[QE-users] NVE simulation in cp.x - large fluctuation in temperature
Jie Peng
jiepeng at umd.edu
Sat Apr 14 20:18:40 CEST 2018
Ari:
Indeed! You are right on spot. The too small size unit cell that leads to
inaccurate structure and energy is responsible for large temperature
fluctuation here.
I am trying to increase the size of the supercell now.
Thanks!
On Sat, Apr 14, 2018 at 6:06 AM, Ari P Seitsonen <Ari.P.Seitsonen at iki.fi>
wrote:
>
> Dear Jie,
>
> I do not know about the other options, but
>
> 1) simulating a periodic system of only three atoms with only the Gamma
> point cannot lead to an accurate description of the electronic structure,
> and thus the forces on the ionic cores,
>
> 2) the standard deviation in the fluctuations is supposed to be
> ~sqrt[2/(3*N_atoms)) * T_average ~= 350 K in your case, and the
> instantaneous fluctuations are of course larger
>
> Just my quick thoughts...
>
> Greetings from Sunny Zurich,
>
> apsi
>
> -=*=-=*=-=*=-=*=-=*=-=*=-=*=-=*=-=*=-=*=-=*=-=*=-=*=-=*=-=*=
> -=*=-=*=-=*=-=*=-
> Ari Paavo Seitsonen / Ari.P.Seitsonen at iki.fi / http://www.iki.fi/~apsi/
> Ecole Normale Supérieure (ENS), Département de Chimie, Paris
> Mobile (F) : +33 789 37 24 25 (CH) : +41 79 71 90 935
>
>
> On Fri, 13 Apr 2018, Jie Peng wrote:
>
> Dear all
>> I have been running MD simulations on HfS2 using cp.x code in Quantum
>> espresso. I start from initial
>> configuration obtained from pwscf vc-relax, and relax the system using
>> cp.x by consecutive steps of:
>> electron relaxation->ionic relaxation->cell relaxation. Then, I just
>> directly start a NVE simulation
>> starting from the equilibrium configuration. I expect the system to
>> almost stay stationary or the
>> temperature should be very small since I am allowing dynamics in a system
>> that is already in
>> equilibrium. However, what I see is a huge fluctuation in the tmpp output
>> of cp.x, as I attach a figure
>> showing variation of tmpp (Ionic temperature) with simulation time
>> [IMAGE]
>>
>>
>> I did this because it is suggested in the user guide you should apply an
>> initial displacement to the
>> atoms in your system after the relaxation since otherwise there will not
>> be any dynamics. But what I
>> see here is a large fluctuation of the system temperature.
>>
>> The thinking or questions here are
>>
>> 1.Does the tmpp represents the physical temperature of the system here? I
>> think it should be since it
>> is the temperature corresponding to kinetic energy of the ions.
>>
>> 2.It above point is true, why is the temperature varying so fiercely? Am
>> I setting incorrect
>> parameters, for instance the timestep or the fictitious mass? But I took
>> those from previous simulation
>> steps where I did the relaxation, and they all worked well since they
>> successfully drived my system to
>> equilibrium, satisfying the convergence threshold on total energy, forces
>> acting on atoms, and the
>> fictitious electron kinetic energy. I am confused at this point.
>>
>> The input file for NVE simulation is attached here:
>>
>> &control
>> calculation='cp',
>> title='Halfnium disulfide'
>> restart_mode='restart',
>> ndr=53,
>> ndw=54,
>> nstep=50000,
>> iprint=10
>> isave=100,
>> tstress = .true.
>> tprnfor = .true.
>> dt=10,
>> wf_collect=.true.
>> etot_conv_thr=1e-6
>> forc_conv_thr=1e-3
>> ekin_conv_thr=1e-5
>> prefix='HfS2',
>> pseudo_dir='/home/jpeng/HfS2/potential'
>> outdir='./tmp/',
>> /
>> &system
>> ibrav= 4,
>> a=3.6529
>> c=5.6544
>> nat= 3, ntyp= 2,
>> ecutwfc =50
>> vdw_corr='DFT-D',
>> ! lspinorb=.true.
>> ! noncolin=.true.
>> ! ecutrho=300
>> ! nbnd=14
>> ! occupations='smearing'
>> ! smearing='gaussian'
>> ! degauss=0.01
>> ! nspin=2
>> ! starting_magnetization(1)=0.1
>> ! Hf 95.94 Hf.pbe-mt_fhi.UPF
>> ! S 32.065 S.pbe-mt_fhi.UPF
>> /
>> &electrons
>> electron_dynamics='verlet'
>> electron_velocities='zero'
>> emass=400
>> emass_cutoff=1
>> /
>> &ions
>> ion_dynamics = 'verlet'
>> ion_damping=0.1
>> ! ion_nstepe=10
>> /
>> &cell
>> cell_dynamics = 'none'
>>
>> /
>> ATOMIC_SPECIES
>> Hf 95.94 Hf.pbe-mt_fhi.UPF
>> S 32.065 S.pbe-mt_fhi.UPF
>> ATOMIC_POSITIONS (crystal)
>> Hf -0.000000000 -0.000000000 -0.000000000
>> S 0.666666667 0.333333333 0.257234636
>> S 0.333333333 0.666666667 -0.257234636
>>
>> Anyone could help me on it? Thank you very much.
>>
>> Best
>> Jie
>> --
>> ------------------------------------------------------------
>> ------------------------------------------
>> ------------------
>> Jie Peng
>> PhD student
>> 2134 Glenn Martin Hall, Mechanical Engineering, University of Maryland
>> College Park, Maryland, USA
>> Phone:(+1) 240-495-9445
>> Email: jiepeng at umd.edu
>>
>>
>>
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--
------------------------------------------------------------------------------------------------------------------------
Jie Peng
PhD student
2134 Glenn Martin Hall, Mechanical Engineering, University of Maryland
College Park, Maryland, USA
Phone:(+1) 240-495-9445
Email: jiepeng at umd.edu
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