This lesson aims at showing how to get the following physical properties, for an insulator :
The case of the linear responses (Born effective charge, dielectric constant, piezoelectric tensor) is treated independently in other tutorials (lesson Response-Function 1, lesson on Elastic properties), using Density-Functional Perturbation Theory. You will learn here how to get these quantities using the finite difference techniques within ABINIT. To that end, we will describe how to compute the polarization, in the Berry phase formulation, and how to perform finite electric field calculations.
This lesson should take about 1 hour and 30 minutes.
The basic theory for Berry phase computation of the polarization was proposed by R.D. King-Smith and D. Vanderbilt, Phys. Rev. B 47, 1651 (1993). The longer (excellent) paper D. Vanderbilt and R.D. King-Smith, Phys. Rev. B 48, 4442 (1993) clarifies many aspects of this theory (especially in view of application to AlAs, as in this tutorial). One might benefit also from a reading of R. Resta, Rev. Mod. Physics 66, 899 (1994).
In order to gain the theoretical background needed to perform a calculation with a finite electric field, you should consider reading the following papers:
Finally, the extension to the PAW formalism specifically in ABINIT is discussed in Gonze et al., Comp. Phys. Commun. 180, 2582 (2009) and Zwanziger et al., Comp. Mater. Sci. 58, 113 (2012).
Before beginning, you might consider working in a different subdirectory, as for the other lessons. Why not create "Work-ffield" in ~abinit/tests/tutorespfn/Input ?
In this tutorial we will assume that the ground-state properties of AlAs have been previously obtained, and that the corresponding convergence studies have been done. We will adopt the following set of generic parameters :
acell 10.53 ixc 3 ecut 2.8 (results with ecut = 5 are also reported in the discussion) ecutsm 0.5 dilatmx 1.05 nband 4 (=number of occupied bands) ngkpt 6 6 6 nshiftk 4 shiftk 0.5 0.5 0.5 0.5 0.0 0.0 0.0 0.5 0.0 0.0 0.0 0.5 pseudopotentials 13al.pspnc 33as.pspnc
In principle, the acell to be used should be the one corresponding to the optimized structure at the ecut, and ngkpt combined with nshiftk and shiftk, chosen for the calculations. Unfortunately, for the purpose of this tutorial, in order to limit the duration of the runs, we have to work at an unusually low cutoff of 2.8 Ha for which the optimized lattice constant is equal to 7.45*0.707*2 Bohr=10.53 Bohr (instead of the converged value of 10.64 Bohr). For comparison, results with ecut=5 are also reported and, in that case, were obtained at the optimized lattice constant of 10.64 bohr. For those who would like to try later, convergence tests and structural optimizations can be done using the file ~abinit/tests/tutorespfn/Input/tnlo_1.in. Before going further, you might refresh your memory concerning the other variables : ixc, ecutsm, dilatmx.
In this section, you will learn how to perform a Berry phase calculation of the polarization. As a practical problem we will try to compute the Born effective charges from finite difference of the polarization (under finite atomic displacements), for AlAs.
You can now copy the file ~abinit/tests/tutorespfn/Input/tffield_1.in and ~abinit/tests/tutorespfn/Input/tffield_x.files in Work-ffield, and modify the latter as usual. You can start the calculation. It should take 90 seconds on a PC 3GHz. Then, examine the tffield_1.in file. It is made of three datasets corresponding to the reference optimized structure (tau=0) and to structure with the Al atom displaced from 0.01 bohr right and left (referred to as tau = +0.01 and tau = -0.01). This is typically the amplitude of atomic displacement to be considered in this kind of computations.
There are two implementations of the Berry phase within ABINIT. One corresponds to positive values of berryopt and was implemented by Na Sai. The other one corresponds to negative values of berryopt was implemented by Marek Veithen. Both are suitable to compute the polarization. Here we will focus on the implementation of Marek Veithen for two reasons. First, the results are directly provided in cartesian coordinate at the end of the run (while the implementation of Na Sai reports them in reduced coordinates). Second the implementation of Marek Veithen is the one to be used for the finite electric field calculation as described in the next Section. Finally, note also that Veithen's implementation works with kptopt = 1 or 2 while Na Sai implementation is restricted to kptopt = 2, which is less convenient.
The file is the one of a usual self-consistent calculation. On top of usual variables, for the Berry phase calculation we simply need to define berryopt and rfdir:
berryopt -1 rfdir 1 1 1
Make the run, then open the output file and look for the occurrence "Berry". The output reports values of the Berry phase for individual k-point strings.
Computing the polarization (Berry phase) for reciprocal vector: 0.16667 0.00000 0.00000 (in reduced coordinates) -0.01583 0.01583 0.01583 (in cartesian coordinates - atomic units) Number of strings: 144 Number of k points in string: 6 Summary of the results Electronic Berry phase 2.025853583E-03 Ionic phase -7.500000000E-01 Total phase -7.479741464E-01 Remapping in [-1,1] -7.479741464E-01 Polarization -1.557862805E-02 (a.u. of charge)/bohr^2 Polarization -8.913274881E-01 C/m^2
tau = 0
Polarization in cartesian coordinates (a.u.): (the sum of the electronic and ionic Berry phase has been folded into [-1, 1]) Electronic berry phase: 0.730821479E-04 0.730821479E-04 0.730821479E-04 Ionic: -0.270560574E-01 -0.270560574E-01 -0.270560574E-01 Total: -0.269829753E-01 -0.269829753E-01 -0.269829753E-01 Polarization in cartesian coordinates (C/m^2): (the sum of the electronic and ionic Berry phase has been folded into [-1, 1]) Electronic berry phase: 0.418137766E-02 0.418137766E-02 0.418137766E-02 Ionic: -0.154800587E+01 -0.154800587E+01 -0.154800587E+01 Total: -0.154382450E+01 -0.154382450E+01 -0.154382450E+01
tau = +0.01
Polarization in cartesian coordinates (a.u.): (the sum of the electronic and ionic Berry phase has been folded into [-1, 1]) Electronic berry phase: 0.410028779E-04 0.730922946E-04 0.730922946E-04 Ionic: -0.269532804E-01 -0.270560574E-01 -0.270560574E-01 Total: -0.269122775E-01 -0.269829652E-01 -0.269829652E-01 Polarization in cartesian coordinates (C/m^2): (the sum of the electronic and ionic Berry phase has been folded into [-1, 1]) Electronic berry phase: 0.234596988E-02 0.418195820E-02 0.418195820E-02 Ionic: -0.154212551E+01 -0.154800587E+01 -0.154800587E+01 Total: -0.153977954E+01 -0.154382392E+01 -0.154382392E+01
tau = -0.01
Polarization in cartesian coordinates (a.u.): (the sum of the electronic and ionic Berry phase has been folded into [-1, 1]) Electronic berry phase: 0.105181709E-03 0.730922946E-04 0.730922946E-04 Ionic: -0.271588345E-01 -0.270560574E-01 -0.270560574E-01 Total: -0.270536528E-01 -0.269829652E-01 -0.269829652E-01 Polarization in cartesian coordinates (C/m^2): (the sum of the electronic and ionic Berry phase has been folded into [-1, 1]) Electronic berry phase: 0.601794637E-02 0.418195820E-02 0.418195820E-02 Ionic: -0.155388624E+01 -0.154800587E+01 -0.154800587E+01 Total: -0.154786829E+01 -0.154382392E+01 -0.154382392E+01
From the previous data, we can extract the Born effective charge of Al. Values to be used are those in a.u., in order to find the charge in electron unit. It corresponds to (the volume of the primitive unit cell must be specified in Bohr too) :
Z* = \Omega_0 (P[tau=+0.01] - P[tau=-0.01]) / (2*tau) = 291.89 (-0.269122775E-01 - -0.270536528E-01) / 0.02 = 2.06
You can review how to use DFPT thanks to the lesson Response-function 1 and lesson Response-function 2 tutorials. For now, go ahead and run the input file, and have a look at the output file, to identify the place where the Born effective charge is written (search for the phrase "Effective charges" in the output file). The value we get from DFPT is 2.06, in agreement with the above-mentioned value of 2.06. This level of agreement is fortuitous for unconverged calculations, though both methods (finite-difference and DFPT) will tend to the same value for better converged calculations.
The DDB generated by ~abinit/tests/tutorespfn/Input/tffield_2.in can be fed in anaddb, thanks to the ~abinit/tests/tutorespfn/Input/tffield_3.in input file and the tffield_3.files file. The latter gives the DFPT value for the piezoelectric constants (as well as the elastic constants).
Proper piezoelectric constants (clamped ion) (unit:c/m^2) ... -0.64879283 0.00000000 0.00000000 ... Proper piezoelectric constants (relaxed ion) (unit:c/m^2) ... 0.04574987 0.00000000 0.00000000Restarting case ffield_2 and ffield_3 with ecut=5 (three minutes on a PC 3 GHz), one gets the following values
Proper piezoelectric constants (clamped ion) (unit:c/m^2) ... -0.68377667 0.00000000 0.00000000 ... Proper piezoelectric constants (relaxed ion) (unit:c/m^2) ... 0.03384772 0.00000000 0.00000000The latter value, where the ionic relaxation largely suppresses the electronic piezoelectricity, will be much more difficult to converge than the clamped ion result.
Using the Berry phase approach it is also possible to compute the piezoelectric constant from finite difference of polarization with respect to strains. This can be done considering clamped ions or relaxed ions configurations. For this purpose, have a look to the files ~abinit/tests/tutorespfn/Input/tffield_4.in (clamped ions) and ~abinit/tests/tutorespfn/Input/tffield_5.in (relaxed ions). They should give the following final results (obtained by taking finite difference expressions of the strains for different electric fields)
Proper piezoelectric constants(clamped ion)(Unit:c/m^2) = -0.6491 Proper piezoelectric constants(relaxed ion)(Unit:c/m^2) = 0.0430For example, the clamped ion piezoelectric constant was obtained from tffield_4.out :
Polarization in cartesian coordinates (C/m^2): (the sum of the electronic and ionic Berry phase has been folded into [-1, 1]) Electronic berry phase: -0.230212263E-02 0.421671951E-02 0.421671986E-02 Ionic: -0.154692152E+01 -0.155466099E+01 -0.155466099E+01 Total: -0.154922364E+01 -0.155044427E+01 -0.155044427E+01and
Polarization in cartesian coordinates (C/m^2): (the sum of the electronic and ionic Berry phase has been folded into [-1, 1]) Electronic berry phase: 0.106812992E-01 0.417465885E-02 0.417465885E-02 Ionic: -0.154692152E+01 -0.153919172E+01 -0.153919172E+01 Total: -0.153624022E+01 -0.153501707E+01 -0.153501707E+01The difference between -0.154922364E+01 (x-strain is +0.01) and -0.153624022E+01 (x-strain is -0.01) gives the finite difference -0.012983, that, divided by 0.02 (the change of strain) gives -0.6491, announced above.
Proper piezoelectric constants(clamped ion)(Unit:c/m^2) = -0.6909505 Proper piezoelectric constants(relaxed ion)(Unit:c/m^2) = 0.0326305in excellent agreement with the above-mentioned DFPT values.
You can now copy the file ~abinit/tests/tutorespfn/Input/tffield_6.in in Work-ffield, and modify the tffield_x.files accordingly. You can start the run immediately, it will take one minute on a PC 3GHz. It performs a finite field calculation at clamped atomic positions. You can look at this input file to identify the features specific to the finite field calculation.
As general parameters, one has to specify nband, nbdbuf and kptopt:
nband 4 nbdbuf 0 kptopt 1
As a first step (dataset 11), the code must perform a Berry phase calculation in zero field. For that purpose, it is necessary to set the values of berryopt and rfdir:
berryopt11 -1 rfdir11 1 1 1
Important warning: you cannot use berryopt to +1 to initiate a finite field calculation. You must begin with berryopt -1.
After that, there are different steps corresponding to various value of the electric field, thanks to efield. For those steps, it is important to take care of the following parameters here reported for dataset 21:
berryopt21 4 efield21 0.0001 0.0001 0.0001 getwfk21 11
The electric field is here applied along the  direction. It must be incremented step by step (it is not possible to go to high field directly). At each step, the wavefunctions of the previous step must be used. When the field gets larger, it is important to check that it does not significantly exceeds the critical field for Zener breakthrough (the drop of potential over the Born-von Karmann supercell must be smaller than the gap). In practice, the number of k-point must be enlarged to reach the convergence. However, at the same time, the critical field becomes smaller. In practice, reasonable fields can still be reached for k-point grids providing a reasonable degree of convergence. A compromise must however be found.
As these calculations are quite long, the input file has been limited to very small fields. Three cases have been selected : E = 0, E = +0.0001 and E = -0.0001. If you have time later, you can relax this constraint and perform a more exhaustive calculations for a larger set of fields.
You can now start the run. Various quantities can be extracted from the finite field calculation at clamped ions using finite difference techniques: the Z* can be extracted from the forces, the optical dielectric constant can be deduced from the polarization, the clamped ion piezoelectric tensor can be deduced from the stress tensor. As an illustration we will focus here on the computation of Z*.
You can look at your output file. For each field, the file contains various quantities that can be collected. For the present purpose, we can look at the evolution of the forces with the field and extract the following results from the output file :
cartesian forces (hartree/bohr) at end: 1 0.00000000000000 0.00000000000000 0.00000000000000 2 0.00000000000000 0.00000000000000 0.00000000000000
E = +0.0001
cartesian forces (hartree/bohr) at end: 1 0.00020614538503 0.00020614538503 0.00020614538503 2 -0.00020614538503 -0.00020614538503 -0.00020614538503
E = -0.0001
cartesian forces (hartree/bohr) at end: 1 -0.00020650900243 -0.00020650900243 -0.00020650900243 2 0.00020650900243 0.00020650900243 0.00020650900243
In a finite electric field, the force on atom A in direction i can be written as :
F_Ai = Z*_A,ii * E + \Omega_0 dchi/dtau E^2
The value for positive and negative fields above are nearly the same, showing that the quadratic term is almost negligible. This clearly appears in the figure below where the field dependence of the force for a larger range of electric fields is plotted.
We can therefore extract with a good accuracy the Born effective charge as :
Z*_Al = (F_Al[E=+0.0001] - F_Al[E=-0.0001])/(2*0.0001) = (0.00020614538503 + 0.00020650900243)/0.0002 = 2.06
This value is similar to the value reported from DFPT. If you do calculations for more electric fields, fitting them with the general expression of the force above (including the E^2 term), you can find the dchi/dtau term. At ecut=5 you should get dchi/dtau for Al = -0.06169. This will be useful later for the lesson on static Non-linear properties.
Going back to the output file, you can also look at the evolution of the polarization with the field.
Polarization in cartesian coordinates (a.u.): (the sum of the electronic and ionic Berry phase has been folded into [-1, 1]) Electronic: 0.730821479E-04 0.730821479E-04 0.730821479E-04 Ionic: -0.270560574E-01 -0.270560574E-01 -0.270560574E-01 Total: -0.269829753E-01 -0.269829753E-01 -0.269829753E-01
E = +0.0001
Polarization in cartesian coordinates (a.u.): (the sum of the electronic and ionic Berry phase has been folded into [-1, 1]) Electronic: 0.129869542E-03 0.129869542E-03 0.129869542E-03 Ionic: -0.270560574E-01 -0.270560574E-01 -0.270560574E-01 Total: -0.269261879E-01 -0.269261879E-01 -0.269261879E-01
E = -0.0001
Polarization in cartesian coordinates (a.u.): (the sum of the electronic and ionic Berry phase has been folded into [-1, 1]) Electronic: 0.163575373E-04 0.163575372E-04 0.163575371E-04 Ionic: -0.270560574E-01 -0.270560574E-01 -0.270560574E-01 Total: -0.270396999E-01 -0.270396999E-01 -0.270396999E-01
In a finite electric field, the polarization in terms of the linear and quadratic susceptibilities as
P = \chi * E + \chi(2) E^2
The change of polarization for positive and negative fields above are nearly the same, showing again that the quadratic term is almost negligible. This clearly appears in the figure below where the field dependence of the polarization for a larger range of electric fields is plotted.
We can therefore extract with a good accuracy the linear optical dielectric susceptibility :
\chi(l)_11 = (P[E=+0.0001] - P[E=-0.0001])/(2*0.0001) = (-0.269261879E-01+ 0.270396999E-01)/0.0002 = 0.56756
The optical dielectric constant is :
\epsilon_11 = 1+ 4 \pi \chi(1)_11 = 8.13
This value underestimates the value of 9.20 obtained by DFPT. The agreement is not better at ecut=5. Typically, finite field calculations converge with the density of the k point grid more slowly than DFPT calcuations.
If you do calculations for more electric fields, fitting them with the general expression of the force above (including the E^2 term) you can find the non-linear optical susceptibilities \chi(2). At ecut=5 you should get \chi(2) = 29.769 pm/V. This result will be also be useful for the lesson on static Non-linear properties.
Looking at the evolution of the stress (see graphic below), you should also be able to extract the piezoelectric constants. You can try to do it as an exercise. As the calculation here was at clamped ions, you will get the clamped ion proper piezoelectric constants. At ecut=5, you should obtain -0.69088 C/m^2.
Redoing the same kind of finite field calculation when allowing to the ions to relax , one can access the relaxed ion proper piezoelectric constant. At ecut=5 the result is -0.03259.