Commutator of hermitian operators

[Gideon]

i searched the forum, but nothing came up. My question, how do you prove that [A,B] = iC if A and B are hermitian operators? I understand how C is hermitian as well, but i can't figure out how to prove the equation.

 

[seratend]

i searched the forum, but nothing came up. My question, how do you prove that [A,B] = iC if A and B are hermitian operators? I understand how C is hermitian as well, but i can't figure out how to prove the equation.

What do you want to see? You have an equation AB -BA= iC

This equation tells you that ([A,B])^+=(AB-BA)^+ where + is the hermitian conjugate
=> ([A,B])^+= BA - AB=[B,A]=-[A,B]

=> the commutator of hermitian operators is an anti hermitian operator.
And an antihermitian operator is an hermitian operator times i.
[A,B] = iC just relates this fact nothing more.

Seratend.

 

[dextercioby]

Here's how i'd do it

Let's consider the densely defined linear operator

\hat{O}=:\left[\hat{A},\hat{B}\right]_{-}=:\hat{A}\hat{B}-\hat{B}\hat{A} (1)

,where \hat{A},\hat{B} are densly defined linear operators on the Hilbert space \mathcal{H}.

The domain of this operator is

\mathcal{D}_{\hat{O}} \subset \left(\mathcal{D}_{\hat{A}}\cap\mathcal{D}_{\hat{B}}\right)

We want to define the adjoint of \hat{O}.

-Let's consider a vector \phi\in\mathcal{H}.

-We define the action of a linear functional F
*continuous on the image of the linear operator \hat{O}
*associated to the linear operator \hat{O} and to a vector \phi\in\mathcal{H}
on a vector \psi\in\mathcal{D}_{\hat{O}} by the scalar product in \mathcal{H}

F_{\hat{O},\phi}\psi =:\langle \phi,\hat{O}\var\psi \rangle (2)

If for a given \phi\in\mathcal{H} the values of the linear functional (2) admit the representation given by the theorem of Riesz,i.e.

F_{\hat{O},\phi}\psi =:\langle \chi,\psi\rangle (3)

,with \chi\in\mathcal{H} uniquely determined by \hat{O} and \phi,

then there exists a densly defined linear operator denoted by \hat{O}^{\dagger} called the adjoint of the linear operator \hat{O}

which obeys

\chi=:\hat{O}^{\dagger}\phi (4)

Therefore

\phi\in\mathcal{D}_{\hat{O}^{\dagger}} (5)

\chi\in\mathcal{I}_{\hat{O}^{\dagger}} (6)

We thus obtain

\left\langle \hat{O}^{\dagger}\phi,\psi\right\rangle =\left\langle\phi,\hat{O}\psi\right\rangle (6)

To be continued.

Daniel.

 

[HackaB]

Here's how i'd do it

Let's consider the densely defined linear operator

\hat{O}=:\left[\hat{A},\hat{B}\right]_{-}=:\hat{A}\hat{B}-\hat{B}\hat{A} (1)

,where \hat{A},\hat{B} are densly defined linear operators on the Hilbert space \mathcal{H}.

The domain of this operator is

\mathcal{D}_{\hat{O}}=\mathcal{D}_{\hat{A}}\cap\mathcal{D}_{\hat{B}}

...

To be continued.

Daniel.

WTF are you talking about? It appears that you have been reading too many math books, and that it has affected your brain. Or perhaps you are just trying to show off.

 

[selfAdjoint]

WTF are you talking about? It appears that you have been reading too many math books, and that it has affected your brain. Or perhaps you are just trying to show off.

There speaks a man ever so proud of his own ignorance (or if you are a lady, switch the appropriate pronouns).

 

[HackaB]

SelfAdjoint:

Please explain to me the usefulness of Daniel's post. Seratend had already answered the question in two lines.

 

[dextercioby]

So that's how the adjoint of the commutator is defined.

F_{-\left[\hat{A},\hat{B}\right]_{-},\phi} =\left\langle\phi,-\left[\hat{A},\hat{B}\right]_{-}\psi\right\rangle =\left\langle\phi,\hat{B}\hat{A}\psi\right\rangle-\left\langle\phi,\hat{A}\hat{B}\psi\right\rangle (7)

\psi\in\mathcal{D}_{\left[\hat{A},\hat{B}\right]_{-}} \Rightarrow \psi\in\mathcal{D}_{\hat{A}} \ \mbox{and} \ \psi\in\mathcal{D}_{\hat{B}} (8)

By hypothesis

\hat{A}\subset\hat{A}^{\dagger} (9)

\hat{B}\subset\hat{B}^{\dagger} (10)

From (8),(9) and (10) we conclude that

\psi\in\mathcal{D}_{\hat{A}^{\dagger}} \ \mbox{and} \ \psi\in\mathcal{D}_{\hat{B}^{\dagger}} (11)

Moreover

\hat{A}\hat{B}\psi=\hat{A}^{\dagger}\hat{B}^{\dagger} \psi (12)

\hat{B}\hat{A}\psi=\hat{B}^{\dagger}\hat{A}^{\dagger} \psi (13)


Using (7),(12) and (13),one gets

F_{-\left[\hat{A},\hat{B}\right]_{-},\phi} =\left\langle\phi,\left(\left(B^{\dagger}\hat{A}^{\dagger}-\hat{A}^{\dagger}\hat{B}^{\dagger}\right)\psi\right\rangle=\left\langle\phi,\left(\left(\hat{A}\hat{B}\right)^{\dagger}-\left(\hat{B}\hat{A}\right)^{\dagger}\right)\psi\right\rangle (14)

,where i used the operatorial inclusion

\left(\hat{A}\hat{B}\right)^{\dagger} \supseteq \hat{B}^{\dagger}\hat{A}^{\dagger} (15)

Using in (14) another operatorial inclusion

\left(\hat{A}-\hat{B}\right)^{\dagger}\supseteq \hat{A}^{\dagger}-\hat{B}^{\dagger} (16)

and the definition of the commutator,one gets

F_{-\left[\hat{A},\hat{B}\right]_{-},\phi} =F_{\left[\hat{A},\hat{B}\right]_{-}^{\dagger},\phi} (17)

Q.e.d.

Daniel.

 

[dextercioby]

WTF are you talking about? It appears that you have been reading too many math books, and that it has affected your brain. Or perhaps you are just trying to show off.

You call it "show off",i call it "quantum mechanics in its splendor"

Daniel.

 

[HackaB]

OK, call it whatever you want. While you're here, how does that "proof that group multiplication is associative" go again?

 

[dextercioby]

I hope everyone sees that (17) implies

-\left[\hat{A},\hat{B}\right]_{-}\subset \left[\hat{A},\hat{B}\right]_{-}^{\dagger}

,even though I've clearly proven only the equality of the 2 images.I've only hinted the way to prove the inclusion of the domains.

Daniel.

 

[dextercioby]

OK, call it whatever you want. While you're here, how does that "proof that group multiplication is associative" go again?

You'll descover through those 7000+ posts many more mistakes.The important thing is that I've learned from each and everyone of them...

Daniel.