Quantum operator hermiticity. Show that S is Hermitian

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SUMMARY

The discussion centers on demonstrating the hermiticity of the spin operator S, defined by its action on the eigenvectors |R> and |L>. The operator S satisfies the condition for being Hermitian, as shown by the equation <ψ|S|L> = * and the orthonormality of the eigenvectors. The participant seeks clarification on how to determine the action of S on any arbitrary function |ψ> and requests an algorithm to verify the hermiticity of operators.

PREREQUISITES
  • Understanding of quantum mechanics, specifically spin operators.
  • Familiarity with the concept of Hermitian operators in linear algebra.
  • Knowledge of eigenvectors and their properties in quantum systems.
  • Proficiency in bra-ket notation and inner product definitions.
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  • Research the properties of Hermitian operators in quantum mechanics.
  • Learn about the implications of eigenvalue equations for quantum operators.
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Students and researchers in quantum mechanics, particularly those studying operator theory and the properties of spin systems.

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Homework Statement


Spin Operator S has eigenvectors |R> and |L>,
S|R> = |R>
S|L> =-|L>

eigenvectors are orthonormal

Homework Equations


Operator A is Hermitian if <ψ|A|Θ> = <Θ|A|ψ>*



The Attempt at a Solution


<ψ|S|L> = <L|S|ψ>* // Has to be true if S is Hermitian
LHS: <ψ|S|L> = <ψ|-|L>
<ψ|-|L>* = <L|-|ψ>

Question: how do i know how S acts on any function like |ψ> ?
Could somebody provide an algorithm to find if an operator is Hermitian.
I have another example of operator P, where P|R> = |L>
P|L> = |R>
How should i go on about this?
 
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Use the definition of a hermitian operator:

\langle\psi|S|\psi\rangle^{\dagger} = \langle\psi|S^{*}|\psi\rangle = \langle\psi|S|\psi\rangle
 

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