As per the Bose-Einstein system,
The particles are indistinguishable.
Let total number of particle in the system is "n_i" , energy "E_i"
and let the statistical weight factor(degeneracy) is "g_i"
.Now, the way of the distribution of "n_i" particle into "g_i" space,
So, the distribution "\\dfrac{(n_i-g_i-1)!}{n_i(g_i-1)!}"
for "n_o" particle,
we know that thermodynamic probability "w=\\dfrac{(n_o-g_o-1)!}{n_o(g_o-1)!}.\\dfrac{(n_1-g_1-1)!}{n_1(g_1-1)!}.........\\dfrac{(n_i-g_i-1)!}{n_i(g_i-1)!}"
So, we can write it as "w=\\Pi\\dfrac{(n_i-g_i-1)!}{n_i(g_i-1)!}"
Hence "\\ln w=\\sum {\\ln((n_i-g_i-1)!)- \\ln n_i-\\ln(g_i-1)!}"
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