Is the Hermitian Conjugation Identity Correct?

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Homework Help Overview

The discussion revolves around the Hermitian conjugation identity for operators, specifically examining the expression \((\hat A \times \hat B)^* = -\hat B^* \times \hat A^*\). Participants explore the implications of this identity in the context of Hermitian operators and the properties of the cross product.

Discussion Character

  • Conceptual clarification, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Some participants attempt to derive the identity using specific operator examples and component-wise definitions. Others question the assumptions regarding the commutativity of the operators involved and the proper use of indices in the equations presented.

Discussion Status

The discussion is ongoing, with participants providing insights and corrections regarding the formulation of the identity. There is a mix of agreement and disagreement on the interpretations of the mathematical expressions, and some guidance has been offered regarding the properties of Hermitian operators.

Contextual Notes

There is a noted ambiguity regarding whether the operators are assumed to be Hermitian, as the original problem statement does not explicitly state this. Participants are also addressing the implications of antisymmetry in the context of the cross product and Hermitian conjugation.

Dyatlov
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Homework Statement


##(\hat A \times \hat B)^*=-\hat B^* \times \hat A^*##
Note that ##*## signifies the dagger symbol.

Homework Equations


##(\hat A \times \hat B)=-(\hat B \times \hat A)+ \epsilon_{ijk} [a_j,b_k]##

The Attempt at a Solution


Using as example ##R## and ##P## operators:
##(\hat R \times \hat P)^*_i=-(\hat P \times \hat R)^*_i+ \epsilon_{ijk} [Y,P_z]##
##(\hat R \times \hat P)^*_i=-(\hat P \times \hat R)^*_i##
##(\hat R \times \hat P)^*=-\hat P^* \times \hat R^*##
 
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Dyatlov said:

Homework Statement


##(\hat A \times \hat B)^*=-\hat B^* \times \hat A^*##
Note that ##*## signifies the dagger symbol.
Start instead from a component-wise definition:
$$(A \times B)_i ~=~ \epsilon_{ijk} A_j B_k $$ (where the usual summation convention applies to repeated indices).
 
Since ##\epsilon_{ijk}## is antisymmetric then we have
##\epsilon_{ijk}A_jB_k=A_jB_k-A_kB_j##
##A_jB_k-A_kB_j=-(B_jA_k-B_kA_j)##
##(A \times B)_i=-(B \times A)_i##
Since A and B are Hermitian the same equlity holds for their self-adjoint counterparts.
 
Last edited:
Dyatlov said:
Since ##\epsilon_{ijk}## is antisymmetric then we have
##\epsilon_{ijk}A_jB_k=A_jB_k-A_kB_j##
That equation does not make sense. On the LHS, ##i## is a free index, but ##j,k## are dummy summation indices. However, on your RHS both ##j## and ##k## are free indices, and there's no ##i## at all. Both left and right hand sides of such an equation must have exactly the same free indices.

The LHS uses a version of the summation convention. It is short for $$\sum_{j,k} \epsilon_{ijk}A_jB_k $$
##A_jB_k-A_kB_j=-(B_jA_k-B_kA_j)##
This is wrong if ##B_j## and ##A_k## don't commute (which is presumably the case here, since the problem statement didn't specify commutativity). So you can't blithely interchange ##A## and ##B## like that.

##(A \times B)_i=-(B \times A)_i##
Since A and B are Hermitian
Your original problem statement doesn't say that ##A,B## are Hermitian.

the same equality holds for their self-adjoint counterparts.
But that doesn't solve the problem as stated.

Start with this: $$\left( \sum_{j,k} \epsilon_{ijk}A_jB_k \right)^\dagger ~=~ \dots\,? \dots $$ Hint: for arbitrary operators ##X,Y##, what is ##(XY)^\dagger## ?
 
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Thanks for the replies.
The title mentions that I am solving the identity for Hermitian operators.
I know that ##\epsilon_{ijk}A_jB_k## is a sum over j and k, with ##j,k=1,2,3##.
##(\epsilon_{ijk}A_jB_k)^\dagger=(\epsilon_{ijk}B^\dagger_kA^\dagger_j)=-(B^\dagger \times A^\dagger)_i##
Therefore:
##(A \times B)^\dagger_i=-(B^\dagger \times A^\dagger)_i##
 
Dyatlov said:
The title mentions that I am solving the identity for Hermitian operators.
No it doesn't -- it mentions "Hermitian conjugation", which is an operation which can be performed on any operator.

Anyway, I take it you're now happy with the solution.
 
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Bad wording I guess then.
Thanks for the help, anyway!
 

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