Quantum physics - Symmetrizer operator

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Homework Help Overview

The discussion revolves around the properties of the Symmetrizer and Antisymmetrizer operators in the context of identical particles in quantum mechanics. Participants explore the implications of these operators being Hermitian and their eigenkets, questioning how these eigenkets can form a basis for the space of kets.

Discussion Character

  • Conceptual clarification, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants attempt to analyze a specific example in a 4-dimensional state space to identify the eigenvalues and eigenspaces of the Symmetrizer. Questions arise about the completeness of the eigenkets and whether every ket can be expressed as a linear combination of symmetric or antisymmetric kets.

Discussion Status

The discussion is active, with participants providing insights and questioning the completeness of the eigenket set for the Symmetrizer. There is exploration of the relationship between the eigenkets of the Symmetrizer and Antisymmetrizer, with some participants suggesting that certain kets may not belong to the eigenspace of the Symmetrizer.

Contextual Notes

Participants note the potential missing information regarding the eigenkets and the implications of the Hermitian nature of the operators. There is an ongoing examination of the definitions and properties of the operators in question.

vabite
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Hi everyone.

I am studying 'identical particles' in quantum mechanics, and I have a problem with the properties of the Symmetrizer (S) and Antisymmetrizer (A) operators.

S and A are hermitian operators. Therefore, for what I know, their set of eigenkets must constitute a basis of the space ket.
However, the set of eigenkets of S (A) contains only symmetric (antisymmetric) kets. Given an arbitrary ket (not necessarily symmetrical or antisymmetrical), I don't think it is always possible to write it as linear combination of only symmetrical (antisymmetrical) kets. Therefore, I can't understand how the eigenkets of S (A) can constitute a basis of the space ket.
 
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Try a 4-dimensional example: Consider the state space V spanned by {|1>|1>, |1>|2>, |2>|1>, |2>|2> }. What are the eigenvalues of S? What are the corresponding eigenspaces?
 
I think in this case the eingevalue is 1 (4 times degenerate), and the eigenkets
|1>|1>
(1/√2) (|1>|2>+|2>|1>)
(1/√2) (|2>|1>+|1>|2>)
|2>|2>
So.. 4 eigenkets for a 4D space. Does this mean that every ket can be obtained as a linear combination of symmetric (antisymmetric) kets?
 
vabite said:
I think in this case the eingevalue is 1 (4 times degenerate), and the eigenkets
|1>|1>
(1/√2) (|1>|2>+|2>|1>)
(1/√2) (|2>|1>+|1>|2>)
|2>|2>

Addition is commutative, so your middle two kets are the same. :smile:
 
Err... right. I did not solve the eigenvalue equation, but I can't see a 4th eigenket of S...

I guess the missing one to form a basis of the ket space is:
(1/√2) (|1>|2>-|2>|1>)
that is an eigenket of A (and thus not of S).
 
vabite said:
Err... right. I did not solve the eigenvalue equation, but I can't see a 4th eigenket of S...

I guess the missing one to form a basis of the ket space is:
(1/√2) (|1>|2>-|2>|1>)
that is an eigenket of A (and thus not of S).

Are you sure this isn't an eigenket of S?
 
S [(1/√2) (|1>|2>-|2>|1>)]=
(1/2)(P12+P21) [(1/√2) (|1>|2>-|2>|1>)] =
(1/2) {[(1/√2) (|1>|2>-|2>|1>)] + [(1/√2) (|2>|1>-|1>|2>)]} =
0
...

At this point, the only thing I can imagine is that
(1/√2) (|1>|2>-|2>|1>)
is an eigenket of S with eigenvalue 0.
 
vabite said:
S [(1/√2) (|1>|2>-|2>|1>)]=
(1/2)(P12+P21) [(1/√2) (|1>|2>-|2>|1>)] =
(1/2) {[(1/√2) (|1>|2>-|2>|1>)] + [(1/√2) (|2>|1>-|1>|2>)]} =
0
...

At this point, the only thing I can imagine is that
(1/√2) (|1>|2>-|2>|1>)
is an eigenket of S with eigenvalue 0.

Yup.

S [(1/√2) (|1>|2>-|2>|1>)] = 0 [(1/√2) (|1>|2>-|2>|1>)].

Things are sort of reversed for A.
 
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Great: thanks!
 

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