Electronic Structure Methods



Similar documents
Excitation energies for molecules by Time-Dependent. based on Effective Exact Exchange Kohn-Sham potential

Gravitation. Definition of Weight Revisited. Newton s Law of Universal Gravitation. Newton s Law of Universal Gravitation. Gravitational Field

Basis Sets in Quantum Chemistry C. David Sherrill School of Chemistry and Biochemistry Georgia Institute of Technology

Electric Potential. otherwise to move the object from initial point i to final point f

Perturbation Theory and Celestial Mechanics

Molecular Dynamics. r F. r dt. What is molecular dynamics?

(Semi)Parametric Models vs Nonparametric Models

Efficient Evolutionary Data Mining Algorithms Applied to the Insurance Fraud Prediction

A Coverage Gap Filling Algorithm in Hybrid Sensor Network

Green's function integral equation methods for plasmonic nanostructures

Imperial College London

Keywords: Transportation network, Hazardous materials, Risk index, Routing, Network optimization.

Orbit dynamics and kinematics with full quaternions

A New replenishment Policy in a Two-echelon Inventory System with Stochastic Demand

Drag force acting on a bubble in a cloud of compressible spherical bubbles at large Reynolds numbers

A Novel Lightweight Algorithm for Secure Network Coding

1240 ev nm 2.5 ev. (4) r 2 or mv 2 = ke2

An Algorithm For Factoring Integers

Modeling and computing constrained

The Development of Web Log Mining Based on Improve-K-Means Clustering Analysis

5.74 Introductory Quantum Mechanics II

AREA COVERAGE SIMULATIONS FOR MILLIMETER POINT-TO-MULTIPOINT SYSTEMS USING STATISTICAL MODEL OF BUILDING BLOCKAGE

Mean Molecular Weight

SIMULATION OF THERMAL AND CHEMICAL RELAXATION IN A POST-DISCHARGE AIR CORONA REACTOR

2 r2 θ = r2 t. (3.59) The equal area law is the statement that the term in parentheses,

Additional File 1 - A model-based circular binary segmentation algorithm for the analysis of array CGH data

Order-Degree Curves for Hypergeometric Creative Telescoping

SPEE Recommended Evaluation Practice #6 Definition of Decline Curve Parameters Background:

12.1. FÖRSTER RESONANCE ENERGY TRANSFER

PCA vs. Varimax rotation

The Electric Potential, Electric Potential Energy and Energy Conservation. V = U/q 0. V = U/q 0 = -W/q 0 1V [Volt] =1 Nm/C

Episode 401: Newton s law of universal gravitation

Shielding Equations and Buildup Factors Explained

Simultaneous Detection and Estimation, False Alarm Prediction for a Continuous Family of Signals in Gaussian Noise

RESEARCH ON DUAL-SHAKER SINE VIBRATION CONTROL. Yaoqi FENG 1, Hanping QIU 1. China Academy of Space Technology (CAST)

Time Series Perturbation by Genetic Programming

A PARTICLE-BASED LAGRANGIAN CFD TOOL FOR FREE-SURFACE SIMULATION

PREVENTIVE AND CORRECTIVE SECURITY MARKET MODEL

(a) The centripetal acceleration of a point on the equator of the Earth is given by v2. The velocity of the earth can be found by taking the ratio of

A frequency decomposition time domain model of broadband frequency-dependent absorption: Model II

Lab M4: The Torsional Pendulum and Moment of Inertia

econstor zbw

Security of Full-State Keyed Sponge and Duplex: Applications to Authenticated Encryption

(6)(2) (-6)(-4) (-4)(6) + (-2)(-3) + (4)(3) + (2)(-3) = = 0

The Greedy Method. Introduction. 0/1 Knapsack Problem

The Can-Order Policy for One-Warehouse N-Retailer Inventory System: A Heuristic Approach

International Business Cycles and Exchange Rates

LINES ON BRIESKORN-PHAM SURFACES

Prejudice and the Economics of Discrimination

Vector Calculus: Are you ready? Vectors in 2D and 3D Space: Review

Electric Dipole moments as probes of physics beyond the Standard Model

Time Value of Money. Types of Interest. Compounding and Discounting Single Sums. Page 1. Ch. 6 - The Time Value of Money. The Time Value of Money

Bending Stresses for Simple Shapes

TRUCK ROUTE PLANNING IN NON- STATIONARY STOCHASTIC NETWORKS WITH TIME-WINDOWS AT CUSTOMER LOCATIONS

Vasicek s Model of Distribution of Losses in a Large, Homogeneous Portfolio

Rotation Kinematics, Moment of Inertia, and Torque

Symmetric polynomials and partitions Eugene Mukhin

The OC Curve of Attribute Acceptance Plans

Realistic Image Synthesis

Joint Virtual Machine and Bandwidth Allocation in Software Defined Network (SDN) and Cloud Computing Environments

The force between electric charges. Comparing gravity and the interaction between charges. Coulomb s Law. Forces between two charges

8.5 UNITARY AND HERMITIAN MATRICES. The conjugate transpose of a complex matrix A, denoted by A*, is given by

Chapter 7: Answers to Questions and Problems

Chapter 30: Magnetic Fields Due to Currents

Solutions of the Schrödinger equation for the ground. helium by finite element method

An Introduction to Hartree-Fock Molecular Orbital Theory

Portfolio Loss Distribution

benefit is 2, paid if the policyholder dies within the year, and probability of death within the year is ).

REAL TIME MONITORING OF DISTRIBUTION NETWORKS USING INTERNET BASED PMU. Akanksha Eknath Pachpinde

A DATA MINING APPLICATION IN A STUDENT DATABASE

Magnetic Field and Magnetic Forces. Young and Freedman Chapter 27

7.5. Present Value of an Annuity. Investigate

3.32 In aircraft control systems, an ideal pitch response ( qo) versus a pitch command ( qc) is described by the transfer function

PY1052 Problem Set 8 Autumn 2004 Solutions

SUPPORT VECTOR MACHINE FOR BANDWIDTH ANALYSIS OF SLOTTED MICROSTRIP ANTENNA

An Alternative Way to Measure Private Equity Performance

Support Vector Machines

The LCOE is defined as the energy price ($ per unit of energy output) for which the Net Present Value of the investment is zero.

Multiple stage amplifiers

Voltage ( = Electric Potential )

Mixed Task Scheduling and Resource Allocation Problems

12. Rolling, Torque, and Angular Momentum

Determinants of Borrowing Limits on Credit Cards Shubhasis Dey and Gene Mumy

Formulating & Solving Integer Problems Chapter

LATIN SQUARE DESIGN (LS) -With the Latin Square design you are able to control variation in two directions.


An Integrated Semantically Correct 2.5D Object Oriented TIN. Andreas Koch

University of Maryland Fraternity & Sorority Life Spring 2015 Academic Report

Transcription:

Electonc Stuctue Methods One-electon models e.g., Huckel theoy Semempcal methods e.g., AM, PM3, MNDO Sngle-efeence based ab nto methods Hatee-Fock Petubaton theoy MP, MP3, MP4 Coupled cluste theoy e.g., CCSD(T) Mult-confguatonal based ab nto methods MCSCF and CASSCF (also GVB) MR-MP and CASPT MR-CI Ab Into Methods fo IPs, EAs, exctaton eneges CI sngles (CIS) TDHF EOM and Geens functon methods CC

Densty functonal theoy (DFT)- Combne functonals fo exchange and fo coelaton Local densty appoxmaton (LDA) Pedew-Wang 9 (PW9) Becke-Pedew (BP) BeckeLYP(BLYP) Becke3LYP (B3LYP) Tme dependent DFT (TDDFT) (fo excted states) Hybd methods QM/MM Solvaton models

Why so many methods to solve Hψ = Eψ? Electonc Hamltonan, BO appoxmaton H = Z A + + A j j A B Z AZ R / j s what makes t tough (nonsepaable)!! Hatee-Fock method: Wavefuncton antsymmetzed poduct of obtals In geneal, τ efes to both spatal and spn E = Fo the -electon case Ψ = ϕ τ ) ϕ ( τ ) = [ ϕ ( τ ) ϕ ( τ ) ϕ ( τ ) ϕ ( )] AB Enegy mnmzed vaatonal pncple Ψ H Ψ Ψ Ψ h ϕ = ε ϕ obtals and obtal eneges B (n a.u.) Ψ = φ ( τ ) φ ( τ ) Slate detemnant N N accounts fo ndstngushablty of electons ( τ coodnates Vay obtals to mnmze E, keepng obtals othogonal h Z = A A + ( J K ) ϕ() ϕ() K = d j ϕ() ϕ() j j j J = φ ( ) d j

Chaactestcs Each e - sees aveage chage dstbuton due to othe e -. (It s a mean feld method.) Electon coelaton mssng In-out Left-ght h depends on the obtals one s tyng to solve. Reques an teatve (self-consstent) soluton. Pattonng of Hamltonan H = F + V F = Σh Fφ = ε φ V = Σ(/ j ) - Σ(J -K ) (weake than Σ/j) E HF = <ψ H ψ > = <ψ F ψ > + <ψ V ψ > 0 th ode st ode Note: E not just a sum of obtal eneges (would double count Coulomb nteactons)

Soluton of the HF poblem Intoduce a bass set (usually atomc obtals) Evaluate - and -electon ntegals Geneate an ntal guess fo the MO s Constuct Fock matx Dagonalze new obtals and obtal eneges Rebuld Fock matx + teate (SCF) Stop when specfed convegence cteon met Obsevatons Bute foce (/8)N 4 -el. ntegals χ a( d d ) χb( ) χc( ) χd ( ) Cleve codes - scale as N 3 o weake Can be multple solutons!! These ae nonlnea equatons, and the soluton can depend on the ntal guess o the teatve pocedue mght not convege.

Most QC codes usng GTOs (Gaussans) s e α p ( x, y, z) e α Usually these ae contacted e.g., s = 3 j= c j e α j The contacton coeffs. c j and exponents α j ae fxed and ae dffeent fo each element. The above functon counts as 3 fo the ntegal evaluaton, but only fo the sze of the SCF. Example: 3-G - s (3 pmtves), tght sp ( pmtves), extended s'p' ( pmtve) Conventonal vs. dect SCF Conventonal stoe ntegals Dect compute ntegals on the fly Essental fo bg systems

Some common Gaussan bass sets Bass set H L-Ne Na-A STO-3G s sp 3sp 3-G s 3sp 4s3p 6-3G(d) s 3spd 4s3pd 6-3G(d,p) sp 3spd 4s3pd 6-3G(d,p) 3sp 4s3pd 5s4pd 6-3G(df,pd) 3spd 4s3psf 5s4pdf 6-3++G(d,p) 4sp 5s4pd 6s5pd cc-pvdz sp 3spd 4s3pd cc-pvtz 3spd 4s3pdf 5s4pdf cc-pvqz 4s3pdf 5s4p3dfg 6s5p3dfg aug-cc-pvdz 3sp 4s3pd 5s4pd

Geneal emaks about atom-centeed bass sets Pople bass sets ( ) polazaton functons + dffuse functons anons, polazablty Dunnng coelaton-consstent bass sets Valence double-zeta, tple-zeta, etc. Aug adds one dffuse functon of each angula momentum type aleady n the bass. Cusp condtons Ψ' dscontnous as 0 Neve acheved n a sngle confguatonal wavefuncton Reques vey hgh angula momentum bass functons Also makes t had to satsfy the val theoem <V>/<T> = - Bass set supeposton eo (BSSE) Consde AB A uses functons on B and B uses functons on A to lowe the eneges atfcal enegy loweng at shot dstances. Countepose coecton Lnea dependency poblems Plane-wave bass sets Commonly employed by physcs/mateals scence communty At pesent only used wth DFT methods

Hatee-Fock calculatons The HF potental fo H does not dssocate coectly: E(H, R = nf.) *E(H) H + H + H - + H + σ g = ( L + R) = ( L + R ) + ( LR + H + H RL) σ g, σ u obtals degeneate as R nfnty Solve by usng Ψ = C ϕgϕg + C σ u σ u

LUMO HOMO Closed-shell, S = 0 Open-shell, snglet (S = 0) o tplet (S = ) Open-shell snglet cannot be descbed by HF method!!!! Dadcal HF also not vald