Kinetic and Potential energy operators commutation

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SUMMARY

The discussion centers on the commutation of kinetic energy (KE) and potential energy (PE) operators within the context of the Schrödinger equation, specifically the Hamiltonian operator H. Participants clarify that while KE and PE do not commute, they can still share a common wave function, Psi, when considered as part of the total Hamiltonian. The key takeaway is that the eigenfunctions of the total Hamiltonian do not need to be eigenfunctions of the individual operators, which is a fundamental concept in quantum mechanics. An example involving matrices A and B illustrates this principle effectively.

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Dinara
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Hi All,
Perhaps I am missing something. Schrödinger equation is HPsi=EPsi, where H is hamiltonian = sum of kinetic energy operator and potential energy operator. Kinetic energy operator does not commute with potential energy operator, then how come they share the same wave function Psi? The operators that do not commute cannot have the same wave function. Please help me to figure this out. Thanks.
 
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Does the sum of them commute?
 
The sum doesn't matter. The thing is (KE+PE) psi is a wrong expression - since KE and PE operators have to have different wave functions. Yet, in every single quantum chemistry text it is this (KE+PE) psi that is solved for the hydrogen atom!
 
Why do you say that if they occur together?
 
Dinara said:
The sum doesn't matter. The thing is (KE+PE) psi is a wrong expression - since KE and PE operators have to have different wave functions. Yet, in every single quantum chemistry text it is this (KE+PE) psi that is solved for the hydrogen atom!

Do you know what functional analysis is ?
 
No - I don't. Is the answer to my question in functional analysis?
 
Dinara said:
The sum doesn't matter.
Sorry, but it does matter.

The thing is (KE+PE) psi is a wrong expression
No, it's a correct expression. One finds eigenfunctions for the total Hamiltonian. It doesn't matter that such an eigenfunction might not also be an eigenfunction for KE and PE separately.
 
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dextercioby said:
Pretty much so.
strangerep said:
Sorry, but it does matter.

No, it's a correct expression. One finds eigenfunctions for the total Hamiltonian. It doesn't matter that such an eigenfunction might not also be an eigenfunction for KE and PE separately.
This does not make sense! (KE+PE)(psi) = KE (psi) + PE (psi), It does matter that eigenfunction has to be an eigenfunction of both KE and PE.
 
  • #10
No! You obviously misunderstood the concept of eigenvectors and eigenvalues completely. Which book are you using to study QT? I'm pretty sure, this utmost important topic is treated there. So please, have a look again and then come back with concrete questions.

Here you should really understand that if ##\hat{H}=\hat{H}_1+\hat{H}_2## then the eigenvectors of ##\hat{H}## need not be eigenvectors of ##\hat{H}_1## or ##\hat{H}_2##. That's only the case if ##\hat{H}_1## and ##\hat{H}_2## commute. That's also a very important concept: Two self-adjoint operators have a common complete set of orthonormalized eigenvectors if and only if they commute, and only then the two observables represented by these two operators are compatible, i.e., you can define states (the common eigenstates of the two operators), for which both observables take determined values, namely the corresponding eigenvalues.
 
  • #11
Dinara said:
This does not make sense!

Maybe not to you, but it's easy to find examples. Here's one: the ground state wave function of the electron in the idealized hydrogen atom (i.e., a spinless "electron" in the Coulomb potential of the nucleus). This wave function is not an eigenstate of either KE or PE separately, but it is an eigenstate of the total Hamiltonian H.
 
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  • #12
Dinara said:
This does not make sense! (KE+PE)(psi) = KE (psi) + PE (psi), It does matter that eigenfunction has to be an eigenfunction of both KE and PE.
Consider the following operators:$$A=\begin{bmatrix}0&1\\1&0\end{bmatrix}~~B=\begin{bmatrix}1&0\\0&-1\end{bmatrix}~~C=A+B=\begin{bmatrix}1&1\\1&-1\end{bmatrix}$$
The eigenvectors of A are ##\begin{bmatrix}1\\1\end{bmatrix}## and ##\begin{bmatrix}1\\-1\end{bmatrix}##
The eigenvectors of B are ##\begin{bmatrix}1\\0\end{bmatrix}## and ##\begin{bmatrix}0\\1\end{bmatrix}##
The eigenvectors of C are ##\begin{bmatrix}1\\ \sqrt{2}-1\end{bmatrix}## and ##\begin{bmatrix}-1\\ \sqrt{2}+1\end{bmatrix}##
A and B do not commute and have no common eigenvectors. Nonetheless, their sum C has eigenvectors and they are not eigenvectors of either A or B. It's the same thing with the Hamiltonian, which is the sum of the non-commuting kinetic and potential energy operators.

[It would be a good exercise to check my algebra here]
 
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  • #13
Nugatory said:
[It would be a good exercise to check my algebra here]
Heh, I was about to suggest the exact same exercise (so I'd already "checked" your algebra before your posted). :oldwink:

[Moderator's note: off topic comment deleted.]
 
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  • #14
Nugatory said:
Consider the following operators:$$A=\begin{bmatrix}0&1\\1&0\end{bmatrix}~~B=\begin{bmatrix}1&0\\0&-1\end{bmatrix}~~C=A+B=\begin{bmatrix}1&1\\1&-1\end{bmatrix}$$
The eigenvectors of A are ##\begin{bmatrix}1\\1\end{bmatrix}## and ##\begin{bmatrix}1\\-1\end{bmatrix}##
The eigenvectors of B are ##\begin{bmatrix}1\\0\end{bmatrix}## and ##\begin{bmatrix}0\\1\end{bmatrix}##
The eigenvectors of C are ##\begin{bmatrix}1\\ \sqrt{2}-1\end{bmatrix}## and ##\begin{bmatrix}-1\\ \sqrt{2}+1\end{bmatrix}##
A and B do not commute and have no common eigenvectors. Nonetheless, their sum C has eigenvectors and they are not eigenvectors of either A or B. It's the same thing with the Hamiltonian, which is the sum of the non-commuting kinetic and potential energy operators.

[It would be a good exercise to check my algebra here]
Nugatory said:
Consider the following operators:$$A=\begin{bmatrix}0&1\\1&0\end{bmatrix}~~B=\begin{bmatrix}1&0\\0&-1\end{bmatrix}~~C=A+B=\begin{bmatrix}1&1\\1&-1\end{bmatrix}$$
The eigenvectors of A are ##\begin{bmatrix}1\\1\end{bmatrix}## and ##\begin{bmatrix}1\\-1\end{bmatrix}##
The eigenvectors of B are ##\begin{bmatrix}1\\0\end{bmatrix}## and ##\begin{bmatrix}0\\1\end{bmatrix}##
The eigenvectors of C are ##\begin{bmatrix}1\\ \sqrt{2}-1\end{bmatrix}## and ##\begin{bmatrix}-1\\ \sqrt{2}+1\end{bmatrix}##
A and B do not commute and have no common eigenvectors. Nonetheless, their sum C has eigenvectors and they are not eigenvectors of either A or B. It's the same thing with the Hamiltonian, which is the sum of the non-commuting kinetic and potential energy operators.

[It would be a good exercise to check my algebra here]

Thank you so much! Great example!
 
  • #15
Everyone, please keep the discussion civil. I have deleted an off topic comment and an off topic post.
 

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