# Free particle partition function in microcanonical ensemble

From M. Tuckerman, Statistical Mechanics, 3.5 The free particle and ideal gas

It is said that the 1D free particle would have partition function

$$\Omega = \frac{E_0L\sqrt{2m}}{h\sqrt{E}}$$

where $E_0$ is the width of the "thickness "of the microcanonical $\delta$ funciton shell, and $E$ is the energy of the particle. It is really anti-intuition to see that the particle would have less possible states and less entropy when it has more energy. Could anyone explain?

That is correct: when the 1D particle is going faster, the energy width $\Delta E$ corresponds to a smaller slice $\Delta p$ in momentum, and so the shell takes up less area in phase space.
Remember that ensembles are just probability distributions. The variable $E_0$ here is how accurately you know the energy of the particle. If $E_0$ is a constant (for some reason), then for faster states you really do know the state more accurately and there is a smaller information entropy.
It's worth noting there is an alternative entropy you can define which is the "volume entropy", counting all states below energy $E$. This obviously does not correspond to information entropy since it doesn't depend on $E_0$. However, this entropy does strictly increase with $E$. With volume entropy you do recover some equations which look like thermodynamics, however it has some other problems (see also Gibbs link above).
If you want a valid temperature, you have to use the canonical ensemble, and lo and behold, one finds the entropy and temperature increase with energy in this case. The energy you get is simply $kT/2$.