Approximation methods

variational method

The variational method is a clever way to estimate a system's lowest energy without solving its equations exactly. It rests on a guarantee: the average energy computed for any guessed state can never dip below the true ground-state energy. So if we cook up a family of plausible guesses and compute the energy of each, the smallest value we find is our best upper bound on the real answer — and it can only be too high, never too low.

In practice we write down a trial wavefunction with a few adjustable knobs — a width, a spread, a shape parameter — compute the average energy as a function of those knobs, and then turn the knobs to make that energy as small as possible. The minimum we reach is an estimate of the ground-state energy, and the shape that achieves it is an approximation to the ground-state wavefunction itself. The richer and more flexible the trial form, the closer we can creep toward the truth.

What makes the method so beloved is its honesty and robustness. Even a crude guess gives a respectable energy estimate, because the energy is insensitive to small errors in the state near the true ground state. It powers practical calculations across chemistry and physics, from estimating atomic and molecular energies to the foundations of methods used in modern quantum chemistry, where exact solutions are simply out of reach.

E_trial = ⟨ψ|H|ψ⟩ / ⟨ψ|ψ⟩ ≥ E_ground, then minimize

Any trial state's average energy is an upper bound; tune the trial to push it as low as you can.

A low energy does not guarantee a good wavefunction everywhere. The energy can come out close to the truth even when the trial state misrepresents the real one in fine detail, so other properties may be less accurate.

Also called
variational techniqueRayleigh-Ritz method里兹变分法瑞利-里茲變分法