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I'm not sure I see the difficulty in the black hole information paradox. The outgoing Hawking radiation is not causally connected with the information in the particles inside. If the hole has evaporated you can't tell what was inside by looking at the Hawking photons. Strominger said that black holes are the cause of the breakdown of the physical laws in our universe. He and two others made a huge calculation to solve the paradox and rescue the physical laws. They assumed soft hair for a BH. Like this, no information is lost. Firewalls are not needed anymore (these were proposed to deal with the problem of entanglement monogamy). About 5000 math terms were needed to arrive at the a priori known value of 12J, the angular momentum of the hole. Rather incredibly they arrived exactly at 12.

But anyhow, why is it so hard to assume that information is lost? If you can't trace matter back to matter that is not there anymore, so what? If the (outgoing) Hawking photons can't be causally connected with the stuff inside the hole, so what? Particles inside disappear and particles appear on the outside. As simple as that. Is unitarity lost? Isn't that also in the case of a wave function collapse? Or when a particle pair is created? The created particles have no causal relation with what came before.

So why inventing strange kinds of entanglements of the Hawking photons with the interior of the hole? Why is the disappearance of particles constituting the BH and an independently appearing of Hawking radiation problematic?

John Hunter
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2 Answers2

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Quantum mechanical evolution via the Schrodinger equation (or whatever your favorite formalism is) is unitary. We can start with a pure state with some particles and no black holes, and throw these particles at each other to form a black hole. We then wait for the black hole to evaporate. Eventually it evaporates completely and, according to Hawking, we get radiation that is thermal. This means the state is a mixed state. There is no unitary transformation that takes us from a pure state to a mixed state, so quantum mechanical unitary evolution has apparently broken down [Note: if you don't know about mixed states, the key takeaway is that unitary evolution is not possible of taking us from the initial state to the final state]. This is a contradiction if we assume that the whole system can be described quantum mechanically.

A solution to the problem needs to explain exactly goes wrong. For many (including me), preserving unitarity and quantum mechanics is paramount, which suggests there must be a problem with Hawking's calculation and that the radiation is not really exactly thermal (if only we could calculate its state). If you want to solve the paradox by saying that there is some measurement that happens breaking unitarity, you have to explain exactly where and why the measurement occurs, and how this measurement produces a thermal spectrum. You're perfectly free to wave your hands and think about things you find more interesting, but you won't make a contribution appreciated by people who take the problem seriously without a detailed derivation showing how your mechanism reproduces Hawking's calculation.

Andrew
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    When things accelerate and the Unruh effect takes place, is this a unitary process? – Andrew Steane Jul 22 '21 at 09:58
  • Everything in this argument would go smoothly if we had a proper quantum theory in curved spacetimes. Do we have it? As far as I know, work is in progress. Missing that, the whole argument should be taken a purely speculative, IMHO. – GiorgioP-DoomsdayClockIsAt-90 Jul 22 '21 at 13:36
  • I've never seen Hawking's calculation that Hawking radiation is thermal. But what is the big problem with saying Hawking radiation isn't thermal, and is rather a highly entangled many-body quantum state that 'looks' thermal when you don't know the details of the state? My understanding is that the generic many-body state is this way (for example electrons in a metal). – Jagerber48 Jul 22 '21 at 14:34
  • Only seems like a "paradox" if there is some strong reason to cling to the notion that Hawking radiation MUST be a non-pure state.. – Jagerber48 Jul 22 '21 at 14:35
  • @AndrewSteane There is a horizon in Rindler space. If you trace over the parts of Hilbert space outside of the Rindler horizon, then you do indeed get a mixed state, just as in a black hole background. In this case, there is no problem because we know in reality all that's happened is that we took a trace over a subset of the degrees of freedom, which are entangled with the degrees of freedom in our Rindler wedge. The difference with the black hole case is that the black hole evaporates. So the information is really lost (apparently), as opposed to simply missing in our calculation. – Andrew Jul 23 '21 at 12:35
  • @GiorgioP There is a well-developed framework known as "the effective field theory of gravity" which can consistently treat gravity as an effective quantum theory that applies when deviations from a known background spacetime are small. This is the setting for the information loss paradox. One possible explanation is that the effective field theory framework does not apply -- but as I said above it's not enough to simply say these words, one needs to explain why it doesn't apply, which is not so easy because according to normal rules of effective field theory there's nothing obviously wrong. – Andrew Jul 23 '21 at 12:38
  • @Jagerber48 The problem is that you can calculate what the state is within the effective field theory of gravity, and the state is exactly thermal, and not a highly entangled state. It's not enough to simply state in words this result is wrong, one has to provide a rigorous argument that explains why the original calculation is wrong (if it is). Here's Hawking's original paper on the paradox, which is well worth reading: https://journals.aps.org/prd/abstract/10.1103/PhysRevD.14.2460 – Andrew Jul 23 '21 at 12:41
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With Hawking radiation being thermal (carries no information), black hole evaporation is fundamentally irreversible. This is incompatible with quantum theory, as @Andrew says. So, the problem is to find out what happens with the information.

Solution Attempts Summary:

  1. Denial: Nothing falls in/black holes don’t form. Nope. Just wrong. Note, this kind of solution isn't Hawking being misquoted, or whether they form being not well defined.
  2. Anger: The observer burns up in a giant firewall. Not Even Wrong.
  3. Bargaining: Information comes out. Presently the most popular solution, as it is supported by the gauge/gravity duality.
  4. Depression: Remnants/information stays in. Unpopular because nothing can be calculated.
  5. Acceptance: Non-unitarity. Not ruled out, but even more unpopular than remnants.

Reference: Sabine Hossenfelder

Mr Anderson
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  • (1) is not "just wrong": whether black holes form or not is not well defined — unlike what can be observed about them. – Ruslan Jul 22 '21 at 16:52
  • @Ruslan. No worries, clarified (1) – Mr Anderson Jul 22 '21 at 23:46
  • @Ruslan Ah, a link to an answer of a community college instructor who couldn’t plot correct Penrose diagrams, didn’t know that the Kerr singularity was timelike, and ended up quitting this site. Nice. – safesphere Jul 23 '21 at 22:20
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    @MrAnderson Thank you for sorting out the state of psychology in physics. Without this invaluable analysis the physics community would be disoriented. Finally someone with authority has clarified what is right and what is wrong. Being completely opinion based is perfectly fine. Opinions of professionals don’t count since they do it for living and care only for the paycheck. However your opinion as an enthusiast is motivated only by the truth. Please keep up a good work and keep us informed of any future breakthroughs you make to guide the physics community in the proper direction. – safesphere Jul 23 '21 at 22:36