EE243 Advanced Electromagnetic Theory Lec # 22 Scattering and Diffraction. Reading: Jackson Chapter 10.1, 10.3, lite on both 10.2 and 10.

Similar documents
E F. and H v. or A r and F r are dual of each other.

Effect of Ground Conductivity on Radiation Pattern of a Dipole Antenna

EE243 Advanced Electromagnetic Theory Lec # 23 Scattering and Diffraction. Reading: Jackson Chapter , lite

School of Electrical Engineering. Lecture 2: Wire Antennas

1. Radiation from an infinitesimal dipole (current element).

FI 3103 Quantum Physics

Hydrogen atom. Energy levels and wave functions Orbital momentum, electron spin and nuclear spin Fine and hyperfine interaction Hydrogen orbitals

Sources. My Friends, the above placed Intro was given at ANTENTOP to Antennas Lectures.

Acoustics and electroacoustics

8 - GRAVITATION Page 1

Aakash. For Class XII Studying / Passed Students. Physics, Chemistry & Mathematics

Molecules and electronic, vibrational and rotational structure

The angle between L and the z-axis is found from

5- Scattering Stationary States

Propagation of Current Waves along Quasi-Periodical Thin-Wire Structures: Accounting of Radiation Losses

Solid state physics. Lecture 3: chemical bonding. Prof. Dr. U. Pietsch

Fourier transforms (Chapter 15) Fourier integrals are generalizations of Fourier series. The series representation

SUPPLEMENTARY INFORMATION

CHAPTER 5 CIRCULAR MOTION

Using Multiwavelength Spectroscopy. Alicia C. Garcia-Lopez

Polarized Transmittance-Reflectance Scatterometry Measurements of 2D Trench Dimensions on Phase-Shift Masks

Q Q N, V, e, Quantum Statistics for Ideal Gas and Black Body Radiation. The Canonical Ensemble

GAUSS PLANETARY EQUATIONS IN A NON-SINGULAR GRAVITATIONAL POTENTIAL

The geometric construction of Ewald sphere and Bragg condition:

International Journal of Scientific & Engineering Research, Volume 7, Issue 9, September ISSN

1 Fundamental Solutions to the Wave Equation

While flying from hot to cold, or high to low, watch out below!

1.2 Differential cross section

(, ) which is a positively sloping curve showing (Y,r) for which the money market is in equilibrium. The P = (1.4)

STATISTICAL MECHANICS OF DIATOMIC GASES

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

GRAVITATION 4) R. max. 2 ..(1) ...(2)

* Meysam Mohammadnia Department of Nuclear Engineering, East Tehran Branch, Islamic Azad University, Tehran, Iran *Author for Correspondence

Free carriers in materials

Lecture Principles of scattering and main concepts.

DIELECTRICS MICROSCOPIC VIEW

PH672 WINTER Problem Set #1. Hint: The tight-binding band function for an fcc crystal is [ ] (a) The tight-binding Hamiltonian (8.

Current Status of Orbit Determination methods in PMO

Physics 505 Electricity and Magnetism Fall 2003 Prof. G. Raithel. Problem Set 7 Maximal score: 25 Points. 1. Jackson, Problem Points.

Advanced Quantum Mechanics

Collisionless Hall-MHD Modeling Near a Magnetic Null. D. J. Strozzi J. J. Ramos MIT Plasma Science and Fusion Center

1.2 Partial Wave Analysis

Differential Kinematics

6.Optical and electronic properties of Low

19 th WIEN2k Workshop Waseda University Tokyo Relativistic effects & Non-collinear magnetism. (WIEN2k / WIENncm)

NEWTON S THEORY OF GRAVITY

CDS 101/110: Lecture 7.1 Loop Analysis of Feedback Systems

Total Wave Function. e i. Wave function above sample is a plane wave: //incident beam

A Study of Generalized Thermoelastic Interaction in an Infinite Fibre-Reinforced Anisotropic Plate Containing a Circular Hole

dt d Chapter 30: 1-Faraday s Law of induction (induced EMF) Chapter 30: 1-Faraday s Law of induction (induced Electromotive Force)

FREQUENCY DETECTION METHOD BASED ON RECURSIVE DFT ALGORITHM

5.61 Fall 2007 Lecture #2 page 1. The DEMISE of CLASSICAL PHYSICS

Objectives. We will also get to know about the wavefunction and its use in developing the concept of the structure of atoms.

1.2 Faraday s law A changing magnetic field induces an electric field. Their relation is given by:

θ θ φ EN2210: Continuum Mechanics Homework 2: Polar and Curvilinear Coordinates, Kinematics Solutions 1. The for the vector i , calculate:

Implementation of RCWA

Shor s Algorithm. Motivation. Why build a classical computer? Why build a quantum computer? Quantum Algorithms. Overview. Shor s factoring algorithm

Lecture 1. time, say t=0, to find the wavefunction at any subsequent time t. This can be carried out by

2. Background Material

Lecture 3.2: Cosets. Matthew Macauley. Department of Mathematical Sciences Clemson University

Physics 202, Lecture 5. Today s Topics. Announcements: Homework #3 on WebAssign by tonight Due (with Homework #2) on 9/24, 10 PM

Lecture 8 February 18, 2010

SME 3033 FINITE ELEMENT METHOD. Bending of Prismatic Beams (Initial notes designed by Dr. Nazri Kamsah)

Roger Pynn. Basic Introduction to Small Angle Scattering

Jackson 3.3 Homework Problem Solution Dr. Christopher S. Baird University of Massachusetts Lowell

Physics 111. Lecture 38 (Walker: ) Phase Change Latent Heat. May 6, The Three Basic Phases of Matter. Solid Liquid Gas

Overview. 1 Recall: continuous-time Markov chains. 2 Transient distribution. 3 Uniformization. 4 Strong and weak bisimulation

FI 2201 Electromagnetism

Chapter 6: Polarization and Crystal Optics

Jackson 4.7 Homework Problem Solution Dr. Christopher S. Baird University of Massachusetts Lowell

Lossy Transmission Lines. EELE 461/561 Digital System Design. Module #7 Lossy Lines. Lossy Transmission Lines. Lossy Transmission Lines

Electron energy in crystal potential

ECE Spring Prof. David R. Jackson ECE Dept. Notes 5

APP-IV Introduction to Astro-Particle Physics. Maarten de Jong

Finite Element Method Modeling for Computational Electromagnetics Development of a Perfectly Matched Layer for Domain Termination

Solution Set #3

u 3 = u 3 (x 1, x 2, x 3 )

3. Electromagnetic Waves II

4.2 Design of Sections for Flexure

Chemistry 342 Spring, The Hydrogen Atom.

Frictional effects, vortex spin-down

Mutual Inductance. If current i 1 is time varying, then the Φ B2 flux is varying and this induces an emf ε 2 in coil 2, the emf is

The Great Wave Hokusai. LO: Recognize physical principles associated with terms in sonar equation.

3.012 Fund of Mat Sci: Bonding Lecture 5/6. Comic strip removed for copyright reasons.

Auxiliary Sources for the Near-to-Far-Field Transformation of Magnetic Near-Field Data

Study on the Classification and Stability of Industry-University- Research Symbiosis Phenomenon: Based on the Logistic Model

Scattering in Three Dimensions

EE 5337 Computational Electromagnetics (CEM) Method of Lines

3.46 PHOTONIC MATERIALS AND DEVICES Lecture 10: LEDs and Optical Amplifiers

0WAVE PROPAGATION IN MATERIAL SPACE

Chapter 5. Control of a Unified Voltage Controller. 5.1 Introduction

Geometrical Analysis of the Worm-Spiral Wheel Frontal Gear

Extinction Ratio and Power Penalty

Basic properties of X- rays and neutrons

Lecture 2: Frequency domain analysis, Phasors. Announcements

Derivation of Electron-Electron Interaction Terms in the Multi-Electron Hamiltonian

BEHAVIOUR OF THE ELECTROMECHANICAL COUPLING FACTOR OF CYLINDER SHAPED PIEZOCERAMICS WITH DIFFERENT ASPECT RATIOS.

ECE theory of the Lamb shift in atomic hydrogen and helium

Q Q N, V, e, Quantum Statistics for Ideal Gas. The Canonical Ensemble 10/12/2009. Physics 4362, Lecture #19. Dr. Peter Kroll

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.

Transcription:

Appid M Fa 6, Nuuth Lctu # V //6 43 Advancd ctomagntic Thoy Lc # Scatting and Diffaction Scatting Fom Sma Obcts Scatting by Sma Dictic and Mtaic Sphs Coction of Scatts Sphica Wav xpansions Scaa Vcto Rading: Jackson Chapt.,.3, it on both. and.4 Copyight 6 Rgnts of Univsity of Caifonia

Appid M Fa 6, Nuuth Lctu # V //6 Ovviw Scatting is simia to adiation but oftn quis simutanousy moding th cation of poaization and cunts fom stimuation by an xtna souc. Sma scatts a tatd by dipo momnts. Intmdiat scatts qui xpansion in many sphica hamonics. Lag scatts can b tatd by appoximation in vaious scaa and vctod diffaction intgas Copyight 6 Rgnts of Univsity of Caifonia

Appid M Fa 6, Nuuth Lctu # V //6 Scatting by Dipos Inducd in Sma Scatts n n Incidnt fid is in diction n and has poaization Thy induc ctic and magntic dipo momnts Scattd fid is in diction n and has poaization Not that fo th fa fid th a two choics fo ach of and but on choic ativ to th pan fomd by n and n Copyight 6 Rgnts of Univsity of Caifonia 3

Appid M Fa 6, Nuuth Lctu # V //6 Scatting by Dipos Inducd in Sma Scatts H p m H sc sc nˆ 4πε iknˆ ˆ n k sc Z x Z inducd _ ctic _ dipo inducd _ magntic _ dipo ik [( nˆ p) n n m / c] Jackson..A Incidnt fids induc ctic and magntic dipo momnts Fa fids fom a thn found fom ths momnts Copyight 6 Rgnts of Univsity of Caifonia 4

Appid M Fa 6, Nuuth Lctu # V //6 Diffntia Scatting Coss Sction dσ dω dσ dω ( nˆ, ˆ; nˆ, ˆ ) ( nˆ, ˆ; nˆ, ˆ ) Z ˆ Z k ( 4πε ) 4 ˆ ˆ sc p + ( nˆ ˆ ) m / c n is in obsvation diction with poaization, whi idnt fux is in diction n with poaization. Dfind as th outgoing pow adiatd p unit soid ang dividd by th idnt pow p unit aa. It is atd to th bistatic coss sction. Thn spciaiz to th cas of th ctic and magntic dipo momnts of sma scatts. Intgating ov both poaizations and a angs givs th ffctiv aa of th scatt Copyight 6 Rgnts of Univsity of Caifonia 5

Copyight 6 Rgnts of Univsity of Caifonia 6 Appid M Fa 6, Nuuth Lctu # V //6 Scatting fom a Sma Dictic Sph Dipo p is in th diction of th idnt fid and qua to th static poaization (sam wight facto and popotiona to voum). Radiation is popotiona th obsvation poaization diction dottd with th idnt poaization. This givs cosθ in on ang and constant in φ. Stngth is 6-th pow of siz (voum squad) and 4-th pow ativ to siz in wavngths. (This xpains th cation of th bu sky succss of hoizontay poaizd sun gasss). Stongst and qua in fowad and backwad dictions. ( ) 6 4 6 4 3 3 8 ˆ ˆ ˆ, ˆ ˆ; ˆ, 4 + Ω Ω + Ω + a k d d d a k n n d d a p ε ε π σ σ ε ε σ ε ε πε Jackson..B p p

Appid M Fa 6, Nuuth Lctu # V //6 Scatting fom a Sma p..c. Sph p m dσ dω 4πε a πa 3 3 ( ) ( ) ( ) 4 6 nˆ, ˆ; nˆ, ˆ k a ˆ ˆ nˆ ˆ nˆ ˆ H Jackson..C p and m Both xist A at ight angs Intf cohnty poduc a + b cosθ typ pattns ow fowad (/3) and high backwad (x) scatting Copyight 6 Rgnts of Univsity of Caifonia 7

Appid M Fa 6, Nuuth Lctu # V //6 dσ dω q F F ( q ) ( q ) ( nˆ, ˆ; nˆ, ˆ ) knˆ knˆ Coction of Scatts iq x i iq ( 4πε ) ( x x ) i k 4 [ p + ( n ) m c] ˆ ˆ ˆ / Assum p and m coctd fo bing insid mdia Sum ov a scatts uding ativ phas masud with spct to idnt diction n and scattd diction n F(q) is N (numb of scatts) in fowad diction and dops quicky to zo xcpt fo cysta stuctus with Bagg ffct. Can b usd to masu ang of intmocua focs that poduc dnsity fuxuations (citica opascnc). Copyight 6 Rgnts of Univsity of Caifonia iq x Jackson..D 8

Appid M Fa 6, Nuuth Lctu # V //6 Scaa Sphica Wav Rpsntation Ψ Ψ h h ( x, ω) f ( ) Y ( θ, φ) [ ] Y ( θ, φ) () () ( ) ( ( x, ω) A h + A h ) (), m, m i + [ ] ( ) ( h ) m m k ik m Soution to scaa wav quation Sphica Hamonics Y m (θ,φ) Radia vaiation dpnds ony on indx m Match bounday conditions on sufac(s) at fixd m Jackson..D Copyight 6 Rgnts of Univsity of Caifonia 9

Appid M Fa 6, Nuuth Lctu # V //6 Scaa Sphica Wav Rpsntation: xamps ik x ik x ik x x 4π x x ik i i ik J ( ) () k h ( k ) Y ( θ, φ ) Y ( θ, φ) Y ( θ, φ ) Y ( θ, φ) 4π J m < m ( + ) J Y ( γ ) Scaa Gn s Function Pan wav in two foms Rpac Numica Gid outsid obct (Mi Mthod) Tansation/otation in coodinat systms Addition Thom fo Sphica Hamonics Sph-Sph intactions > Copyight 6 Rgnts of Univsity of Caifonia m m m ( ) h Jackson 9.6,.3 m Numica Sphica Hamonic xpansion Outsid

Appid M Fa 6, Nuuth Lctu # V //6 L X H g f Vcto Sphica Wav Rpsntation i m ( ) ( θ, φ), m Z a, m A B ( + ) ( θ, φ) (, m) f X a (, m) a k (, m) f X + a (, m) () () ( ) ( ) h () () ( ) ( ) h LY + A + B m m h h g Opato L givs compact notation xpssd in tms of ctic and magntic mutipos Souc and Bounday conditions on sufac at fixd Radia and H componnt on a Sph a adquat Copyight 6 Rgnts of Univsity of Caifonia i k M m M X g Jackson.3 m X m

Appid M Fa 6, Nuuth Lctu # V //6 Vcto Sphica Wav Rpsntation: xamp Jackson.4 Tota fid sum of idnt and scattd xpand scattd fid Outgoing wavs (ony) outsid Both typs but no idint fid insid Rotationay symmtic m + and - (ony) Bounday conditions tan and H tan continuous on bounday of sph Tactab fo Conducting Sph (Mi) Dictic Sph? Usfu fo chcking numica simuatos Copyight 6 Rgnts of Univsity of Caifonia