How do I simplify <n|n> for Hermetian Operators?

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SUMMARY

The discussion focuses on simplifying the expression for Hermitian operators in the context of a harmonic oscillator. The average value is computed by breaking it down into three components: m=n, m=n+2, and m=n-2, leading to the final expression = (1/4) ħ²ω²(2n+1)² + (1/2)(ħ/mω)². The orthonormality of the basis states is emphasized, confirming that =δ_{mn}.

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Biest
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Hi,

So for an harmonic oscillator we need to to find the average value for [tex]x^4[/tex], so [tex]<n|x^4|n>[/tex]. We split it up to [tex]\sum_m |<n|x^2|n>|^2[/tex] and recognize that only m = n+2, m=n and m = n-2 can be used. We find that

m=n

[tex]\frac{\hbar}{2m\omega}<n|\hat{A}\hat{A^\dagger}|n>[/tex]

m= n+2 [tex]\frac{\hbar}{2m\omega}<n+2|\hat{A^\dagger}\hat{A^\dagger}|n>[/tex]

m = n-2

[tex]\frac{\hbar}{2m\omega}<n-2|\hat{A}\hat{A}|n>[/tex]

So we can reduce it all to

[tex]<n|x^4|n> = \frac{1}{4} \hbar^2 \omega^2 (2n+1)^2 + \frac{1}{2} (\frac{\hbar}{m \omega})^2 <n|n>[/tex]How I simplify the [tex]<n|n>[/tex].

Thanks.

Cheers,

Biest
 
Last edited:
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The basis states are orthonormal, so [itex]<n|m>=\delta_{mn}[/itex].
 

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