What are the expansions of Bose functions for studying thermodynamic behavior?

AI Thread Summary
The discussion focuses on deriving expansions of Bose functions \( g_0(z) \), \( g_1(z) \), and \( g_2(z) \) to analyze thermodynamic behavior as \( z \) approaches 1, with \( \alpha = -\ln z \) being a small positive number. The expression for \( g_1(\alpha) \) is provided, showing its expansion in powers of \( \alpha \). Additionally, \( g_0(\alpha) \) is derived as the negative derivative of \( g_1(\alpha) \), leading to its own expansion. A suggestion is made to rewrite \( z \) in terms of \( \alpha \) and utilize series expansions to facilitate the derivation. The thread emphasizes the importance of these expansions in understanding Bose gas behavior.
erbilsilik
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Homework Statement


To study the thermodynamic behavior of the limit $$z\rightarrow1$$ it is useful to get the expansions of $$g_{0}\left( z\right),g_{1}\left( z\right),g_{2}\left( z\right)$$

$$\alpha =-\ln z$$ which is small positive number. From, BE integral,
$$g_{1}\left( \alpha \right) =-ln\left( 1-z\right) =-ln\alpha+\dfrac {\alpha } {2}-\dfrac {\alpha ^{2}} {24}+O({\alpha ^{4}})$$
and hence

$$g_{0}\left( \alpha \right) =-\dfrac {\partial } {\partial \alpha }g_{1}\left( \alpha \right)=\dfrac {1} {\alpha }-\dfrac {1} {2}+\dfrac {\alpha } {12}O({\alpha ^{3}})$$

[Source: A.Khare, Fractional Statistics and Quantum Theory, Two Dimensional Bose Gas, p.113]

Could anyone help me to derive this expressions? I can't figure out what does it mean writing this functions in the powers of α.

Homework Equations


https://en.wikipedia.org/wiki/Polylogarithm (BE integral)

The Attempt at a Solution



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erbilsilik said:

Homework Statement


To study the thermodynamic behavior of the limit $$z\rightarrow1$$ it is useful to get the expansions of $$g_{0}\left( z\right),g_{1}\left( z\right),g_{2}\left( z\right)$$

$$\alpha =-\ln z$$ which is small positive number. From, BE integral,
$$g_{1}\left( \alpha \right) =-ln\left( 1-z\right) =-ln\alpha+\dfrac {\alpha } {2}-\dfrac {\alpha ^{2}} {24}+O({\alpha ^{4}})$$
and hence

$$g_{0}\left( \alpha \right) =-\dfrac {\partial } {\partial \alpha }g_{1}\left( \alpha \right)=\dfrac {1} {\alpha }-\dfrac {1} {2}+\dfrac {\alpha } {12}O({\alpha ^{3}})$$

[Source: A.Khare, Fractional Statistics and Quantum Theory, Two Dimensional Bose Gas, p.113]

Could anyone help me to derive this expressions? I can't figure out what does it mean writing this functions in the powers of α.

Homework Equations


https://en.wikipedia.org/wiki/Polylogarithm (BE integral)

The Attempt at a Solution


[/B]
Suggestion: Write ## z=exp(-\alpha) ## and you get a term ## ln(exp(\alpha)-1) ## plus another term ## ln(exp(\alpha))=\alpha ## In the first term (inside the ## ln ## ) expand ## exp(\alpha) =1+\alpha+(\alpha)^2/2 +... ## and subtract the 1. Then factor out ## \alpha ## and you get ## ln(\alpha)+ln(1+\alpha/2+..) ## The expansion of ## ln(1+u)=u ## for small ## u ##.
 
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