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(4.10) |
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(4.11) |
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(4.12) |
On the other hand the short range potential decays very fast in real space
and the sum converges very quickly. Since
in Eq.(4.9)
depends linearly on the potential, we can easily decompose two contributions:
a short-range and a long range one. Then the latter can be more easily
evaluated in Fourier space:
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For Coulomb interaction the potential energy becomes:
In the potential energy 4.16
the parameters
determines the convergence speed in the real and Fourier space series.
For a given choice of
we have chosen a real-space cutoff distance
and a
cutoff in the Fourier space. The cutoff
determines the total number of Fourier components,
, where
is a positive integer. This parameter has been choosen in such a way that the error on the Ewald summation is much smaller than the Quantum Monte Carlo statistical one.
A careful choice of the parameter
can minimize the error in the summation (see Ref. (80)). In our simulation we have chosen
, where
is the size of the simulation box. With this cutoff it is sufficient to sum the short range part in the eq. 4.16 only on the first image of each particle.
Notice that during each VMC or DMC simulation the ionic coordinates are fixed throughout the calculation. Therefore the contribution of the ion-ion Coulomb interaction in the short-range part can be evaluated only at the beginning of the simulation. As an electron
is moved during a VMC calculation the sum of the short range part of the eq. 4.16 is easily updated subtracting the old contribution electron-electron and electron-ion due to the electron
, and adding the new one.
The sum in Fourier space can be written as: