Operator that interchanges variables

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Homework Help Overview

The discussion revolves around an operator L in the context of a Quantum Mechanics homework problem. The operator is defined such that it interchanges the variables of a function f(x,y), leading to the eigenvalue equation Lf = λf. Participants explore the properties of the eigenfunctions and the possible eigenvalues associated with this operator.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants consider the implications of the operator's action on eigenfunctions, particularly focusing on symmetric and antisymmetric functions. Questions arise regarding the completeness of these classifications and the potential existence of other eigenfunctions.

Discussion Status

The discussion is active, with participants providing hints and exploring various properties of the operator. Some guidance has been offered regarding the implications of applying the operator multiple times and the nature of the eigenvalues.

Contextual Notes

There is an ongoing examination of the conditions under which eigenfunctions exist, particularly concerning the trivial solution and the implications of the operator being its own inverse.

ELESSAR TELKONT
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Homework Statement



I suppose that this is not directly a quantum mechanical problem, but this have been assigned as homework for the Quantum Mechanics course.

Let be an operator L and eigenvalue equation Lf=\lambda f. This operator, applied to a function f(x,y), interchanges the variables i.e. Lf(x,y)=f(y,x). What's the general property of the eigenfunctions of this problem? Get the possible eigenvalues.

Homework Equations


The Attempt at a Solution



Well. I think that if Lf(x,y)=f(y,x) then if f is an eigenfunction, obviously, \lambda f(x,y)=f(y,x). One possible kind of f that fills conditions is one that is symmetric, that is f(x,y)=f(y,x) then \lambda for this kind of eigenfunctions will be \lambda=1. Others are the antisymmetric ones, those for is true f(y,x)=-f(x,y) and then the eigenvalue for this kind is \lambda=-1

But I'm sure that there are more conditions that generate other kinds of eigenfunctions, not only symmetric nor antisymmetric. My question is: there are more or the antisymmetric and symmetric ones are the only ones, and if there are more how I get them and their eigenvalues?
 
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If f(y,x)=\lambda f(x,y) is to be true for all (x,y), then surely it must be true for x=y...what does that tell you?:wink:
 
it tells me \lambda=1?
 
Here's another hint: what happens if you act on f with L twice? What does that tell you about \lambda^2?
 
ELESSAR TELKONT said:
it tells me \lambda=1?
Or that f(x,x)=0.
 
Or that operator L is an involution, that's, it's its own inverse.
 
and then \lambda=\pm 1 necessarily and takes all values only if f\equiv 0. In fact zero function is symmetric and antisymmetric function at the same time.
 
f(x,y)=0 is a trivial solution, and not really an eigenfunction...so it should be discarded.

That leaves you with \lambda=1 and symmetric eigenfunctions, or \lambda=-1 and antisymmetric eigenfunctions.
 

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