Annihilation Operator Hermitian Without Adjoint Condition?

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Homework Statement



How do I show that the annihilation operator \hat{a} is hermitian WITHOUT explicitly using the condition where an operator X is hermitian if its adjoint is also X ie. X=X^+

Homework Equations



none.

The Attempt at a Solution



I could show \hat{a} \hat{x} \neq \hat{x} \hat{a} where \hat{x} is the position operator, but that only shows non-hermiticity for that one operator...
Is there a more elegant way to show non-hermiticity simply?
 
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Commuting with operators doesn't have much to do with hermiticity. In the last problem you posted you found an eigenstate of the 'a' operator. What were it's eigenvalues like? Hermitian operators have real eigenvalues.
 
oh yes offcourse - the eigenvalue was real...stupid me. :biggrin:
 
The point is that the operator has eigenvalues that AREN'T real. Hope you misspoke.
 
yeah sorry I was meant to say: "...the eigenvalues are meant to be real..."

And the question did give a complex eigenvalue...
 
To solve this, I first used the units to work out that a= m* a/m, i.e. t=z/λ. This would allow you to determine the time duration within an interval section by section and then add this to the previous ones to obtain the age of the respective layer. However, this would require a constant thickness per year for each interval. However, since this is most likely not the case, my next consideration was that the age must be the integral of a 1/λ(z) function, which I cannot model.
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