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My PhD thesis - Condensed Matter Theory - Imperial College London

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Chapter 4<br />

Errors in QMC simulations<br />

This chapter will describe the most significant errors inherent in extended-system<br />

QMC simulations. Two of these — statistical noise and the fixed-node error —<br />

have already been mentioned in the previous chapter; when attempting to simulate<br />

extended systems, finite-size errors also become important. 1<br />

4.1 Finite-size errors<br />

The QMC methods described in Chapter 3 apply to finite systems. To investigate the<br />

properties of materials which have infinite extent in at least one spatial dimension,<br />

some kind of scheme for extrapolation is required.<br />

In practice, such materials are studied by placing a finite set of particles in a<br />

simulation cell, which is then subjected to periodic boundary conditions. This defines<br />

a lattice (see figure 4.1). To complicate things, the particles must also undergo<br />

interactions with their periodically-repeated images; the best way to take account<br />

of this is not obvious. In this report, the particles will be exclusively electrons,<br />

interacting via the Coulomb force, the long-ranged nature of which is a key part of<br />

the problem.<br />

1 The use of pseudopotentials introduces additional errors in the simulation of real atoms, but<br />

these will not be discussed in this work.<br />

57

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