Can a Measurable Function V Exist for Given Quantum Energy Eigenvalues?

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Discussion Overview

The discussion revolves around the existence of a measurable function \( V \) that can yield a specified set of quantum energy eigenvalues through a Hamiltonian operator. The context includes aspects of quantum mechanics, differential equations, and operator theory, with participants exploring the implications and relationships to other mathematical concepts, such as the Riemann zeta function and the Berry Conjecture.

Discussion Character

  • Exploratory
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant poses the question of whether a measurable function \( V:\mathbb{R}\to\mathbb{R} \) exists such that the eigenvalues of the operator \( H = -\frac{1}{2}\partial_x^2 + M_V \) correspond to a given set of real numbers \( E(n) \).
  • Another participant questions if this inquiry is equivalent to asking whether a Hamiltonian can have eigenvalues that are the zeros of the Riemann zeta function, though they express uncertainty about the connection.
  • A participant introduces a non-linear mapping related to eigenvalue problems, suggesting that every eigenvalue problem can be framed in terms of finding zeros of some function.
  • Clarifications arise regarding the distinction between eigenvalues and eigenvectors in the context of the original question.
  • One participant relates the problem to the Berry Conjecture, noting that the conjecture may require a more general form of Hamiltonian than what is being considered.
  • References to recent literature are made, including a paper discussing Landau levels and Riemann zeros, indicating ongoing research in related areas.

Areas of Agreement / Disagreement

Participants express differing views on the relationship between the original question and concepts like the Riemann zeta function and the Berry Conjecture. The discussion remains unresolved, with no consensus on the existence of such a measurable function \( V \) or its implications.

Contextual Notes

Participants highlight the complexity of the problem, noting potential dependencies on definitions and the need for a more general form of Hamiltonian in some contexts. There are also unresolved connections to other mathematical constructs, such as the zeros of the Riemann zeta function.

jostpuur
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This is about quantum mechanics, but it is sufficiently difficult existence question dealing with DE and operator theory, that I think it fits the DE subforum the best:

Let [tex]E:\mathbb{N}\to\mathbb{R}[/tex] be an arbitrary map, but so that [tex]\textrm{Im}(E)[/tex] is bounded from below. Does there exist a measurable function [tex]V:\mathbb{R}\to\mathbb{R}[/tex] such that the eigenvalues of the operator

[tex] H = -\frac{1}{2}\partial_x^2 + M_V[/tex]

are the given [tex]E(n)[/tex]?

Here [tex]M_V:\mathbb{C}^{\mathbb{R}}\to \mathbb{C}^{\mathbb{R}}[/tex] is the multiplication operator [tex](M_V\psi)(x) = V(x)\psi(x)[/tex].

For the sake of rigor we can give the following definition for the domain of H,

[tex] D(H) = \{\psi\in L^2(\mathbb{R},\mathbb{C})\;|\; \psi\;\textrm{is piece wisely}\;C^2\quad\textrm{and}\quad \int dx\;\Big|-\frac{1}{2}\partial_x^2\psi(x) + V(x)\psi(x)\Big|^2 < \infty\}[/tex]

So H is a mapping [tex]H:D(H)\to L^2(\mathbb{R},\mathbb{C})[/tex].
 
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I'm not a math person, so just a wild question:is your question equivalent to asking whether a Hamiltonian exists whose eigenvalues are the zeros of the Riemann zeta function?
 
I don't know enough of Riemann zeta function to answer that. I'll say that I don't know how precisely my question would be related to it now.

If [tex]T:\mathcal{H}\to\mathcal{H}[/tex] is some linear operator on some inner product space, we can define a new non-linear mapping

[tex] f:\mathcal{H}\to\mathcal{H},\quad f(\psi) = T\psi - \frac{(\psi|T\psi)}{\|\psi\|^2}\psi[/tex]

which has the property

[tex] f(\psi)=0\quad\Leftrightarrow\quad T\psi\propto\psi,[/tex]

so in this sense every eigenvalue problem is related to a problem of finding zeros of some function. So... who knows?
 
Now I read your post more carefully. You were speaking about eigenvalues being zeros of some function, and I was about eigenvectors being zeros of some function. So this seems to be different thing.
 
jostpuur said:
Now I read your post more carefully. You were speaking about eigenvalues being zeros of some function, and I was about eigenvectors being zeros of some function. So this seems to be different thing.

Let's see, I understood your question to be:
Given a countable set of real numbers, does a Hamiltonian exist such that its eigenvalues are the elements of the given set?

(A little more strictly, you asked if a V(x) exists such that the eigenvalues of the Hamiltonian are the elements of the given set.)
 
I see. So the problem I described, seems to be similar to the Berry Conjecture.
 
jostpuur said:
I see. So the problem I described, seems to be similar to the Berry Conjecture.

Hmm, reading the Berry conjecture, it seems they need a more general form of the Hamiltonian than in your problem. I wonder whether they've already ruled out "nice" Hamiltonians, and if so, how they did that.
 

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