Zero-variance zero-bias quantum Monte Carlo estimators of the spherically and system-averaged pair density
arXiv:0705.0721 · doi:10.1063/1.2746029
Abstract
We construct improved quantum Monte Carlo estimators for the spherically- and system-averaged electron pair density (i.e. the probability density of finding two electrons separated by a relative distance u), also known as the spherically-averaged electron position intracule density I(u), using the general zero-variance zero-bias principle for observables, introduced by Assaraf and Caffarel. The calculation of I(u) is made vastly more efficient by replacing the average of the local delta-function operator by the average of a smooth non-local operator that has several orders of magnitude smaller variance. These new estimators also reduce the systematic error (or bias) of the intracule density due to the approximate trial wave function. Used in combination with the optimization of an increasing number of parameters in trial Jastrow-Slater wave functions, they allow one to obtain well converged correlated intracule densities for atoms and molecules. These ideas can be applied to calculating any pair-correlation function in classical or quantum Monte Carlo calculations.
13 pages, 9 figures, published version
Cited by in corpus (4)
- Applications of quantum Monte Carlo methods in condensed systems
- Full optimization of Jastrow-Slater wave functions with application to the first-row atoms and homonuclear diatomic molecules
- Kohn-Sham potentials in exact density-functional theory at non-integer electron numbers
- Heavy-tailed random error in quantum Monte Carlo