by Rostam Golesorkhtabar & Pasquale Pavone for exciting carbon
Purpose: In this tutorial you will learn how to set up and execute exciting calculations using the ElaStic@exciting interface, which allows to obtain full elastic tensors (elastic constants) of crystal systems for any crystal structure. In addition, the application of ElaStic@exciting to the determination of the elastic constants of C in the diamond phase and of hexagonal Be is explicitly presented.
Table of Contents

0. Define relevant environment variables
Read the following paragraphs before starting with the rest of this tutorial!
Before starting, be sure that relevant environment variables are already defined as specified in How to set environment variables for tutorials scripts. Here is a list of the scripts which are relevant for this tutorial with a short description.
 ElaStic@excitingsetup.py: Python script for generating structures at different strains.
 ElaStic@excitingsubmit.sh: (Bash) shell script for running a series of exciting calculations.
 ElaStic@excitinganalyze.py: Python script for fitting the energyvsstrain and CVevsstrain curves.
 ElaStic@excitingclean.sh: (Bash) shell script for cleaning unnecessary files.
 ElaStic@excitingresult.py: Python script for calculating elastic constants.
 ElaStic_Result_Energy_2nd.py: Python script for calculating secondorder elastic constants.
 ElaStic_Result_Energy_3rd.py: Python script for calculating thirdorder elastic constants.
 ElaStic_xyz2XYZ.py: Python script for the conversion of secondorder elastic constants to different coordinate systems.
 exciting2sgroup.xsl: xsl script for converting the exciting input to an sgroup input file.
 Grace.par: File containing xmgrace parameters needed by visualization tools.
Requirements: Bash shell. Python numpy, lxml, math, sys and os libraries. xmgrace (visualization tool).
From now on the symbol $ will indicate the shell prompt.
Extra requirement: Tool for spacegroup determination
The scripts in this tutorial use the sgroup tool. If you have not done before, this tool should be downloaded and installed.
1. Set up the calculations
i) Preparation of the input file
The first step is to create a directory for each system that you want to investigate. In this tutorial, we first consider as an example carbon in the diamond structure (the procedure we use is, nevertheless, valid for any system). Thus, we will create a directory C_2nd and we move inside it.
$ mkdir C_2nd
$ cd C_2nd
Inside this directory, we create or copy an optimized structure file for diamond named C_2nd.xml. This file could look like the following.
<input> <title>Diamond: 2ndorder elastic constants</title> <structure speciespath="$EXCITINGROOT/species"> <crystal scale="6.7165"> <basevect> 0.5 0.5 0.0 </basevect> <basevect> 0.5 0.0 0.5 </basevect> <basevect> 0.0 0.5 0.5 </basevect> </crystal> <species speciesfile="C.xml" rmt="1.30"> <atom coord="0.00 0.00 0.00"/> <atom coord="0.25 0.25 0.25"/> </species> </structure> <groundstate xctype="GGA_PBE_SOL" ngridk="6 6 6" swidth="0.0001" gmaxvr="18"> </groundstate> <relax/> </input>
This file can be saved with any name. In this tutorial is not necessary to rename the exciting input file as input.xml, because this file is the input of ElaStic@exciting and not of exciting itself. Please, notice that the input file for a direct exciting calculation must be always called input.xml.
Be sure to set the correct path for the exciting root directory (indicated in this example by $EXCITINGROOT) to the one pointing to the place where the exciting directory is placed. In order to do this, use the command
$ SETUPexcitingroot.sh C_2nd.xml
ii) Generation of input files for distorted structures
All strains considered in this tutorial are Lagrangian strains.
In order to generate input files for a series of distorted structures, you have to run the script ElaStic@excitingsetup.py, which will produce the following output on the screen.
$ ElaStic@excitingsetup.py
2nd => 2
3rd => 3
>>>> Please choose the order of the elastic constant (choose '2' or '3'): 2
>>>> Please enter the exciting input file name: C_2nd.xml
Number and name of space group: 227 (F d 3 m) [origin choice 2]
Cubic I structure in the Laue classification.
This structure has 3 independent secondorder elastic constants.
>>>> Please enter the maximum Lagrangian strain
The suggested value is between 0.030 and 0.150: 0.05
The maximum Lagrangian strain is 0.05
>>>> Please enter the number of the distorted structures [odd number > 4]: 11
The number of the distorted structures is 11
$
Entry values must be typed on the screen when requested. In this case, the entries are the following.
 2, the order of the elastic constants in which you are interested.
 C_2nd.xml, the name of the input file.
 0.05, the absolute value of the maximum strain for which we want to perform the calculation.
 11, the number of deformed structures equally spaced in strain, which are generated between the maximum negative strain and the maximum positive one.
The script generates some new directories and files, which you can list using the following command (in the C_2nd directory).
$ ls
C_2nd.xml Distorted_Parameters Dst01 Dst02 Dst03 INFO_ElaStic Structures_exciting sgroup.out
$
You may also list the single directories, e.g., if you list Dst01 you will see the following (sub)directories.
$ ls Dst01
Dst01_01 Dst01_02 Dst01_03 Dst01_04 Dst01_05 Dst01_06 Dst01_07 Dst01_08 Dst01_09 Dst01_10 Dst01_11
$
3. Execute the calculations
To execute the series of calculations, run (in the C_2nd directory) the script ElaStic@excitingsubmit.sh, which will produce an output on the screen similar to the following.
$ ElaStic@excitingsubmit.sh
++
 SCF calculation of "Dst01_01" starts 
++
Elapsed time = 0m11s
Thu Jul 10 11:53:01 CEST 2014
++
 SCF calculation of "Dst01_02" starts 
++
Elapsed time = 0m11s
Thu Jul 10 11:53:12 CEST 2014
++
 SCF calculation of "Dst01_03" starts 
++
...
++
 SCF calculation of "Dst03_11" starts 
++
Elapsed time = 0m44s
Thu Jul 10 12:05:36 CEST 2014
$
After the complete run, elastic constants can be calculated.
The running time necessary for performing a complete calculation of the elastic constants of diamond using computational parameters as included in the above file C_2nd.xml, is less than one hour (depending on the machine processor you are using).
4. Analyzing the calculations
Elastic constants are obtained from energy calculations using a similar method to the one illustrated in Energy vs. strain calculations. Within this approach, second derivatives of the energy curves are evaluated with the help of a curve fitting. Calculations performed above were producing 11 points for each energy curve. The quality of the fitting procedure can be improved by increasing the number of data points per energy curve. The main results (INFO.OUT for all distortions) obtained for diamond using 41 data points per curve can be downloaded here.
Now, in order to calculate elastic constants, we have to analyze our calculations. The script ElaStic@excitinganalyze.py allows the analysis of the dependence of the calculated derivatives of the energyvsstrain curve on
 the range of distortions included in the fitting procedure (the x axis in xmgrace plots),
 the degree of the polynomial fit used in the fitting procedure (different color curves in xmgrace plots).
The ElaStic@excitinganalyze.py script is executed as follows.
$ ElaStic@excitinganalyze.py
At this point, six xmgrace plots will appear on your screen automatically (for more information on how to deal with xmgrace plots, see Xmgrace: A Quickstart). The plots obtained using 41 data points per energy curve should be similar to the ones displayed in the following.
 Results for the distortion Dst01
 Results for the distortion Dst02
 Results for the distortion Dst03
The previous plots can be used to determine the best range of deformations and order of polynomial fit for each distortion.
As an example, we analyze the first plot, corresponding to the distortion Dst01. Distortion types are listed in the file Distorted_Parameter. By examining this file, we can see that the Dst01 distortion corresponds to an applied Lagrangian strain in the Voigt notation with the form (η,η,η,0,0,0), where η is a strain parameter. This deformation type is directly connected with the bulk module B_{0}. For each distorsion type, two plots appear. The first plot contains the second derivative of the energy with respect to the strain parameter η as a function of the maximum strain and of the order of polynomial fit. In a similar way, the second plot shows the corresponding crossvalidation error. By analyzing the first plot for the Dst01 distortion, we notice that curves corresponding to the higher order of the polynomial used in the fit show a horizontal plateau at about 40604080 GPa. This can be assumed to be the converged value for the second derivative, from the point of view of the fit (further information on this topic can be found here). For this distortion type, this value equals 9 times the bulk modulus. Thus, the extracted value of the bulk modulus is 451453 GPa.
The script ElaStic@excitinganalyze.py generates the file ElaStic_2nd.in, which will be discussed and used in the next section.
5. Numerical values of the elastic constants
In order to obtain the numerical values of the secondorder elastic constants of diamond, you should use the following procedure. The first step is to edit the file ElaStic_2nd.in, which should have the form
Dst01 eta_max Fit_order
Dst02 eta_max Fit_order
Dst03 eta_max Fit_order
In each row of this file, you should insert a value for eta_max and Fit_order. According to the result of the visual analisys of the previous figures, these two values are extracted by considering the plateau regions of the corresponding plot: eta_max is a value of maximum distortion located in the plateau region of the curve representing the polynomial fit of order Fit_order. In our case, we can choose the parameters as listed in the example ElaStic_2nd.in below
Dst01 0.05 4
Dst02 0.05 4
Dst03 0.05 6
Now, in order to calculate elastic constants and moduli, you should run the ElaStic@excitingresult.py script.
$ ElaStic@excitingresult.py
Finally, numerical values of the elastic constants for diamond are written in the output file ElaStic_2nd.out.
Experimental reference elastic constants for diamond:
 C_{11} = 1076 GPa
 C_{12} = 125 GPa
 C_{44} = 577 GPa
 B_{0} = 452 GPa
Exercise
 Repeat all calculations using a denser kpoint grid and a larger number of strain points.
6. Set up the calculation for Be
In the next example, we consider the calculation of the elastic constants of hexagonal Be.
First, create a new directory Be_2nd and move inside it.
$ mkdir Be_2nd
$ cd Be_2nd
Inside this directory, create the file Be_2nd.xml corresponding to the optimized input file for the equilibrium structure of Be.
<input> <title>Be: 2ndorder elastic constants</title> <structure speciespath="$EXCITINGROOT/species"> <crystal scale="4.3207"> <basevect> 1.00000000 0.00000000 0.00000000 </basevect> <basevect> 0.50000000 0.86602540 0.00000000 </basevect> <basevect> 0.00000000 0.00000000 1.52257736 </basevect> </crystal> <species speciesfile="Be.xml" rmt="1.85"> <atom coord="0.66666667 0.33333333 0.75000000"/> <atom coord="0.33333333 0.66666667 0.25000000"/> </species> </structure> <groundstate xctype="GGA_PBE_SOL" ngridk="6 6 4" rgkmax="6.5"> </groundstate> <relax/> </input>
Do not forget to update the string "$EXCITINGROOT" inside the file Be_2nd.xml.
Then, we generate a set of exciting input files with the script ElaStic@excitingsetup.py.
$ ElaStic@excitingsetup.py
2nd => 2
3rd => 3
>>>> Please choose the order of the elastic constant (choose '2' or '3'): 2
>>>> Please enter the exciting input file name: Be_2nd.xml
Number and name of space group: 194 (P 63/m m c)
Hexagonal I structure in the Laue classification.
This structure has 5 independent secondorder elastic constants.
>>>> Please enter the maximum Lagrangian strain
The suggested value is between 0.030 and 0.150: 0.04
The maximum Lagrangian strain is 0.04
>>>> Please enter the number of the distorted structures [odd number > 4]: 41
The number of the distorted structures is 41
$
From now on, the procedure is completely equivalent to the one used for diamond. However, note that in this case the entry values are chosen in such a way to correspond to more accurate calculations. In turn, this means that the running time for completing the calculation of the elastic constants of hexagonal Be will be much longer than in the example of diamond. For a fast analysis, you can find here a tar.gz archive with the relevant output files (INFO.OUT for all distortions). The analysis of the result can be made as in the previous example.