From the very beginning, quantum statistical mechanics can be formulat
ed in terms of a thermodynamic potential, which has the electron densi
ty as the basic variable. By employing a well-known procedure in quant
um statistical mechanics for the construction of stationarity principl
es [ T. D. Lee and C.N. Yang, Phys. Rev. 113, 1165, (1959); 117,. 22 (
1960)], the variational principles of Hohenberg, Kohn [ P. Hohenberg a
nd W. Kohn, Phys. Rev. B, 136, 864 (1964)], and Mermin [ N. D. Mermin,
Phys. Rev. A 137, 1441 (1965)] are obtained as are generalizations th
ereof.