Born-Oppenheimer Approximation and Nonadiabatic Effects. Hans Lischka University of Vienna

Similar documents
Technical Report: Bessel Filter Analysis

Math 7409 Homework 2 Fall from which we can calculate the cycle index of the action of S 5 on pairs of vertices as

Prof. Dr. I. Nasser atomic and molecular physics -551 (T-112) February 20, 2012 Spin_orbit.doc. The Fine Structure of the Hydrogen Atom

Quantum Mechanics Lecture Notes 10 April 2007 Meg Noah

= 5! 3! 2! = 5! 3! (5 3)!. In general, the number of different groups of r items out of n items (when the order is ignored) is given by n!

Chapter 8 Complex Numbers

Relation (12.1) states that if two points belong to the convex subset Ω then all the points on the connecting line also belong to Ω.

Supplementary materials. Suzuki reaction: mechanistic multiplicity versus exclusive homogeneous or exclusive heterogeneous catalysis

physicsandmathstutor.com

2012 GCE A Level H2 Maths Solution Paper Let x,

Office: JILA A709; Phone ;

Electron states in a periodic potential. Assume the electrons do not interact with each other. Solve the single electron Schrodinger equation: KJ =

Lecture 2: Stress. 1. Forces Surface Forces and Body Forces

Strong Result for Level Crossings of Random Polynomials

AB-INITIO SIMULATIONS IN MATERIALS SCIENCE

Strong Result for Level Crossings of Random Polynomials. Dipty Rani Dhal, Dr. P. K. Mishra. Department of Mathematics, CET, BPUT, BBSR, ODISHA, INDIA

Magnetic symmetry of the plain domain walls. in ferro- and ferrimagnets

Zeros of Polynomials

Multi-Electron Atoms-Helium

Masses and orbits of minor planets with the GAIA mission

Using Difference Equations to Generalize Results for Periodic Nested Radicals

Appendix: The Laplace Transform

REFLECTION AND REFRACTION

Advanced Physical Geodesy

1 Adiabatic and diabatic representations

physicsandmathstutor.com

5.80 Small-Molecule Spectroscopy and Dynamics

3.2 Properties of Division 3.3 Zeros of Polynomials 3.4 Complex and Rational Zeros of Polynomials

Theory of Periodic Systems Based on the All-Electron DFT FP-LAPW Method Applications to Surfaces and Clusters

Ch 3.4 Binomial Coefficients. Pascal's Identit y and Triangle. Chapter 3.2 & 3.4. South China University of Technology

De Moivre s Theorem - ALL

THE ANALYTIC LARGE SIEVE

a) The average (mean) of the two fractions is halfway between them: b) The answer is yes. Assume without loss of generality that p < r.

ECE Spring Prof. David R. Jackson ECE Dept. Notes 20

By the end of this section you will be able to prove the Chinese Remainder Theorem apply this theorem to solve simultaneous linear congruences

Cylindrical quantum well of finite depth in external magnetic field.

The Pigeonhole Principle 3.4 Binomial Coefficients

KEY. Math 334 Midterm II Fall 2007 section 004 Instructor: Scott Glasgow

Orthogonal transformations

Multivector Functions

Announcements: The Rydberg formula describes. A Hydrogen-like ion is an ion that

OVERVIEW OF THE COMBINATORICS FUNCTION TECHNIQUE

Question 1: The magnetic case

On a Problem of Littlewood

Solutions to Homework 1

Recursion. Algorithm : Design & Analysis [3]

( ) 1 Comparison Functions. α is strictly increasing since ( r) ( r ) α = for any positive real number c. = 0. It is said to belong to

Phys 6303 Final Exam Solutions December 19, 2012

ANSWERS, HINTS & SOLUTIONS HALF COURSE TEST VII (Main)

Module II: Part A. Optical Fibers

PARTIAL DIFFERENTIAL EQUATIONS SEPARATION OF VARIABLES

ATOMIC STRUCTURE EXERCISE # 1

Using Counting Techniques to Determine Probabilities

ON CERTAIN CLASS OF ANALYTIC FUNCTIONS

Complex Numbers Solutions

1. Using Einstein Summation notation, prove the identity: = A

On ARMA(1,q) models with bounded and periodically correlated solutions

Green Functions. January 12, and the Dirac delta function. 1 x x

PAPER : IIT-JAM 2010

Lecture 6: October 16, 2017

UNIVERSITY OF CALIFORNIA - SANTA CRUZ DEPARTMENT OF PHYSICS PHYS 116C. Problem Set 4. Benjamin Stahl. November 6, 2014

2-D Raster Graphics. Graphics Pipeline. Conversion to. Conversion. to Pixel Values. Pixel Values

Properties and Tests of Zeros of Polynomial Functions

MATH /19: problems for supervision in week 08 SOLUTIONS

CHAPTER 5. Theory and Solution Using Matrix Techniques

Applications of the Dirac Sequences in Electrodynamics

LESSON 15: COMPOUND INTEREST

MATH Midterm Solutions

Castiel, Supernatural, Season 6, Episode 18

Calculation of Matrix Elements in the Foldy-Wouthuysen Representation

Disjoint Sets { 9} { 1} { 11} Disjoint Sets (cont) Operations. Disjoint Sets (cont) Disjoint Sets (cont) n elements

Lacunary Almost Summability in Certain Linear Topological Spaces

CHAPTER 5 : SERIES. 5.2 The Sum of a Series Sum of Power of n Positive Integers Sum of Series of Partial Fraction Difference Method

Range Symmetric Matrices in Minkowski Space

PROBLEM SET I (Suggested Solutions)

1. Szabo & Ostlund: 2.1, 2.2, 2.4, 2.5, 2.7. These problems are fairly straightforward and I will not discuss them here.

FIXED POINT AND HYERS-ULAM-RASSIAS STABILITY OF A QUADRATIC FUNCTIONAL EQUATION IN BANACH SPACES

International Journal of Mathematical Archive-3(5), 2012, Available online through ISSN

Mapping Radius of Regular Function and Center of Convex Region. Duan Wenxi

Flight and Orbital Mechanics. Exams

Math 113 Exam 4 Practice

Solutions of the D-dimensional Schrödinger equation with the Hyperbolic Pöschl Teller potential plus modified ring shaped term

n 3 ln n n ln n is convergent by p-series for p = 2 > 1. n2 Therefore we can apply Limit Comparison Test to determine lutely convergent.

Minimization of the quadratic test function

EDEXCEL NATIONAL CERTIFICATE UNIT 28 FURTHER MATHEMATICS FOR TECHNICIANS OUTCOME 2- ALGEBRAIC TECHNIQUES TUTORIAL 1 - PROGRESSIONS

Reccurent sequenses in solving the Schrödinger equation

The Gamma function. Marco Bonvini. October 9, dt e t t z 1. (1) Γ(z + 1) = z Γ(z) : (2) = e t t z. + z dt e t t z 1. = z Γ(z).

Let us give one more example of MLE. Example 3. The uniform distribution U[0, θ] on the interval [0, θ] has p.d.f.

Chapter 4 Postulates & General Principles of Quantum Mechanics

Review Questions, Chapters 8, 9. f(y) = 0, elsewhere. F (y) = f Y(1) = n ( e y/θ) n 1 1 θ e y/θ = n θ e yn

Lesson 10: Limits and Continuity

6.003 Homework #3 Solutions

Fourier Series and their Applications

Chapter 4 : Laplace Transform

Chapter 4. Fourier Series

ALGEBRAIC GEOMETRY COURSE NOTES, LECTURE 5: SINGULARITIES.

Discussion 02 Solutions

Chapter 7: The z-transform. Chih-Wei Liu

Lecture 19. Curve fitting I. 1 Introduction. 2 Fitting a constant to measured data

Special Modeling Techniques

Transcription:

Bo-Oppeheie Appoxiatio ad Noadiabatic Effects Has Lischa Uivesity of Viea

Typical situatio. Fac-Codo excitatio fo the iiu of the goud state. Covetioal dyaics possibly M* ad TS 3. Coical itesectio fuel apid adiatioless tasitio to the goud state 4. Covetioal dyaics i the goud state leadig to P ad/o P F. Beadi M. Olivucci ad M. A. obb Che. Soc. ev. 996 3.

Coical Itesectios The itesectio space ca epeset a lage stuctual vaiatio seach fo selected poits e.g. iia o the cossig sea MXS eactio paths dyaics Gaavelli Beadi Olivucci Veve Klei Celai ad obb Faaday Discuss. 0 5 998 Ceba Beadi Olivucci ad Gaavelli JACS 6 608 004 3

Coical Itesectios Degees of Feedo J. v. Neua ud E. Wige Physi. Zeitschift XXX 467 99 How ay degees of feedo ae ecessay i ode to achieve degeeacy of two states? Coside a geeal eal syetic atix ad cout the ube of degees of feedo i case of o degeeacy ad with oe degeeacy: Two geoetical paaetes eed to be used i ode to achieve a degeeacy itesectio. 4

No-cossig ule Assuptio: Eigefuctios fo all but two states ae ow: ϕ ϕ Ψ 3 Ψ. Ψ c ϕ c ϕ H E H c H H E c Coditio fo degeeacy: H - H 0 H 0 No-cossig ule: Fo a diatoic olecule AB oly oe paaete AB is available. Siultaeous fulfillet of both equatios is ot possible except oe coditio H 0 is fulfilled autoatically by syety. 5 0

6 G. Hezbeg ud H.C. Loguett-Higgis Disc. Faaday Soc. 35 77 963 Lieaized odel close to a coical itesectio 0 c c E x W ly ly E x W y l x x W E ± Double coe

Pola coodiates: x cosθ ly si θ x l y Fo the lowe oot: E W x - i.e. c c si θ cosθ cosθ si θ si θ c cos θ c cosθ ta si θ θ Whe Ψ eal the c θ si c Movig oce aoud the oigi θ: 0 π chages the sig of the wave fuctio Bey phase M.V. Bey Poc.. Soc. Lodo A 39 45 984 θ cos 0 7

Bo-Oppeheie Appoxiatio ad Noadiabatic Couplig Total Hailtoia H Tel TN V Electoic Hailtoia fo fixed uclei H el T el V Electoic Schödige equatio el el H E 0 Total Schödige equatio H E Ψ 0 Expasio of the total wave fuctio Ψ M. Bo K. Huag Dyaical Theoy of Cystal Lattices Claedo Oxfod 956 Appedix VIII 8

9 Δ N M T Kietic eegy of the uclei Δ Δ M T N Multiplicatio fo the left with ad itegatio ove electoic coodiates gives: Δ Δ M T

0 Fial esult P C E E T el N B P A M C P A P B

ca be chose as eal. The 0 d i A The Schödige equatio ca be witte as follows: N P C E U T 0 el B M E U Neglectig the couplig eleets C leads to the adiabatic appoxiatio with 0 E U T N

Divisio of iteal coodiates x ad x descibe the coical itesectio x 3 x descibe the eaiig coodiates The plae x x defies the bachig space degeeacy is lifted except at oigi Alog the hypelie i the --diesioal space itesectio space the eegies of the two states ae degeeate x ad x ae always pepedicula to the itesectio space

Noadiabatic Couplig at CI level f x Ψ J / xψi f x ci x csf f f x f ci x I J E E J x I c H c CSF Fo E I E J 0 the f ci te will doiate x epesets a uclea coodiate B. H. Legsfield III P. Saxe ad D.. Yaoy J. Phys. Che. 8 4549 984 3

Itesectio-adapted Coodiates g h E E C t J I x H x C J I I ode to descibe the coe at we eed the gadiets ad the oadiabatic couplig vecto 4

s Aalytic epesetatio of the Coe ˆ s G J G I g G J G x g / g g g ; y h / h h Topogaphic paaetes ˆ s ˆ ˆ I h g h / x s x y s y Δgh d g gh d gh h E Δ s x x s y y ± d gh y / gh x y x. 5

Miiu o the Cossig Sea Pojected gadiet techique: M. J. Beapa M. A. obb ad H. B. Schlegel Che. Phys. Lett. 3 69 994 Lagage ultiplie appoach: M.. Maaa ad D.. Yaoy J. Che. Phys. 99 55 993 6