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This was a question on my exam and I don't know how to solve it.

Use the variational principle to prove that the first order perturbation theory always overestimates the energy of the fundamental state. Also prove that the second order term is always negative. Any Ideas?

Assume that the perturbation operator is hermitian.

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Hi Presbitero - questions like this where you just ask for a solution aren't appropriate on this site. This is a place for conceptual physics questions, so if you'd like to edit your question to focus on the concept that is giving you trouble, someone can reopen it. See our homework policy for more information. – David Zaslavsky♦ Jan 23 at 11:13
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The reason this is not a conceptual physics question is that you're not asking about a concept, you're asking us to solve a problem for you. It has nothing to do with the fact that the problem came from an exam. You can find some examples of good (conceptual) questions in the homework policy I linked to. – David Zaslavsky♦ Jan 23 at 12:02
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First order perturbation theory result $E_0^{(1)} = E_0^{(0)} +V_{00}$ overestimates the value of $E_0$ because the second-order correction is negative (see the corresponding formula). However, it is implied that the perturbation operator $\hat{V}$ is Hermitian. If it is not Hermitian, the second order correction can be positive. – Vladimir Kalitvianski Jan 23 at 12:21
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@DavidZaslavsky I'm not so sure I agree it's too localized. First order perturbation theory is going to miss the true energy, but it's mildly interesting that it definitively overshoots not undershoots, and that the second order term goes the other way (I haven't checked that it does!) – twistor59 Jan 23 at 12:24
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@twistor59: It is interesting question because a perturbation theory is a Taylor expansion of a function in a small parameter, and nothing prevents the second derivative from having any sign at the expansion point. – Vladimir Kalitvianski Jan 23 at 12:28
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closed as too localized by David Zaslavsky♦ Jan 23 at 11:11

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