It's given a gas of particles all identical which has T fixed and spin S. Let's ##g(\epsilon)## the density of orbital states and
##g(\epsilon) = g_0## for ##\forall \epsilon \in [\epsilon_0, \epsilon_1]##, zero otherwise.
How to compute the number of accessible quantum states of one particle?
This is my attempt, and I suspect that is not good. Let S=0 and then bosons in a system.
Simply, if we have the density of orbitals we have to integrate ##g(\epsilon)## and we have...