Wave mechanics : self-adjoint problem

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Homework Help Overview

The discussion revolves around the properties of self-adjoint operators in the context of wave mechanics, specifically focusing on the commutation relation between two operators P and Q. The original poster attempts to show that the operator [P,Q] is anti-self-adjoint, given that [P,Q] equals ic, where c is a real number.

Discussion Character

  • Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants question the original poster's approach of setting [P,Q] equal to zero and the introduction of a wavefunction phi. They emphasize the definition of the commutation relation and its implications. There are discussions about the adjoint of the commutation relation and the properties of Hermitian operators.

Discussion Status

Participants are actively engaging with the definitions and properties of the operators involved. Some have provided guidance on how to approach the proof, while others caution against using assumptions that are not explicitly stated in the problem. Multiple interpretations of the problem are being explored, particularly regarding the definitions of adjoints and the implications of the operators being Hermitian.

Contextual Notes

There is a noted uncertainty regarding whether the operators P and Q are indeed Hermitian, which affects the validity of certain arguments being made in the discussion. Participants are also navigating the implications of the given commutation relation and its adjoint.

noblegas
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Homework Statement


The operators P and Q are self-adjoint and satisfy the commutation relation [P,Q]=ic where c is a real number. Show that the operator [P,Q] is anti-self-adjoint, that is , that the adjoint of the operator is the negative of the operator, consistent with the right-hand side of the equation.


Homework Equations





The Attempt at a Solution



I know a self-adjoint operator Q*=Q where * represents the dagger. [P,Q]=(PQ-QP)*phi=ic=0=PQphi-QPphi= PQ*phi-Q*Pphi=0?
 
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Why are you setting [itex][P,Q][/itex] equal to zero? and what is 'phi'...an example wavefunction?...There is no need to introduce any wavefunctions here.

By definition, [itex][P,Q]=PQ-QP[/itex]...you are told that this is equal to [itex]ic[/itex].

What is the definition of [itex][P,Q]^\dagger[/itex]?
 
gabbagabbahey said:
Why are you setting [itex][P,Q][/itex] equal to zero? and what is 'phi'...an example wavefunction?...There is no need to introduce any wavefunctions here.

By definition, [itex][P,Q]=PQ-QP[/itex]...you are told that this is equal to [itex]ic[/itex].

What is the definition of [itex][P,Q]^\dagger[/itex]?

Right... matrices don't commute. By definition , [itex][P,Q]^\dagger[/itex]=[itex][Q,P]=QP-PQ[/itex]

I think I got it . PQ=ic+QP => [Q,P]=QP-PQ=QP-(ic+QP)=-ic ?
 
Last edited:
While its true that [itex][P,Q]^{\dagger}=[Q,P][/itex] (but only since [itex]Q[/itex] and [itex]P[/itex] are Hermitian), that's not really the definition of [itex][P,Q]^{\dagger}[/itex]. In fact, it's basically the very thing you are trying to prove, so I wouldn't use it as the basis of your proof!

By definition,

[tex][P,Q]^{\dagger}=(PQ-QP)^{\dagger}=(PQ)^{\dagger}-(QP)^{\dagger}[/tex]

Now, use the fact that [itex](AB)^{\dagger}=B^{\dagger}A^{\dagger}[/itex] for any two operators [itex]A[/itex] and [itex]B[/itex], along with the fact that [itex]Q[/itex] and [itex]P[/itex] are Hermitian...
 
gabbagabbahey said:
While its true that [itex][P,Q]^{\dagger}=[Q,P][/itex] (but only since [itex]Q[/itex] and [itex]P[/itex] are Hermitian), that's not really the definition of [itex][P,Q]^{\dagger}[/itex]. In fact, it's basically the very thing you are trying to prove, so I wouldn't use it as the basis of your proof!

By definition,

[tex][P,Q]^{\dagger}=(PQ-QP)^{\dagger}=(PQ)^{\dagger}-(QP)^{\dagger}[/tex]

Now, use the fact that [itex](AB)^{\dagger}=B^{\dagger}A^{\dagger}[/itex] for any two operators [itex]A[/itex] and [itex]B[/itex], along with the fact that [itex]Q[/itex] and [itex]P[/itex] are Hermitian...

[tex][P,Q]^{\dagger}=(PQ-QP)^{\dagger}=(PQ)^{\dagger}-(QP)^{\dagger}[/tex]=[tex]Q^{\dagger}P^{\dagger}-P^{\dagger}Q^{\dagger}[/tex]; since [tex]Q^{\dagger}=Q[/tex] , then [tex]P^{\dagger}=P[/tex], therefore [tex]Q^{\dagger}P^{\dagger}-P^{\dagger}Q^{\dagger}=QP-PQ=[Q,P][/tex]

therefore [tex][P,Q]^{\dagger}=[Q,P][/tex]
 
Right, but your problem statement doesn't actually tell you the operators are Hermitian, so you won't want to use that.

Instead, just take the adjoint of both sides of the equation you are given...

[tex][P,Q]=ic\implies [P,Q]^{\dagger}=(ic)^{\dagger}=-ic=-[P,Q][/tex]
 

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