How to understand operators representing observables are Hermitian?

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Discussion Overview

The discussion revolves around the nature of operators representing observables in quantum mechanics, specifically focusing on the Hermitian property of these operators and the implications for their eigenfunctions. Participants explore theoretical aspects, mathematical reasoning, and conceptual clarifications regarding the momentum operator and its eigenfunctions in different contexts, including the 1D infinite well and the Rigged Hilbert space formalism.

Discussion Character

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

Main Points Raised

  • Some participants assert that all operators representing observables are Hermitian, contingent on the system being described by a wavefunction or a vector in L2.
  • One participant questions the validity of the momentum operator's eigenfunctions, noting that they do not vanish at infinity and thus may not represent physical states.
  • Another participant discusses the implications of the Rigged Hilbert space formalism, suggesting that physically realizable states are test functions, while other functions can approximate them.
  • There is a debate about the completeness of eigenfunctions for self-adjoint operators, with some arguing that self-adjoint operators in infinite dimensions may not have a complete set of eigenfunctions.
  • Participants discuss the specific case of the momentum operator in the 1D infinite well, questioning whether it has eigenfunctions under the given boundary conditions.
  • Clarifications are made regarding the distinction between Hermitian and self-adjoint operators, particularly in relation to their spectral properties.
  • One participant references a statement from Griffiths' book about eigenvectors spanning the space, raising concerns about its applicability in the context of the infinite well and the momentum operator.

Areas of Agreement / Disagreement

Participants express differing views on the completeness of eigenfunctions for self-adjoint operators, particularly in infinite-dimensional spaces. There is no consensus on whether the momentum operator has eigenfunctions in the context of the 1D infinite well, and the discussion remains unresolved regarding the implications of the Rigged Hilbert space formalism.

Contextual Notes

Participants highlight limitations in understanding the spectral properties of operators, particularly the need to consider the domains of unbounded operators and the implications for their Hermitian and self-adjoint properties.

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  • #32
The book written by the Nobel Prize winner is intended as a gentle presentation of the formalism/content of the theory and its main results. It's not about the mathematical foundations/formulation of quantum mechanics. That's why no distinction is made between hermitean and self adjoint. A distinction exists and is made at a higher level of rigor than the books by Ballentine, Grifftihs, Weinberg, Sakurai, Merzbacher, Messiah, Cohen-Tannoudji, etc.

(2) as you wrote is the second postulate (the 1st postulate regards the states, the second is about observables, the third is usually the Born rule and the 4th is the evolution equations for states/observables).
 
  • #33
George Jones said:
When first learning quantum mechanics, I recommend against delving too deeply into these issues.

I fully concur.

When I first learned QM properly I became caught up with this damnable Dirac Delta function. It took me on a long detour into Rigged Hilbert spaces and such. I emerged with my questions answered but the cost was my understanding of QM took a hiatus.

Much better in my view is put such things aside at the moment, knowing they have an answer, but it requires a more advanced background. You can get that background by reading up on some functional analysis. I have a few texts, but one I like is Applied Analysis by John Hunter.

While doing that Ballentine is reasonably mathematically complete and would give you a good foundation in the physics.

Thanks
Bill
 
Last edited:
  • #34
George Jones said:
When first learning quantum mechanics, I recommend against delving too deeply into these issues.

For the difference between "selfadjoint" and "hermitian", see

https://www.physicsforums.com/showthread.php?p=1887619#post1887619

Excuse me, in your post #6 https://www.physicsforums.com/showthread.php?p=1887619#post1887619, you said "all Hermitian operators are self-adjoint, but not all self-adjoint operators are Hermitian. "

However my understanding is the opposite: "all self-adjoint operators are Hermitian, but not all Hermitian operators are self-adjoint". Did I get it wrong?
 
  • #35
Yes.
 
  • #36
For the momentum operator a particle in a 1-dimensional infinite well, see "Self-adjoint extensions of operators and the teaching of quantum mechanics",

http://arxiv.org/abs/quant-ph/0103153
 
  • #37
George Jones said:
Yes.

No, I disagree. You have as definition that hermitian immediately implies that it's bounded. I don't think this is a very common definition. All definitions I've seen is that symmetric and hermitian are equivalent, and thus hermitian is not necessarily bounded. See for example Reed & Simon, page 255. So I would say that the OP has it exactly right.
 
  • #38
R136a1 said:
No, I disagree. You have as definition that hermitian immediately implies that it's bounded. I don't think this is a very common definition. All definitions I've seen is that symmetric and hermitian are equivalent, and thus hermitian is not necessarily bounded. See for example Reed & Simon, page 255. So I would say that the OP has it exactly right.

Well, I have (at least) a couple of books that only use "Hermitian" with respect to bounded operators:

1) Introductory Functional Analysis by Kreyszig (the text for a course I took as a student);

2)Hilbert Space Operators in Quantum Physics by Blank, Exner, and Havilcek.

Both of these references define symmetric unbounded operators, but don not associate the term "Hermitian" with such operators.

Some references (e.g., Riesz and Nagy) do not use "Hermitian" at all. In the recent book "Quantum Theory for Mathematicians" by Hall, "Hermitian" is used only in the sentence "Physicists refer to self-adjoint operators as Hermitian." Hall does not use "Hermitian" (but does use symmetric and sel-adjoint) when doing actual functional analysis.
 
  • #39
That's my mind, too. <Hermitean> is not modern terminology in functional analysis. It belongs now only in linear algebra which is done in finite dimensional spaces, of course. It stands in front of the words matrix+matrices.
 

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