Wave function is a combination of eigenfunction?

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Discussion Overview

The discussion revolves around the nature of wave functions in quantum mechanics, particularly whether they are combinations of eigenfunctions and the implications of measurement on these states. Participants explore various interpretations of quantum mechanics, including the orthodox interpretation and the many-worlds interpretation, while addressing the complexities surrounding the concept of wave function collapse.

Discussion Character

  • Debate/contested
  • Conceptual clarification
  • Exploratory

Main Points Raised

  • Some participants assert that the orthodox interpretation, which involves wave function collapse into an eigenfunction upon measurement, remains valid.
  • Others argue that there are competing interpretations, such as the many-worlds interpretation, and that no interpretation can be definitively proven right or wrong.
  • One participant expresses skepticism about the necessity of the collapse assumption in practical quantum theory applications, suggesting it should be avoided.
  • Another participant contends that while the collapse interpretation is problematic, it cannot be mathematically or experimentally disproven.
  • Concerns are raised regarding the implications of the EPR paradox on realistic interpretations of wave functions, suggesting that a minimal statistical interpretation may be more appropriate.
  • Some participants discuss specific measurement scenarios, such as the polarization of photons, to illustrate that not all measurements lead to a projection into an eigenstate.
  • There is a distinction made between measurement and preparation, with some arguing that certain measurement processes can be viewed as preparations rather than direct measurements.
  • Participants debate the validity of the collapse interpretation in light of experimental evidence, with some asserting that no experiment has definitively disproven it.

Areas of Agreement / Disagreement

Participants express a range of views on the interpretations of quantum mechanics, with no consensus reached. While some agree on the validity of the orthodox interpretation, others present competing perspectives, leading to an unresolved discussion on the nature of wave function collapse and measurement.

Contextual Notes

The discussion highlights the complexities and nuances in interpretations of quantum mechanics, including the dependence on philosophical considerations and the challenges in proving or disproving various interpretations. Limitations in the arguments presented include unresolved assumptions about the nature of measurements and the implications of different interpretations.

wasi-uz-zaman
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hi, i read in quantum mechanics wave function is a combination of eigenfunctions and according to Orthodox interpretation measurement causes the wave function to collapse into one of the eigenfunction of the quantity being measured. Is this explanation still valid?
 
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This interpretation as "orthodox interpretation" is still valid. But there are other, competing interpretations like "many-worlds". No interpretation is right or wrong. They are all in agreement with physics (that's why these are competing intpretations, not competing theories)
 
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The collapse is by no means unproblematic. In my opinion it's not a necessary assumption for the use of quantum theory to real physical situations and thus one should avoid it. It's also for sure not even true. Often the measured object, like a photon, is even destroyed in the measuring process.Then for sure after such a measurement the state of the system is not in an eigenstate of the measured observable's representing operator.
 
vanhees71 said:
Often the measured object, like a photon, is even destroyed in the measuring process.Then for sure after such a measurement the state of the system is not in an eigenstate of the measured observable's representing operator.
Where's the problem? When the photon is destroyed the state is in the zero-photon subspace.

The problem with your argument is the following: you can construct interpretations of the state vector which are in conflict with some other interpretations or philosophical considerations regarding "reality" etc.; but afaik you cannot prove or falsify (mathematically or experimentally) that the collapse interpretation is physically wrong.

Therefore I agree with
vanhees71 said:
The collapse is by no means unproblematic. In my opinion it's not a necessary assumption for the use of quantum theory to real physical situations and thus one should avoid it.
but I do not agree with
vanhees71 said:
It's also for sure not even true.
 
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But what about the good old EPR paradoxon? The socalled "realistic" interpretations of the state, i.e., of the wave function or the state vector, representing a pure state, (or perhaps even the general case of a statistical opertor?) as a physical entity leads to the trouble with Einstein causality as detailed in EPR's famous paper.

So I think it's more save to follow the minimal statistical interpretation (or ensemble interpretation), according to which the state describes the probabilistic features of physically real systems (say an electron, just to avoid the additional quibbles with massless particles like photons), which can only be assessed by preparing ensembles of systems in the state to be investigated.

Formally, then not the abstract entities of the theory (vectors/statistical operators in Hilbert space representing the states and self-adjoint operators representing the observables) but equivalence classes of definite preparation procedures represent the "real system".
 
vanhees71 said:
But what about the good old EPR paradoxon? The socalled "realistic" interpretations of the state, i.e., of the wave function or the state vector, representing a pure state, (or perhaps even the general case of a statistical opertor?) as a physical entity leads to the trouble with Einstein causality as detailed in EPR's famous paper.

So I think it's more save to follow the minimal statistical interpretation (or ensemble interpretation), according to which the state describes the probabilistic features of physically real systems (say an electron, just to avoid the additional quibbles with massless particles like photons), which can only be assessed by preparing ensembles of systems in the state to be investigated.

Formally, then not the abstract entities of the theory (vectors/statistical operators in Hilbert space representing the states and self-adjoint operators representing the observables) but equivalence classes of definite preparation procedures represent the "real system".
I could agree to everything what you are saying regarding interpretations, reality, their problems etc., but that's not the point. I think I was clear in my last post: you can neither disprove (mathematicall) nor falsify (experimentally) the collapse interpretation. Therefore I do not agree with
vanhees71 said:
It's also for sure not even true.
 
But, when I measure, e.g., a photon's polarization by the observation that it is absorbed by a polarization foil, I do not have a photon in the corresponding polarization. This is a very simple example for the fact that not all measurements lead to a projection into the corresponding eigenstate.

There are some measurement procedures, known as ideal von Neumann measurements, that allow the filtering into a given eigenstate of the measured quantity, e.g., the Stern-Gerlach experiment, where you split an unpolarized beam of (neutral) particles in spatially well separated angular-momentum eigenstates (through entanglement of position and angular momentum!). Filtering out one beam then leads to a pure angular-momentum eigenstate. In this sense, sometimes you have a kind of collapse. Such procedures I'd rather call a preparation than a measurement.
 
if the photon is absorbed then there is no photon anymore and therefore it makes no sense to say that it has some polarization; it collapsed to a "no photon eigenstate"

but if the photon passes the polarization filter it has exactly its polarization - which does not mean that you have prepared it, as you say; but later you can check the polarization n times applying n filters - and the photon will pass all n filters; therefore it is safe to say that the photon collapsed into a corresponding "polarization eigenstate"
 
Why don't you call that a preparation?
 
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It doesn't matter how I call it; I don't see the conflict between the "collaps interpretation" and any experiment; I think nobody does

Some claim that "Copenhagen" is out, has problems, ballast, is unphysical, or that MWI means "taking QM literally", that MWI has less ontological ballast (others claim that MWI has more ontological ballast), ...

But I do not see any experiment that proves "Copenhagen" or "collaps" to be wrong; therefore I do not agree to your sentence that "It's also for sure not even true." If by "it" you mean the interpretation than these are only words. But if you mean physics than you are not right, otherwise you would have to show us an experiment which falsifies "Copenhagen"
 

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