Standard deviation of the energy of a system in a heat bath

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The mean energy of a system in a heat bath is expressed using the partition function Z and the variable β, which is related to temperature. The standard deviation of energy, represented as (ΔE)², is defined through the second derivative of the logarithm of the partition function with respect to β. A derivation of this relationship can be found in Eric Poisson's Statistical Physics II notes, specifically on page 40. The discussion highlights the connection between statistical mechanics and thermodynamic properties. The notes are noted to be useful for additional insights into the subject.
Narcol2000
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Given the mean energy of a system in a heat bath is

<br /> \bar{E} = - \frac{\partial ln(Z)}{\partial \beta}<br />

Where Z is the partition function and \beta = k_BT

Why is the standard deviation of E defined by:

<br /> (\Delta E)^2 = \frac{\partial^2 ln(Z)}{\partial \beta ^2}<br />

I can't seem to find any proof of how the second derivative is related to the standard deviation.
 
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Eric Poisson has a derivation on p40 of his Statisical Physics II notes: http://www.physics.uoguelph.ca/~poisson/research/notes.html.
 
Thanks a lot those notes are also pretty useful in other respects as well.
 
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