Department of Chemistry Chapter 4 continued

Similar documents
Waves and Polarization in General

3. Electromagnetic Waves II

Physics 505 Homework No. 9 Solutions S9-1

11) A thin, uniform rod of mass M is supported by two vertical strings, as shown below.

Electromagnetism Physics 15b

Chapter 2 Classical propagation

Physics 221 Lecture 41 Nonlinear Absorption and Refraction

Qualifying Examination Electricity and Magnetism Solutions January 12, 2006

ECE 6340 Intermediate EM Waves. Fall Prof. David R. Jackson Dept. of ECE. Notes 4

16.1 Permanent magnets

1 Fundamental Solutions to the Wave Equation

As is natural, our Aerospace Structures will be described in a Euclidean three-dimensional space R 3.

Introduction to Accelerator Physics

Vector d is a linear vector function of vector d when the following relationships hold:

3D-Central Force Problems II

Inverse Square Law and Polarization

Physics 2A Chapter 10 - Moment of Inertia Fall 2018

MODULE 5a and 5b (Stewart, Sections 12.2, 12.3) INTRO: In MATH 1114 vectors were written either as rows (a1, a2,..., an) or as columns a 1 a. ...

Physics 506 Winter 2006 Homework Assignment #9 Solutions

Solutions. V in = ρ 0. r 2 + a r 2 + b, where a and b are constants. The potential at the center of the atom has to be finite, so a = 0. r 2 + b.

MAGNETIC FIELD AROUND TWO SEPARATED MAGNETIZING COILS

PROBLEM SET #1 SOLUTIONS by Robert A. DiStasio Jr.

Phys 774: Ellipsometry

Geometry of the homogeneous and isotropic spaces

Module 9: Electromagnetic Waves-I Lecture 9: Electromagnetic Waves-I

Preliminary Exam: Quantum Physics 1/14/2011, 9:00-3:00

EFFECTS OF FRINGING FIELDS ON SINGLE PARTICLE DYNAMICS. M. Bassetti and C. Biscari INFN-LNF, CP 13, Frascati (RM), Italy

Supporting Information Wedge Dyakonov Waves and Dyakonov Plasmons in Topological Insulator Bi 2 Se 3 Probed by Electron Beams

Outline. Classes of polarizing devices Polarization states. Eigen-polarization of crystals. Momentum matching at boundaries Polarization calculations

Phys101 Lectures 30, 31. Wave Motion

The geometric construction of Ewald sphere and Bragg condition:

Appendix A. Appendices. A.1 ɛ ijk and cross products. Vector Operations: δ ij and ɛ ijk

( )( )( ) ( ) + ( ) ( ) ( )

Stress, Cauchy s equation and the Navier-Stokes equations

Velocimetry Techniques and Instrumentation

School of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007

Sources of Magnetic Fields (chap 28)

Physics 2020, Spring 2005 Lab 5 page 1 of 8. Lab 5. Magnetism

Class XII - Physics Wave Optics Chapter-wise Problems. Chapter 10

Paramagnetic spin pumping with microwave magnetic fields

Sources of the Magnetic Field. Moving charges currents Ampere s Law Gauss Law in magnetism Magnetic materials

I. CONSTRUCTION OF THE GREEN S FUNCTION

Physics 121 Hour Exam #5 Solution

FI 3221 ELECTROMAGNETIC INTERACTIONS IN MATTER

Basic Interference and. Classes of of Interferometers

Magnetic field due to a current loop.

Supplementary Figure 1. Circular parallel lamellae grain size as a function of annealing time at 250 C. Error bars represent the 2σ uncertainty in

AP Centripetal Acceleration Lab

EXAM NMR (8N090) November , am

Electromagnetic scattering. Graduate Course Electrical Engineering (Communications) 1 st Semester, Sharif University of Technology

Chapter 3 Optical Systems with Annular Pupils

Physics NYB problem set 5 solution

MOLECULES BONDS. ENERGY LEVELS electronic vibrational rotational. P461 - Molecules 1

Physics 2B Chapter 22 Notes - Magnetic Field Spring 2018

ANTENNAS. Vector and Scalar Potentials. Maxwell's Equations. D = εe. For a linear, homogeneous, isotropic medium µ and ε are contant.

CBN 98-1 Developable constant perimeter surfaces: Application to the end design of a tape-wound quadrupole saddle coil

COORDINATE TRANSFORMATIONS - THE JACOBIAN DETERMINANT

PHZ 3113 Fall 2017 Homework #5, Due Friday, October 13

Three dimensional flow analysis in Axial Flow Compressors

7.2.1 Basic relations for Torsion of Circular Members

Introduction to General Relativity 2

Antennas & Propagation

Homework # 3 Solution Key

Class 2. Lesson 1 Stationary Point Charges and Their Forces. Basic Rules of Electrostatics. Basic Rules of Electrostatics

1.2 Differential cross section

Do not turn over until you are told to do so by the Invigilator.

1 Spherical multipole moments

Question 1: The dipole

Ultrafast effects in 3D Metamaterials

Section 26 The Laws of Rotational Motion

Rydberg-Rydberg Interactions

COLLISIONLESS PLASMA PHYSICS TAKE-HOME EXAM

Multipole Radiation. February 29, The electromagnetic field of an isolated, oscillating source

PHYS 705: Classical Mechanics. Small Oscillations

Chapter 5 Force and Motion

This gives rise to the separable equation dr/r = 2 cot θ dθ which may be integrated to yield r(θ) = R sin 2 θ (3)

F Q E v B MAGNETOSTATICS. Creation of magnetic field B. Effect of B on a moving charge. On moving charges only. Stationary and moving charges

An Exact Solution of Navier Stokes Equation

MATH 417 Homework 3 Instructor: D. Cabrera Due June 30. sin θ v x = v r cos θ v θ r. (b) Then use the Cauchy-Riemann equations in polar coordinates

Appendix B The Relativistic Transformation of Forces

Search for a Critical Electron Temperature Gradient in DIII-D L-mode Discharges

Theme Music: MGMT Electric Feel* Cartoon: Bob Thaves Frank & Ernest

ECE 3318 Applied Electricity and Magnetism. Spring Prof. David R. Jackson Dept. Of ECE. Notes 20 Dielectrics

Electromagnetic Waves

Physics 235 Chapter 5. Chapter 5 Gravitation

Electric field generated by an electric dipole

Today in Physics 218: radiation from moving charges

to point uphill and to be equal to its maximum value, in which case f s, max = μsfn

LINEAR PLATE BENDING

Math Section 4.2 Radians, Arc Length, and Area of a Sector

e.g: If A = i 2 j + k then find A. A = Ax 2 + Ay 2 + Az 2 = ( 2) = 6

PHY 114 A General Physics II 11 AM-12:15 PM TR Olin 101

This brief note explains why the Michel-Levy colour chart for birefringence looks like this...

Lab #9: The Kinematics & Dynamics of. Circular Motion & Rotational Motion

Chapter 22: Electric Fields. 22-1: What is physics? General physics II (22102) Dr. Iyad SAADEDDIN. 22-2: The Electric Field (E)

Quantum Mechanics II

Generalized functions and statistical problems of. orbital mechanics

Micro-bunching: Longitudinal Bunch Profile Measurements at TTF

( ) Make-up Tests. From Last Time. Electric Field Flux. o The Electric Field Flux through a bit of area is

15 Solving the Laplace equation by Fourier method

Transcription:

Chapte 4 continued Chial o not chial esponse functions otational aveages linea and nonlinea signals

Undestanding this

And maybe this

Non-linea signal signal ( ( ( ( f E( tn sf... E( t2 q E( t 0q aveage ove oientations * f ˆ fs s e dψ f ( ψ ( s f q n ( t n ( t ( s 0 2 ( t 2 Incoming fields Sample Polaize defining emitted field (compae NM Detecto

E( t M α L E( t E α e e α E( t α β... { X Y Z} l m... { x y z} Fame Tansfomation Genealization E Polaization of field in lab fame ( χ φ M α ( α χ φ ϑ ϑ α L L L L ( (... ( ( pol n α β γ.. l... γ n n... β 2 Field oientations 2 α 2 m pol l n Tansition dipole in molecula fame m Column index (latin molecule... 2 Tansition dipole components γ l... Aveage ove otation matix elements β α - sinφ sinχ + cosθ cosφ cosχ sinφ cos χ cosφ sin χ cosθ cosφ sinθ sinχ cosφ + sinφ cosθ cosχ -sinφ cosθ sinχ - cosφ cosχ sinφ sinθ cos χ sinθ sin χ sinθ cosθ ow index α (gee fields

D. L. Andews and T. Thiunamachandan J. Chem. Phys. 67 (977 5026-5033 Oientational aveages ae invaiant unde otation of coodinate system Any otationally invaiant tenso can be witten in tems of Konece Deltas and Levi Civita symbols and can be deived fom geneal goup-theoetical aguments Oientational Aveage γ β α α γ β α β γ α β γ 4 4 4 30 l m l m m l l m l l αβγ α β γ 6 αβ α β 3 else if 0 β α αβ γ α γ β β α αβγ αβγ αβγ o if anticyclic if cyclic if 0 Absoption CD OD SHG sum-fequency mixing Photon echo 2D aman

Linea Spectoscopy X Y X b Y ; m E-field Electic dipoleallowed B-field Magnetic and electic dipoleallowed

X Y X b Y ; L L ( X ( X 0 Linea Spectoscopy Y 0 0 Y m m m L L ( ( 0 0 0 YY 0 0 0 0 0 0 X XX X 0 0 0 2 Electic dipoleallowed Magnetic and electic dipoleallowed

Geneal polaization ules Allowed Field polaizations: (ection polaize in X-diection l l l 2 m l lm m l m T 2 3 αβγ γ β α α γ β α β γ α β γ ββγ 4 4 4 30 l m l m m l l m lm T 5.. +.. +.. Coesponding molecula quantities: Absoption SHG sum-fequency mixing Photon echo 2D aman Fluoescence

Allowed Field polaizations: (ection polaize in X-diection Geneal polaization ules Consequences st ode If the sample is isotopic CD and OD ae the only linea signals that could be measued with cossed polaizes. Magnetic dipole inteaction equied. Coesponding molecula quantities: m m CD ( t Y X Sample Polaize defining Detecto OD Optical activity: otation of polaization independent of oientation!

Allowed Field polaizations: (ection polaize in X-diection In isotopic samples thee is no second hamonic geneation (fequency doubling because all fields ae in the same XY plane when they popagate along the same Z axis. 2 ( t 2 ( t Sample Geneal polaization ules Consequences 2nd ode Polaize defining Detecto Coesponding molecula quantities: l l l 2 esonant l 2 χ ( l l Non- esonant Suface-sensitive spectoscopy (not full ot. Symmety!

Allowed Field polaizations: (ection polaize in X-diection In non-collinea sum fequency mixing (fequency doubling 3 fields can be pependicula to each othe Geneal polaization ules Consequences 2nd ode Coesponding molecula quantities: l l 2 esonant l 2 ( t 2 ( t Sample Polaize defining Detecto l χ ( l 2 l Non- esonant

Allowed Field polaizations: (ection polaize in X-diection Geneal polaization ules Consequences 2nd ode Coesponding molecula quantities: In non-collinea sum fequency mixing 3 fields can be pependicula to each othe. No magnetic dipole inteaction needed! l χ l (2 l χ + χ + χ xyz yzx zxy χ χ χ xzy yxz zyx 2 ( t 2 The sample esponse vanishes unless the molecule is chial! ( t Sample Polaize defining Detecto Half - esonant

Chial SFG SPP PSP 2 ( t 2 ection Y vis ω << I ω vis sum X 2 ( t Z I Sample Polaize defining Belin M. A.; Kulaov T. A.; Enst K. H.; Yan L.; Shen Y.. Phys. ev. Lett. 2000 85 4474.

chial bacgound: achial SFG 2 ( t 2 vis ( t I Sample Polaize defining Belin M. A.; Kulaov T. A.; Enst K. H.; Yan L.; Shen Y.. Phys. ev. Lett. 2000 85 4474.

bacgound: achial SFG achial m 2 ( t 2 vis PPP ( t Sample Polaize defining I Belin M. A.; Kulaov T. A.; Enst K. H.; Yan L.; Shen Y.. Phys. ev. Lett. 2000 85 4474.

bacgound: achial SFG achial m 2 ( t 2 vis PPP ( t I Sample Polaize defining Belin M. A.; Kulaov T. A.; Enst K. H.; Yan L.; Shen Y.. Phys. ev. Lett. 2000 85 4474.

What maes the signal chial? Chial signal Achial bacgound ( E ( B m ( E ( E wea stong Fast polaization modulation equied ( E ( E ( E ( E ( E ( B ( ( E E ( t E q wea Bacgound fee ( E ( E ( E ( B m vey wea ( E ( E ( E ( E vey wea stong Fast polaization modulation o filteing equied 4 D

Why cicula polaized light? X ( t Sample Y Polaize defining Tansmitted signal would be vey wee No distinction between enantiomes! m cos( ωt x cos( ωt x + CD sin( ωt On esonance emitted field is phase shifted by +/-90 depending on enantiome y

Why cicula polaized light? Linea polaization cos( ωt x ight-handed cicula cos( ωt x sin( ωt y Destuctive intefeence CDsin( ωt sin( ωt y y X CDsin( ωt y cos( ωt x + sin( ωt y CDsin( ωt + sin( ωt y y Y z Left-handed cicula Constuctive intefeence

Why cicula polaized light? ight-handed cicula cos( ωt x sin( ωt y Destuctive intefeence CD sin( ωt y E sin( ωt y y CD y ± E y y 2 CD 2 + E y 2 ± 2 e( CD E y Without polaize: intefeence E x x cos( ωt geneates CD y sin( ωt E y y cos( ωt CD x cos( ωt intefeence

Field view of optical activity Signal geneation Intefeence

Signal Sign in Chial SFG

Signal Sign in Chial SFG SPP Chial 2nd ode ection SPPS ω0 ω ω 2 ω +ω 2 Achial 3d ode (solvent ( t Static electic field Y Opposite sign fo enantiomes 2 ( t 2 Z Y X Sample X Polaize defining Opposite sign fo opposite static electic fields

Signal Sign in Chial SFG S (2 chial x ± S (3 achial x 2 S (2 chial 2 + S (3 achial 2 ± 2 e( S (2 chial S (3 achial ( t Static electic field Y Opposite sign fo enantiomes 2 ( t 2 Z Y X Sample X Polaize defining Opposite sign fo opposite static electic fields

3d ode chial spectoscopy

3d ode chial spectoscopy signal ( ( ( ( 0 E( tn 0 E( t2 0 B( t m0 aveage ove oientations SSSP 3 ( t 3 ( t 0 2 ( t 2 Incoming fields Sample Polaize defining emitted field (compae NM Detecto

3d ode (chial spectoscopy sign-sensitivity signal ( ( ( ( 0 E( tn 0 E( t2 0 B( t m0 aveage ove oientations SSSP ( t 0 Signal is ovelapped with additional field 3 ( t 3 2 ( t 2 Sample Polaize defining Detecto Incoming fields emitted field (compae NM

B850 B800

Chial pump-pobe spectoscopy signal ( ( ( ( 0 E( tn 0 E( t2 0 B( t m0 aveage ove oientations SSSP pump pobe 3 ( t 3 2 ( t 2 ( t Incoming fields Sample Polaize defining emitted field (compae NM 0 Signal is ovelapped with pobe pulse Detecto

Chial pump-pobe spectoscopy Niezboala C.; Hache F. J. Am. Chem. Soc. 2008 30 2783.

Chial pump-pobe spectoscopy Niezboala C.; Hache F. J. Am. Chem. Soc. 2008 30 2783.

Chial pump-pobe spectoscopy

I pobe λ-selection polaize x etadation (PEM Time-esolved VCD sample visible pump Detecto Cicula pobe L L Delay τ VCD with pump VCD without pump Tansient VCD Bonmain Helbing Opt. Lett. 33 (2008 2086 Xie and Simon 992 (electonic CD

I pobe λ-selection polaize x etadation (PEM Time-esolved VCD sample visible pump Detecto Pobe A Cicula pobe N Cl N Co Cl 0.4 0.2 B A 6 C 32 C -0.3-0.6-0.9 VCD and Absoption change Pobe B 25 OD 0.3 mod 2900 2850 2900 2850 Bonmain Helbing Opt. Lett. 33 (2008 2086 Xie and Simon 992 (electonic CD -00 0 00 Time (ps