A new many-body theoretical scheme based on the functional Schrodinger
picture is presented. It is shown that the many-particle Schrodinger
equation becomes a functional differential equation in this formalism.
Using the Hubbard Hamiltonian and the BCS superconductivity as exampl
es, the functional differential equations;the solved variationally to
yield both the symmetry conserving and the symmetry breaking mean-fiel
d solutions. Extension of the theory to finite temperature is also dis
cussed using the density matrix formalism. This formalism is shown to
lead to successful calculations of the Helmholtz free energy and the t
otal energy of the electron gas system.