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Veritasium
What happens if you drop 0.125 grams of antimatter?
What happens if you drop 0.125 grams of antimatter?
Veritasium
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58:53 · Apr 5, 2026
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There is a prequel to the Da Vinci Code.
0:02
It's called Angels and Demons.
0:04
And in it, terrorists steal 1/8 of a gram of antimatter
0:08
from CERN to try to blow up the Vatican.
0:11
Because the thing is, when antimatter
0:13
and matter meet, they annihilate,
0:16
turning nearly 100% of their combined mass into pure energy.
0:20
This is via E= MC².
0:23
It is the most violent process physics allows. >> Let's go. Oh my god.
0:32
>> Now that was just a novel, but CERN actually is making antimatter
0:37
and we got to visit it.
0:41
>> This is CERN's antimatter factory.
0:43
There's anti-roton going beneath our >> They are under our feet at this time.
0:48
Here, protons are accelerated
0:50
up to the speed of light
0:53
and smashed into an aridium target
0:56
to produce 20 million anti-rotons every minute.
1:01
This is so much bigger than I was thinking. This is crazy.
1:04
Antimatter is the most expensive
1:06
substance in the universe.
1:08
1 billion per >> No way. Go up.
1:11
We are missing zeros
1:13
>> And CERN makes it to do something that seems impossible.
1:16
So, you're making anti-atoms?
1:19
>> CERN made the first anti-hydrogen
1:21
atoms back in 1995,
1:24
but they quickly ran into a problem
1:26
because those anti-atoms only survived for 40 billionth of a second before annihilating,
1:32
which is way too short to do anything useful with it.
1:35
If only they could figure out how to store antimatter,
1:38
then they could study it and try to find ways in which it might
1:41
differ from normal matter.
1:43
They knew that any unexpected
1:45
difference could reveal entirely new physics.
1:48
So, how do you store antimatter
1:50
in a world full of matter?
1:53
Well, that's one of the problems CERN has been obsessing
1:56
over for the last 30 plus years.
1:59
It has allowed them to do some of the most precise
2:02
tests of antimatter to date.
2:04
And they even managed
2:05
to trap antimatter in a box,
2:07
load it onto a truck, and ship it.
2:10
And they are doing all of this to try and solve one of the
2:14
biggest unsolved mysteries in all of physics.
2:18
To understand it, we must go back to a discovery made around 100 years ago.
2:25
Previously on Veritasium, we learned how a strange physicist
2:29
Paul the Rock came up with an equation to unite special relativity with quantum mechanics.
2:34
It worked surprisingly well, but The Rock was stumped by his own equation
2:38
because the solution for an electron at rest was kind of strange.
2:42
There were two possible energies,
2:44
E= MC^2 and E= minus MC^2.
2:49
But how could an electron have negative energy?
2:52
Well, instead of throwing away his negative energy solution,
2:55
The Rock ended up proposing something radical.
2:58
This negative energy solution
3:00
corresponded to an entirely
3:02
new particle unknown to physics at the time.
3:04
It would have the same mass as an electron
3:07
but carry opposite charge.
3:09
It would be an anti-electron or positron.
3:13
Miraculously, a year later, the first posetron
3:16
was observed by accident in nature.
3:19
Over the following decades,
3:20
physicists built on the rock's equation
3:23
to form an entirely
3:24
new framework of quantum mechanics. quantum field theory.
3:29
This didn't just explain why there are antiparticles,
3:32
but it also answered a more fundamental
3:34
question, which is why is every electron
3:37
in the universe exactly the same?
3:40
The answer began to take shape when people figured out that fundamental
3:44
particles aren't just particles
3:46
or waves, but rather excitations
3:48
of a quantum field.
3:50
So you'd have an electron field that permeates all of space.
3:54
And this field can get excited,
3:56
but only in identical
3:57
discrete units, each with the same mass, spin, and charge.
4:02
And that's why every electron is the same.
4:05
They're all excitations of the same field.
4:08
Now, you could have several excitations,
4:10
that would be several electrons,
4:12
and they can move around, too.
4:14
The only requirement is that they can never overlap exactly.
4:18
Of course, there is nothing special about this kind of excitation.
4:22
You could just as well have a mirror opposite.
4:24
In fact, the equations
4:26
that describe this field require
4:28
such excitations to exist.
4:30
They have the same mass and spin
4:33
but with opposite charge.
4:35
This is the idea of an anti-electron
4:38
or It's exactly what that minus sign in the rock's equation was revealing.
4:44
And just like an electron,
4:46
posetrons can move around, too.
4:48
Only posetrons can overlap with electrons.
4:51
But watch what happens when they do.
4:53
Now, I'm simplifying a little here,
4:55
but because they're each other's mirror images,
4:58
the opposite charges cancel each other out.
5:00
The excitations disappear and the field returns back to its ground state.
5:06
But that would predict that the particles just disappear.
5:09
So, how is that possible?
5:11
Where did the mass go?
5:13
Well, the only way this could work is if that mass got converted into
5:17
something else, energy according to E= MC².
5:22
The energy got transferred into a different quantum field, the photon field.
5:27
And that is what we mean by annihilation.
5:30
Now, people realize that most fundamental
5:32
particles could be described
5:34
using the same approach
5:35
where each could be seen as an excitation
5:38
of their very own quantum field.
5:40
Now, this meant two things.
5:42
The first is that most particles
5:44
must have an antiparticle
5:46
twin because they're just mirror excitations
5:48
in the same field.
5:50
There are some exceptions
5:51
though, like the photon and hig boson,
5:54
which are their own antiparticle.
5:56
And the second and more important implication
5:59
is that each antiparticle
6:01
must be exactly equal to a normal particle
6:04
just with the opposite
6:07
But then around the mid1 1960s,
6:09
people realized that there was a big issue with this explanation.
6:13
And it all stemmed from how it fit in with the newly accepted big bang theory.
6:19
In the very first moments
6:21
after the big bang,
6:22
the universe was extremely
6:24
hot and dense and photons had so much energy
6:27
that the reverse process of annihilation happened.
6:30
So two photons could come together and spontaneously
6:32
convert their energy into the mass and kinetic energy of a particle antiparticle pair.
6:38
And so the universe was filled with these pairs continuously
6:41
popping into and out of existence.
6:44
But as the universe continued to expand,
6:47
it cooled and those photons
6:49
lost energy until around 3 seconds after the big bang, they had lost so
6:53
much energy that pair production stopped.
6:57
And this is what troubled physicists
6:59
in the 1960s because they believe that in those initial stages
7:03
an equal amount of matter and antimatter
7:06
should have been created.
7:08
But if an equal amount of matter and antimatter
7:11
were created then every particle
7:14
should have found its antiparticle
7:15
twin and annihilated meaning there should be no stuff around us.
7:20
No matter and no antimatter
7:22
just photons only radiation.
7:26
So this became known as the big bang radiation
7:29
catastrophe because clearly when we look around us
7:34
we see a lot more than just energy.
7:36
The universe is filled with matter.
7:38
But how can that be?
7:40
Why is there now more matter than antimatter in the universe?
7:44
Where did that asymmetry come from?
7:46
Well, that is one of the biggest
7:48
unsolved mysteries in all of physics.
7:52
Initially, some people tried to brush this away and they argued that perhaps
7:57
there is no asymmetry at all.
7:59
>> Maybe we happen to be in a pocket
8:01
that because of blind random chance, some reasonable
8:04
statistical fluctuations where most surrounded by matter and there' be some region that would
8:09
again be like like a Marvel movie, like some mirror universe,
8:12
there would be mo slightly,
8:13
you know, imbalance in the other direction.
8:16
>> Paul the Rock seemed to have favored this approach.
8:18
He argued that there might be entire anti-stars
8:21
and he ended his 1943
8:23
Nobel lecture by saying
8:25
there may be half the stars of each kind.
8:27
The two kinds of stars would both show exactly the same spectra
8:31
and there would be no way of distinguishing
8:33
them by present astronomical methods.
8:36
Physicist Edward Harrison took this one step further,
8:39
saying there should even be entire anti-galaxies.
8:44
And then people realize, well, if that's the case, there'd be regions where these
8:47
boundaries where the two regions would meet, and that should be lighting up the sky.
8:51
Should be tons of matter, antimatter annihilations.
8:54
Should be tons of of very high energy light.
8:57
So, people surfed the sky looking for these hot spots,
9:00
but they didn't find any.
9:02
And so, this possibility was ruled out.
9:05
There really is more matter than antimatter in our universe.
9:08
There really is an asymmetry.
9:10
So the next obvious question
9:12
is well how large is that asymmetry?
9:15
If we go back to around 10 seconds after the big bang we
9:19
can figure it out.
9:21
By this time pair production had long stopped a full 7 seconds ago
9:26
and by now just about every antiparticle
9:28
had annihilated with its particle counterpart
9:31
and turned into photons.
9:33
Now, the universe was filled with just some leftover particles
9:36
like electrons and protons whizzing around at incredible
9:40
speeds and those remnant photons.
9:43
But because these electrons and protons were traveling so fast, they couldn't come together to form atoms.
9:48
So, you had this plasma
9:50
of charged particles and that meant that when photons were going around, they scattered
9:54
off those charged particles.
9:56
So, they couldn't travel very far without interacting with matter.
10:00
That all changed around 380,000
10:03
years after the Big Bang.
10:04
By now, the electrons and protons had slowed down enough to form neutral atoms,
10:08
and photons could only be absorbed by electrons in atoms
10:12
if they had exactly the right energy to move the electron
10:15
up an energy level.
10:17
In practice, this meant that photons
10:19
could now basically travel through space
10:22
Those atoms then went on to form all the stars and galaxies,
10:26
and those photons stuck around, too.
10:29
They've gone on to make up the low-level radiation
10:31
that permeates the entire observable
10:34
universe, the cosmic microwave background or CMB.
10:39
And when we estimate
10:40
the total number of photons
10:42
in that CMB, we find that there are about 10 to the 89.
10:46
And because almost all of those photons
10:48
were originally created during those very first seconds after the big bang,
10:52
that original annihilation, we can infer that there must originally
10:56
have been around 10 to the 89
10:59
particles and Now, we can also estimate how many ordinary matter particles
11:04
like protons and neutrons
11:06
there are in the observable universe today.
11:09
The ones that survived that annihilation.
11:12
And what we find is that there are about 10 to the 80
11:16
So that means that for every billion antimatter
11:18
particles and billion matter particles there were in the early universe
11:22
when they annihilated they did so almost perfectly.
11:26
But there was one
11:27
one out of a billion matter particles that somehow survived.
11:31
And everything we see around us today is a descendant
11:34
of those lucky one in a billion particles.
11:38
Every person, animal, jungle, and ocean,
11:41
every asteroid colliding or galaxy
11:43
spiraling, every single dot of light in the night sky
11:47
is made up of one of those lucky
11:50
one in a billion particles.
11:53
And that brings us to the craziest part because it tells us that there
11:57
must be a difference between matter
11:58
and antimatter and how they evolve according to the laws of physics.
12:03
But it's not just any difference.
12:05
No, it would make sense if they behaved completely different.
12:08
I mean, you would just have different laws of physics governing
12:11
each type of particle
12:12
or it would make sense if they were governed by the exact same laws.
12:16
But in that case, there would be no difference.
12:19
It would be completely symmetric.
12:21
What's really weird here is that the laws are almost
12:24
exactly the same, but with a tiny difference.
12:28
And that doesn't make any sense.
12:30
For the past 70 years, physicists
12:33
have tried to explain where this asymmetry comes from.
12:36
But so far, all attempts have failed.
12:39
And part of the reason this has been so difficult
12:42
is because our laws of physics are full of
12:47
In the mid 1950s,
12:49
there were three symmetries
12:50
all particles were believed to obey.
12:53
Charge, par, and time reversal symmetry.
12:56
Charge symmetry is super simple.
12:58
It just means that if you swap all positive charges
13:01
with negative ones and vice versa,
13:03
then the interactions don't change.
13:06
In other words, there is nothing special about a positive or negative charge.
13:10
Just that one is exactly equal and opposite to the other.
13:14
To understand parity symmetry,
13:16
consider this mirror which creates a sort of parallel universe
13:20
where everything is the same but reflected.
13:23
So my left hand becomes my right hand and vice versa.
13:26
Now take this molecule
13:28
here which is llanine
13:30
an important amino acid we need to make proteins.
13:33
Now that L is in its name because the amine group this NH2
13:36
part over here is on the left but in the mirror you see its
13:40
sister molecule dlanine that NH2
13:43
part is now on the right.
13:45
And if you try to make elanine in a lab you'll find that you'll
13:48
get 50% llanine and 50% dlanine.
13:51
In other words, there is no experiment you could do that determines whether you're
13:55
in our universe or in the mirror universe.
13:59
And the same is true for many left and right-handed molecules.
14:02
If you just try to make them normally in a lab, you'll get 50% of each.
14:07
So, our universe doesn't favor left or right-handedness.
14:11
Lastly, time reversal symmetry means that the laws of physics work the same whether
14:15
time is running forwards or backwards.
14:18
Now, out of all of these, time reversal symmetry
14:21
might feel strange because there are many things that clearly
14:25
don't work backwards in time.
14:27
You can't uncook an egg, unshhatter
14:29
a wine glass, or turn a plant back into a seat.
14:33
But all of these follow from the second law of thermodynamics,
14:36
which describes how many interacting
14:38
particles evolve from less likely states,
14:41
typically more ordered, to more likely states, typically a mess.
14:45
But this is a statistical law.
14:47
It's not a fundamental law of physics.
14:50
If you zoom in to the level of individual particles,
14:53
then every interaction is perfectly reversible.
14:56
You can tell whether these collisions happen forwards
14:58
or backwards in time.
15:00
Now, the combination of all of these symmetries combined is called CPT symmetry.
15:05
And CPT symmetry, it turns out, is kind of a big deal.
15:09
>> What happens if CPT gets broken?
15:12
>> Well, literally cats and dogs start living together. Time flows backwards.
15:14
all kinds of things start uh breaking in our in our description of nature.
15:18
Now, one of the reasons why
15:19
why CPT and the standard model go
15:22
so well together is because it really is built into the very structure of special relativity.
15:28
>> Special relativity is built on one core principle
15:31
which is that the laws of physics are the same for all inertial
15:35
observers and this includes
15:37
any measurement they make of the speed of
15:41
In the 1950s, Julian Schwinger,
15:43
Hardert Lutters, and Wolffrang
15:45
Pi proved that if our universe obeys this principle,
15:48
which we strongly believe it does,
15:50
then it must be CPT symmetric.
15:53
But the reverse is also true.
15:55
If you break CPT
15:56
symmetry, then this core principle also breaks.
16:00
And that's where things get tricky
16:02
because after the Rock united special relativity
16:04
with quantum mechanics, all following quantum theories also incorporated special relativity.
16:10
And so our best theories of reality,
16:12
quantum field theory and the standard model
16:14
are built on that exact same principle.
16:18
So now we have a paradox
16:19
because on the one hand we need a symmetry to explain why we're here.
16:24
But on the other hand, if CPT symmetry
16:26
breaks, it tears down our best theories with it.
16:30
So physicists started off on a hunt for a special kind of asymmetry.
16:34
an asymmetry that could explain that one in a billion discrepancy
16:38
while also maintaining the larger CPT symmetry.
16:42
The first clue that such as
16:44
might exist came in the mid1 1950s.
16:47
Up until then, every interaction that had been studied conserved the individual symmetries
16:52
of CP and T
16:54
and so conserved CPT as a whole.
16:56
But in 1956, theoretical
16:58
physicists Sunung Da and Chen Niny Young
17:01
realized that no one had checked whether parity is conserved in the weak nuclear force.
17:07
So they set out to test whether the universe favored left or
17:11
And to do it, they enlisted the help of one of Lee's colleagues,
17:15
one of the world's best experimentalists,
17:18
Chen Shung Buu, also known as Madame Wu.
17:22
Once the idea of the experiment was pitched to her, then she just went all in. She canceled trips.
17:27
She worked straight over holiday breaks.
17:29
It was really a a all hands-on deck operation
17:32
over a very frenzied few months.
17:34
When Powi learned of the experiment, he said, "I do not believe that the
17:38
Lord is a weak left-hander,
17:40
and I am ready to bet a very high sum that the experiments
17:43
will give symmetric Now, all that was left to do was run the experiment.
17:50
It worked something like this.
17:53
She started with cobalt 60, an isotope of cobalt where the nucleus has an
17:57
intrinsic angular momentum or spin.
18:00
When she applied a strong magnetic field, she forced all the spins to point
18:05
in the same direction.
18:06
But cobalt 60 is also radioactive.
18:09
So every once in a while a neutron inside one of its nuclei
18:13
decays into a proton
18:14
releasing an electron and anti-utrino
18:17
and leaving a nickel 60 atom behind.
18:20
Now the electrons emitted could travel in two directions.
18:24
They could either go in the same direction as the nuclear spin
18:28
or they could go in the opposite way.
18:30
But if spin is clockwise in our universe,
18:33
then it is also clockwise
18:35
when reflected in the mirror.
18:37
Which means it points in the same direction in both universes.
18:40
So the only way the experiment could be the same in our universe and
18:44
the mirror universe is if the electrons were emitted in equal amounts in each direction.
18:50
It should be 50% on each side.
18:53
But what Wu actually found was that around 60%
18:56
of the electrons moved in the opposite
18:58
direction to the nuclear spin,
19:00
which would mean that 60%
19:02
moved in the same direction as the nuclear spin in the mirror universe.
19:06
But that meant that there is an experiment you could do to tell whether
19:10
you're in our universe
19:11
or the mirror universe.
19:13
So it proved that par is not conserved.
19:16
This shocked the physics
19:19
PI upon being informed of the results exclaimed that's total nonsense.
19:24
>> Very smart people Nobel laureates said
19:27
that can't be right. Do it again.
19:30
I don't believe it.
19:30
I you know and and
19:33
in a sense you can see where they're coming from.
19:35
There had been no
19:36
hint as yet that the that that kind of the universe would care whether
19:39
I'm looking at myself
19:41
you know in a mirror or not.
19:43
>> So others repeated the experiment
19:45
and by 1957 there was no further room for doubt.
19:49
God really was a weak
19:53
That same year, Lee and Young won the Nobel Prize in physics for the
19:56
discovery of parity violation,
19:58
but Wu's name was left off.
20:00
Lee and Young acknowledged her during their speech
20:03
and tried to get her nominated for a prize another year.
20:06
But the Nobel Committee never honored her.
20:08
In a way, she was robbed of the Nobel Prize.
20:11
1988 winner Jack Steinberger
20:13
called this the biggest mistake in the Nobel Committee's history.
20:17
But her work had done something important.
20:19
It had cast doubt on the long-held
20:21
belief that charge parity
20:23
and time reversal were fundamental
20:25
symmetries of our universe.
20:28
This made many physicists uncomfortable.
20:30
So they came up with a workaround.
20:33
Maybe it's okay if parity symmetry was broken
20:36
because that's not a fundamental symmetry of nature.
20:38
It's just part of a larger symmetry charge par.
20:42
The idea was that if you reflected
20:45
everything in a mirror and swapped all the particles for their antiparticles,
20:49
then the symmetry would be restored
20:51
and all would be good again.
20:54
But then 7 years later, two physicists
20:56
found that some particles
20:58
also violated the combined charge parity symmetry.
21:02
Now physicists were getting really nervous.
21:04
Two symmetries that they believed were fundamental
21:06
parts of our universe were broken.
21:09
So the next big question on everyone's mind was
21:12
is CPT symmetry also
21:14
going to fail and take down the standard model with it.
21:18
Then in 1973 something seemingly miraculous happened.
21:22
Makot Kobayashi and Toshihida
21:25
Mascawa found a way to explain
21:27
all the observed P and CP violation
21:30
while maintaining CPT symmetry
21:32
and it all fit directly
21:34
within the standard model.
21:36
The only issue is that when it comes to the matter antimatter
21:40
asymmetry, it can only account for an asymmetry
21:42
of 10 to the minus 18,
21:44
which is a billion times less than we need to explain the observed matter antimatter asymmetry.
21:51
So the ingredients are there,
21:53
which is cool cuz we didn't think even the ingredients were there,
21:56
>> but they're not there in a large enough strength.
21:58
You don't have a strong enough rate of CP violation if you just strict
22:03
with stick with strictly the standard model.
22:05
And so are people now getting nervous about CPT?
22:08
>> Not nervous, I'd say excited.
22:09
>> And that's because this means there is likely new physics
22:13
beyond the standard model.
22:14
But to find out what that might be,
22:16
we must study antimatter
22:18
up close to see if there are any ways in which it might be
22:22
different from normal matter.
22:23
Ways that could explain that asymmetry.
22:26
So you know where we're >> Oh. Oh, look. There it is. CERN, baby. Woo!
22:32
CERN is best known for the Large Hadron
22:34
Collider, a 27 km
22:36
underground ring where protons
22:38
are accelerated up to
22:43
the speed of light.
22:44
Beams traveling in opposite directions are smashed together,
22:48
releasing huge amounts of energy.
22:50
It's the closest we get to the high energy conditions of the early universe.
22:55
But at the southern edge of the LHC,
22:57
there is a smaller
22:58
proton accelerator called the proton synretron.
23:02
Protons in this ring are only accelerated
23:04
to 99.93% the speed of light.
23:08
And some of that proton beam is fed out of the ring and ends up here.
23:13
This is CERN's antimatter factory.
23:16
And in here you make anti-rotons. How many?
23:19
>> Uh, usually it's around
23:21
40 million every couple of minutes.
23:23
We are now going to enter
23:25
the facility by actually a technical building which is
23:28
not very interesting to watch.
23:30
>> I find this all interesting to watch.
23:32
>> To make sure we're safe, we always had to carry around these devices.
23:36
So, you've got two
23:38
what are they called? >> Yeah.
23:41
Just to be safe.
23:42
>> These are standard devices
23:44
to measure the amount of
23:46
uh dose of radiation that you get.
23:48
This is a supervised
23:50
radiation environment which means it's it's an environment in which we keep an eye
23:55
onto the amount of radiation we get as radiation workers.
23:58
>> Where are we going now?
23:59
>> So now we are going to
24:01
enter into the main building.
24:04
>> There's antimatter behind this behind this door. >> Yes. Under our feet. >> Oh wow. >> Yeah. We'll see. You'll see.
24:12
>> Please guys, this is
24:15
this is a huge place.
24:19
This is so much bigger than I was This is crazy.
24:26
Well, I feel like I'm a kid in a candy store looking at this.
24:29
>> This place is pretty It's pretty fun, huh?
24:31
The first time you see it.
24:32
>> Yeah, it's so impressive.
24:34
>> Here you see pretty much the scheme of how this facility is working.
24:38
You get protons coming from one of the CERN accelerators,
24:41
the the PS, which smash onto a target.
24:45
The protons are accelerated
24:47
up to around 99.93%
24:49
the speed of light and have energies
24:51
up to 26 ga electron volts.
24:54
They're aimed at a remarkably small target, an iridium
24:57
rod 3 mm in diameter and 55
25:00
mm across which itself is embedded in a graphite
25:04
and then in a titanium alloy structure.
25:07
Iridium was chosen because it's the second densest element on Earth.
25:11
And that means that there are a lot of nuclei
25:14
packed in a small space,
25:16
which increases the odds that the protons will hit something.
25:19
But when one of these protons hits an aridium nucleus,
25:23
it doesn't bounce off like you'd expect in most collisions.
25:26
It is going so fast and has so much energy
25:29
that it penetrates the nucleus
25:31
where it collides directly
25:33
with one of the neutrons or protons.
25:36
And to understand what happens next, we need to look at what's going on inside the proton.
25:42
Because a proton is not a fundamental particle.
25:45
Instead, it is made up of three fundamental
25:47
particles known as quarks.
25:49
Specifically, two up and one down quark.
25:52
Those quarks whiz around close to the speed of light.
25:55
So to keep all those quirks contained,
25:57
traveling at such incredible
25:59
speeds and in such a small space
26:01
requires a very strong force,
26:04
which is why it's called the strong force.
26:07
And it's mediated by particles known as gluons.
26:11
You can think of this force as acting like a rubber band.
26:15
But you can bring this past its breaking point.
26:18
If you keep putting in energy,
26:20
then you can put in so much energy
26:22
that another quark anti-quark
26:23
pair will be created.
26:25
This bond breaking into pair creation
26:28
can happen several times in a row and results in this sort of shower
26:31
of quark anti-quark pairs.
26:34
And a similar thing happens when a proton collides with a neutron or proton
26:38
inside an aridium nucleus.
26:40
Now most of those pairs stay just like that
26:43
pairs and they travel off.
26:45
But occasionally you will get two anti-up
26:48
and one anti-own quark to come close enough
26:51
and they form a new particle
26:53
made of free anti-quarks.
26:55
They form an anti-roton
26:57
and their counterparts will go on to form a
27:01
Now all of this this entire process
27:04
from initial collision to the shower of particles and the formation of the anti-roton
27:09
happened in the span of 10
27:11
to the minus23 seconds.
27:14
That is a 100 billion
27:16
trillionth of a second.
27:17
It is absolutely insane.
27:20
And every time you hit the target, you get trillions of these collisions.
27:24
And out the other side
27:26
comes a chaotic spray of protons,
27:28
anti-roton, and a bunch of other particles
27:31
all traveling at around 96%
27:34
the speed of light.
27:35
Magnets then filter out the anti-rotons
27:37
from the other particles, and they're sent on to the next stage.
27:41
And then we collect these anti-rotons,
27:43
bring them into the ring, the anti-roton
27:46
decelerator ring, which is the one we are staring on top of.
27:49
And then they they circulate in the ID for a while while they get cooled down.
27:53
So the idea here is really
27:55
that we get these antirotons
27:56
every 2 minutes more or less.
27:58
It's about 30 million of them.
28:00
>> How expensive is it antimatter?
28:02
>> Look guys, what is what is value?
28:04
It's a bit difficult to evaluate it, right? For sure.
28:07
It's probably the most expensive
28:08
state of matter we can build on Earth
28:11
>> How about I name some numbers and you tell me if it's cheap or too expensive?
28:16
>> $1 billion per gram. >> No way. >> It's too cheap.
28:20
>> Orders of magnitude too cheap.
28:23
But many orders of >> mag.
28:25
That's what I was thinking.
28:27
$100 billion per gram. >> No way. Go up.
28:31
I think uh probably you miss other three zeros. free zeros. >> I think so. Per gram. Yes. At least.
28:40
>> If you're wondering what you would do with all that money,
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I'd like to thank SoFi
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29:45
And now, back to antimatter.
29:53
There's anti-roton going beneath our >> They are under our feet at this time. Yes, indeed.
29:58
>> And it's not dangerous.
29:59
>> No, no, it's not dangerous.
30:00
There's no risk whatsoever.
30:02
>> Strong electric fields in the decelerator
30:05
slow down the anti-rotons
30:06
from 96% to 10%
30:09
the speed of light.
30:10
But that's still about 100 million kmh.
30:14
To do experiments with them, they need to be slowed down more.
30:19
Initially, this was done in a kind of crazy way.
30:22
The anti-proton beam was fired at a thin plastic foil which annihilated
30:27
99.9% of all the anti-roton.
30:30
But around 0.1% of those anti-rotons
30:33
survived and they came out slow enough to do experiments with them.
30:37
Of course, this was very inefficient.
30:39
And so in 2015
30:41
and 2016, a secondary ring called Elena was installed.
30:45
Elena slows the anti-rotons
30:47
to 1.5% the speed of light.
30:50
A nice slow 16.2
30:52
million kilometers per hour. >> This is running.
30:57
>> You are watching a live anti-roton
31:01
>> Are the anti-rotons going around in these circles? >> Exactly.
31:04
The blue devices are magnets,
31:06
dipole magnets, which by lawren force make the particles turn.
31:10
Then you have the orange ones which are quadruple
31:12
magnets which manage the focusing of this beam.
31:15
They're like lenses for particles.
31:17
It's a pretty pretty thin
31:19
pipe almost that they go for. >> Yeah.
31:21
I mean, you don't need much there, right?
31:23
Because as long as you don't bend the particles, they just want to go straight.
31:26
You need to keep good vacuum in there.
31:28
Very good vacuum in fact.
31:29
Otherwise, they would anhilate.
31:31
>> And how often do you have annihilations
31:33
in this loop >> in here? >> Yeah.
31:35
Because you can't have perfect >> Well, no. No.
31:38
you have a bit of losses but you know the entire process of catching
31:42
I mean from the moment of catching
31:44
to the moment of extraction to the experiments
31:47
I think these days
31:48
we are about 86%
31:50
efficiency they have made it very efficient
31:53
after the anti-roton have been slowed down in Alena
31:56
they are sent onto five different experiments
31:59
each of which is designed to study different properties of antimatter
32:02
to try and find ways in which antimatter
32:05
behaves differently from normal matter
32:08
One of the first experiments that was done which happened before the antimatter
32:12
factory was built was testing whether the mass of a proton and anti-roton are the same.
32:18
But to do that it brings us back to our original problem.
32:22
How do you store antimatter?
32:24
The way they solve this problem is pretty clever.
32:27
They started with a tube which was pumped down to a vacuum.
32:30
A superconducting magnet sits around this tube and it creates a magnetic field that
32:35
confines charged particles to the center.
32:38
At the same time, electrodes
32:40
generate electric fields that function as endcaps,
32:43
preventing the particles from escaping out the ends.
32:46
The whole tube is then cooled down to around 4 kel or -269°.
32:53
This causes almost all the remaining particles to condense
32:56
and freeze, resulting in a vacuum pressure comparable to outer space.
33:01
So now they could fill this tube with something like anti-roton.
33:05
And once inside, those anti-rotons
33:07
have nothing to annihilate with and nowhere to go. They are trapped.
33:13
They had just built a real life antimatter trap.
33:16
The technical term for this is a penning trap after France penning whose work
33:21
inspired the first one.
33:23
Fittingly, the team that did this at CERN was called trap.
33:27
With the anti-roton trapped, they measured the charge to mass ratio of the anti-roton
33:32
and compared it to that of the proton
33:35
and they found it was equal to one part in 10 billion.
33:39
Now, the pinning traps made studying antimatter
33:42
much easier, and so it became a key tool that the other experiments
33:46
at the factory adopted.
33:48
In 2017, the base experiment
33:50
used it to measure the anti-roton's
33:52
magnetic moment, and they found that within their level of accuracy,
33:56
it was equal and opposite
33:58
to that of the proton.
34:00
So, thus far, everything was behaving just as predicted.
34:04
But there is one force that they hadn't directly probed yet. Gravity. gravity.
34:10
Could that be part of the solution?
34:12
>> It very likely will be.
34:13
Ultimately, part of why is because
34:15
gravity does not obey
34:17
the rules of special relativity,
34:20
which means it doesn't have to obey the CPT
34:22
theorem like the SE model does.
34:24
And so, in principle, that's
34:26
um an area within which one could
34:28
more naturally expect larger
34:31
values of violations of C and CP and and so on or even a CPT altogether.
34:36
In fact, back in the 1950s,
34:38
a few physicists entertained the idea of anti-gravity,
34:41
that antimatter would be gravitationally repulsive.
34:44
So, while matter falls down in the Earth's gravitational
34:46
field, antimatter would rise up.
34:49
You had a basketball made of antimatter, that would be easy to test, but
34:52
getting a basketball of antimatter without it blowing up on you is pretty hard.
34:56
So, it's it's not an easy thing to do um gravity experiments on particles.
35:02
You can't just drop an anti-roton
35:04
and see if it falls because anti-rotons
35:06
are negatively charged and the electric force is much stronger than gravity.
35:10
So even small stray electric fields would influence them way more than gravity would.
35:15
So what you need is something neutral.
35:18
What you need is an anti-atom.
35:22
>> So you're making anti-atoms.
35:23
>> How do you make the anti-atom?
35:25
So what we do is
35:27
we we use antipotons
35:29
and basically we merge them
35:33
they become >> Now there are several ways to make antihydrogen
35:38
and different experiments do it in different ways
35:41
but for Gar it all starts here in this bunker.
35:45
>> In this bunker we have a small accelerator.
35:48
So we make our ourselves our
35:50
positrons and then we
35:53
capture them in a trap here.
35:55
They accelerate a beam of electrons up to 99.9%
35:59
the speed of light and then fire those at a tungsten target.
36:03
Now while tungsten itself is electrically
36:05
neutral at the high speed those electrons
36:08
enter the tungsten they get close enough to the nuclei
36:11
that the electron cloud can no longer screen the intense positive charge within.
36:16
Thus, these nuclei create strong electric fields,
36:19
and those fields then yank the electrons around,
36:22
causing them to rapidly decelerate
36:24
as if they've just slammed on the brakes.
36:27
But the thing is, when these electrons
36:29
break, they lose energy by emitting photons.
36:32
The Germans have a great word for this.
36:34
It's called Brealum or breaking radiation.
36:38
This breaking radiation produces a wide range of photons
36:42
ranging from low energy X-rays
36:44
all the way up to nearly 9 mega electron volt gamma rays.
36:49
Now, out of all of these photons,
36:51
it's the gamma rays above roughly
36:53
one mega electron fold that are important
36:56
because when one of these gamma rays passes close to a tungsten nucleus,
37:00
there's a chance that it transfers its momentum to that nucleus and converts all
37:05
its energy into the mass and kinetic energy of an electron posetron pair.
37:10
But unfortunately, this isn't a clean process that just makes electron posetron pairs.
37:16
It produce posetrons but it also produce a lot of photons,
37:19
gamma rays, neutrons and these are
37:22
deadly >> and that particle mass creates two problems.
37:27
The first is that deadly
37:28
radiation >> supposed to be one of the highest
37:31
strongest source of radiation at sun.
37:35
>> This is one of the highest. >> Yes.
37:37
If you enter while it is
37:40
working you die in 10 seconds.
37:42
>> You die in 10 seconds. >> You cannot escape. >> It's terrifying.
37:45
You melt from inside.
37:47
>> You melt from inside.
37:49
You're saying that way too casually.
37:52
>> And the second problem is that what comes out of the tungsten
37:55
isn't a nice uniform beam of posetrons.
37:58
Instead, you get a shower of electrons,
38:01
neutrons, posetrons, and photons
38:03
all mixed together, all traveling at different angles and different
38:08
The first problem is solved by encasing
38:10
the entire setup with massive
38:12
1.2 2 m thick,
38:14
67% concrete, and 33% iron blocks.
38:19
>> And this is enough to shield us. >> because it's photons. >> Yes.
38:25
This is 1,400 tons. >> Okay. Okay.
38:28
I feel a bit better now.
38:29
Is it running now? >> No.
38:31
But even if it runs, we can see just outside and it's okay. >> Okay. So, we're safe.
38:36
You wear >> your badge. Okay.
38:39
So, you would know. >> Yeah.
38:41
But I guess 10 seconds, not >> too late. >> Too late.
38:45
>> Solving the second problem is a little more involved.
38:48
And it's honestly one of the coolest combinations
38:50
of physics and engineering
38:52
I've ever come across. So strap in.
38:55
When the posetrons leave the tungsten target,
38:58
some are traveling at a few%
38:59
the speed of light, while others are traveling at more than 90%
39:03
the speed of light.
39:05
Now, this massive spread makes it very hard to work with.
39:08
So, we need to slow them down to around 0.34%
39:12
the speed of light
39:13
or around 3.7 million km hour.
39:17
The way they do this is kind of crazy
39:20
because they shoot the positrons.
39:22
Remember those are antiparticles
39:24
at a mesh of ultra fine
39:26
20 micrometer diameter tungsten
39:28
wires which of course are made of normal matter.
39:32
When a fast posetron
39:33
enters the tungsten wire,
39:35
it immediately loses energy due to scattering
39:38
off the tungsten atoms.
39:40
And this happens so fast that within around 10 picos seconds,
39:43
that is 10 trillionths
39:45
of a second, the posetron
39:47
has slowed down to match the thermal energy of the tungsten.
39:51
But now the posetron
39:52
is still trapped inside the wire.
39:55
So from here on, through a random walk of collisions and scattering,
39:58
it needs to find its way out.
40:01
And if it bumps into an electron
40:02
or gets stuck in a defect,
40:04
it never makes it out.
40:07
So you might expect almost none of these posetrons
40:09
to make it out and for almost all of them to find an electron and annihilate.
40:15
And you'd be right.
40:16
The efficiency of this process is terrible.
40:19
For every thousand fast posetrons
40:21
entering the mesh, only about one comes out as a usable slow posetron.
40:27
Another problem is that these posetrons
40:29
don't come out as a nice organized beam.
40:32
Instead, they are emitted at all kinds of angles.
40:35
So, we need to find a way to focus them.
40:38
This is done by letting the shower of particles go through a solenoid,
40:42
which is a long coiled wire with a current running through.
40:45
That current creates a magnetic field inside the coil that acts as a magnetic
40:50
lens and focuses the
40:53
This lets us capture many of the posetrons
40:55
emitted at wide angles that would otherwise be lost.
40:59
But right now we still have a mix of posetrons,
41:02
electrons, neutrons, and photons.
41:05
So the next step is to separate these.
41:07
To do this, we use another magnetic field.
41:10
This curves the electrons one way into a beam dump.
41:14
The photons and neutrons
41:15
because they have no electric charge are unaffected.
41:18
So they go straight through and are absorbed by shielding.
41:21
And the posetrons because of their positive charge
41:24
curve the opposite way to electrons
41:27
and they go on to the next stage.
41:30
Now we're left with a beam of just posetrons.
41:33
The only issue is that because of the terrible efficiency
41:36
from slowing down those posetrons,
41:38
each single shot only generates
41:41
around a thousand usable slow posetrons.
41:44
But we need millions
41:45
or even billions of slow posetrons
41:48
for the next stage.
41:49
So the solution is to accumulate
41:51
the posetrons in a particle
41:53
trap where over several minutes it builds up a posetron
41:57
cloud of around 100 million or more posetrons
42:00
which is enough for the next stage.
42:04
I said you merge positrons and antipotons
42:06
but we do even more complicated.
42:07
First we make posetronium.
42:09
Posetronum is >> Posetronium is an electron and a posetron
42:15
orbiting each other like a binary star system.
42:18
It's an exotic form of matter and it only lasts about 110th
42:22
to 142 nonds before the two come together and annihilate.
42:28
The way they make this is by using strong magnetic fields to compress the
42:31
cloud of posetrons and fire it at porous silicon dioxide films.
42:36
When these posetrons enter these films,
42:38
they rip away electrons from their atoms
42:40
and some of those electrons
42:42
then bind with posetrons to form posetronium.
42:45
And then a part of that posetronium
42:47
diffuses out of the films
42:48
into the vacuum of the next stage,
42:50
the interaction chamber where it's time for the final step.
42:55
>> So this is what we prepare this here. >> That's the posetronium. >> that's crazy.
43:02
>> We send antipotons to the posetronum
43:04
where it makes antihydrogen.
43:06
>> Now since posetronium only survives for about
43:09
142 nonds, this needs to be timed perfectly.
43:13
So, if you want to see where we
43:15
we catch the anti-roton.
43:17
>> Yes, I would love to see where you catch the anti-roton.
43:20
I was not expecting to get this close. >> It's right here. >> That's awesome. Okay.
43:27
So, we get the anti-rotons here.
43:30
>> And then what what what happens?
43:32
>> So, it goes there inside this box.
43:35
>> Inside the box, it will meet the
43:38
>> Oh, there meets the posetronium.
43:41
Kind of scared, honestly.
43:43
It It sounds like there's music in here.
43:46
>> As the posetronium enters the interaction chamber, the anti-roton
43:49
beam needs to be fired through at that exact moment.
43:53
When done correctly, around 3 million anti-rotons
43:56
or so pass through the posetronium.
43:58
If all goes well, around one to a few of those anti-rotons
44:02
steal a posetron to create an atom of
44:08
Okay, so we've got posetrons
44:10
coming through here, all the way through here.
44:11
And this is where you capture the
44:13
>> Yes, we accumulate them.
44:14
>> You accumulate them and then you shoot them through there and you make the
44:17
posetronium and then you shoot that into that chamber.
44:21
So it mixes with the anti-roton. >> So cool. It's so cool.
44:26
Right in here is where they make anti-atoms, anti-hydrogen.
44:31
They shoot the anti-rotons
44:33
through and they capture
44:35
they capture those anti-eleronss
44:37
to form anti-hydrogen which then travels through here and then you know it will
44:42
go all the way along there and they do their experiments. It's absolutely insane.
44:47
I feel like I should not be in here
44:49
but it's so cool.
44:51
Now one question I had after learning all of this is why?
44:55
I mean why do this?
44:57
Because the alpha G experiment
44:58
can already make 100 anti-hydrogen
45:01
atoms in 4 hours
45:03
using a much simpler process.
45:05
So why is the Gar team spending years
45:08
to build a particle accelerator,
45:10
a posetronium converter, and a way to shoot the anti-roton
45:14
through this posetronium just to make fewer
45:18
anti-hydrogen atoms in a slower
45:20
and more difficult way.
45:22
Especially when you consider that in 2023,
45:25
Alpha G did its own test to see whether anti-hydrogen
45:29
falls up or down.
45:31
Well, to understand why, we need to understand exactly
45:34
what it is that Alpha G did.
45:36
Their setup works something like this.
45:39
Phosetrons are created by a radioactive
45:41
source, accumulated, and are then injected up and trapped.
45:45
Anti-rotons then come in from Elena
45:47
are accumulated in a trap and then also injected in a trap that sits
45:51
just below the posetrons.
45:54
Next, the two antiparticle
45:55
clouds are gently merged.
45:57
This causes some of the anti-rotons
45:59
to capture a posetron and form anti-hydrogen.
46:03
Now, antihydrogen is neutral,
46:05
which means that the penning trap can no longer hold it.
46:08
So if nothing else was done, the anti-hydrogen
46:10
atoms would form, drift off, and within micros seconds
46:14
annihilate at one of the walls.
46:16
It would all be for nothing.
46:18
And this is exactly what happened with the earliest antihydrogen experiments.
46:22
They couldn't hold on to it.
46:24
Fortunately, there is a way to trap antihydrogen
46:27
because it has a small magnetic moment.
46:30
So a second magnetic trap was engineered
46:32
around the device which could capture the antihydrogen.
46:36
Unfortunately, that trap is pretty weak.
46:38
So, most anti-hydrogen atoms escape and annihilate,
46:42
but a few stay.
46:43
And the idea then is simple.
46:45
Slowly weaken the magnetic field holding them.
46:48
And as the trap gets weaker and weaker,
46:50
anti-atoms start to escape.
46:52
And if gravity pulls antimatter
46:54
down, like normal matter,
46:56
then more atoms should escape through the bottom than through the top.
47:00
So, what did they find?
47:01
Does antimatter fall up or down?
47:04
They found that antimatter falls down.
47:07
So it rules out any exotic theories of anti-gravity.
47:11
They measured the gravitational
47:12
acceleration as 75% of normal gravity
47:16
plus - 13% plus - 16%.
47:19
Which is possibly consistent with normal gravity.
47:22
But of course the error bars are huge.
47:25
And this is also why GBAR is so important
47:28
because their hope is to get the measurement accuracy
47:30
down to 1% and ultimately
47:33
to one in 100,000.
47:35
See, when you're doing a gravity experiment on atoms like this,
47:39
you want those atoms to be as still as possible before you drop them.
47:43
In other words, you want them to be as cold as possible.
47:47
Now, alpha G can get really cold to about 0.5
47:50
Kelvin, which is half a degree above absolute zero.
47:54
But GBAR wants to bring this way down to less than 10 micro Kelvin.
47:58
That is 50,000 times colder.
48:02
The way they plan on doing this is actually not by making antihydrogen
48:06
atoms, but by making an anti-hydrogen
48:09
ion, one anti-proton and two posetrons.
48:13
The hope is that once an anti-hydrogen
48:15
atom has formed, it runs into a second posetronium
48:19
atom and steals another posetron.
48:21
At first, that might seem strange because now we're back to having a charged particle.
48:26
And as we learned, you can just drop a charged particle and measure the
48:30
effects of gravity, but charged particles are actually much easier to trap and cool.
48:35
And we can use that
48:37
because now it can be held in a much stronger electromagnetic trap.
48:41
And once there, you can inject
48:43
ultra cold like 10 ml
48:45
burillium ions that have been laser cooled.
48:48
The anti-hydrogen ion then bounces around and collides with these burillium
48:52
ions slowly transferring its kinetic energy to them and thus cooling down
48:57
and they won't annihilate
48:59
because both particles are positively
49:01
charged so they repel each other.
49:03
Then you keep cooling down the burillium
49:06
ions using more advanced techniques
49:08
until you hit the micro kelvin range
49:11
and this is ultimately how they hope to reach a temperature of around 10 micro kelvin.
49:17
Now with the anti-hydrogen
49:19
ion as still as possible,
49:21
they shoot a laser pulse at it, dislodging
49:23
one of its posetrons
49:25
and resulting in a neutral anti-hydrogen atom.
49:29
And as a result, the electromagnetic
49:31
trap can no longer hold it and so it falls around 20 cm.
49:36
At that temperature and over that distance,
49:39
you can time the fall precisely
49:40
enough to measure the gravitational
49:42
acceleration to about 1%.
49:45
So all of this the particle accelerator
49:48
making the posetronium and then the hard way of cooling it
49:52
all of it is just to watch a single anti-atom
49:54
fall 20 cm because this process is the only known way to make anti-hydrogen
50:00
ions and using those ions is the only way to get antimatter
50:04
cold enough to perform an accurate enough experiment.
50:08
Now they haven't managed to do this yet.
50:11
So far, they've only made anti-hydrogen,
50:13
but if they can manage,
50:15
then it would be the most precise measurement of antimatter
50:18
under gravity, although this is likely still years away.
50:23
Now, one thing that makes this research
50:25
so tricky and also relatively
50:27
slow is that there is only one antimatter
50:30
factory in the world.
50:31
And so, the number of places that can study real antimatter is very limited.
50:36
But that might soon change.
50:38
All thanks to another experiment at the factory.
50:42
The base experiment was built to measure the magnetic moment of the anti-roton.
50:47
If CPT symmetry holds, then it should be exactly equal
50:51
and opposite to that of the proton.
50:53
But they kept running into a problem.
50:55
>> Accelerator is continuously ramping magnetic fields in the background. >> Right?
51:00
Even though these fluctuations
51:01
were tiny, around 20,000
51:03
times weaker than the Earth's magnetic field,
51:05
at the precision Bass was working at, they hit a wall.
51:09
>> The only concept um basically to overcome
51:12
this problem is to move the particles out of the accelerator.
51:16
>> So they built a penning trap with its own power supply,
51:20
its own cooling system, and two storage holds for anti-roton.
51:24
So now they could fill those holes with anti-rotons,
51:27
store them, and carry them to wherever they wanted.
51:30
They just created the world's
51:32
first portable antimatter trap.
51:36
So of course, I asked them a pressing scientific question.
51:40
Are you going to make it look super futuristic?
51:42
Because it it's got to be
51:44
the most badass transport container ever made.
51:48
>> I just have this
51:50
um trap here in my office.
51:52
Maybe I can show it to you.
51:54
>> this is one of these panning traps
51:56
and they are inside the superconducting magnet.
51:59
So the the the heavy part is basically the superconducting magnet.
52:03
But these are these trap electrodes and it works.
52:06
They have cracked the code of storing the most volatile
52:09
substance in the universe.
52:11
Their current record for storing anti-roton is 614 days.
52:16
That is they can store antimatter.
52:18
You know, the stuff that annihilates
52:20
as soon as it touches matter
52:21
for close to two years. That is absurd.
52:25
>> This is this anti-roton
52:26
reservoir trap that stores
52:28
um antirotons for longer than 1 or 2 years. >> That's awesome.
52:33
>> But here's what that means.
52:35
Because if you can store antimatter
52:37
for years in a box and you can put that box on a truck,
52:42
then why not ship it?
52:44
we can start distributing
52:46
anti-rotons to ambitious experiments
52:49
all around the planet and everyone
52:50
who has a good idea
52:52
what we could do with these particles
52:55
will get these particles.
52:56
I'm just imagining this map in my head where you have the big antimatter
53:00
factory and then it's going to be sending
53:02
antimatter all over the world to all the top research >> That's great, right?
53:08
That's a fantastic >> Yes. Yes. Yes.
53:13
And they've already started.
53:14
On the 24th of March 2026,
53:18
a crane lifted an 800 kg
53:20
trap out of the antimatter
53:21
factory and loaded it onto a truck
53:24
which then drove on a 10 km loop around CERN
53:28
and it was filled with 92 anti-rotons.
53:33
So perhaps Angels and Demons wasn't that far off after all.
53:37
In the near future,
53:38
there could be actual boxes of antimatter
53:41
that, at least in theory, could be stolen.
53:44
So, does that also mean that they were right about that 1/8
53:47
of a gram of antimatter?
53:48
Well, we wanted to find out,
53:50
so we tested it.
53:52
I mean, we simulated it.
53:54
>> This is like the most super villain call I've ever got.
53:57
>> I'm really getting into my villain arc here.
54:00
Okay, so let's find
54:03
our poor target, Fatican City.
54:06
We've got an eighth of a gram,
54:08
you know, selected right there. 0.125.
54:10
Who wants to do a >> Three, two, one. Let's go. Let's go.
54:20
>> Okay, so we we've got a few levels of destruction here.
54:23
We've got the fireball.
54:25
This is just all instantly vaporized.
54:27
It's turned into pure plasma, which is insane. >> Oh, St. Peter's Basilica.
54:32
It's got a temperature
54:34
of about 100 million degrees Celsius, which is, you know, pretty chill.
54:39
You can see it released about
54:43
* 10 13 jewels, or I guess about
54:46
22 trillion jewels, which is the equivalent of like
54:52
36% of the Hiroshima blast.
54:55
If we zoom out, this is the area of third degree burn.
54:58
So, your skin gets molten.
55:01
Bro, you're having way too much fun with this.
55:03
>> Can I ask this question?
55:05
Like, do we have a
55:06
an eighth of a gram of antimatter available for this?
55:09
Ask him for a
55:10
>> Can you really steal an eighth of a gram from CERN?
55:13
>> That's a good good question.
55:15
>> Do you know how much antimatter
55:17
you've made in total in this factory?
55:19
>> We make uh in the order of 10 to the 10
55:22
uh protons antirotons per year.
55:25
Now, we can make an estimate.
55:26
This facility is is around since 25 years.
55:30
So let's say this is 10 to the 11 protons.
55:34
A gram would mean
55:36
uh 10 to the 23.
55:39
So we are talking here of
55:42
uh well I'm not very good at man math but it's like
55:45
>> a trillionth of a gram.
55:48
>> That means that to make 1/8 of a gram of antimatter
55:50
the factory would have to run for longer than the age of the universe.
55:55
In fact, if you took all the 10 billion anti-rotons
55:58
they make in a year and annihilated
56:00
them all at once,
56:01
you would produce enough energy to heat 1 milll of water
56:05
by about 1° C.
56:08
>> I'd love to see Croatia
56:10
get just for for size and scale. >> How much? >> You tell me. >> All right.
56:15
10 g of antimatter.
56:17
>> Sure, let's do it. >> Oh my god.
56:22
So, while 10 g of antimatter
56:24
would destroy an entire city, >> bye-bye hometown.
56:28
>> The amounts of antimatter
56:29
they're making at CERN are in no way dangerous.
56:32
Which is also part of the reason we had some fun with this simulation
56:37
because for the fareseeable
56:38
future, it's just not realistic
56:40
to talk about having macroscopic amounts of antimatter. >> Yeah.
56:44
So, if people want to play around with this, we'll put a link in the description.
56:47
Uh yeah, have fun.
56:51
>> Or if you'd rather get some antimatter
56:53
yourself without having to rub CERN,
56:56
then I'll tell you how to get some.
56:58
Just go to your local supermarket
57:00
and buy yourself this some bananas.
57:05
That's because a banana contains trace amounts of the radioactive isotope potassium 40.
57:10
And roughly every 75
57:12
minutes, one of these atoms decays
57:14
and releases a posetron.
57:16
Which means that if you wanted to match the antimatter
57:19
facto's output in terms of antiparticles,
57:21
you would need about a billion bananas.
57:27
Now, that's a lot of bananas,
57:29
and I don't recommend eating that many.
57:31
But the thing is,
57:32
even if you never eat any bananas,
57:35
odds are there are some trace amounts of radioactive
57:38
materials inside of you,
57:40
and some of those will produce antimatter.
57:43
One article estimates that the average human makes around
57:47
180 posetrons per hour.
57:49
And so there truly is no need to be scared of antimatter
57:53
because you have been your own little antimatter factory all along.
58:01
Hey, just a few final things.
58:04
The first thing is I want to give a big shout out to Physics
58:06
Girl who made an amazing video for the antimatter factory years ago.
58:11
And ever since I watched that video, I've always wanted to go.
58:14
So, it's been a huge inspiration
58:16
and I highly recommend you check out that video here.
58:19
The other thing is I want to give a quick shout out to all
58:22
the people at CERN.
58:23
Those who helped us with all the animations,
58:26
those who've hosted us and taken the time to explain their live work and
58:29
everyone else, thank you so much.
58:32
And the third and final thank you is of course, as always, to you.
58:36
Thank you so much for watching and I'm excited to see you at the next one. Anti-Casper. Casper annihilate. >> All right, that's
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