QSGW calculations for ErAs starting from LDA+U
This tutorial presents an LDA+U calculation for ErAs. The LDA provides a very poor description of the Er f states (a large number of minority states are improperly clustered at the Fermi level). It is followed QSGW calculation, using LDA+U as the starting point.
Note: this page is under construction.
blm --nit=20 --nk=6 --gmax=9 --mag --gw eras
nano actrl.eras
cp actrl.eras ctrl.eras
lmfa eras
mpix -np=16 lmf-MPIK ctrl.eras -vnit=20
mpix -np=16 lmf-MPIK ctrl.eras -vnit=1 --rs=1,0 -vldau=t eras
rm mixm.eras
mpix -np=16 lmf-MPIK ctrl.eras -vnit=20 -vldau=t eras
lmfgwd ctrl.eras -vnit=1 -vumix=1 -vldau=t --job=-1
nano GWinput
Table of Contents
Input file setup
ErAs forms in the rocksalt structure with a lattice constant 5.408 a0. However, it is thought to be an antiferromagnet, with Er along the [111] line alternating spins. There for the the unit cell of the rocksalt structure must be doubled to accommodate two inequivalent Er atoms The spin magnetic moment of 3 μB. This information is encapsulated in init file below.
Copy the contents in the box below into init.eras. Note that a trial moment of ±3 μB is assumed; this will be determined in the course of a self-consistent calculation.
LATTICE
ALAT=10.83
PLAT= 0.5 0.5 1.0 0.5 1.0 0.5 1.0 0.5 0.5
SPEC
ATOM=Er MMOM=0,0,0,3 PZ=0 0 0 5.5 # Trial spin moment on the f channel
IDMOD=0,1
INCLUDE ldauparm
ATOM=Er2 MMOM=0,0,0,-3 PZ=0 0 0 5.5 # Trial spin moment on the f channel
IDMOD=0,1
INCLUDE ldauparm
SITE
ATOM=Er POS= 0.0 0.0 0.0
ATOM=Er2 POS= 1.0 1.0 1.0
ATOM=As POS= 0.5 0.5 0.5
ATOM=As POS= 1.5 1.5 1.5
Note also the line INCLUDE ldauparm
. There is little point in attempting an LDA calculation. We will begin directly with an LDA+U calculation; parameters U and J are supplied in file ldauparm. Copy the contents in the box below into ldauparm.
% ifdef ldau==2
IDU=0,0,0,112 UH=0,0,0,0 JH=0,0,0,0
% elseif ldau
IDU= 0 0 0 112 UH= 0 0 0 0.632 JH= 0 0 0 0.055
% endif