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The aim of this section is to introduce the Quantum Monte Carlo (QMC)
technique, its origins and the current state of progress in the field.
It concentrates on the aspects of QMC relevant to the work
carried out in section
, specifically the Variational Quantum
Monte Carlo technique (VMC) and the choice of trial wavefunction used in
VMC. Attention is drawn to the limitations of the technique
such as the restrictions on the choice of the variational trial
wavefunction due to the cusp condition and the problem of the fixed
nodal surface of the wavefunction. Some of these problems also relate
to the Diffusion Quantum Monte Carlo (DMC) technique which is also briefly
introduced.
Andrew Williamson
Mon May 22 14:48:37 BST 1995