Concerning psi and black holes

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Discussion Overview

The discussion revolves around the implications of quantum theory in the context of black holes, specifically addressing the probability of finding a particle and the behavior of wavefunctions as particles interact with black holes. The conversation touches on theoretical interpretations and the challenges of reconciling quantum mechanics with general relativity.

Discussion Character

  • Exploratory
  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • One participant claims that the total probability of finding a particle in space is always zero, questioning the legality of this in the context of black holes.
  • Another participant challenges this assertion, asking for clarification on the version of quantum theory being referenced.
  • Some participants suggest that the original statement likely intended to convey that the probability should be one, not zero.
  • There is speculation about whether a particle that falls into a black hole remains part of the universe and how this affects probability density.
  • One participant proposes that the integrated probability of a particle being found outside a black hole decreases over time, suggesting that the black hole "sucks up" the wavefunction.
  • A complex question is raised regarding entangled particles, specifically what happens to the wavefunction of a particle that falls into a black hole and its correlation with its partner outside the black hole.
  • Another participant notes that the concept of wavefunctions being defined everywhere and normalized to unity may not apply in the context of black holes, highlighting the challenges of describing matter motion in such geometries.
  • References are made to the "quantum information riddle at a black hole" and the lack of a fully developed theory to address these issues.
  • One participant mentions a bet involving Stephen Hawking and John Preskill related to the information paradox, indicating ongoing debates in the field.
  • A later reply acknowledges a mistake in stating zero probability, clarifying that the intention was to refer to one.

Areas of Agreement / Disagreement

Participants express differing views on the interpretation of quantum theory in relation to black holes, with no consensus reached on the implications of probability and wavefunction behavior in this context.

Contextual Notes

Participants note that the discussion involves complex interactions between quantum mechanics and general relativity, with unresolved questions about the nature of black holes and the behavior of particles within them.

shaan_aragorn
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According to quantum theory the total probability of finding the particle somewhere in space is always zero. So if a particle vanishes in a black hole will that mean (psi)^2 = 0, which is illegal?
 
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shaan_aragorn said:
According to quantum theory the total probability of finding the particle somewhere in space is always zero.

Say what?

What version of "quantum theory" is this? Can you give an exact citation where you read this?

Zz.
 
I think s/he meant one, not zero.
 
shaan_aragorn said:
According to quantum theory the total probability of finding the particle somewhere in space is always zero. So if a particle vanishes in a black hole will that mean (psi)^2 = 0, which is illegal?

i'm going to assume that the poster meant 1, and not 0.

I don't know if you'll find a sufficient answer to your question...if a particle falls into a black hole, is it still in this universe? if yes, then the probability density over all space holds. if not, then is it even relevant, since the equation says nothing about this?

so a) i don't think that your scenario violates the equation and b) i also don't think that we can even speculate since, to my knowledge, black holes are still largely not understood entities.
 
At the risk of re-railing this thread, I think over time the integrated probability
of the particle being found outside the black hole would decrease, so yes
the hole would be "sucking up" [tex]\Psi[/tex]. If this is true, the inside of the hole should
be considered part of the "Universe" but an inaccessible part.

Let me add a serious twist to the question. What happens if one member
of an entangled pair of particles falls in? If even light can't escape, can
a measuement "from beneath" the event horizon bring about a new quantum state which
is still correlated with it's partner outside the black hole?

Conservation laws say it must.

General relativity says no information can come out of the hole. So
how does the change in the wavefunction take place outside based
on something that happens to the particle's correlated pair inside?
 
Last edited:
Gokul43201 said:
I think s/he meant one, not zero.

Yes, and even in that case, this is only the case in NON-relativistic QM - of a single particle - so we are far from a treatment where we have black holes :-)

I think that the answer is hence two-fold: the "psi defined everywhere and normalized to unity" is a concept that comes from non-relativistic quantum mechanics and hence not applicable to the situation at hand as such. Nevertheless, the crux of the problem remains, formulated differently: how can the motion of matter be described by a unitary operator in a black hole geometry (which is supposed to be reversible). That's the famous "quantum information riddle at a black hole".
As far as I know, we don't have a fully working theory of that. But some bricolage seems to show that the problem goes away (I think Hawking recently lost an encyclopedia over it, in a bet with another one) when you consider superpositions of "more or less flat space" and "hole forms and evaporates". These are exotic superpositions indeed, but I think Hawking had some indications that the overall operation can be unitary.
 
vanesch said:
(I think Hawking recently lost an encyclopedia over it, in a bet with another one)

Yes, he lost it to John Preskill. He was so glad he won, he dedicated part of his personal website to it :)

Preskill's VICTORY

regards
marlon
 
I don't know what I was thinking when i wrote zero! I meant one.
 

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