Why all operators in QM have a Hermitian Matrices

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In quantum mechanics (QM), not all operators are Hermitian; only self-adjoint operators are. Anti-Hermitian operators, such as i times any Hermitian operator, exist and highlight this distinction. Observables must be represented by Hermitian operators to ensure real eigenvalues, which are essential for physical interpretation, such as energy values in the case of the Hamiltonian. The reality of eigenvalues is supported by the mathematical properties of Hermitian operators, which are derived from QM postulates. Ultimately, the choice of Hermitian operators allows for consistent physical outcomes regardless of the basis used in quantum state representation.
mwalmasri
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Why all operators in QM have a Hermitian Matrices ?
 
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yes so all operators have a self-adjoint Matrices, which operator can be Represented as anti-Hermitian operators?
 
mwalmasri said:
yes so all operators have a self-adjoint Matrices, which operator can be Represented as anti-Hermitian operators?

It's not true that all operators are Hermitian, The simplest example would be i times any Hermitian operator, it's anti-Hermitian.
You may be asking why any operator representing observable is Hermitian. There is no proof for this because this is simply one of the postulates of QM. But if it's not true, you will have an observable that has complex-value eigenvalue, which doesn't make any physical sense.
 
yes,when I asked the question I mean a physical operator like a Hamiltonian... maybe I must be clear enough in my question. Hermitian is used because its have a real eigenvalue that is right...
Thanks
 
The eigenvalues of a hermitian operator are real,like hamiltonian which should be hermitian operator because it's eigenvalues are simply energy,which should be a real quantity.So all observables are associated with hermitian operator.
Assume a hermitian operator,and the eigenvalue eqn
A|a>=a|a>,assuming normalization of eigenstates,multiplying by <a|
<a|A|a>=a
taking complex conjugate of both sides,
<a|A|a>*=a*,
By hermiticity condition,<a|A|a>=<a|A|a>*,so a=a* implying reality of eigenvalues.
 
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Basically it's a postulate of QM.

The way I like to look at it however is as follows. Suppose we have some observational apparatus with n possible outcomes that have some real number yi assigned to each outcome. List them out as a vector and write it as sum yi |bi>. Now we come to a problem - its not basis independent - change to another basis and the yi change - but since the choice of basis is entirely arbitrary we expect nature to be independent of that choice. To get around that problem QM simply replaces the |bi> by |bi><bi| to give sum yi |bi><bi| which is the same regardless of basis. It is a Hermitian operator whose eigenvalues are the possible outcomes of the observation.

Thanks
Bill
 

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