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Exit code for early stop due to Fermi shift
Fixes #57 We introduce an exit code for the early stop of `hp.x` when it detects an insulator treated as a metal, which would otherwise finish with exit status 0, but without any actual useful data produced.
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Original file line number | Diff line number | Diff line change |
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&INPUTHP | ||
conv_thr_chi = 1.0000000000d-06 | ||
determine_q_mesh_only = .true. | ||
find_atpert = 3 | ||
iverbosity = 2 | ||
max_seconds = 3.4200000000d+03 | ||
nq1 = 4 | ||
nq2 = 4 | ||
nq3 = 4 | ||
outdir = 'out' | ||
perturb_only_atom(13) = .true. | ||
prefix = 'aiida' | ||
/ |
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Program HP v.7.2 starts on 5Jun2023 at 13:54:28 | ||
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This program is part of the open-source Quantum ESPRESSO suite | ||
for quantum simulation of materials; please cite | ||
"P. Giannozzi et al., J. Phys.:Condens. Matter 21 395502 (2009); | ||
"P. Giannozzi et al., J. Phys.:Condens. Matter 29 465901 (2017); | ||
"P. Giannozzi et al., J. Chem. Phys. 152 154105 (2020); | ||
URL http://www.quantum-espresso.org", | ||
in publications or presentations arising from this work. More details at | ||
http://www.quantum-espresso.org/quote | ||
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Parallel version (MPI), running on 48 processors | ||
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MPI processes distributed on 1 nodes | ||
K-points division: npool = 16 | ||
R & G space division: proc/nbgrp/npool/nimage = 3 | ||
24962 MiB available memory on the printing compute node when the environment starts | ||
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=---------------------------------------------------------------------------= | ||
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Calculation of Hubbard parameters using the HP code based on DFPT | ||
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Please cite the following papers when using this program: | ||
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- HP code : Comput. Phys. Commun. 279, 108455 (2022). | ||
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- Theory : Phys. Rev. B 98, 085127 (2018) and | ||
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Phys. Rev. B 103, 045141 (2021). | ||
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=-----------------------------------------------------------------------------= | ||
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Reading xml data from directory: | ||
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out/aiida.save/ | ||
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IMPORTANT: XC functional enforced from input : | ||
Exchange-correlation= PBESOL | ||
( 1 4 10 8 0 0 0) | ||
Any further DFT definition will be discarded | ||
Please, verify this is what you really want | ||
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Parallelization info | ||
-------------------- | ||
sticks: dense smooth PW G-vecs: dense smooth PW | ||
Min 905 905 271 30463 30463 5034 | ||
Max 906 906 271 30465 30465 5035 | ||
Sum 2717 2717 813 91393 91393 15103 | ||
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Using Slab Decomposition | ||
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Check: negative core charge= -0.000036 | ||
Reading collected, re-writing distributed wavefunctions | ||
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bravais-lattice index = 0 | ||
lattice parameter (alat) = 12.3672 (a.u.) | ||
unit-cell volume = 1453.9300 (a.u.)^3 | ||
number of atoms/cell = 16 | ||
number of atomic types = 2 | ||
kinetic-energy cut-off = 60.00 (Ry) | ||
charge density cut-off = 240.00 (Ry) | ||
conv. thresh. for NSCF = 1.0E-11 | ||
conv. thresh. for chi = 1.0E-06 | ||
Input Hubbard parameters (in eV): | ||
V ( 1, 1) = 5.0000 | ||
V ( 1, 229) = 0.0000 | ||
V ( 1, 230) = 0.0000 | ||
V ( 2, 2) = 5.0000 | ||
V ( 2, 6) = 0.0000 | ||
V ( 2, 405) = 0.0000 | ||
V ( 3, 3) = 5.0000 | ||
V ( 4, 4) = 5.0000 | ||
V ( 5, 5) = 0.0000 | ||
V ( 5, 34) = 0.0000 | ||
V ( 5, 209) = 0.0000 | ||
V ( 6, 2) = 0.0000 | ||
V ( 6, 6) = 0.0000 | ||
V ( 6, 209) = 0.0000 | ||
V ( 7, 7) = 0.0000 | ||
V ( 8, 8) = 0.0000 | ||
V ( 9, 9) = 0.0000 | ||
V ( 10, 10) = 0.0000 | ||
V ( 11, 11) = 0.0000 | ||
V ( 12, 12) = 0.0000 | ||
V ( 13, 13) = 0.0000 | ||
V ( 14, 14) = 0.0000 | ||
V ( 15, 15) = 0.0000 | ||
V ( 16, 16) = 0.0000 | ||
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celldm(1) = 12.36723 celldm(2) = 0.00000 celldm(3) = 0.00000 | ||
celldm(4) = 0.00000 celldm(5) = 0.00000 celldm(6) = 0.00000 | ||
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crystal axes: (cart. coord. in units of alat) | ||
a(1) = ( 0.5609 0.5784 0.5924 ) | ||
a(2) = ( 0.5609 -0.5784 -0.5924 ) | ||
a(3) = ( -0.5609 0.5784 -0.5924 ) | ||
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reciprocal axes: (cart. coord. in units 2 pi/alat) | ||
b(1) = ( 0.8915 0.8645 0.0000 ) | ||
b(2) = ( 0.8915 0.0000 -0.8440 ) | ||
b(3) = ( 0.0000 0.8645 -0.8440 ) | ||
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Atoms inside the unit cell (Cartesian axes): | ||
site n. atom mass positions (alat units) | ||
1 W 183.8400 tau( 1) = ( -0.28043 0.57835 -0.55568 ) | ||
2 W 183.8400 tau( 2) = ( 0.84128 0.00000 -0.03673 ) | ||
3 W 183.8400 tau( 3) = ( 0.28043 0.00000 -0.55450 ) | ||
4 W 183.8400 tau( 4) = ( 0.28043 0.57835 -0.03791 ) | ||
5 O 15.9994 tau( 5) = ( 0.00000 0.00000 0.00000 ) | ||
6 O 15.9994 tau( 6) = ( 0.56086 0.00000 0.00000 ) | ||
7 O 15.9994 tau( 7) = ( 0.56086 0.57835 0.00000 ) | ||
8 O 15.9994 tau( 8) = ( 0.00000 0.57835 0.00000 ) | ||
9 O 15.9994 tau( 9) = ( 0.28043 0.28397 0.03317 ) | ||
10 O 15.9994 tau( 10) = ( 0.28043 0.29438 -0.62558 ) | ||
11 O 15.9994 tau( 11) = ( -0.28043 0.29438 -0.55923 ) | ||
12 O 15.9994 tau( 12) = ( 0.84128 0.28397 -0.03317 ) | ||
13 O 15.9994 tau( 13) = ( 0.28043 0.00000 -0.87440 ) | ||
14 O 15.9994 tau( 14) = ( 0.28043 0.57835 0.28199 ) | ||
15 O 15.9994 tau( 15) = ( 0.28043 0.00000 -0.26540 ) | ||
16 O 15.9994 tau( 16) = ( 0.28043 0.57835 -0.32701 ) | ||
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Atom which will be perturbed: | ||
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13 O 15.9994 tau(13) = ( 0.28043 0.00000 -0.87440 ) | ||
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Reading xml data from directory: | ||
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out/aiida.save/ | ||
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IMPORTANT: XC functional enforced from input : | ||
Exchange-correlation= PBESOL | ||
( 1 4 10 8 0 0 0) | ||
Any further DFT definition will be discarded | ||
Please, verify this is what you really want | ||
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Parallelization info | ||
-------------------- | ||
sticks: dense smooth PW G-vecs: dense smooth PW | ||
Min 905 905 271 30463 30463 5034 | ||
Max 906 906 271 30465 30465 5035 | ||
Sum 2717 2717 813 91393 91393 15103 | ||
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Using Slab Decomposition | ||
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Check: negative core charge= -0.000036 | ||
Reading collected, re-writing distributed wavefunctions | ||
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===================================================================== | ||
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PERTURBED ATOM # 13 | ||
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site n. atom mass positions (alat units) | ||
13 O 15.9994 tau(13) = ( 0.28043 0.00000 -0.87440 ) | ||
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===================================================================== | ||
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The perturbed atom has a type which is not unique! | ||
Changing the type of the perturbed atom and recomputing the symmetries... | ||
The number of symmetries is reduced : | ||
nsym = 4 nsym_PWscf = 8 | ||
Changing the type of the perturbed atom back to its original type... | ||
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# Lots of lines neglected | ||
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=--------------------------------------------= | ||
SOLVE THE LINEAR SYSTEM | ||
=--------------------------------------------= | ||
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atom # 2 q point # 1 iter # 1 | ||
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Pert. # 1: Fermi energy shift (Ry) = -4.4413E+01 -2.8580E-03 | ||
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WARNING: The Fermi energy shift is zero or too big! | ||
This may happen in two cases: | ||
1. The DOS at the Fermi level is too small: | ||
DOS(E_Fermi) = -0.3691E-05 | ||
This means that most likely the system has a gap, | ||
and hence it should NOT be treated as a metal | ||
(otherwise numerical instabilities will appear). | ||
2. Numerical instabilities due to too low cutoff | ||
for hard pseudopotentials. | ||
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Stopping... | ||
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Solution (for magnetic insulators): | ||
Try to use the 2-step scf procedure as in HP/example02 | ||
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# Lots of lines neglected | ||
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Called by init_run: | ||
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Called by electrons: | ||
v_of_rho : 0.17s CPU 0.21s WALL ( 2 calls) | ||
v_h : 0.01s CPU 0.01s WALL ( 2 calls) | ||
v_xc : 0.17s CPU 0.20s WALL ( 2 calls) | ||
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Called by c_bands: | ||
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Called by sum_band: | ||
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Called by *egterg: | ||
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Called by h_psi: | ||
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General routines | ||
fft : 0.09s CPU 0.16s WALL ( 22 calls) | ||
davcio : 0.00s CPU 0.02s WALL ( 6 calls) | ||
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Parallel routines | ||
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Hubbard U routines | ||
alloc_neigh : 0.33s CPU 0.34s WALL ( 2 calls) | ||
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init_vloc : 0.37s CPU 0.37s WALL ( 2 calls) | ||
init_us_1 : 0.02s CPU 0.03s WALL ( 2 calls) | ||
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PRINTING TIMING FROM HP ROUTINES: | ||
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PRINTING TIMING FROM LR MODULE: | ||
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HP : 2.09s CPU 3.79s WALL | ||
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This run was terminated on: 13:54:32 5Jun2023 | ||
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=------------------------------------------------------------------------------= | ||
JOB DONE. | ||
=------------------------------------------------------------------------------= |
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