Four bosons are distributed in a sheet of 5 states . The number of microstates ( ways ) is
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In the previous parts of this course, we derived the Boltzmann
distribution, which described how the number of distinguishable
particles in different energy states varied with the energy of
those states, at different temperatures:
nj =
N
Z
e
−
εj
kT . (1)
However, in systems consisting of collections of identical
fermions or identical bosons, the wave function of the system
has to be either antisymmetric (for fermions) or symmetric (for
bosons) under interchange of any two particles. With the
allowed wave functions, it is no longer possible to identify a
particular particle with a particular energy state. Instead, all
the particles are “shared” between the occupied states.
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