In computational physics, variational Monte Carlo (VMC) is a quantum Monte Carlo method that applies the variational method to approximate the ground state of a quantum system. The basic building block is a generic wave function | Ψ ( a ) ⟩ {\displaystyle |\Psi (a)\rangle } depending on some parameters a {\displaystyle a} . The optimal values of the parameters a {\displaystyle a} is then found upon minimizing the total energy of the system. In particular, given the Hamiltonian H {\displaystyle {\mathcal {H}}} , and denoting with X {\displaystyle X} a many-body configuration, the expectation value of the energy can be written as:
E ( a ) = ⟨ Ψ ( a ) | H | Ψ ( a ) ⟩ ⟨ Ψ ( a ) | Ψ ( a ) ⟩ = ∫ | Ψ ( X , a ) | 2 H Ψ ( X , a ) Ψ ( X , a ) d X ∫ | Ψ ( X , a ) | 2 d X . {\displaystyle E(a)={\frac {\langle \Psi (a)|{\mathcal {H}}|\Psi (a)\rangle }{\langle \Psi (a)|\Psi (a)\rangle }}={\frac {\int |\Psi (X,a)|^{2}{\frac {{\mathcal {H}}\Psi (X,a)}{\Psi (X,a)}}\,dX}{\int |\Psi (X,a)|^{2}\,dX}}.}
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