Materials Science with WIEN2k on vsc1 and vsc2
|
|
- Mervin Ward
- 6 years ago
- Views:
Transcription
1 Materials Science with WIEN2k on vsc1 and vsc2 P. Blaha Institute of Materials Chemistry TU Wien
2 Computational Materials Science describe materials by quantummechanical simulations ab initio (parameter free) simulate: infinite ( perfect ) bulk solids impurities, vacancies in solids surfaces nanostructures atoms + molecules
3 Computational Materials Science atomic structure geometry stability phase transitions mechanical properties
4 Computational Materials Science electronic structure bandstructure + density of states magnetism chemical bonding,. spectroscopies (IR, Raman, XPS, XAS, XES, EELS,Mössbauer, NMR, STM)
5 Method: DFT calculations numerical solution of a Schrödinger-like equation (Kohn-Sham) 2 potential V: 1 2 classical Coulomb potentials between nuclei and electrons quantummechanical electron-electron interaction density-functional-theory (DFT Walter Kohn) in principle: exact in practice: various approximations LDA GGA Hybrid-DFT dynamical mean field theory V ( r) k i k i k i
6 Walter Kohn, Nobel Prize 1998 Chemistry i are illegitimate children of DFT time-dependent DFT, GW, BSE, DMFT
7 Method: DFT calculations numerical solution of a Schrödinger-like equation (Kohn-Sham) k k k V ( r) i i i 2 expansion into augmented plane waves basisfunctions Kn : variational principle 1 2 k = C K n k n k < E n n APWs / atom < H > < E >= < > C k n > = 0 generalized eigenvalue problem H C=E S C Setup and diagonalization of (real or complex) matrices of size to (up to 200 Gb memory, only 10% of i )
8 Loops: loop 1: different structures (atomic positions) loop 2: scf-cycle (solve [-½ 2 +V] = E new V iterate) loop 3: k-loop (solve H =E for different k-points) loop 4: setup + diagonalization of HC= E SC largest effort, highest optimization, best parallelization, scaling of time and memory processors F90, mpi, Scalapack, blas loop over APWs in parallel (via scripts, slow network, common NFS) sequential (efficient multi-secant BROYDEN-mixing; L.Marks PRB 78, ) coarse grain parallel (different jobs) or sequential (forces new positions)
9 WIEN2k software package An Augmented Plane Wave Plus Local Orbital Program for Calculating Crystal Properties Peter Blaha Karlheinz Schwarz Georg Madsen Dieter Kvasnicka Joachim Luitz November 2001 Vienna, AUSTRIA Vienna University of Technology developed over more than 25 years 2000 registered groups 1800 mailinglist users Europe: A, B, CH, CZ, D, DK, ES, F, FIN, GR, H, I, IL, IRE, N, NL, PL, RO, S, SK, SL, SI, UK, ETH Zürich, MPI Stuttgart, FHI Berlin, DESY, TH Aachen, ESRF, Prague, IJS Ljubjlana, Paris, Chalmers, Cambridge, Oxford America: ARG, BZ, CDN, MX, USA (MIT, NIST, Berkeley, Princeton, Harvard, Argonne NL, Los Alamos NL, Oak Ridge NL, Penn State, Purdue, Georgia Tech, Lehigh, John Hopkins, Chicago, Stony Brook, SUNY, UC St.Barbara, UCLA) far east: AUS, China, India, JPN, Korea, Pakistan, Singapore,Taiwan (Beijing, Tokyo, Osaka, Kyoto, Sendai, Tsukuba, Hong Kong) 55 industries (Canon, Eastman, Exxon, Fuji, Hitachi, IBM, Idemitsu Petrochem., Kansai, Komatsu, Konica-Minolta, A.D.Little, Mitsubishi, Mitsui Mining, Motorola, NEC, Nippon Steel, Norsk Hydro, Osram, Panasonic, Samsung, Seiko Epson, Siemens, Sony, Sumitomo,TDK,Toyota).
10 setup and iter. diagonalization of HC=ESC ifort: vsc1 2x faster mkl: (dgemm) vsc1 1.5 x faster diag with scalapack: (blocked davidson) vsc1 ~ 1.2 x faster (256 cores) vsc2 does not scale for more than 768 cores vsc2 (even with 2048 cores) cannot beat 768 vsc1-cores (matrix size: , real*8)
11 speedup: speedup of own mpi-code close to optimal little communication sequential parts < 0.1 (1% seq: 50 x speedup on 100 cores max 100 x on 1000 cores ) iter. diag using scalapack: VSC-2 scaling limited to ~768 cores (even for VERY large problem) pdsymm (m-m mult) does not scale well some smaller parts show constant time time for diag of small sub-space (10000) problem increases 2x and dominates needs some additional code optimizations
12 calculate density from eigenvectors: 2 way parallelization: N-core = N-atoms * N-energies (less cpu) (less comm +I/O) cores: VSC-1 NE= VSC-2 NE= NE= NE= read 5GB + distribute to N-atom cores (mpi_bcast, mpi_scatter) VSC-1 NE= VSC-2 NE= NE= NE= I/O or infiniband bottlenecks on vsc2?
13 I/O or infiniband problems of vsc2: $HOME (NFS): jobs hang frequently during longer calc. $GLOBAL: jobs hang much less ls -als of large dir: 7s ( 0s on vsc1) loading of 500MB file in vi: 7s (<3s on vsc1)
14 starting 16 single-core jobs on one node: time command of such a parallel run: irregular run time with up to 50% overhead r01n01(1) u 0.348s 1: % r01n01(1) u 0.264s 1: % r01n01(1) u 0.197s 1: % r01n01(1) u 0.197s 1: % r01n01(1) u 0.199s 1: % r01n01(1) u 0.245s 1: % r01n01(1) u 0.215s 1: % r01n01(1) u 0.235s 1: % r01n01(1) u 0.217s % r01n01(1) u 0.226s 1: % r01n01(1) u 0.240s 1: % r01n01(1) u 0.227s 1: % r01n01(1) u 0.209s % r01n01(1) u 0.250s 1: % problem has been fixed using taskset command. All jobs finish after ~60 sec (within 2-3 sec).
15 wish-list vsc-3: don t look at Top-500 performance, but ensure sustained performance (mpi, scalapack - scaling) faster cpus (instead of more cores)
16 Thank you for your attention!
Computational 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 informationIterative Diagonalization in Augmented Plane Wave Based Methods in Electronic Structure Calculations
* 0. Manuscript Click here to view linked References 1 1 1 1 0 1 0 1 0 1 0 1 0 1 Iterative Diagonalization in Augmented Plane Wave Based Methods in Electronic Structure Calculations P. Blaha a,, H. Hofstätter
More informationChapter 3. The (L)APW+lo Method. 3.1 Choosing A Basis Set
Chapter 3 The (L)APW+lo Method 3.1 Choosing A Basis Set The Kohn-Sham equations (Eq. (2.17)) provide a formulation of how to practically find a solution to the Hohenberg-Kohn functional (Eq. (2.15)). Nevertheless
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 informationCountry
Total A 36,3 31,1 B 33,8 36,9 37,4 D 41,4 D-W 41,6 37,7 40,7 42,4 D-E 28,2 36,9 36,8 DK 55,8 49,1 48,8 E 33,2 39,5 33,2 28,9 F 44,4 33,1 36,3 FIN 62,2 30,9 50,6 54,6 GB 26,1 26,2 27,1 GR 14,5 I 34,5 32,1
More informationDensity functional theory (DFT) and the concepts of the augmented-plane-wave plus local orbital (L)APW+lo method
Density functional theory (DFT) and the concepts of the augmented-plane-wave plus local orbital (L)APW+lo method Karlheinz Schwarz Institute for Material Chemistry TU Wien Vienna University of Technology
More informationCountry
Total EU-12 89,6 89,4 85,7 82,9 85,9 86,9 87,4 EU-15 89,6 85,7 83,1 86,2 87,0 87,5 EU-25 87,9 A 95,1 90,2 88,0 90,8 88,2 93,7 B 80,7 91,1 84,6 84,3 86,3 89,6 85,8 D 95,1 94,1 86,1 86,3 88,0 86,4 89,4 D-W
More informationComparison of various abinitio codes used in periodic calculations
Comparison of various abinitio codes used in periodic calculations 1 Prof.P. Ravindran, Department of Physics, Central University of Tamil Nadu, India & Center for Materials Science and Nanotechnology,
More informationVASP: running on HPC resources. University of Vienna, Faculty of Physics and Center for Computational Materials Science, Vienna, Austria
VASP: running on HPC resources University of Vienna, Faculty of Physics and Center for Computational Materials Science, Vienna, Austria The Many-Body Schrödinger equation 0 @ 1 2 X i i + X i Ĥ (r 1,...,r
More informationDensity functional theory (DFT) and the concepts of the augmented-plane-wave plus local orbital (L)APW+lo method
Density functional theory (DFT) and the concepts of the augmented-plane-wave plus local orbital (L)APW+lo method Karlheinz Schwarz Institute for Material Chemistry TU Wien Vienna University of Technology
More informationab initio Electronic Structure Calculations
ab initio Electronic Structure Calculations New scalability frontiers using the BG/L Supercomputer C. Bekas, A. Curioni and W. Andreoni IBM, Zurich Research Laboratory Rueschlikon 8803, Switzerland ab
More informationCRYSTAL in parallel: replicated and distributed (MPP) data. Why parallel?
CRYSTAL in parallel: replicated and distributed (MPP) data Roberto Orlando Dipartimento di Chimica Università di Torino Via Pietro Giuria 5, 10125 Torino (Italy) roberto.orlando@unito.it 1 Why parallel?
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 informationELSI: A Unified Software Interface for Kohn-Sham Electronic Structure Solvers
ELSI: A Unified Software Interface for Kohn-Sham Electronic Structure Solvers Victor Yu and the ELSI team Department of Mechanical Engineering & Materials Science Duke University Kohn-Sham Density-Functional
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 informationIntroduction to Density Functional Theory
1 Introduction to Density Functional Theory 21 February 2011; V172 P.Ravindran, FME-course on Ab initio Modelling of solar cell Materials 21 February 2011 Introduction to DFT 2 3 4 Ab initio Computational
More informationParallel Eigensolver Performance on High Performance Computers
Parallel Eigensolver Performance on High Performance Computers Andrew Sunderland Advanced Research Computing Group STFC Daresbury Laboratory CUG 2008 Helsinki 1 Summary (Briefly) Introduce parallel diagonalization
More informationPseudopotentials: design, testing, typical errors
Pseudopotentials: design, testing, typical errors Kevin F. Garrity Part 1 National Institute of Standards and Technology (NIST) Uncertainty Quantification in Materials Modeling 2015 Parameter free calculations.
More informationDirect Self-Consistent Field Computations on GPU Clusters
Direct Self-Consistent Field Computations on GPU Clusters Guochun Shi, Volodymyr Kindratenko National Center for Supercomputing Applications University of Illinois at UrbanaChampaign Ivan Ufimtsev, Todd
More informationElectronic structure calculations with GPAW. Jussi Enkovaara CSC IT Center for Science, Finland
Electronic structure calculations with GPAW Jussi Enkovaara CSC IT Center for Science, Finland Basics of density-functional theory Density-functional theory Many-body Schrödinger equation Can be solved
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 informationLarge Scale Electronic Structure Calculations
Large Scale Electronic Structure Calculations Jürg Hutter University of Zurich 8. September, 2008 / Speedup08 CP2K Program System GNU General Public License Community Developers Platform on "Berlios" (cp2k.berlios.de)
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 informationThe electronic structure of materials 2 - DFT
Quantum mechanics 2 - Lecture 9 December 19, 2012 1 Density functional theory (DFT) 2 Literature Contents 1 Density functional theory (DFT) 2 Literature Historical background The beginnings: L. de Broglie
More informationParallelization of the Molecular Orbital Program MOS-F
Parallelization of the Molecular Orbital Program MOS-F Akira Asato, Satoshi Onodera, Yoshie Inada, Elena Akhmatskaya, Ross Nobes, Azuma Matsuura, Atsuya Takahashi November 2003 Fujitsu Laboratories of
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 informationA Green Function Method for Large Scale Electronic Structure Calculations. Rudolf Zeller
A Green Function Method for Large Scale Electronic Structure Calculations Rudolf Zeller Institute for Advanced Simulation, Forschungszentrum Jülich Electronic structure calculations (density functional
More informationIntroduction to Density Functional Theory
Introduction to Density Functional Theory S. Sharma Institut für Physik Karl-Franzens-Universität Graz, Austria 19th October 2005 Synopsis Motivation 1 Motivation : where can one use DFT 2 : 1 Elementary
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 informationAll-electron density functional theory on Intel MIC: Elk
All-electron density functional theory on Intel MIC: Elk W. Scott Thornton, R.J. Harrison Abstract We present the results of the porting of the full potential linear augmented plane-wave solver, Elk [1],
More informationBasic introduction of NWChem software
Basic introduction of NWChem software Background NWChem is part of the Molecular Science Software Suite Designed and developed to be a highly efficient and portable Massively Parallel computational chemistry
More informationParallel Eigensolver Performance on the HPCx System
Parallel Eigensolver Performance on the HPCx System Andrew Sunderland, Elena Breitmoser Terascaling Applications Group CCLRC Daresbury Laboratory EPCC, University of Edinburgh Outline 1. Brief Introduction
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 informationPerformance optimization of WEST and Qbox on Intel Knights Landing
Performance optimization of WEST and Qbox on Intel Knights Landing Huihuo Zheng 1, Christopher Knight 1, Giulia Galli 1,2, Marco Govoni 1,2, and Francois Gygi 3 1 Argonne National Laboratory 2 University
More informationHECToR CSE technical meeting, Oxford Parallel Algorithms for the Materials Modelling code CRYSTAL
HECToR CSE technical meeting, Oxford 2009 Parallel Algorithms for the Materials Modelling code CRYSTAL Dr Stanko Tomi Computational Science & Engineering Department, STFC Daresbury Laboratory, UK Acknowledgements
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 informationReferences. Documentation Manuals Tutorials Publications
References http://siesta.icmab.es Documentation Manuals Tutorials Publications Atomic units e = m e = =1 atomic mass unit = m e atomic length unit = 1 Bohr = 0.5292 Ang atomic energy unit = 1 Hartree =
More informationFirst-Principles Vibrational spectroscopy and lattice dynamics of materials in the solid state
First-Principles Vibrational spectroscopy and lattice dynamics of materials in the solid state Keith Refson Computational Science and Engineering Department STFC Rutherford Appleton Laboratory First principles
More informationDensity Functional Theory. Martin Lüders Daresbury Laboratory
Density Functional Theory Martin Lüders Daresbury Laboratory Ab initio Calculations Hamiltonian: (without external fields, non-relativistic) impossible to solve exactly!! Electrons Nuclei Electron-Nuclei
More informationDept of Mechanical Engineering MIT Nanoengineering group
1 Dept of Mechanical Engineering MIT Nanoengineering group » Recap of HK theorems and KS equations» The physical meaning of the XC energy» Solution of a one-particle Schroedinger equation» Pseudo Potentials»
More informationBasic introduction of NWChem software
Basic introduction of NWChem software Background! NWChem is part of the Molecular Science Software Suite! Designed and developed to be a highly efficient and portable Massively Parallel computational chemistry
More informationOrbital Density Dependent Functionals
Orbital Density Dependent Functionals S. Kluepfel1, P. Kluepfel1, Hildur Guðmundsdóttir1 and Hannes Jónsson1,2 1. Univ. of Iceland; 2. Aalto University Outline: Problems with GGA approximation (PBE, RPBE,...)
More informationBlock Iterative Eigensolvers for Sequences of Dense Correlated Eigenvalue Problems
Mitglied der Helmholtz-Gemeinschaft Block Iterative Eigensolvers for Sequences of Dense Correlated Eigenvalue Problems Birkbeck University, London, June the 29th 2012 Edoardo Di Napoli Motivation and Goals
More informationA Package for calculating elastic tensors of cubic 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 cubic Phases by using second-order derivative with WIEN2k Package User s guide, Cubic-elastic_13.2 (Release 27.08.2013) Morteza Jamal
More informationINITIAL INTEGRATION AND EVALUATION
INITIAL INTEGRATION AND EVALUATION OF SLATE PARALLEL BLAS IN LATTE Marc Cawkwell, Danny Perez, Arthur Voter Asim YarKhan, Gerald Ragghianti, Jack Dongarra, Introduction The aim of the joint milestone STMS10-52
More informationIntroduction to density-functional theory. Emmanuel Fromager
Institut de Chimie, Strasbourg, France Page 1 Emmanuel Fromager Institut de Chimie de Strasbourg - Laboratoire de Chimie Quantique - Université de Strasbourg /CNRS M2 lecture, Strasbourg, France. Institut
More informationFEAST eigenvalue algorithm and solver: review and perspectives
FEAST eigenvalue algorithm and solver: review and perspectives Eric Polizzi Department of Electrical and Computer Engineering University of Masachusetts, Amherst, USA Sparse Days, CERFACS, June 25, 2012
More informationFirst principle calculations of plutonium and plutonium compounds: part 1
First principle calculations of plutonium and plutonium compounds: part 1 A. B. Shick Institute of Physics ASCR, Prague, CZ Outline: u Lecture 1: Methods of Correlated band theory DFT and DFT+U u Lecture
More informationStatic-scheduling and hybrid-programming in SuperLU DIST on multicore cluster systems
Static-scheduling and hybrid-programming in SuperLU DIST on multicore cluster systems Ichitaro Yamazaki University of Tennessee, Knoxville Xiaoye Sherry Li Lawrence Berkeley National Laboratory MS49: Sparse
More informationHigh pressure core structures of Si nanoparticles for solar energy conversion
High pressure core structures of Si nanoparticles for solar energy conversion S. Wippermann, M. Vörös, D. Rocca, A. Gali, G. Zimanyi, G. Galli [Phys. Rev. Lett. 11, 4684 (213)] NSF/Solar DMR-135468 NISE-project
More informationwoptic: Transport Properties with Wannier Functions and Adaptive k-integration
woptic: Transport Properties with Wannier Functions and Adaptive k-integration Elias Assmann Institute of Solid State Physics, Vienna University of Technology Split, 2013-09-29 About this presentation
More informationCyclops Tensor Framework: reducing communication and eliminating load imbalance in massively parallel contractions
Cyclops Tensor Framework: reducing communication and eliminating load imbalance in massively parallel contractions Edgar Solomonik 1, Devin Matthews 3, Jeff Hammond 4, James Demmel 1,2 1 Department of
More informationAccelerated Quantum Molecular Dynamics
Accelerated Quantum Molecular Dynamics Enrique Martinez, Christian Negre, Marc J. Cawkwell, Danny Perez, Arthur F. Voter and Anders M. N. Niklasson Outline Quantum MD Current approaches Challenges Extended
More informationComputational Nanoscience: Do It Yourself!
John von Neumann Institute for Computing (NIC) Computational Nanoscience: Do It Yourself! edited by Johannes Grotendorst Stefan Blugel Dominik Marx Winter School, 14-22 February 2006 Forschungszentrum
More informationCRYSTAL in parallel: replicated and distributed (MPP) data
CRYSTAL in parallel: replicated and distributed (MPP) data Lorenzo Maschio Dipar0mento di Chimica, Università di Torino lorenzo.maschio@unito.it Several slides courtesy of Roberto Orlando lorenzo.maschio@unito.it
More informationDFT / SIESTA algorithms
DFT / SIESTA algorithms Javier Junquera José M. Soler References http://siesta.icmab.es Documentation Tutorials Atomic units e = m e = =1 atomic mass unit = m e atomic length unit = 1 Bohr = 0.5292 Ang
More informationElectron Correlation
Electron Correlation Levels of QM Theory HΨ=EΨ Born-Oppenheimer approximation Nuclear equation: H n Ψ n =E n Ψ n Electronic equation: H e Ψ e =E e Ψ e Single determinant SCF Semi-empirical methods Correlation
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 informationIntroduction to Hartree-Fock Molecular Orbital Theory
Introduction to Hartree-Fock Molecular Orbital Theory C. David Sherrill School of Chemistry and Biochemistry Georgia Institute of Technology Origins of Mathematical Modeling in Chemistry Plato (ca. 428-347
More informationarxiv: v2 [cond-mat.str-el] 15 May 2008
Many-body Electronic Structure of Metallic α-uranium Athanasios N. Chantis, R. C. Albers, M. D. Jones, Mark van Schilfgaarde, 3 and Takao Kotani 3 Theoretical Division, Los Alamos National Laboratory,
More informationPractical Guide to Density Functional Theory (DFT)
Practical Guide to Density Functional Theory (DFT) Brad Malone, Sadas Shankar Quick recap of where we left off last time BD Malone, S Shankar Therefore there is a direct one-to-one correspondence between
More informationThe Power of FirstPrinciples Simulation
The Power of FirstPrinciples Simulation From electronic structure to real materials Keith Refson Scientific Computing Department STFC Rutherford Appleton Laboratory Computer Simulation Supercomputer Laws
More informationKevin Driver 1 Shuai Zhang 1 Burkhard Militzer 1 R. E. Cohen 2.
Quantum Monte Carlo Simulations of a Single Iron Impurity in MgO Kevin Driver 1 Shuai Zhang 1 Burkhard Militzer 1 R. E. Cohen 2 1 Department of Earth & Planetary Science University of California, Berkeley
More informationwien2wannier and woptic: From Wannier Functions to Optical Conductivity
wien2wannier and woptic: From Wannier Functions to Optical Conductivity Elias Assmann Institute of Solid State Physics, Vienna University of Technology AToMS-2014, Bariloche, Aug 4 Outline brief introduction
More informationIFM Chemistry Computational Chemistry 2010, 7.5 hp LAB2. Computer laboratory exercise 1 (LAB2): Quantum chemical calculations
Computer laboratory exercise 1 (LAB2): Quantum chemical calculations Introduction: The objective of the second computer laboratory exercise is to get acquainted with a program for performing quantum chemical
More informationBand calculations: Theory and Applications
Band calculations: Theory and Applications Lecture 2: Different approximations for the exchange-correlation correlation functional in DFT Local density approximation () Generalized gradient approximation
More informationSome notes on efficient computing and setting up high performance computing environments
Some notes on efficient computing and setting up high performance computing environments Andrew O. Finley Department of Forestry, Michigan State University, Lansing, Michigan. April 17, 2017 1 Efficient
More informationSupporting Information
Supporting Information The Origin of Active Oxygen in a Ternary CuO x /Co 3 O 4 -CeO Catalyst for CO Oxidation Zhigang Liu, *, Zili Wu, *, Xihong Peng, ++ Andrew Binder, Songhai Chai, Sheng Dai *,, School
More informationAll electron optimized effective potential method for solids
All electron optimized effective potential method for solids Institut für Theoretische Physik Freie Universität Berlin, Germany and Fritz Haber Institute of the Max Planck Society, Berlin, Germany. 22
More informationSpeed-up of ATK compared to
What s new @ Speed-up of ATK 2008.10 compared to 2008.02 System Speed-up Memory reduction Azafulleroid (molecule, 97 atoms) 1.1 15% 6x6x6 MgO (bulk, 432 atoms, Gamma point) 3.5 38% 6x6x6 MgO (k-point sampling
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 informationDFT and beyond: Hands-on Tutorial Workshop Tutorial 1: Basics of Electronic Structure Theory
DFT and beyond: Hands-on Tutorial Workshop 2011 Tutorial 1: Basics of Electronic Structure Theory V. Atalla, O. T. Hofmann, S. V. Levchenko Theory Department, Fritz-Haber-Institut der MPG Berlin July 13,
More informationComputational Methods. Chem 561
Computational Methods Chem 561 Lecture Outline 1. Ab initio methods a) HF SCF b) Post-HF methods 2. Density Functional Theory 3. Semiempirical methods 4. Molecular Mechanics Computational Chemistry " Computational
More informationElectronic structure, atomic forces and structural relaxations by WIEN2k
Electronic structure, atomic forces and structural relaxations by WIEN2k Peter Blaha Institute of Materials Chemistry TU Vienna, Austria Outline: APW-based methods (history and state-of-the-art) WIEN2k
More informationParallel Eigensolver Performance on High Performance Computers 1
Parallel Eigensolver Performance on High Performance Computers 1 Andrew Sunderland STFC Daresbury Laboratory, Warrington, UK Abstract Eigenvalue and eigenvector computations arise in a wide range of scientific
More informationMany electrons: Density functional theory Part II. Bedřich Velický VI.
Many electrons: Density functional theory Part II. Bedřich Velický velicky@karlov.mff.cuni.cz VI. NEVF 514 Surface Physics Winter Term 013-014 Troja 1 st November 013 This class is the second devoted to
More informationWRF performance tuning for the Intel Woodcrest Processor
WRF performance tuning for the Intel Woodcrest Processor A. Semenov, T. Kashevarova, P. Mankevich, D. Shkurko, K. Arturov, N. Panov Intel Corp., pr. ak. Lavrentieva 6/1, Novosibirsk, Russia, 630090 {alexander.l.semenov,tamara.p.kashevarova,pavel.v.mankevich,
More informationBefore we start: Important setup of your Computer
Before we start: Important setup of your Computer change directory: cd /afs/ictp/public/shared/smr2475./setup-config.sh logout login again 1 st Tutorial: The Basics of DFT Lydia Nemec and Oliver T. Hofmann
More information2.1 Introduction: The many-body problem
Chapter 2 Smeagol: Density Functional Theory and NEGF s 2.1 Introduction: The many-body problem In solid state physics one is interested in systems comprising many atoms, and consequently many electrons.
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 informationUNMIXING 4-D PTYCHOGRAPHIC IMAGES
UNMIXING 4-D PTYCHOGRAPHIC IMAGES Mentors: Dr. Rick Archibald(ORNL), Dr. Azzam Haidar(UTK), Dr. Stanimire Tomov(UTK), and Dr. Kwai Wong(UTK) PROJECT BY: MICHAELA SHOFFNER(UTK) ZHEN ZHANG(CUHK) HUANLIN
More informationDensity Functional Theory
Density Functional Theory Iain Bethune EPCC ibethune@epcc.ed.ac.uk Overview Background Classical Atomistic Simulation Essential Quantum Mechanics DFT: Approximations and Theory DFT: Implementation using
More informationParallelization of the QC-lib Quantum Computer Simulator Library
Parallelization of the QC-lib Quantum Computer Simulator Library Ian Glendinning and Bernhard Ömer VCPC European Centre for Parallel Computing at Vienna Liechtensteinstraße 22, A-19 Vienna, Austria http://www.vcpc.univie.ac.at/qc/
More informationIntro to ab initio methods
Lecture 2 Part A Intro to ab initio methods Recommended reading: Leach, Chapters 2 & 3 for QM methods For more QM methods: Essentials of Computational Chemistry by C.J. Cramer, Wiley (2002) 1 ab initio
More informationTeoría del Funcional de la Densidad (Density Functional Theory)
Teoría del Funcional de la Densidad (Density Functional Theory) Motivation: limitations of the standard approach based on the wave function. The electronic density n(r) as the key variable: Functionals
More informationHalf-metallicity in Rhodium doped Chromium Phosphide: An ab-initio study
Half-metallicity in Rhodium doped Chromium Phosphide: An ab-initio study B. Amutha 1,*, R. Velavan 1 1 Department of Physics, Bharath Institute of Higher Education and Research (BIHER), Bharath University,
More informationPerformance evaluation of scalable optoelectronics application on large-scale Knights Landing cluster
Performance evaluation of scalable optoelectronics application on large-scale Knights Landing cluster Yuta Hirokawa Graduate School of Systems and Information Engineering, University of Tsukuba hirokawa@hpcs.cs.tsukuba.ac.jp
More informationTime-dependent density functional theory (TDDFT)
Advanced Workshop on High-Performance & High-Throughput Materials Simulations using Quantum ESPRESSO ICTP, Trieste, Italy, January 16 to 27, 2017 Time-dependent density functional theory (TDDFT) Ralph
More informationFast Eigenvalue Solutions
Fast Eigenvalue Solutions Techniques! Steepest Descent/Conjugate Gradient! Davidson/Lanczos! Carr-Parrinello PDF Files will be available Where HF/DFT calculations spend time Guess ρ Form H Diagonalize
More informationFundamentals and applications of Density Functional Theory Astrid Marthinsen PhD candidate, Department of Materials Science and Engineering
Fundamentals and applications of Density Functional Theory Astrid Marthinsen PhD candidate, Department of Materials Science and Engineering Outline PART 1: Fundamentals of Density functional theory (DFT)
More informationDmitrii Nabok Humboldt-Universität zu Berlin. August 8th, 2016
GW@ Dmitrii Nabok Humboldt-Universität zu Berlin August 8th, 2016 Outline Introduction G0W0 approximation Implementation Program workflow Product basis representation Matrix form of GW equations Usage
More informationQ-Chem 4.0: Expanding the Frontiers. Jing Kong Q-Chem Inc. Pittsburgh, PA
Q-Chem 4.0: Expanding the Frontiers Jing Kong Q-Chem Inc. Pittsburgh, PA Q-Chem: Profile Q-Chem is a high performance quantum chemistry program; Contributed by best quantum chemists from 40 universities
More informationOVERVIEW OF QUANTUM CHEMISTRY METHODS
OVERVIEW OF QUANTUM CHEMISTRY METHODS Outline I Generalities Correlation, basis sets Spin II Wavefunction methods Hartree-Fock Configuration interaction Coupled cluster Perturbative methods III Density
More informationPlane waves and pseudopotentials (Part II)
Bristol 2007 Plane waves and pseudopotentials (Part II) X. Gonze Université Catholique de Louvain, Louvain-la-neuve, Belgium Plane Waves - Pseudopotentials, Bristol March 2007 1 In view of practical calculations,
More informationSakurai-Sugiura algorithm based eigenvalue solver for Siesta. Georg Huhs
Sakurai-Sugiura algorithm based eigenvalue solver for Siesta Georg Huhs Motivation Timing analysis for one SCF-loop iteration: left: CNT/Graphene, right: DNA Siesta Specifics High fraction of EVs needed
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 informationCHEM6085: Density Functional Theory Lecture 10
CHEM6085: Density Functional Theory Lecture 10 1) Spin-polarised calculations 2) Geometry optimisation C.-K. Skylaris 1 Unpaired electrons So far we have developed Kohn-Sham DFT for the case of paired
More informationMulti-Scale Modeling from First Principles
m mm Multi-Scale Modeling from First Principles μm nm m mm μm nm space space Predictive modeling and simulations must address all time and Continuum Equations, densityfunctional space scales Rate Equations
More informationJacobi-Based Eigenvalue Solver on GPU. Lung-Sheng Chien, NVIDIA
Jacobi-Based Eigenvalue Solver on GPU Lung-Sheng Chien, NVIDIA lchien@nvidia.com Outline Symmetric eigenvalue solver Experiment Applications Conclusions Symmetric eigenvalue solver The standard form is
More informationTime-dependent density functional theory (TDDFT)
04/05/16 Hands-on workshop and Humboldt-Kolleg: Density-Functional Theory and Beyond - Basic Principles and Modern Insights Isfahan University of Technology, Isfahan, Iran, May 2 to 13, 2016 Time-dependent
More information