[QE-users] bad convergence in field-effect configuration calculations
Bin Shao
bshaonku at outlook.com
Mon Sep 16 16:29:19 CEST 2019
Dear Thomas,
Thank you so much for your reply! I redo the calculation with a lower doping level and hide the gate in the barrier as you suggested. The calculation successfully gets converged. However, I have another question that if we relax the lattice constant of 2D materials, e.g. graphene, under the field-effect setup, i.e. the influence of gating on the lattice constant of 2D materials. Is this meaningful? If yes, can we do this by setting calculation = ‘relax-vc’ or by calculating the curve of energy vs. lattice constant?
Best,
Bin
________________________________
From: Dr. Thomas Brumme <thomas.brumme at uni-leipzig.de>
Sent: Monday, September 16, 2019 7:42:59 PM
To: Quantum ESPRESSO users Forum <users at lists.quantum-espresso.org>; bshaonku at outlook.com <bshaonku at outlook.com>
Subject: Re: [QE-users] bad convergence in field-effect configuration calculations
Dear Bin,
I can't check your input thoroughly as I'm on vacation, but there are
2 things I noticed:
1. The doping seems quite high - maybe you're close to the van Hove
singularity which could explain problems. Can you try with less doping
and then - if this converges - increase the doping till you get
problems? And plot the total potential - maybe the charge is already
spilling into the vacuum?! This is connected to the second problem:
2. It can help if you "hide" the gate in the barrier. A typical setup
I used recently:
zgate = 0.589,
emaxpos = 0.59,
eopreg = 0.01,
block = .true.,
block_1 = 0.50,
block_2 = 0.60,
block_height = 2.50,
and the system is below 0.5... E.g. for your case, try
zgate = 0.1311111
block = .true.
block_1 = 0.13
block_2 = 0.23
block_height = 2.5
edir = 3
emaxpos = 0.13
eopreg = 0.01
The barrier starts with the dipole correction and the gate is right
behind the dipole... Compare with Fig. 2 of the PRB (2014). Also note
that 2.5 Ry for the barrier height is an arbitrarily chosen value - I
noticed other people now also use 2.5 Ry even if 2 Ry or even 1.5 Ry
should be enough. Yet, the higher the doping, the higher the dipole
correction the higher the barrier (if you "hide" everything in the
barrier)...
Regards & Greeting from the lake Garda in Italy
Thomas
Zitat von Bin Shao <bshaonku at outlook.com>:
> Dear all,
>
> I would like to learn how to set up calculations of field-effect
> configuration in quantum espresso. I read the paper "T. Brumme, M.
> Calandra, F. Mauri; PRB 89, 245406 (2014)." and started with
> graphene as an example. The input file is as follows. During the scf
> calculation, there are a lot of warnings like " c_bands: 1
> eigenvalues not converged". And the calculation could not get
> converged after 800 iterations, could anyone help me with the input
> file? Thanks in advance!
>
> Best regards,
> Bin
>
> ========================================================================
> &CONTROL
> calculation = 'scf'
> etot_conv_thr = 2.0000000000d-05
> forc_conv_thr = 1.0000000000d-04
> outdir = './out/'
> prefix = 'aiida'
> pseudo_dir = './pseudo/'
> tprnfor = .true.
> tstress = .true.
> gate = .true.
> dipfield = .true.
> tefield = .true.
> verbosity = 'high'
> /
> &SYSTEM
> degauss = 0.02
> ecutrho = 500
> ecutwfc = 45
> ibrav = 0
> nat = 2
> ntyp = 1
> occupations = 'smearing'
> smearing = 'cold'
> tot_charge = -0.2
> zgate = 0.1
> block = .true.
> block_1 = 0.13
> block_2 = 0.23
> block_height = 2.5
> edir = 3
> emaxpos = 0.005
> eopreg = 0.01
> /
> &ELECTRONS
> conv_thr = 1.0000000000d-9
> electron_maxstep = 800
> mixing_beta = 0.4
> mixing_mode = 'local-TF'
> /
> ATOMIC_SPECIES
> C 12.011 C.pbe-n-kjpaw_psl.1.0.0.UPF
> ATOMIC_POSITIONS crystal
> C 0.0000000000 0.0000000000 0.3500000000
> C 0.3333333000 0.6666667000 0.3500000000
> K_POINTS automatic
> 65 65 1 0 0 0
> CELL_PARAMETERS angstrom
> 2.4638000000 0.0000000000 0.0000000000
> -1.2319000000 2.1336508000 0.0000000000
> 0.0000000000 0.0000000000 35.0000000000
> ======================================================================================
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