next up previous contents
Next: 9.6 Volume vs. energy Up: 9 Theoretical Background Previous: 9.4.3 Improved functional form

9.5 Forces

 

Within the finite temperature LDA forces are defined as the derivative of the generalized free energy. This quantity can be evaluated easily. The functional F depends on the wavefunctions tex2html_wrap_inline4687 the partial occupancies f and the positions of the ions R. In this section we will shortly discuss the variational properties of the free energy and we will explain why we calculate the forces as an derivative of the free energy. The formulas give are very symbolic and we do not take into account any constraints on the occupation numbers or the wavefunctions. We denote the whole set of wavefunctions as tex2html_wrap_inline4687 and the set of partial occupancies as f.

The electronic groundstate is determined by the variational property of the free energy i.e.

displaymath5015

for arbitrary variations of tex2html_wrap_inline4687 and f. We can rewrite the right hand side of this equation as

displaymath5016

For arbitrary variations this quantity is zero only if tex2html_wrap_inline5039 and tex2html_wrap_inline5041 , leading to a system of equations which determines tex2html_wrap_inline4687 and f at the electronic groundstate. We define the forces as derivatives of the free energy with respect to the ionic positions i.e.

displaymath5017

At the groundstate the first two terms are zero and we can write

displaymath5018

i.e. we can keep tex2html_wrap_inline4687 and f fixed at their respective groundstate values and we have to calculate the partial derivative of the free energy with respect to the ionic positions only. This is relatively easy task.

Previously we have mentioned that the only physical quantity is the energy for tex2html_wrap_inline4433 . It is in principle possible to evaluate the derivatives of E( tex2html_wrap_inline4433 ) with respect to the ionic coordinates but this is not easy and requires additional computer time.



MASTER USER VASP
Mon Mar 29 10:38:29 MEST 1999