[QE-users] under pressure PbTaSe2 vc-relax calculation

Nicola Marzari nicola.marzari at epfl.ch
Wed May 26 10:35:44 CEST 2021



Dear all,


1) a perennial recommendation of mine is indeed to make sure the cutoffs 
for wfcs and rho are both enough to have the stress well converged - 
this was one key critiations for the SSSP (that you can find here 
https://www.materialscloud.org/discover/sssp/). Reasonably tuned 
parameters and appropriate pseudopotentials for any input structure can 
be obtained from here:
https://www.materialscloud.org/work/tools/qeinputgenerator

Your mileage might vary, and you might be able to get away with looser 
thresholds, or need tighter ones, but that is a recommended starting 
point, to understand what you need.

2) a second recommendaiton in dealing with solids is to use PBEsol 
rather than PBE as a first default choice.

As always, test crtically these input parameters to understand how they 
are affecting your calculations.

			nicola


On 26/05/2021 10:28, Stefano de Gironcoli wrote:
> more than with a different set of k-points, the last scf  is done 
> resetting the spherical cutoff according to the last cell (during the 
> vc-relaxation the G vectors in the list are deformed but the miller 
> indices included in the list are not updated and the sphere actually 
> deforms into an ellipsoid ).
> 
> As the pressure converges slowly with cutoff if the pressure changes 
> significantly this is an indication that the cutoff might have been too 
> low or that  the cell has changed a lot.
> 
> stefano
> 
> On 26/05/21 09:40, mkondrin wrote:
>> Dear Rencong,
>>
>> I believe that the last step in vc-relax calculations is made in 
>> slightly different Brillouin zone (calculated in relaxed variable cell 
>> parameters), so the pressure calculated in the last step may be 
>> different from whose obtained in the previous step (where Brillouin 
>> zone of the original cell was used convergence criteria with desired 
>> pressure is checked).
>>
>> It also seems to me that your pressure is rather small. May be it has 
>> sense to increase the pressure to at least 10 kbar.
>>
>> Sincerely yours,
>> M. V. Kondrin
>>
>>
>> On 26.05.2021 05:48, 连云龙 wrote:
>>> Dear Rencong,
>>>
>>> I had similar experiences when I use QE pw.x to relax structures 
>>> under pressure and I want to follow this conversation.
>>>
>>> My experience is that, the behaviour and result of relaxation depend 
>>> largely on the pesudopotential.
>>>
>>> It is also helpful to investigate the energy and pressure during the 
>>> relaxation.
>>>
>>> In order for other experts to help you, could you please provide:
>>> (1) the pseudopotentials used in the calculation
>>> (2) the entire output file of pw.x, or at least the section contains 
>>> the final coordinates? (search "End of BFGS" in the output file)
>>> (3) your name and affiliation (this is the rule of the mailing list)
>>>
>>> Best,
>>> Yunlong
>>>
>>>
>>>
>>> -- 
>>> Yunlong LIAN ORCID : https://orcid.org/0000-0002-9474-2181 CSNS, 
>>> Dongguan Neutron Science Center Dongguan, Guangdong, P. R. China 连云 
>>> 龙 中国散裂中子源 中子科学部 A1-629 (内线 303) 中国广东省东莞市
>>> -----Original Messages-----
>>> From:Amadeus <760158264 at qq.com>
>>> Sent Time:2021-05-25 15:22:02 (Tuesday)
>>> To: users <users at lists.quantum-espresso.org>
>>> Cc:
>>> Subject: [QE-users] under pressure PbTaSe2 vc-relax calculation
>>>
>>>
>>> Dear QE developer
>>>
>>>
>>> I did the structural relaxation calculation for Pb at pressure of 
>>> 3kbar, this is relax.in
>>>
>>>
>>> &CONTROL
>>>    prefix='PbTaSe2',
>>>    calculation='vc-relax', pseudo_dir='../../', outdir='./tmp', 
>>> verbosity='high',
>>>    tprnfor=.true., tstress=.true., forc_conv_thr=1.0d-4, nstep=100,
>>> /
>>> &SYSTEM
>>>    ibrav= 0, nat= 4, ntyp= 3,
>>>    occupations = 'smearing', smearing = 'gauss', degauss = 1.0d-2,
>>>    ecutwfc = 50, ecutrho = 500,
>>> /
>>> &ELECTRONS
>>>    conv_thr = 1.0d-8
>>>    mixing_beta = 0.7d0
>>> /
>>> &IONS
>>> /
>>> &CELL
>>>    cell_dynamics  = "bfgs"
>>>    press          =  2.70000e+00
>>>    press_conv_thr =0.1
>>> /
>>> ATOMIC_SPECIES
>>>    Ta 180.9479 Ta.UPF
>>>    Pb 207.2 Pb.UPF
>>>    Se 78.96 Se.UPF
>>> CELL_PARAMETERS (angstrom)
>>>     3.4834700000  0.0000000000  0.0000000000
>>>    -1.7417350000  3.0167735133  0.0000000000
>>>     0.0000000000  0.0000000000  9.4755300000
>>> ATOMIC_POSITIONS (crystal)
>>>    Pb  0.0000000000  0.0000000000  0.0000000000
>>>    Se  0.0000000000  0.0000000000  0.3246710000
>>>    Ta  0.3333330000  0.6666670000  0.5000000000
>>>    Se  0.0000000000  0.0000000000  0.6753290000
>>> K_POINTS {automatic}
>>>    15 15 5 0 0 0
>>>
>>>
>>> In relax.in, press=3.0kbar. But after pw.x is done, relax.out show 
>>> that total stress  (Ry/bohr**3)  (kbar)     P=-0.83, and This is 
>>> inconsistent with press=3. this is part of relax.out
>>>
>>>
>>> [rencong at mu01 phonon]$ grep 'Computing stress (Cartesian axis) and 
>>> pressure' -A 15 relax.out
>>>
>>>
>>> ....
>>>
>>>
>>>       Computing stress (Cartesian axis) and pressure
>>>
>>>
>>>            total   stress  (Ry/bohr**3) (kbar)     P=        2.93
>>>     0.00002030  -0.00000000   0.00000000            2.99 -0.00 0.00
>>>    -0.00000000   0.00002030  -0.00000000           -0.00 2.99 -0.00
>>>    -0.00000000   0.00000000   0.00001921           -0.00 0.00 2.83
>>>
>>>
>>>       kinetic stress (kbar)  26877.23      0.00      0.00
>>>                                  0.00  26877.23     -0.00
>>>                                  0.00      0.00  26796.57
>>>
>>>
>>>       local   stress (kbar)-103340.53      0.03      0.00
>>>                                  0.03-103340.50      0.00
>>>                                  0.00      0.00  89394.48
>>>
>>>
>>>       nonloc. stress (kbar)   7797.15      0.00      0.00
>>> -- 
>>>       Computing stress (Cartesian axis) and pressure
>>>
>>>
>>>            total   stress  (Ry/bohr**3) (kbar)     P=        2.96
>>>     0.00002009  -0.00000000   0.00000000            2.96 -0.00 0.00
>>>    -0.00000000   0.00002009  -0.00000000           -0.00 2.96 -0.00
>>>     0.00000000  -0.00000000   0.00002028            0.00 -0.00 2.98
>>>
>>>
>>>       kinetic stress (kbar)  26879.49      0.00      0.00
>>>                                  0.00  26879.49     -0.00
>>>                                  0.00     -0.00  26798.86
>>>
>>>
>>>       local   stress (kbar)-103299.75      0.03      0.00
>>>                                  0.03-103299.72      0.00
>>>                                  0.00      0.00  89348.84
>>>
>>>
>>>       nonloc. stress (kbar)   7797.79     -0.00      0.00
>>> -- 
>>>       Computing stress (Cartesian axis) and pressure
>>>
>>>
>>>            total   stress  (Ry/bohr**3) (kbar)     P=       -0.83
>>>    -0.00000653  -0.00000000  -0.00000000           -0.96 -0.00 -0.00
>>>     0.00000000  -0.00000653   0.00000000            0.00 -0.96 0.00
>>>     0.00000000   0.00000000  -0.00000384            0.00 0.00 -0.56
>>>
>>>
>>>       kinetic stress (kbar)  26883.07      0.00     -0.00
>>>                                  0.00  26883.07     -0.00
>>>                                 -0.00     -0.00  26802.38
>>>
>>>
>>>       local   stress (kbar)-103303.36      0.03      0.00
>>>                                  0.03-103303.33      0.00
>>>                                  0.00      0.00  89345.22
>>>
>>>
>>>       nonloc. stress (kbar)   7795.83     -0.00      0.00
>>>
>>>
>>> _______________________________________________
>>> Quantum ESPRESSO is supported by MaX (www.max-centre.eu)
>>> users mailing list users at lists.quantum-espresso.org
>>> https://lists.quantum-espresso.org/mailman/listinfo/users
>>
>> _______________________________________________
>> Quantum ESPRESSO is supported by MaX (www.max-centre.eu)
>> users mailing list users at lists.quantum-espresso.org
>> https://lists.quantum-espresso.org/mailman/listinfo/users
> _______________________________________________
> Quantum ESPRESSO is supported by MaX (www.max-centre.eu)
> users mailing list users at lists.quantum-espresso.org
> https://lists.quantum-espresso.org/mailman/listinfo/users


-- 
----------------------------------------------------------------------
Prof Nicola Marzari, Chair of Theory and Simulation of Materials, EPFL
Director, National Centre for Competence in Research NCCR MARVEL, EPFL
http://theossrv1.epfl.ch/Main/Contact http://nccr-marvel.ch/en/project


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