like unless you can tomorrow do an

1:42:44

experiment that rules out or proves your

1:42:46

theory, it's not worth entertaining. That's just

1:42:48

entirely unrealistic about how science actually works.

1:42:50

Fell Trash says, do you see any

1:42:52

silver lining in the end of the

1:42:55

USFG as the leader of the free

1:42:57

world? For example, I'm not sure what

1:42:59

USFG means. I'm going to take it

1:43:01

to be something about the United States.

1:43:03

For example, the veil being lifted on

1:43:06

US exceptionalism. Clearly the matter in which

1:43:08

it's being done is unlawful and moral

1:43:10

and dumb, but what good might come

1:43:12

of it. I think it's stretching to

1:43:14

think much good might come of it.

1:43:17

You know, I never believed in U.S.

1:43:19

exceptionalism. I don't think many people believe

1:43:21

in U.S. exceptionalism. That's the kind of

1:43:23

thing that a politician might refer to

1:43:25

just as sort of a speech to

1:43:28

get hearts racing and, you know, make

1:43:30

people feel good about themselves. I don't

1:43:32

think that the world has really bought

1:43:34

into much of an idea of U.S.

1:43:36

exceptionalism. You know, correct me if I'm

1:43:39

wrong, but that's been my impression. I

1:43:41

think that the United States has for

1:43:43

a certain number of decades served as

1:43:45

a something like a good example for

1:43:47

a lot of countries in the sense

1:43:50

that we've had democratic elections, that we've

1:43:52

been relatively materially prosperous, that we've tried

1:43:54

to do some good things in the

1:43:56

world, with all the footnotes that say

1:43:58

we've done some terrible things in the

1:44:01

world, that our democracy has been very

1:44:03

flawed in various ways, that our prosperity

1:44:05

has not been shared universally. That's fine,

1:44:07

but I do think that as an

1:44:09

example to live up to, I would

1:44:12

like the United States to be doing

1:44:14

the best it possibly can. and the

1:44:16

fact that the United States starts doing

1:44:18

badly, I don't think that makes the

1:44:21

world a better place. I do think

1:44:23

that... Maybe it's good if other countries

1:44:25

in the world don't rely on leadership

1:44:27

from one particular country. A multipolar world

1:44:29

would be good in that case. I

1:44:32

have no special desire for the United

1:44:34

States to be the boss of the

1:44:36

world, certainly. That's the last thing I

1:44:38

want. But I don't want someone else

1:44:40

to be the boss of the world

1:44:43

either. And you might say I want

1:44:45

a multipolar world, but it's hard to

1:44:47

pull off because various countries are going

1:44:49

to want to be the boss, right?

1:44:51

So... I don't know. I think that

1:44:54

I would like every country to succeed

1:44:56

and be free and democratic and prosperous,

1:44:58

and that includes the United States as

1:45:00

well as everybody else. Eric says, looking

1:45:02

at websites like scale of universe.com, I

1:45:05

notice that the interesting bits like life

1:45:07

are roughly in the middle of the

1:45:09

biggest and smallest things. Is there some

1:45:11

general principle from complexity theory that would

1:45:13

make that so? I think roughly there

1:45:16

is, for one thing, you had to

1:45:18

be very careful about this claim that

1:45:20

the interesting bits are in the middle.

1:45:22

It's a very, very rough idea, right?

1:45:24

Because the smallest things, what do you

1:45:27

mean by the smallest things? Do you

1:45:29

mean an atom? Do you mean a

1:45:31

proton? Do you mean the plank scale?

1:45:33

Those are very, very different in size.

1:45:35

So it is only a very, very

1:45:38

rough guideline. But given that, I think

1:45:40

there are good reasons to expect that

1:45:42

the most small things

1:45:44

just can't be that

1:45:46

complex. There's not

1:45:49

enough room for them

1:45:51

to be complex.

1:45:53

I talk about this

1:45:55

actually in Quanta

1:45:58

and Fields in the

1:46:00

most recent book

1:46:02

because of the feature

1:46:04

of field theory

1:46:06

that we already have

1:46:09

mentioned. When you

1:46:11

try to make something

1:46:13

small in quantum

1:46:15

mechanics or field theory,

1:46:17

you increase its

1:46:20

energy. So if you

1:46:22

try to do interesting things inside an

1:46:24

atom or a proton or whatever,

1:46:26

you can only do that by adding

1:46:28

more energy than is already there.

1:46:30

And that generally means that the thing

1:46:32

just decays right away into something

1:46:34

of lower energy. So if you're very

1:46:36

small, and this is even true

1:46:38

in a sort of less dramatic sense

1:46:40

for medium small things like molecules

1:46:42

or whatever, there just isn't that much

1:46:44

room to have things arranged in

1:46:47

interesting ways to have too many moving

1:46:49

parts to be complex. On the

1:46:51

largest scales, there's just simply a matter of

1:46:53

time as we were talking about before

1:46:55

for countries being conscious. The

1:46:58

universe that we

1:47:00

observe is billions of light years

1:47:02

across. That means it takes billions

1:47:04

of years for a signal to

1:47:06

travel from one side to the

1:47:08

other. There is not enough time

1:47:10

for many interesting interactions to have

1:47:13

happened on very large scale things

1:47:15

that would let you settle into

1:47:17

some interestingly complex configuration. There's an

1:47:19

analogous thing you can say about

1:47:21

low entropy and high entropy in

1:47:23

very, very low entropy situations. You

1:47:25

can't be complex because there's not

1:47:28

enough room and not enough states that

1:47:30

look that way. In very,

1:47:32

very high entropy situations you are in

1:47:34

equilibrium and everything is smooth and

1:47:36

boring. So I think that it's not

1:47:38

a rigorous theorem, but there are

1:47:41

general reasons to expect that complexity falls

1:47:43

in the middle of these various

1:47:45

extremes. Jameson

1:47:47

says is there any reason at all to

1:47:49

find solace in the block universe? For example,

1:47:51

should it be comforting? Should it be a

1:47:53

comforting thought when dealing with the death of

1:47:55

a loved one that in some other equally

1:47:57

real past moment of time circumstances are different? I

1:48:01

don't see why it would be

1:48:03

comforting. No, I don't think that

1:48:05

that's a source of solace. I

1:48:07

mean, compared to presentism, I guess,

1:48:09

I don't think that the block

1:48:11

universe is more... comforting in any

1:48:13

way. There's a famous quote by

1:48:15

Einstein that disagrees with me here

1:48:17

saying that you know time is

1:48:19

just an illusion all moments are

1:48:21

equally real. He was trying to

1:48:23

console the I think the widow

1:48:25

or Marshall Grossman or something like

1:48:27

that. But it's a bit of

1:48:30

you know rhetoric. I don't think

1:48:32

it's very rigorous. The fact that

1:48:34

I treat moments of the past

1:48:36

and future as ontologically real has

1:48:38

no impact on how I think

1:48:40

about a loved one who has

1:48:42

just passed away. Like they were

1:48:44

always in the past, they were

1:48:46

always in the future, that doesn't

1:48:48

provide me with much solace. What

1:48:50

matters to me is what's going

1:48:52

on now. I think it's better

1:48:54

to accept what is happening in

1:48:56

the present and what might happen

1:48:58

in the future than to take

1:49:00

some weird metaphysical solace in a

1:49:03

view, a perspective on which... elements

1:49:05

of time, which moments of time

1:49:07

count as truly real. Roe says

1:49:09

Microsoft claims to have invented a

1:49:11

new state of matter, the world's

1:49:13

first topo conductor. This revolutionary class

1:49:15

materials enables us to create topological

1:49:17

superconductivity, a new state of matter

1:49:19

that previously existed only in theory.

1:49:21

Is this a real thing or

1:49:23

is it marketing BS? I'm not

1:49:25

an expert on the particular technology

1:49:27

here. The experts that I know

1:49:29

are very widely dismissive of this.

1:49:31

And it's not that hard to

1:49:33

see why they are dismissive of

1:49:36

it. A paper was written by

1:49:38

the Microsoft research team that seems

1:49:40

to be, as far as I

1:49:42

can tell, pretty careful. You know,

1:49:44

they tried to make this topological

1:49:46

configuration that might help us build

1:49:48

tolerant cubits someday down the road.

1:49:50

But they said very clearly they're

1:49:52

not sure whether they succeeded in

1:49:54

making it. And then there was

1:49:56

a press release that entirely, as

1:49:58

far as I can tell, misrepresented

1:50:00

what was the paper that way

1:50:02

overclaimed what actually happened. So in

1:50:04

between the scientists doing the work

1:50:06

and the general public hearing about

1:50:09

it, there was science that was

1:50:11

done, but a certain amount of

1:50:13

marketing BS absolutely, apparently did inject

1:50:15

itself along the way. Reese Johns says,

1:50:17

doesn't it get boring teaching students

1:50:19

the same material every year? Well,

1:50:21

I haven't been teaching students the

1:50:23

same material every year for quite

1:50:25

a long time. In my three

1:50:27

years at Hopkins so far, I've

1:50:29

taught six different courses. Never one

1:50:32

repeating. Next year, I'm hoping to

1:50:34

teach what is a repeat of

1:50:36

my philosophy of physics course from

1:50:38

a couple years ago, but... No, even

1:50:40

if I were teaching it the same material

1:50:42

every year, I don't think it really gets

1:50:44

boring. For one thing, it's a year apart.

1:50:47

A year is a pretty long period of

1:50:49

time. If another thing, you can continue to

1:50:51

get better at it. You can kind of

1:50:53

think about how to teach the material, what

1:50:55

things to include. For a third thing, the

1:50:57

students are different, right? So it's a different

1:51:00

slight experience every time. So of all the

1:51:02

things to fret about being an academic or

1:51:04

professor, teaching the same thing over and over

1:51:06

and over and over again. It's not high

1:51:08

on my list. Peter Newell says, in Newtonian

1:51:10

mechanics, I would argue that the Earth

1:51:12

orbits the Sun and not the other

1:51:15

way around, because you can construct an

1:51:17

inertial reference frame where the Earth basically

1:51:19

goes around the Sun at least on

1:51:21

the timescale of years. However, in GR,

1:51:24

the concept of a global inertial reference

1:51:26

frame doesn't really exist, so the argument

1:51:28

might break down. Here's my question. Can

1:51:30

I make an argument valid in GR

1:51:32

framework simply by asserting that Newtonian gravity

1:51:35

is the regime of GR that adequately

1:51:37

describes the situation? Sure, you can make

1:51:39

an argument, you're allowed to make

1:51:41

such an argument. I mean, basically,

1:51:43

I think that you have the

1:51:46

right facts of what the theories

1:51:48

are saying, but you're sort of,

1:51:50

as I've seen other people do,

1:51:52

clinging to the idea that, but

1:51:54

come on, really, we know that

1:51:57

the earth goes around the sun. And

1:51:59

the fact... that if you're careful

1:52:01

about what the words goes around

1:52:03

means and you're careful about how

1:52:05

we think about these things in

1:52:07

general relativity, that is not an

1:52:10

objectively true statement. There are reference

1:52:12

frames in which we describe the

1:52:14

earth as going around the sun,

1:52:16

reference frames in which we describe

1:52:18

the sun as going around the

1:52:20

earth. There is also, as you

1:52:22

point out, a Newtonian limit to

1:52:25

general relativity, and that Newtonian limit

1:52:27

is a very good approximation in

1:52:29

the solar system. And there you

1:52:31

have absolute space and time in

1:52:33

that Newtonian regime. And you can

1:52:35

make more objective statements like the

1:52:37

center of mass of the earth -moon

1:52:40

system, the barycenter around which things

1:52:42

orbit is deep within the sun,

1:52:44

not deep within the earth. So

1:52:46

there is a sense in which

1:52:48

it is objectively true, in that

1:52:50

case, that the earth goes around

1:52:52

the sun. So you can concatenate

1:52:55

these things to go from general

1:52:57

relativity to Newtonian gravity to the

1:52:59

sense in which the earth goes

1:53:01

around the sun. Or you can

1:53:03

just face up to the fact

1:53:05

that we understand the universe better

1:53:07

and the concept of one thing

1:53:10

in space objectively going around the

1:53:12

other is not perfectly well defined.

1:53:14

It's an approximation that helps us

1:53:16

under certain circumstances. So by all

1:53:18

means, refer to it when we

1:53:20

all agree on what's going on.

1:53:22

But I don't get the, there's

1:53:25

an impulse, I'm not necessarily saying

1:53:27

you have it, but there's an

1:53:29

impulse in certain circles to sort

1:53:31

of really insist that there has

1:53:33

to be some objective sense in

1:53:35

which this is absolutely true. And

1:53:37

I think that that's not quite

1:53:40

the right way to think about

1:53:42

it. Rad Antonov says, In Quentin

1:53:44

Fields, the approach in the early

1:53:46

chapters is predominantly wave function focused

1:53:48

as opposed to matrix mechanics, commutator

1:53:50

algebra, and operators as generators of

1:53:52

translations or rotations. That you adopt

1:53:55

this approach for pedagogical reasons or

1:53:57

is it a reflection of a

1:53:59

philosophical view? It's not a reflection

1:54:01

of a philosophical view. It is

1:54:03

the way that I think is

1:54:05

easier to think about these things

1:54:07

in a wide variety of circumstances.

1:54:10

For those of you who don't

1:54:12

know, you know, in quantum mechanics, going back to Heisenberg versus

1:54:14

Schrodinger, there's kind of two different ways. In fact, there's an infinite

1:54:16

number of ways, but there's two major ways to encapsulate the dynamics

1:54:18

of the system. One is to say I have a quantum state,

1:54:20

that's usually the way you hear me talking, and it obeys the

1:54:22

Schrodinger equation. So the quantum state evolves with time. And then I

1:54:25

can do things, as you know, observationally. to the quantum state. I

1:54:27

can measure a position, measure a momentum, or whatever. And I would

1:54:29

say that, oh, if a particle's moving, if there's

1:54:31

like a little wave packet that is

1:54:33

localized, then it has momentum in some

1:54:35

direction, then if I measure it at

1:54:38

this point versus another point, it will

1:54:40

have moved to left or whatever. but

1:54:42

there's an equally good way of doing

1:54:44

it, which is the Heisenberg kind of

1:54:46

way of doing it, where you don't

1:54:49

have states that evolve with time. You

1:54:51

just have the quantum state period, but

1:54:53

you have the operators, the observables, evolve

1:54:55

with time. So you just, instead of

1:54:58

saying... The observable position is a fact.

1:55:00

It does the same thing to any

1:55:02

quantum state, but the quantum states change.

1:55:04

You're saying the quantum state is a

1:55:07

fact. It is the same quantum state

1:55:09

for everything, but the observables change. It's

1:55:11

completely equivalent, and there's literally a mathematical

1:55:14

procedure to go back and forth. But

1:55:16

I do think that especially because of

1:55:18

how we think about classical mechanics, for

1:55:21

me and for many people, thinking about

1:55:23

the Schrodinger evolving quantum state way of

1:55:25

talking about things is just more natural.

1:55:28

So that's why I decided to talk

1:55:30

about it that way. I'm not trying

1:55:32

in these books which are meant for

1:55:34

a popular audience to talk about every

1:55:36

possible way of doing quantum mechanics. Hussein

1:55:39

asks a priority question. Given the political

1:55:41

climate that we live in, you've made

1:55:43

it a point to dedicate time on

1:55:45

your podcast to uplift and emphasize the

1:55:47

importance of having an objective mainstream media

1:55:49

for maintaining a healthy democratic society. However,

1:55:51

over the past 16 months, my faith

1:55:53

in the mainstream media has been significantly

1:55:56

eroded. This has been largely due to

1:55:58

the media's coverage of the war. slash

1:56:00

genocide in Gaza. I understand that this

1:56:02

is only one war in one place,

1:56:04

that the media is covering, however I

1:56:07

cannot help it separate the bias that

1:56:09

I perceive they've engaged in in their

1:56:11

coverage on Gaza and apply it to

1:56:14

the rest of their coverage. In short,

1:56:16

I can't get myself to take the

1:56:18

mainstream media as a source of authority

1:56:21

anymore. Am I wrong in how I've

1:56:23

reacted to the media's coverage? Well, you're

1:56:25

not completely wrong. There's something there, but

1:56:27

I don't. ever think it should be

1:56:30

thought of as a source of authority,

1:56:32

right? I don't, I think that was,

1:56:34

if the hope was that there's some

1:56:37

media outlet that is simply authoritative and

1:56:39

always correct and we can trust it

1:56:41

a hundred percent, I was just never

1:56:44

tended to think that way. So nothing

1:56:46

has changed for me. The things that

1:56:48

we think of as mainstream media outlets,

1:56:51

absolutely have their blind spots and their

1:56:53

biases. I don't think it's very plausible

1:56:55

to deny that that's true. But that's...

1:56:57

beside the point of whether or not

1:57:00

we would like to have an objective

1:57:02

mainstream media. I was not making the

1:57:04

argument ever that the mainstream media that

1:57:07

we have now is ideal or even

1:57:09

all that great. I was just saying

1:57:11

that it would be better to live

1:57:14

in a world where there were trustworthy,

1:57:16

objective mainstream media outlets that we could

1:57:18

have as reliable sources of facts to

1:57:21

the extent that is possible. That is

1:57:23

not something that exists. is an ideal

1:57:25

to which I think it is worth

1:57:27

moving. And therefore, the thing to do

1:57:30

is not to give up on the

1:57:32

idea of objective mainstream media. It is

1:57:34

to try to make the mainstream media

1:57:37

better, more objective, and more reliable. The

1:57:39

other thing, of course, is that if

1:57:41

you say, well, I don't like the

1:57:44

mainstream media, What is the alternative to

1:57:46

the mainstream media? And the answer is

1:57:48

almost always things that are much more

1:57:51

biased in one way or the other.

1:57:53

You might like their biases better. And

1:57:55

sometimes that's fine for certain specialized things,

1:57:57

for certain sort of opinion-based things, or

1:58:00

activism-based things. it makes perfect sense to

1:58:02

not worry about being objective and to

1:58:04

get your information from someone who aligns

1:58:07

with your pre-existing points of view on

1:58:09

things. But that's again a separate thing

1:58:11

and you better admit that if you're

1:58:14

getting all of your information from bias

1:58:16

sources intentionally, then you're going to have

1:58:18

to correct for those biases at some

1:58:20

point or another. Leon Enriquez says in

1:58:23

episode 304 James Evans mentions abductive discoveries

1:58:25

that come from the surprise and experimental

1:58:27

results that that experimental results can produce

1:58:30

on a scientist. He are used based

1:58:32

on C. as perse's ideas. By the

1:58:34

way, if you ever see C.S. perse's

1:58:37

name spelled, it looks like pierce, but

1:58:39

it's pronounced perse, I promise you. Based

1:58:41

on C.S. purses' ideas, then maybe the

1:58:44

resources for those discoveries can come from

1:58:46

other fields different from where the surprise

1:58:48

happens. In my musicology field, I find

1:58:50

a lot of truth to this. Is

1:58:53

this something you've tried successfully in your

1:58:55

field of theoretical physics? If so, what,

1:58:57

and if not why? Well, yeah, I

1:59:00

mean, you see the fruits of that

1:59:02

attempt in the podcast that you are

1:59:04

listening to. Part of my motivation for

1:59:07

doing Mindscape is to be myself personally

1:59:09

exposed to a whole bunch of ideas

1:59:11

from a whole bunch of different corners,

1:59:14

different fields, different perspectives, and so forth.

1:59:16

I could make a lot more money

1:59:18

just doing a physics podcast, you know,

1:59:20

physics news of the day or, you

1:59:23

know, spicy opinions about physics things. That

1:59:25

would be more popular. There's no question

1:59:27

about that, but it would be much

1:59:30

less useful for me. So I want

1:59:32

to hear and learn from all these

1:59:34

different fields. Obviously, I'm literally a member

1:59:37

of a philosophy department, so that is

1:59:39

a different field that has helped me

1:59:41

out a lot, but in different ways

1:59:43

there's other fields that help a lot

1:59:46

also. So I think that it's not...

1:59:48

To me, that's not a surprising thing.

1:59:50

You know, the overall piece of wisdom

1:59:53

is that the space of ideas and

1:59:55

the space of possibilities are very, very

1:59:57

large and there's no possible way for

2:00:00

a human being to think of every

2:00:02

possibility. idea or to contemplate every possible

2:00:04

possibility. We need to choose strategies for

2:00:07

working our way through these ultimately large

2:00:09

spaces, and one of them is to

2:00:11

keep being jostled by ideas from outside

2:00:13

our comfort zone. I think that's a

2:00:16

good thing to do. Nicholas Katsantonus says,

2:00:18

how can you explain and if possible

2:00:20

conceptualize how the exchange of particles leads

2:00:23

to attractive forces? Two negatively charged electrons

2:00:25

exchanging electrons exchanging photons analogized by imagining

2:00:27

two people, one throwing a ball at

2:00:30

one another and being pushed in the

2:00:32

opposite direction by throwing, but also catching.

2:00:34

That real-world example, in my understanding, is

2:00:37

explained by contact forces which themselves are

2:00:39

related to electrodynamics in exchange of particles.

2:00:41

So the analogy seems to be an

2:00:43

accessible one, but nonetheless an analogy doesn't

2:00:46

offer a true explanation. How can we

2:00:48

understand the exchange of particles leads to

2:00:50

attraction like a proton and electron coming

2:00:53

together due to opposite electric charges? Well,

2:00:55

it is not a very good analogy.

2:00:57

It is, you know, it might help

2:01:00

you a little bit, but not too

2:01:02

much. The truth is that the... force

2:01:04

between protons and electrons in a static

2:01:06

situation, i.e. an electron that is bound

2:01:09

to the nucleus of an atom, is

2:01:11

very very difficult to understand as an

2:01:13

exchange of particles. You can do it.

2:01:16

There are ways to do it, but

2:01:18

the number of particles being exchanged is

2:01:20

infinite, and there are subtleties there. It

2:01:23

is easier to understand it as a

2:01:25

static electromagnetic field than as an exchange

2:01:27

of particles. If you are scattering dynamically

2:01:30

two particles off of each other, then

2:01:32

it's easier to understand that as an

2:01:34

exchange of photons. But they are virtual

2:01:36

photons. They are not real photons. And

2:01:39

that... changes things in important ways. I

2:01:41

talk about this also in quantum and

2:01:43

fields. The fact that they're not real

2:01:46

is true. They're not real. They're virtual

2:01:48

particles, which is a way of talking

2:01:50

about the action of the underlying quantum

2:01:53

fields, using particle-like language, even though they're

2:01:55

not real particles. And all of this

2:01:57

is a war. up to say if

2:02:00

you want to use the analogy of

2:02:02

two people throwing a baseball back and

2:02:04

forth to each other, the relevant baseball

2:02:06

has to have negative momentum. So if

2:02:09

you think about conservation of momentum, if

2:02:11

I am on a frictionless surface or

2:02:13

on roller skates or whatever, and I

2:02:16

throw a ball in one direction, conservation

2:02:18

of momentum means I move in the

2:02:20

other direction. As long as, the thing

2:02:23

I'm throwing has a positive momentum. If

2:02:25

the thing I'm throwing has a negative

2:02:27

momentum, then to conserve momentum, I need

2:02:29

to start moving in the same direction.

2:02:32

as the direction in which I've thrown

2:02:34

the ball. And you go through the

2:02:36

math and indeed, for attractive forces, the

2:02:39

virtual particles have negative momentum when they're

2:02:41

being exchanged. And if you say, but

2:02:43

particles don't have negative momentum, the answer

2:02:46

is, real particles don't have negative momentum,

2:02:48

but virtual particles have no problem with

2:02:50

that at all. Michael Kramer says if

2:02:53

Einstein had not developed general relativity when

2:02:55

he did, how soon would it have

2:02:57

been developed? Well, we don't know. I

2:02:59

don't think it would have taken that

2:03:02

long, like it wouldn't have taken 50

2:03:04

or 100 years. We already had all

2:03:06

the tools, right? We had Riemannian geometry.

2:03:09

We had special relativity. It's possible, for

2:03:11

example, that Minkowski, or Minkovsky, to be

2:03:13

a little bit more correct, would have

2:03:16

developed it. Herman Minkowski, of course, um...

2:03:18

was the first to promote the idea

2:03:20

of thinking about relativity in terms of

2:03:23

space time, and he was a mathematician.

2:03:25

He had actually taught Einstein. So it

2:03:27

was 1907, two years after Einstein's special

2:03:29

relativity papers, that Minkowski first said, we

2:03:32

should think about it in terms of

2:03:34

space time. Einstein eventually settled on general

2:03:36

relativity in 1915, but Minkowski passed away

2:03:39

in 1909. So he didn't really get

2:03:41

a chance to follow up on his

2:03:43

insight that we should think about things

2:03:46

in terms of space time. Maybe he

2:03:48

would have come up with it. But

2:03:50

you know, it's an interesting fact about

2:03:53

the progress of physics, that the progress

2:03:55

of physics on theoretical physics, is usually

2:03:57

led by physicists, not by mathematicians, with

2:03:59

overwhelming problems. Not that it's impossible to

2:04:02

imagine mathematicians doing it, but when we

2:04:04

think back to how general relativity came

2:04:06

about and there were real mathematical issues

2:04:09

there and a lot of important steps

2:04:11

were taken by mathematicians. Binkovsky is one,

2:04:13

David Hilbert of course is another, but

2:04:16

still was a physicist. It was Albert

2:04:18

Einstein who actually put it together because

2:04:20

that physics insight... about the principle of

2:04:22

equivalents and how gravity works and things

2:04:25

like that. That's the bread and butter

2:04:27

of physicists, not mathematicians. The question is,

2:04:29

was there any other physicist who would

2:04:32

have thought the same way as Einstein?

2:04:34

There were certainly physicists who had the

2:04:36

same mathematical chops that Einstein did, but

2:04:39

the physical insight that he had was

2:04:41

unmatched since Galileo, basically, and still been

2:04:43

unmatched since. So it might have taken

2:04:46

a while, but the tools were there,

2:04:48

so I don't think it would have

2:04:50

taken too long. Jonathan Bird

2:04:52

says, in physics and philosophy Werner

2:04:55

Heisenberg said, the world thus appears

2:04:57

as a complicated tissue of events

2:04:59

in which connections of different kinds

2:05:01

alternate or overlap or combine and

2:05:03

thereby determine the texture of the

2:05:05

whole. The word texture is refreshing

2:05:07

and sensual. It even feels unscientific,

2:05:10

but maybe that is a philosophical

2:05:12

problem that Heisenberg is trying to

2:05:14

get at. I'd love to hear

2:05:16

what you think about the texture

2:05:18

of the universe and the role

2:05:20

of literary emotional language in describing

2:05:22

it. Well, you know, I'm all

2:05:24

in favor of literary emotional language.

2:05:27

It's too bad that some of

2:05:29

the best physicists in the world

2:05:31

aren't the best describers or poets

2:05:33

or writers in the world. I

2:05:35

think that helps. It prevents a

2:05:37

lot of people from really feeling

2:05:39

what we physicists feel about the

2:05:41

universe in a way that I

2:05:44

would like them to be able

2:05:46

to do. Having said that, so

2:05:48

even though I'm all in favor

2:05:50

of that kind of move... Heisenberg

2:05:52

in particular in this particular passage

2:05:54

is is trying to sell you

2:05:56

something that I don't believe in.

2:05:59

This is you know Heisenberg was

2:06:01

at least as much as Neil's

2:06:03

bore the champion of the Copenhagen

2:06:05

interpretation of quantum mechanics. And it's

2:06:07

an interesting story. You know, John

2:06:09

Wheeler was another of Neil's Boer's

2:06:11

echleights. And Wheeler was, despite being

2:06:13

Hugh Everett's thesis advisor, Wheeler was

2:06:16

really an advocate of the Copenhagen

2:06:18

interpretation of quantum mechanics. And his

2:06:20

Wheeler's famous paper, It From Bit,

2:06:22

that's not the name of the

2:06:24

paper, but the quote that is

2:06:26

remembered from the paper, is It

2:06:28

From Bit. It makes people... think

2:06:31

that Wheeler was saying that reality

2:06:33

is really made of information. And

2:06:35

indeed, there's a whole large effort

2:06:37

right now called it from Cupid,

2:06:39

where we say, well, it's really

2:06:41

quantum information, not classical information that

2:06:43

is doing the work. But that's

2:06:45

not what Wheeler was on about.

2:06:48

That is not his point. His

2:06:50

point being a Copenhagen person is

2:06:52

that what really exists... is not

2:06:54

a wave function or anything like

2:06:56

that. What really exists are the

2:06:58

measurement outcomes. Done by various measurements.

2:07:00

Like before you do the measurement,

2:07:02

this is a very Heisenbergian point.

2:07:05

Wheeler was trying to say like

2:07:07

before you do that measurement, there

2:07:09

isn't any it. Right? And when

2:07:11

you do the measurement in quantum

2:07:13

mechanics, he tried to make an

2:07:15

argument that quantum outcomes are necessarily

2:07:17

discrete. That's not obvious because things

2:07:20

like position of momentum and conventional

2:07:22

quantum mechanics are continuous, but he

2:07:24

took as the paradigm the measurement

2:07:26

of a spin and you get

2:07:28

a yes-no answer. So... John Wheeler

2:07:30

knew about quantum mechanics. He could

2:07:32

have invented it from cubit himself,

2:07:34

but he didn't because he was

2:07:37

making a different point than that.

2:07:39

And that's the point Heisenberg is

2:07:41

making. When he says a complicated

2:07:43

tissue of events, that's not just

2:07:45

poetic language. He means measurement outcomes.

2:07:47

When you're not looking at it,

2:07:49

the thing doesn't exist. That is

2:07:52

the Copenhagen point of view, or

2:07:54

at least there's no sense of

2:07:56

existence that we can objectively talk

2:07:58

about. We should only talk about,

2:08:00

says the Copenhagen interpretation, the results

2:08:02

of measurement. and that's the point

2:08:04

that Heisenberg is aiming at here.

2:08:06

Henry Jacob says multiplying integers is

2:08:09

easy, factoring integers is hard. There's

2:08:11

a directionality. Can this be, can

2:08:13

this difficulty be interpreted entropically, and

2:08:15

does it have any bearing outside

2:08:17

math such as in physics? You

2:08:19

know, I don't actually know. So

2:08:21

you say, can it be interpreted

2:08:24

entropically? And I guess the question

2:08:26

is, is there a colorful analogy

2:08:28

between the two things? Entropy increases.

2:08:30

It's easy to go one way

2:08:32

rather than the other way. certain

2:08:34

mathematical processes are easy one way

2:08:36

not the other way? Or is

2:08:38

there like a really hardcore connection?

2:08:41

Can you derive one from the

2:08:43

other or something like that? This

2:08:45

statement that multiplying in is easy

2:08:47

factoring is hard. This is a

2:08:49

specific example of a more general

2:08:51

idea, as I'm sure Henry you

2:08:53

probably know, but in complexity theory,

2:08:55

like we talked with Scott Aronson

2:08:58

on the podcast some time ago.

2:09:00

One separates problems one can ask

2:09:02

into different levels of complexity and

2:09:04

there is the set of problems

2:09:06

P that are easy to solve,

2:09:08

relatively speaking. There's a set of

2:09:10

problems N.P. And N.P. is not

2:09:13

defined as problems that are hard

2:09:15

to solve. It's defined as problems

2:09:17

whose... prospective answers are easy to

2:09:19

check. Okay? So maybe there are

2:09:21

problems that are hard to solve,

2:09:23

but it's easy to check an

2:09:25

answer. Maybe there's not. That's the

2:09:27

P versus N.P. question. But most

2:09:30

mathematicians, logicians, philosophers think that P

2:09:32

and N.P. are in fact not

2:09:34

equal to each other, which is

2:09:36

a way of saying I believe

2:09:38

there are problems that are hard

2:09:40

to solve, but it's easy to

2:09:42

check a supposed solution. So that

2:09:45

isn't a directionality, an asymmetry between

2:09:47

solving and checking in general. And

2:09:49

there's other things in math that

2:09:51

are like that. Differentiation is kind

2:09:53

of easy, integration is kind of

2:09:55

hard. I don't want to say

2:09:57

that that is the same thing

2:09:59

as entropy increasing. over time. I

2:10:02

don't see why it has to

2:10:04

be, but maybe I've certainly suggested

2:10:06

myself that they sound similar in

2:10:08

some ways. Is that similarity deeper?

2:10:10

I truly don't know. Gary

2:10:13

Miller says in your October 2024

2:10:15

AMA you mentioned James the Just

2:10:17

as likely being a real person. Do

2:10:19

you think that there was historical Jesus

2:10:21

someone you could meet if you traveled

2:10:24

back 2000 years or is Jesus primarily

2:10:26

a retelling of earlier mythological figures? So

2:10:28

James the Just for those of you

2:10:31

who don't know was Jesus's brother and

2:10:33

he was a leader of the

2:10:35

Jerusalem Christians after Jesus was crucified and

2:10:37

there is you know enough... evidence in

2:10:40

the archaeological slash historical records to say

2:10:42

that James existed maybe arguably more than

2:10:44

Jesus. But of course that all depends

2:10:47

on what you think about the New

2:10:49

Testament. The books in the New Testament

2:10:51

are not eyewitness accounts. The earliest books

2:10:54

in the New Testament were written by

2:10:56

Paul and Paul never met Jesus. Paul

2:10:58

never, you know... got to know about

2:11:01

Christianity until after Jesus had already

2:11:03

been crucified. So there's nothing in the

2:11:05

in the New Testament that is an

2:11:07

eyewitness testimony. The Gospels, we believe, are

2:11:10

things that were written down decades after

2:11:12

the fact. They were passed down as

2:11:14

oral traditions before they were written down.

2:11:17

So it's not completely crazy to ask

2:11:19

whether or not Jesus could have been

2:11:21

completely made up. Like there's no such

2:11:24

person as Jesus or not, because we

2:11:26

don't have eyewitness testimony. But I

2:11:28

think that there's plenty of other kinds

2:11:30

of other kinds of testimony. unless you

2:11:33

believe that all of history is completely

2:11:35

unreliable, there's plenty of reasons to think

2:11:37

that Jesus existed. There's very little reason

2:11:40

to think that any quote attributed to

2:11:42

Jesus in the Gospels is very believable,

2:11:45

right? These are supposed to be words

2:11:47

handed down by oral traditions through decades

2:11:49

from person to person. The chance of

2:11:52

distortion or even outright fabrication are

2:11:54

very very large. So I would not

2:11:56

put a lot of credence in any

2:11:58

specific claim about what happened to Jesus

2:12:01

or what he said. but I think

2:12:03

that he almost certainly did exist. Ramone

2:12:05

Van Fleet says, how do you feel

2:12:08

about the ethics surrounding NBA player trades?

2:12:10

I've always found it somewhat curious that

2:12:12

a player can essentially be forced to

2:12:15

move to a new state, work for

2:12:17

a new employer, and leave friends and

2:12:19

family behind without any say in

2:12:21

the matter. I get that the counter

2:12:24

argument is that they're millionaires, and if

2:12:26

they want to do something else they

2:12:28

can, but it still strikes me as

2:12:31

something that we wouldn't be legal in

2:12:33

almost any other setting. You know, I

2:12:35

think it's a reasonable question to ask,

2:12:38

but I think there's another fact in

2:12:40

addition to the fact that they get

2:12:42

paid handsomely for moving around, which is

2:12:45

that you kind of need some

2:12:47

system like that. Even though we have

2:12:49

individual NBA teams, the kind of money-making

2:12:51

entity is the league, not the team.

2:12:54

I mean, de facto, that's not true.

2:12:56

De facto individual teams earn money, but

2:12:58

one team by itself. without a league

2:13:01

to play in, wouldn't earn any money,

2:13:03

okay? You need some kind of cooperative

2:13:05

agreement among many teams. And as part

2:13:08

of having revenues and having competitive balance,

2:13:10

etc., they have the idea of

2:13:12

making trades. I don't think that many...

2:13:14

players have even argued that there just

2:13:17

shouldn't be trades at all. It's interesting

2:13:19

to contemplate what that would be like

2:13:21

if there weren't trades. There's various ways

2:13:24

to imagine tweaking the system, but there

2:13:26

are often trades that benefit everybody, as

2:13:28

perhaps you know, there's certain times when

2:13:31

players demand to be traded, right? And

2:13:33

maybe that benefits both the team and

2:13:36

the player. So I think the system

2:13:38

is very far from perfect, but

2:13:40

something like the system makes sense to

2:13:42

me. Alexander Kondratzki says, one

2:13:45

aspect of quantum measurement has been

2:13:47

bothering me so please correct my

2:13:49

chain of reasoning. It seems that

2:13:51

measurement collapses or slices the wave

2:13:53

function to some eigenstate, but isn't

2:13:55

that dependent on a choice of

2:13:57

basis? Spin-up of an electron is

2:13:59

relative to what you consider. up?

2:14:01

At a fundamental level, how do

2:14:03

we force a basis when we

2:14:06

make a measurement in a laboratory?

2:14:08

Well, the answer is that we

2:14:10

choose what it is, we're going

2:14:12

to measure. So, for example, the

2:14:14

classic example of a quantum measurement

2:14:16

is the Stern-Gurlock experiment. This is

2:14:18

where you send a spinning particle

2:14:20

through an inhomogeneous magnetic field. So

2:14:22

a straight magnetic field wouldn't do

2:14:24

anything, but a magnetic field which

2:14:26

sort of pinched in one direction.

2:14:29

interacts with the spinning particle in

2:14:31

a way that if the spin

2:14:33

is up in the direction that

2:14:35

you've arranged your magnetic field then

2:14:37

the particles deflected up and if

2:14:39

it's pointed down then it's deflected

2:14:41

down and it is a fact

2:14:43

of quantum mechanics that you might

2:14:45

think well what if it's spinning

2:14:47

halfway in between what if it's

2:14:50

spinning perpendicular to the magnetic field

2:14:52

the miracle of quantum mechanics is

2:14:54

that a perpendicularly oriented spin is

2:14:56

a superposition, can be thought of

2:14:58

as a superposition, of a vertically

2:15:00

up and a vertically down, oriented

2:15:02

spin, and those two components get

2:15:04

separated by interacting with the magnetic

2:15:06

field. But you chose to orient

2:15:08

your magnetic field up and down.

2:15:11

You could also choose to orient

2:15:13

it left and right or whatever.

2:15:15

And that would correspond to measuring

2:15:17

a different fact about the spin,

2:15:19

the X-pin or the Y-spin, rather

2:15:21

than the up-up-spin or down-spin, okay?

2:15:23

So it's just a fact of

2:15:25

physics. real physical measurements happen because

2:15:27

you have an apparatus and some

2:15:29

object that are interacting with the

2:15:31

system you're measuring in some very

2:15:34

particular way and what that particular

2:15:36

field but you chose to orient

2:15:38

your magnetic field up and down

2:15:40

you could also choose to orient

2:15:42

it left and right or whatever

2:15:44

and that would correspond to measuring

2:15:46

a different fact about the spin

2:15:48

the X-pin or the Y-spin rather

2:15:50

than the upspin or downspin okay

2:15:52

so It's just a fact of

2:15:55

physics, like real physical measurements happen.

2:15:57

because you have an apparatus and

2:15:59

some object that are interacting with

2:16:01

the system you're measuring in some

2:16:03

very particular way. And what that

2:16:05

particular way is and what your

2:16:07

apparatus is doing tells me whether

2:16:09

I'm measuring the vertical spin or

2:16:11

the horizontal spin or am I

2:16:13

measuring position or momentum or whatever.

2:16:16

All these different things are measured

2:16:18

using different actual experiments. So it's

2:16:20

not like the rules of quantum

2:16:22

mechanics force it on us. It's

2:16:24

our choice of experiment forces it

2:16:26

on us. Enrique Areola says, regarding

2:16:28

the second law of thermodynamics, wouldn't black hole radiation be

2:16:30

a violation of this law, given that black holes have

2:16:32

the highest entropy possible? And that their radiation leads to

2:16:35

their eventual disappearance, which means that entropy would essentially decrease?

2:16:37

So no, because black holes do not have the highest

2:16:39

entropy possible. I kind of rained on about this in

2:16:41

my first trade book from eternity to here. In fact,

2:16:43

I upset Roger Penrose. Roger Penrose was nice enough to

2:16:45

blurb the book. But he has made this statement that

2:16:48

black holes have the highest entry possible, and it's not

2:16:50

true, and he knows it's not true. They have the

2:16:52

highest entropy possible in a given region of space. But

2:16:54

when they evaporate, when they dissolve into particles that are

2:16:56

radiated away by a hawking radiation, the particles that carry

2:16:58

away the energy are spread over a much larger region

2:17:01

of space. And you can calculate what the entropy is

2:17:03

of all the hawking radiation and is larger than the...

2:17:05

initial entropy of the black hole. It's just not squeezed

2:17:07

into a small region of space. So I pointed out

2:17:09

in the book that Penrose was wrong about this and

2:17:11

he asked me to change the phrasing to be something

2:17:14

that indicated that he knew that all along, which is

2:17:16

probably true, so I can't really complain. Dave Whipp says,

2:17:18

if I pick a few points on the edge of

2:17:20

a circle, an attempt to draw lines to the center,

2:17:22

most likely they will be at a triangle or some

2:17:24

other polygon. It's really hard to draw them precisely to

2:17:27

meet at a point. Yet the story of Hubble is

2:17:29

that when we observed a handful of galaxies moving away

2:17:31

from us, and then plotting the movement in reverse concludes

2:17:33

universe must have started from

2:17:35

a point of infinite density

2:17:37

period. What leads the conclusion

2:17:40

that radial lines must have

2:17:42

started classically from a singular

2:17:44

point rather than at some

2:17:46

region that simply was smaller

2:17:48

than today but finite? Is

2:17:50

this pop story overly simplified?

2:17:53

This is a perfectly good

2:17:55

question, and I get to

2:17:57

talk about Roger Penrose once

2:17:59

again. If the particles in

2:18:01

the universe didn't have any

2:18:03

forces acting on them, in

2:18:06

particular didn't have gravity acting

2:18:08

on them, then indeed they

2:18:10

would move on straight lines,

2:18:12

and it would be really,

2:18:14

really strange indeed to imagine

2:18:16

we could extrapolate them backward

2:18:19

to a singularity. But they

2:18:21

do have gravity acting on

2:18:23

them, and even in Newtonian

2:18:25

gravity they would come close

2:18:27

but ultimately miss each other.

2:18:29

But general relativity is different.

2:18:32

General relativity becomes stronger when

2:18:34

things become very, very dense.

2:18:36

That's why you can make

2:18:38

black holes and things like

2:18:40

that. And so it was

2:18:42

Penrose who first proved a

2:18:45

theorem that was extrapolated to

2:18:47

the cosmological case by Stephen

2:18:49

Hawking. But the theorem basically

2:18:51

says if you have enough

2:18:53

energy density in a region

2:18:55

and it obeys certain conditions

2:18:58

that are mathematically straightforward to

2:19:00

write down, then you will

2:19:02

inevitably have a singularity. This

2:19:04

is a feature of general

2:19:06

relativity. Now, general relativity might

2:19:08

not be right, who knows,

2:19:11

at large energies or something

2:19:13

like that where quantum mechanics

2:19:15

kicks in. But I think

2:19:17

it is, that's why Roger

2:19:19

Penrose won the Nobel Prize

2:19:21

for proving that singularities in

2:19:24

black holes, and also for

2:19:26

that matter in the past

2:19:28

at what we call the

2:19:30

Big Bang, are a prediction

2:19:32

of classical general relativity. Philip

2:19:34

Rothlin says, I asked GPT

2:19:37

to analyze all previously asked

2:19:39

questions in all AMAs to

2:19:41

identify recurring topics and determine

2:19:43

your areas of expertise. Based

2:19:45

on this analysis, I wanted

2:19:47

GPT to generate a fresh,

2:19:50

insightful question that has not

2:19:52

yet been asked, but aligns

2:19:54

with your knowledge. Here's the

2:19:56

question it came up with.

2:19:58

Many of your discussions revolve

2:20:00

around AI. However, one aspect

2:20:03

that hasn't yet been deeply

2:20:05

explored. how AI intersects with emerging fields like neuroscience

2:20:07

or ethics. What are some underappreciated insights or challenges at

2:20:09

this intersection that you find particularly compelling? So I

2:20:11

don't think GPD did a very good

2:20:13

job at this one. Sorry, Philip. I

2:20:16

don't think it's your fault. But, uh...

2:20:18

Of all the things to ask me

2:20:20

about, AI is a weird one, especially

2:20:22

because, you know, I have certain things

2:20:24

I feel strong about AI, but many

2:20:26

things I don't, because I try to

2:20:28

keep track of what I am not

2:20:31

an expert in. Specifically, you know, how,

2:20:33

and also the form of the question

2:20:35

isn't the best. You know, this is...

2:20:37

repeating back to the previous question about,

2:20:39

you know, can we ask questions over

2:20:42

and over again, this kind of very

2:20:44

vague open-ended question is sub-ideal. It's okay,

2:20:46

but just saying like, what underappreciated insights

2:20:48

or challenges do you find particularly compelling?

2:20:50

That's exactly the kind of question I'm

2:20:52

unlikely to answer because it's a little

2:20:54

bit too vague. If you have your

2:20:56

favorite insider challenge that you would like

2:20:59

me to comment on, you're more likely

2:21:01

to get... me to answer that kind

2:21:03

of question. I don't know. So the

2:21:05

answer is I don't know. So I

2:21:07

probably wouldn't pick this question. I'm picking

2:21:09

the question because of the cute AI

2:21:12

framing of it, but the actual question

2:21:14

being asked, I probably wouldn't pick, because

2:21:16

I don't have any special, anything especially

2:21:18

interesting to say about that, especially ethics.

2:21:21

I'm not sure why AI would have,

2:21:23

I mean, obviously there's questions about ethics

2:21:25

of AI, of, you know, could we

2:21:27

imagine building an AI that was conscious

2:21:30

and had agency and deserved rights? Those

2:21:32

are interesting questions. My answer to that

2:21:34

is we can imagine it, but we're

2:21:37

not close to doing it. But the

2:21:39

existence of AI as being something that

2:21:41

we would use to explore ethics, I'm

2:21:43

really not sure why that would happen.

2:21:46

Colin Small says you talked at

2:21:48

lengths about your love for basketball

2:21:50

as a fan, but do you

2:21:52

play basketball as well? Does Sean

2:21:54

Carroll dunk can Sean Carroll splash

2:21:57

threes? So anyone can splash threes

2:21:59

given enough... time, given enough opportunities.

2:22:01

No, I'm not very good at playing

2:22:03

basketball these days. I am of a

2:22:05

certain age where my basketball playing days

2:22:07

are largely behind me. I mean, I

2:22:09

could, but it's just that my environment

2:22:12

does not lend itself to doing that

2:22:14

very easily. I'm not so decrepit that

2:22:16

I cannot get out there on a

2:22:18

basketball court, but as a matter of

2:22:20

fact, it's been a long time since

2:22:23

I have. When I was an undergraduate

2:22:25

and even more so when I was

2:22:27

a graduate student, I was playing quite

2:22:29

regularly. And I was entirely mediocre. I

2:22:31

was, you know, in our set of

2:22:34

astronomers who made up our intramural basketball

2:22:36

team, which I was on. I was

2:22:38

not a star, nor was I the

2:22:40

worst player on the team. There was

2:22:42

no dunking involved, certainly not on a

2:22:45

regulation rim anyway. The only interesting thing

2:22:47

I can say about that is that

2:22:49

there's a chance, and I truly don't

2:22:51

know if it's true, but there's a

2:22:53

chance that I once played basketball against

2:22:56

Barack Obama. I wouldn't have known it

2:22:58

at the time, but we had an

2:23:00

intramural basketball team, and I was a

2:23:02

grad student between 88 and 93, and

2:23:04

I think that my first three years

2:23:07

there at Harvard... coincided with Barack Obama's

2:23:09

law school career at Harvard, and we

2:23:11

definitely played intramural teams from the law

2:23:13

school, and he was a basketball player.

2:23:15

So it's completely possible that I guarded

2:23:18

Barack Obama once, but I have no

2:23:20

recollection of it right now. Sorry about

2:23:22

that. Ben Lloyd says, you've talked briefly

2:23:24

a few times about the idea of

2:23:26

bubble universes being a plausible answer as

2:23:29

to how we think about this unusual

2:23:31

low entropy at the Big Bang. Do

2:23:33

you think this hypothesis is not talked

2:23:35

about enough? And if so, why? I

2:23:37

know Stephen Hawking was a proponent of

2:23:40

it, but I don't see many other

2:23:42

physicists talking about it. I'm guessing that's

2:23:44

due to it being hard to get

2:23:46

lots of empirical evidence for at the

2:23:48

moment. Also, and maybe this is a

2:23:51

silly question... But how does this hypothesis

2:23:53

align with other prevailing theories such as

2:23:55

cyclic models and inflation? Is there a

2:23:57

potential for overlap or are these theories

2:23:59

generally considered to be mutually exclusive? Well

2:24:02

certainly the way that Jennifer Chen and

2:24:04

I... imagined it in our paper from

2:24:06

2004, we use inflation as part of

2:24:08

the story, but it's not a traditional

2:24:10

eternal inflation model or a cyclic model

2:24:13

for the simple reason that those ideas,

2:24:15

again the traditional version of those ideas,

2:24:17

have an arrow of time that points

2:24:19

in the same direction for all eternity.

2:24:21

So you have to bake it in.

2:24:24

You are not explaining why there's an

2:24:26

arrow of time. You're just putting it

2:24:28

in to your hypothesis. Our attempt was

2:24:30

to explain why there's an arrow of

2:24:32

time and the way that we did

2:24:35

it was to have the arrow point

2:24:37

toward the future and point toward the

2:24:39

far far past early in the pre-big

2:24:41

bang scenario. So I think that it...

2:24:43

I would be happy if there was

2:24:46

more talk about this scenario, but you

2:24:48

know, it is based on highly speculative

2:24:50

ill-understood physics in our particular version of

2:24:52

it. I am working on a paper

2:24:54

about this scenario right now to sort

2:24:57

of push it forward, but there's a

2:24:59

lot we don't know. So, and that's

2:25:01

perfectly fine. You know, scientists will... make

2:25:03

choices about what to work on, and

2:25:05

it's not just because a question is

2:25:08

interesting, but also because they think they

2:25:10

can make progress on the question. That's

2:25:12

a perfectly legitimate idea for scientists to

2:25:14

have. I personally think that this question

2:25:16

is much more interesting than the average

2:25:19

person, because I'm very aware of this

2:25:21

arrow of time issue that I think

2:25:23

other people are not paying enough attention

2:25:25

to. Rob Patro says, Doge and

2:25:27

the administration have made it clear, I think, that

2:25:30

the assault on science is not just an effort

2:25:32

to cut costs, but an effort to either destroy

2:25:34

science outright in America or to diminish and censor

2:25:36

it to such an extent that it becomes unrecognizable,

2:25:39

imperiling American scientific excellence in our national security in

2:25:41

one fell swoop. As a scientist, I'm someone at

2:25:43

a loss what to do in this brave new

2:25:45

world. My question to you is twofold. What should

2:25:47

scientists be doing to help salvage what we can

2:25:50

of our institutions and the systems that have made

2:25:52

America a world leader? Along the same lines,

2:25:54

and if it does make

2:25:56

sense to think about

2:25:59

abandoning ship for a country

2:26:01

with administration that doesn't

2:26:03

view scientists as the enemy,

2:26:05

but rather a national

2:26:07

resource. You

2:26:10

know, I don't quite want

2:26:12

to agree with the premise

2:26:14

of the question right away.

2:26:16

So I don't think that

2:26:18

they made it clear that

2:26:20

it is an effort to

2:26:22

destroy science outright in America.

2:26:24

I think that's an overly

2:26:26

simplistic way of putting it.

2:26:28

There's some aspect of it.

2:26:31

I mean, there's no question

2:26:33

that various members of the

2:26:35

administration, most obviously JD Vance,

2:26:37

the vice president, but others

2:26:39

as well, have taken an

2:26:41

explicitly anti -academic, anti -intellectual point

2:26:43

of view on things. Vance

2:26:45

has said, professors are the

2:26:47

enemy, universities are the enemy,

2:26:49

etc. And I think it's

2:26:51

unmistakable that certain aspects of

2:26:53

university existence and life are

2:26:55

looked down upon by the

2:26:57

administration. But honestly, I think

2:26:59

that, you know, you can't

2:27:01

undersell the idea that it's

2:27:03

not even that intentional what

2:27:05

they're doing. What they want

2:27:07

to do is cut costs

2:27:09

and there's an attitude that

2:27:11

they know better than everybody

2:27:13

else. It's a fundamentally anti

2:27:15

-expertise philosophy, right? Like the

2:27:17

idea that there are people

2:27:19

who know a lot about

2:27:21

things and, you know, should

2:27:23

be trusted with the hardest

2:27:25

decisions is anathema to the

2:27:27

people who are running the

2:27:29

country right now. And it's

2:27:31

in part a reflection of

2:27:33

a Silicon Valley ethos. It's

2:27:35

not hard to dig up

2:27:37

quotes by Silicon Valley leaders

2:27:39

disparaging the idea of reading

2:27:41

books in favor of, you

2:27:43

know, everything interesting should be

2:27:45

put in a blog post

2:27:47

or something like that, right?

2:27:49

The idea of like hard

2:27:51

earned, very careful expert level

2:27:53

knowledge is just not something

2:27:55

that is respected. So they

2:27:57

don't see why they should

2:27:59

spend all this money on

2:28:01

science and education and things

2:28:03

like that. It's really just

2:28:05

a matter of whipping the

2:28:07

workers to work harder. That's

2:28:09

what we really need. Right? So, of

2:28:11

course, de facto these align. At the end of the

2:28:13

day, you end up destroying science, destroying trust in science,

2:28:15

destroying trust in the United States from scientists abroad and

2:28:17

so forth. As far as when and if it makes

2:28:19

sense to think about abandoning ship, you know, you can

2:28:21

always think about it. That's a very personal decision. As

2:28:23

I've said before, my inclination is always to stay and

2:28:25

fight and to make things better, but... You can

2:28:27

imagine things becoming so bad

2:28:30

or opportunities arising elsewhere that

2:28:32

you might want to do

2:28:34

that. I can't offer any

2:28:37

individual advice. What can scientists

2:28:39

do? You know, I honestly don't

2:28:41

know a lot. We're not a

2:28:43

lot of the electorate. I think

2:28:45

that we can try. Yeah, I

2:28:47

guess... The reason I'm hesitating is

2:28:49

because there's obviously things to do,

2:28:52

but they're all kind of vague

2:28:54

and none of them are immediately

2:28:56

effectual. I think that scientists need

2:28:58

to get more support from the

2:29:00

world. We need to be a

2:29:02

little bit less insular and focused

2:29:04

on talking to each other and

2:29:06

more devoted to talking to people

2:29:09

outside, both science, but also academia

2:29:11

or our political perspectives or

2:29:13

what have you. people on

2:29:15

the street need to be

2:29:18

convinced of the importance of

2:29:20

science, and to be convinced

2:29:22

of the importance of intellectual

2:29:24

life more broadly. Scientists are

2:29:27

just as able to have

2:29:29

internecine... battles, you know, disparaging

2:29:31

other departments in the university

2:29:33

as anyone else is. And

2:29:36

I think that we need

2:29:38

to understand that we are

2:29:40

on the same side overall in

2:29:42

this, and I think that we

2:29:44

need to reinvigorate not just respect

2:29:46

for education, but also education.

2:29:48

We need to make higher

2:29:50

education cheaper and more prevalent,

2:29:52

so that people understand what's

2:29:55

going on a little bit

2:29:57

better. Part of that is

2:29:59

as straightforward as decreasing the

2:30:01

debt that students come out of

2:30:03

college with, right? Making it more

2:30:05

accessible by letting more people in

2:30:07

and letting it be more affordable

2:30:09

to more people. And then of

2:30:11

course I think that, you know,

2:30:13

universities can't, as people very often

2:30:15

said, cannot acquiesce prematurely. There's this

2:30:18

very, very embarrassing thing that it

2:30:20

just happens with Columbia University. You

2:30:22

might know that... Columbia was at

2:30:24

the center of accusations of anti-Semitism

2:30:26

because there were protests on Colombia's

2:30:28

campus against Israel's war in Gaza,

2:30:30

and I did not follow that

2:30:32

very very carefully myself, but I

2:30:35

have zero doubt that some people

2:30:37

at some point involved in those

2:30:39

protests said anti-Semitic things. and I'm

2:30:41

not in favor of being anti-Semitic

2:30:43

or supporting anti-Semitism. I am in

2:30:45

favor of allowing protests on campus,

2:30:47

and so it's the university's job

2:30:49

to balance these values and allow

2:30:51

people to speak their minds without

2:30:54

being threatening or racist or anything

2:30:56

like that. So Columbia... had a

2:30:58

lot of protests and for whatever

2:31:00

reasons, again I don't know, I

2:31:02

haven't been following it too carefully,

2:31:04

they were the epicenter of criticism

2:31:06

by Republicans in Congress for allowing

2:31:08

these things to go forward. And

2:31:10

so the university, so the administration

2:31:13

just... canceled or threatened to cancel,

2:31:15

you never know with this administration

2:31:17

whether they're actually doing something or

2:31:19

just blustering about doing something, but

2:31:21

they threatened to cancel $400 million

2:31:23

worth of grant money to Columbia.

2:31:25

And in response, Columbia basically completely

2:31:27

folded and said, oh, well, we're

2:31:29

sorry and we'll try to do

2:31:32

better. And I think that that's,

2:31:34

it's just a strategic mistake. It's

2:31:36

both a values-based mistake. We shouldn't

2:31:38

be those people. We should be

2:31:40

better than that. But it's also

2:31:42

as an absolutely practical matter a

2:31:44

mistake because It's not like the

2:31:46

people who are trying to cut

2:31:49

money to universities will hear you

2:31:51

grovel and say, oh, okay, I

2:31:53

changed my mind, you get your

2:31:55

money back. There's no amount of

2:31:57

groveling that will get the money

2:31:59

back. So long-wind the way of

2:32:01

saying, I think universities need to

2:32:03

stand up. They need to be

2:32:05

very, very clear about their support

2:32:08

for free speech, for intellectual inquiry,

2:32:10

for science, for the humanities, for

2:32:12

everything else that we're supposed to

2:32:14

stand for as institutes of higher

2:32:16

education. Will that help? Maybe it

2:32:18

will help down the road. I

2:32:20

don't know what the short-term effects

2:32:22

will be. Mark V. says, you've

2:32:24

mentioned that advanced civilizations could try

2:32:27

to make contact through long-lasting objects.

2:32:29

Imagine such a civilization had visited

2:32:31

Earth around the time land vertebrates

2:32:33

with eyes had evolved. They had

2:32:35

also determined that our moon was

2:32:37

a promising geologically stable location to

2:32:39

place such an object. Moreover, the

2:32:41

civilization was capable of modifying the

2:32:43

surface of the moon to draw

2:32:46

a large-scale message that would be

2:32:48

visible from Earth. Assuming they prioritized

2:32:50

geological stability in long-term visibility, what

2:32:52

kind of symbols or patterns might

2:32:54

they create to ensure their message

2:32:56

is noticeable as intentional communication. Well,

2:32:58

it wouldn't be that hard, right?

2:33:00

I mean, you could just like

2:33:03

write a bullseye or a little,

2:33:05

you know, cartoon image of an

2:33:07

atom or something like that. Or

2:33:09

you could be more clever and

2:33:11

do something like we had on

2:33:13

the Voyager spacecraft, right? The Golden

2:33:15

Record thing that tried to have

2:33:17

little symbols representing where we are

2:33:19

in the cosmos and things like

2:33:22

that. So there's many things that

2:33:24

you could do. But I think

2:33:26

that that's not really the way

2:33:28

that I would think. I think

2:33:30

that's a pretty kind of kind

2:33:32

of... dumb way for the aliens

2:33:34

to leave a message for us.

2:33:36

I mean, remember it's hard to

2:33:38

conceptualize this, but we're imagining civilizations

2:33:41

that are enormously more technologically advanced

2:33:43

than us. They could do better

2:33:45

than paint the moon. They could

2:33:47

invent, you know, in... long lasting

2:33:49

machines, self-reparing, running on solar power,

2:33:51

you know, etc. that could repaint

2:33:53

the moon every three days, right?

2:33:55

They could send us signals in

2:33:58

all sorts of ways. You know,

2:34:00

again, I think that whatever the

2:34:02

aliens wanted to do, they could

2:34:04

do it. So either they haven't

2:34:06

done that? or they, and this

2:34:08

way that I'm thinking of, you

2:34:10

know, could be triggered by certain

2:34:12

signals in the earth, you know,

2:34:14

global warming, or the detonation of

2:34:17

nuclear warheads, or radio waves indicating

2:34:19

advanced technology, right? I mean, there's

2:34:21

all sorts of ways that they

2:34:23

could trigger some... machine that they

2:34:25

had left behind in the solar

2:34:27

system to sort of come to

2:34:29

life and give us messages. So

2:34:31

either they haven't wanted to do

2:34:33

that, or you know, maybe they're

2:34:36

waiting for more advancement than we

2:34:38

have. Maybe they have a little

2:34:40

trigger that says, wait until we

2:34:42

hear radio waves and then wait

2:34:44

another 10,000 years. Right? Who knows?

2:34:46

I really don't know. I think

2:34:48

if aliens want to talk to

2:34:50

us, it wouldn't be hard to

2:34:52

notice. Benjamin Zand says, do you

2:34:55

have any plans to host to

2:34:57

organize another moving Naturalism Forward seminar

2:34:59

like you did in 2012? We

2:35:01

know you're busy, but you can

2:35:03

count on support for Mindscape listeners.

2:35:05

Yeah, you know, that's something that

2:35:07

would be one among many, many

2:35:09

fun things that one could do.

2:35:12

I don't have any plans to

2:35:14

do that. For those of you

2:35:16

who don't know, in 2012 we

2:35:18

got together a small group of

2:35:20

people in Stockbridge, Massachusetts, and the

2:35:22

idea was to get-together people who

2:35:24

were... naturalists in many different fields,

2:35:26

naturalists in the sense of not

2:35:28

like studying plants, but not theists,

2:35:31

okay, so bait the atheists, and

2:35:33

rather than figure it, talk about,

2:35:35

you know, ways of combating theism

2:35:37

or intelligent design or whatever, it

2:35:39

agree that we all are on

2:35:41

the same boat in the same

2:35:43

track with this. question, but there's

2:35:45

still questions that remain unanswered that

2:35:47

we need to think about moving

2:35:50

forward with. So we talked about

2:35:52

consciousness and free will and morality

2:35:54

and things like that. It was

2:35:56

really, it was quite, I think

2:35:58

it was quite a success. I

2:36:00

mean, maybe you could always be

2:36:02

more successful. We didn't ask anyone

2:36:04

to write a document or a

2:36:06

paper or anything, but we did

2:36:09

videotape everything and they're all quite

2:36:11

well edited and on YouTube. For

2:36:13

whatever reason, the YouTube videos never

2:36:15

took off. They never got a

2:36:17

lot of... hits. I will try

2:36:19

to remember to put a link

2:36:21

in the show notes to the

2:36:23

Moving Naturalism Forward videos. But doing

2:36:26

it again, well, it was a

2:36:28

special event. There were people there

2:36:30

who are no longer with us,

2:36:32

like Dan Dennett and Stephen Weinberg.

2:36:34

And it would be a different

2:36:36

group of people, obviously, but I

2:36:38

think there's other things to be

2:36:40

done. Like I did that. In

2:36:42

fact, David Wallace and I have

2:36:45

talked a lot about a moving

2:36:47

Everett Forward conference, where we get

2:36:49

people who are only allowed to

2:36:51

come if you're a believer in

2:36:53

the ever interpretation of quantum mechanics,

2:36:55

and we admit that there's lots

2:36:57

of questions unanswered yet, and we

2:36:59

work on answering them. But who

2:37:01

knows whether that will happen? There's

2:37:04

a lot of things that we

2:37:06

need to do. Ask me after

2:37:08

I've done. Tom S asks a

2:37:10

priority question. I've been bothered by

2:37:12

this question since the early 90s.

2:37:14

It involves special relativity. Given that

2:37:16

a photon does not experience time,

2:37:18

it should also be... the distance

2:37:20

traveled from the photon's frame of

2:37:23

reference is zero. In essence, to

2:37:25

the photon, it is simply jumping

2:37:27

from one atom to an adjacent

2:37:29

atom. Since no time elapses for

2:37:31

the photon, since leaving the source

2:37:33

atom and being at the destination

2:37:35

atom, the destination atom had to

2:37:37

be fixed when the photon left

2:37:40

the source. So from my frame

2:37:42

of reference, I walked into my

2:37:44

backyard at night, stare up into

2:37:46

the sky, and a photon from

2:37:48

a star a thousand years away

2:37:50

strikes my eye. would suggest to

2:37:52

me that there is no free

2:37:54

will. I had no choice but

2:37:56

to be born and walk out

2:37:59

at them. the destination atom had

2:38:01

to be fixed when the photon

2:38:03

left the source. What does the

2:38:05

word when mean in that question?

2:38:07

Because the whole point of relativity

2:38:09

is that dividing up space time

2:38:11

into space and time is different

2:38:13

for different observers. What you mean

2:38:15

is in the photons frame of

2:38:17

reference, the atom is in the

2:38:19

same... time in some null coordinates

2:38:21

as when the photon left the

2:38:24

source. But not in mine, right?

2:38:26

Not in the frame of reference

2:38:28

of the thing that emitted the

2:38:30

photon in the first place. There,

2:38:32

the thing was set up long

2:38:34

before it was absorbed. Okay? So

2:38:36

this is a prospective relative question

2:38:38

and different people are going to

2:38:40

say different things about it. Really,

2:38:42

I think the issue here is

2:38:44

not anything about special relativity or

2:38:46

photons. It's just about determinism. If

2:38:48

you believe that the world is

2:38:50

deterministic, then you know what happens

2:38:53

now and you're going to be

2:38:55

able to, you know that what

2:38:57

happens now will enable you to

2:38:59

predict what happens in the future.

2:39:01

Even as an indeterministic person, since

2:39:03

I think the quantum mechanics exists,

2:39:05

I am a block universe person,

2:39:07

so there is a fact of the

2:39:09

matter about what will happen in the

2:39:11

future, even though I don't know what

2:39:13

it is. And then of course the

2:39:15

question is, does this have any bearing

2:39:17

at all on the question of free

2:39:19

will? That's a longer... conversation that I've

2:39:21

talked about many different places, but I

2:39:23

think of free will as perfectly compatible

2:39:25

with determinism because I'm a compatibleist. I

2:39:27

think that free will is a higher

2:39:29

level emergent phenomenon, at least in the

2:39:31

way that I think about people making

2:39:33

choices. If you want to define free

2:39:35

will as the ability to violate the

2:39:37

laws of physics in a libertarian sense,

2:39:40

then I don't believe in that. So

2:39:42

you really, I would suggest if you

2:39:44

care about these questions, really dig into

2:39:46

the issues of compatibleism and the meaning

2:39:48

of free will. You know, talk to

2:39:51

or listen to the podcast I did

2:39:53

with Jan Nismayel or Dan Dennett or

2:39:55

one of the various people that we

2:39:57

went over that question with. Kelly

2:40:00

Hoogland says, I was listening to an

2:40:02

episode of Radio Lab, which is a

2:40:04

science storytelling podcast. In this episode, they

2:40:06

were briefly explaining quantum entanglement. Without giving

2:40:08

you any direct quotes, given that the

2:40:11

words in the way that I think

2:40:13

about people making choices. If you want

2:40:15

to define free will as the ability

2:40:17

to violate the laws of physics, in

2:40:19

a libertarian sense, then I don't believe

2:40:21

in that. So you really, I would

2:40:23

suggest if you care about these questions,

2:40:26

really dig into the issues of compatibleism

2:40:28

and the meaning of free will. You

2:40:30

know, talk to or listen to the

2:40:32

podcast I did with in Anismail or

2:40:34

Dan Dennett or one of the various

2:40:36

people that we went over that question

2:40:39

with. Kelly Hoogland says, I

2:40:41

was listening to an episode of

2:40:43

Radio Lab, which is a science

2:40:45

storytelling podcast. In this episode, they

2:40:47

were briefly explaining quantum entanglement. Without

2:40:49

giving you any direct quotes, given

2:40:51

that the words observer or superposition

2:40:53

were not used once, how good

2:40:55

a job could they have done?

2:40:57

I think you didn't give me

2:40:59

quite enough information to tell you

2:41:01

how good a job they could

2:41:03

have done. Certainly, if the question

2:41:05

is secretly, can one... adequately explain

2:41:07

entanglement without using words or equivalent

2:41:09

words to observer and superposition, I

2:41:11

don't think that the word observer

2:41:13

or observation or measurement plays any

2:41:15

role at all in explaining entanglement.

2:41:17

I don't think that's what entanglement

2:41:19

is about. But I would think

2:41:21

that, since I am in ever

2:41:23

ready and never ready, in this

2:41:25

don't think that measurements or observations

2:41:27

are special things, it's all just

2:41:29

the wave function obeying the Schrodinger

2:41:31

equation at the end of the

2:41:33

day. The word superposition is harder

2:41:35

to avoid when you're talking about

2:41:37

entanglement. To explain entanglement, when I

2:41:39

explain it, I first have to

2:41:41

say if there's a spin, a

2:41:43

particle with spin, it can be

2:41:45

in a superposition of spin-up and

2:41:47

spin-down, for example. And if you

2:41:49

have two spins, it's not true

2:41:52

that they are just separately in

2:41:54

superpositions of spin-up and spin-down. They

2:41:56

are in superpositions of an entangled

2:41:58

superposition. They can be entangled superposition.

2:42:00

One of them is up, the

2:42:02

other is down, if the other

2:42:04

one is down, if the first

2:42:06

one is down, the other one

2:42:08

is up. So could you explain

2:42:10

that without using the word or

2:42:12

concept of superposition? That would be

2:42:14

very, very difficult. I mean, somehow

2:42:16

to explain entanglement, you have to

2:42:18

get across the idea of what

2:42:20

a quantum state is. That's why

2:42:22

observations don't matter how I observe

2:42:24

the quantum state. What really matters

2:42:26

is what quantum states are. And

2:42:28

you don't need to use the

2:42:30

word superposition in explaining what quantum

2:42:32

states are, but given that we

2:42:34

usually start by thinking about classical

2:42:36

observable phenomena, it is traditionally easiest

2:42:38

to talk about superpositions when we

2:42:40

do that. Rory Cochran says, I

2:42:42

keep coming back in my mind

2:42:44

to what I feel like is

2:42:46

a clash between your December 2023

2:42:48

immortality address, in which you conclude

2:42:50

that humanity is doomed because the

2:42:52

universe is headed for a heat

2:42:54

death in city space, and David

2:42:56

Deutsch's ideas in the beginning of

2:42:58

infinity in which he says words

2:43:00

to the effect that any problem

2:43:02

can in principle be solved once

2:43:04

the knowledge of how to do

2:43:06

it is discovered, with the only

2:43:08

limit being whether or not the

2:43:10

solution is prohibited by the law

2:43:12

of physics. be done about the

2:43:14

looming key death of the universe?

2:43:16

Can we say for certain that

2:43:18

humans or intelligent life could never

2:43:20

work out some novel piece of

2:43:22

universe? Some engineering perhaps with elegantly

2:43:25

placed black holes or little big

2:43:27

bangs or something? If we can't

2:43:29

rule it out then there's hope

2:43:31

for immortality yet. Well, I hope

2:43:33

that if you are a long-time

2:43:35

listener of Mindscape, you know that

2:43:37

questions about categorically saying things and

2:43:39

being certain about things are always

2:43:41

met with, no, we cannot categorically

2:43:43

say things, we cannot be certain

2:43:45

about things. That's just not how

2:43:47

the way things work. We can

2:43:49

make provisional statements subject to certain

2:43:51

assumptions. So... If you assume, as

2:43:53

I tried to assume in the

2:43:55

talk about immortality, that we really

2:43:57

are going to live in dissiter

2:43:59

space with a forever eternal cosmological

2:44:01

constant that will never decay, and

2:44:03

you assume that our... understanding of

2:44:05

what it means to reach equilibrium

2:44:07

in a thermodynamic system is more

2:44:09

or less correct, and you agree

2:44:11

that thinking in any real substantive

2:44:13

sense increases entropy and requires an

2:44:15

out of equilibrium condition, then it

2:44:17

is just a fact that the

2:44:19

laws of physics, even up to

2:44:21

David Deutsch's way of thinking about

2:44:23

it, prohibit immortality. in this universe.

2:44:25

Now of course all those assumptions

2:44:27

could be wrong in one way

2:44:29

or another. After all we could

2:44:31

be living in a simulation. for

2:44:33

all we know, right? And we

2:44:35

might think of it as very

2:44:37

unlikely, but could be, it's possible,

2:44:39

it's possible to cause module constant

2:44:41

will go away, it's possible that

2:44:43

the universe will reclapse, who knows?

2:44:45

There's many hopes that you could

2:44:47

hold out for, but I'd like

2:44:49

to think that it's useful to

2:44:51

think through our best understanding of

2:44:53

the universe and to try to

2:44:55

figure out what is compatible and

2:44:58

incompatible with that understanding, even admitting

2:45:00

that that that understanding might need

2:45:02

to be modified someday. Arminio Maginzini

2:45:04

says, the gravity waves we have

2:45:06

detected have been created by the

2:45:08

collision of black holes and neutron

2:45:10

stars. Are these the only objects

2:45:12

that produce gravity waves, or are

2:45:14

these the only objects that LIGO

2:45:16

can detect? That is, is LIGO

2:45:18

incapable of detecting weaker waves? Mostly,

2:45:20

it's incapable of detecting weaker waves.

2:45:22

There's plenty of other ways to

2:45:24

make gravitational waves, but it's not

2:45:26

just a matter of weakness. It's

2:45:28

also a matter of frequency, right?

2:45:30

Just like there are telescopes that

2:45:32

look at... visible light and different

2:45:34

telescopes that look at radio waves

2:45:36

and different telescopes that look at

2:45:38

x-rays, gravitational wave observatories have a

2:45:40

bandwidth. They have a region of

2:45:42

the gravitational wave spectrum to which

2:45:44

they are sensitive. So, for example,

2:45:46

we are pretty sure that there's

2:45:48

lots of gravitational waves being made

2:45:50

by spinning neutron stars, or spinning

2:45:52

white dwarfs for that matter, possibly

2:45:54

by supernova explosions, almost certainly by

2:45:56

medium-sized black holes spiraling into supermassive

2:45:58

black holes in our... galaxy and

2:46:00

elsewhere. We think that all these

2:46:02

are out there. There might even

2:46:04

be a cosmic gravitational wave background

2:46:06

from the early universe for all

2:46:08

that we know. But LIGO is

2:46:10

just not sensitive to the relevant

2:46:12

bands for those kinds of things.

2:46:14

I think we have a shot

2:46:16

at the supernovae. I forget, actually.

2:46:18

But Lego is sensitive to, you

2:46:20

know, relatively quick gravitational wave frequencies,

2:46:22

so you need to pack a

2:46:24

lot of matter and energy into

2:46:26

a relatively small region of space

2:46:29

to have it move quickly enough

2:46:31

to emit those frequencies and... you

2:46:33

also need to be heavy enough

2:46:35

to give off gravitational waves that

2:46:37

are detectably strong. So if you

2:46:39

put those two requirements together relatively

2:46:41

quick and therefore small, but also

2:46:43

very, very massive, you're more or

2:46:45

less left with inspiring black holes

2:46:47

and or neutron stars. Ethan Richardson

2:46:49

says in the midst of all

2:46:51

the real-world turmoil and... and horror,

2:46:53

how about a softball I've been

2:46:55

mean to ask since I learned

2:46:57

your cat's names years ago? As

2:46:59

a lifelong Shakespeare fan and one

2:47:01

lucky enough to have had the

2:47:03

opportunity to play Caliban, as a

2:47:05

senior in high school, I'd love

2:47:07

to know more about your own

2:47:09

relationship to his work. Things such

2:47:11

as your favorite plays, quotes, is

2:47:13

he really the goat, the greatest

2:47:15

of all time, and if you

2:47:17

cared a way in, as a

2:47:19

good Bayesian, on why some folks

2:47:21

are so invested in the notion

2:47:23

that he didn't write his plays.

2:47:25

So yeah, Ariel and Caliban, as

2:47:27

many of you know, are named

2:47:29

after characters in The Tempest by

2:47:31

Shakespeare. Puck is also named after

2:47:33

a... character famously in Midsummer Night's

2:47:35

Dream. And yeah, you know, Shakespeare,

2:47:37

is he the greatest of all

2:47:39

time? I think that he has

2:47:41

a better claim than anybody else,

2:47:43

okay? But I would absolutely respect

2:47:45

people for thinking that they like

2:47:47

somebody else different. I don't think

2:47:49

that there is an absolute ranking

2:47:51

of greatness in authors. Shakespeare is

2:47:53

kind of special, I think, kind

2:47:55

of unique in his ability to

2:47:57

write poetic... language that is just

2:47:59

very vivid and imaginative and especially

2:48:02

in coming up with new words.

2:48:04

I once went to a performance

2:48:06

of Hamlet in Washington, D.C. by

2:48:08

a Russian theater troop that specialized

2:48:10

in silent. performances. So they had

2:48:12

a version of Hamlet with no

2:48:14

words. And you know, it was

2:48:16

fine, but a lot of me

2:48:18

is thinking like that's entirely besides

2:48:20

the point. Like Shakespeare is not

2:48:22

celebrated for his plots. That's just

2:48:24

not his strong point. I mean,

2:48:26

they're pretty good. Some of the

2:48:28

plots, they can be heartbreaking in

2:48:30

sections, etc. But really, you're there

2:48:32

for the language. And when you

2:48:34

literally take away the language, I

2:48:36

think that you're probably not... showing

2:48:38

off the plays in the best

2:48:40

light. Favorite plays and so forth.

2:48:42

I like the tempest. I like

2:48:44

some of the classics, Macbeth and

2:48:46

Hamlet and so forth. I find

2:48:48

Othello heartbreaking, too much to really

2:48:50

enjoy. Julia Caesar is one that

2:48:52

I really like. I was exposed

2:48:54

to that relatively early. I like

2:48:56

the dramas more in the comedies.

2:48:58

I think the sort of slapstick

2:49:00

comedy of errors, mistaking twins for

2:49:02

each other kind of Shakespeare loves

2:49:04

in his comedies. or not my

2:49:06

style. So I'm a drama kind

2:49:08

of guy on that. Why are

2:49:10

some folks invested in the notion

2:49:12

he didn't write his plays? Yeah,

2:49:14

people like conspiracies and fun mysteries

2:49:16

and things like that. There's no

2:49:18

good evidence for it. I mean,

2:49:20

maybe there is some argument not...

2:49:22

for Shakespeare not being the author

2:49:24

of his plays, but for why

2:49:26

people are so interested in it,

2:49:28

there is sort of an almost

2:49:30

class-based argument, because Shakespeare was relatively

2:49:32

uneducated. He was somewhat educated, but

2:49:35

he wasn't like super aristocratic hoity-to-hoity,

2:49:37

and there's a certain set of

2:49:39

people who think that he was

2:49:41

so good with language that he

2:49:43

must have been aristocratic in hoity-to-to-dee-so,

2:49:45

so they want to attribute his

2:49:47

plays to some aristocrat. Obviously, I

2:49:49

don't think that's a very compelling.

2:49:51

logical train of thought there. All

2:49:53

right, my voice is going as

2:49:55

you might notice. here so we're

2:49:57

going to reach the end. We're

2:49:59

not quite at the end yet,

2:50:01

but only a few more questions

2:50:03

left. Mark Schoyern says, do you

2:50:05

still have your BMW I3? In

2:50:07

general, has your experience with an

2:50:09

electric car been good? Yeah, we

2:50:11

still have the I3. It's convenient.

2:50:13

It's perfect for our purposes, which

2:50:15

is that we have two cars,

2:50:17

and if we really need to

2:50:19

go a long way, we can

2:50:21

get in the gas-powered car. The

2:50:23

I-3, for those of you who

2:50:25

don't know, is a tiny little

2:50:27

car. It's very, very well-designed, so

2:50:29

that it's actually pretty good space inside,

2:50:31

even though it's tiny on the outside.

2:50:33

It's kind of similar to a mini,

2:50:35

if you know what that looks like.

2:50:37

And it was always meant as a

2:50:39

to totaling around... town car. It was

2:50:41

never meant to take you very far.

2:50:43

It's for commuting and things like that.

2:50:45

So Jennifer, I don't drive very much.

2:50:47

She works from home. I can walk

2:50:49

to work, right? So we don't need

2:50:51

a car to take us very far.

2:50:53

And the I-3 is perfect for getting

2:50:55

around town. It's the car we usually

2:50:58

drive from place to place. and also

2:51:00

they just they had fun like I

2:51:02

don't know I don't know what happened

2:51:04

but the BMW designers when they decided

2:51:06

to enter the electric car game had

2:51:09

fun with it they came out with

2:51:11

two cars the I-3 which is like

2:51:13

this little tiny thing that maneuvers really

2:51:15

great and it's kind of fun to

2:51:18

drive because it's so sporty and and

2:51:20

and interestingly designed from the inside like

2:51:22

our I-3 has a interior design package

2:51:25

that uses carbon fiber and fabric and

2:51:27

metal and everything and it's just very

2:51:29

very interesting compared to the vast

2:51:31

majority of interior car designs. And

2:51:33

then the other one they made was

2:51:36

the I-8, which was like this hyper

2:51:38

sports car kind of thing, which apparently

2:51:40

was very expensive and very difficult to

2:51:42

get in and out of, so I

2:51:44

never have driven one, I don't know.

2:51:47

But then, you know, they canceled both

2:51:49

of those and are now making a

2:51:51

very bland selection of BMW sedans and

2:51:53

crossover SUVs, just like everybody else. So

2:51:56

what can you do? The electric car

2:51:58

experience itself has been wonderful. You know,

2:52:00

you don't need to go to the gas

2:52:02

station. We just charge our car in our

2:52:04

garage every night, so we don't even need

2:52:06

to worry about charging stations or anything like

2:52:08

that, because we're not taking it on road

2:52:11

trips. There's a certain amount of, you know,

2:52:13

it's a relatively new technology compared to internal

2:52:15

combustion engines. So we've had to get the

2:52:17

battery replaced, even though there's less than 20,000

2:52:19

miles on the car. But overall, very, very

2:52:21

happy with that I'm hoping that given how

2:52:23

little we drive it, it, it, it will

2:52:25

last another 20 years, it will last another

2:52:28

20 years, easy. Fonke Town

2:52:30

says in episode 305 of Liliana

2:52:32

Mason you talked about media provocateurs

2:52:34

stroking anger and leveraging status threat

2:52:36

to get people to vote a

2:52:38

certain way. I'd like to know

2:52:40

if you have an opinion about

2:52:42

some of those big-name pundits as

2:52:44

to whether or not they actually

2:52:46

believe what they are saying or

2:52:48

rather driven by ego wanting to

2:52:50

be influential monetary gain or something

2:52:52

else entirely. Well, you know, it's

2:52:54

kind of a vague question because

2:52:56

of course the... category of big-name

2:52:58

pundits covers a lot of ground.

2:53:00

And you know, I think that

2:53:03

I would prefer to not... if

2:53:05

I can avoid it, attribute bad

2:53:07

faith to people whose job is

2:53:09

punditry. You know, like Ezra Klein

2:53:11

is someone who we had on

2:53:13

the podcast, and I think we

2:53:15

had a very interesting discussion of

2:53:17

the origin of polarization, and he's

2:53:19

very big in the pundit game

2:53:21

right now, and sometimes people on

2:53:23

the more or less liberal side

2:53:25

of the ledger who Ezra is

2:53:27

also on that side of the

2:53:29

ledger, but they accuse him of

2:53:31

being too sympathetic to centrism in

2:53:33

various ways. I think that's literally

2:53:35

just who he is. I think

2:53:37

he's always been that way. I

2:53:39

known Ezra for a long time

2:53:42

because he and I joined the

2:53:44

blogosphere near the same time in

2:53:46

the early 2000s, and we both

2:53:48

had relatively small time blogs, but

2:53:50

there weren't that many blogs, so

2:53:52

we read each other. And he

2:53:54

was very young at the time,

2:53:56

obviously, and he just always. was

2:53:58

like that. He's not making it

2:54:00

up to get more clicks or

2:54:02

a better job. anything like that.

2:54:04

He's an institutionalist by nature. He's

2:54:06

a liberal institutionalist, but nevertheless an

2:54:08

institutionalist. And I think that a

2:54:10

lot of people who are big-name

2:54:12

pundits are like that. They're not

2:54:14

really playing a game. They're showing

2:54:16

you who they are. Not everyone.

2:54:18

Of course, some people are entirely

2:54:20

cynical, etc. Believe me. But I

2:54:23

think that your first guess should

2:54:25

be that people are just being

2:54:27

honest. Some people are notoriously inconsistent

2:54:29

or hypocritical, but again, I think

2:54:31

that your first guess should be

2:54:33

is that that's just who they

2:54:35

are. Like, they don't have coherent

2:54:37

thoughts in their brains, and they're

2:54:39

saying one thing one day and

2:54:41

something else the other day, not

2:54:43

because they're especially cynical or for

2:54:45

monetary gain. It's just, at the

2:54:47

moment, they think that's true, right?

2:54:49

You know, that's not true for

2:54:51

everybody. That's not the case for

2:54:53

everybody, but I think that that

2:54:55

should be your first... Your priors

2:54:57

should be large, that that is

2:54:59

what is going on, before we

2:55:02

leap right to associating nefarious purposes

2:55:04

to what people are saying. Bran

2:55:06

Muffin says, could ER equals EPR

2:55:08

be established to the same level

2:55:10

of rigor as ADSCFT? What implications

2:55:12

would such a proof have for

2:55:14

the field? So for those of

2:55:16

you who don't know, ER equals

2:55:18

EPR is an idea that connects

2:55:20

the geometry of space time with

2:55:22

quantum entanglement. And it came out,

2:55:24

it's due to one Maltesana and

2:55:26

Lenny Suskind, and it came out

2:55:28

in the context of ADSCFT, the

2:55:30

boundary bulk correspondence relating holographically field

2:55:32

theory without gravity, to a bulk

2:55:34

theory in one more dimension with

2:55:36

gravity. And so what Maltesina and

2:55:38

Suskind noticed is that... if you

2:55:41

have basically two copies of an

2:55:43

ADSCFT, right? So you have two

2:55:45

CFTs, and both of them could,

2:55:47

depending on the quantum states inside

2:55:49

them, have a bulk anti-decider space

2:55:51

emerge holographically, but if you entangled

2:55:53

the two CFTs. If you entangled

2:55:55

them by a lot, what you

2:55:57

would see is essentially a wormhole

2:55:59

connecting them. That would be the

2:56:01

single emergent geometry. So ER is

2:56:03

Einstein and Rosen. Those are the

2:56:05

folks who first really wrote about

2:56:07

worm holes in the context of

2:56:09

the short-chil solution. This is back

2:56:11

in 1935. And then EPR is

2:56:13

Einstein Fodolski in Rosen. Same guys

2:56:15

plus. Boris Padulski writing about entanglement

2:56:17

in the same year, 1935. So

2:56:20

two papers in the same year

2:56:22

by almost the same authors with

2:56:24

normally nothing to do with each

2:56:26

other, and Malda Saini and Suscan

2:56:28

said, maybe they do have something

2:56:30

to do with each other. Maybe

2:56:32

in a holographic sense, there's some

2:56:34

connection between entanglement and the geometry

2:56:36

of space time in particular wormholes.

2:56:38

And they extrapolated it boldly like

2:56:40

great scientists will do. And they

2:56:42

said, if I just have... two

2:56:44

particles entangled with each other, maybe

2:56:46

there is some sense in which

2:56:48

there is a microscopic non-traversable wormhole

2:56:50

connecting them. That's the ER equals

2:56:52

EPR conjecture. So I really haven't

2:56:54

followed the details of discussion of

2:56:56

ER equals EPR a lot. So

2:56:59

don't trust my impressions, but I'll

2:57:01

give you the impressions that I

2:57:03

have from sort of halfway knowing

2:57:05

about it, which is that it

2:57:07

works really well if you have

2:57:09

a huge amount of entanglement as

2:57:11

in the original construction with, you

2:57:13

know, an entire field theory entangled

2:57:15

with a whole nother field theory

2:57:17

where we understand the ADSCFT wormhole

2:57:19

that would connect them, it's much

2:57:21

less clear what the conjecture even

2:57:23

is when you have just a

2:57:25

tiny amount of entanglement, like one

2:57:27

particle entangled with one other particle.

2:57:29

It's not supposed to be that

2:57:31

there's a wormhole that you could

2:57:33

literally travel through connecting these two

2:57:35

particles, so it's not clear to

2:57:38

me what it does mean. And

2:57:40

there are other people who understand

2:57:42

it much better than I do,

2:57:44

so we should ask them. But

2:57:46

I think that it has led

2:57:48

to people thinking about entanglement and

2:57:50

geometry in interesting ways. Yes, we

2:57:52

would like to have a rigorous,

2:57:54

well, you say, can it be

2:57:56

established? I think it's not even

2:57:58

a matter of establishing, it's a

2:58:00

matter of defining it, of formulating

2:58:02

the conjecture in such a way

2:58:04

that it could even be checked

2:58:06

rigorously. But I don't think that

2:58:08

we have that firm foundation or

2:58:10

are close to it right now.

2:58:12

All right, final question is from

2:58:14

Marie Rosskew, who says, you said

2:58:16

several months ago on Robin Ince's

2:58:19

BBC podcast that looking at the

2:58:21

Milky Way can make you dizzy.

2:58:23

I wonder if you have ever

2:58:25

felt dizzy or anxious or even

2:58:27

depressed out of too much knowledge.

2:58:29

I'm in my 40s and I've

2:58:31

always loved to study. I have

2:58:33

just finished your book The Biggest

2:58:35

Ideas in the Universe, Space Time

2:58:37

and Motion, and jump straight into

2:58:39

the quanta and fields, and I

2:58:41

find it so fascinating. But then

2:58:43

people, like my mom, often tell

2:58:45

me that one day I will

2:58:47

go crazy as a result of

2:58:49

all the knowledge. So, um... Two

2:58:51

things. One is the milky way

2:58:53

making me dizzy is really a

2:58:55

straightforward physical response, not a wow,

2:58:58

the cosmos is so big kind

2:59:00

of response. It's not about thinking,

2:59:02

it's about like I am on

2:59:04

the edge of a giant disc

2:59:06

that is spinning. And I know

2:59:08

intellectually of course that it's spinning

2:59:10

very slowly and I shouldn't be

2:59:12

dizzy, but there you go. You

2:59:14

know, the mind is a mysterious

2:59:16

thing. As to whether or not

2:59:18

you should be dizzy or anxious

2:59:20

about too much knowledge, I am

2:59:22

certainly in no danger of that.

2:59:24

I know nobody on earth who

2:59:26

is in danger of being overly

2:59:28

anxious or depressed by knowing too

2:59:30

many things. I tend to think

2:59:32

that it's mostly the other way

2:59:34

around that people become anxious because

2:59:37

they don't know enough things. The

2:59:39

number, no matter how many things

2:59:41

you learn, the number of things

2:59:43

that you don't know, the things

2:59:45

that you have yet to learn,

2:59:47

is always enormously, enormously greater than

2:59:49

the number of things you know.

2:59:51

So even if you're worried that

2:59:53

someday it is possible to know

2:59:55

too much, I am here to

2:59:57

tell you that day is nowhere

2:59:59

close.

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