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Variational method quantum mechanics - Introduction |  | Variational method quantum mechanics - Introduction: Encyclopedia II - Variational method quantum mechanics - Introduction |  | Suppose we are given a Hilbert space and a Hermitian operator over it called the Hamiltonian H. Ignoring complications about continuous spectra, we look at the discrete spectrum of H and the corresponding eigenspaces of each eigenvalue λ (see spectral theorem for Hermitian operators for the mathematical background):
with
and
.
Physical states are normalized, meaning that their norm is equal to 1. Once again ignoring complica ...
See also:Variational method quantum mechanics, Variational method quantum mechanics - Introduction, Variational method quantum mechanics - Ansatz |  | | Variational method quantum mechanics, Variational method quantum mechanics - Ansatz, Variational method quantum mechanics - Introduction, Hartree-Fock method, Ritz method |  | |
|  |  | Variational method quantum mechanics: Encyclopedia II - Variational method quantum mechanics - Introduction
Variational method quantum mechanics - Introduction
Suppose we are given a Hilbert space and a Hermitian operator over it called the Hamiltonian H. Ignoring complications about continuous spectra, we look at the discrete spectrum of H and the corresponding eigenspaces of each eigenvalue λ (see spectral theorem for Hermitian operators for the mathematical background):
with
and
.
Physical states are normalized, meaning that their norm is equal to 1. Once again ignoring complications involved with a continuous spectrum of H, suppose it is bounded from below and that its greatest lower bound is E0. Suppose also that we know the corresponding state |ψ>. The expectation value of H is then
Other related archivesHamiltonian, Hartree-Fock method, Hermitian operator, Hilbert space, Quantum mechanics, Ritz method, ansatz, continuous spectra, discrete spectrum, eigenspaces, eigenvalue, expectation value, global minimum, greatest lower bound, ground state, quantum mechanics, spectral theorem for Hermitian operators, variational principle
 Adapted from the Wikipedia article "Introduction", under the G.N U Free Docmentation License. Please also see http://en.wikipedia.org/wiki |
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