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ODDONLYGW and EVENONLYGW:
reducing the
-grid for the response functions
ODDONLYGW= .TRUE. | .FALSE.
EVENONLYGW= .TRUE. | .FALSE.
ODDONLYGW allows to avoid the inclusion of the
-point in the evaluation of response functions.
The independent particle polarizability
is given by:
 |
(84) |
If the
point is included in the summation over
, convergence
is very slow for some materials (e.g. GaAs).
To deal with this problem the flag ODDONLYGW has been included.
In the automatic mode, the
-grid is given by (see Sec. 5.5.3):
If the three integers
sum to an odd value, the
-point is included in
the previous summation in the GW routine (ODDONLYGW=.TRUE.).
Note that other routines (linear optical properties) presently do not recognize this flag.
EVENONLYGW=.TRUE. is only of limited use and restricts the summation to
-points with
being even (
-point and from there on ever second k-point included).
Accelerations are also possible by evaluating the response function
itself at a restricted number of
-points.
Note that the GW loop, involves a sum over
, and a second one over
(the index in the response function). To
some extend both can be varied independently. The former one by
using ODDONLYGW, and the latter one
using the Hartree-Fock related flags NKRED, NKREDX, NKREDY, NKREDZ and EVENONLY, ODDONLY.
As explained in Sec. 6.69.9 the index
can be restricted to the values
 |
(85) |
The integer grid reduction factors are either set separately through
=NKREDX,
=NKREDY, and
=NKREDZ, or simultaneously
through
=NKRED.
Next: LSELFENERGY: the frequency dependent
Up: Frequency dependent GW calculations
Previous: ENCUTGWSOFT soft cutoff for
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Martijn Marsman
2012-06-01