WEBVTT

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It's amazing when you really think about it.

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Everything we see around us, like everything,

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this table, these microphones, even us, you and

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me, is made from the same tiny building blocks,

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protons, neutrons, and electrons. Yeah, it really

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is. And it doesn't stop there. We look out into

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space at planets, stars, even entire galaxies,

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and as far as we can tell, it's the same recipe

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everywhere. You've got these three basic ingredients,

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and they're just arranged in countless ways.

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Countless ways, exactly. But there's a big mystery

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here. You see, for decades, scientists have been

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searching for something else. Something like

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a mirror image of all this familiar matter. We

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call it anti -matter. And it's a really fundamental

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question. Why is the universe so chock full of

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matter like a us. But we haven't seen much of

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this antimatter counterpart. Early on, physics

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seemed to suggest a beautiful symmetry, almost

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like the universe should have been made with

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equal parts of matter and antimatter. It's a

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real head -scratcher. So for this deep dive,

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we're going on a journey into the world of antimatter.

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We'll explore what it is, some of its weirder

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characteristics, and the groundbreaking research

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going on at places like CERN. all in an effort

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to unpack this cosmic imbalance. And just to

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be clear, we're not talking about some science

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fiction fantasy here. No, not at all. Antimatter

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is real. It's a solid part of our best understanding

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of physics, something we've known about for almost

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a century now. That's right. The story really

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takes off in 1932. Carl Anderson was working

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at Caltech using something called a cloud chamber.

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Oh the cloud chamber classic. He was studying

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cosmic rays these incredibly energetic particles

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that are constantly bombarding Earth from space.

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See in a cloud chamber charged particles leave

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a trail and when you put a magnet around it they

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curve. Right like the little bar magnets we used

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to play with. Exactly. The direction of that

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curve tells you if it's a positive or negative

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charge and how much it curves tells you how massive

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the particle is. So Anderson saw particles curving

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one way, electrons negatively charged, no surprise

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there. But then he saw something strange. These

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other particles, positively charged, but way

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too light to be protons. In fact, they had the

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same mass as electrons, but with a positive charge.

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Whoa, like finding a mirror image. A plus instead

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of a minus. Exactly. That's how we first detected

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antimatter. Those anti -electrons we now call

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positrons. A monumental discovery. And he absolutely

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deserved the Nobel Prize he got for it in 36.

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Definitely a Nobel -worthy discovery. But here's

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the kicker. These positrons weren't a complete

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surprise, were they? You're right. A few years

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before, around 1928, Paul Dirac, this brilliant

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physicist, had actually predicted them. He was

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working on a way to describe electrons using

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both quantum mechanics and Einstein's theory

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of special relativity. A tough problem. Trying

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to mesh those two giants. Yeah. And when he did,

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his math showed something wild. There couldn't

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just be one type of electron. The equations only

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worked if there were two. One with a negative

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charge, that's our everyday electron, and another

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with a positive charge, the positron. The math

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forced the positron into existence. Pretty much.

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This mathematical object he found, called the

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Dirac Spiner, basically said, hey, there should

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be a twin particle for every electron, but with

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the opposite charge. He predicted antimatter

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before anyone had ever seen it. Amazing, right?

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It really is and it gets even crazier this twin

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particle idea. This isn't just about electrons

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Absolutely, not there's an antimatter twin for

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every type of particle exactly for every single

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one You've got quarks which make up protons and

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neutrons. Well, they're anti quarks, too They

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team up to make anti protons and anti neutrons

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and you can go even further these antimatter

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building blocks can actually combine To form

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whole anti atoms even anti molecules. Okay mind

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blown So in theory you could have an entire planet

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a star, maybe even a galaxy, all made of antimatter.

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And if you saw it through a telescope, you wouldn't

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be able to tell it was antimatter just from looking.

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Nope, not at all. An antimatter planet, if we

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could observe one from afar, would look, behave,

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and even interact gravitationally, just like

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any other planet we see. Whoa. It just really

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drives home this big question, this fundamental

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asymmetry. If matter and antimatter are so similar,

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why is the universe we see basically just matter?

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That's the million dollar question, isn't it?

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This imbalance, which scientists call the baryonic

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asymmetry of the universe, has been a driving

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force behind research for a long time. And that's

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where places like CERN come in. With their huge

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particle accelerators, they're able to create,

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trap, and study antimatter in ways we never could

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before. Yeah, those guys are pushing the boundaries

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of what we know. So we know it exists, but what

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makes antimatter tick? How does it behave compared

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to the regular stuff? Well, we've studied isolated

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antiparticles, and their fundamental properties,

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like their mass, are identical to their matter

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partners. A positron weighs the same as an electron,

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an antiproton the same as a proton. It's a perfect

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mirror image as far as mass is concerned. But

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what about their behavior? How they interact

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with the forces of nature? Let's start with electromagnetism.

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That's the force responsible for, well, electricity

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and magnetism and how charged particles interact.

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The one we're most familiar with in our daily

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lives. Exactly. Experiments show antiparticles

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act exactly like the theory predicts, just with

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the opposite charge. Remember Anderson's cloud

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chamber. Positrons curving the opposite way to

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electrons. That's the opposite charge in action.

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Right. But there are other forces at play too,

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right? Gravity, the weak nuclear force, the strong

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nuclear force. Is it there where things get a

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bit less symmetrical? You're getting to the heart

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of it. Things get really interesting when we

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look at the weak nuclear force. Back in the 50s

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and 60s, physicists found some surprising differences

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in how it treats particles and antiparticles.

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The first one had to do with a property called

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handedness, or chirality. Handedness. I know

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my right hand from my left, but for tiny particles.

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Yeah, it's a bit abstract. Think of it like this.

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Ordinary particles, the matter kind, only feel

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the weak force if they have a specific orientation,

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like a left -handed spin, if you will. And antiparticles

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only interact if they're right -handed. So it's

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like the weak force is a bit picky. Yeah, you

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could say that. It only shakes hands with certain

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particles, depending on their handedness. That's

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wild, but it gets even weirder, right? It's not

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just that it interacts, but the strength of the

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interaction is different, too. You got it. The

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second, even more surprising finding was that

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this difference in handedness also meant a difference

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in the strength of the weak force. Right -handed

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antiparticles don't just interact differently

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with the weak force. They actually experience

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a different strength of this interaction compared

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to left -handed ordinary particles. Whoa, okay.

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So what does this all mean in the grand scheme

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of things? What are the real -world consequences

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of this difference in strength? Well, one way

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this plays out is in radioactive decay. That's

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a process governed by the weak force. Because

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of this difference in strength, the chances of

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a nucleus decaying radioactively are slightly

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different for regular matter compared to antimatter.

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So the mirror isn't perfectly reflecting here.

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Exactly. This subtle but crucial asymmetry was

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first observed back in 1963 by James Cronin and

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Valfitch and actually won them a Nobel Prize.

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Another Nobel -worthy discovery. So I imagine

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when this asymmetry was first discovered there

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was a lot of excitement. This difference in the

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weak force wasn't seen as a potential answer

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to this matter -antimatter imbalance. That was

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definitely the hope. You know, maybe the weak

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force had this slight bias towards creating matter

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over antimatter in the early universe. The weak

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force nudged the scales. Maybe, but the math

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didn't quite add up. Turns out this difference,

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while important, wasn't big enough to explain

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the huge amount of matter we see and the lack

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of antimatter. It's like finding a tiny crack

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in the mirror, but not the huge shatter that

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would explain everything. So great discovery,

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Nobel Prize earned, but the ultimate mystery

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remained. Okay, so the weak force isn't the whole

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story. What about the strong force? That's the

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one that binds protons and neutrons together

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in the nucleus. Super strong, as the name suggests.

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You would think, following the pattern with the

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weak force, that there might be some difference

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in how left -handed particles and right -handed

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antiparticles feel the strong force, right? Yeah,

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seems logical. Well, once again, antimatter threw

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us a curveball. Every experiment, and I mean

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every single one, shows the strong force doesn't

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care if it's dealing with matter or antimatter.

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It treats them exactly the same. No asymmetry,

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no difference in strength, nothing. So the strong

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force is totally blind to this matter -antimatter

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difference. Blind is a bat. Which brings us to

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gravity, that final fundamental force. And this

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is where things are getting really interesting

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at CERN. They're trying to nail down, once and

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for all, if gravity acts differently on matter

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and antimatter. Absolutely, it's a really exciting

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area of research. But it sounds like most physicists

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are betting it won't, right? That's the common

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assumption. Think back to Galileo dropping objects

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from the Leaning Tower of Pisa, or Newton's law

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of universal gravitation. The key takeaway is

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that gravity doesn't care what something's made

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of, just how much mass it has. A cannonball and

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a feather in a vacuum will fall at the same rate.

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Right, a classic physics demo. And this is a

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cornerstone of Einstein's theory of general relativity,

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his equivalence principle. It says that the mass

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that determines how much something resists being

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pushed, its inertia, and the mass that makes

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it feel gravity are the same thing. So, in a

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gravitational field, everything falls at the

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same rate, no matter what it's made of. So, given

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this well -established principle, why bother

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trying to measure gravity's effect on antimatter?

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It seems like a huge undertaking for something

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we think we already know the answer to. Well,

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there are a couple of good reasons. First, there's

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that mystery of the baryonic asymmetry, the matter

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-antimatter imbalance. We have to explore all

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avenues, even the unlikely ones. Leave no stone

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unturned. Exactly. The second reason is a bit

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more speculative. Some theories trying to explain

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dark matter and dark energy to big cosmic mysteries

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suggest that antimatter might actually have a

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negative gravitational charge. Segetive gravitational

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charge, meaning it would fall up, wouldn't that

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be a sight to see? It would defy our everyday

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experience for sure. So, to test this, a few

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very sophisticated experiments are running at

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CERN. Aegis, GBAR, and LFA. In fact, the LFA

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team recently published some big findings in

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the journal Nature, giving us actual data on

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how antimatter accelerates under Earth's gravity.

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After decades of assumptions, we finally have

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hard evidence to work with. It must have been

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a huge moment finally getting some concrete data

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after all this time. But how did they manage

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to measure something so incredibly subtle? It

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sounds impossibly difficult. Oh, it was a phenomenal

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feat. It started with generating a beam of positrons.

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Remember those anti -electrons? from a radioactive

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form of sodium, sodium -22. Now, when positrons

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meet normal matter, they usually annihilate each

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other in a burst of energy. Gone. Exactly. But

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a tiny fraction of these positrons actually survive.

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And the researchers managed to capture those

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survivors, cool them down to ridiculously low

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temperatures, and then trap them using carefully

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arranged electric and magnetic fields. But you

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said earlier that measuring gravity's effect

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on individual positrons is almost impossible,

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right? They're just too light, and even the tiniest

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electromagnetic fields could mess everything

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up. You're absolutely right. So they needed a

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trick, and it was a brilliant one. They took

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those trapped positrons and combined with antiprotons

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to make neutral anti -hydrogen atoms. Antiprotons

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are made by smashing high -energy protons into

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a metal target. And since these new anti -hydrogen

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atoms are neutral, meaning no net electric charge,

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they're way less affected by stray electromagnetic

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fields, making them ideal for gravity experiments.

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Like trying to measure the fall of a feather

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in a hurricane, but now you've somehow managed

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to shield the feather from the wind. That's a

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great analogy. So now they have these anti -hydrogen

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atoms, the neutral ones, but how do they isolate

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them and actually measure the effect of gravity?

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Yeah, especially since gravity is such a weak

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force compared to the other ones. They use a

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special chamber with a near -perfect vacuum to

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minimize unwanted interactions. Inside, the anti

00:12:12.960 --> 00:12:15.379
-hydrogen atoms are trapped, using a complex

00:12:15.379 --> 00:12:18.000
arrangement of magnetic fields, sort of like

00:12:18.000 --> 00:12:21.360
a magnetic bottle. Then... They carefully, and

00:12:21.360 --> 00:12:24.659
I mean very carefully, weaken the vertical magnetic

00:12:24.659 --> 00:12:26.500
fields that are holding those anti -hydrogen

00:12:26.500 --> 00:12:28.799
atoms. What does that do? Well, because those

00:12:28.799 --> 00:12:30.799
atoms are always jiggling around due to their

00:12:30.799 --> 00:12:33.539
thermal energy, this weakening of the field allows

00:12:33.539 --> 00:12:36.500
them to slowly escape, either from the top or

00:12:36.500 --> 00:12:38.639
the bottom of the chamber, over about 20 seconds.

00:12:38.899 --> 00:12:41.399
I see. So it's like tilting that magnetic bottle

00:12:41.399 --> 00:12:43.799
ever so slightly, allowing them to dribble out

00:12:43.799 --> 00:12:46.960
one by one. Exactly. Now here's the crucial part.

00:12:47.049 --> 00:12:49.950
When one of these escaping anti -hydrogen atoms

00:12:49.950 --> 00:12:52.190
hits the wall of the chamber, which is made of

00:12:52.190 --> 00:12:55.309
regular matter, they annihilate, releasing a

00:12:55.309 --> 00:12:58.350
burst of light. Ah, that poof again. Yep, but

00:12:58.350 --> 00:13:01.509
a very useful poof. By carefully counting the

00:13:01.509 --> 00:13:03.409
number of annihilation events happening at the

00:13:03.409 --> 00:13:05.809
top versus the bottom of the chamber, they can

00:13:05.809 --> 00:13:07.889
figure out which way gravity is pulling those

00:13:07.889 --> 00:13:10.529
anti -hydrogen atoms. Okay, so if gravity is

00:13:10.529 --> 00:13:12.710
pulling antimatter down, like normal matter,

00:13:12.830 --> 00:13:14.809
they should see more annihilations at the bottom

00:13:14.809 --> 00:13:17.559
of the chamber. You got it. To make sure they

00:13:17.559 --> 00:13:19.440
were interpreting things correctly, they ran

00:13:19.440 --> 00:13:22.700
simulations. These simulations show that if anti

00:13:22.700 --> 00:13:25.480
-hydrogen experiences normal gravity, they'd

00:13:25.480 --> 00:13:28.139
expect about 85 % of the annihilations to happen

00:13:28.139 --> 00:13:30.940
at the bottom. If antimatter was falling upwards,

00:13:31.059 --> 00:13:34.080
only 20 % would be at the bottom. And if gravity

00:13:34.080 --> 00:13:37.299
had no effect at all, it would be about 50 -50,

00:13:37.700 --> 00:13:40.100
with some slight variation due to imperfections

00:13:40.100 --> 00:13:42.960
in the experiment. Drumroll, please. What did

00:13:42.960 --> 00:13:45.679
they actually see? The results were pretty clear.

00:13:45.799 --> 00:13:48.759
Roughly 75 % of the anti -hydrogen atoms that

00:13:48.759 --> 00:13:50.940
escaped ended up annihilating at the bottom of

00:13:50.940 --> 00:13:54.080
the chamber. That strongly points to normal downward

00:13:54.080 --> 00:13:56.480
gravity for antimatter, just like we'd expect

00:13:56.480 --> 00:13:58.820
for regular stuff. Okay, that seems pretty convincing.

00:13:59.179 --> 00:14:00.840
But I imagine they didn't just stop there, did

00:14:00.840 --> 00:14:03.610
they? Oh no. To double check and eliminate any

00:14:03.610 --> 00:14:05.909
potential biases in their setup, they did the

00:14:05.909 --> 00:14:08.730
experiment multiple times, each time adding a

00:14:08.730 --> 00:14:11.169
small controlled magnetic force, either pushing

00:14:11.169 --> 00:14:13.649
the anti -hydrogen atoms up or down to simulate

00:14:13.649 --> 00:14:15.450
different gravity conditions. So like adding

00:14:15.450 --> 00:14:18.870
a little extra push or pull? Exactly. Then they

00:14:18.870 --> 00:14:20.730
compared the results from these different runs

00:14:20.730 --> 00:14:23.669
to their simulations for various gravity scenarios.

00:14:24.169 --> 00:14:26.450
The best match, the one that fit the data the

00:14:26.450 --> 00:14:29.210
closest, was for downward gravity acting just

00:14:29.210 --> 00:14:31.370
like it does on regular matter. But you said

00:14:31.370 --> 00:14:34.049
their best estimate for the gravitational acceleration

00:14:34.049 --> 00:14:36.889
was slightly lower than the usual 9 .8 meters

00:14:36.889 --> 00:14:39.169
per second squared where you stay, right? Yes.

00:14:39.429 --> 00:14:42.090
It came out to about 0 .75 g. But here's the

00:14:42.090 --> 00:14:44.649
important thing. Their measurements had uncertainties,

00:14:44.950 --> 00:14:47.029
which are super important in any experiment.

00:14:47.350 --> 00:14:49.429
You always need to know how precise your result

00:14:49.429 --> 00:14:52.690
is. The infamous error bars. Right. After accounting

00:14:52.690 --> 00:14:55.470
for everything, their best estimate, with error

00:14:55.470 --> 00:15:00.330
bars included, was 0 .75 g. plus or minus 0 .13g

00:15:00.330 --> 00:15:02.929
due to potential systematic errors, and plus

00:15:02.929 --> 00:15:06.429
or minus 0 .16g from random statistical fluctuations.

00:15:07.049 --> 00:15:09.789
This means a full 1g acceleration is still comfortably

00:15:09.789 --> 00:15:12.090
within their margin of error, completely compatible

00:15:12.090 --> 00:15:14.389
with their findings. So while future experiments

00:15:14.389 --> 00:15:16.710
might refine this measurement, it's safe to say

00:15:16.710 --> 00:15:19.450
this groundbreaking work effectively rules out

00:15:19.450 --> 00:15:22.090
those more outlandish ideas of antimatter falling

00:15:22.090 --> 00:15:26.039
up. Pretty much. It seems antimatter while strange

00:15:26.039 --> 00:15:29.200
and exotic, still obeys the same gravitational

00:15:29.200 --> 00:15:32.519
rules as the rest of us. So, to summarize, we

00:15:32.519 --> 00:15:35.200
know antimatter is real. It has the same mass

00:15:35.200 --> 00:15:37.820
but opposite charge as its matter counterparts.

00:15:38.519 --> 00:15:40.820
Its electromagnetic interactions are as expected,

00:15:41.240 --> 00:15:43.419
but the weak force treats it a bit differently,

00:15:43.679 --> 00:15:45.860
though not enough to explain the matter dominance

00:15:45.860 --> 00:15:48.879
of the universe. And now, it seems, gravity plays

00:15:48.879 --> 00:15:51.639
by the same rules for both matter and antimatter.

00:15:51.700 --> 00:15:54.440
But that still leaves the big question unanswered.

00:15:54.539 --> 00:15:58.019
Why are we here, in a universe made almost entirely

00:15:58.019 --> 00:16:00.899
of matter? It's a puzzle that continues to baffle

00:16:00.899 --> 00:16:04.080
physicists. If the laws of physics, as far as

00:16:04.080 --> 00:16:06.419
we can tell, are mostly symmetrical for matter

00:16:06.419 --> 00:16:08.759
and antimatter, then the overwhelming presence

00:16:08.759 --> 00:16:10.940
of matter in the universe is a huge mystery.

00:16:11.320 --> 00:16:13.559
It suggests we might be missing something fundamental

00:16:13.559 --> 00:16:16.120
in our understanding of physics, or perhaps the

00:16:16.120 --> 00:16:17.879
very beginning of the universe, the Big Bang

00:16:17.879 --> 00:16:20.269
itself. started with an imbalance baked right

00:16:20.269 --> 00:16:22.769
in. A huge imbalance playing out over billions

00:16:22.769 --> 00:16:24.590
of years. It's a lot to wrap your head around.

00:16:24.789 --> 00:16:27.669
It is. But that's the beauty of science. It's

00:16:27.669 --> 00:16:29.750
a never -ending quest to understand the universe

00:16:29.750 --> 00:16:32.830
and our place in it. Well said. A big thanks

00:16:32.830 --> 00:16:35.169
to you for diving into the fascinating world

00:16:35.169 --> 00:16:37.769
of antimatter with me. And to you, dear listener,

00:16:37.929 --> 00:16:40.330
I'll leave you with this. We've learned that

00:16:40.330 --> 00:16:42.899
antimatter, despite its weirdness, doesn't float

00:16:42.899 --> 00:16:46.019
away due to antigravity. It seems gravity keeps

00:16:46.019 --> 00:16:48.679
everything grounded, even the exotic stuff. But

00:16:48.679 --> 00:16:51.299
it's this very similarity that deepens the mystery.

00:16:52.039 --> 00:16:54.740
If matter and antimatter are so alike in so many

00:16:54.740 --> 00:16:57.139
ways, then what tipped the scales in the early

00:16:57.139 --> 00:16:59.379
universe? What made matter win out? What made

00:16:59.379 --> 00:17:01.639
our existence possible? It's a cosmic riddle.

00:17:01.919 --> 00:17:04.200
And maybe, just maybe, you'll be the one to help

00:17:04.200 --> 00:17:06.039
solve it. It would be quite a feat to unlock

00:17:06.039 --> 00:17:08.339
that mystery. Keep those brains buzzing, folks.

00:17:08.519 --> 00:17:10.460
And until next time, happy exploring.
