Accelerating Performance and Scalability with NVIDIA Gpus on HPC Applications
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Accessing the Accuracy of Density Functional Theory Through Structure
This is an open access article published under a Creative Commons Attribution (CC-BY) License, which permits unrestricted use, distribution and reproduction in any medium, provided the author and source are cited. Letter Cite This: J. Phys. Chem. Lett. 2019, 10, 4914−4919 pubs.acs.org/JPCL Accessing the Accuracy of Density Functional Theory through Structure and Dynamics of the Water−Air Interface † # ‡ # § ‡ § ∥ Tatsuhiko Ohto, , Mayank Dodia, , Jianhang Xu, Sho Imoto, Fujie Tang, Frederik Zysk, ∥ ⊥ ∇ ‡ § ‡ Thomas D. Kühne, Yasuteru Shigeta, , Mischa Bonn, Xifan Wu, and Yuki Nagata*, † Graduate School of Engineering Science, Osaka University, 1-3 Machikaneyama, Toyonaka, Osaka 560-8531, Japan ‡ Max Planck Institute for Polymer Research, Ackermannweg 10, 55128 Mainz, Germany § Department of Physics, Temple University, Philadelphia, Pennsylvania 19122, United States ∥ Dynamics of Condensed Matter and Center for Sustainable Systems Design, Chair of Theoretical Chemistry, University of Paderborn, Warburger Strasse 100, 33098 Paderborn, Germany ⊥ Graduate School of Pure and Applied Sciences, University of Tsukuba, Tennodai 1-1-1, Tsukuba, Ibaraki 305-8571, Japan ∇ Center for Computational Sciences, University of Tsukuba, 1-1-1 Tennodai, Tsukuba, Ibaraki 305-8577, Japan *S Supporting Information ABSTRACT: Density functional theory-based molecular dynamics simulations are increasingly being used for simulating aqueous interfaces. Nonetheless, the choice of the appropriate density functional, critically affecting the outcome of the simulation, has remained arbitrary. Here, we assess the performance of various exchange−correlation (XC) functionals, based on the metrics relevant to sum-frequency generation spectroscopy. The structure and dynamics of water at the water−air interface are governed by heterogeneous intermolecular interactions, thereby providing a critical benchmark for XC functionals. -
Density Functional Theory
Density Functional Approach Francesco Sottile Ecole Polytechnique, Palaiseau - France European Theoretical Spectroscopy Facility (ETSF) 22 October 2010 Density Functional Theory 1. Any observable of a quantum system can be obtained from the density of the system alone. < O >= O[n] Hohenberg, P. and W. Kohn, 1964, Phys. Rev. 136, B864 Density Functional Theory 1. Any observable of a quantum system can be obtained from the density of the system alone. < O >= O[n] 2. The density of an interacting-particles system can be calculated as the density of an auxiliary system of non-interacting particles. Hohenberg, P. and W. Kohn, 1964, Phys. Rev. 136, B864 Kohn, W. and L. Sham, 1965, Phys. Rev. 140, A1133 Density Functional ... Why ? Basic ideas of DFT Importance of the density Example: atom of Nitrogen (7 electron) 1. Any observable of a quantum Ψ(r1; ::; r7) 21 coordinates system can be obtained from 10 entries/coordinate ) 1021 entries the density of the system alone. 8 bytes/entry ) 8 · 1021 bytes 4:7 × 109 bytes/DVD ) 2 × 1012 DVDs 2. The density of an interacting-particles system can be calculated as the density of an auxiliary system of non-interacting particles. Density Functional ... Why ? Density Functional ... Why ? Density Functional ... Why ? Basic ideas of DFT Importance of the density Example: atom of Oxygen (8 electron) 1. Any (ground-state) observable Ψ(r1; ::; r8) 24 coordinates of a quantum system can be 24 obtained from the density of the 10 entries/coordinate ) 10 entries 8 bytes/entry ) 8 · 1024 bytes system alone. 5 · 109 bytes/DVD ) 1015 DVDs 2. -
Octopus: a First-Principles Tool for Excited Electron-Ion Dynamics
octopus: a first-principles tool for excited electron-ion dynamics. ¡ Miguel A. L. Marques a, Alberto Castro b ¡ a c, George F. Bertsch c and Angel Rubio a aDepartamento de F´ısica de Materiales, Facultad de Qu´ımicas, Universidad del Pa´ıs Vasco, Centro Mixto CSIC-UPV/EHU and Donostia International Physics Center (DIPC), 20080 San Sebastian,´ Spain bDepartamento de F´ısica Teorica,´ Universidad de Valladolid, E-47011 Valladolid, Spain cPhysics Department and Institute for Nuclear Theory, University of Washington, Seattle WA 98195 USA Abstract We present a computer package aimed at the simulation of the electron-ion dynamics of finite systems, both in one and three dimensions, under the influence of time-dependent electromagnetic fields. The electronic degrees of freedom are treated quantum mechani- cally within the time-dependent Kohn-Sham formalism, while the ions are handled classi- cally. All quantities are expanded in a regular mesh in real space, and the simulations are performed in real time. Although not optimized for that purpose, the program is also able to obtain static properties like ground-state geometries, or static polarizabilities. The method employed proved quite reliable and general, and has been successfully used to calculate linear and non-linear absorption spectra, harmonic spectra, laser induced fragmentation, etc. of a variety of systems, from small clusters to medium sized quantum dots. Key words: Electronic structure, time-dependent, density-functional theory, non-linear optics, response functions PACS: 33.20.-t, 78.67.-n, 82.53.-k PROGRAM SUMMARY Title of program: octopus Catalogue identifier: Program obtainable from: CPC Program Library, Queen’s University of Belfast, N. -
1-DFT Introduction
MBPT and TDDFT Theory and Tools for Electronic-Optical Properties Calculations in Material Science Dott.ssa Letizia Chiodo Nano-bio Spectroscopy Group & ETSF - European Theoretical Spectroscopy Facility, Dipartemento de Física de Materiales, Facultad de Químicas, Universidad del País Vasco UPV/EHU, San Sebastián-Donostia, Spain Outline of the Lectures • Many Body Problem • DFT elements; examples • DFT drawbacks • excited properties: electronic and optical spectroscopies. elements of theory • Many Body Perturbation Theory: GW • codes, examples of GW calculations • Many Body Perturbation Theory: BSE • codes, examples of BSE calculations • Time Dependent DFT • codes, examples of TDDFT calculations • state of the art, open problems Main References theory • P. Hohenberg & W. Kohn, Phys. Rev. 136 (1964) B864; W. Kohn & L. J. Sham, Phys. Rev. 140 , A1133 (1965); (Nobel Prize in Chemistry1998) • Richard M. Martin, Electronic Structure: Basic Theory and Practical Methods, Cambridge University Press, 2004 • M. C. Payne, Rev. Mod. Phys.64 , 1045 (1992) • E. Runge and E.K.U. Gross, Phys. Rev. Lett. 52 (1984) 997 • M. A. L.Marques, C. A. Ullrich, F. Nogueira, A. Rubio, K. Burke, E. K. U. Gross, Time-Dependent Density Functional Theory. (Springer-Verlag, 2006). • L. Hedin, Phys. Rev. 139 , A796 (1965) • R.W. Godby, M. Schluter, L. J. Sham. Phys. Rev. B 37 , 10159 (1988) • G. Onida, L. Reining, A. Rubio, Rev. Mod. Phys. 74 , 601 (2002) codes & tutorials • Q-Espresso, http://www.pwscf.org/ • Abinit, http://www.abinit.org/ • Yambo, http://www.yambo-code.org • Octopus, http://www.tddft.org/programs/octopus more info at http://www.etsf.eu, www.nanobio.ehu.es Outline of the Lectures • Many Body Problem • DFT elements; examples • DFT drawbacks • excited properties: electronic and optical spectroscopies. -
The CECAM Electronic Structure Library and the Modular Software Development Paradigm
The CECAM electronic structure library and the modular software development paradigm Cite as: J. Chem. Phys. 153, 024117 (2020); https://doi.org/10.1063/5.0012901 Submitted: 06 May 2020 . Accepted: 08 June 2020 . Published Online: 13 July 2020 Micael J. T. Oliveira , Nick Papior , Yann Pouillon , Volker Blum , Emilio Artacho , Damien Caliste , Fabiano Corsetti , Stefano de Gironcoli , Alin M. Elena , Alberto García , Víctor M. García-Suárez , Luigi Genovese , William P. Huhn , Georg Huhs , Sebastian Kokott , Emine Küçükbenli , Ask H. Larsen , Alfio Lazzaro , Irina V. Lebedeva , Yingzhou Li , David López- Durán , Pablo López-Tarifa , Martin Lüders , Miguel A. L. Marques , Jan Minar , Stephan Mohr , Arash A. Mostofi , Alan O’Cais , Mike C. Payne, Thomas Ruh, Daniel G. A. Smith , José M. Soler , David A. Strubbe , Nicolas Tancogne-Dejean , Dominic Tildesley, Marc Torrent , and Victor Wen-zhe Yu COLLECTIONS Paper published as part of the special topic on Electronic Structure Software Note: This article is part of the JCP Special Topic on Electronic Structure Software. This paper was selected as Featured ARTICLES YOU MAY BE INTERESTED IN Recent developments in the PySCF program package The Journal of Chemical Physics 153, 024109 (2020); https://doi.org/10.1063/5.0006074 An open-source coding paradigm for electronic structure calculations Scilight 2020, 291101 (2020); https://doi.org/10.1063/10.0001593 Siesta: Recent developments and applications The Journal of Chemical Physics 152, 204108 (2020); https://doi.org/10.1063/5.0005077 J. Chem. Phys. 153, 024117 (2020); https://doi.org/10.1063/5.0012901 153, 024117 © 2020 Author(s). The Journal ARTICLE of Chemical Physics scitation.org/journal/jcp The CECAM electronic structure library and the modular software development paradigm Cite as: J. -
Application Profiling at the HPCAC High Performance Center Pak Lui 157 Applications Best Practices Published
Best Practices: Application Profiling at the HPCAC High Performance Center Pak Lui 157 Applications Best Practices Published • Abaqus • COSMO • HPCC • Nekbone • RFD tNavigator • ABySS • CP2K • HPCG • NEMO • SNAP • AcuSolve • CPMD • HYCOM • NWChem • SPECFEM3D • Amber • Dacapo • ICON • Octopus • STAR-CCM+ • AMG • Desmond • Lattice QCD • OpenAtom • STAR-CD • AMR • DL-POLY • LAMMPS • OpenFOAM • VASP • ANSYS CFX • Eclipse • LS-DYNA • OpenMX • WRF • ANSYS Fluent • FLOW-3D • miniFE • OptiStruct • ANSYS Mechanical• GADGET-2 • MILC • PAM-CRASH / VPS • BQCD • Graph500 • MSC Nastran • PARATEC • BSMBench • GROMACS • MR Bayes • Pretty Fast Analysis • CAM-SE • Himeno • MM5 • PFLOTRAN • CCSM 4.0 • HIT3D • MPQC • Quantum ESPRESSO • CESM • HOOMD-blue • NAMD • RADIOSS For more information, visit: http://www.hpcadvisorycouncil.com/best_practices.php 2 35 Applications Installation Best Practices Published • Adaptive Mesh Refinement (AMR) • ESI PAM-CRASH / VPS 2013.1 • NEMO • Amber (for GPU/CUDA) • GADGET-2 • NWChem • Amber (for CPU) • GROMACS 5.1.2 • Octopus • ANSYS Fluent 15.0.7 • GROMACS 4.5.4 • OpenFOAM • ANSYS Fluent 17.1 • GROMACS 5.0.4 (GPU/CUDA) • OpenMX • BQCD • Himeno • PyFR • CASTEP 16.1 • HOOMD Blue • Quantum ESPRESSO 4.1.2 • CESM • LAMMPS • Quantum ESPRESSO 5.1.1 • CP2K • LAMMPS-KOKKOS • Quantum ESPRESSO 5.3.0 • CPMD • LS-DYNA • WRF 3.2.1 • DL-POLY 4 • MrBayes • WRF 3.8 • ESI PAM-CRASH 2015.1 • NAMD For more information, visit: http://www.hpcadvisorycouncil.com/subgroups_hpc_works.php 3 HPC Advisory Council HPC Center HPE Apollo 6000 HPE ProLiant -
The CECAM Electronic Structure Library and the Modular Software Development Paradigm
The CECAM electronic structure library and the modular software development paradigm Cite as: J. Chem. Phys. 153, 024117 (2020); https://doi.org/10.1063/5.0012901 Submitted: 06 May 2020 . Accepted: 08 June 2020 . Published Online: 13 July 2020 Micael J. T. Oliveira, Nick Papior, Yann Pouillon, Volker Blum, Emilio Artacho, Damien Caliste, Fabiano Corsetti, Stefano de Gironcoli, Alin M. Elena, Alberto García, Víctor M. García-Suárez, Luigi Genovese, William P. Huhn, Georg Huhs, Sebastian Kokott, Emine Küçükbenli, Ask H. Larsen, Alfio Lazzaro, Irina V. Lebedeva, Yingzhou Li, David López-Durán, Pablo López-Tarifa, Martin Lüders, Miguel A. L. Marques, Jan Minar, Stephan Mohr, Arash A. Mostofi, Alan O’Cais, Mike C. Payne, Thomas Ruh, Daniel G. A. Smith, José M. Soler, David A. Strubbe, Nicolas Tancogne-Dejean, Dominic Tildesley, Marc Torrent, and Victor Wen-zhe Yu COLLECTIONS Paper published as part of the special topic on Electronic Structure SoftwareESS2020 This paper was selected as Featured This paper was selected as Scilight ARTICLES YOU MAY BE INTERESTED IN Recent developments in the PySCF program package The Journal of Chemical Physics 153, 024109 (2020); https://doi.org/10.1063/5.0006074 Electronic structure software The Journal of Chemical Physics 153, 070401 (2020); https://doi.org/10.1063/5.0023185 Siesta: Recent developments and applications The Journal of Chemical Physics 152, 204108 (2020); https://doi.org/10.1063/5.0005077 J. Chem. Phys. 153, 024117 (2020); https://doi.org/10.1063/5.0012901 153, 024117 © 2020 Author(s). The Journal ARTICLE of Chemical Physics scitation.org/journal/jcp The CECAM electronic structure library and the modular software development paradigm Cite as: J. -
Lawrence Berkeley National Laboratory Recent Work
Lawrence Berkeley National Laboratory Recent Work Title From NWChem to NWChemEx: Evolving with the Computational Chemistry Landscape. Permalink https://escholarship.org/uc/item/4sm897jh Journal Chemical reviews, 121(8) ISSN 0009-2665 Authors Kowalski, Karol Bair, Raymond Bauman, Nicholas P et al. Publication Date 2021-04-01 DOI 10.1021/acs.chemrev.0c00998 Peer reviewed eScholarship.org Powered by the California Digital Library University of California From NWChem to NWChemEx: Evolving with the computational chemistry landscape Karol Kowalski,y Raymond Bair,z Nicholas P. Bauman,y Jeffery S. Boschen,{ Eric J. Bylaska,y Jeff Daily,y Wibe A. de Jong,x Thom Dunning, Jr,y Niranjan Govind,y Robert J. Harrison,k Murat Keçeli,z Kristopher Keipert,? Sriram Krishnamoorthy,y Suraj Kumar,y Erdal Mutlu,y Bruce Palmer,y Ajay Panyala,y Bo Peng,y Ryan M. Richard,{ T. P. Straatsma,# Peter Sushko,y Edward F. Valeev,@ Marat Valiev,y Hubertus J. J. van Dam,4 Jonathan M. Waldrop,{ David B. Williams-Young,x Chao Yang,x Marcin Zalewski,y and Theresa L. Windus*,r yPacific Northwest National Laboratory, Richland, WA 99352 zArgonne National Laboratory, Lemont, IL 60439 {Ames Laboratory, Ames, IA 50011 xLawrence Berkeley National Laboratory, Berkeley, 94720 kInstitute for Advanced Computational Science, Stony Brook University, Stony Brook, NY 11794 ?NVIDIA Inc, previously Argonne National Laboratory, Lemont, IL 60439 #National Center for Computational Sciences, Oak Ridge National Laboratory, Oak Ridge, TN 37831-6373 @Department of Chemistry, Virginia Tech, Blacksburg, VA 24061 4Brookhaven National Laboratory, Upton, NY 11973 rDepartment of Chemistry, Iowa State University and Ames Laboratory, Ames, IA 50011 E-mail: [email protected] 1 Abstract Since the advent of the first computers, chemists have been at the forefront of using computers to understand and solve complex chemical problems. -
Quantum Chemical Calculations of NMR Parameters
Quantum Chemical Calculations of NMR Parameters Tatyana Polenova University of Delaware Newark, DE Winter School on Biomolecular NMR January 20-25, 2008 Stowe, Vermont OUTLINE INTRODUCTION Relating NMR parameters to geometric and electronic structure Classical calculations of EFG tensors Molecular properties from quantum chemical calculations Quantum chemistry methods DENSITY FUNCTIONAL THEORY FOR CALCULATIONS OF NMR PARAMETERS Introduction to DFT Software Practical examples Tutorial RELATING NMR OBSERVABLES TO MOLECULAR STRUCTURE NMR Spectrum NMR Parameters Local geometry Chemical structure (reactivity) I. Calculation of experimental NMR parameters Find unique solution to CQ, Q, , , , , II. Theoretical prediction of fine structure constants from molecular geometry Classical electrostatic model (EFG)- only in simple ionic compounds Quantum mechanical calculations (Density Functional Theory) (EFG, CSA) ELECTRIC FIELD GRADIENT (EFG) TENSOR: POINT CHARGE MODEL EFG TENSOR IS DETERMINED BY THE COMBINED ELECTRONIC AND NUCLEAR WAVEFUNCTION, NO ANALYTICAL EXPRESSION IN THE GENERAL CASE THE SIMPLEST APPROXIMATION: CLASSICAL POINT CHARGE MODEL n Zie 4 V2,k = 3 Y2,k ()i,i i=1 di 5 ATOMS CONTRIBUTING TO THE EFG TENSOR ARE TREATED AS POINT CHARGES, THE RESULTING EFG TENSOR IS THE SUM WITH RESPECT TO ALL ATOMS VERY CRUDE MODEL, WORKS QUANTITATIVELY ONLY IN SIMPLEST IONIC SYSTEMS, BUT YIELDS QUALITATIVE TRENDS AND GENERAL UNDERSTANDING OF THE SYMMETRY AND MAGNITUDE OF THE EXPECTED TENSOR ELECTRIC FIELD GRADIENT (EFG) TENSOR: POINT CHARGE MODEL n Zie 4 V2,k = 3 Y2,k ()i,i i=1 di 5 Ze V = ; V = 0; V = 0 2,0 d 3 2,±1 2,±2 2Ze V = ; V = 0; V = 0 2,0 d 3 2,±1 2,±2 3 Ze V = ; V = 0; V = 0 2,0 2 d 3 2,±1 2,±2 V2,0 = 0; V2,±1 = 0; V2,±2 = 0 MOLECULAR PROPERTIES FROM QUANTUM CHEMICAL CALCULATIONS H = E See for example M. -
The Soul Is an Octopus the Soul and the Ancient Ideas Body an Is O Life of Octopus
THE SOUL IS AN OCTOPUS ANCIENT IDEAS OF LIFE AND THE THE SOUL IS AN OCTOPUS AN IS SOUL THE BODY THE SOUL IS AN OCTOPUS Berliner Medizinhistorisches MuseuM der charité excellence cluster topoi THE SOUL IS AN OCTOPUS ANCIENT IDEAS OF LIFE AND THE BODY edited By uta KornMeier With contriButions By sean coughlin philip van der eijK ricardo julião uta KornMeier giouli KoroBili orly leWis thoMas schnalKe chiara thuMiger and illustrations By christoph geiger Preface 7 gerd grashoff, Michael Meyer Mapping Body and Soul. The Making of an Exhibition 9 philip van der eijK, thoMas schnalKe, uta KornMeier BODY, SOUL AND LIFE IN ANCIENT MEDICINE 16 philip van der eijK DISSECTION AS A METHOD OF DISCOVERY 24 orly leWis LOCALISING THE SOUL IN THE BODY 30 orly leWis BRAIN AND HEART AS ORGANS OF THE SOUL 36 orly leWis SUBSTANCES IN SERVICE OF THE SOUL 44 orly leWis PHYSIOLOGY OF PERCEPTION 52 sean coughlin REPRODUCTION AND THE SOUL 62 sean coughlin NUTRITION, LIFE AND HEALTH OF THE ENSOULED BODY 68 giouli KoroBili MOVEMENT AS A SIGN OF LIFE 76 ricardo julião DISEASES OF THE SOUL, INSANITY AND MENTAL HEALTH 84 chiara thuMiger On Textual and Material Sources of Ancient Medicine 99 philip van der eijK, uta KornMeier Appendix Chronological Table of Authors and Schools 110 Glossary 112 Catalogue of Images 117 References to Ancient Texts 121 Ancient Texts: Editions and Translations Used 125 Select Bibliography 128 Short Biographies Exhibition Team 132 Acknowledgements 134 Imprint 135 Preface It is always a challenge for scholars to convey historical and philosophical ideas and concepts to the broader public. -
Stochastic Quantum Molecular Dynamics for Finite and Extended
Stochastic quantum molecular dynamics for finite and extended systems Heiko Appela,b,c,∗, Massimiliano Di Ventrab aFritz-Haber-Institut der Max-Planck-Gesellschaft, Faradayweg 4-6, D-14195 Berlin, Germany bUniversity of California San Diego, La Jolla, California 92093, USA cEuropean Theoretical Spectroscopy Facility Abstract We present a detailed account of the technical aspects of stochastic quantum molecular dynamics, an ap- proach introduced recently by the authors [H. Appel and M. Di Ventra, Phys. Rev. B 80 212303 (2009)] to describe coupled electron-ion dynamics in open quantum systems. As example applications of the method we consider both finite systems with and without ionic motion, as well as describe its applicability to extended systems in the limit of classical ions. The latter formulation allows the study of important phenomena such as decoherence and energy relaxation in bulk systems and surfaces in the presence of time-dependent fields. 1. Introduction the measurement apparatus itself which necessarily projects non-unitarily the state of the system onto Time-dependent density-functional theory states of the observables. This is generally true for (TDDFT) calculations in the linear-response both electrons and ions, so that a first-principles limit are currently enjoying a large popularity description of their coupled dynamics in the presence due to their efficiency and success in describing of one or more environments is of fundamental low-lying excitation energies in molecular systems importance in order to describe phenomena and [1]. Beyond linear-response, many applications have compare with experiments. At this point, it is worth been investigated with TDDFT. Examples include noting that present quantum molecular dynamics electronic transport [2, 3, 4, 5], nonlinear optical (QMD) approaches, (e.g., the Born-Oppenheimer, response [6], or atoms and molecules in strong laser Ehrenfest or Car-Parrinello methods) either do not fields [7, 8]. -
Cdt-2019-Day2
SBM CDT 2019 Computational Module Day 2 Dr Fernanda Duarte Department of Chemistry, University of Oxford http://fduartegroup.org 1 Workplan Tuesday Wednesday Friday 9:00-10:00 Lecture 2 Lecture 3* 10:30-12:00 Lecture 1 Project Work Project Work 14:00- 17:00 Lab session Project Work Presentations Lab session Project Work Presentations 2 Outline (Lecture 2) •Day 1 •The good side: Applications of DFT in Chemistry •The other side …. Challenges in DFT modelling •A bit more on Functionals and Basis sets !3 !3 Computational Chemistry Why should you care? Hˆ = Hˆ + Hˆ HEˆ Y = Y Born-Oppenheimer Approximation N e Y =y ey N ElectronicTheory Schrödinger Equation Modelling ˆ Hey e = Eey e 2 electrons electrons nuclei electrons ˆ -! 2 Z A 1 Hei= ååååÑ- + 2m iiAijrRiA- < rrij- Kinetic energy Coulomb attraction Electronic repulsion (nuclei-electrons) Experiments Synthesis Kinetics spectroscopy “Artificial Intelligence will not replace chemists. But chemists who doesn’t use (AI) will be replace by those who do” Willem Van Hoorn 4 Computational Chemistry What is - and why is it relevant? Which System Do I Have? What Do You Want to Compute (and Why)? Which Model /Method Should I Choose? Verify Approach (vs. Experiment) Interpret/Analyse 5 Computational Chemistry Which System Do I Have? 10 atoms – organic molecule – singlet 6 Computational Chemistry What Do I Want to Compute (and Why)? Asymmetric Induction via 1,2-Addition to Carbonyl Compounds Conformations for the starting material and TS Which product is preferred? What is the molecular origin of such