Chapter 7
Temperature-Dependent Perturbation Theory
Consider the partition function
with β = 1/kT, N0 the number operator for electrons, and the hamiltonian H = H0 + V split into an unperturbed part H0 and a perturbation V. The factorization
is introduced, where the relation S(β) = exp[β(H0 – μN0)] exp[– β(H – μN0)] is used. Correspondingly, the unperturbed partition function
is defined permitting the expression Z(β) = Z0(β)S(β)0, where the average …0 is formed with the density operator ρ = Z0–1(β) exp[–β(H0 – μN0)].
Since S(0) = 1, it follows that Explicit differentiation yields
and the notation ...
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