Episode Transcript
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0:00
We've heard of all
0:02
the usual stuff. Electrons,
0:04
protons, quarks, neutrinos, and if you're
0:06
a fan of this show then
0:08
you've also heard of some of
0:10
the other rarer particles, you know?
0:13
the wimps, the tachyons, the
0:15
monopoles, the whole family of
0:17
supersymmetric partners, that the the
0:19
electrons, the squarks, and yes. even
0:22
the we know bosons. But
0:25
that's not enough to satisfy
0:27
your curiosity, is it? Like
0:30
a collector of rare and priceless artifacts
0:32
you feel compelled to go just a
0:34
little bit deeper, a little bit. weirder.
0:38
I understand that desire and I am
0:40
here to help. So come over
0:42
here, I've got something to show. you. Five
0:45
of the weirdest, strangest, rarest,
0:47
most hypothetical particles in
0:49
the universe. These particles are
0:51
so rare, we're not
0:53
even sure they even exist.
0:55
And I think you're gonna like them. I
0:58
have to give my usual disclaimer
1:00
whenever I give a list of
1:02
things. These are presented in no
1:04
particular order, so feel free to
1:06
rank them by whatever criteria you
1:08
prefer. you know, interestingness, cheerfulness, propensity
1:10
for potential cheese making in and
1:12
so on. but let's get
1:15
started. Number one is
1:17
the dark photon. Everybody loves
1:19
the photon. know, it gets
1:21
along with so many particles,
1:23
it has infinite range, it
1:25
makes flashlights work, but it
1:27
may not be the only
1:29
kind of photon out there. And
1:31
that's why we think there might be
1:33
the dark photon, which is like the
1:35
regular photon, but dark. So
1:38
the motivation here is what the
1:40
heck is going on with dark
1:42
matter and dark energy. that
1:44
know, learned over the past
1:46
few decades. that visible matter, normal
1:48
matter, something we call baryonic
1:50
matter. know, the stuff of
1:52
protons, neutrons, and electrons with
1:54
all of our complicated forces,
1:56
you know, make. up less
1:58
than 5%. of the total
2:01
energy contents of the universe. We
2:03
know a huge component, dark matter,
2:05
is about 25 % of the
2:07
universe, and this is some invisible
2:10
form of matter that we have
2:12
yet to identify that makes up
2:14
the mass of almost every single
2:16
galaxy and anything larger. And
2:18
then there's Dark Energy, which is
2:20
the name we give to the
2:22
accelerated expansion of the universe, which
2:24
makes up about 70 % of the
2:26
stuff in the universe. and
2:30
I do need to take
2:32
a quick break to mention that
2:34
this show is brought to
2:36
you by BetterHelp and it's 2025,
2:38
we're here and there's a
2:40
whole year waiting for us. One
2:42
way to say it is
2:44
there are 365 blank pages waiting
2:47
to be filled in. That
2:49
kind of void can be scary,
2:51
but let me tell you
2:53
as someone who has researched the
2:55
void in the real universe,
2:57
cosmic voids, that the voids are
2:59
full of potential. This is where
3:01
you can make changes happen. This
3:03
is where things become possible because
3:05
once something happens, once something is
3:07
filled, you remove all possibilities. this
3:09
is, I want you to look
3:11
forward to the year and celebrate
3:13
the possibilities that might come down
3:15
the road and what you can
3:18
create. And I've been able to
3:20
develop this kind of perspective through
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therapy. And I'd like you to
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3:51
Okay, so we've got
3:53
these two giant components to
3:55
the universe and we have
3:57
to ask. The physics. that
4:00
we know about, is which
4:02
is the baryonic physics, the
4:04
light loving physics, is absurdly
4:06
complicated. We have a particle a
4:09
we have multiple forces, we have
4:11
all sorts of interesting interactions, we
4:13
have chemistry, we have the
4:15
whole deal. chemistry, is the
4:17
rest of the rest matter and
4:19
dark energy? Are they big
4:21
and simple and dumb? and simple
4:24
they big big complex
4:26
and rich and interesting?
4:28
Are there additional forces operating between
4:30
and matter and dark energy?
4:32
Are there different species of
4:34
dark matter particles that interact
4:36
with each other? Are there
4:38
new forces of nature that
4:40
only operate in what we
4:42
call the call sector of the
4:44
universe, the the of dark
4:46
matter and dark energy? and What's
4:49
adding a little bit
4:51
of gasoline to this
4:53
speculation? speculation? is that that and
4:55
matter and dark energy are
4:57
weirdly There's a
4:59
lot of dark energy and lot of dark energy,
5:01
and there's a lot of dark matter,
5:03
and there's more dark energy than there
5:06
is dark matter, is dark matter, If
5:08
we look at the span of
5:10
history... throughout evolution, billions of years
5:12
ago, there was there was essentially
5:14
energy. energy and of years from
5:16
now, from the universe will be
5:19
almost completely dark energy. You
5:21
get more dark energy as
5:23
the universe expands. as the universe expands
5:26
live in this extremely
5:28
coincidental time. time where
5:30
dark matter and dark energy just
5:32
happen to be roughly within the
5:35
same order of magnitude ballpark of
5:37
each other. of each other. Or there's
5:39
something fishy going on. There are
5:41
additional forces between dark matter
5:43
and dark energy dark keep them
5:45
on track with each other, that
5:48
make them interact so that
5:50
they always have roughly the same
5:52
amount of energy density in
5:54
the universe. universe. don't know. know,
5:56
but we we are developing
5:58
theoretical models. to explore these these
6:01
options and these theoretical models include
6:03
new forces of nature. ways that there
6:05
are new ways that dark matter
6:07
can interact with itself. There are
6:09
ways that dark matter and dark
6:11
energy can talk to each other
6:13
and so on. each other these forces
6:15
need force carriers, and we call
6:17
those force carriers carriers, photons. photons. Now
6:19
anytime you create a new particle,
6:21
you around around bored one day and
6:23
you're like, you know what, I
6:26
think there should be a new
6:28
particle in the universe. You
6:30
can't just come up with
6:32
a cool name, come up that is
6:34
priority number one. but
6:36
after you come up with a cool name, you need
6:38
to list a cool name you need need to
6:40
list its property you need to list its
6:42
mass it's type, it's charge, how
6:44
does it how does it interact
6:47
with the other particles that
6:49
we know of in the
6:51
universe? And so with the so with
6:53
the dark photon, this isn't
6:55
just one kind of particle, it's
6:57
actually a family of particles
6:59
that have the general characteristic more
7:01
they talk more to the dark
7:03
sector of the universe than
7:05
they do to the light side
7:08
of the universe. But within
7:10
that family, There are a
7:12
broad range of possible masses
7:14
and a broad range of
7:16
possible interactions with normal matter.
7:18
We're not gonna cut it
7:20
off completely. say, okay, maybe the dark
7:22
maybe the dark photon exists and
7:24
it almost always talks to dark
7:26
matter and dark energy. energy. But maybe sometimes
7:28
a a dark photon interacts with
7:30
like a regular photon, or
7:32
you and me, just just rarely. rarely.
7:34
would have seen it by
7:36
now. seen it by maybe it's
7:38
not impossible. And so
7:40
go out we come up with these up
7:42
with these families of particles, and
7:45
then we try experiments to go
7:47
looking for them. when it when
7:49
it comes to the dark if it doesn't
7:51
If it doesn't have mass, if the
7:53
actual dark photon actually exists and
7:55
it doesn't have mass, then we will
7:57
never be able to see it or
7:59
directly. detected. will always be hidden
8:01
in the dark sector of the universe
8:03
and will only ever get circumstantial
8:05
evidence for its existence. if
8:08
it does. have
8:10
mass if it has just a little bit
8:12
of mass. then
8:14
it can interact or
8:16
potentially interact with normal
8:19
matter. It opens up
8:21
some channels. because if it
8:23
does have mass, then the
8:25
dark photon can spontaneously decay
8:27
into other particles. It
8:29
maybe it spontaneously decays dark
8:31
matter, but also maybe it
8:33
spontaneously decays into a positron
8:36
and electron pairs, or it
8:38
converts into a normal photon.
8:40
Yeah, we don't know. We're
8:42
just guessing here. We're just
8:44
creating opportunities for the dark
8:47
photon to be detectable in
8:49
our experiments. And
8:51
we have a wide variety of
8:53
potential experiments where we can go
8:55
hunting for dark photons because once
8:57
you introduce a new particle
8:59
into the universe that has mass
9:01
that can spontaneously decay, that can
9:04
interact with other stuff. You
9:06
start messing with the physics of
9:08
the universe, so So talking particle
9:10
collider experiments. You're gonna get different
9:12
results if dark photons are at
9:14
play. You're gonna get different
9:16
results with Big Bang Nucleosynthesis with
9:18
the production of the first elements
9:20
in the first few minutes of
9:22
the Big Bang because there's an
9:24
extra player playing around, messing up
9:26
with the physics. You're gonna mess
9:28
with cosmic rays. They can also
9:30
mess up the interiors of neutron
9:32
stars. They can change how
9:35
quickly or slowly they lose
9:37
their heat. The most fun
9:39
way, in my opinion, of
9:41
detecting dark photons is through
9:44
something called black hole super
9:46
radiance, which deserves its own
9:48
episode. because there's another cool concept
9:50
behind black hole super radiance, which
9:52
is something called black hole bombs, which
9:54
sounds really fun, but is not
9:56
today's subject. Don't let me get sidetracked,
9:58
but feed. please feel free to
10:01
ask. But the general gist behind
10:03
Super Radiance is that is photons can
10:05
get trapped in orbit around spinning black
10:07
holes and then they get their
10:09
energy boosted and then they just like
10:11
boosted and then they just like blow up.
10:13
If the if photon exists,
10:15
it's nearly impossible to find.
10:17
We've searched in our
10:20
laboratories, in our experiments, in
10:22
astronomical observations, and we've
10:24
found. and we've found nothing. we see
10:26
no no evidence for the existence
10:28
of the of the dark And so
10:30
we've so intense limits on the
10:32
properties it's allowed to have.
10:34
So so we've drew out out this
10:36
broad family of particles with potential
10:38
masses, potential interaction strengths potential interaction
10:40
channels, energy levels where they tend
10:43
to show up and we
10:45
can just start checking it off
10:47
the list. Like, okay, can't
10:49
be that. that can't be that mass, can't
10:51
have that interaction channel, can't have
10:54
that interaction strength, they are
10:56
just moving right down the list
10:58
moving now the possibility of the
11:00
now the existing is very, very
11:02
slim. existing is very very slim If
11:04
it does exist, its ability to
11:06
mix into regular matter must be
11:08
very limited as something like. as
11:10
something like a trillion a trillion even
11:13
lower lower. On On the other hand,
11:15
it may exist only in the dark
11:17
sector and will never be able to
11:19
directly detect it. And we can only
11:21
build circumstantial evidence for it. which
11:23
is an unsavory state of affairs,
11:25
but that's the way it is
11:27
with state rare particles. the way it is
11:29
with these particle today. Our number
11:31
two the today is the
11:33
kervaton. That's right, this is
11:36
not a a Transformers bad guy. a
11:38
It is a real hypothetical particle. I
11:40
don't don't know if that's an
11:42
oxymoron, but here we are. are. So
11:44
let's go back in time. in time
11:46
a bit to explore the
11:48
Kerbitan, because we need to
11:50
talk about inflation. inflation. You know, Your
11:52
inflation is this hypothetical event
11:54
that occurred in the extremely
11:57
early universe where the cosmos
11:59
rapidly in a in a blink
12:01
of an eye it expanded by a
12:03
factor of 10 to the 60 the
12:05
60 in less less than to the minus
12:07
35 35 You know something crazy crazy.
12:10
and inflation... was powered
12:13
by an powered by an
12:15
entity. There was something behind
12:17
inflation. We believe it
12:19
was driven by a by a quantum
12:21
field. This quantum field
12:23
we call the the inflatan, because
12:26
that That sounds convenient. The
12:29
Inflatan drove drove inflation. Now
12:31
what Now what inflation did, it did two
12:33
things. One, it made the universe really, really big.
12:36
and then big. the end
12:38
the end of and this is kind of
12:40
a big deal. kind of a big deal, it
12:42
laid down the seeds of structure
12:44
formation. So what we see
12:46
as galaxies and clusters today
12:48
got their start at the
12:50
end of inflation in that
12:52
very, very early early epoch. Now
12:54
we have have no idea what
12:56
powered inflation, we have no idea
12:59
what the what is. Again, remember,
13:01
remember one is the cool name
13:03
cool then priority number two is
13:05
everything else. everything We don't know what
13:07
the know was. We don't know what
13:09
properties it had. We don't know why
13:11
it kicked into high gear. it In the
13:13
early universe, we don't know why it
13:15
went away and stopped when it did.
13:17
away in fact, the most annoying thing
13:19
about inflation. annoying thing is that it's
13:21
really tricky to get right. get right.
13:23
Because if inflation lasts too long,
13:25
then you end up with
13:27
a cold, frozen frozen wasteland
13:30
of a universe. ends If it
13:32
ends too quickly, then you're
13:34
not able to solve some
13:36
of the problems that inflation
13:38
was designed to solve. solve. And
13:40
so you need to tune inflation
13:42
a little bit to get it to
13:44
behave in the way we expect
13:46
it to behave. behave. And the real
13:49
problem is is that are many natural
13:51
or simple models of inflation
13:53
that do the job. the
13:55
way that behave the way inflation is supposed to
13:57
behave, where it turns on at the right
13:59
time. expands the the universe in
14:01
the right way and then turns off
14:03
at the right time. There are ways to
14:05
build relatively simple models that do not
14:08
require a lot of fine of fine inflation
14:10
just does its thing. just does its thing, we
14:12
have a lot of trouble getting those
14:14
models. that allow allow inflation to
14:16
do its thing without really needing
14:18
to go in and fine and
14:20
sharpen get get these precise values it's just
14:22
it's just like, you if you
14:24
have an with with these generic properties,
14:26
the the universe inflates and you're
14:28
done. you're done. We We have a hard time. reconciling
14:31
those those models? what with
14:34
what inflation needs to do
14:36
at the very end, which the seeds
14:38
of lay down the seeds of
14:40
structure. frustrating is frustrating because we would
14:42
like everything to just line up
14:44
and be nice nice you have a
14:46
simple generic model. model that
14:48
there is is some quantum field. and
14:51
through its very nature of existence,
14:53
you know, the properties it's supposed
14:55
to have. to just drives
14:57
inflation, expands the universe, and then lays
14:59
down the seeds at the end.
15:02
It seems like we can't have both.
15:04
we can't have both. So the inflation
15:06
wasn't alone. Maybe the the wasn't the
15:08
only thing out there in the
15:10
early universe. Maybe there was something
15:12
else, the there was something else, is a
15:14
companion to the to the And
15:16
the idea here is that
15:18
here is that during while the Inflaton
15:20
is powering the accelerated expansion
15:22
of the universe, of the
15:24
universe, the kervaton out. just
15:27
hanging out. grab an a soda.
15:29
Then at the at the end, once
15:31
the goes goes away and
15:33
inflation is over, the Curviton
15:35
takes. over the cosmic the
15:37
cosmic scene? space-time a a little,
15:39
lays down the seeds of future
15:41
structures, and and then goes away. away. The
15:43
The advantage of this is that that
15:45
now you have a lot
15:48
more freedom for inflation to be
15:50
natural or simple where
15:52
inflation just naturally arises out of
15:54
the universe the of the fundamental
15:56
properties of quantum fields that you
15:58
that you don't need worry about
16:00
anything else? and you don't you don't
16:02
need the to to do all
16:04
the work of inflating the creating the
16:07
creating the seeds of structure, because
16:09
now you have something else teeing
16:11
over that second job. is that The
16:13
disadvantage is that idea that we have no
16:15
idea how inflation works, and we do
16:17
not even know the identity. to give
16:20
the it's a little cheeky to to introduce
16:22
yet another unknown entity the the cosmos, but
16:24
what are you gonna do? to do?
16:26
Honestly, the Curviton probably doesn't
16:28
exist, but these models are
16:30
still helpful because we are
16:32
trying our best to poke
16:34
and prod at the extremely
16:37
early early It's not like
16:39
we have direct observational evidence of this epoch,
16:41
so we don't have a lot to
16:43
go on, so we just have our models,
16:45
we just have our creative ideas. we just
16:47
have our we explore
16:49
in any viable
16:52
direction, including... including introducing
16:55
new... entities into the early
16:57
universe like the the Kerbiton. Maybe
16:59
we might we might strike upon some...
17:01
Something interesting, maybe we might
17:03
find an interesting combination that
17:05
is testable that is testable lot more
17:07
about how inflation works. inflation works.
17:10
if the if the did exist,
17:12
it doesn't exist it doesn't exist anymore.
17:15
as soon as it did its job
17:17
by design, it has to go away
17:19
and not leave an imprint on the on
17:21
the later because... If it
17:23
did, you you have the Curviton
17:25
lasting minutes or hours or years
17:27
into the Bang, then you're then you're
17:29
gonna mess up Big Bang Nucleosynthesis,
17:31
you're gonna mess up the Cosmic
17:33
Microwave mess up the we don't see any
17:35
evidence of Big Bang Nucleosynthesis of
17:37
Cosmic Microwave Background or anything else
17:39
being messed up and so or anything
17:41
else had to go away, but it still
17:44
had an impact, so that counts. But it still
17:46
had an impact, so that counts. I
17:48
need to take another very brief
17:50
break. break. and mention that this
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plan. our
19:20
number three weird particle
19:22
today. is the
19:24
glue ball. If you
19:26
crack open a proton, you'll find three
19:28
quarks. bound together with
19:30
the strong nuclear force. The
19:33
carrier of the strong nuclear force
19:35
is a particle known as the
19:37
gluon of which there are nine
19:39
varieties. Just for reference,
19:41
the electromagnetic force has only
19:43
one carrier. the photon. And
19:45
the weak nuclear force has three
19:47
carriers. In the
19:49
delightful parlance of nuclear particle
19:52
physics, the quarks have a
19:54
property known as color charge,
19:56
which basically means that they
19:58
can feel the strong nuclear
20:00
force. Particles without color can't feel
20:03
that force, just like electrically
20:05
neutral particles can't feel the
20:07
electromagnetic force. Here's the
20:09
fun thing about the thing those
20:11
carriers of the strong nuclear
20:13
force. strong they have They have
20:15
color charge too. right, you right, you heard
20:17
it here. The carriers of the
20:19
strong nuclear force can feel the
20:22
strong nuclear force. strong nuclear And
20:24
so our best models of the
20:26
proton tell us that they are
20:28
us that hot of of strong force
20:30
interactions you you have quarks exchanging gluons to
20:32
glue themselves together, but then the
20:34
then the themselves feel that same strong
20:36
force and so they interact with
20:38
each other and so on. each
20:40
other and so on. not the only
20:42
the only of strong nuclear -forced
20:44
interactions. The protons are
20:46
made of three quarks with their their
20:49
and so are the neutrons. There's
20:51
this whole other family of
20:53
particles the the which which
20:56
contain just two quarks plus
20:58
all their And in general, the
21:00
general, the strong nuclear force
21:02
is really, really good
21:04
at making large composite particles,
21:06
big with big particles with
21:08
big complicated interactions. got all these So
21:11
we've got all these combinations of
21:13
quarks and with the strong together with the
21:15
strong nuclear force and we give different
21:17
names to these different combinations. but
21:20
if glueons feel the strong
21:22
nuclear force force anyway, why don't
21:24
we just skip the quark part? the quirk
21:26
I mean, why make it so complicated? Just
21:29
keep it simple. And that's how
21:31
we came up with the that's how
21:33
we which is a hefty
21:35
particle, massive composite particle,
21:37
made of nothing more than
21:39
a collection of of nothing more
21:41
than a well, glued together,
21:43
I guess. well, glued We're
21:45
talking guess. We're particle. of a made
21:48
of nothing but... force
21:50
carriers, which which is of of weird
21:52
and also kind of cool. What
21:54
makes the the so elusive is that
21:56
it's incredibly ephemeral.
21:58
It lives less than and then a microsecond,
22:00
which isn't that surprising, you know, know,
22:03
every single combination of quarks and
22:05
and the proton is also unstable
22:07
in isolation. Yes, even the neutron,
22:09
if you take a neutron out
22:11
of a nucleus. take a neutron out of
22:13
a let it free float, it will decay
22:15
in about 15 minutes. decay in But
22:18
the minutes. are expected to
22:20
have exceptionally short lifetimes.
22:22
short lifetimes. would have seen them
22:24
floating around in our around in now and we
22:26
don't so we know they can't live long. live
22:28
long. but that one of the
22:30
challenges with the with the glue that
22:33
the predicted mass of the glue
22:35
ball is in the is in of just just
22:37
about every other composite particle.
22:39
made in particle colliders. So
22:42
So we turn on our particle
22:44
colliders, we make these showers of
22:46
particles. We see all sorts of
22:48
protons and neutrons. We see all
22:50
sorts of we We see more exotic
22:52
ones. we see more exotic ones,
22:54
and the glue ball... is probably sitting
22:56
in there with them. we
22:59
have a but we have a hard
23:01
time telling it apart from the
23:03
other ones. you you just see
23:05
a particle, if if you giant some
23:07
giant experiment and you crack these
23:09
atoms open and you let their
23:11
guts spill out and they start
23:13
transforming into all these showers of
23:15
particles. usually the
23:17
first the first thing you get to the
23:20
the easiest thing to quantify in a
23:22
new experiment is a is a mass. mass.
23:24
You You say, okay, you look at all at all the
23:26
proxy, you say, you say, we've got some particles
23:28
over here with this mass, we've got some
23:31
particles over here with that mass. got some Usually
23:33
you don't get to see the
23:35
other properties. You need more detailed experiments
23:37
to get those other properties. more detailed
23:40
this case... to get those other
23:42
When we run these
23:45
experiments, we see run
23:47
these experiments, We see
23:49
new particles appearing. particles that
23:51
have the right the right mass to
23:53
be a a glue ball. But the
23:55
problem is, these candidate particles, these new
23:57
particles show show up that we've
23:59
never seen before, also masses
24:01
that are compatible with
24:03
with like just new kinds
24:06
of mazons or new kinds or new kinds
24:08
of - other other
24:10
combinations of quarks and
24:12
It's hard to tell hard to tell
24:14
when we see that interesting new particle
24:16
and it shows up on our plot. our If
24:18
it's a glue a glue which
24:21
would be would exciting. exciting, or just
24:23
another which is is kind of
24:25
exciting but not as exciting
24:27
as a a glue ball. So
24:29
nowadays there's a whole experiment
24:31
called called glue is designed to
24:33
find balls not just based on
24:35
their their mass we have a
24:37
bunch of candidates that might
24:39
be glueballs. might be glue balls but
24:41
to verify that what we're
24:43
seeing is actually a glue a glue
24:45
on what it decays into. into
24:48
because a ball when it finally
24:50
disappears and decays into a shower
24:52
of other things. things The the
24:54
products that it creates be
24:57
be different what what a mason
24:59
or baryon Berion creates. only but
25:01
it's only through those Just
25:03
tiny, tiny. one in a million in
25:05
a million differences will be able to
25:07
be able to definitively say that
25:09
a glue ball exists. that's And
25:12
that's hard, we haven't done it
25:14
yet. yet, but reason we are so
25:16
interested in glue in glue that is that
25:18
are the last major undetected prediction
25:20
of the standard model. The The
25:22
standard model of particle physics emerged in
25:24
the emerged in the and
25:26
made all sorts of
25:29
predictions about the nature of
25:31
fundamental particles, the Large
25:33
Hadron Collider was designed to.
25:35
designed to finally determine the last
25:37
predictions of the standard
25:39
model and then also
25:41
hopefully move beyond it. One
25:44
of One of those last major untested
25:46
predictions was the Higgs boson, which we
25:48
found. And then the other one was
25:50
the existence of the of the glue which we
25:52
have yet to find. We have candidates.
25:55
We see some interesting signals, but
25:57
we can't yet determine if
25:59
those were... are glue balls, but but the hunt
26:01
is on. Our number four number four
26:03
particle today is known by the
26:06
cryptic name of which like
26:08
a secret which sounds like a
26:10
secret military base, but yet it's just cool again
26:12
a cool name for a particle. We've
26:14
been trying to move past the standard model
26:16
of particle physics. of pretty much as soon
26:18
as we invented it. as soon as
26:20
model is hugely successful, perhaps
26:22
the most successful scientific. perhaps
26:25
the most successful scientific theory
26:27
of all time. all time. Some Some
26:29
predictions by by
26:31
the model are validated to within one
26:34
part in a quadrillion, which
26:36
is indeed pretty impressive. But
26:38
despite that success, or that success
26:40
or because of that success, we've
26:42
been trying to find any crack in
26:44
any flaw in the so that we can that
26:46
we can move We know know the
26:48
standard model is incomplete. There's
26:50
a whole list of things do do not
26:52
understand about particle physics. Please feel free
26:55
to ask about to are the major
26:57
outstanding questions in the standard model. in the
26:59
would be a very, very fun episode. would
27:01
be a very, so we've been trying,
27:03
we've been trying to find a
27:05
flaw trying to find a flaw because we use
27:07
that flaw to learn something
27:09
new about the universe and move
27:11
past it. it. One One of
27:14
the difficulties of this is that
27:16
experiments testing the standard model
27:18
are huge, extremely carefully calibrated, and
27:20
take years of data to
27:22
lead to a result. So So
27:24
is a little slow. slow. But in 2015,
27:26
physicists got a signal that something
27:28
might be wrong with the
27:31
standard model. It was It was at Atomki,
27:33
Hungarian Institute for Nuclear Research. Research.
27:36
and the team had assembled an
27:38
apparatus to search for dark
27:40
photons of all things. things. The
27:42
setup involved firing protons at at lithium-7,
27:44
which then transformed into a
27:46
beryllium -8, then that and then that
27:48
beryllium -8 promptly decayed and produced
27:50
pairs of electrons and positrons. These
27:52
pairs go off -flying at various
27:54
angles, and then you can
27:56
use nuclear physics calculations to predict
27:59
the spread. of those angles.
28:01
And then if you're getting extra
28:03
of these particles compared to where
28:05
you expect them to be at
28:07
various positions, it might be
28:09
because dark photons are getting involved
28:11
that then decay into normal matter
28:13
as they might or might not
28:15
do and just generally mess up
28:17
your experiment. And what do you
28:19
know? The Hungarian team found extra
28:21
electrons and positrons more than they
28:24
expected from theoretical calculations from the
28:26
standard model. To recreate the signal,
28:28
there had to be a new
28:30
particle involved in the process with
28:32
a mass of 17 mega volts,
28:34
which to give you a sense
28:36
of scale is about 34 times. the
28:38
mass of the electron. And
28:40
so, this mysterious new particle got a
28:42
name, X17. In
28:45
the following years, the Hungarian team
28:47
has built up an impressive list
28:49
of accomplishments that all point to
28:51
the reality of this new particle.
28:54
They've calculated the statistical significance of
28:56
the signal and it's up
28:58
above six sigma, where five sigma
29:00
is considered the gold standard
29:02
in particle physics. And here they
29:05
are at even one sigma
29:07
higher. like that the probability
29:09
of this result being due to
29:11
random chances is so incredibly
29:13
small. They've changed up the
29:15
experimental setup, the number of detectors,
29:17
they've played around with their experiment
29:20
and they still see a signal.
29:22
They tried it again with helium
29:24
for a different atomic nucleus and
29:26
they saw the exact same signal.
29:28
They've tried different beam input energies.
29:30
See if that's causing the issue.
29:33
Nope, they still see the signal. And
29:35
they've worked with collaborators around
29:37
the world to build experiments.
29:39
then those experiments also see
29:41
a signal. X17 would
29:43
be huge. If this
29:45
were a real particle, because this
29:47
would be a primo dark matter candidate,
29:50
you're talking about a lightweight particle
29:52
that hardly if ever interacts
29:54
with normal matter, that is the
29:56
definition of dark matter. And so
29:58
this would be huge. But
30:01
But despite all of this, most of
30:03
the most of the mainstream physics community
30:05
has its doubts. its doubts. All the
30:07
independent confirmations
30:10
around around the world have
30:12
some sort of fingerprint from
30:14
the original Hungarian team in in
30:16
them. They participate in
30:18
the collaboration they they go help
30:20
build the detector or they work very
30:23
they work very closely and
30:25
a exchange a lot of
30:27
information as the other group
30:29
builds their experiment. And And
30:31
nobody else outside of the
30:33
Hungarian team has been able
30:35
to reproduce the someone not connected to
30:37
connected to them, not talking
30:39
to them, building their own
30:41
experiment with their own design
30:43
to search for the signal.
30:45
Whenever someone does that, they
30:47
don't see anything. And other
30:49
And other researchers have pointed
30:52
out that and has the exists the
30:54
has the properties that the
30:56
team says it does. it in
30:58
other we should have seen it
31:00
in other history. experiments throughout history. this
31:02
if there's this particle does it does
31:04
this thing, do can't just do that
31:06
one thing in your experiment. It has
31:08
to do that thing throughout the
31:10
entire universe. So like we talked about
31:12
with dark photons dark general. Once
31:14
you you create a new particle, it's
31:17
there throughout the the entire so it should
31:19
be it up neutron stars It should be
31:21
messing up cosmic microwave background. You should
31:23
see it in the large You should see it
31:25
in should have seen it in particle
31:27
experiments from the it in particle There should be
31:29
evidence for it and we don't see
31:31
it anywhere else in the universe see it
31:33
anywhere the Hungarian group has a group
31:36
has a... history of claiming claiming new
31:38
of of particles only for those
31:40
claims to just kind of vanish
31:42
over time so they don't
31:44
exactly have the most reputable track
31:47
record. track record. And are
31:49
some there are plausible explanations
31:51
for the anomaly for to
31:53
the geometry of the detector
31:55
of the it might be
31:57
more efficient at at detecting...
32:00
electrons and positrons at certain angles.
32:02
And so it looks like a
32:04
bump in the signal. It looks
32:06
like you're getting extra. getting extra
32:08
the theoretical calculations, but that's
32:10
only because your detector setup
32:12
is more efficient at that setup
32:14
is more efficient at so it would
32:17
look like a strong signal.
32:19
It It would look like a
32:21
Six Sigma but but it would
32:23
actually be totally bogus because you
32:25
you didn't account systematic uncertainty or systematic
32:28
error in your experiment, which is
32:30
why it's a bad idea
32:32
in general to rely only on
32:34
statistical significance, but that's a
32:36
separate discussion. a separate Given that we don't
32:38
see any new evidence for the particle as
32:41
much as I would like for as to
32:43
exist like for I'm not going to get my hopes up. going
32:45
to get my hopes up yet. And And
32:47
our last particle today, particle
32:49
number five is five, is the
32:51
That's patreon.com slash slash p.m. P
32:53
M S is T E R.
32:55
It is through your contributions
32:57
that this show keeps going.
33:00
I can't thank you enough
33:02
for all of your support.
33:04
I do do appreciate it. just
33:06
kidding. just kidding, it's
33:08
this out. Okay, you've Check this
33:11
out. Okay, you've got your
33:13
fundamental elements like and aluminum. And
33:15
there are so many of them. best we
33:17
the best we could do for a
33:19
hundred years would list and catalog them.
33:22
But then we discovered that the
33:24
fundamental elements weren't so fundamental after all.
33:26
after And actually, all these elements are
33:28
just combinations of three more
33:30
fundamental particles, the the proton, the the
33:32
neutron, and the electron. And so
33:34
this was a massive step forward
33:36
in simplifying the universe. You have
33:38
have the of elements, and then you discover
33:40
that the zoo of of Elm... is
33:43
really just interesting combinations
33:45
of only particles. But then
33:47
in the mid-20th then in the mid
33:49
-20th century, particle colliders started popping
33:51
out ridiculous numbers of particles. And
33:54
like the pion, the cayon, and then we caion, and
33:56
then we actually had to stop giving
33:58
them names and just assign letters to them,
34:00
like the K minus, the D and
34:02
the B. If we're just throwing letters
34:04
out there, that were producing so many
34:06
different kinds of particles. The
34:08
best we could do for decades was list
34:10
and catalog But then we
34:12
discovered that the fundamental particles
34:14
weren't so fundamental after all, and
34:16
they're actually just made of
34:19
combinations of a few fundamental, even
34:21
more fundamental sub -particles, the quarks
34:23
and the electrons. The
34:25
electrons got to stay electrons.
34:27
but the protons and the neutrons and
34:29
the pions and the kons and
34:31
the d's and the b's were all
34:33
just made of quarks. This was
34:35
a massive simplification. We were
34:37
able to reduce the complexity of
34:40
these particles that we were observing
34:42
because we discovered that they were
34:44
really just interesting combinations of. a
34:46
fewer number of sub And
34:50
now? Well, we don't
34:52
have a zoo of elements or a
34:54
zoo of particles, but we have
34:56
a zoo of these fundamental sub -particles.
34:58
We now know that there are six
35:00
quarks. and there are six leptons. The
35:02
electron is just one of those.
35:04
There are also the muon and the
35:06
tau and the three neutrinos. Plus
35:08
there are all the antiparticles, plus there
35:10
are all the force carriers. And
35:13
right now all we can do is
35:15
list and catalog them. So
35:17
maybe. just maybe. The
35:19
fundamental sub -particles, the quarks
35:21
and the leptons. aren't
35:24
so fundamental after all. And
35:26
they're really made of
35:28
even smaller object called prions.
35:31
Not prions as in mad
35:33
cow disease, but pre as
35:35
in pre -quarks, as in before
35:38
-quarks. Prions. The
35:40
idea is that there are only
35:42
a small number of prions. In
35:44
one model, there are just four
35:46
of them called plus, anti -plus
35:48
zero, and anti -zero. and
35:50
that these prions combine in interesting ways to
35:52
make all the varieties of quarks and
35:54
leptons, which then go on to be
35:57
protons and neutrons and atoms, and then
35:59
go on. to be the elements. One
36:01
of the biggest biggest motivations for preons,
36:03
from the fact that this
36:05
general strategy of reduction has
36:07
been working well for quite
36:10
some time, so why stop
36:12
now? so why stop that many
36:14
particles are extremely similar to
36:16
each other, but just differ
36:18
in some tiny way. way like
36:20
the the positron and electron, have
36:22
the exact same mass? mass. the
36:25
The exact same spend, they just differ
36:27
in their charge. their charge. the electron
36:29
and the muon, muon, same charge, exact
36:31
same spin, they just differ in
36:33
the mass, or the up and
36:35
down up and down quarks, they have
36:38
different charges and just
36:40
different masses. when
36:42
you see all these particles. that
36:44
that have but not not quite
36:46
the same properties, it's very
36:48
tempting to suspect that they
36:50
may arise from some other
36:52
interactions. I mean, I mean, theory theory
36:54
has followed a similar logical
36:57
pathway can't we can't just
36:59
throw out the concept altogether. Preons
37:01
have been proposed to explain just
37:03
about every outstanding problem in
37:05
the the model model there are only
37:07
three generations of particles to
37:09
the nature of dark matter, matter,
37:11
but nothing ever quite seems to
37:13
stick, and that's because no
37:15
experiment has given any has given quarks
37:17
and leptons are composite particles,
37:19
so that stinks. so that We try
37:21
as hard as we can to smash
37:23
smash and and apart, but they just keep
37:26
on being themselves. being And then
37:28
there's this massive problem with
37:30
the mass. the mass. Experiments have
37:32
shown that quarks and leptons
37:34
are point to less than
37:36
thousandth the the width of a
37:38
proton. and so so quark which we know
37:40
is which we know is no
37:42
bigger than 1 if it's made the
37:44
width of a proton, or if
37:46
it's made of a those preons of
37:48
prions, those prions have to be
37:50
moving around. to be but they have
37:52
to be moving around an to
37:54
an incredibly small volume. Heisenberg
37:57
uncertainty principle tells us.
37:59
us that it If these particles are
38:01
confined to that small of a of
38:03
a then they they have
38:05
an incredibly high momentum. They
38:07
have to be buzzing around
38:09
in that tiny, tiny little
38:11
box with incredible velocities, with
38:13
incredible energies, with incredible
38:15
mass. with This means means the
38:18
preons have to be so massive
38:20
that they're more massive than the
38:22
quarks and leptons that they supposedly build
38:24
up to be. So in order
38:26
for this to work, there has
38:28
to be some sort of binding
38:31
energy of some sort of interaction
38:33
that cancels out all that mass. seems
38:35
a But that seems a little weird
38:37
and non trying to you're trying to
38:39
build quarks and leptons out of
38:41
preons, but the prions have to
38:43
be more massive than the quarks
38:45
and leptons themselves. So you need
38:48
to introduce some in to interaction, which
38:50
is making this whole point of
38:52
simplification a little too complex. complex. So
38:54
So jury still out on
38:56
There's honestly honestly work in this a
38:58
lot of work in this direction
39:00
I just of the issues I just
39:02
mentioned. people And also to many. their want
39:04
to risk their careers on an idea
39:06
that seems unlikely to pan out. string
39:09
which is unfortunate all the theory has sucked all
39:11
the air out of the particle physics room
39:13
for the past few decades and doesn't have much
39:15
to show for it, but that's a different a
39:17
different show. But like I said, this program
39:19
of reductionism has been working well for
39:21
so long, let's not quit now. now.
39:23
Prions? You all have a y 'all have a place
39:25
in my heart. And And that's it.
39:28
that is my is my list of
39:30
rare particles, but don't particles, but don't
39:32
worry folks, that's only the end
39:34
of this list. five I picked
39:36
five weird particles for today's episode. but
39:39
but there are plenty more out there. out there. have
39:41
to save those oddities. for
39:43
another day. day. Thank you you to
39:45
Lucas L and Jacqueline R R for the
39:47
questions that led to today's episode.
39:50
And thank you to all. to all.
39:52
my patron supporters, that's patreon.com/p.m.
39:54
I would like to thank
39:56
to thank my top contributors this
39:58
month. They are Justin Chris L. Berto M.
40:00
Duncan M. Corey D. Robert Robert
40:02
B. Sam R. R. John Joshua Scott
40:05
M. Rob H. Scott M.
40:07
Lewis M. M. John W.
40:09
Alexis Gilbert M. Jessica M.
40:11
Jules R. Mike M. Jim L.
40:13
R. David S. R. David Heather
40:15
S. Scott H. Steve S. S. Pete
40:17
C. S. Watt, Kuzi Kevin B. Lisa.
40:19
Kevin B. G. G.
40:21
Thank you. Everyone, please keep
40:24
those questions coming.
40:26
That's That's.com or email or
40:28
email a gmail.com. You You
40:30
can also ask through Patreon respond to
40:32
even respond to you on Patreon
40:34
and give you a little teaser
40:36
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40:38
a question. Please keep those questions
40:40
coming, keep the reviews coming that
40:42
really helps the show visibility. And
40:45
I will see you next time for more. time for
40:47
more. knowledge of time and space. time and
40:49
space.
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