Proving Properties of Hermitian and Anti-Hermitian Operators

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The discussion centers on proving properties of Hermitian and anti-Hermitian operators, specifically the equality of the Hermitian conjugate of a Hermitian operator and the implications of anti-Hermitian operators having real eigenvalues. It is established that the relation (A_{op}^t)^t = A_{op} holds under specific conditions related to densely defined linear operators on separable Hilbert spaces. The participants clarify that the correct relation involves the inclusion of operators, emphasizing that equality may only hold for essentially self-adjoint operators. Additionally, it is noted that anti-Hermitian operators can only have real eigenvalues under certain conditions, leading to the conclusion that such spectral values are either zero or purely imaginary.
vsage
I think these questions may be so simple that I don't know how to properly prove them, but I am really stumped on how to show especially the first one:

Show that (A_{op}^t)^t=A_{op} Where A_{op} is an operator and 't' is my way of saying hermitian conjugate

Secondly, I'm not too sure at all how to show this:

Show that the anti-hermitian operator, I_{op}^t=-I_{op} has at most one real eigenvalue

Any hints would be greatly appreciated.

Edit: oops! Hidden in the annals of the internet I found the appropriate definition for A_{op}, but I'm still having trouble with the second one.
 
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It's straightforward to see that for an eigenvector of \hat{A} corresponding to a spectral value \lambda

\lambda=\langle \psi|\hat{A}|\psi\rangle =\left(\langle\psi|\hat{A}^{\dagger}|\psi\rangle\right)^{*}=(-\lambda)^{*}

Therefore the spectral value \lambda is either 0 or purely imaginary...

Daniel.
 
To show that the hermitian conjugate of the hermitian conjugate of A is A itself, use the definition of "hermitian conjugate"!
 
For this operatorial equality

\hat{A}=\left(\hat{A}^{\dagger}\right)^{\dagger} (1)

to hold,for a densly defined linear operator A,then the 2 conditions from the definition of operatorial equality on a separable Hilbert space must be met

\mathcal{D}_{\hat{A}}=\mathcal{D}_{\left(\hat{A}^{\dagger}\right)^{\dagger}} (2)

and

\hat{A}|\psi\rangle=\left(\hat{A}^{\dagger}\right)^{\dagger}|\psi\rangle,\forall |\psi\rangle \in \mathcal{D}_{\hat{A}} (3)


Unfortunately,there's no densly defined linear operator on a separable Hilbert space for which (1) (and implicitely (2) & (3)) to hold.

It can be proved that for an arbitrary densly defined linear operator \hat{A} this operatorial inclusion holds true
\hat{A}\subset\left(\hat{A}^{\dagger}\right)^{\dagger} (4)

Since \hat{A}^{\dagger} is a closed operator,we use (4) to assert that \left(\hat{A}^{\dagger}\right)^{\dagger} is a closed extension of the operator \hat{A}.

Ergo,equality (1) doesn't hold true for any densly defined linear operator on a separable Hilbert space...

Daniel.

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NOTE:Red=Incorrect statements.Relation (4) doesn't hold for essentially self adjoint densly defined linear operators.See disclaimer in post #6.
 
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What I'm saying is that u can't prove something which is incorrect...:wink:

Daniel.
 
DISCLAIMER!

:redface: My professor of QM was wrong (and it's my fault i didn't check other sources on functional analysis)...

The correct relation is

\hat{A}\subseteq \left(\hat{A}^{\dagger}\right)^{\dagger} (1)

Among the operators for which the equality holds,one finds operators which are called ESSENTIALLY SELFADJOINT densly defined linear operators.They form a subset of the set of selfadjoint (not hermitian/symmetric) linear operators acting on a separable Hilbert space for which their adjoint is selfadjoint.They satisfty the relations

\hat{A}=\hat{A}^{\dagger} (the operator is selfadjoint) (2)
\hat{A}^{\dagger}=\left(\hat{A}^{\dagger}\right)^{\dagger} (its adjoint is selfadjoint) (3)

The relation (1) coupled with the relations (2) & (3) prove that for most of the selfadjoint operators,their adjoint is not selfadjoint,but hermitean/symmetric.

See [1] for a proof that H-atom Hamiltonian (Dirac formulation-Schrödinger picture-coordinate representation) is essentially selfadjoint...

As a comment to post #5,u need to prove the relation (1) and show that the equality limit holds true,only under certain conditions (u need to find these conditions);for example,if the operator is essentially selfadjoint,then it verifies the equality limit.

Daniel.

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[1]J.Prugoveçki:"Quantum Mechanics in Hilbert Space".
 
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I addition to post #6,i would reccomend you to read Akhiezer & Glazman's "The Theory of Linear Operators in Hilbert Space",2nd.ed,Dover,1993.

In section #22,he proves that for a bounded linear ooperator defined on the whole Hilbert space the equality limit holds.On page #80 he mentions the strict inclusion,though he mentions that there are operators for which the equality relation holds...:eek:

Daniel.
 
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