Hawking Radiation and the Black Hole Information Paradox

The Quark Side - Quantum Physics Podcast

Hawking radiation showed that black holes slowly evaporate, raising a deep conflict with quantum theory over whether information is truly lost. Physicists now turn to ideas like holography, entanglement, and string theory to resolve one of modern physics’ greatest paradoxes.
2026-02-11 35 min Transcript

Available Results

Generated results are saved to the knowledge database for reuse and search.

No generated results are available for this episode yet.

Extract Knowledge

Pick what you want extracted first. Model, scope, and chapter options appear after a template is selected.

Generated results for public episodes are saved to the knowledge database so they can be reused and searched later.

Transcript

<v Speaker 1>Welcome to the quart Side Quantum Physics Podcast, an exploration
<v Speaker 1>of the fundamental structure of reality, where quantum laws govern matter, energy,
<v Speaker 1>and information. Here, uncertainty is a feature, not a flaw,
<v Speaker 1>and understanding begins at the smallest scales.
<v Speaker 2>Welcome back to the show. Today, we're looking at something, well,
<v Speaker 2>it's not really an object or a place. We're looking
<v Speaker 2>at a battleground.
<v Speaker 3>That's a good way to put it.
<v Speaker 2>And I don't just mean a metaphorical debate in a
<v Speaker 2>university hall. I mean a literal, honest to goodness conflict
<v Speaker 2>in the laws of physics themselves.
<v Speaker 3>The conflict where the universe needs to be arguing with itself. Yeah,
<v Speaker 3>and we're caught in the middle trying to figure out
<v Speaker 3>who's right.
<v Speaker 2>It feels incredibly dramatic because as we've been preparing for
<v Speaker 2>this exploration, it's become clear this is a fifty year
<v Speaker 2>old standoff between the two pillars of modern science.
<v Speaker 3>It really is. And this standoff, this paradox, it doesn't
<v Speaker 3>just bend the rules of reality, it seems to snap
<v Speaker 3>them in half.
<v Speaker 2>And it keeps physicists awake at night. I mean, if
<v Speaker 2>you follow the logic all the way to its conclusion.
<v Speaker 2>It might even mean that space and time, well, they
<v Speaker 2>aren't what we think they are at all.
<v Speaker 3>It truly is the ultimate mystery. We are talking, of course,
<v Speaker 3>about the black hole information paradox.
<v Speaker 2>I have to admit when I first heard that term,
<v Speaker 2>I thought, okay, black holes, they're mysterious, big, dark, scary,
<v Speaker 2>We get it. But this is so much deeper.
<v Speaker 3>It's not just about not knowing what's inside right.
<v Speaker 2>It's about a logical contradiction. It's like a mathematician proving
<v Speaker 2>that two plus two equals five. It threatens to bring
<v Speaker 2>the whole structure down.
<v Speaker 3>The gravity of the situation, if you'll excuse the pun,
<v Speaker 3>is immense. Since nineteen seventy four, this specific problem has
<v Speaker 3>been the engine driving so much of theoretical.
<v Speaker 2>Physics, because it forces general relativity.
<v Speaker 3>Einstein's grand theory of gravity, space and.
<v Speaker 2>Time into a case match with quantum mechanics.
<v Speaker 3>The theory of the very small of particles and forces,
<v Speaker 3>and the terrifying thing. The central problem is that in
<v Speaker 3>this specific scenario they cannot both be right. One of
<v Speaker 3>them has to give.
<v Speaker 2>So that's our mission for this investigation. We are going
<v Speaker 2>to try to figure out what happens to information to
<v Speaker 2>the story of something when it falls into a black hole?
<v Speaker 3>Does it get deleted from the universe?
<v Speaker 2>Does it get stored somewhere? Does it I don't know,
<v Speaker 2>sneak back out in disguise, and.
<v Speaker 3>We're going to see why the answer to that question
<v Speaker 3>could literally determine the ultimate fate of the entire universe.
<v Speaker 2>To get there, we have to trace the journey of
<v Speaker 2>the black hole itself. We'll start with the simple classical view,
<v Speaker 2>the gravity prison.
<v Speaker 3>Then we'll move into the quantum revolution that Stephen Hawking started,
<v Speaker 3>and from there we'll get into the really wild proposed solutions.
<v Speaker 2>And some of these sound like science fiction. We're talking
<v Speaker 2>about things called fuzzballs, firewalls, and even the idea that
<v Speaker 2>the universe is a kind of hologram.
<v Speaker 3>It's where physics gets very, very strange. But the strangeness
<v Speaker 3>is necessary to solve the problem.
<v Speaker 2>I love that physics terms can sound like something from
<v Speaker 2>a fantasy novel. I cast fuzzball. But before we get
<v Speaker 2>to any of that, we have to start at the beginning,
<v Speaker 2>the before picture classical view. Exactly before nineteen seventy four,
<v Speaker 2>before Hawking shook the world, what did we think a
<v Speaker 2>black hole was?
<v Speaker 3>You have to go back to Einstein pure general relativity,
<v Speaker 3>and in that picture, a black hole is well. It's
<v Speaker 3>elegantly simple and absolutely terrifying.
<v Speaker 2>It's a region of space time.
<v Speaker 3>Where gravity is so powerful, so unbelievably intense, that nothing
<v Speaker 3>can escape.
<v Speaker 2>And when you say nothing, you mean nothing, not even light.
<v Speaker 3>And since light is the cosmic speed limit, the absolute
<v Speaker 3>fastest anything can travel.
<v Speaker 2>If late can't get out, then forget it.
<v Speaker 3>Nothing else has a chance, exactly. And the key feature here,
<v Speaker 3>the thing everyone's heard of, is the event.
<v Speaker 2>Horizon, the point of no return.
<v Speaker 3>It is the ultimate point of no return. Think of
<v Speaker 3>it like one way door in space time. You can
<v Speaker 3>pass through it going in, no problem.
<v Speaker 2>But you can't come back out.
<v Speaker 3>You can't even try to come back out. Inside the horizon.
<v Speaker 3>The curvature of space time is so extreme that every
<v Speaker 3>possible path you could take, every direction, every single direction,
<v Speaker 3>whether you fire your rockets or just float, leads to
<v Speaker 3>one place. Yeah, the center, the singularity. The direction out
<v Speaker 3>literally ceases to exist. It's like trying to go south
<v Speaker 3>from the south pole.
<v Speaker 2>So it's the ultimate root motel. You check in, but you.
<v Speaker 3>Never check out. And this idea comes from the schwartz
<v Speaker 3>Child metric. Carl Schwarzschild solved Einstein's equations just months after
<v Speaker 3>they were published back in nineteen fifteen.
<v Speaker 2>An incredible achievement.
<v Speaker 3>It really was. And he showed that for any amount
<v Speaker 3>of mass, there's a critical size a radius where if
<v Speaker 3>you crush that mass down into that volume, gravity just wins.
<v Speaker 3>It overwhelms everything and collapses.
<v Speaker 2>I always have trouble getting my head around the densities
<v Speaker 2>we're talking about here. Can you give us a sense
<v Speaker 2>of scale?
<v Speaker 3>Sure, Let's take the Sun, a gigantic ball of fusing plasma.
<v Speaker 3>To turn it into a black hole, you'd have to
<v Speaker 3>crush all of its mass down into a sphere with
<v Speaker 3>the radius of just three kilometers.
<v Speaker 2>It's the entire Sun into the size of a small town.
<v Speaker 3>Or even more dramatically, take the Earth, our whole planet,
<v Speaker 3>every mountain, every ocean, all of it. To make the
<v Speaker 3>Earth a black hole, you'd have to crush it down
<v Speaker 3>to the size of a sugar cube.
<v Speaker 2>Sugar cube, that's that's just unimaginable.
<v Speaker 3>It's a density that defies intuition. And the main takeaway
<v Speaker 3>for our story in this classical view is that black
<v Speaker 3>holes are these stable eternal prisons. They are endpoints. They
<v Speaker 3>eat matter, they grow, and then they just sit there forever, so.
<v Speaker 2>A one way street. They only get bigger, they never
<v Speaker 2>get smaller. That seems, I don't know, a little too
<v Speaker 2>neat and tidy, and physics usually hates things that are
<v Speaker 2>too neat.
<v Speaker 3>It absolutely does, because when you find a rule that
<v Speaker 3>seems that absolute, it often means you're not looking at
<v Speaker 3>the whole picture.
<v Speaker 2>And that's where the first crack in the armor appeared.
<v Speaker 2>It didn't come from quantum mechanics initially, it came from thermodynamics.
<v Speaker 3>That's right, the physics of deam engines, of all things.
<v Speaker 2>It feels like such a clash of eras nineteenth century
<v Speaker 2>industrial physics meaning twentieth century cosmic horror.
<v Speaker 3>It is. Specifically, we're talking about one of the most
<v Speaker 3>sacred laws in all of science, the second law thermo dynamics.
<v Speaker 2>Okay, remind us what that is.
<v Speaker 3>In simple terms, it says that the total entropy of
<v Speaker 3>a closed system can never decrease.
<v Speaker 2>And entropy is basically a measure of disorder.
<v Speaker 3>Yeah, messiness, messiness, disorder, or even hidden information. That's why
<v Speaker 3>a broken egg doesn't spontaneously reassemble itself. The universe tends
<v Speaker 3>toward more disorder, not less.
<v Speaker 2>Okay, so things get messier over time.
<v Speaker 3>Got it?
<v Speaker 2>How does that connect to black holes?
<v Speaker 3>Well, here's the problem. Imagine you have something with very
<v Speaker 3>high entropy, like a burning library. All the ordered information
<v Speaker 3>in the books is being turned into disordered smoke.
<v Speaker 2>And ash, maximum messiness exactly.
<v Speaker 3>Now, what if you take that entire burning library and
<v Speaker 3>you just dump it into a black hole? Okay, according
<v Speaker 3>to classical general relativity, that mess is just gone. It's
<v Speaker 3>been removed from our observable universe. The black hole itself,
<v Speaker 3>in this classical picture is perfectly smooth and simple, has
<v Speaker 3>no hair, as they say, it only has mass, spin,
<v Speaker 3>and charge, no other features.
<v Speaker 2>So if the mass disappears from the universe and the
<v Speaker 2>black hole doesn't get any mess here on the outside,
<v Speaker 2>did I just violate the second law? Did I just
<v Speaker 2>clean up the universe's room?
<v Speaker 3>That was the terrifying question. It looked like a perfect
<v Speaker 3>cosmic crime, a way to delete entropy and break one
<v Speaker 3>of the most fundamental rules of nature.
<v Speaker 2>And nature does not like its rules being broken, not.
<v Speaker 3>At all, And for a long time, physicists kind of
<v Speaker 3>swept this under the rug they figured, well, gravity a
<v Speaker 3>special maybe the rules just don't apply here.
<v Speaker 2>They just ignored it pretty.
<v Speaker 3>Much until the early nineteen seventies, when a graduate student
<v Speaker 3>named Jacob Beckenstein started pushing the issue. He argued that
<v Speaker 3>black holes must have entropy, and if they.
<v Speaker 2>Have entropy, then they must have a temperature, right.
<v Speaker 3>And if they have a temperature, they have to radiate heat.
<v Speaker 2>Which totally contradicts the whole nothing can escape idea.
<v Speaker 3>Precisely Beaekenstein was on the right path, but he didn't
<v Speaker 3>have the mechanism. The person who found the mechanism improved
<v Speaker 3>it with math was Stephen Hawking, and in nineteen seventy
<v Speaker 3>four he dropped a bombshell that changed everything.
<v Speaker 2>This is it the moment that kicks off the whole paradox?
<v Speaker 2>What did Hawking find? What did you do differently?
<v Speaker 3>He did something no one had successfully done before. He
<v Speaker 3>brought the two great theories together. He applied quantum field
<v Speaker 3>theory to the curved space time right at the edge
<v Speaker 3>of the event horizon.
<v Speaker 2>He looked at the quantum world in the most extreme
<v Speaker 2>gravitational field possible, and.
<v Speaker 3>He discovered that black holes are not completely black.
<v Speaker 2>They glow in a.
<v Speaker 3>Very particular, very subtle way. Yes, they emit what we
<v Speaker 3>now call Hawking radiation.
<v Speaker 2>Okay, let's unpack this slowly, because this is the absolute
<v Speaker 2>core of the problem. How does a prison that nothing
<v Speaker 2>can escape from suddenly start spitting things out? Is it leaking?
<v Speaker 3>That's the crucial point. Not leaking from the inside. The
<v Speaker 3>radiation is generated outside the event horizon, right at the edge.
<v Speaker 3>How to understand that, you have to understand the quantum vacuum.
<v Speaker 3>In quantum mechanics, empty space isn't empty at all. It's
<v Speaker 3>a roiling, fizzing sea of energy.
<v Speaker 2>The virtual particles.
<v Speaker 3>Exactly thanks to the uncertainty principle, pairs of particles and
<v Speaker 3>antiparticles are constantly popping into existence out of borrowed energy.
<v Speaker 3>They exist for an infinitesimally small moment.
<v Speaker 2>And then they find each other and annihilate, paying back
<v Speaker 2>the energy loan. Poof.
<v Speaker 3>Right, It's happening everywhere all the time, in this room,
<v Speaker 3>in deep space, everywhere. But normally it's just a background hum.
<v Speaker 2>So what's different At the edge of a black hole?
<v Speaker 3>The gravity is so extreme, the space time is so
<v Speaker 3>warped that something dramatic can happen. Imagine a pair of
<v Speaker 3>these virtual particles pops into existence right on the razor's
<v Speaker 3>edge of the event horizon.
<v Speaker 2>Okay, one is just inside, one is just.
<v Speaker 3>Outside, precisely, and the intense gravity can physically rip them
<v Speaker 3>apart before they have a chance to annihilate.
<v Speaker 2>It separates them permanently, exactly.
<v Speaker 3>The particle that popped into existence inside the horizon is doomed.
<v Speaker 3>It falls for the singularity. But the one on the
<v Speaker 3>outside it's now an orphan. Its partner is gone forever.
<v Speaker 3>It can't annihilate, so it's stuck. It's stuck, and it's real.
<v Speaker 3>It escapes out into the universe, and to a distant
<v Speaker 3>observer like us with a telescope, it looks for all
<v Speaker 3>the world like the black hole just spat out a.
<v Speaker 2>Particle that is just mind bending. The black hole is
<v Speaker 2>conjuring particles out of the vacuum at its edge. Ye.
<v Speaker 2>But physics is all about balance sheets. Nothing comes from nothing.
<v Speaker 2>There's always a cost.
<v Speaker 3>You're absolutely right. Conservation of energy is king. If that
<v Speaker 3>escaping particle carries positive energy away into the universe, which
<v Speaker 3>it must, then that energy has to be paid for,
<v Speaker 3>and it's paid for by the black hole itself.
<v Speaker 2>So the black hole loses mass.
<v Speaker 3>It loses mass. You can think of the particle that
<v Speaker 3>fell in as having a kind of negative energy from
<v Speaker 3>the perspective of the outside universe. When it gets eaten,
<v Speaker 3>its subtracts from the black hole's total mass. Energy. The
<v Speaker 3>books have to balance.
<v Speaker 2>And this was the revolutionary discovery.
<v Speaker 3>This was it. Black holes aren't eternal, they have a lifespan,
<v Speaker 3>they shrink, they evaporate.
<v Speaker 2>That just completely upends the classical picture. And there's a
<v Speaker 2>formula for this, right, the Hawking temperature. It's famous for
<v Speaker 2>being this beautiful mess of letters.
<v Speaker 3>It is. The formula itself is T T A C
<v Speaker 3>three E g KPM.
<v Speaker 2>Okay, don't worry about the numbers, but let's talk about
<v Speaker 2>the letters, because it's like a guest list for the
<v Speaker 2>Party of the century.
<v Speaker 3>In physics, it really is a profound equation. You've got
<v Speaker 3>daybar h bar, which is the symbol of quantum mechanics.
<v Speaker 2>World of the small.
<v Speaker 3>You've got Davoter Newton's constant, which represents gravity. You've got
<v Speaker 3>t bowl order the speed of light from Einstein's relativity
<v Speaker 3>the world, and you've got Keeler ball Er Bill Boltzmann's constant,
<v Speaker 3>which is the cornerstone of thermodynamics.
<v Speaker 2>The world of heat and disorder. It's like the avengers
<v Speaker 2>of physics, all assembled in one equation to describe one
<v Speaker 2>an object.
<v Speaker 3>It's the first real signpost on the road to a
<v Speaker 3>theory of quantum gravity. It proves black holes are where
<v Speaker 3>all these theories are forced to talk to each other.
<v Speaker 2>But there's a weird twist in there. The m for
<v Speaker 2>mass is on the bottom of the fraction.
<v Speaker 3>Yes, it's in the denominator, which means.
<v Speaker 2>The bigger the black hole, the lower the temperature.
<v Speaker 3>Exactly. It's completely counterintuitive. A supermassive black hole at the
<v Speaker 3>center of a galaxy is incredibly frigidly cold, colder than
<v Speaker 3>the background temperature of space. It's barely radiating at all.
<v Speaker 2>But a small one.
<v Speaker 3>A small black hole is scorching hot, and as it radiates,
<v Speaker 3>it loses mass, which makes it even.
<v Speaker 2>Smaller, which makes it even hotter, and.
<v Speaker 3>It radiates even faster. It's a runaway process, so in
<v Speaker 3>its very final moments, a tiny microscopic black hole would
<v Speaker 3>evaporate in a final brilliant flash of high energy radiation. Wow.
<v Speaker 2>So biggers are cold and quiet, small ones are hot
<v Speaker 2>and explosive. That's the opposite of what you'd think it is.
<v Speaker 3>In this discovery, this whole thermoe dynamic picture, it actually
<v Speaker 3>solved that old entropy.
<v Speaker 2>Problem, right the burning library.
<v Speaker 3>Hawking and Beeckenstein show that, yes, black holes have entropy,
<v Speaker 3>and the amount of entropy they have is enormous. So
<v Speaker 3>when you throw your messy library in, the black hole's
<v Speaker 3>own entropy increases by more than enough to account for
<v Speaker 3>what you threw in. The second law is saved.
<v Speaker 2>Okay, phew, so the laws of physics are safe. But
<v Speaker 2>wait a minute. The title of this investigation has the
<v Speaker 2>word paradox in it, So fixing one problem must have
<v Speaker 2>created a much, much worse one.
<v Speaker 3>And that's exactly what happened. In patching the hole in
<v Speaker 3>the wall of thermodynamics, Hawking tore out the entire foundation
<v Speaker 3>of quantum mechanics.
<v Speaker 2>Okay, before we get to that crack in the foundation, though,
<v Speaker 2>you mentioned something important the way the entropy is stored.
<v Speaker 2>You called it the area law.
<v Speaker 3>Yes, this is a massive clue and it's going to
<v Speaker 3>become very important later.
<v Speaker 2>So explain this. Why is it so strange?
<v Speaker 3>Well, think about any normal object, a hard drive of
<v Speaker 3>book your brain. The amount of information you can store
<v Speaker 3>is proportional to its volume.
<v Speaker 2>Right, more space, more stuff. If I buy a bigger
<v Speaker 2>hard drive, I could store more data.
<v Speaker 3>It's a three D storage system, but for a black hole.
<v Speaker 3>Beieckenstein and Hawking found that the entropy the information it's
<v Speaker 3>hiding is not proportional to its three D volume. It's
<v Speaker 3>proportional to the two D surface area of its event horizon.
<v Speaker 2>That's really weird. That's like saying the amount of data
<v Speaker 2>on my hard drive depends on the size of the
<v Speaker 2>sticker on the outside, not how many platters are inside.
<v Speaker 3>That is a perfect analogy. It's as if all the
<v Speaker 3>information of everything that ever fell in stars, planets libraries
<v Speaker 3>isn't stored inside the black hole, but is somehow smeared
<v Speaker 3>out and encoded on its surface, so it's plastered on
<v Speaker 3>the walls precisely. And this was the very first hint
<v Speaker 3>of something called the holographic principle, the idea that a
<v Speaker 3>description of a three D volume of space can be
<v Speaker 3>encoded on a two D boundary.
<v Speaker 2>Okay, let's put a pin in that holography. I feel
<v Speaker 2>like we're definitely coming back to that, but for now,
<v Speaker 2>let's face the crisis. We have evaporation, we have entropy.
<v Speaker 2>Why do we have a paradox?
<v Speaker 3>Okay, this is the heart of it. All boils down
<v Speaker 3>to the fate of the information itself. Yea. And it's
<v Speaker 3>a direct conflict between two concepts unitarity versus.
<v Speaker 2>Thermal radiation unitarity. Okay, that's a big physics word. Break
<v Speaker 2>it down for us. It's basically a core belief in
<v Speaker 2>quantum mechanics, right.
<v Speaker 3>It is the absolute bedrock of the theory. Unitarity means
<v Speaker 3>that information is never ever destroyed in the universe. Never never.
<v Speaker 3>The theory is reversible. If you know the precise state
<v Speaker 3>of a system, now you can run the clock forward
<v Speaker 3>and predict its future, and you can run the clock
<v Speaker 3>backward to perfectly reconstruct its past.
<v Speaker 2>So if I burn a book, in practice, it's gone.
<v Speaker 3>But in principle, in principle, if you could capture every
<v Speaker 3>single particle of ash, every molecule of smoke, every photonic
<v Speaker 3>heat and light, the laws of quantum mechanics, that you
<v Speaker 3>could reverse the process and get the exact book back.
<v Speaker 3>The information isn't deleted, it's just scrambled.
<v Speaker 2>So quantum mechanics has a perfect memory it never forgets exactly.
<v Speaker 3>Now, compare that to Hawking radiation. Hawking's original calculations show
<v Speaker 3>that the radiation coming out is thermal, meaning it's just heat.
<v Speaker 3>It's random, it's a perfect black body spectrum. Its properties
<v Speaker 3>depend only on the mass, charge and spin of the
<v Speaker 3>black hole. It does not depend on what fell in
<v Speaker 3>to create it.
<v Speaker 2>Wait, so you're telling me that if I make a
<v Speaker 2>black hole out of a collapsing star, or I make
<v Speaker 2>an identical black hole out of a giant pile of
<v Speaker 2>encyclopedias or giant ball of rubber ducts, oh in, radiation
<v Speaker 2>that comes out at the end is exactly the same
<v Speaker 2>in all three.
<v Speaker 3>Cases, according to the original calculation. Yes, yes, the radiation
<v Speaker 3>has no memory of what it used to be. It's generic,
<v Speaker 3>featureless heat.
<v Speaker 2>I see the problem, I think I see the collision
<v Speaker 2>course here. Let's make it super concrete with a thought experiment. Okay,
<v Speaker 2>I build a quantum computer. It contains the most complex
<v Speaker 2>information imaginable, the cure for all diseases, the works of Shakespeare,
<v Speaker 2>my personal diary. It's a unique, highly ordered state. I
<v Speaker 2>take this quantum computer and I throw it into a
<v Speaker 2>black hole.
<v Speaker 3>Okay, the black hole gets a tiny bit bigger. Then
<v Speaker 3>over googles of years, it slowly radiates away, gets smaller
<v Speaker 3>and smaller, and then poof.
<v Speaker 2>It's gone, completely gone, and was left behind just.
<v Speaker 3>A uniform, expanding cloud of warm, random Hawking radiation.
<v Speaker 2>And if that radiation is truly random, truly thermal, there
<v Speaker 2>is no way to look at that cloud of heat
<v Speaker 2>and reconstruct my quantum computer.
<v Speaker 3>No way at all. The information, Shakespeare, the cures your
<v Speaker 3>diary has been utterly and completely erased from the universe.
<v Speaker 2>So let's recap the conflict. General relativity says the information
<v Speaker 2>fell past the point of no return. It's inside.
<v Speaker 3>Quantum mechanics says the information must be conserved, it can't
<v Speaker 3>be deleted. That's illegal.
<v Speaker 2>But Hawking radiation says the information was converted into random heat,
<v Speaker 2>and then the black hole disappeared, erasing it forever.
<v Speaker 3>You've just stated the paradox perfectly. We start with what's
<v Speaker 3>called a pure state, the ordered quantum computer, and we
<v Speaker 3>end up with a mixed state, the disordered heat. According
<v Speaker 3>to the rules of quantum mechanics, that transforms is forbidden.
<v Speaker 2>So physics itself is breaking its own laws. And if
<v Speaker 2>information can be destroyed, then then what.
<v Speaker 3>The quantum mechanics, the theory that describes everything from transistors
<v Speaker 3>to stars, is fundamentally wrong. We lose predictability, we lose
<v Speaker 3>the connection between past and future. It's chaos.
<v Speaker 2>Okay, so we have a crisis. The laws of reality
<v Speaker 2>are on trial. Now let's talk about the proposed solutions.
<v Speaker 2>Physicists have spent fifty years trying to find a way
<v Speaker 2>out of this box, and.
<v Speaker 3>There are really only a few possible escape routes. You
<v Speaker 3>either have to modify quantum mechanics or modify general relativity,
<v Speaker 3>or find some clever loophole that lets them both be right.
<v Speaker 2>Let's start with solution A, the original position. What did
<v Speaker 2>Hawking himself think? At first?
<v Speaker 3>Hawking was nothing if not bold. He looked at his
<v Speaker 3>own calculation and took it at face value. He said, yep,
<v Speaker 3>the information is just lost.
<v Speaker 2>He accepted defeat for quantum mechanics.
<v Speaker 3>He did. He argued that gravity is special and that
<v Speaker 3>in the presence of bla black holes, the sacred rule
<v Speaker 3>of unitarity is violated. He famously made a bet with
<v Speaker 3>physicists Kip Thorn and John Preskill. Hawking and Thorn bet
<v Speaker 3>that information was destroyed, that.
<v Speaker 2>Seems almost nihilistic, just saying, oh, well, the universe has
<v Speaker 2>a delete button.
<v Speaker 3>It was a radical stance, but it was consistent with
<v Speaker 3>his math. But over the years this position became extremely
<v Speaker 3>unpopular because if you allow information loss, it creates all
<v Speaker 3>sorts of other paradoxes and problems. You get violations of
<v Speaker 3>energy conservation. Things get very messy.
<v Speaker 2>So physicists didn't like it.
<v Speaker 3>They really didn't, and eventually needed it Hawking in two
<v Speaker 3>thousand and four he publicly announced that he'd been wrong.
<v Speaker 3>He conceded the bet to Priskill and gave him an
<v Speaker 3>encyclopedia of his choice.
<v Speaker 2>And encyclopedia yeah for the preservation of information.
<v Speaker 3>That's clever. Okay. So solution A, information is lost is
<v Speaker 3>off the table. What's solution B.
<v Speaker 2>Solution B is the idea of black hole.
<v Speaker 3>Remnants, remnants like leftovers exactly.
<v Speaker 2>The idea is, maybe the evaporation process, it doesn't go
<v Speaker 2>all the way to zero. Maybe it stops when the
<v Speaker 2>black hole shrinks down to the smallest possible size, the
<v Speaker 2>plank length, which is incredibly tiny.
<v Speaker 3>So it leaves behind this little nugget.
<v Speaker 2>A tiny stable nugget, and this remnant, this microscopic speck
<v Speaker 2>would act as a kind of cosmic vault, holding all
<v Speaker 2>the information of everything that ever fell into the original
<v Speaker 2>black hole.
<v Speaker 3>Wait, hold on. If I threw an entire star with
<v Speaker 3>all of its quadrillions of particles into a black hole
<v Speaker 3>and it evaporates down to a speck smaller than an atom,
<v Speaker 3>how does that tiny speck store the information of an
<v Speaker 3>entire star? That is the big glaring problem. It's sometimes
<v Speaker 3>called the clown car problem. For this to work, this
<v Speaker 3>tiny object would need to have a nearly infinite number
<v Speaker 3>of possible internal states to store all that.
<v Speaker 2>Information, and that causes problems.
<v Speaker 3>It causes huge problems for quantum field theory. Also, if
<v Speaker 3>these remnants are stable and can never disappear, then the
<v Speaker 3>universe should be absolutely filled with them from all the
<v Speaker 3>black holes that have ever evaporated. We've never seen any
<v Speaker 3>sign of them.
<v Speaker 2>So remnants are probably not the answer. Too much information
<v Speaker 2>and too small a package. Okay, what's next on the menu?
<v Speaker 2>Solution C sounds cute. The fuzzball.
<v Speaker 3>The fuzzball paradigm. This one comes out of string theory, of.
<v Speaker 2>Course it does. String theory is answer to everything seems
<v Speaker 2>to be more strings.
<v Speaker 3>Well, in a way. Yes. The fuzzball idea, championed by
<v Speaker 3>physicists Samir Mathur and others, argues that our classical picture
<v Speaker 3>of a black hole is just wrong. They say, when
<v Speaker 3>matter collapses, it doesn't form a singularity and a smooth
<v Speaker 3>empty event horizon.
<v Speaker 2>Wait, no event horizon. That's like the defining feature of
<v Speaker 2>a black.
<v Speaker 3>Hole, not a sharp empty one.
<v Speaker 2>No.
<v Speaker 3>Instead, they propose that the fundamental strings that make up
<v Speaker 3>matter get all tangled up into a giant, messy, vibrating ball,
<v Speaker 3>a fuzzball.
<v Speaker 2>So there's no empty space inside. It's filled with a
<v Speaker 2>ball of cosmic yarn.
<v Speaker 3>Pretty much. The surface of the black hole isn't an
<v Speaker 3>abstract point of no return in empty space. It's a
<v Speaker 3>physical object like the surface of the sun, but made
<v Speaker 3>of tangled strings.
<v Speaker 2>Okay, how does that solve the information paradox?
<v Speaker 3>Well, it solves it beautifully. If you throw your quantum
<v Speaker 3>computer into a fuzzball, it's information doesn't disappear into a singularity.
<v Speaker 3>It gets absorbed into the structure of the fuzzball. The
<v Speaker 3>vibrations of the strings change to encode the new information, so.
<v Speaker 2>The data gets stuck in the fuzz exactly.
<v Speaker 3>Then, when the fuzzball radiates. It's not random thermal radiation
<v Speaker 3>from an empty horizon. It's radiation coming off a complex
<v Speaker 3>vibrating object. The vibrations carry the information away like sound
<v Speaker 3>waves echoing off a drum.
<v Speaker 2>So the radiation is a detailed message from the start.
<v Speaker 3>That's the idea. No horizon, no singularity, no information loss,
<v Speaker 3>no paradox.
<v Speaker 2>That actually sounds surprisingly elegant. What's the catch.
<v Speaker 3>The main catch is that it requires string theory to
<v Speaker 3>be the correct description of reality, and we don't know
<v Speaker 3>if that's true, and it completely rewrites Einstein's picture. It says,
<v Speaker 3>if you were to fall into a black hole, you
<v Speaker 3>wouldn't just peacefully float across an invisible line. You would
<v Speaker 3>hit a physical surface, splat against a wall of strings.
<v Speaker 2>Okay, a very different experience for the astronaut, but it
<v Speaker 2>saves the information. Now, let's move on to the really
<v Speaker 2>scary standing one solution D the firewall.
<v Speaker 3>The firewall. This is a much more recent idea, from
<v Speaker 3>twenty twelve. It's often called the Amps paradox after the
<v Speaker 3>four physicists superposed it. Alm Harry, MAROLV. Pulcinski and Sully.
<v Speaker 2>Sounds like a powerful law firm it was.
<v Speaker 3>A powerful paper. They took a very close look at
<v Speaker 3>quantum entanglement. Remember our particle pair at the horizon, one
<v Speaker 3>falls in, one.
<v Speaker 2>Escapes, and they're entangled linked spooky action at a distance.
<v Speaker 3>Exactly Now, for information to eventually get out of the
<v Speaker 3>black hole, that escaping particle, let's call it particle B,
<v Speaker 3>needs to be entangled with all the other hawking radiation
<v Speaker 3>that came out before it. It needs to join the
<v Speaker 3>collective to reconstruct the message.
<v Speaker 2>Okay, so B needs to be linked to the cloud
<v Speaker 2>of earlier radiation.
<v Speaker 3>But here's the problem. Particle B is already maximally entangled
<v Speaker 3>with its original partner, particle A, the one that fell
<v Speaker 3>inside the black hole.
<v Speaker 2>Can it be entangled with both?
<v Speaker 3>Quantum mechanics says no. There's a fundamental rule called the
<v Speaker 3>monogamy of entanglement. A quantum system can only be fully
<v Speaker 3>maximally entangled with one other system at a time. It
<v Speaker 3>can't have two perfect partners.
<v Speaker 2>Quantum mechanics believes in monogamy.
<v Speaker 3>Good to know, so amps argue that something has to
<v Speaker 3>give if the information is going to be saved. If
<v Speaker 3>Particle B is going to join the outside radiation cloud,
<v Speaker 3>then it's entanglement with particle a inside must be violently
<v Speaker 3>broken the moment it's created.
<v Speaker 2>And breaking entanglement that's not a gentle process.
<v Speaker 3>No, breaking that quantum link requires a huge amount of energy,
<v Speaker 3>and they calculated that if this happens for every single
<v Speaker 3>particle pair at the horizon, it would create an intensely
<v Speaker 3>energetic barrier right at that spot, a literal wall of fire.
<v Speaker 2>So if I'm the astronaut falling in instead of a
<v Speaker 2>gentle crossing into darkness, you would.
<v Speaker 3>Hit this wall of high energy quanta and be instantly vaporized,
<v Speaker 3>annihilated to the horizon.
<v Speaker 2>That seems unpleasant for me, But why is it a
<v Speaker 2>problem for physics?
<v Speaker 3>It's a huge problem for Albert Einstein. The absolute cornerstone
<v Speaker 3>of general relativity is the equivalence principle. It was what
<v Speaker 3>Einstein called his happiest thought, which says it says that
<v Speaker 3>the experience of being in free fall in a gravitational
<v Speaker 3>field is indistinguishable from floating in empty space. For an
<v Speaker 3>astronaut falling into a black hole, crossing the event horizon
<v Speaker 3>should be completely uneventful. It's not a special place in space.
<v Speaker 3>You shouldn't even notice when you cross it.
<v Speaker 2>Right, It's just a line on a map, not a
<v Speaker 2>brick wall.
<v Speaker 3>But the firewall says no, it is a brick wall,
<v Speaker 3>a wall of death.
<v Speaker 2>So to save quantum mechanics and its rule of monogamy,
<v Speaker 2>the firewall has to completely shatter Einstein's equivalence principle.
<v Speaker 3>It really feels like every solution breaks something else. One
<v Speaker 3>breaks quantum mechanics, another breaks the structure of the black hole.
<v Speaker 3>This one breaks general relativity. It's like trying to solve
<v Speaker 3>a Rubik's cube, where fixing one side messes up all
<v Speaker 3>the others. That's a perfect description of why this has
<v Speaker 3>been such a persistent problem for fifty years. But in
<v Speaker 3>the last couple of decades, a new heavyweight contender has
<v Speaker 3>entered the ring. It's not so much a specific physical picture,
<v Speaker 3>but a powerful mathematical argument.
<v Speaker 2>And this is where we get back to holography. The
<v Speaker 2>idea called ad SCFT, Yes, the.
<v Speaker 3>Ad s CFT correspondence, proposed by one Meldadicina in nineteen
<v Speaker 3>ninety seven. It's one of the most influential and cited
<v Speaker 3>papers in the history of theoretical physics.
<v Speaker 2>Okay, ad SCFT is a lot of letters. I need
<v Speaker 2>you to give me the soup can analogy.
<v Speaker 3>I read about the soup can analogy is perfect. This
<v Speaker 3>was called a duality. Meldocinas showed a mathematical equivalence between
<v Speaker 3>two theories that look completely different.
<v Speaker 2>Okay, what are the two theories.
<v Speaker 3>First, you have the physics inside a specific kind of
<v Speaker 3>toy universe called anti de Sitter space or ADS. This
<v Speaker 3>is the soup inside the can. It's a universe with gravity,
<v Speaker 3>it has black holes. It's a three D bulk space.
<v Speaker 3>Got it.
<v Speaker 2>The soup gravity lives there.
<v Speaker 3>Then you have a totally different theory, a normal field
<v Speaker 3>theory or CFT. This is a quantum theory of particles
<v Speaker 3>and fields with no gravity, and it lives only on
<v Speaker 3>the boundary of that universe. It's the two D label
<v Speaker 3>on the outside of the soup can.
<v Speaker 2>So a three D universe with gravity inside and a
<v Speaker 2>two D quantum universe without gravity on the label.
<v Speaker 3>And here is Meldosine is incredible discovery. He proved that
<v Speaker 3>the physics of the soup is mathematically identical to the
<v Speaker 3>physics on the label. There are two different descriptions of
<v Speaker 3>the exact same system, a dictionary between them, a perfect dictionary.
<v Speaker 3>Every event that happens in the three D gravitational world
<v Speaker 3>of the soup corresponds exactly to some event happening among
<v Speaker 3>the two D quantum particles on the label.
<v Speaker 2>So if a black hole forms inside the soup, can.
<v Speaker 3>That corresponds to something like a hot, swirling fluid of
<v Speaker 3>particles interacting on the two D label. And here's the
<v Speaker 3>genius move go on. The theory on the label, the
<v Speaker 3>CFT is a standard quantum field theory. We know for
<v Speaker 3>a fact that it obeys the rules. It is unitary.
<v Speaker 3>Information is never lost in that theory.
<v Speaker 2>Oh, I see where this is going. If the theory
<v Speaker 2>on the label is unitary and never loses information.
<v Speaker 3>And the label is just a different description of the soup.
<v Speaker 2>Then the soup must be unitary too.
<v Speaker 3>Exactly. It proves mathematically that a theory of quantum gravity
<v Speaker 3>must preserve information even if we don't know the exact
<v Speaker 3>physical mechanism of how the black hole gives the information back.
<v Speaker 3>The duality guarantees that it does.
<v Speaker 2>That feels like I don't know a brilliant cheak code.
<v Speaker 2>It's like saying I don't know how to solve this
<v Speaker 2>impossible three D puzzle, but I found the two D
<v Speaker 2>instruction Manual and it says on the last page, this
<v Speaker 2>puzzle is solvable.
<v Speaker 3>That's a great way to put it. It gave physicists
<v Speaker 3>enormous confidence that information is ultimately safe. Now there's a
<v Speaker 3>big caveat which is our real universe is not an
<v Speaker 3>anti de Sitter space. It's a different shape. So this
<v Speaker 3>is a proof of principle in a toy universe, not
<v Speaker 3>a direct map of our reality. But the principle is
<v Speaker 3>believed to be general.
<v Speaker 2>And this idea has led to real progress.
<v Speaker 1>Right.
<v Speaker 2>It led to the calculation of something called Page curve.
<v Speaker 2>This feels like the most recent breakthrough it is.
<v Speaker 3>This is based on work by Don Page back in
<v Speaker 3>the nineties. He thought about the entanglement entropy of the
<v Speaker 3>Hawking radiation as the black hole evaporates.
<v Speaker 2>Okay, so he's basically tracking how messy or how entangled
<v Speaker 2>the radiation is over time.
<v Speaker 3>Right, And he made a prediction. If information is truly lost,
<v Speaker 3>as Hawking first thought, then the entropy of the radiation
<v Speaker 3>just keeps going up and up and up as more
<v Speaker 3>random particles are emitted, until the black hole is.
<v Speaker 2>Gone, a straight line going up more or less.
<v Speaker 3>But age argued, if information is conserved, something different has
<v Speaker 3>to happen. The entropy should go up for the first
<v Speaker 3>half of black hole's life, but then it has to
<v Speaker 3>hit a peak the page time and start coming back down.
<v Speaker 3>Why would it come down, Because in the second half
<v Speaker 3>of the evaporation, the radiation that's coming out is now
<v Speaker 3>deeply entangled with the radiation that came out in the
<v Speaker 3>first half. It starts to purify the system. It's releasing
<v Speaker 3>the key to the scrambled message. By the time the
<v Speaker 3>black hole is completely gone, the total entropy of all
<v Speaker 3>the radiation has to drop back down to zero because
<v Speaker 3>it has reformed a pure state.
<v Speaker 2>The original information is all there, just unscrambled. And recently
<v Speaker 2>physicists actually managed to calculate this curve.
<v Speaker 3>Yes, this was the huge breakthrough. In twenty nineteen, using
<v Speaker 3>tools from the holographic principle, two different groups of physicists
<v Speaker 3>finally figured out how to do the calculation for an
<v Speaker 3>evaporating black hole, and they reproduce the page curve exactly.
<v Speaker 3>They saw the entropy go up and then come back down.
<v Speaker 2>That feels like the smoking gun. It feels like we
<v Speaker 2>finally have concrete mathematical proof that information gets out.
<v Speaker 3>It's the strongest evidence we have to date. It suggests
<v Speaker 3>that somehow, through subtle correlations and entanglement, the information does escape.
<v Speaker 3>But it still leads us with a nagging question, which
<v Speaker 3>is how and why does the radiation look so random
<v Speaker 3>and thermal? If it's secretly carrying this complex message.
<v Speaker 2>Right, if it contains Shakespeare, why can't we just read it?
<v Speaker 3>And the answer seems to be the difference between something
<v Speaker 3>that is truely random and something that is pseudorandom.
<v Speaker 2>Like a secret code.
<v Speaker 3>Precisely, if I take a long novel and I encrypt
<v Speaker 3>it with a powerful modern encryption key, what I get
<v Speaker 3>out looks like total.
<v Speaker 2>Gibberish, just random noise.
<v Speaker 3>You could run every statistical test you want on it
<v Speaker 3>and it would look perfectly random. But it's not. It
<v Speaker 3>contains all the information of the original novel in a hidden,
<v Speaker 3>correlated form.
<v Speaker 2>And if you have the key.
<v Speaker 3>If you have the key, you could decrypt it and
<v Speaker 3>get the novel back perfectly. The modern consensus is that
<v Speaker 3>Hawking radiation is like that. It's not random heat. It's
<v Speaker 3>the most complexly encrypted message in the universe.
<v Speaker 2>So the black hole is not a shredder it's an
<v Speaker 2>ultimate scrambler.
<v Speaker 3>That is the picture that's emerging. It scrambles the information
<v Speaker 3>so completely that for any practical purpose it's gone. But
<v Speaker 3>in principle, the universe holds onto the key.
<v Speaker 2>What an incredible journey. We've gone from a simple eternal prison,
<v Speaker 2>to a leaky radiator, to a fretter, to a hard drive,
<v Speaker 2>to a ball of fuzz, to a wall of fu
<v Speaker 2>and now to a holographic scrambler.
<v Speaker 3>It's a perfect example of how science pushes at the
<v Speaker 3>boundaries of what we know, and how each new idea
<v Speaker 3>reveals a deeper level of reality.
<v Speaker 2>So let's bring it all home. Let's talk about the
<v Speaker 2>big picture. Why should someone listening right now care about
<v Speaker 2>burning encyclopedias in space? What are the real stakes here?
<v Speaker 3>The stakes are everything. This paradox isn't really about black holes.
<v Speaker 3>Black holes are just the laboratory the universe has given us.
<v Speaker 3>This is the crucible where we are trying to forge
<v Speaker 3>a theory of quantum gravity.
<v Speaker 2>The holy grail of physics, the theory that unites the
<v Speaker 2>very big and the very small.
<v Speaker 3>The theory of everything. Solving this paradox will tell us
<v Speaker 3>something profound about the fundamental nature of space and time themselves.
<v Speaker 2>What do you mean by that? How could it change
<v Speaker 2>our idea of space and time?
<v Speaker 3>Well, this holographic principle we've been talking about, it's a
<v Speaker 3>radical idea and suggests that space time might not be
<v Speaker 3>the fundamental bedrock of reality. It might be.
<v Speaker 2>Emergent, emergent like it's made of something else exactly.
<v Speaker 3>Think about temperature. A single atom doesn't have a temperature.
<v Speaker 3>Temperature is an emergent property of a large collection of
<v Speaker 3>atoms moving around. The idea gaining ground is that space
<v Speaker 3>time itself might be like that. It might emerge from
<v Speaker 3>a deeper network of quantum entanglement.
<v Speaker 2>So space is built out of quantum connections between things.
<v Speaker 3>That's the frontier. The slogan some physicists use is it
<v Speaker 3>from quibit, the idea that the geometry of space time
<v Speaker 3>is determined by the entanglement structure of quantum information. If
<v Speaker 3>you bring the entanglement, the space itself falls apart.
<v Speaker 2>That's a lot to wrap your head around. It makes
<v Speaker 2>reality sound like a giant quantum computer.
<v Speaker 3>In some sense, it might be. And the amazing thing
<v Speaker 3>is this isn't just philosophy anymore. We have observational tools
<v Speaker 3>coming online that could actually test some.
<v Speaker 2>Of this, like the event horizon telescope exactly, which gave
<v Speaker 2>us that first incredible image.
<v Speaker 3>We have gravitational wave detectors that can listen to black
<v Speaker 3>holes merging. And there's even the possibility of finding primordial
<v Speaker 3>black holes.
<v Speaker 2>Tiny ones left over from the big bag.
<v Speaker 3>Yes, and if they exist, some of them should be
<v Speaker 3>finishing their evaporation and exploding right now. If we could
<v Speaker 3>detect one of those final flashes.
<v Speaker 2>You could analyze the radiation directly, we could actually see
<v Speaker 2>if it follows the page curve.
<v Speaker 3>It would be the most profound discovery, imaginable, definitive proof
<v Speaker 3>one way or the other.
<v Speaker 2>It's just a stunning reminder that even with all our knowledge,
<v Speaker 2>we're still just scratching the surface. The universe is so
<v Speaker 2>much stranger than we can imagine.
<v Speaker 3>Absolutely, the paradox isn't a failure of physics. It's a
<v Speaker 3>signpost pointing us toward a deeper, more interconnected reality.
<v Speaker 2>So as we close, here is a final provocative thought
<v Speaker 2>for you to take with you. We talked about holograms.
<v Speaker 2>We talked about how all the information of a three
<v Speaker 2>D black hole might just be stored on its two
<v Speaker 2>D surface. Yes, and you mentioned that some theories, like
<v Speaker 2>at SCFT, suggests that the entire universe might work that way,
<v Speaker 2>a three D soup with a two D label that
<v Speaker 2>describes it all.
<v Speaker 3>It's a leading theoretical possibility. Yes.
<v Speaker 2>So if a black hole is just scrambled information painted
<v Speaker 2>on a horizon, and if the whole universe is a hologram,
<v Speaker 2>then what are we? Are we really three D beings
<v Speaker 2>living in a three D space or are we just
<v Speaker 2>part of the two D information painted on the distant
<v Speaker 2>edge of the cosmos having a very convincing hallucination that
<v Speaker 2>we have depth.
<v Speaker 3>That is a question that pushes right up against the
<v Speaker 3>limits of physics and into philosophy. But the math doesn't
<v Speaker 3>say no, we might just be a.
<v Speaker 2>Projection on that slightly unsettling thought. Thank you for joining
<v Speaker 2>us on this exploration of the impossible, Stay curious, and.
<v Speaker 3>Never stop questioning the nature of your reality.
<v Speaker 2>We'll see you next time.

Chapters

No chapters available.