With , set
Then
Part (b) gives
For identical classical non-interacting particles,
Using ,
where
This is the canonical partition function for an ultrarelativistic gas in a power-law trap.
Only the term depends on , so
Thus the equation of state is
Write . Since contains ,
Consequently
in the thermodynamic limit: relative energy fluctuations vanish.
The normalized one-particle spatial density gives the local number density
The radial probability density is proportional to
Its logarithmic derivative vanishes when
so the most likely radius is

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