[Wannier] understanding the wannier function of Si
Yongsheng Zhang
yshzhang88 at yahoo.com
Sun Oct 13 16:17:15 CEST 2019
Dear all,
I am trying to learnthe wannier90 code using the well-known Si compound, which is an example fromthe tutorial. “num_bands = 12 and num_wann = 8” and “initial projections: Si :sp3”. Everything looks fine: no any error message is generated and WF bandstructures are good agreement with the DFT band structures. However, when I visualize thegenerated 8 WF (name. xsf), there are two points against my intuitions.
1. The WF at each Si does looks like the sp3 hybridizations.But why the WF at the two inequilibrium Siatoms does not look similar in shape and size. I believe it’s due to the DFT calculationaccuracy. However, with increasing the k-mesh from (4x4x4) to (6x6x6), it doesnot improve too much.
2. In principle, the sp3 hybridized functions at two inequilibriumSi sites form the covalence bonds. It means that the hybridized functions withthe same sign from the two Si atoms should “mix” with each other and form thecovalence bonds. However, from the current WF, it seems that the sp3 hybridizedfunctions with the opposite signs from the two Si atoms sit on the bond (see attachment).It is really confused me.
Please help me understanding the WFs of Si.The followings are the si.nscf and si.win file. Many thanks.
Best
Yongsheng Zhang
Si.nscf
&control
calculation = 'nscf'
restart_mode = 'from_scratch'
prefix = 'si'
pseudo_dir = 'pseudo/'
outdir = 'out/'
/
&system
ibrav = 0
nat = 2
ntyp = 1
ecutwfc = 25.0
ecutrho = 200.0
nbnd = 12
/
&electrons
conv_thr = 1.0d-12
diagonalization = 'cg'
diago_full_acc = .true.
/
ATOMIC_SPECIES
Si 28. Si.pbe-n-van.UPF
ATOMIC_POSITIONS crystal
Si -0.25 0.75 -0.25
Si 0.00 0.00 0.00
CELL_PARAMETERS bohr
-5.1 0.0 5.1
0.0 5.1 5.1
-5.1 5.1 0.0
K_POINTS crystal
64
0.00000000 0.00000000 0.00000000 1.562500e-02
0.00000000 0.00000000 0.25000000 1.562500e-02
0.00000000 0.00000000 0.50000000 1.562500e-02
0.00000000 0.00000000 0.75000000 1.562500e-02
0.00000000 0.25000000 0.00000000 1.562500e-02
0.00000000 0.25000000 0.25000000 1.562500e-02
0.00000000 0.25000000 0.50000000 1.562500e-02
0.00000000 0.25000000 0.75000000 1.562500e-02
0.00000000 0.50000000 0.00000000 1.562500e-02
0.00000000 0.50000000 0.25000000 1.562500e-02
0.00000000 0.50000000 0.50000000 1.562500e-02
0.00000000 0.50000000 0.75000000 1.562500e-02
0.00000000 0.75000000 0.00000000 1.562500e-02
0.00000000 0.75000000 0.25000000 1.562500e-02
0.00000000 0.75000000 0.50000000 1.562500e-02
0.00000000 0.75000000 0.75000000 1.562500e-02
0.25000000 0.00000000 0.00000000 1.562500e-02
0.25000000 0.00000000 0.25000000 1.562500e-02
0.25000000 0.00000000 0.50000000 1.562500e-02
0.25000000 0.00000000 0.75000000 1.562500e-02
0.25000000 0.25000000 0.00000000 1.562500e-02
0.25000000 0.25000000 0.25000000 1.562500e-02
0.25000000 0.25000000 0.50000000 1.562500e-02
0.25000000 0.25000000 0.75000000 1.562500e-02
0.25000000 0.50000000 0.00000000 1.562500e-02
0.25000000 0.50000000 0.25000000 1.562500e-02
0.25000000 0.50000000 0.50000000 1.562500e-02
0.25000000 0.50000000 0.75000000 1.562500e-02
0.25000000 0.75000000 0.00000000 1.562500e-02
0.25000000 0.75000000 0.25000000 1.562500e-02
0.25000000 0.75000000 0.50000000 1.562500e-02
0.25000000 0.75000000 0.75000000 1.562500e-02
0.50000000 0.00000000 0.00000000 1.562500e-02
0.50000000 0.00000000 0.25000000 1.562500e-02
0.50000000 0.00000000 0.50000000 1.562500e-02
0.50000000 0.00000000 0.75000000 1.562500e-02
0.50000000 0.25000000 0.00000000 1.562500e-02
0.50000000 0.25000000 0.25000000 1.562500e-02
0.50000000 0.25000000 0.50000000 1.562500e-02
0.50000000 0.25000000 0.75000000 1.562500e-02
0.50000000 0.50000000 0.00000000 1.562500e-02
0.50000000 0.50000000 0.25000000 1.562500e-02
0.50000000 0.50000000 0.50000000 1.562500e-02
0.50000000 0.50000000 0.75000000 1.562500e-02
0.50000000 0.75000000 0.00000000 1.562500e-02
0.50000000 0.75000000 0.25000000 1.562500e-02
0.50000000 0.75000000 0.50000000 1.562500e-02
0.50000000 0.75000000 0.75000000 1.562500e-02
0.75000000 0.00000000 0.00000000 1.562500e-02
0.75000000 0.00000000 0.25000000 1.562500e-02
0.75000000 0.00000000 0.50000000 1.562500e-02
0.75000000 0.00000000 0.75000000 1.562500e-02
0.75000000 0.25000000 0.00000000 1.562500e-02
0.75000000 0.25000000 0.25000000 1.562500e-02
0.75000000 0.25000000 0.50000000 1.562500e-02
0.75000000 0.25000000 0.75000000 1.562500e-02
0.75000000 0.50000000 0.00000000 1.562500e-02
0.75000000 0.50000000 0.25000000 1.562500e-02
0.75000000 0.50000000 0.50000000 1.562500e-02
0.75000000 0.50000000 0.75000000 1.562500e-02
0.75000000 0.75000000 0.00000000 1.562500e-02
0.75000000 0.75000000 0.25000000 1.562500e-02
0.75000000 0.75000000 0.50000000 1.562500e-02
0.75000000 0.75000000 0.75000000 1.562500e-02
Si.win:
use_ws_distance = .true.
num_bands = 12
num_wann = 8
num_iter = 100
dis_num_iter = 100
dis_froz_max = 6.5
dis_win_max = 17
iprint = 2
num_dump_cycles = 10
num_print_cycles = 10
!! To plot the WFs
! restart = plot
wannier_plot = true
wannier_plot_supercell = 3
! wannier_plot_list = 1,5
!! To plot the WF interpolatedbandstructure
bands_plot = .true.
bands_num_points = 200
begin kpoint_path
L 0.50000 0.50000 0.5000 G 0.00000 0.000000.0000
G 0.00000 0.00000 0.0000 X 0.50000 0.000000.5000
X 0.50000 -0.50000 0.0000 K 0.37500-0.37500 0.0000
K 0.37500 -0.37500 0.0000 G 0.00000 0.00000 0.0000
end kpoint_path
begin projections
Si : sp3
end projections
mp_grid = 4 4 4
begin kpoints
0.00000000 0.00000000 0.00000000
0.00000000 0.00000000 0.25000000
0.00000000 0.00000000 0.50000000
0.00000000 0.00000000 0.75000000
0.00000000 0.25000000 0.00000000
0.00000000 0.25000000 0.25000000
0.00000000 0.25000000 0.50000000
0.00000000 0.25000000 0.75000000
0.00000000 0.50000000 0.00000000
0.00000000 0.50000000 0.25000000
0.00000000 0.50000000 0.50000000
0.00000000 0.50000000 0.75000000
0.00000000 0.75000000 0.00000000
0.00000000 0.75000000 0.25000000
0.00000000 0.75000000 0.50000000
0.00000000 0.75000000 0.75000000
0.25000000 0.00000000 0.00000000
0.25000000 0.00000000 0.25000000
0.25000000 0.00000000 0.50000000
0.25000000 0.00000000 0.75000000
0.25000000 0.25000000 0.00000000
0.25000000 0.25000000 0.25000000
0.25000000 0.25000000 0.50000000
0.25000000 0.25000000 0.75000000
0.25000000 0.50000000 0.00000000
0.25000000 0.50000000 0.25000000
0.25000000 0.50000000 0.50000000
0.25000000 0.50000000 0.75000000
0.25000000 0.75000000 0.00000000
0.25000000 0.75000000 0.25000000
0.25000000 0.75000000 0.50000000
0.25000000 0.75000000 0.75000000
0.50000000 0.00000000 0.00000000
0.50000000 0.00000000 0.25000000
0.50000000 0.00000000 0.50000000
0.50000000 0.00000000 0.75000000
0.50000000 0.25000000 0.00000000
0.50000000 0.25000000 0.25000000
0.50000000 0.25000000 0.50000000
0.50000000 0.25000000 0.75000000
0.50000000 0.50000000 0.00000000
0.50000000 0.50000000 0.25000000
0.50000000 0.50000000 0.50000000
0.50000000 0.50000000 0.75000000
0.50000000 0.75000000 0.00000000
0.50000000 0.75000000 0.25000000
0.50000000 0.75000000 0.50000000
0.50000000 0.75000000 0.75000000
0.75000000 0.00000000 0.00000000
0.75000000 0.00000000 0.25000000
0.75000000 0.00000000 0.50000000
0.75000000 0.00000000 0.75000000
0.75000000 0.25000000 0.00000000
0.75000000 0.25000000 0.25000000
0.75000000 0.25000000 0.50000000
0.75000000 0.25000000 0.75000000
0.75000000 0.50000000 0.00000000
0.75000000 0.50000000 0.25000000
0.75000000 0.50000000 0.50000000
0.75000000 0.50000000 0.75000000
0.75000000 0.75000000 0.00000000
0.75000000 0.75000000 0.25000000
0.75000000 0.75000000 0.50000000
0.75000000 0.75000000 0.75000000
end kpoints
begin atoms_frac
Si -0.25 0.75 -0.25
Si 0.00 0.00 0.00
end atoms_frac
begin unit_cell_cart
bohr
-5.10 0.00 5.10
0.00 5.10 5.10
-5.10 5.10 0.00
end unit_cell_cart
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