A Package for calculating elastic tensors of cubic Phases by using second-order derivative with WIEN2k Package
|
|
- Dorothy Young
- 5 years ago
- Views:
Transcription
1 IR E L A S T + W I E N 2k A Package for calculating elastic tensors of cubic Phases by using second-order derivative with WIEN2k Package User s guide, Cubic-elastic_13.2 (Release ) Morteza Jamal Ghods City-Tehran-Iran
2 MANDATORY CONDITIONS: In any publication in the scientific literature please reference the program as follows: M. Jamal, Cubic-elastic, (2012). ACKNOWLEDGMENT I gratefully appreciate B.Z. Yanchitsky for fruitful discussions, P. Blaha and S. Jalali Asadabadi for suggestions, and Carol Phillips for editing. For suggestions or bug reports please contact the author by m_jamal57@yahoo.com
3 1- Introduction Cubic-elastic is a Package for finding elastic constants of cubic symmetries with WIEN2k. This Package calculates elastic constants by second-order derivative ( E ( δ) ) of Polynomial fit ( E=E(δ) ) of Energy vs. strains ( δ) at zero strain (δ =0). This called energy approach [1]. 2- Cubic-elastic and Thomas Charpin Packages I think there will be a question for users of this Package. What is difference between Cubic-elastic and Thomas Charpin [2] Package? Since for cubic symmetry, the bulk modulus given by: So in Thomas Charpin Package, it calculates (C 11 +2C 12 ) by using Equation Of State (EOS) and as a result bulk modulus. Also it calculates (C 44 ) by a rhombohedral strain which results: While Cubic-elastic calculates (C 11 +2C 12 ) and (C 44 ) without any detours. For more information see background theory section. So, a new source of error may come from bulk modulus calculation in Thomas Charpin Package. 3- Background theory (energy approach) Elastic constants are defined by means of a Taylor expansion of the total energy for the system, with respect to a small strain ( ) of the lattice. If we consider the bravais lattice vectors of a cubic crystal structure as a matrix form the distortion of the lattice ( ) is expressed by multiplying with a symmetric ( ) distortion matrix i.e. ( ), which is written as,
4 And in Voigt notation ( It is often convenient to change to the Voigt notation to reduce the number of indices. The Voigt notation replaces 1, 2, 3, (and ) 4, (and ) 5, (and ) 6 ) We express the energy of the strained system by means of a Taylor expansion in the distortion parameters, The linear terms vanish if the strain causes no changes in the volume of the crystal. Otherwise, are related to the strain on the crystal and are elastic constants and is the volume of unstrained cubic system and we use it to evaluate the elastic constants. To obtain elastic constants of cubic structure I have used the strain method (energy approach). In this method elastic constants were calculated by applying small strains to the unstrained lattice. There are three independent elastic constants for a cubic symmetry, called C 11, C 12, and C 44. Since we have three independent elastic constants, we need three different strains to determine these elastic constants. The three distortions used
5 in the Cubic-elastic Package are described below. These three distortions are written as [3-5] and D 1 is volume-conserving orthorhombic distortion and D 2 changes the lattice parameter in the a-lattice direction. The symmetry of the strained lattice is therefore still cubic, however the volume of the distortion lattice changes by using D 2. D 3 is volume-conserving monoclinic distortion and the energy for these distortions can be obtained as And Respectively,
6 4- File structure and program flow The following table describes input and output files for each program of the Cubic-elastic Package. Program needs generates C_set_elast_lapw case.struct init.struct runcommand1 runcommand2 pwdname command_init_lapw C_command_run_lapw C_setup11m12 C_setupc1112 C_setupc44 getcalljobc makestructc init.struct pwdname runcommand1 runcommand2 init.struct.styp CUBIC.job auto_init_lapw runcommand1 runcommand2.vper.styp CUBIC.job number.strain StypX_Y.struct vol.optimize C_modifyjob_lapw C_calljob_lapw CUBIC.job VstVene C_fitdivELC number.strain ELCorder.fit vol.optimize ELC.output.styp ELC.fit VstVene C_ana_elastc_lapw VstVene case.outputeos ELC.fit vol.optimize ELC.ps C_ana_elast_lapw ELC.output ELC-matrix case.output_elastic C_InverseELC ELC-matrix INVELC-matrix MassRho init.struct.rho vol.optimize C_ana_elastorder_lapw ELCorder.fit output-order sgroupcheck_lapw StypX_Y.struct case.struct command_intso_lapw.infso command_initu_lapw.infldau auto_initso_lapw.infso case.inso auto_initu_lapw.infldau case.inorb case.indm/c Bold font is OPTIONAL Italic bold font means it is the user s choice
7 4-2- Short description for input and output files case.struct init.struct pwdname runcommand1/2 Is a WIEN2k standard struct file. Is a copy of the case.struct file. Contains the name of present work directory. Contains the run commands for running. It looks similar to: run_lapw ec p in1new 2 auto_init_lapw A C-shell program which automatically runs the initialization. It looks similar to:.vper.styp CUBIC.job #!/bin/csh -f set RM = not if ( $RM == 'not' ) then init_lapw -vxc 13 -ecut -6 -mix 0.2 -numk b else init_lapw -red 0 -vxc 13 -ecut -6 -mix 0.2 -numk b endif Defines the percent of changes for different strains. Defines the type of strain. A C-shell program which calculates the energy for each strain by using the WIEN2k Package. It looks similar to: #!/bin/csh -f #STRAIN TYPE IS 1 #Modify this script according to your needs unalias rm set co = 1 set name set bj set file = `pwd` set file = $file:t if (-e VstVene ) then set i=`/bin/ls VstVene* wc ` echo " saving pervious VstVene to VstVene_$i[1]" cp VstVene VstVene_$i[1] rm VstVene endif # # to reuse previous scf runs (without a new scf run) set answscf=y # and use the same "savename". # When you make modifications (RKmax, k-mesh, XC-potentials) choose # answscf=no and a new savename (eg. "_pbe_rk8_1000k"). set answscf=y
8 set savename= if (-e cscl.clmsum && \! -z cscl.clmsum) then x dstart -super endif if (-e cscl.clmup && \! -z cscl.clmup ) then x dstart -super -up x dstart -super -dn endif foreach i ( \ ) echo "*******************************" echo $i set name=`echo "$name $i"` echo "*******************************" Styp1_-3.0 \ Styp1_-2.0 \ Styp1_-1.0 \ Styp1 0.0 \ Styp1 1.0 \ Styp1 2.0 \ Styp1 3.0 \ StypX_Y.struct VstVene number.strain case.outputeos A WIEN2k struct file for each value of changes and for each strain type where X and Y denote type of strain and value of changes, respectively. The main information file, contains values of changes (strains) and energies for each type of strain, for the calculation of the elastic constant. Contains the number of strains. A WIEN2k output of equation of states(eos). For finding the best values of elastic constants, find EOS and then copy the case.outputeos in the "case" directory Within the c11+2c12, c11-c12 and c44 directories. Otherwise, it sets the optimized volume from the original struct file i.e. case.struct vol.optimize Contains the optimize volume. ELCorder.fit Contains the elastic constants for different values of order of fit. ELC.output Contains the elastic constants for order of fit =2 ELC.fit Contains the data to plot curve of energy vs value of changes (strains) for each strain type. ELC-matrix Defines the elastic constant matrix for each symmetry. case.output_elastic Contains the final elastic constant values. INVELC-matrix Defines the inverse of elastic constant matrix.
9 .rho.infso.infldau Contains density of mass and atomic volume. Contains information for making case.inso file for running spin-orbit coupling. Contains information for making case.inorb and case.indm/c files for LDA+U calculations Flow and short description for programs The Cubic-elastic Package consists of several FORTRAN and SHELL SCRIPTS which are described below. A flowchart of the program is shown in the following diagram. C_set_elast_lapw : Makes an elast-constant directory in present work directory ( PWD ) and c11+2c12, c11-c12 and c44 directories in the elast-constant directory. The C_set_elast_lapw program also copies information of "PWD" into the c11+2c12, c11-c12 and c44 directories and calls "command_init_lapw", C_command_run_lapw, C_setupc1112, C_setupc11m12 and C_setupc44 programs. command_init_lapw : Gets informations for making "auto_init_lapw". C_command_run_lapw : Gets the run commands for making CUBIC.job. C_setupcX (X=1112, 11m12, 44) : Gets the type of strain and calls the getcalljobc program. getcalljobc : Calls makestructc program and makes the CUBIC.job file. makestructc : Makes StypX_Y.struct files where X and Y stand for type of strain and value of changes, respectively and the vol.optimize file. C_modifyjob_lapw : Edits the job files according to the user s needs. C_calljob_lapw : Calls the CUBIC.job files for running. C_ana_elast_lapw : Calls the C_ana_elastc_lapw program for calculation elastic constants then calculates
10 the Voigt, Reuss, and Hill bulk, shear, and Young modulus as well as the Poisson ratio. After that it calls the C_InverseELC and MassRho programs and calculates sound velocity and Debye temperature then makes two output files in the elastconstant directory with the name case.output_elastic and the INVELC-matrix which is elastic compliance constants generated by inverting the elastic constant matrix. At the end it calls C_ana_elastorder_lapw program. C_ana_elastc_lapw : Calls the C_fitdivELC program with appropriate libraries for calculating C11-C12, C11+2C12, and C44. C_InverseELC : Makes the Elastic compliance constants generated by inverting the elastic constant matrix. MassRho : Finds density of mass and atomic volume. C_ana_elastorder_lapw : Checks the sensitivity of the elastic constants to the order of fit. sgroupcheck_lapw : Finds the best value of tol in sgroup [6] program and copies case.struct_sgroup as case.struct.
11 C_set_elast_lapw command_init_lapw generates auto_init_lapw C_command_run_lapw generates commandrun1/2 C_setupcX X=1112, 11m12, 44 getcalljobc generates CUBIC.job makestructc generates StypX_Y.struct sgroupcheck_lapw CUBIC.job generates VstVene auto_init_lapw C_ana_elastorder_lapw generates ELCorder.fit C_ana_elast_lapw C_ana_elastc_lapw C_InverseELC MassRho ELASTIC CONSTANTS IS READY generates case.output_elastic and INVELC-matrix C_fitdivELC calls Libraries generates C 11 -C 12, C 11 +2C 12, C 44 Program flow in Cubic-elastic Dash arrow means user must run
12 5 Elastic constants calculation 1. Create a struct file and validate it by running "sgroupcheck_lapw". 2. If Spin-Orbit calculations are required run "command_initso_lapw. 3. If LDA+U calculations are required run "command_initu_lapw" and then "auto_initu_lapw". 4. Run "C_set_elast_lapw". 5. Now you must adapt the job files according to your needs (you can run "C_modifyjob_lapw" in Terminal ). It is not necessary to do step 5 if you define the COMMAND RUN commands in step Now you must run the job files ( you can run "C_calljob_lapw" in Terminal ). It will take time. 7. Run "C_ana_elast_lapw". This package calculates elastic constants by second-order derivative ( E (δ) ) of Polynomial fit ( E=E(δ) ) of Energy vs. strains (є) at zero strain ( δ =0) so, you must use values of strain around zero and from the viewpoint of fit convergence, we usually expect to see a minimum when we plot Energy vs. strain ( this Package plots it ). It is recommended that the sensitivity of the results is checked to the order of fit. This program shows them. 5-1 Notes about elastic constants calculation After using distortions for calculation C11-C12 and C44 the symmetry of the cubic compound changes and usually the number of atoms change. So when you run "command_initso_lapw" or "command_initu_lapw", in the section name of an atom, type "all <name of atom>" ( for example: all Mn). With this command, you use SO or LDA+U calculations for example for all Mn atoms. When you want to rerun job files with modifications in (RKmax, k-mesh, XC-potentials ) call command_init_lapw and after that choose "answscf=no" in the CUBIC.job files and a new "savename" (eg. "_use_pbe_rk8"). Optionally you can specify more cases by rerunning C_setupcX (X=1112, 11m12, 44 see section 5-3 ). Specify also your old cases. The old results will then be taken
13 automatically into account without recalculation ( unless you modify job files i.e: set answscf=no ). For the calculation of the best values of elastic constants, please find EOS and then copy case.outputeos in "case" directory within c11+2c12, c11-c12 and c44 directories. Otherwise, it sets the optimized volume from the original struct file i.e. case.struct. 5-2 One calculation To calculate C 11 +2C 12 or C 44 the following steps should be performed for example for calculation of C 44 : 1. Make a directory for example c Make a "case" directory in c44 directory. 3. Make a "case.struct" file in "case" directory and name it "init.struct". Creat "pwdname" file and write in it "case." and save it. 4. Run the command_init_lapw 5. chmod +x auto_init_lapw 6. For SO calculations, run the command_initso_lapw. 7. For LDA+U calculations, run the command_initu_lapw and auto_initu_lapw To avoid step 10, you can run C_command_run_lapw for setting the COMMAND RUN commands for making CUBIC.job. 8. Run the C_setupc44 program. 9. chmod +x CUBIC.job file. 10. Modify the CUBIC.job file. 11. Call CUBIC.job 12. Call C_ana_elastc_lapw 5-3 Run with more data points Optionally you can specify more data points, for calculation of the elastic constants, by rerunning C_setupcX (X=1112, 11m12, 44 ). Specify also your old data points. The old results will then be taken automatically into account without recalculation ( unless you modify job files i.e: set answscf=no ). Please do the following steps for this goal for example for c cd to the elast-constant directory. 2. cd to the c44 directory. 3. cd to the case directory. 3-1) To avoid step 6, you can run C_command_run_lapw for setting the COMMAND RUN commands for making the CUBIC.job. 4. Run C_setupc44 program. 5. If you want to rerun job files with modifications in (RKmax, k-mesh, XC-
14 potentials ) call command_init_lapw and then choose "answscf=no" in CUBIC.job files and a new "savename" (eg. "_use_pbe_rk8"). 6. Modify the CUBIC.job file. 7. Call CUBIC.job 8. Call C_ana_elastc_lapw 5-4 Elastic constants calculation for CsCl CsCl compound is a test case for elastic constants calculation. The CsCl structure is described in detail in the following: CsCl P LATTICE,NONEQUIV.ATOMS: 2 MODE OF CALC=RELA unit=bohr ATOM 1: X= Y= Z= MULT= 1 ISPLIT= 0 Cs NPT= 781 R0= RMT= Z: 55.0 LOCAL ROT MATRIX: ATOM 2: X= Y= Z= MULT= 1 ISPLIT= 0 Cl NPT= 781 R0= RMT= Z: 17.0 I selected the following parameters for calculation: Xc = PBE-sol, R_Kmax = 9, L_max = 10 and nkpoint = 4000 After calculation, we have : ================================================================================ Atom name = Cs Atomic Mass from Periodic table = (gr/mol) Atomic Mass from Periodic table = *10^(-23) (gr) Atom name = Cl Atomic Mass from Periodic table = (gr/mol) Atomic Mass from Periodic table = *10^(-23) (gr) Volume in unit of cm^3 = *10^(-24) (cm^3) Mass of Compound : *10^(-23) (gr) Density of Compound : (gr/cm^3) ================================================================================ C11 = GPa C12 = GPa C44 = GPa ================================================================================
15 Prediction VOIGT Bulk modulus by using elastic constant values Prediction REUSS Bulk modulus by using elastic constant values Prediction HILL Bulk modulus by using elastic constant values = (GPa) = (GPa) = (GPa) Prediction VOIGT Shear modulus by using elastic constant values = (GPa) Prediction REUSS Shear modulus by using elastic constant values = (GPa) Prediction HILL Shear modulus by using elastic constant values = (GPa) Prediction VOIGT Young modulus by using elastic constant values = (GPa) Prediction REUSS Young modulus by using elastic constant values = (GPa) Prediction HILL Young modulus by using elastic constant values = (GPa) Prediction VOIGT Poisson's coefficient by using elastic constant values =.270 Prediction REUSS Poisson's coefficient by using elastic constant values =.284 Prediction HILL Poisson's coefficient by using elastic constant values =.277 ================================================================================ By using HILL data Transverse elastic wave velocity = (m/s) Longitudinal elastic wave velocity = (m/s) The average wave velocity = (m/s) Debye Temperature = (K) ================================================================================ Melting Temperature = K or K ================================================================================ CsCl (our Cal) (Exp) 7 Method FPLAPW - Exchange PBE-sol - a (bohr) C C C
16 6 Installation of the Cubic-elastic package The Cubic-elastic package comes as a compress and tar file namely cubic2-elasticderiative-method-2012-p.tar.gz or cubic2-elastic.tar.gz. To install the package firstly copy the file to a directory of your choice. Now, uncompress and expand it as: tar zxvf cubic2-elastic-deriative-method-2012-p.tar.gz cd cubic2-elastic
17 Run buildc2irelast_lapw This program helps you to create the "Makefile" and then compile cubic2-elastic. By default, the Makefile expects the lapack_lapw and blas_lapw to be in the location../src_lib. This should be changed to the correct location by modifying the FOPT parameter as shown below. This Program helps you to define Fortran compiler, Fortran options, and Library options if you have installed WIEN2k. As you can see here this program defines Fortran compiler, Fortran options, and Library options as automatically. Otherwise you can define compiler and linker options as well as the path of mkl library depending on the your selected system. /home/mylib/mkl/lib/em64t is the path of my mkl library. To make Makefile by the lapack_lapw and blas_lapw libraries in the location../src_lib and gfortran use the following options: Fortran compiler: gfortran Fortran options: -ffree-form Library options (Lapack and BLAS): $(FOPT) L/home/physicsprogram/SRC_lib lpthread static llapack_lapw lblas_lapw the location../src_lib should be changed to the correct location by modifying the FOPT parameter as shown above. PS: To install with -ffree-form, you should compile the lapack_lapw and blas_lapw libraries with -ffree-form options. Otherwise it might was caused error.
18 If you view the OPTIONS file of the WIEN2k package you can use the FOPT, LDFLAGS, and R_LIBS of it for compiling. After defining the Fortran compiler, Fortran options, and Library options press Enter key.
19 The Environment Variable ELASTC2_PATH is then defined and added to the end of the.bashrc file. Thus you will be able to call cubic2-elastic s programs for any location. If you edit.bashrc file. You can see :
20 If you view the.bashrc file you can see Now logout from your Linux system and then login.
21 7 References [1] R. Stadler, W. Wolf, R. Podloucky, G. Kresse, J. Furthmller, J. Hafner, Phys. Rev. B 54 (1996) [2] P. Blaha, K. Schwarz, G.K.H. Madsen, D. Kvasnicka, J. Luitz, WIEN2k, An Augmented Plane Wave + Local Orbitals Program for Calculating Crystal Properties (Karlheinz Schwarz, Techn. Universität Wien, Austria), ISBN , [3] Michael J. Mehl, Phys. Rev. B 47 (1993) [4] D. Connétable, O. Thomas, Phys. Rev. B 79 (2009) [5] O. Beckstein, J. E. Klepeis, G. L. W. Hart, and O. Pankratov, Phys. Rev. B 64 (2001) [6] B. Z. Yanchitsky, A. N. Timoshevskii, Determination of the space group and unit cell for a periodic solid, Comp. Phys. Comm. 139 (2001) [7] D.D. Slagle, H. A. McKinstry, J. Appl. Phys. 38 (1967) 446. [8] V. Ganesan, K. Girirajan, Pramāna-J. Phys. 27 (1986) 472.
A Package for calculating elastic tensors of rhombohedral Phases by using second-order derivative with Wien2k Package
IR ELAST + WIEN2k A Package for calculating elastic tensors of rhombohedral Phases by using second-order derivative with Wien2k Package User s guide, Rhom-elastic_13.1 (Release 16.09.2013) Morteza Jamal
More informationA Package for calculating elastic tensors of tetragonal Phases by using second-order derivative with Wien2k Package
IR ELAST + WIEN2k A Package for calculating elastic tensors of tetragonal Phases by using second-order derivative with Wien2k Package User s guide, Tetra-elastic_13.2 (Release 27.08.2013) Morteza Jamal
More informationA Package for calculating elastic tensors of hexagonal Phases by using second-order derivative with Wien2k Package
IR E L A S T + W I E N 2k A Package for calculating elastic tensors of hexagonal Phases by using second-order derivative with Wien2k Package User s guide, Hex-elastic_13.2 (Release 27.08.2013) Morteza
More informationThis package performs a convenient 2-Dimensional structure optimization ( Volume and c/a ) for hexagonal or tetragonal spacegroups.
Package 2Doptimize -------------------------- This package performs a convenient 2-Dimensional structure optimization ( Volume and c/a ) for hexagonal or tetragonal spacegroups. If you want to use this
More informationCOMPUTATIONAL TOOL. Fig. 4.1 Opening screen of w2web
CHAPTER -4 COMPUTATIONAL TOOL Ph.D. Thesis: J. Maibam CHAPTER: 4 4.1 The WIEN2k code In this work, all the calculations presented are performed using the WIEN2k software package (Blaha et al., 2001). The
More informationExercises: In the following you find some suggestions for exercises, which teach you various tasks one may perform with WIEN2k.
Exercises: In the following you find some suggestions for exercises, which teach you various tasks one may perform with WIEN2k. New WIEN2k users should start with the first basic exercises (1-5), covering:
More informationColloque National sur les Techniques de Modélisation et de Simulation en Science des Matériaux, Sidi Bel-Abbès Novembre 2009
Colloque National sur les Techniques de Modélisation et de Simulation en Science des Matériaux, Sidi Bel-Abbès. 23-24 Novembre 2009 Elastic, electronic and optical properties of SiGe 2N 4 under pressure
More informationA DFT Study on Electronic Structures and Elastic Properties of AgX (X=C, N) in Rock Salt Structure
Invertis Journal of Jameson Science Maibam, and Technology, Kh. Kabita, Vol. B. Indrajit 7, No. 2, Sharma, 2014. R.K. ; pp. Thapa 114-118 and R.K. Brojen Singh A DFT Study on Electronic Structures and
More informationAb-initio Calculations of Structural, Electronic, Elastic and Mechanical Properties of REIn 3 and RETl 3 (RE= Yb & Lu) Intermetallic Compounds
Abstract Ab-initio Calculations of Structural, Electronic, Elastic and Mechanical Properties of REIn 3 and RETl 3 (RE= Yb & Lu) Intermetallic Compounds Jisha Annie Abraham 1, 2, Gitanjali Pagare 1,* and
More informationELECTRONIC AND MAGNETIC PROPERTIES OF BERKELIUM MONONITRIDE BKN: A FIRST- PRINCIPLES STUDY
ELECTRONIC AND MAGNETIC PROPERTIES OF BERKELIUM MONONITRIDE BKN: A FIRST- PRINCIPLES STUDY Gitanjali Pagare Department of Physics, Sarojini Naidu Govt. Girls P. G. Auto. College, Bhopal ( India) ABSTRACT
More informationNew tetranuclear manganese clusters with [MnII3MnIII] and [MnII2MnIII2] metallic cores exhibiting the low and high spin ground state
Electronic Supplementary Material (ESI) for Dalton Transactions. This journal is The Royal Society of Chemistry 2016 New tetranuclear manganese clusters with [MnII3MnIII] and [MnII2MnIII2] metallic cores
More informationCHAPTER 3 WIEN2k. Chapter 3 : WIEN2k 50
CHAPTER 3 WIEN2k WIEN2k is one of the fastest and reliable simulation codes among computational methods. All the computational work presented on lanthanide intermetallic compounds has been performed by
More informationEOS-FIT V6.0 R.J. ANGEL
EOS-FIT V6. R.J. AGEL Crystallography Laboratory, Dept. Geological Sciences, Virginia Tech, Blacksburg, VA46, USA http://www.geol.vt.edu/profs/rja/ ITRODUCTIO EosFit started as a program to fit equations
More informationComputational Material Science Part II-1: introduction. Horng-Tay Jeng ( 鄭弘泰 ) Institute of Physics, Academia Sinica
Computational Material Science Part II-1: introduction Horng-Tay Jeng ( 鄭弘泰 ) Institute of Physics, Academia Sinica Outline Introduction of Computational Material Science (CMS) Density Functional Theory
More informationAnalysis of an Electric-Field Gradient (EFG): the EFG-switch in LAPW2
Analysis of an Electric-Field Gradient (EFG): the EFG-switch in LAPW2 Katrin Koch Stefaan Cottenier August 10, 2011 0.1 In brief: the EFG and how it is obtained in LAPW The EFG is a traceless symmetric
More informationAb Initio Study of Electronic, Structural, Thermal and Mechanical Characterization of Cadmium Chalcogenides 65
Ab Initio Study of Electronic, Structural, Thermal and Mechanical Characterization of Cadmium Chalcogenides 65 Devi Prasadh P.S. 1, a, B.K. Sarkar 2, b 1 Department of Physics, Dr. Mahalingam College of
More informationGaAs -- MLWF. Special thanks to Elias Assmann (TU Graz) for the generous help in preparation of this tutorial
GaAs -- MLWF + + Special thanks to Elias Assmann (TU Graz) for the generous help in preparation of this tutorial YouTube video: https://youtu.be/r4c1yhdh3ge 1. Wien2k SCF Create a tutorial directory, e.g.
More informationIntroduction to Condensed Matter Physics
Introduction to Condensed Matter Physics Elasticity M.P. Vaughan Overview Overview of elasticity Classical description of elasticity Speed of sound Strain Stress Young s modulus Shear modulus Poisson ratio
More informationTHERMOPHYSICAL PROPERTIES OF THORIUM COMPOUNDS FROM FIRST PRINCIPLES
THERMOPHYSICAL PROPERTIES OF THORIUM COMPOUNDS FROM FIRST PRINCIPLES Vinayak Mishra a,* and Shashank Chaturvedi a a Computational Analysis Division, Bhabha Atomic Research Centre, Visakhapatnam 530012,
More informationThe quadrupole moments of Zn and Cd isotopes an update
Hyperfine Interact DOI 10.1007/s10751-010-0211-6 The quadrupole moments of Zn and Cd isotopes an update H. Haas J. G. Correia Springer Science+Business Media B.V. 2010 Abstract The nuclear quadrupole moments
More informationElectronic structure of Ce 2 Rh 3 Al 9
Materials Science-Poland, Vol. 24, No. 3, 2006 Electronic structure of Ce 2 Rh 3 Al 9 J. GORAUS 1*, A. ŚLEBARSKI 1, J. DENISZCZYK 2 1 Institute of Physics, University of Silesia, ul. Bankowa 12, 40-007
More informationElasticity of hcp nonmagnetic Fe under pressure
PHYSICAL REVIEW B 68, 054103 003 Elasticity of hcp nonmagnetic Fe under pressure S. L. Qiu Department of Physics, Alloy Research Center, Florida Atlantic University, Boca Raton, Florida 33431-0991, USA
More informationSome surprising results of the Kohn-Sham Density Functional
arxiv:1409.3075v1 [cond-mat.mtrl-sci] 10 Sep 2014 Some surprising results of the Kohn-Sham Density Functional L. G. Ferreira 1, M. Marques 2, L. K. Teles 2, R. R. Pelá 2 1 Instituto de Física, Universidade
More informationAs an example we consider the stacking and analysis of a 2-ply symmetric laminate. First we clear the Matlab space and close figures.
Program Lam 1 Introduction The collection of Matlab command and function files in the package lam allows the stacking and analysis of a laminate. In fact only a representative piece of a laminate is considered,
More information1.1 Contribution to the total energy For the LDA+U and orbital polarization methods a correction to the total energy appears E corr = E orb T r(v orb
Orbital package in WIEN P. Novak Institute of Physics, Prague, Czech Republic, novakp@fzu.cz April 2002 1 Description of SRC orb package Orbital package calculates the orbitally dependent potentials V
More informationFULL POTENTIAL LINEARIZED AUGMENTED PLANE WAVE (FP-LAPW) IN THE FRAMEWORK OF DENSITY FUNCTIONAL THEORY
FULL POTENTIAL LINEARIZED AUGMENTED PLANE WAVE (FP-LAPW) IN THE FRAMEWORK OF DENSITY FUNCTIONAL THEORY C.A. Madu and B.N Onwuagba Department of Physics, Federal University of Technology Owerri, Nigeria
More informationStructural, electronic, optical and mechanical properties of CsCaCl 3 and KCdF 3 cubic perovskites
International Journal of Materials Science ISSN 0973-4589 Volume 12, Number 1 (2017), pp. 137-147 Research India Publications http://www.ripublication.com Structural, electronic, optical and mechanical
More informationby investigation of elastic constants
Journal of Physics: Conference Series PAPER OPEN ACCESS Comparison between layering NbSe 2 and rod characteristic of MgB 2 by investigation of elastic constants To cite this article: Asiye Shokri et al
More informationFIRST PRINCIPLES STUDY OF AlBi
Available at: http://publications.ictp.it IC/2008/025 United Nations Educational, Scientific and Cultural Organization and International Atomic Energy Agency THE ABDUS SALAM INTERNATIONAL CENTRE FOR THEORETICAL
More informationCrystalline and Magnetic Anisotropy of the 3d Transition-Metal Monoxides
Crystalline and of the 3d Transition-Metal Monoxides Institut für Festkörpertheorie und -optik Friedrich-Schiller-Universität Max-Wien-Platz 1 07743 Jena 2012-03-23 Introduction Crystalline Anisotropy
More informationLindgren CRYSTAL SYMMETRY AND ELASTIC CONSTANTS MICHAEL WANDZILAK. S.B., Massachusetts Institute of Technology (196'7)
CRYSTAL SYMMETRY AND ELASTIC CONSTANTS by MICHAEL WANDZILAK S.B., Massachusetts Institute of Technology (196'7) Submitted in partial fulfillment of the requirements for the degree of Master of Science
More informationMaterials that you may find helpful when working through this exercise
Detailed steps illustrating how to use VASP on the Suns in Fitz 177 For use in lab: 11/10/2009 (Original file by Dr. Rachel Getman, 11/18/2007. Editted for use by Dorrell McCalman 11/09/2009.) Note on
More informationPredicting the Structure of Solids by DFT
Questions? Hudson Hall 235 or Hudson Hall 1111 Predicting the Structure of Solids by DFT Hands-On Instructions Contents 1 Cohesive Energy for Bulk Phases of Si 11 Setting up the Structures 12 Structure-Dependent
More informationExercises: In the following you find some suggestions for exercises, which teach you various tasks one may perform with WIEN2k.
Exercises: In the following you find some suggestions for exercises, which teach you various tasks one may perform with WIEN2k. Please note, that often calculational parameters are set to minimal cpu-time
More informationA two-dimensional FE truss program
A two-dimensional FE truss program 4M020: Design Tools Eindhoven University of Technology Introduction The Matlab program fem2d allows to model and analyze two-dimensional truss structures, where trusses
More informationStrain-related Tensorial Properties: Elasticity, Piezoelectricity and Photoelasticity
Strain-related Tensorial Properties: Elasticity, Piezoelectricity and Photoelasticity Torino, Italy, September 4-9, 2016 Alessandro Erba Dipartimento di Chimica, Università di Torino (Italy) alessandro.erba@unito.it
More informationMATERIAL MECHANICS, SE2126 COMPUTER LAB 4 MICRO MECHANICS. E E v E E E E E v E E + + = m f f. f f
MATRIAL MCHANICS, S226 COMPUTR LAB 4 MICRO MCHANICS 2 2 2 f m f f m T m f m f f m v v + + = + PART A SPHRICAL PARTICL INCLUSION Consider a solid granular material, a so called particle composite, shown
More informationPhotoelectron Interference Pattern (PEIP): A Two-particle Bragg-reflection Demonstration
Photoelectron Interference Pattern (PEIP): A Two-particle Bragg-reflection Demonstration Application No. : 2990 Beamlime: BL25SU Project Leader: Martin Månsson 0017349 Team Members: Dr. Oscar Tjernberg
More informationOPENATOM for GW calculations
OPENATOM for GW calculations by OPENATOM developers 1 Introduction The GW method is one of the most accurate ab initio methods for the prediction of electronic band structures. Despite its power, the GW
More informationconnect/setup of w2web environment
connect/setup of w2web environment Connect to pleiades.bc.edu using NoMachine as indicated in the instructions and with the username/pw you got during registration. open a terminal and connect to your
More informationThe Augmented Spherical Wave Method
Introduction Institut für Physik, Universität Augsburg Electronic Structure in a Nutshell Outline 1 Fundamentals Generations 2 Outline 1 Fundamentals Generations 2 Outline Fundamentals Generations 1 Fundamentals
More informationLecture 4 Implementing material models: using usermat.f. Implementing User-Programmable Features (UPFs) in ANSYS ANSYS, Inc.
Lecture 4 Implementing material models: using usermat.f Implementing User-Programmable Features (UPFs) in ANSYS 1 Lecture overview What is usermat.f used for? Stress, strain and material Jacobian matrix
More informationMustafa Uludogan 1, Tahir Cagin, William A. Goddard, III Materials and Process Simulation Center, Caltech, Pasadena, CA 91125, U.S.A.
Ab Initio Studies On Phase Behavior of Barium Titanate Mustafa Uludogan 1, Tahir Cagin, William A. Goddard, III Materials and Process Simulation Center, Caltech, Pasadena, CA 91125, U.S.A. 1 Physics Department,
More informationSupporting Information
Supporting Information Yi et al..73/pnas.55728 SI Text Study of k z Dispersion Effect on Anisotropy of Fermi Surface Topology. In angle-resolved photoemission spectroscopy (ARPES), the electronic structure
More informationMcMAT 2007 Micromechanics of Materials Austin, Texas, June 3 7, 2007
McMAT 2007 Micromechanics of Materials Austin, Texas, June 3 7, 2007 RANDOM POLYCRYSTALS OF GRAINS WITH CRACKS: MODEL OF ELASTIC BEHAVIOR FOR FRACTURED SYSTEMS James G. Berryman Earth Sciences Division
More informationNOT FOR DISTRIBUTION REVIEW COPY. Na 2 IrO 3 as a molecular orbital crystal
Na 2 IrO 3 as a molecular orbital crystal I. I. Mazin, 1 Harald O. Jeschke, 2 Kateryna Foyevtsova, 2 Roser Valentí, 2 and D. I. Khomskii 3 1 Code 6393, Naval Research Laboratory, Washington, DC 237, USA
More informationSpin-orbit coupling in Wien2k
Spin-orbit coupling in Wienk Robert Laskowski rolask@ihpc.a-star.edu.sg Institute of High Performance Computing Singapore Dirac Hamiltonian Quantum mechanical description of electrons, consistent with
More information1 Runwien user's and reference guide
1 Runwien user's and reference guide Authors: Alberto Otero-de-la-Roza and Víctor Luaña Contact: alberto@carbono.quimica.uniovi.es Address: Departamento de Química Física y Analítica, Universidad de Oviedo,
More informationWannier functions. Macroscopic polarization (Berry phase) and related properties. Effective band structure of alloys
Wannier functions Macroscopic polarization (Berry phase) and related properties Effective band structure of alloys P.Blaha (from Oleg Rubel, McMaster Univ, Canada) Wannier functions + + Wannier90: A Tool
More informationSpin transport in Magnetic Tunnel Junctions
Spin transport in Magnetic Tunnel Junctions Tutorial on spin transport in Fe-MgO-Fe Version 2015.2 Spin transport in Magnetic Tunnel Junctions: Tutorial on spin transport in Fe-MgO-Fe Version 2015.2 Copyright
More informationOn Dynamic and Elastic Stability of Lanthanum Carbide
Journal of Physics: Conference Series On Dynamic and Elastic Stability of Lanthanum Carbide To cite this article: B D Sahoo et al 212 J. Phys.: Conf. Ser. 377 1287 Recent citations - Theoretical prediction
More informationDMDW: A set of tools to calculate Debye-Waller factors and other related quantities using dynamical matrices.
DMDW: A set of tools to calculate Debye-Waller factors and other related quantities using dynamical matrices. DMDW is a set of tools developed to calculate Debye-Waller (DW) factors and other related quantities
More informationInvestigation of mechanical stability of possible structures of PtN using first-principles computations
Investigation of mechanical stability of possible structures of PtN using first-principles computations S. K. R. Patil, S. V. Khare, * B. R. Tuttle, 3 J. K. Bording, 4 and S. Kodambaka 5 Department of
More informationChemical bonding, elasticity, and valence force field models: A case study for -Pt 2 Si and PtSi
PHYSICAL REVIEW B, VOLUME 64, 550 Chemical bonding, elasticity, and valence force field models: A case study for -Pt 2 Si and PtSi J. E. Klepeis, O. Beckstein, 2 O. Pankratov, 2 and G. L. W. Hart 3 Lawrence
More informationThe Linearized Augmented Planewave (LAPW) Method
The Linearized Augmented Planewave (LAPW) Method David J. Singh Oak Ridge National Laboratory E T [ ]=T s [ ]+E ei [ ]+E H [ ]+E xc [ ]+E ii {T s +V ks [,r]} I (r)= i i (r) Need tools that are reliable
More informationTwo-dimensional Phosphorus Carbide as Promising Anode Materials for Lithium-ion Batteries
Electronic Supplementary Material (ESI) for Journal of Materials Chemistry A. This journal is The Royal Society of Chemistry 2018 Supplementary Material for Two-dimensional Phosphorus Carbide as Promising
More informationCHAPTER: 8. ELECTRONIC STRUCTURE AND ELASTIC PROPERTIES OF CrC AND CrN. 8.1 Introduction. Ph.D. Thesis: J. Maibam
CHAPTER -8 CHAPTER: 8 ELECTRONIC STRUCTURE AND ELASTIC PROPERTIES OF CrC AND CrN 8.1 Introduction In this chapter, we have selected CrC and CrN from group VIB transition metal carbides and nitrides for
More information16.21 Techniques of Structural Analysis and Design Spring 2003 Unit #5 - Constitutive Equations
6.2 Techniques of Structural Analysis and Design Spring 2003 Unit #5 - Constitutive quations Constitutive quations For elastic materials: If the relation is linear: Û σ ij = σ ij (ɛ) = ρ () ɛ ij σ ij =
More informationEquilibrium state of a metal slab and surface stress
PHYSICAL REVIEW B VOLUME 60, NUMBER 23 15 DECEMBER 1999-I Equilibrium state of a metal slab and surface stress P. M. Marcus IBM Research Division, T. J. Watson Research Center, Yorktown Heights, New York
More informationComputational Materials Science with the WIEN2k code
Computational Materials Science with the WIEN2k code P. Blaha Institute of Materials Chemistry TU Wien pblaha@theochem.tuwien.ac.at http://www.wien2k.at Computational Materials Science describe materials
More informationDynamics of the Atmosphere GEMPAK Lab 3. 3) In-class exercise about geostrophic balance in the real atmosphere.
Dynamics of the Atmosphere GEMPAK Lab 3 Goals of this lab: 1) Learn about Linux scripts. 2) Learn how to combine levels in GEMPAK functions. 3) In-class exercise about geostrophic balance in the real atmosphere.
More informationExample: H 2 O (the car file)
Example: H 2 O (the car file) As a practical example of DFT methods we calculate the energy and electronic properties of the water molecule. In order to carry out the DFT calculation you will need a set
More informationTable of Contents. Table of Contents Spin-orbit splitting of semiconductor band structures
Table of Contents Table of Contents Spin-orbit splitting of semiconductor band structures Relavistic effects in Kohn-Sham DFT Silicon band splitting with ATK-DFT LSDA initial guess for the ground state
More informationSupplementary Materials
Supplementary Materials Atomistic Origin of Brittle Failure of Boron Carbide from Large Scale Reactive Dynamics Simulations; Suggestions toward Improved Ductility Qi An and William A. Goddard III * Materials
More informationarxiv:physics/ v2 [physics.atom-ph] 31 May 2004
arxiv:physics/0405136v2 [physics.atom-ph] 31 May 2004 Pure spin angular momentum coefficients for non scalar one particle operators in jj coupling G. Gaigalas a and S. Fritzsche b a Institute of Theoretical
More informationPROMAL2012 SOFTWARE PACKAGE A USER GUIDE
PROMAL2012 SOFTWARE PACKAGE A USER GUIDE 1. This manual is only for VISTA, WINDOWS 7 and WINDOWS 8 users. The PROMAL2012 software and manual are available at http://www.eng.usf.edu/~kaw/promal2012/ 2.
More informationarxiv:cond-mat/ v2 [cond-mat.mtrl-sci] 10 Jun 2001
First principles elastic constants and electronic structure of α-pt 2 Si and PtSi arxiv:cond-mat/0008200v2 [cond-mat.mtrl-sci] 0 Jun 200 O. Beckstein, () J. E. Klepeis, (2) G. L. W. Hart, (3) and O. Pankratov
More informationCalculating anisotropic physical properties from texture data using the MTEX open source package
Calculating anisotropic physical properties from texture data using the MTEX open source package David Mainprice 1, Ralf Hielscher 2, Helmut Schaeben 3 February 10, 2011 1 Geosciences Montpellier UMR CNRS
More informationPuckering and spin orbit interaction in nano-slabs
Electronic structure of monolayers of group V atoms: Puckering and spin orbit interaction in nano-slabs Dat T. Do* and Subhendra D. Mahanti* Department of Physics and Astronomy, Michigan State University,
More informationElectronic structure and elastic properties of ATiO 3 (A = Ba, Sr, Ca) perovskites: A first principles study
Indian Journal of Pure & Applied Physics Vol. 53, February 015, pp. 10-109 Electronic structure and elastic properties of ATiO 3 (A = Ba, Sr, Ca) perovskites: A first principles study Anup Pradhan Sakhya
More informationLab 3: Handout Quantum-ESPRESSO: a first principles code, part 2.
1 Lab 3: Handout Quantum-ESPRESSO: a first principles code, part 2. In this lab, we will be using Quantum-ESPRESSO as our first-principles code again. In problem 1, we will compare energy between allotropes
More informationexciting in a nutshell
http://exciting-code.org exciting in a nutshell Pasquale Pavone Humboldt-Universität zu Berlin http://exciting-code.org exciting in a (coco)nutshell Pasquale Pavone Humboldt-Universität zu Berlin Outline
More informationEBIS-PIC 2D. 2D EBIS Simulation Code. Version 0.1. Copyright ( ) January FAR-TECH, Inc Science Center Dr., Ste 150. San Diego CA 92121
EBIS-PIC 2D 2D EBIS Simulation Code Version 0.1 Copyright ( ) January 2017 by 10350 Science Center Dr., Ste 150 San Diego CA 92121 Phone 858-455-6655 Email support@far-tech.com URL http://www.far-tech.com
More informationPWSCF First examples
PWSCF First examples (much more in espresso 3.1.1/examples directory!) Guido Fratesi (Università di Milano) Urbana, August 2006 A pw.x input file &CONTROL / &SYSTEM / &ELECTRONS title calculation restart_mode
More informationTABLE OF CONTENTS. Mechanics of Composite Materials, Second Edition Autar K Kaw University of South Florida, Tampa, USA
Mechanics of Composite Materials, Second Edition Autar K Kaw University of South Florida, Tampa, USA TABLE OF CONTENTS 1. INTRODUCTION TO COMPOSITE MATERIALS 1.1 Introduction... 1.2 Classification... 1.2.1
More informationIAP 2006: From nano to macro: Introduction to atomistic modeling techniques and application in a case study of modeling fracture of copper (1.
IAP 2006: From nano to macro: Introduction to atomistic modeling techniques and application in a case study of modeling fracture of copper (1.978 PDF) http://web.mit.edu/mbuehler/www/teaching/iap2006/intro.htm
More informationStructural and Optical Properties of ZnSe under Pressure
www.stmjournals.com Structural and Optical Properties of ZnSe under Pressure A. Asad, A. Afaq* Center of Excellence in Solid State Physics, University of the Punjab Lahore-54590, Pakistan Abstract The
More informationResidual Stress analysis
Residual Stress analysis Informations: strains Macro elastic strain tensor (I kind) Crystal anisotropic strains (II kind) Fe Cu C Macro and micro stresses Applied macro stresses Residual Stress/Strain
More informationand strong interlayer quantum confinement
Supporting Information GeP3: A small indirect band gap 2D crystal with high carrier mobility and strong interlayer quantum confinement Yu Jing 1,3, Yandong Ma 1, Yafei Li 2, *, Thomas Heine 1,3 * 1 Wilhelm-Ostwald-Institute
More informationChapter: 22. Visualization: Making INPUT File and Processing of Output Results
Chapter: 22 Visualization: Making INPUT File and Processing of Output Results Keywords: visualization, input and output structure, molecular orbital, electron density. In the previous chapters, we have
More informationMATERIAL ELASTIC ANISOTROPIC command
MATERIAL ELASTIC ANISOTROPIC command.. Synopsis The MATERIAL ELASTIC ANISOTROPIC command is used to specify the parameters associated with an anisotropic linear elastic material idealization. Syntax The
More informationAERSYS KNOWLEDGE UNIT
-7016 1. INTRODUCTION The scope of this document is to provide a clarification and a deeper understanding of the two different ways to move the mid plane of the element out of the nodal plane. Although
More informationModule 2: Quantum Espresso Walkthrough
Module 2: Quantum Espresso Walkthrough Energy and Geometry Optimization of the H 2 Molecule We will be using the PWSCF code for quantum mechanical calculations of extended systems. The PWSCF program is
More informationSurface stress and relaxation in metals
J. Phys.: Condens. Matter 12 (2000) 5541 5550. Printed in the UK PII: S0953-8984(00)11386-4 Surface stress and relaxation in metals P M Marcus, Xianghong Qian and Wolfgang Hübner IBM Research Center, Yorktown
More informationCalculation of the Structural, Electrical, and Optical Properties of κ-al 2 O 3 by Density Functional Theory
CHINESE JOURNAL OF PHYSICS VOL. 46, NO. 2 APRIL 2008 Calculation of the Structural, Electrical, and Optical Properties of κ-al 2 O 3 by Density Functional Theory S. J. Mousavi, 1, S. M. Hosseini, 2 M.
More informationDue: since the calculation takes longer than before, we ll make it due on 02/05/2016, Friday
Homework 3 Due: since the calculation takes longer than before, we ll make it due on 02/05/2016, Friday Email to: jqian@caltech.edu Introduction In this assignment, you will be using a commercial periodic
More informationRelativistic effects & magnetism. in WIEN2k
4 th WIENk Workshop Vienna 7 Relativistic effects & magnetism in WIENk Xavier Rocquefelte Institut des Sciences Chimiques de Rennes (UMR 66) Université de Rennes, FRANCE 4 th WIENk Workshop Vienna 7 Talk
More informationMagnetism (FM, AFM, FSM)
Magnetism (FM, AFM, FSM) Karlheinz Schwarz Institute of Materials Chemistry TU Wien Localized vs. itinerant systems In localized systems (e.g. some rare earth) the magnetism is mainly governed by the atom
More informationScientific Programming in C XIII. Shell programming
Scientific Programming in C XIII. Shell programming Susi Lehtola 11 December 2012 Introduction Often in scientific computing one needs to do simple tasks related to renaming of files file conversions unit
More informationTwo implementations of the Projector Augmented Wave (PAW) formalism
Introduction The tools available for detailed first-principles studies of materials have benefited enormously from the development of several international collaborations engaged in developing open source
More informationFirst-principles study of the structural stability of Mn 3 Z (Z=Ga, Sn and Ge) Heusler compounds
First-principles study of the structural stability of Mn 3 Z (Z=Ga, Sn and Ge) Heusler compounds Delin Zhang 1, Binghai Yan 1,2,3, Shu-Chun Wu 1, Jürgen Kübler 4, Guido Kreiner 1, Stuart S. P. Parkin 4,
More informationStatus report on the showering of Alpgen events with Herwig++ for ATLAS
Status report on the showering of Alpgen events with Herwig++ for ATLAS University of Oslo December 202 Introduction We want to set up and validate the processing of Alpgen events with Herwig++ in ATLAS,
More informationElasticity Constants of Clay Minerals Using Molecular Mechanics Simulations
Elasticity Constants of Clay Minerals Using Molecular Mechanics Simulations Jin-ming Xu, Cheng-liang Wu and Da-yong Huang Abstract The purpose of this paper is to obtain the elasticity constants (including
More informationSymmetry Assumptions, Kramers Kronig Transformation and Analytical Continuation in Ab Initio Calculations of Optical Conductivities
Physica Scripta. Vol. T09, 70 74, 2004 Symmetry Assumptions, Kramers Kronig Transformation and Analytical Continuation in Ab Initio Calculations of Optical Conductivities Helmut Rathgen and Mikhail I.
More informationBoris Mantisi. Contents. Context 2. How to install APoGe 3. How APoGe works 4. Input File 5. Crystal File 8. How to use APoGe 10
Boris Mantisi Contents Context 2 How to install APoGe 3 How APoGe works 4 Input File 5 Crystal File 8 How to use APoGe 10 Context Polycrystalline structure plays an important role in the macroscopic properties
More informationSIMULATION OF FLUID-STRUCTURAL INTERACTION
SIMULATION OF FLUID-STRUCTURAL INTERACTION USING OPENFOAM Hua-Dong Yao Department of Applied Mechanics, Chalmers University of Technology Sep 15, 2014 Hua-Dong Yao Simulation of FSI using OpenFOAM Sep
More informationMinnesota Functional Module Version 1.8
1 Minnesota Functional Module Version 1.8 Subroutines for evaluating the M05, M05-2X, M06-L, M06-HF, M06, M06-2X, M08-HX, M08-SO, M11, M11-L, MN12-L, SOGGA, SOGGA11, SOGGA11-X, N12, N12-SX Functionals
More informationELECTRONIC STRUCTURE AND CHEMICAL BONDING IN LAVES PHASES Al 2 Ca, Be 2 Ag AND Be 2 Ti. D. Shapiro, D. Fuks, A. Kiv
Computer Modelling and New Technologies, 2009, Vol.13, No.1, 7 16 Transport and Telecommunication Institute, Lomonosova 1, LV-1019, Riga, Latvia ELECTRONIC STRUCTURE AND CHEMICAL BONDING IN LAVES PHASES
More informationSpacegroup P4 2 /mnm. Structure given by: spacegroup lattice parameter positions of atoms (basis)
Spacegroup P4 2 /mnm Structure given by: spacegroup lattice parameter positions of atoms (basis) Rutile TiO 2 : P4 2 /mnm (136) a=8.68, c=5.59 bohr Ti: (0,0,0) O: (0.304,0.304,0) Specify: Structure generator
More informationMSE 201A Thermodynamics and Phase Transformations Fall, 2008 Problem Set No. 7
MSE 21A Thermodynamics and Phase Transformations Fall, 28 Problem Set No. 7 Problem 1: (a) Show that if the point group of a material contains 2 perpendicular 2-fold axes then a second-order tensor property
More information