Wave mechanics : self-adjoint problem

In summary: The operator [P,Q] is anti-self-adjoint, that is, that the adjoint of the operator is the negative of the operator. This is consistent with the right-hand side of the equation.
  • #1
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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  • #2
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]?
 
  • #3
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 ?
 
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  • #4
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...
 
  • #5
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]
 
  • #6
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]
 

Related to Wave mechanics : self-adjoint problem

1. What is wave mechanics?

Wave mechanics is a branch of physics that studies the behavior and properties of waves, such as light waves, sound waves, and water waves. It is based on the principles of quantum mechanics and is used to describe the behavior of particles at the microscopic level.

2. What is a self-adjoint problem in wave mechanics?

A self-adjoint problem in wave mechanics refers to a mathematical equation or system of equations that is symmetric under certain conditions. This means that the equation remains unchanged when the variables are switched, making it easier to solve and interpret.

3. Why is it important to have self-adjoint problems in wave mechanics?

Having self-adjoint problems in wave mechanics is important because it allows for more accurate and reliable predictions of the behavior of particles. It also simplifies the equations and makes them easier to solve, which is crucial in understanding and studying complex physical phenomena.

4. How are self-adjoint problems solved in wave mechanics?

Self-adjoint problems in wave mechanics are typically solved using mathematical methods such as eigenvector decomposition and spectral theory. These methods involve breaking down the problem into simpler components and finding solutions that satisfy the given conditions.

5. What are some real-life applications of wave mechanics?

Wave mechanics has many practical applications, including in the fields of electronics, optics, and materials science. It is used to design electronic devices, such as transistors and lasers, and to understand the properties of materials, such as semiconductors and superconductors. It is also essential in medical imaging technologies, such as MRI machines, and in the development of new materials for various industries.

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