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Homework Help Overview

The discussion revolves around the properties of wave functions and eigenfunctions in the context of quantum mechanics, specifically relating to the Schrödinger equation and parity considerations.

Discussion Character

  • Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants explore the relationship between wave functions and eigenfunctions, questioning the conditions under which they can be even or odd. There are attempts to apply mathematical methods, such as the parity operator, to clarify these concepts.

Discussion Status

The discussion is ongoing, with various interpretations being explored. Some participants provide guidance on applying specific mathematical operators, while others express uncertainty about proving certain properties of wave functions.

Contextual Notes

There appears to be confusion regarding the definitions and requirements of wave functions versus eigenfunctions, as well as the implications of parity in quantum states.

woodywood
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How about ψ=ψeo (where, of course, ψ must statisfy Schroedinger equation), and then prove that ψe≠0 and ψo≠0 cannot be simultaneously true.
 
Emm...By wave function I assume you're talking about eigenfunction. Even though I can only prove that we can always find even solutions and odd solutions. As for what you said "prove wave function can be only even or odd." I really have no idea how to do it. I tried turin's method but didn't manage to get the desired answer. Let's wait for other people's opinion.
 
kof9595995 said:
Emm...By wave function I assume you're talking about eigenfunction. Even though I can only prove that we can always find even solutions and odd solutions. As for what you said "prove wave function can be only even or odd." I really have no idea how to do it. I tried turin's method but didn't manage to get the desired answer. Let's wait for other people's opinion.

No, I'm pretty sure he needs wavefunctions and not eigenfunctions

woodywood, you may want to consider the parity operator:

[tex] P\Psi(x,y,z,t)=\Psi(-x,-y,-z,t)[/tex]

and apply it to both the [itex]H\Psi[/itex] and [itex]\Psi[/itex] (after which you take the Hamiltonian of this latter one too--you should have [itex]PH\Psi[/itex] & [itex]HP\Psi[/itex]) then see how the two relate.
 
I'm pretty sure the OP needs eigenfunctions, not just wavefunctions in general. In fact, I'm pretty sure it is even more restricted to stationary eigenstates, because it is trivial to construct, by superposition, a general wavefunction that lacks definite parity, from any spectrum that includes both even and odd states.
 
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