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When the energy curve for bulk system is calculated as a function
of the lattice parameter, a sudden change of the number of real space grids
is a serious problem which produces an erratic discontinuity
on the energy curve. In fact, we see the discontinuity
in cases of 200 and 290 (Ryd) in Fig. 5 when the cutoff energy
is fixed. The discontinuity occurs at the lattice parameter where
the number of grids changes. To avoid the discontinuity on the energy
curve, a keyword 'scf.Ngrid' is available.
scf.Ngrid 32 32 32 # n1, n2, and n3 for a-, b-, and c-axes
When the number of grids is explicitly specified by the keyword,
the axis is discretized by the number without depending on
the keyword 'scf.energycutoff'. We see in Fig. 5 that the fixed grids
with 32x32x32 gives a smooth curve.
Figure 5:
The total energy of bcc iron as a function of lattice parameter,
where the equilibrium lattice constant a
is 2.87 Å.
A cubic unit cell including two atoms was considered.
The input file is Febcc2.dat in the directory 'work'.
 |
Next: Fixing the relative position
Up: Cutoff energy
Previous: Convergence
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2009-08-28