KE operator and eigenfunctions

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Discussion Overview

The discussion revolves around whether the wavefunction \( u = x - iy \) is an eigenfunction of the kinetic energy operator in three dimensions. Participants explore the implications of the operator's action on the wavefunction, its physical realizability, and the mathematical definitions of eigenfunctions in quantum mechanics.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • Some participants argue that since applying the kinetic energy operator to \( u \) yields zero, it should be considered an eigenfunction with eigenvalue zero.
  • Others contend that \( u \) is not a proper eigenfunction because it is not square-integrable and does not satisfy the requirements of being orthogonal to other eigenfunctions with nonzero eigenvalues.
  • One participant notes that the wavefunction \( u \) is not physically realizable due to its behavior at infinity, which complicates its classification as an eigenfunction.
  • There is a discussion about the implications of degeneracy and pathological cases associated with eigenvalues of zero.
  • Some participants express confusion regarding the mathematical definition of eigenfunctions and whether normalization is a necessary condition for classification.
  • One suggestion is to impose boundary conditions to restrict the wavefunctions to be square-integrable, which would exclude \( u \) from being a valid solution.

Areas of Agreement / Disagreement

Participants do not reach a consensus on whether \( u \) qualifies as an eigenfunction. There are competing views regarding the definitions and conditions necessary for a function to be considered an eigenfunction in the context of quantum mechanics.

Contextual Notes

Limitations include the lack of clarity on the definitions of eigenfunctions in different contexts, the implications of normalization, and the potential confusion arising from introductory-level questions that introduce complex concepts without sufficient background.

Who May Find This Useful

This discussion may be of interest to students and self-learners in quantum mechanics, particularly those grappling with the concepts of eigenfunctions, operators, and the mathematical frameworks underpinning these ideas.

dyn
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I have just done a question and then looked at the solution which I don't get. The question gives a wavefunction as u = x - iy. It then asks if this function is an eigenfunction of the kinetic energy operator in 3-D. Applying this operator to u gives zero. I took this to mean that u is an eigenfunction with eigenvalue zero but the solution says that u is not an eigenfunction. Am I right or what is wrong with my argument ? Thanks
 
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It is zero - so is an eigenfunction with eigenvalue 0.

Its not physically realisable of course - but formally it is true.

Thanks
Bill
 
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The kinetic energy operator contains a Laplacian which involves 2nd derivatives in x , y , z so the function u becomes zero. The solution agreed with me that the KE operator acting on the function gives zero but I took that to mean u is an eigenfunction with eigenvalue zero but the solution says it is not an eigenfunction.
 
Well obviously it is - there is an error.

What it may be alluding to is its not physically realisable since its non zero at infinity. But then again so are the normal solutions.

Thanks
Bill
 
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Just to expand a bit further what's going on is you have run into a pathological case with degeneracy issues due to an eigenvalue of zero.

If you solve the free SE via separation of variables you end up with the multiple of wave solutions. But things get tricky when those waves have infinite wavelength as in your example. Work through the detail - I just did and its interesting.

Thanks
Bill
 
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I suppose the most straightforward argument that that is not an eigenvector is simply that it is not orthogonal to any of the eigenvectors with nonzero eigenvalue. Since the operator is Hermitian, it is not a proper eigenfunction (pun intended!)
 
fzero said:
I suppose the most straightforward argument that that is not an eigenvector is simply that it is not orthogonal to any of the eigenvectors with nonzero eigenvalue. Since the operator is Hermitian, it is not a proper eigenfunction (pun intended!)

In QM, the usual meaning of "eigenfunction" is a square-integrable function that has a definite value for some operator. But \psi = x - iy isn't square-integrable, so it's not a legitimate wave function. In many instances in quantum mechanics, it's the constraint that the wavefunction be square-integrable that forces its eigenvalues to be discrete. So usually when people talk about the eigenvalues of an operator O, they mean those values \lambda such that there is a square-integrable function \psi with O \psi = \lambda \psi.
 
stevendaryl said:
In QM, the usual meaning of "eigenfunction" is a square-integrable function that has a definite value for some operator. But \psi = x - iy isn't square-integrable, so it's not a legitimate wave function. In many instances in quantum mechanics, it's the constraint that the wavefunction be square-integrable that forces its eigenvalues to be discrete. So usually when people talk about the eigenvalues of an operator O, they mean those values \lambda such that there is a square-integrable function \psi with O \psi = \lambda \psi.

I am pretty sure that's the reason they wanted it excluded as an eigenfunction - it blows up to infinity at infinity. My concern is I have zero doubt wherever the OP got it from would have the usual wave solution to the free particle SE. That, while not blowing up to infinity, is nonetheless bounded there so is not valid either. This is the type of thing that can easily confuse a beginning student that actually thinks.

In fact it can confuse more advanced students until they come to grips with Rigged Hilbert Spaces.

Thanks
Bill
 
the question was from an introductory QM course. At that level Rigged Hilbert Spaces are unheard of. So at the introductory level is there a definite answer of eigenfunction or not ?
 
  • #10
dyn said:
the question was from an introductory QM course. At that level Rigged Hilbert Spaces are unheard of. So at the introductory level is there a definite answer of eigenfunction or not ?

No it isn't because it blows up at infinity so isn't normalisable - but like I said its inconsistent.

Thanks
Bill
 
  • #11
Sorry to be a pain here but the mathematical definition of eigenvectors doesn't put any requirements on whether they can be normailised or not. So if it is given as a wavefunction surely it is an eigenfunction with eigenvalue zero. Another part of the question asked whether Aexp(ikx) + Bexp(-ikx) was an eigenfunction of the kinetic energy operator and gave the answer that it was but this function is also not square-integrable
 
  • #12
dyn said:
Sorry to be a pain here but the mathematical definition of eigenvectors doesn't put any requirements on whether they can be normailised or not.

They are part of a normed vector space - that vector has infinite norm.

That function you gave has exactly the same issue but is considered valid - but it really isn't - that's the part that makes thinking students pull their hair out.

I could explain what's going on but it will involve a long sojourn into distribution theory:
https://terrytao.wordpress.com/2009/04/19/245c-notes-3-distributions/#more-2072

Really your teacher needs to explain it - post here with what he/she says - it should prove interesting.

Thanks
Bill
 
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  • #13
I don't have a teacher. Just self-studying. Obviously the QM case is never straight forward - no surprise there but I have a last question. If it was just a maths question regarding eigenvalues and I had a function similar to the KE operator and the function x-iy would it be an eigenfunction with eigenvalue zero ? Whenever I have done eigenfunction questions I have just had to check if it satisfies the eigenvalue equation. Is this not enough ? Do I now need to check normed vector spaces ?
 
  • #14
dyn said:
I don't have a teacher. Just self-studying. Obviously the QM case is never straight forward - no surprise there but I have a last question. If it was just a maths question regarding eigenvalues and I had a function similar to the KE operator and the function x-iy would it be an eigenfunction with eigenvalue zero ? Whenever I have done eigenfunction questions I have just had to check if it satisfies the eigenvalue equation. Is this not enough ? Do I now need to check normed vector spaces ?

You need to specify a space. To really understand this stuff you need to study linear algebra first, then Hilbert Spaces. For now my advice is simply to persevere and move on.

Thanks
Bill
 
  • #15
One way to deal with this kind of issue, at least in part, and without going to the full machinery of rigged Hilbert spaces, is to put the particle in a box with some boundary conditions, like the wave function must vanish on the walls, or periodic boundary conditions. Then require wave functions to be square integrable. Then x-iy is not an allowed wave function, because it doesn't satisfy the boundary conditions.

Whatever source the OP had that asked the original question is badly written and should be dropped.
 
  • #16
Avodyne said:
Whatever source the OP had that asked the original question is badly written and should be dropped.

Agreed.

Students should not be confronted with tricky issues like this to start with.

Thanks
Bill
 
  • #17
Thanks guys. I'm going to forget I ever saw that question.
 

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