Determination of past vs future probability

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Discussion Overview

The discussion explores the differences and similarities between estimating probabilities of future events versus past events, particularly in the context of quantum mechanics and general relativity. It touches on theoretical frameworks, interpretations of quantum mechanics, and the implications of wavefunction collapse.

Discussion Character

  • Exploratory
  • Debate/contested
  • Technical explanation

Main Points Raised

  • Some participants propose that theoretically, using the time-dependent Schrödinger equation, estimating probabilities for future and past events should be similar, differing only by the time variable.
  • Others argue that once an event has occurred, the probability wave collapses, leaving no probability associated with that event, unless it has not been observed.
  • One participant questions whether wavefunction collapse could occur in reverse, suggesting that quantum mechanics and general relativity are time symmetric.
  • Another participant explains that quantum mechanics has two developments: a smooth, reversible evolution of the wavefunction when unobserved, and an irreversible collapse upon observation, leading to discussions about interpretations like the many-worlds theory.
  • Some participants mention that the many-worlds interpretation is not the only time-symmetric model, referencing time-symmetric Bohmian models and their implications for understanding time and causation.
  • A participant suggests that memory and prediction could be viewed as time-reversed processes relative to each other.

Areas of Agreement / Disagreement

Participants express multiple competing views regarding the nature of probability in quantum mechanics and the implications of wavefunction collapse. The discussion remains unresolved with no consensus on the interpretations presented.

Contextual Notes

Limitations include the dependence on interpretations of quantum mechanics, the unresolved nature of wavefunction collapse, and the varying perspectives on time symmetry in different models.

Loren Booda
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How is estimating the probability that a future event might happen different from estimating the probability that a past event might have happened?
 
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I haven't taken a full fledged quantum class (that's next year for me),
but I know that if I answer, someone will tell me I'm wrong and thus, answer your question, so I'll conjecture purely for your sake... :blushing:

There's two ways I can think of to look at this. If we look at it theoretically, like say, take a time-dependent schroedinger equation, that it should be exactly the same, just at a different time, t. In this case, you'd have two t's for your limit of integration, t future, and t past.

I think, however, in reality, if an event has already occurred, than the probability wave has already collapsed. The event has already occurred, so there is no probability attached to it, just a definite.

Unless of course, you haven't observed the event, than it still exists as a probability until you observe it.
 
Both quantum mechanics (concerning microscopic probability) and general relativity (concerning macroscopic probability) are time symmetric. I would guess that excludes wavefunction collapse. Could wavefunction collapse ever occur in reverse?
 
Quantum mechanics, as the formalism is normally presented, has two kinds of development. The development of the wavefunction when not observed is smooth ("unitary", preserving probability measures). It is therefore reversable.

The other development is the "collapse of the wavefunction" as a result of observation. This is NOT reversable or unitary. Some people are offended by the existence of this awkwardness, and would seek to eliminate it and have an all-unitary physics. To do this leads to the Everett many-worlds theory.
 
selfAdjoint said:
Quantum mechanics, as the formalism is normally presented, has two kinds of development. The development of the wavefunction when not observed is smooth ("unitary", preserving probability measures). It is therefore reversable.

The other development is the "collapse of the wavefunction" as a result of observation. This is NOT reversable or unitary. Some people are offended by the existence of this awkwardness, and would seek to eliminate it and have an all-unitary physics. To do this leads to the Everett many-worlds theory.

Have you ever read "In search of Schroedinger's Cat" by Jon Gribbins?

He supports the many-worlds theory. Interesting book.
 
Could memory and prediction be processes time-reversed relative to each other?
 
selfAdjoint said:
The other development is the "collapse of the wavefunction" as a result of observation. This is NOT reversable or unitary. Some people are offended by the existence of this awkwardness, and would seek to eliminate it and have an all-unitary physics. To do this leads to the Everett many-worlds theory.
the many-worlds model is not the only time-symmetric attempt at an interpretation of QM (and not all many-worlds interpretations are necessarily time-symmetric). There are time-symmetric Bohmian models also. Here is just a couple of such papers :

http://arxiv.org/PS_cache/quant-ph/pdf/0210/0210207.pdf#search=%22time%20symmetric%20bohmian%20mechanics%22

http://arxiv.org/abs/quant-ph/0601095

and from a paper entitled "Arrows of Time in Bohmian Mechanics" by Shelly Goldstein and Roderich Tumulka :
Bohmian mechanics is a theory about point particles moving in space according to a law of motion (an ordinary differential equation) involving a quantum mechanical wave function. It is a consequence of this law of motion that in a typical world governed by Bohmian mechanics, observers would observe for the results of their experiments exactly the frequencies predicted by quantum mechanics. Since the theory is time symmetric, arrows of time are grounded in the specialness of the initial wave function. A more complex situation arises in some recently studied relativistic variants of the law of motion: they imply backwards causation, though only in a very special and limited way that is free of causal paradoxes.

And in a time-symmetric deterministic interpretation, estimating probabilities of future events is essentially the same as estimating probabilities of past events - limited only by our epistemic perspective.

Best Regards
 
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