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This is a problem (Problem 3.16) from the book Statistical Mechanics 2nd Ed. by Pathria. In the problem I have to calculate the partition function of an ultra-relativistic 1D gas ($E_i=cp_i$) consisting in $3N$ particles moving in one dimension. I know that the partition function is given by

$$Q_{3N}=\frac{1}{(3N)!h^{3N}} \int e^{-\beta H(q,p)}d\omega,$$

where $d\omega$ denotes a volume element of the phase space. In this case

$$d\omega=dq_1dp_1\cdots dq_{3N}dp_{3N},$$



Then, making the substitution I find that

$$Q_{3N}=\frac{L^{3N}}{(3N)!h^{3N}} \left[\int_{-\infty}^{+\infty} e^{-\beta c p_j}dp_j\right]^{3N}.$$

$L$ being the "length" of the space available. But I'm pretty sure that this integral does not converge.

Where am I wrong?

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1 Answer 1

up vote 2 down vote accepted

Energy has to be bounded below. The relationship between energy & momentum in this case is $E_i = c |p_i|$, not $E_i =c p_i$. So the integral you should be trying is $\int_{-\infty}^\infty e^{-\beta c |p_i|} dp_i$, which converges just fine.

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Yes, you are right. Because for each particle $E=cp$ where $p=\sqrt{\mathbf{p}\cdot\mathbf{p}}=\sqrt{p_{x}^{2}+p_{y}^{2}+p_{z}^{2}}=|p_{x}|‌​$ if we consider that the motion is along the x-axis. Thanks! –  Anuar Dec 1 '12 at 20:22

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