I Is information lost in wavefunction collapse?

[atyy]

Huh? "Supporting MWI" does not mean believing that the black hole information paradox can only be formulated under the MWI. Indeed, the whole point of "supporting MWI" with regard to black holes and information is that there is no paradox at all under the MWI, since everything is always unitary. Only under a collapse interpretation is there a paradox at all.
No, but it's an interpretation of standard QM.
This can't be right, since MWI is an interpretation of standard QM, and has entirely unitary time evolution with no collapse.

All of this is wrong.

MWI is not a solution to the black hole information paradox, in any sense that Copenhagen is not.

The Carroll post you put in support of MWI states "These are the serious issues for EQM ..." and "But even given the real challenges of the preferred-basis issue and the probability issue, I think EQM is way ahead of any proposed alternative."

Standard QM has collapse - see the texts by Dirac, Landau and Lifshitz, Cohen-Tannoudji et al, Weinberg, Sakurai, Griffiths.

 

[PeterDonis]

Standard QM has collapse

Again, this can't be right, since MWI is an interpretation of standard QM and it doesn't have collapse.

see the texts by Dirac, Landau and Lifshitz, Cohen-Tannoudji et al, Weinberg, Sakurai, Griffiths.

Do any of these texts claim that MWI is not a valid interpretation?

 

[PeterDonis]

MWI is not a solution to the black hole information paradox

"Everything is always unitary" is a solution, or at least a claimed solution; and that implies the MWI.

 

[atyy]

"Everything is always unitary" is a solution, or at least a claimed solution; and that implies the MWI.

Yes, but it does not imply MWI. The usual approach, eg, AdS/CFT to try to solve the paradox would also solve it for Copenhagen. The interpretations have nothing to do with the paradox. Introducing different degrees of freedom is the usual approach.

 

[atyy]

Do any of these texts claim that MWI is not a valid interpretation?

I edited my reply above before seeing your reply. Carroll states that MWI has serious issues, as does David Deutsch. If even supporters of MWI still think there are major problems with MWI, then it cannot be considered textbook physics.

 

[PeterDonis]

Carroll states that MWI has serious issues

But he also says, as you quote, that it is "way ahead of any proposed alternative".

If even supporters of MWI still think there are major problems with MWI, then it cannot be considered textbook physics.

By this reasoning, no interpretation of QM can be considered "textbook physics". Is that your position?

 

[PeterDonis]

The usual approach, eg, AdS/CFT to try to solve the paradox would also solve it for Copenhagen.

Unless "everything is always unitary" is consistent with what you mean by "Copenhagen", I don't see how this could be true. And if "everything is always unitary" is consistent with what you mean by "Copenhagen", then I am very confused as to what you mean by "Copenhagen".

 

[Nugatory]

If even supporters of MWI still think there are major problems with MWI, then it cannot be considered textbook physics.

All interpretations have major issues - that's why we can spend so much time arguing about them, and also why pointing out the issues cannot settle these arguments.

It would be a bad thing if this thread were to degenerate into another form of "your interpretation is uglier than mine".

 

[Stephen Tashi]

What is the technical definition for "information" in the context of this thread?

 

[romsofia]

I had a similar question months ago, (https://www.physicsforums.com/threads/where-does-the-energy-go.930637/)Even though it wasn't mentioned in the thread, if you take the collapse interpretation to be true, I believe you are essentially saying that your information (states) are not coupled to the environment until a measurement is taken place. So no information is loss even in the Copenhagen interpretation because as far the environment knows, there was really only one option?

If your information is coupled to the environment, then in theory, you would be able to measure the energy output of each state via some gravitational wave (I think Davies worked out some hand-wavy calculations in the 60/70s, i'll send references for anyone interested)... but maybe that's not for this thread :).

There are so many ifs when dealing with which is why...

What is the technical definition for "information" in the context of this thread?

I think to make any movement in a thread like this, this is the right way to go. Otherwise we will all just talk around each other using ambiguous words. Math triumphs. As far as I'm aware, information in QM is referred to as states! But what states are we considering? An energy operator is different than a position operator, and then some other people started talking about bits! If we start talking about bits, then there is already a reason how THAT information loss is handled! If we start to think as information as bits, then why not just invoke Launder's principle and call it a day?

Just to clarify, as far as I'm aware Launder's principle might not apply to quantum systems, but I'm not an expert in quantum computing nor computing in general!

 

[atyy]

Unless "everything is always unitary" is consistent with what you mean by "Copenhagen", I don't see how this could be true. And if "everything is always unitary" is consistent with what you mean by "Copenhagen", then I am very confused as to what you mean by "Copenhagen".

Well it depends on what one means by "everything". For the information paradox, there is a reasonable definition of everything. In Copenhagen, everything is unitary between measurements.

 

[atyy]

By this reasoning, no interpretation of QM can be considered "textbook physics". Is that your position?

Yes, except for Copenhagen or whatever one wishes to call what is in the textbooks.

 

[atyy]

It would be a bad thing if this thread were to degenerate into another form of "your interpretation is uglier than mine".

It has nothing to do with ugliness, but correctness. It is not correct, in a thread which mentions standard QM, and makes sense within standard QM, to tell the OP that his question doesn't make sense, by bringing in speculative approaches to the measurement problem as if it is settled physics - here I use speculative in the sense that string theory is speculative and not settled physics (although I do think it is the leading approach to quantum gravity).

 

[atyy]

It would be a bad thing if this thread were to degenerate into another form of "your interpretation is uglier than mine".

To add to my comment above, the OP is not a question about interpretations. Bringing in interpretations as Peter Donis did is irrelevant to the OP. The point is that the non-unitary evolution of collapse, and that of the information paradox are not related as I tried to say in post #20, and as Demystifier says clearly in post #30.

 

[stevendaryl]

Even though collapse and apparent disappearance of information by black hole evaporation both violate unitarity, those two processes are not directly related. They violate unitarity in very different ways.
In a collapse, a pure state evolves (jumps) into another pure state.
By black hole evaporation, a pure state evolves into a mixed state.

I'm not sure I understand the distinction you are making. The way I understand "mixed state" in quantum mechanics, there are two different sources of mixed states:

1. If you don't know what the state of a system is, then you can represent it as a mixed state, where the probabilities reflect your subjective uncertainty about what the pure state is.
2. A pure state involving two subsystems (the system of interest and the environment, say) can be treated as a mixed state of just one of the subsystems, by a kind of averaging over the system that you're not interested in.

When people say that a black hole turns a pure state into a mixed state, I'm not exactly sure what notion of "mixed state" is meant. But if it is #1, then it seems to me equivalent to a measurement collapsing the wave function, but you don't know what the measurement result was.

 

[PeterDonis]

To add to my comment above, the OP is not a question about interpretations. Bringing in interpretations as Peter Donis did is irrelevant to the OP. The point is that the non-unitary evolution of collapse, and that of the information paradox are not related as I tried to say in post #20, and as Demystifier says clearly in post #30.

I agree with the point you and @Demystifier make that these two things (collapse vs. BH information paradox) are different. Are you saying that that, in itself, is a sufficient answer to the question in the OP? If so, I would like the OP to say whether he agrees with that.

 

[PeterDonis]

It is not correct, in a thread which mentions standard QM, and makes sense within standard QM, to tell the OP that his question doesn't make sense, by bringing in speculative approaches to the measurement problem as if it is settled physics

But in "standard QM", the OP's question can't be answered, because standard QM allows both kinds of interpretations: interpretations in which information is not lost in "wave function collapse" (because "collapse" is not a real process but just a calculational rule, no real non-unitary processes ever happen--for example, the MWI), and interpretations in which information is lost in collapse, because collapse is a real, non-unitary process.

 

[PeterDonis]

it depends on what one means by "everything"

Yes, which is exactly why the answer to the OP's question must be interpretation dependent: some interpretations, like the MWI, mean by "everything" literally everything--nothing non-unitary ever happens, anywhere in the universe. Whereas other interpretations only interpret "everything" to mean "everything between measurements" (and some go on to claim that during a measurement, an actual non-unitary process, wave function collapse, happens, while others are agnostic about this).

 

[Demystifier]

I'm not sure I understand the distinction you are making. The way I understand "mixed state" in quantum mechanics, there are two different sources of mixed states:

1. If you don't know what the state of a system is, then you can represent it as a mixed state, where the probabilities reflect your subjective uncertainty about what the pure state is.
2. A pure state involving two subsystems (the system of interest and the environment, say) can be treated as a mixed state of just one of the subsystems, by a kind of averaging over the system that you're not interested in.

When people say that a black hole turns a pure state into a mixed state, I'm not exactly sure what notion of "mixed state" is meant. But if it is #1, then it seems to me equivalent to a measurement collapsing the wave function, but you don't know what the measurement result was.

It is neither #1 nor #2. It is

3. Initially you have a pure state involving two entangled subsystems, one inside the black hole and the other outside of the black hole. So initially it corresponds to your 2. But then the inside subsystem gets destroyed in the black hole singularity, so what remains is only the outside subsystem, which is in a mixed state but no longer entangled with anything.

 

[stevendaryl]

It is neither #1 nor #2. It is

3. Initially you have a pure state involving two entangled subsystems, one inside the black hole and the other outside of the black hole. So initially it corresponds to your 2. But then the inside subsystem gets destroyed in the black hole singularity, so what remains is only the outside subsystem, which is in a mixed state but no longer entangled with anything.

Thanks. So that really is something new.

So the idea is that you create an EPR pair---an electron and positron with entangled anticorrelated spins. You throw the positron into a black hole, which then vanishes in a puff of Hawking radiation. Now, you still have the electron, but the electron by itself was not in a pure state, it was in an entangled state. So how do you describe it now that its entangled partner no longer exists? A mixed state.

Now that I say it out loud, it occurs to me that in the case of spin entanglement, you might still have the electron entangled, rather than in mixed state. When the positron falls into the black hole, it imparts a tiny bit of angular moment to the black hole. When the black hole evaporates, that angular momentum is distributed among the particles produced by the Hawking radiation. So in that particular case, it seems that the electron's spin would be entangled with the resulting Hawking radiation. So I think to really illustrate the information loss, you would need some property of a pair of particles that is nonconserved?

 

[Dr. Courtney]

All the major textbooks use Copenhagen. Standard QM is the Copenhagen interpretation.

Agreed, but standard here just means a standard presentation in Physics education.

Yes, except for Copenhagen or whatever one wishes to call what is in the textbooks.

Sure, but the presence in textbooks is a stronger case for a consensus regarding what to teach students, it may not represent a consensus regarding a preference for truth or correctness.

It's an imperfect analogy, but one might argue that Newtonian mechanics is the "right" version of mechanics, because it is found in many more introductory textbooks (and therefore more textbooks, since most texts are introductory.) However, it is completely equivalent to Lagrangian mechanics and Hamiltonian mechanics. The consensus to teach Newtonian mechanics first (which I believe is correct) is based more on its usefulness with the math skills of most students in these classes rather than some sense that it is more correct than Lagrangian or Hamiltonian.

I would not make any more from the lack of alternate QM interpretations in the textbooks than I'd make from the piles and piles of Physics texts that ignore Lagrangian and Hamiltonian mechanics.

 

[Demystifier]

Thanks. So that really is something new.

So the idea is that you create an EPR pair---an electron and positron with entangled anticorrelated spins. You throw the positron into a black hole, which then vanishes in a puff of Hawking radiation. Now, you still have the electron, but the electron by itself was not in a pure state, it was in an entangled state. So how do you describe it now that its entangled partner no longer exists? A mixed state.

Now that I say it out loud, it occurs to me that in the case of spin entanglement, you might still have the electron entangled, rather than in mixed state. When the positron falls into the black hole, it imparts a tiny bit of angular moment to the black hole. When the black hole evaporates, that angular momentum is distributed among the particles produced by the Hawking radiation. So in that particular case, it seems that the electron's spin would be entangled with the resulting Hawking radiation.

That's correct.

So I think to really illustrate the information loss, you would need some property of a pair of particles that is nonconserved?

No. Instead of angular momentum, consider e.g. lepton number which is supposed to be conserved. If you have electron with positive lepton number outside and positron with negative lepton number inside, the total lepton number is zero. However, the lepton number cannot be seen in the external properties of geometry of the black hole (this is the so called no-hair theorem). When the black hole finally evaporates, the negative lepton number in the inside disappears. Hence the black hole evaporation violates the lepton number conservation, which otherwise is conserved.

 

[stevendaryl]

No. Instead of angular momentum, consider e.g. lepton number which is supposed to be conserved

I would say that quantities such as lepton number or baryon number are not actually conserved. It just happens to be that there are no interactions that cause it to change.

I of course didn't understand it, but t'Hooft gave an argument a long time ago to the effect that baryon number is not conserved in the standard model. So proton decay, for example, is a prediction of the standard model, even though no finite number of Feynman diagrams can show it. It's a nonperturbative effect. I'm pretty sure that he didn't consider black holes. (This prediction does not contradict the experimental evidence that protons don't decay, because t'Hooft's mechanism is way too weak to produce a detectable number of proton decay events. It's many orders of magnitude smaller than the number of decays predicted by various GUT theories.)

 

[stevendaryl]

I would say that quantities such as lepton number or baryon number are not actually conserved. It just happens to be that there are no interactions that cause it to change.

I of course didn't understand it, but t'Hooft gave an argument a long time ago to the effect that baryon number is not conserved in the standard model. So proton decay, for example, is a prediction of the standard model, even though no finite number of Feynman diagrams can show it. It's a nonperturbative effect. I'm pretty sure that he didn't consider black holes. (This prediction does not contradict the experimental evidence that protons don't decay, because t'Hooft's mechanism is way too weak to produce a detectable number of proton decay events. It's many orders of magnitude smaller than the number of decays predicted by various GUT theories.)

It is stated here (http://inspirehep.net/record/16152/files/v16-n1-p23.pdf) that decays by t'Hooft's mechanism are $10^{-77}$ less common than predicted decays by GUT theories.

 

[Demystifier]

I would say that quantities such as lepton number or baryon number are not actually conserved. It just happens to be that there are no interactions that cause it to change.

I of course didn't understand it, but t'Hooft gave an argument a long time ago to the effect that baryon number is not conserved in the standard model. So proton decay, for example, is a prediction of the standard model, even though no finite number of Feynman diagrams can show it. It's a nonperturbative effect. I'm pretty sure that he didn't consider black holes. (This prediction does not contradict the experimental evidence that protons don't decay, because t'Hooft's mechanism is way too weak to produce a detectable number of proton decay events. It's many orders of magnitude smaller than the number of decays predicted by various GUT theories.)

Even in GUT theories one has a conservation of a difference between baryon and lepton number B-L, but black hole evaporation violates it too.

 

[atyy]

I agree with the point you and @Demystifier make that these two things (collapse vs. BH information paradox) are different. Are you saying that that, in itself, is a sufficient answer to the question in the OP? If so, I would like the OP to say whether he agrees with that.

Yes, I do mean that those two things are sufficient for answering the OP (or at least for correcting the use of the black hole information paradox as motivation for the question in the OP). There is no need to bring in interpretations of QM.

There is the additional question of whether information is lost in collapse. This needs to be defined a bit better (eg. as stevendaryl has discussed at various points in this thread, but one can use standard QM, which includes collapse).

 

[atyy]

But in "standard QM", the OP's question can't be answered, because standard QM allows both kinds of interpretations: interpretations in which information is not lost in "wave function collapse" (because "collapse" is not a real process but just a calculational rule, no real non-unitary processes ever happen--for example, the MWI), and interpretations in which information is lost in collapse, because collapse is a real, non-unitary process.

stevendaryl's post #25 frames and answers this question in a way that is independent of the subtleties you mentioned. (As a side point, it is not really common to take collapse to be physical in Copenhagen. Physical collapse usually refers to alternative theories like GRW or CSL).

 

[atyy]

Sure, but the presence in textbooks is a stronger case for a consensus regarding what to teach students, it may not represent a consensus regarding a preference for truth or correctness.

It's an imperfect analogy, but one might argue that Newtonian mechanics is the "right" version of mechanics, because it is found in many more introductory textbooks (and therefore more textbooks, since most texts are introductory.) However, it is completely equivalent to Lagrangian mechanics and Hamiltonian mechanics. The consensus to teach Newtonian mechanics first (which I believe is correct) is based more on its usefulness with the math skills of most students in these classes rather than some sense that it is more correct than Lagrangian or Hamiltonian.

I would not make any more from the lack of alternate QM interpretations in the textbooks than I'd make from the piles and piles of Physics texts that ignore Lagrangian and Hamiltonian mechanics.

Yes, but the difference is that there are many advanced textbooks teaching the Lagrangain and Hamiltonian formalisms and their equivalence to Newtonian mechanics, and there is consensus in the community about these issues.

In the case of MWI, there are no advanced textbooks stating that MWI is standard QM - Cohen-Tannoudji, Sakurai and Weinberg are senior undergraduate level textboks, about the same level at which the Lagrangian and Hamiltonian formalisms are usually discussed. In fact, the research level discussions state problems MWI, even by people who are proponents of the approach. Stating unresolved physics as if it is standard is bad for beginners, because it is misleading false advertising, Stating unresolved physics as if it is standard is also bad for people who support the approach, because it means that we should stop research into these open questions, which ultimately means that the questions will never pass from being unresolved to resolved.

 

[PeterDonis]

it is not really common to take collapse to be physical in Copenhagen

If that is the case, then I don't think it's correct to describe the standard QM collapse as non-unitary.

 

[PeterDonis]

stevendaryl's post #25 frames and answers this question

No, it doesn't. The last sentence of that post highlights the issue: standard QM does not specify where the information has gone. But that doesn't mean the information is lost, or that it's not lost. It just means standard QM can't tell you whether it's lost or not.