Eigenvalue degeneracy in real physical systems

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Discussion Overview

The discussion revolves around the concept of eigenvalue degeneracy in real physical systems, particularly in the context of quantum mechanics and its implications for measurement and simulation. Participants explore the relationship between distinguishable and indistinguishable eigenvalues of Hermitian operators, the implications of degeneracy, and the computational aspects related to these concepts.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant questions whether real-world physical systems exist with indistinguishable eigenvalues, referencing the computable Universe hypothesis.
  • Another participant acknowledges the existence of quantum degeneracy but expresses uncertainty about its relevance to the original question.
  • Some participants discuss the association of degeneracies with symmetry or topological characteristics of quantum systems, citing examples such as time reversal in fermionic systems.
  • There is a discussion about the implications of measurement in quantum mechanics, particularly regarding the projection of states onto eigenspaces and the role of the measurement apparatus.
  • One participant mentions free particles as an example of completely degenerate energy eigenstates, while noting that interactions typically break accidental degeneracies in bound systems.
  • Concerns are raised about the computational aspects of determining eigenvalue multiplicity and its implications for measurement outcomes.
  • Some participants argue that knowing the eigenvalues to the precision of the measurement apparatus is sufficient for practical physics, regardless of whether the eigenvalues are degenerate or not.
  • There is a debate about the practical versus theoretical implications of detecting degeneracy and how it affects measurements.

Areas of Agreement / Disagreement

Participants express a range of views on the nature of eigenvalue degeneracy, its implications for measurement, and the computational aspects involved. There is no consensus on the relationship between these concepts, and multiple competing perspectives remain throughout the discussion.

Contextual Notes

Participants highlight the dependence of their arguments on specific interpretations of quantum mechanics, measurement processes, and the definitions of eigenvalues and eigenspaces. The discussion reflects a variety of assumptions and conditions that are not universally agreed upon.

  • #91
bhobba said:
I think you mean continuous variables.

? POVMs are problematic when coupled with continuous variables? I thought in exactly the opposite way. Nevertheless, I don't care about continuous variables. The key problem of this story is: you can't computationally define the operator's spectrum, let alone eigenstates/projections. That's it. There is certainly a way to avoid such a treatment.
 
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  • #92
ErikZorkin said:
I don't care about continuous variables. The key problem of this story is: you can't computationally define the operator's spectrum, let alone eigenstates/projections.

Then there is no issue.

QM has nothing to do with the practicalities of computing eigenvalues any more than classical mechanics has anything to do with the practicalities of numerically solving a differential equation. It leas to interesting things like the butterfly - but has nothing to do with the theories validity.

Thanks
Bill
 
  • #93
bhobba said:
Then there is no issue.

I am pretty sure! I thought I almost found an answer (POVMs), but then I got a bit concerned about the difficuleties as pointed out by rubi. Forgive me my ignorance, but do you apply spectral theorem when dealing the POVM--based QM?
 
  • #94
ErikZorkin said:
I am pretty sure! I thought I almost found an answer (POVMs), but then I got a bit concerned about the difficuleties as pointed out by rubi. Forgive me my ignorance, but do you apply spectral theorem when dealing the POVM--based QM?

No. Please, please read the link I gave. The spectral theorem only applies to what's called resolutions of the identity which are disjoint POVM's.

Thanks
Bill
 
  • #95
ErikZorkin said:
Nice example! But, again, it's not always possible to split the eigenvalues, as far as I understand.

I think as long as we have experiment as a guide, it is ok. The theorem you cite assumes finite dimensions and fails for infinite dimensions. For finite dimensions, the degeneracy cannot be greater than the dimensionality. Let the dimensionality be N. Then we guess the number of eigenvalues m to range between 1 .. N. For each guess, we compute the predictions. Although we will never know with certainty which m is correct, we just take the provisional answer to be the one that matches observations most closely.

This will be fine, because in practice, even for non-degenerate Hamiltonians, our ability to do a brute-force diagonalization is already insufficient. For typical Hamiltonians in condensed matter, we quickly run out of electrons in the universe that can do the computation, eg. http://fqxi.org/data/essay-contest-files/Swingle_fqxi2012.pdf.
 
  • #96
vanhees71 said:
QT as a mathematical theory is consistent

What's QT? Quantum mechanics or QFT? First of all, the very formal foundation of QM is not done yet. Second, you can't prove its consistency. Because your axiomatic system would necessarily include arithmetic whose consistency can't be proven in arithmetic alone.
 
  • #97
ErikZorkin said:
First of all, the very formal foundation of QM is not done yet.

Von Neumann sorted that out ages ago. Dirac's elegant formulation is now rigorous since Rigged Hilbert Spaces have been worked out.

Please, please read a good book on QM such as Ballentine.

Thanks
Bill
 
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  • #98
  • #99
ErikZorkin said:
Because your axiomatic system would necessarily include arithmetic whose consistency can't be proven in arithmetic alone.

Godels theorem is irrelevant in this context. Its as consistent as any other physical theory ie as consistent as geometry, arithmetic etc etc.

Thanks
Bill
 
  • #100
bhobba said:
Von Neumann sorted that out ages ago. Dirac's elegant formulation is now rigorous since Rigged Hilbert Spaces have been worked out.

Please, please read a good book on QM such as Ballentine.

Thanks
Bill

Well, the axioms of QM are far from what's called a formal mathematical axiom. cf. axioms of ZFC
 
  • #101
bhobba said:
Godells theorem is irrelevant in this context. Its as consistent as any other physical theory ie as consistent as geometry, arithmetic etc etc.

Thanks
Bill

Consistency of arithmetic can't even be proven. I believe you mean not the consistency, as mathematicians define it but rather informally since it allows for accurate predicitons.
 
  • #104
ErikZorkin said:
Well, the axioms of QM are far from what's called a formal mathematical axiom. cf. axioms of ZFC

If that what you want then here is the book:
https://www.amazon.com/dp/0387493859/?tag=pfamazon01-20

Be warned - it what mathematicians call non trivial - meaning its HARD. But it does what you want.

Thanks
Bill
 
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  • #105
ErikZorkin said:
Postulates are not formal axioms

Sure, but no one doubts they can be formulated in ZFC.
 
  • #106
ErikZorkin said:
Postulates are not formal axioms

For that matter, the article you cite in the OP is not a formal proof.
 
  • #107
Then why are there still so many attempts at axiomatization of QM?
 
  • #108
atyy said:
For that matter, the article you cite in the OP is not a formal proof.

No, sir, it is!
 
  • #109
For this matter, such works as this are closer to what's called formal axiomatic foundation.

But I fear that this discussion went in a wrong direction a bit.
 
  • #110
ErikZorkin said:
Then why are there still so many attempts at axiomatization of QM?

There are two major lines of foundational research nowadays.

The first takes the Copenhagen interpretation (and does not attempt to solve the measurement problem), and the axioms as given for example in the articles by Paris and Busch as correct. The research is to find a more "intuitive" derivation of the axioms, eg. http://arxiv.org/abs/1011.6451 or http://arxiv.org/abs/1303.1538 or http://arxiv.org/abs/1403.4621.

The second tries to solve the measurement problem of Copenhagen, eg. Bohmian mechanics, Many-Worlds, Consistent Histories etc
 
  • #111
ErikZorkin said:
Consistency of arithmetic can't even be proven. I believe you mean not the consistency, as mathematicians define it but rather informally since it allows for accurate predicitons.

Precisely what has that got to with QM not being fully worked out yet? All physical theories are like that even when expressed in highly abstract mathematics such as Symplectic geometry. Why are you shifting context?

Thanks
Bill
 
  • #112
ErikZorkin said:
No, sir, it is!

Of course it is not. It is ordinary mathematical proof.
 
  • #113
atyy said:
Of course it is not. It is ordinary mathematical proof.

Well, since it concerns computable analysis, the proof is constructive and as such can be formalized automatically. That's called proof normalization. And there is software out there that does the job. It's the calssical proof of the spectral theorem that can't be ever formalized.
 
  • #114
ErikZorkin said:
For this matter, such works as this are closer to what's called formal axiomatic foundation.

But I fear that this discussion went in a wrong direction a bit.

Yes, the 3 links I gave in post #110 and that bhobba gave in #104 are in this spirit.

However, that people still work on deriving the axioms does not mean the axioms are not already at the same level of rigour as the article in the OP. It just means that people are looking for more "intuitive" ways to derive the axioms.
 
  • #115
bhobba said:
Why are you shifting context?

Well, if it was I, who shifted the focus, I apologize.
 
  • #116
ErikZorkin said:
Well, since it concerns computable analysis, the proof is constructive and as such can be formalized automatically. That's called proof normalization. And there is software out there that does the job. It's the calssical proof of the spectral theorem that can't be ever formalized.

Sure that's the same as I would say for the axioms of QM.
 
  • #117
atyy said:
Sure that's the same as I would say for the axioms of QM.

For God's sake of course NO!
 
  • #118
ErikZorkin said:
For God's sake of course NO!

Why not?
 
  • #119
ErikZorkin said:
For this matter, such works as this are closer to what's called formal axiomatic foundation..

I think the book I suggested does just that. Its based on the formal logic approach of Von Neumann who was hardly ignorant of such things. It starts out from logic in a formal sense.

Thanks
Bill
 
  • #120
May be way off base here, but is what you're asking equivalent to "are there physical systems for which a complete set of mutually commuting observables is known not to exist?"
 

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