Astrum Space - Where Is All the Antimatter in the Universe?
Episode Date: July 27, 2026This compilation is all about one of the biggest mysteries in physics: antimatter. We’ll explore what it is, where it could be hiding in the universe, and reveal what CERN has discovered so far. Why... are antimatter particles bombarding the Earth? Plus: what would happen if an entire meteor made of antimatter collided with us? ▀▀▀▀▀▀Astrum's newsletter has launched! Want to know what's happening in space? Sign up here: https://astrumspace.kit.comA huge thanks to our Patreons who help make these videos possible. Sign-up here: https://bit.ly/4aiJZNF
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Meteors have the power to transform our planet, to wipe out huge swaths of life on Earth in one impact.
But not all are that dramatic.
We are hit by more than 100 tons of small sand-sized particles every day, and they are essentially unnoticeable.
About once a year, a car-sized meteor comes crashing through our atmosphere,
but the resultant, impressive, fiery streak burns up long before.
hitting the ground.
It's only on the scale of millions of years that we are in danger of being hit by meteors
a kilometer or too wide, big enough to do some serious damage.
But we've not seen one of those since the dinosaurs, lucky for us.
But size isn't everything.
In fact, the biggest impacts may not even be from the largest objects.
If one particularly interesting theory is true, some very rare media media.
meteors may be made of something a little more exotic than rock.
Externally, there would be not much to differentiate these rarer meteors.
In the vacuum of space, they would appear exactly the same as any other space rock.
But while regular meteors might create a fiery streak in the sky, these outliers would have impacts that exceed the largest of nuclear bombs.
And those are just the small ones.
a kilometer-sized meteor of this variety hit the Earth, similar in size to the normal
meteor that killed the dinosaurs, we might not have a planet anymore.
That is the power of a meteor made of antimatter.
Could antimatter meteors really exist?
What clues would help us identify them from regular matter meteors?
And how big would they have to be to become a major problem?
I'm Alex McCulligan and you're watching Astrum.
Join me today as we test the scientific theory behind antimatter meteors and explore the odds
of such objects lurking in our solar system.
Antimatter is a funny substance.
The fact that it exists means that we shouldn't be here.
It is almost identical to regular matter with a few key differences.
One is that it has an inverted charge.
Another is that when antimatter meets regular matter, the two annihilate each other completely,
converting almost entirely into energy.
Now in the early universe, it wasn't just matter that was creating.
In theory, an equal amount of antimatter came into being too.
All the matter should have bumped into the antimatter, and everything would have cancelled each other
out. This would have left no universe for us, as there would be nothing to make the universe
out of. It is one of the mysteries of science that this did not happen, and for some reason
a slightly larger amount of matter coalesced into existence than antimatter, perhaps
as small a discrepancy as a billion matter particles to every billion antimatter ones.
Scientists are still trying to figure out why this might have occurred, but the mystery
remains unsolved for now. Perhaps there is some rule at play that we've not yet identified.
Whatever caused it, this imbalance is the reason the universe we see around us is almost entirely
made of regular matter. And the only place we reliably see antimatter is when they make
tiny amounts of it in experiments at CERN and in other particle accelerators. Some hospitals
even have small particle accelerators to create positrons for pet or positron or positron
electron emission tomography scans.
However, just because we don't see it doesn't mean that tiny pockets of antimatter couldn't exist.
When the raw primordial soup, quark, glue-on plasma of the Big Bang began to form into particles,
while overall there would have been more matter than antimatter, in local areas there were fluctuations.
So it's logical that clumps of antimatter could have emerged and dominated as,
gravity pulled them together. After all, if you flip a coin enough times, you'll inevitably end up
with runs where you flip nothing but heads or nothing but tails. If these clumps were large
enough in scale, they wouldn't annihilate away in a burgeoning solar system. Instead, they would
be the solar system, and it would be pockets of matter that would eventually annihilate out,
leaving behind stars and protoplanetary disks made entirely of antimatter.
This seems highly theoretical, but could such solar systems actually exist?
For the most part, an antistar would be visually identical to a regular one,
as antimatter behaves in all the ways you might expect matter to.
It obeys the same laws of gravity, and mostly looks the same,
The only telltale giveaway would be when regular matter interacted with it, such as when
the interstellar winds met the edge of the fledgling solar system, and resulting annihilations
would emit gamma radiation.
And curiously, there are some systems that seem to do this.
Fourteen such gamma-ray emitting star candidates were found in the Milky Way, thanks to the
Fermi Large Area Telescope in 2021.
If these are antistars, and their profiles do match what we would expect out of antistars,
so this is not ruled out, and they're not other objects that emit gamma rays like pulsars
or black holes, then systems made of antimatter with planets and asteroids do exist.
The ratio of antistars to stars would be about 1 in 400,000.
So the stage is set.
anti-star systems could exist, it's not illogical to think that antimatter meteors do too.
And that leads us to the question, what are the chances of them coming to Earth?
The idea of antimatter meteor striking our planet is not a new one.
Even back in 1940, only a decade or so after the discovery of antimatter as a concept,
Russian-American physicist Vladimir Rajansky began to speculate about their existence.
All it would take was for our solar system to have passed one of these antimatter solar systems
at some point in the past.
The sun's gravity would then knock a few outlying antimatter meteors out of their precarious orbits
and into ours.
Antimatter meteors may not have been able to form in our solar system.
Their particles would have been annihilated by interaction with matter far too early for that.
But in space, just an empty vacuum, somewhat devoid of matter, there would be
nothing for them to annihilate with. So there's a chance they could be among us.
And if they were, would we even notice?
Soon after Rajansky, American astronomer Lincoln-Lapaz began to wonder whether any of the
craters on Earth could be attributed to antimatter meteors. So perhaps this is the time to consider
what an antimatter meteor could do if it came in contact with the Earth, so we know what to look out
for. Thankfully, it's not necessarily a simple journey. The first issue such an antimatter meteor
would encounter before reaching Earth would be our atmosphere. To be fair, this is a problem for regular
meteors too. When one of those trades vacuum for air, the speed at which its travelling causes it
to generate incredible friction, causing some or all of the meteor to burn up on the way down,
depending on its starting size, leading to the fiery streak I mentioned at the start.
However, antimatter meteors would have it much worse.
Each particle of atmosphere that the antimatter meteor encountered on the way down
would annihilate a similar amount of the meteor.
So to understand what happens next, we need to turn to Einstein's famous equation,
E equals MC squared.
The meteor's mass, multiplied by the speed of light squared, tells us how much energy
would be released by the meteor on the way down.
Technically, twice that.
As for each particle of the meteor that's annihilating,
a particle of atmosphere is doing so too.
This is potentially a huge amount of energy being released.
Let's do a bit of a thought experiment to work out how much.
While the dividing line between the atmosphere and space is either 100 kilometers up,
if you're talking to Europeans, or 80 kilometers up if you're talking to Americans,
as the two haven't reached a consensus on that point yet,
over 90% of the massive Earth's atmosphere
is actually clumped below 16 kilometers,
clinging to the planet as closely as possible
thanks to the pole of gravity.
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So by working out how much air exists between this line and the Earth's surface, we can get
a rough idea of how much antimatter you'd need to have before an antimatter meteor hits
the ground.
This is a little tricky to calculate, but thanks to a chart released by the International
Standardization Organization, I was able to add up the sum total of the atmosphere at different
elevations between the surface and 20 kilometers high, and found that in a 1 meter by 1 meter
The corridor between space and the surface, you'd have roughly 10,132 kilograms worth of
atmosphere.
A meteor would need to be roughly this large to even hit the surface, assuming it traveled
the most direct route straight down.
Now, antimatter is similar in mass to matter, so we can assume that they would have comparable
compositions too.
Most meteors are made of chondrites, so assuming an average antimatter meteor meteor made of
of the antimatter version of the same stuff, we can put the density of our antimatter meteor
at around 3,400 kilograms per cubic meter. Of course, there's then a balancing act you need
to do. The bigger the meteor, the larger the surface area, and the more air it thus encounters
before it reaches the surface. However, as volume scales up in cubes, while surface area is only
squared, there is a sweet spot you can hit where the amount of air being annihilated by the meteor
would theoretically perfectly match the amount of mass the meteor possesses.
And then we know that any mass of meteor above that would make it through the atmosphere to hit
the ground, using very rough maths.
I found that a 3x3 by 3 by 3 meter meteor or 27 cubic meters work best for this calculation,
which had a mass of 91,800 kilograms or 3,400 kilograms per cubic meter times 27 cubic meters.
This would only encounter 91,191 kilograms worth of air on the way down, meaning 608 kilograms
worth of meteor would actually hit the surface.
That's approximately the mass of a large gram piano.
How much damage could 600 kilograms of antimatter actually do?
It's time for our equation, E equals mc squared.
Using this calculation, we learn that 600 kilograms of matter.
remaining meteor releases 5.4 times 10 to the power 19 joules of energy, or 54 quintillion
jewels.
Then double that, as the ground being annihilated releases that amount too, so 108 quintillion
joules.
For a point of reference, a one megaton nuke gives our 4.18 times 10 to the power 15
joules of energy.
Even if we scaled up to the largest nuke ever detonated, the Tsar bomber, which had a yield
of 50 megatons, we're still only looking at 2.09 times 10 to the power 17 joules, a full
5,000 times weaker than our antimatter ground piano.
And the Tsar's bomber blast was so great, towns within 55 kilometers, like 70, were leveled.
wooden buildings 160 kilometers away were reportedly damaged.
The light from the blast was seen 1,000 kilometers away.
Windows in Norway and Finland were shattered by the explosion.
If just 600 kilograms of our antimatter meteor impacted in the middle of a state like Texas,
the whole state would be destroyed.
The center vaporized, the rest devastated.
This is just the energy.
release from our antimatter meteor annihilating on the ground, not even going into things like
kinetic energy. But even then, it's actually not just the 600 kilograms that hits the ground
we need to worry about. When you consider the rest of that 91,200 kilograms of mass that
was annihilated in the atmosphere, the blast radius becomes a lot bigger. While some of that
energy would travel upwards into space, minimizing the damage below.
Suddenly, you're not just worrying about Texas.
You're worrying about the entirety of the USA.
All that's just from an antimatter meteor that's comparable in size to a car.
We really do not want to get hit by an antimatter meteor.
So what actually are the risks here?
Let's say that an antimatter meteor had got swept up in the Sun's Graemeanor.
gravity well millions to billions of years ago.
Could it now be one of the 40,155 near-Earth asteroids that NASA tracks?
The good news is no.
For one simple reason.
Space isn't actually empty.
While we talk of space being a vacuum, even in space there are trace amounts of dust floating
in the void.
As such, an antimatter asteroid travelling even though.
even through the interstellar medium, would not likely have a survival rate of longer than
around 300 years.
As we last clipped another star 70,000 years ago, Schultz's star, in case you're interested,
it would have to have been an exceptionally lucky antimatter meteor to not only dodge all the
other asteroids in that time, but also to have not encountered enough dust since then that
it would have disintegrated into gamma radiation.
For this same reason, an interstellar antimatter comet coming through our solar system would
be unlikely.
Small ones would burn up before reaching us, and larger masses would be noticeable.
They would emit a steady stream of gamma rays as they travelled, making them detectable
to our telescopes.
No such sparkling asteroids have ever been detected.
So all in all, while it would be devastating to be hit by an antimatter meteor, it is unlikely
that one would survive long enough to reach our planet, assuming they and antimatter stars exist
in the first place. We are probably quite safe. Besides, if antimatter meteors existed,
we might have seen some evidence of them before. Meteor impacts with unusual destructive
capacity, but leaving no traces of the meteor that caused it, we've not seen anything like
that. Have we? In June 1908, a fireball lit up the sky.
in a remote part of Siberia.
The meteor exploded before hitting the ground, its detonation causing massive forest fires,
and sending trees crashing to the ground like bowling pins in an area of destruction
kilometers wide.
Witnesses more than 30 kilometers away reported seeing a flash brighter than the sun,
followed by a roar of thunder.
Due to its remoteness, scientific teams did not arrive at the site until 1927, but even then,
The destruction caused by the blast was easy to see.
Strangely, for an object that caused such destruction,
almost no trace of the meteor was ever found beyond a few micro particles.
But the Tunguska event couldn't have been caused by an antimatter meteor, could it?
Don't worry, we know that it probably wasn't an antimatter meteor,
but there was a lot of debate about the topic in the past, and we couldn't resist.
being a little spooky.
Have a look around you.
Everything you see from the skin of your hands to the screen you're watching this video on
is a different combination of the same three building blocks of matter,
protons, neutrons and electrons.
Now, let's look a little farther, say at Mars or the Andromeda Galaxy
or even halfway across the observable universe.
and still, there is matter made of protons, neutrons and electrons, as far as the eye can see.
At first, this might not sound all that surprising, but for once the mystery here isn't that we've
seen something we can't explain, but rather that we haven't seen something we were expecting,
a universe just as full of antimatter.
I'm Alex McCulligan and you're watching Astrum.
Join me today as we explore the world of antimatter and learn about its interactions with other particles and even with gravity.
By the end of this video, you'll probably agree that antimatter is a bit weird, but you'll also see why some physicists are frustrated that it isn't weird enough.
Let's get one thing out of the way first. Although it might sound like some physicists,
something straight out of science fiction, antimatter is very real.
It forms a critical part of the standard model of particle physics, and particles of
antimatter have been observed in experiments going back nearly a century.
The very first detection of antimatter dates back to a 1932 experiment conducted by Carl D. Anderson
at Caltech, using a cloud chamber immersed in a magnetic field.
When charged particles from outer space, broadly called cosmic rays, intercept the Earth's orbit
and fly through this chamber, the magnetic field curves their paths according to the charge
and mass of each particle, and the clouds show a visible imprint of their resulting trajectories.
Anderson was hoping this experiment would help determine just what kinds of particles
were streaming into the Earth from the cosmos, and he may have found just a little bit more
than he bargained for.
What Anderson saw was that these cosmic rays included both positively and negatively charged
particles.
The masses of the negatively charged particles lined up exactly with the known mass of an electron,
but some of the positively charged particles were far too light to be protons.
Instead they appeared to have the mass of an electron despite having the opposite charge,
And so these never before-seen particles came to be known as anti-electrons, or later positrons
for short.
In 1936, Anderson would win the Nobel Prize in Physics for this discovery.
Meanwhile, a British physicist, who was also destined to win a Nobel, had been developing
a description of electrons that would fit nicely within the framework of quantum field theory.
His name was Paul Dirac.
By 1928, Dirac had realised that in order to describe electrons as quantum fields in a way that
was physically consistent with special relativity, they had to be part of a larger mathematical
structure, later known as a Dirac spinner, that inevitably gave rise to both positively and
negatively charged versions of the same particle.
In this way, Dirac had predicted the existence of positrons before Anderson had even
even built the cloud chamber that would detect them four years later.
What's even more incredible is that electrons aren't the only fundamental particle to come
in a two-for-one Dirac spinner package.
Other particles matter, like the quarks that make up protons and neutrons, each have
their own anti-quark counterparts.
These anti-quarks can come together to form antiprotons and anti-neutrons, which can then bond
with positrons to form anti-atoms and antimolecules.
You could make a whole planet out of antimatter, and from the outside, it would look quite
similar to an ordinary planet made of ordinary matter.
But if antimatter were too similar to matter, if the only difference were the sign of its charge,
then it would be impossible to explain why our universe contains so much of one and so little
of the other. This cosmic mystery, known as the barionic asymmetry of the universe, sent physicists
on a decades-long quest to try and find as many differences as they could between matter and
antimatter. That quest lives on today, spearheaded by particle colliders at CERN that are capable
of producing, trapping, and studying both positrons and antiprotons. But before we talk about these
experiments, let's try to summarize what we already know about the properties of antimatter.
When studying antiparticles in isolation, experiments have confirmed with ever greater precision
that their intrinsic properties, namely their masses, are exactly the same as for ordinary
particles. And when studying how antiparticles are affected by electromagnetic forces,
experiments have again found that they behave the same exact.
exact way as ordinary particles, except with the opposite electric charge, just as Anderson
had observed in his cloud chamber. But electromagnetism is just one of the four fundamental forces
of nature, alongside gravity and the weak and strong nuclear forces. And as physicists began to
better understand the weak force in the 1950s and 60s, they realized that particles and
antiparticles are actually affected by it quite differently.
The first surprise was that ordinary particles could only feel the weak force if they were left-handed,
and antiparticles could only feel it if they were right-handed.
The concept of handedness or chirality is subtle and difficult to conceptualize for particles
with mass, but a loose analogy can be drawn with a particle's holisticity, which describes whether a
particle is spin up or spin down along its direction of motion. In this analogy, a spin-up
particle is called right-handed, while a spin-down particle is called left-handed.
The second, and even crazier surprise, was that right-handed antiparticles experienced
a different strength of the weak force, as compared to left-handed ordinary particles.
In practice, this means that the quantum probabilities for radioactive
decay in ordinary nuclei are somewhat different from the probabilities of the analogous decay processes
in antinuclei. This fundamental asymmetry between particles and antiparticles was first observed
in a 1963 experiment run by James Cronin and Val Fitch of Princeton University, who would be awarded
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When this asymmetry was discovered, there was some
hope that it would explain the barionic asymmetry of the universe. Perhaps these differences
in the weak force were responsible for the abundance of matter and utter lack of antimatter
around us. But the maths didn't quite work out. There simply wasn't enough of a difference
between the strength of the weak force acting on particles versus antiparticles. That was when
physicists began to turn their attention to the strong nuclear force.
Theoretical models predicted that, just like in the weak interaction, there should be some differences
in how left-handed particles and right-handed particles feel the strong force.
But antimatter just keeps surprising us.
Every experiment to date suggests that the strong force treats particles and antiparticles just
the same.
This brings us to the last of the four fundamental forces and the subject of today.
day's ongoing experiments at CERN, gravity. To be honest, suggesting that gravity might
treat matter and antimatter differently is kind of a long shot. Think back to the popular
legend of Galileo tossing stones of different sizes and materials from the Tower of Pisa. They
all fail at the same rate because the gravitational acceleration on Earth is 9.8 meters per second
squared, regardless of which object is falling. Of course, the experiment works even
better in a vacuum chamber, where air resistance is taken out of the equation. Newton expanded
on this idea and showed in the 17th century that your gravitational acceleration anywhere in space
depends only on the mass of the object pulling you and your distance from it, but not on any of your
personal properties, not even your own mass. This famous result, known as the equivalence principle,
is the foundation of Einstein's theory of general relativity, our most accurate and successful
model of gravity to date.
With that in mind, physics is still an experimental science at its core, and we can't
know for sure whether matter and antimatter obey the same laws of gravity unless we check for
ourselves.
The physicists at CERN set out to do just that, motivated not only by the barionic asymmetry
of the universe, but also by a few speculative papers, suggesting that the cosmological
properties of dark matter and dark energy could be more easily explained if antimatter were
to have a negative gravitational charge, or, to put it simply, if antimatter were to fall
up rather than down. There are several ongoing experiments at CERN testing the gravitational
properties of antimatter, including Aegis, G-bar and Alpha.
Today we will focus specifically on a key experiment coming out of the Alpha Group that was
published in the journal Nature this past September.
After decades of assumptions, this experiment has brought us real-world data on the gravitational
acceleration of antimatter on Earth's surface.
But before we show you the results, let's take a moment to appreciate just a moment.
how intricately this experiment was designed in order to isolate and measure the effects of gravity.
The first step in the experiment is to secure a beam of several million positrons per second
emitted from a radioactive isotope of sodium. Most of these positrons end up colliding
with ordinary matter in the experiment, causing miniature explosions in which positrons
and electrons annihilate each other and release a small burst of energy in the form of light.
But a small fraction of the positrons survive as they are guided through the experimental apparatus,
where they are cooled by low-pressure gases and trapped by electric and magnetic fields.
But observing the effects of gravity on these positrons would be nearly impossible.
Their masses are so small that the tiny force of gravity felt by each particle is overshadowed
by even the smallest fluctuations in the surrounding electromagnetic fields.
That's why this collection of positrons is merged with a separate container of antiprotons,
where they bond and form neutral anti-hydrogen atoms that are much less responsive to stray
electromagnetic fields.
And where did the antiprotons come from?
Suffice it to say that they were produced by firing ordinary protons into a block of metal.
Really, really fast.
Yes, physics is awesome like that.
Once the anti-hydrogen atoms are created, they behave like tiny, weak magnets
that can remain trapped by complicated arrangements of external magnetic fields.
Now, this magnetic interaction is weak enough that it no longer overwhelms the gravitational effect,
that we are trying to measure.
The chamber containing these anti-hydrogen atoms is nearly a vacuum.
There are just about 200,000 atoms of ordinary gas per cubic centimetre,
compared to a typical atmospheric density of 20 quintillion atoms per cubic centimeter.
Under these conditions, the trapped anti-hydrogen atoms almost never collide or annihilate
with atoms of ordinary matter.
Instead, they can more or less.
just float around the chamber for minutes or longer.
But as the magnetic fields used to vertically trap the anti-hydrogen atoms are weakened,
this random floating eventually allows the anti-hydrogen atoms
to escape through either the top or the bottom of the chamber,
where they can collide with a wall of apparatus,
annihilate with some ordinary atoms, and release a small burst of light.
In the Alpha experiment, this happens over the course of about 20.
The theory behind the experiment is that if gravity really pulls antimatter downwards,
more of the anti-hydrogen atoms escape through the bottom than the top.
The stronger the gravitational force, the more atoms escape through the bottom.
The simulations the Alpha Team ran showed that under normal gravitational attraction, about
85% of the anti-hydrogen atoms should escape through the bottom, whereas only 20% of the
20% of them would escape through the bottom if gravity pulled antimatter upwards.
If there were no gravitational force at all, the simulation showed a more even distribution of 55%
escape through the bottom, probably only differing from 50% due to asymmetries in the experimental
apparatus itself.
What did the actual experiment find?
Well, roughly 75% of anti-hydrogen atoms escaped through the bottom of the chamber, showing
a clear preference for downward-pulling gravity.
As any thorough scientist would, the Alpha team repeated this experiment to collect a variety
of data points that could tell a more complete story.
They redid the procedure under various levels of magnetic field bias, which applied external
upward or downward magnetic forces on the anti-hydrogen atoms.
On this graph, a bias of minus 1G means that enough magnetic force is applied to counteract
normal gravity, while a bias of plus 1G means that an extra G of magnetic force is applied
to push the anti-hydrogen atoms downward and so on.
The team made predictions through simulations for each bias and for various possible
gravitational interactions which produce the orange, green and purple curves shown here.
As you can see, the experimental data points shown in blue best match the orange curve,
which represents the normal simulation, where gravity pulls antimatter downwards.
But because the data falls just a bit below this curve, the best fit gravitational acceleration
was only 0.75G.
Three quarters of the strength of gravity acting on ordinary matter.
Does this mean that gravity effects matter and antimatter particles differently after all?
Not necessarily.
Let's have a look at the error bars. They indicate that there are two major forces of uncertainty
in the results, including an uncertainty in the applied bias, possible errors in alignment,
and other systematic and statistical uncertainties. When accounting for these uncertainties, the best fit
gravitational acceleration is actually reported as 0.75g plus or minus 0.13G plus or minus 1.6
G. This means that a full 1G of gravitational acceleration is still fairly consistent with
the collected data. Future experiments will be able to determine more precisely how
strongly gravity acts on antimatter, but we can already rule out speculative theories
that rely on antimatter falling up instead of down.
In the end, despite how weird and backwards the world of antimatter is,
it seems that only the weak force actually applies differently to particles and antiparticles.
But explaining the barionic asymmetry of the universe
would require much more drastic differences between the two,
so scientists aren't done looking for them.
Could there be new forces?
and particles that interact even more weirdly with antimatter?
Or would you be willing to accept that having so much more matter than antimatter around us
is a mere coincidence?
In any case, let us know if you've learned something new about antimatter from watching this video
and whether this is a topic you'd like to hear more on.
800 light years away, there's an unseen antimatter factory churning out high-energy positrons.
tiny particles of antimatter that are streaming through the cosmos and colliding with our planet.
For much of history, we didn't know this strange source existed.
Most of the positrons bombarding us went completely undetected,
instead getting absorbed in our planet's atmosphere.
It wasn't until we started looking from beyond the bounds of our planet that we noticed them.
In 2011, NASA's Alpha Magnetic Spectrometer,
A state-of-the-art particle detector some 200 miles up aboard the International Space Station
was switched on.
What did it find?
You guessed it, positrons.
The presence of these subatomic particles was to be expected, but not in the numbers they
were finding.
Such was the sheer volume of positrons being detected that the usual sources like natural radioactive
decay and cosmic rays no longer offered.
a sufficient explanation.
So where were they coming from?
We've only recently been able to trace the culprit of this cosmic antimatter shower, and
it all comes down to another high-energy discovery, a strange gamma-ray haze named Gaminga,
first identified in the 1970s.
What is this mysterious source of gamma radiation?
And what does it have to do?
the unusual abundance of high energy positrons hitting our planet.
I'm Alex McColgan and you're watching Astrum.
Join me today as we tune into the enigmatic frequency of Gominga, whose gamma radiation has
lit up the world of astrophysics for decades.
Up in our night sky, nestled in the Gemini constellation in the northern celestial hemisphere,
there is something peculiar going on.
In 1972, NASA's small astronomy satellite 2, or SAS 2, identified an unknown source of gamma radiation.
But with the technology available at the time, the best it could do was trace its origin to this wider
region of our Milky Way.
So, the radiation's ultimate source remained hidden among the stars for decades.
Nevertheless, it was given a name, Gaminga.
coined in 1976 by Italian physicist Giovanni Binyami, who would dedicate his career to studying
it.
It's a play on words, a combination of Gemini, the region where it's located, and gamma, the type
of radiation it emits.
Gminga is also a pun in Binyami's Milanese dialect, meaning it's not there.
A fitting name for a gamma ray haze with unknown origin.
It wasn't until 1983 when Binyami and his team finally had their big break.
They managed to identify a weak X-ray signal from Gominga using the Einstein X-ray satellite.
This meant, although its exact position remained unknown, they could narrow down their search
area and were getting closer to uncovering Gominga's hiding place.
But it didn't answer the big question, what is it?
astronomers could still only offer vague guesses about the true nature of the source.
That was until 1991 when they had another lucky break.
Two separate missions identified radiation coming from Gominga and they weren't constant signals,
but pulses.
The first of these discoveries was made with a German-built X-ray telescope known as Rosat,
short for Röhtgen satellite, named after the German.
German word for X-rays.
Rosat was the first to identify pulses in the X-ray signal coming from Gominga, and soon after,
they were also confirmed in the gamma-wave lengths by the energetic gamma-ray experiment telescope,
or EGrit, a telescope aboard NASA's Compton Gamma-ray Observatory satellite.
Not only did these complementary observations demonstrate that the X-rays and the gamma rays
were both coming from Gominga, but for the first time.
First time they revealed what Gaminga was.
With a period of 0.237 seconds, flashing as it spins around its axis a little more than
4 hertz or 4 times per second, Gaminga behaved like a pulsar.
A pulsar is a type of neutron star that spins rapidly, emitting beams of radiation
that sweep across space like a cosmic lighthouse.
From across the galaxy, most pulsars appear to flash in radio waves, anywhere from a few times
a minute to as fast as 700 times per second.
And at this point in the early 90s, they were incredibly rare.
You see, before Rosat and Eagret, only two other high-energy gamma-ray pulsars had ever been
identified, the Crab and Vela pulsars.
And Crab and Vela were different to Kaminga in a colour.
couple of key ways. First, in addition to gamma rays, both of these pulsars also produced
radio waves and were therefore visible using radio telescopes. So if Kaminga was a pulsar,
then it would be the first discovery of one that was apparently radio silent, only emitting
enough radiation to be seen in the gamma and x-ray wavelengths.
And second, Krab and Vela were surrounded by their respective nebula.
remnants from when they were created from supernova explosions.
But Gaminga's nebula was conspicuous by its absence.
So why is Gaminga, this powerful source of gamma rays, so good at hiding from our radio
telescopes?
Where is its nebula?
Or could it be a different type of object altogether?
Well, the answer to the first question is, in part, because we have had a new element
been listening properly, due to the limitations of the available technology and due to our
understanding of the radio emissions of such stellar remnants.
You see, while radio pulsars can emit radio waves across a wide bandwidth, from as low
as 17 megahertz to above 87 gigahertz, around half the radio spectrum, not all of these
frequencies travel well through space.
Even though we've known since the 1970s that radio pulsars often peak between 100 to 200
megahertz, where they are intrinsically brightest, things like the interstellar medium,
background sky temperature, and effects from the ionosphere mean that lower frequencies
are dampened as they make their way across space, resulting in very weak signals that
are much more difficult to detect.
Because those radio signals are so weak, most radio telescopes hadn't been looking at.
for them, instead confining themselves to search in for signals between 430 and 1,600
megahertz.
This would have been fine had Gominga behaved as expected for one of its kind.
Since it did not, it took until 1997 for scientists to realize what was happening.
Three independent observations from the Poshina Radio Astronomy Observatory were able to identify
extremely weak pulses from Gominga using a sensitive transit antenna. The faint radio pulses came in
around 100 megahertz, which explains why previous radio searches for Gominga had come up silent.
Turns out, Gominga wasn't truly hiding and had been sending us signals. We just weren't listening
correctly. That same year, a team led by the late astronomer Janusz Gil theorized that another reason
In Gaminga had appeared to be radio silent, maybe its magnetic field.
Models showed that radio waves may be absorbed or refracted within the pulsars magnetosphere,
leaving only weak pulses around 100 megahertz to be detectable.
This would effectively leave it quiet at the higher radio bands than most telescopes used.
Confirminga was a pulsar, and specifically a gamma-ray pulsar, was a big deal.
In fact, 99% of its output is in the gamma range, making it one of the brightest gamma ray
sources in our entire galaxy.
It is, as it turns out, all that's left after a star, several times more massive than our
sun, exploded about 350,000 years ago.
But its relative radio silence and its apparent lack of a nebula weren't the only unusual
things about this pulsar. When Italian astrophysicists, including Bingami, Gominga's namegiver,
compared a series of observations from the European Southern Observatory's 3.6 metre telescope
and new technology telescope, with observations from the Canada-France-Hawaii telescope,
they found that Gominga was moving. Not only that, it was travelling at an unusually high speed
of around 0.2 arc seconds per year.
As a reminder, an arc second is a very small unit of angular measurement,
use when we need more precise measurements than a degree would allow.
Within each arc degree, there are 60 arc minutes,
and within each arc minute are 60 arc seconds.
These arc seconds are a common unit used in astronomy
to talk about the movement of objects across the sky
from our perspective on Earth.
If you were to draw a circle around the orbit of the moon around the Earth,
there would be 360 degrees around that circular path.
So at any given time of day or night,
assuming nothing is blocking your view of the horizon,
you can see about 180 degrees of the sky,
and from the horizon to the zenith, the top of the sky, is 90 degrees.
If you hold out your little finger at arm's length and close one eye,
the tip of your little finger covers about one degree of the sky roughly.
Next time you're outside on a clear night, try this,
and see if your little finger can cover the moon.
It should, because the moon takes up only about half of a degree,
or about 31 arc minutes in the night sky.
Gaminga travelling 0.2 arc seconds across our sky each year
may not sound like a lot,
But from our perspective on Earth, the typical star only moves a few thousands of an arc second
per year. Yet, despite being 800 light years from us, Gaminga will travel 30 arc minutes,
the equivalent to the apparent diameter of the moon across our sky in just over 10,000 years.
In other words, this stellar corpse is racing through the galaxy at nearly 2,000.
110 kilometers per second.
Heading towards the border between the constellations Gemini and Lynx, and at its current
rate of motion, Gaminga will remain in Gemini for another half million years, but it may
need a new name after that.
However, this mysterious pulsar gets stranger still.
It is its vast speed that helps produce another feature that scientists were about to discover.
As it hurtles through space, Gaminga leaves behind two ghostly X-ray tails that streak
three trillion kilometers across the sky.
As I discussed earlier, despite the fact that this fast-moving pulsar is nearly radio silent,
it certainly isn't quiet in the gamma-ray and x-ray wavelengths.
In 1999, Issa's X-ray multi-mirror mission, or X-MMMNooten, was launched to
appear deeper into this X-ray universe, and four years later, a team led by Patrice
Caraveo uncovered these comet-like X-ray trails. Their shape and brightness are partly explained
by the shockwave created by Gominga's motion through space and its rotation as a pulsar,
but they are also revealing of another attribute, Gominga's colossal mass. Measuring only about 20 to 30
kilometers across, Gaminga is extremely dense, containing about as much mass as one and a half
of our suns.
To put that in perspective, if you had a teaspoon of neutron star material, it would weigh about
four billion tons as much as 10,000 Empire State buildings.
As this dense, high mass object races forward through the low density interstellar medium,
0.06 to 0.15 atoms per cubic centimeter, it compresses the interstellar medium and its own embedded
magnetic field by a factor of 4. Meanwhile, the incessant spinning of the neutron star creates
an environment where electrons and their antimatter counterparts, called positrons, can be accelerated
to extreme energies, powerful enough to emit high-energy gamma rays. While most of the
These electrons are seen in the gamma radiation that escapes from the pulsar, some get trapped
and spiral within this enhanced magnetic field.
In these images from a computer model, the tails can be seen streaking along the edges of
Gominga's three-dimensional shockwave, like the wake created by a boat going through water.
Only this boat is more massive than our sun, and the wake is made up of extremely high-energy
x-rays. But the final piece of the Gominga puzzle wasn't discovered until 2005. It's nebula.
Taking the form of a shell of neutral hydrogen gas with a radius of 0.4 parsecs wide, it turned out to be
what we call a pulsar wind nebula. This type of nebula is created from the wind plasma that
emanates from Apulsar's magnetic poles. The plasma made of child
Large particles that can be accelerated to near light speed surrounds the pulsar, creating
a nebula of high energy particles that give off strong X-ray emissions.
With the confirmation that Gominga did have a nebula, its identity as a pulsar could finally
be confirmed.
But Chandra went even further.
In addition to imaging Gominga, Chandra also looked at a second pulsar called B-03.
B55 plus 54, and by comparing the two, astronomers uncovered another possible explanation for
the absence of radio pulses from Gaminga.
On the surface, these pulsars seem quite similar.
They are both about half a million years old, and they spin about four to five times per second.
However, as you know, Gaminga is seen primarily in gamma-ray pulses, with no bright radio emissions.
By contrast, the other pulsar, which I'll refer to as Pulsar B, is not seen in gamma rays,
and instead is one of the brightest known radio pulsars.
How could these two pulsars be so similar, yet so vastly different in how we see them?
The answer may be as simple as how each of these pulsars are oriented relative to our observation
from Earth.
believers believe that these images of Gominga and Pulsar B have revealed their spin axes
and uncovered a reason for why radio and gamma ray pulses may be present or absent on different
pulsars.
Like our own magnetic field around Earth, both of these pulsars have magnetic poles close
to their spin poles.
These poles are where the beams of pulsing radio emissions come from.
You could try to model this if you skewer a little foam ball.
right down the middle. The foam ball is a pulsar, and the radio beams coming from the poles
are represented by the wooden skewer coming out both ends. If you spin the ball around the skewer
like a spin axis, you create an equator around the middle. To illustrate the gamma ray
source along the spin equator, called the torus, you could cut a hole in a paper plate
and squeeze it over the foam ball. Now you've got yourself a disk of gamma rays beaming out
from the equator in every direction.
With Gominga, the edge of the paper plate is pointing towards us, meaning the gamma rays
are heading to Earth.
But for Pulsar B, its relative position to us is at a different angle, as if looking at the
flat surface of the plate.
The gamma rays are moving perpendicular to our line of sight, therefore missing Earth.
Let's look again at the two Chandra images of Gominga on the left, and Pulsar B.
B on the right, along with artist illustrations of what astronomers believe the pulsar wind
nebulas look like for each of these.
In the image of Pulsar B, the long trailing blue tails represent the radio jets emanating
from its poles, and the skewers coming out of both ends.
Only instead of being straight like a wooden skewer, Pulsar B is moving so fast through space
that these jets appear bent backwards, trailing behind as the pulsar moves through space.
Now look at the image of Gominga.
Here, the long twin tails on either side of the image are the radio jets, trailing behind
as it too rushes through space.
But this time, instead of pointing almost directly toward and away from our vantage point
on Earth, these jets appear to be coming off to the sides, not aimed at Earth.
So when astronomers look at Gaminga, they see powerful gamma-ray emissions from the spin equator,
the radio jets point to the sides and remain unseen.
And when they look at Pulsar B, the opposite happens.
The radio jets are pointed almost straight toward our planet, while the gamma-ray source at
the equator is missing Earth.
Sometimes the most simple explanation is the correct one.
And that finally brings us back to the decades-long mystery of an unusual abundance of antimatter
bombarding our planet.
For more than a decade, a particle detector
called the Alpha Magnetic Spectrometer, or AMS 2, has been attached to the International
Space Station, collecting information on antimatter, dark matter, and cosmic ray sources.
As a reminder, cosmic rays are energetic particles, fragments of atoms that travel through
space at nearly the speed of light.
These can be made by the Sun, by supernova explosions, or other cosmic means.
And in 2013, the first results of the AMS2 experiment were announced.
The detector had recorded more than 400,000 positrons, the largest sample of cosmic ray
positron data ever collected, and increasing the world's total cosmic ray positron data
by a hundredfold.
For years, many astronomers and physicists hope that this excess antimatter may be the
byproduct of a dark matter annihilation, offering.
possible clues about this mysterious substance. After all, dark matter could make up around
27% of the cosmos, and yet we still don't know what it is. Like regular matter, dark matter
holds mass and takes up space, but it doesn't seem to absorb, reflect or interact with light,
at least not in a way we can detect. Some theorize that dark matter may be made of yet
unidentified types of particles. Whatever it is, scientists had
high hopes that the overabundance of antimatter being detected aboard the ISS may hold
clues about dark matter's true nature.
Unfortunately, they've been left disappointed.
The more scientists dig into the data, the clearer it's becoming.
The most likely source of these positrons may actually be pulsars.
Astrophysicists had long suspected this, but until 2017, there simply wasn't proof.
It was the high-altitude water Cherenkov gamma-ray observatory that finally added evidence
to this hypothesis.
A small halo of gamma radiation was identified surrounding Gominga with trillions of times more
energy than is visible to our eyes, from 5 to 40 trillion electron volts, the sort of radiation
usually produced by positrons.
This was the first real observational evidence pointing to a pulsar as a potential source.
Pulsars naturally surround themselves with a haze of both electrons and their positron
counterparts as a result of the star's intense magnetic field.
This intense magnetic field pulls particles from the pulsars surface and accelerates them
to near the speed of light.
Scientists think that these accelerated positrons and electrons are then colliding with starlight,
boosting the light to higher energies, which then radiates as the gamma ray halo observed.
But based on the size of the halo that the Hawke team saw, Gominga's positrons would rarely
have the energy required to reach our planet, and so they believed the excess positrons must
have a more exotic source.
That was until stunning new information was uncovered a few years later thanks to a team
led by astrophysicist Matea Di Maro.
Using a decade of gamma-ray data from Gominga, acquired from Fermi's large area telescope,
is able to observe lower energy light than the Hawke gamma ray observatory, the Maro's team
was able to subtract out all other gamma-ray sources to reveal a spectacular glow coming
from Gominga, much, much bigger than what the scientists had ever seen before.
The vast oblong halo of glowing gamma rays at an energy of 10 billion electron volts spanned
20 degrees of the sky. Similar to the area the big dipper constellation occupies.
And that's not all. The glow of gamma radiation is even bigger at lower energies. If we could see
it all with the naked eye, Gaminga's gamma ray glow would dominate our sky, covering an area 40 times
bigger than the full moon. With this new information, astrophysicist found that the size of Gominga's halo
meant that this one pulsar alone could be responsible for as much as 20% of the excess positrons
detected near Earth. From there, it's no stretch to imagine that other pulsars are the most likely
culprit for the remaining antimatter abundance we found. This explanation may not have solved
the mystery of dark matter, but it is certainly a magnificent revelation.
It was Jocelyn Bell Bennell, who discovered the first pulsar in 1967, back when people
thought that those regular signals could be the work of extraterrestrial life.
In the nearly 60 years that have passed since, we have found thousands of pulsars, and our
understanding of these neutron stars has grown with every one.
And since Gominga was identified as only the third known gamma-ray pulsar in 1991, we've now
spotted over 300 thanks to NASA's Ferm emission. But given Gominga's track record of defying
expectations and furthering science, I like to think that this particular pulsar has more secrets
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