Electromagnetic Properties of Materials Part 2
|
|
- Chester Blake
- 6 years ago
- Views:
Transcription
1 ECE st Century Electromagnetics Instructor: Office: Phone: E Mail: Dr. Raymond C. Rumpf A 337 (915) rcrumpf@utep.edu Lecture #3 Electromagnetic Properties of Materials Part 2 Nonlinear and Anisotropic Materials Lecture 3 1 Lecture Outline Nonlinear materials Anisotropic materials Tensor rotation and unrotation Dispersion relation and index ellipsoids Lecture 3 Slide 2 1
2 Nonlinear Materials Nonlinear Materials All materials are nonlinear; some just have stronger nonlinear behavior than others. For radio frequencies, materials tend to breakdown before they exhibit nonlinear properties. Nonlinear properties are commonly exploited in optics. In general, the polarization of a material is a nonlinear function of the electric field and can be expressed as P E E E e 0 e 0 e Linear response This is what we have done so far. Nonlinear response Lecture 3 Slide 4 2
3 Potential Well Description V is the push required to displace the charge by a distance r. 2 Linear materials have a parabolic potential well. V r This leads to a resonator that oscillates as a perfect sinusoid. r Lecture 3 Slide 5 Potential Well for Nonlinear Materials Nonlinear for large r. This type of resonance does not oscillate as a sinusoid. It can be seen as a series of sinusoids. Linear parabolic region for small r. As bound charges are pushed very hard, the restoring force is no longer linear. This results in anharmonic oscillation. The oscillator is effectively resonating at multiple frequencies at the same time. Lecture 3 Slide 6 3
4 Nonsymmetric Potentials This is a non symmetrical potential and therefore exhibits a preferred direction for polarization. The result is a rectified signal along with potentially other frequency content. DC component Lecture 3 Slide 7 Applications of Nonlinear Materials (1) Materials Ordinary linear materials (2) Materials Rectification can create a DC potential from an optical wave Frequency doubling (second harmonic generation) can make lasers at otherwise impossible wavelengths. Parametric mixing can provide sum and difference frequencies Pockel s effect can introduce birefringence from an applied electric field. Lacks inversion symmetry (3) Materials Kerr effect field dependent dielectric constant Third harmonic generation can generate very short wavelength waves. Raman scattering the mechanical vibration of a molecule can shift the frequency of the wave Brillouin scattering dielectric response changes with applied pressure Two photon absorption two photons are absorbed simultaneously where as a single photon would not be absorbed. Has inversion symmetry Lecture 3 Slide 8 4
5 Anisotropic Materials Anisotropic Materials In some materials, charges are more easily displaced along certain directions. For this reason, the material can become polarized in a direction slightly different than the applied field. In this case, the susceptibility is a tensor quantity. Imagine pushing at an angle against a sliding glass door. The door has a preferred direction for displacement. Real materials are not this dramatic! P E 0 e Isotropic materials are good for simple transmission of electromagnetic waves. Anisotropic materials are good for controlling and manipulating the waves. Lecture 3 Slide 10 5
6 Atomic Scale Picture Charges will oscillate differently in these two directions. Therefore, the susceptibility changes as a function of direction in the lattice. large small Lecture 3 Slide 11 Tensor Relations for Anisotropic Materials The material polarization is now expressed as: Px xx xy xzex Py 0 yx yy yz Ey Pz zx zy zz Ez This is most often treated through a dielectric tensor. r I e The constitutive relation between E and D is then Dx xx xy xz Ex D E y 0 yx yy yz y Dz zx zy zz Ez The dielectric tensor has Hermitian symmetry for the general lossy case. ij * ji This means the field components are no longer independent. But it presents many new possibilities!! Lecture 3 Slide 12 Materials can become polarized in directions that are slightly different than the electric field! 6
7 Principle Axes It is always possible to choose a different coordinate system such that the dielectric tensor becomes diagonal. xˆ yˆ zˆ aˆ bˆ cˆ a, b, and c are called the Principal Axes of the Crystal. a, b, and c are not necessarily at 90 to each other. Da a 0 0 Ea Db 0 0 b 0 Eb Dc 0 0 c Ec Alternative Description: There are only three degrees of freedom for 3D tensors. Numbers can only occur in the off diagonal elements when the tensor is rotated. Lecture 3 Slide 13 Maxwell s Equations with Anisotropic Materials Maxwell s equations remain unchanged. E jb H jd D 0 B 0 The constitutive relations now include tensors D E B H D D x xx xy xz Ex E y yx yy yz y D z zx zy zz E z Lecture 3 Slide 14 7
8 Symmetry and Anisotropy Anisotropy Crystal Symmetry Dielectric Properties Isotropic Cubic Uniaxial Biaxial Hexagonal Tetragonal Monoclinic Triclinic Orthorhombic O O E positive birefringence E E O O negative birefringence a b c a b c Lecture 3 Slide 15 Tensor Rotation and Unrotation 8
9 Definition of a Rotation Matrix b a Rotation matrix [R] is defined as b R a The rotation matrix should not change the amplitude. This implies that [R] is unitary. b a H 1 R R H H RR R R I Lecture 3 17 Derivation of a 2D Rotation Matrix b bx cos sinax b y sin cos a y R a Start with vector a at angle. a a ˆ ˆ xxayy a cos xˆsin yˆ Add angle to rotate the vector b acos xˆsin yˆ Apply trig identities cos cos sinsin xˆ b a sincos cossinyˆ a cos sin ˆ x ay x a cos sin ˆ y ax y Lecture
10 3D Rotation Matrices Rotation matrices for 3D coordinates can be written directly from the previous result. a b b a a b cos 0 sin cos sin 0 Rx 0 cos sin R y R z sin cos 0 0 sin cos sin 0 cos Lecture 3 19 Rotation Matrix that Rotates a Onto b Normalize Vectors a ˆ ˆ b a b a b Algorithm v aˆ bˆ s v i.e. sin ab caˆ bˆ i.e. cos ab 0 v3 v2 v v3 0 v 1 v2 v1 0 1 c 2 s RIv v 2 [R] is such that Ra ˆ bˆ Lecture
11 Tensor Rotation Tensors are rotated in a slightly different manner than vectors. R 1 Rz R z Lecture 3 21 Combinations of Rotations Suppose we wish to first rotate about the x axis by some angle, second rotate about the y axis by some angle, and third rotate about the z axis by some angle. For vectors b R R R z y x a For tensors R 1 R R R R R R 1 1 z y x x y z Lecture
12 Composite Rotation Matrix We can combine multiple rotation matrices into a single composite rotation matrix [R]. R R R R b Ra Tensor rotation using the composite rotation matrix is R 1 y z x R R This equation implies we will rotate first about the x axis, second about the z axis, and third about the y axis. Vector rotation using the composite rotation matrix is Lecture 3 23 Animation of Tensor Rotation Lecture
13 Order of Rotations Matter The order that we multiply the rotation matrices controls the order that the rotations are performed. b Rz45 Ry220 Rx10 a 1. First rotates about the x axis by Second rotates about the y axis by Third rotates about the z axis by 45. In general, we do not get the same result when the order of rotation is changed. R R R R y x x y Lecture 3 25 Numerical Examples (1 of 2) Given: r Rotate about x axis by 20 R x Rotate about y axis by 45 R y Rotate about z axis by 60 R z r r r Lecture
14 Numerical Examples (2 of 2) Given: r Rotate first about x axis by 20 and second about the y axis by 45 R y x R Rotate first about z axis by 60 and second about the y axis by Ry45Rz r Rotate first about x axis by 20, second about the y axis by 45, and third about the z axis by Rz60Ry45Rx Lecture 3 27 r r Tensor Unrotation (1 of 2) A tensor can always be diagonalized along its principle axes. a b c Principle Axes: is along aˆ a is along bˆ b is along cˆ c Convention: But suppose we are given a general nine element tensor. a b c xx xy xz rot yx yy yz zx zy zz How do we determine a, b, c and the principle axes a, b, and c? Lecture
15 Tensor Unrotation (2 of 2) We can relate the original tensor and the rotated tensor through the composite rotation matrix [R]. 1 rot R R We calculate the eigen vectors and eigen values of [ rot ]. rot R is the eigen-vector matrix of rot is the eigen-value matrix of rot Lecture 3 29 Determining Principle Axes (1 of 2) What are the principle axes of [ rot ]? Let s put the original principal axes a, b, and c into a matrix. a x x x P ay by c y az bz c z aˆ b bˆ c cˆ Now let s rotate them according to [R] so they correspond to that of [ rot ]. P R P rot We are not rotating a tensor here so we don t use [R][P][R] -1. Lecture
16 Determining Principle Axes (2 of 2) For the special case of orthorhombic symmetry, the principle axes start off as P aˆ bˆ cˆ [P] is just the identity matrix here. The principle axes of the rotated tensor are then P rot I R R We now have a second interpretation of the eigenvector matrix [R]. These are the principle axes of the rotated tensor (for orthorhombic symmetry). Lecture 3 31 Directly Setting the Principle Axes We may know the orientation that we would like to place our tensor directly in terms of the desired crystal axes a, b, and c. We place these into a matrix and interpret it as the composite rotation matrix. ax bx cx R ay by c y a z bz c z aˆ bˆ cˆ The rotated tensor can be directly calculated from [R]. 1 rot R R Lecture
17 Dispersion Relation & Index Ellipsoids The Wave Vector The wave vector (wave momentum) is a vector quantity that conveys two pieces of information: 1. Wavelength and Refractive Index The magnitude of the wave vector tells us the spatial period (wavelength) of the wave inside the material. When the free space wavelength is known, k conveys the material s refractive index n (more to be said later). 2 2 n k 0 free space wavelength 0 2. Direction The direction of the wave is perpendicular to the wave fronts (more to be said later). k k aˆk bˆ k cˆ a b c Lecture 3 Slide 34 17
18 Dispersion Relations The dispersion relation for a material relates the wave vector to frequency. Essentially, it tells us the refractive index as a function of direction through a material. It is derived by substituting a plane wave solution into the wave equation. For an ordinary linear homogeneous and isotropic (LHI) material, the dispersion relation is: k k k k n a b c 0 This can also be written as: k k k n a b c 2 k Lecture 3 Slide 35 Index Ellipsoids From the previous slide, the dispersion relation for a LHI material was: k k k k n a b c 0 This defines a sphere called an index ellipsoid. The vector connecting the origin to a point on the surface of the sphere is the k vector for that direction. Refractive index is calculated from this. k k n 0 ĉ index ellipsoid For LHI materials, the refractive index is the same in all directions. Think of this as a map of the refractive index as a function of the wave s direction through the medium. â ˆb Lecture 3 Slide 36 18
19 How to Derive the Dispersion Relation (1 of 2) The wave equation in a linear homogeneous anisotropic material is: 2 Ek00rE 0 We are ignoring the magnetic response here. The solution to this equation is still a plane wave, but our allowed values for k (modes) are more complicated. jk r E Ee ˆ ˆ ˆ 0 E0 Ea a Eb b Ec c Substituting this solution into the wave equation leads to the following relation: k k E k E k E 2 r This equation has the form: ˆ aˆ b cˆ 0 Each ( ) term has the form: E E E 0 a b c Each vector component must be set to zero independently. aˆ component: Ea Eb Ec 0 Matrix form bˆ component: Ea Eb Ec 0 cˆ component: Ea Eb Ec 0 Ea E b 0 E c Lecture 3 Slide 37 How to Derive the Dispersion Relation (2 of 2) Solutions for k are the eigen values of the big matrix and derived by setting the determinant to zero. det 0 This leads to the following general equation: k k k 1 k k n k k n k k n a b c a 0 b 0 c It can also be shown that given the wave vector, the polarization of the electric field is: ka kb ˆ kc E ˆ ˆ 0 a b c k k0n a k k0n b k k0n c Lecture 3 Slide 38 19
20 Generalized Dispersion Relation Given the dielectric tensor, 2 a 0 0 n 0 0 a 2 r 0 0 b 0 nb c 0 0 n C The general form of the dispersion relation is: k k k 1 k k n k k n k k n a b c a 0 b 0 c This can be written in a more useful form as: 2 k k k k k k k k k k k k nn nn nn n n n a b c 2 b c a c a b b c a c a b a b c Lecture 3 Slide 39 Dispersion Relation for Uniaxial Crystals Uniaxial crystals have na nb no no ordinary refractive index n n n extraordinary refractive index c E E The general dispersion relation reduces to: ka kb k 2 c ka kb kc 2 k 2 0 k no ne no Sphere Ellipse Ordinary Wave Extraordinary Wave This has two solutions corresponding to the two polarizations (TE and TM). This has two solutions corresponding to the two polarizations (TE and TM). This first solution is the same as for an isotropic material. It acts like it is propagating through a isotropic material with index n O so it is called the ordinary wave. The second solution is an ellipsoid. Depending on its direction, the effective refractive index will be somewhere between n O and n E. Lecture 3 Slide 40 20
21 Index Ellipsoids for Uniaxial Crystals (1 of 2) Ordinary Wave k k k k k k a b c 2 a b c 2 k 2 0 k no ne no Extraordinary Wave k k k a b c 2 k no k k k a b c 2 k ne no n O ne no ne Lecture 3 Slide 41 Index Ellipsoids for Uniaxial Crystals (2 of 2) ne â n O ĉ n O ne n O ˆb Observations Both solutions share a common axis. This common axis looks isotropic with refractive index n 0 regardless of polarization. Since both solutions share a single axis, these crystals are called uniaxial. The common axis is called: o Optic axis o Ordinary axis o C axis o Uniaxial axis Deviation from the optic axis will result in two separate possible modes. Lecture 3 Slide 42 21
22 Dispersion Relation for Biaxial Crystals (1 of 2) Biaxial crystals have all unique refractive indices. Most texts adopt the convention where n n n a b c The general dispersion relation cannot be reduced. ĉ Notes and Observations The convention n a <n b <n c causes the optic axes to lie in the a c plane. optic axes The two solutions can be envisioned as one balloon inside another, pinched together so they touch at only four points. â ˆb Propagation along either of the optic axes looks isotropic, thus the name biaxial. Lecture 3 Slide 43 Dispersion Relation for Biaxial Crystals (2 of 2) There are three special cases when it can be simplified. We can cause these conditions by launching electromagnetic waves at the proper orientation kb k 2 c ka 0: kb kc k0na k nc nb ka kc 2 kb 0: ka kc k0nb k nc na ka kb 2 kc 0: ka kb k0nc k nb na We see that each case has two separate solutions corresponding to the two polarizations (TE and TM). Lecture 3 Slide 44 22
23 Dispersion Surfaces of Magnetoelectric Materials Magnetoelectric materials can exhibit up to 16 singularities. D E H and B H E Alberto Favaro and Friedrich W. Hehl, Light propagation in local and linear media: Fresnel Kummer wave surfaces with 16 singular points, arxiv preprint arxiv: (2015). Lecture 3 Slide 45 Direction of Power Flow Isotropic Materials y P k x Anisotropic Materials y k P x Phase propagates in the direction of k. Therefore, the refractive index derived from k is best described as the phase refractive index. Velocity here is the phase velocity. Energy propagates in the direction of P which is always normal to the surface of the index ellipsoid. From this, we can define a group velocity and a group refractive index. Lecture 3 Slide 46 23
24 Illustration of k versus Raymond C. Rumpf "Engineering the Dispersion and Anisotropy of Periodic Electromagnetic Structures," Solid State Physics, Vol. 66, pp , Negative refraction into a photonic crystal. Lecture 3 Slide 47 Double Refraction in Anisotropic Materials Isotropic Materials y Anisotropic Materials y k 1 x k 1 x k e k 2 k 0 Anisotropic materials have two index ellipsoids one for each polarization. Wave energy can split between the two produce an ordinary and an extraordinary wave. Lecture 3 Slide 48 24
Electromagnetic Waves & Polarization
Course Instructor Dr. Raymond C. Rumpf Office: A 337 Phone: (915) 747 6958 E Mail: rcrumpf@utep.edu EE 4347 Applied Electromagnetics Topic 3a Electromagnetic Waves & Polarization Electromagnetic These
More informationMaxwell s Equations:
Course Instructor Dr. Raymond C. Rumpf Office: A-337 Phone: (915) 747-6958 E-Mail: rcrumpf@utep.edu Maxwell s Equations: Physical Interpretation EE-3321 Electromagnetic Field Theory Outline Maxwell s Equations
More informationEE 5337 Computational Electromagnetics. Preliminary Topics
Instructor Dr. Raymond Rumpf (915) 747 6958 rcrumpf@utep.edu EE 5337 Computational Electromagnetics Lecture #3 Preliminary Topics Lecture 3These notes may contain copyrighted material obtained under fair
More information11/29/2010. Propagation in Anisotropic Media 3. Introduction. Introduction. Gabriel Popescu
Propagation in Anisotropic Media Gabriel Popescu University of Illinois at Urbana Champaign Beckman Institute Quantitative Light Imaging Laboratory http://light.ece.uiuc.edu Principles of Optical Imaging
More informationLecture Outline. Maxwell s Equations Predict Waves Derivation of the Wave Equation Solution to the Wave Equation 8/7/2018
Course Instructor Dr. Raymond C. Rumpf Office: A 337 Phone: (915) 747 6958 E Mail: rcrumpf@utep.edu EE 4347 Applied Electromagnetics Topic 3a Electromagnetic Waves Electromagnetic These notes Waves may
More informationIntroduction to Polarization
Phone: Ext 659, E-mail: hcchui@mail.ncku.edu.tw Fall/007 Introduction to Polarization Text Book: A Yariv and P Yeh, Photonics, Oxford (007) 1.6 Polarization States and Representations (Stokes Parameters
More informationSummary of Fourier Optics
Summary of Fourier Optics Diffraction of the paraxial wave is described by Fresnel diffraction integral, u(x, y, z) = j λz dx 0 dy 0 u 0 (x 0, y 0 )e j(k/2z)[(x x 0) 2 +(y y 0 ) 2 )], Fraunhofer diffraction
More informationLecture 21 Reminder/Introduction to Wave Optics
Lecture 1 Reminder/Introduction to Wave Optics Program: 1. Maxwell s Equations.. Magnetic induction and electric displacement. 3. Origins of the electric permittivity and magnetic permeability. 4. Wave
More informationWaves in Linear Optical Media
1/53 Waves in Linear Optical Media Sergey A. Ponomarenko Dalhousie University c 2009 S. A. Ponomarenko Outline Plane waves in free space. Polarization. Plane waves in linear lossy media. Dispersion relations
More informationChap. 2. Polarization of Optical Waves
Chap. 2. Polarization of Optical Waves 2.1 Polarization States - Direction of the Electric Field Vector : r E = E xˆ + E yˆ E x x y ( ω t kz + ϕ ), E = E ( ωt kz + ϕ ) = E cos 0 x cos x y 0 y - Role :
More informationOptics and Optical Design. Chapter 6: Polarization Optics. Lectures 11-13
Optics and Optical Design Chapter 6: Polarization Optics Lectures 11-13 Cord Arnold / Anne L Huillier Polarization of Light Arbitrary wave vs. paraxial wave One component in x-direction y x z Components
More information4: birefringence and phase matching
/3/7 4: birefringence and phase matching Polarization states in EM Linear anisotropic response χ () tensor and its symmetry properties Working with the index ellipsoid: angle tuning Phase matching in crystals
More informationNonlinear optics: a back-to-basics primer Lecture 1: linear optics
Guoqing (Noah) Chang, October 9, 15 Nonlinear optics: a back-to-basics primer Lecture 1: linear optics 1 Suggested references Robert W. Boyd, Nonlinear optics (8) Geoffrey New, Introduction to nonlinear
More informationNumerical Implementation of Transformation Optics
ECE 5322 21 st Century Electromagnetics Instructor: Office: Phone: E Mail: Dr. Raymond C. Rumpf A 337 (915) 747 6958 rcrumpf@utep.edu Lecture #16b Numerical Implementation of Transformation Optics Lecture
More informationOptics and Optical Design. Chapter 6: Polarization Optics. Lectures 11 13
Optics and Optical Design Chapter 6: Polarization Optics Lectures 11 13 Cord Arnold / Anne L Huillier Polarization of Light Arbitrary wave vs. paraxial wave One component in x direction y x z Components
More informationElectromagnetism II Lecture 7
Electromagnetism II Lecture 7 Instructor: Andrei Sirenko sirenko@njit.edu Spring 13 Thursdays 1 pm 4 pm Spring 13, NJIT 1 Previous Lecture: Conservation Laws Previous Lecture: EM waves Normal incidence
More informationChap. 4. Electromagnetic Propagation in Anisotropic Media
Chap. 4. Electromagnetic Propagation in Anisotropic Media - Optical properties depend on the direction of propagation and the polarization of the light. - Crystals such as calcite, quartz, KDP, and liquid
More informationModern Optics Prof. Partha Roy Chaudhuri Department of Physics Indian Institute of Technology, Kharagpur
Modern Optics Prof. Partha Roy Chaudhuri Department of Physics Indian Institute of Technology, Kharagpur Lecture 08 Wave propagation in anisotropic media Now, we will discuss the propagation of electromagnetic
More informationLecture 5: Polarization. Polarized Light in the Universe. Descriptions of Polarized Light. Polarizers. Retarders. Outline
Lecture 5: Polarization Outline 1 Polarized Light in the Universe 2 Descriptions of Polarized Light 3 Polarizers 4 Retarders Christoph U. Keller, Leiden University, keller@strw.leidenuniv.nl ATI 2016,
More informationWave Propagation in Uniaxial Media. Reflection and Transmission at Interfaces
Lecture 5: Crystal Optics Outline 1 Homogeneous, Anisotropic Media 2 Crystals 3 Plane Waves in Anisotropic Media 4 Wave Propagation in Uniaxial Media 5 Reflection and Transmission at Interfaces Christoph
More informationECE 185 ELECTRO-OPTIC MODULATION OF LIGHT
ECE 185 ELECTRO-OPTIC MODULATION OF LIGHT I. Objective: To study the Pockels electro-optic (EO) effect, and the property of light propagation in anisotropic medium, especially polarization-rotation effects.
More informationLecture Outline. Scattering From a Dielectric Slab Anti Reflection Layer Bragg Gratings 8/9/2018. EE 4347 Applied Electromagnetics.
Course Instructor Dr. Raymond C. Rumpf Office: A 337 Phone: (95) 747 6958 E Mail: rcrumpf@utep.edu EE 4347 Applied Electromagnetics Topic 3k Multiple Scattering Multiple These Scattering notes may contain
More information18. Active polarization control
18. Active polarization control Ways to actively control polarization Pockels' Effect inducing birefringence Kerr Effect Optical Activity Principal axes are circular, not linear Faraday Effect inducing
More informationLecture 3 : Electrooptic effect, optical activity and basics of interference colors with wave plates
Lecture 3 : Electrooptic effect, optical activity and basics of interference colors with wave plates NW optique physique II 1 Electrooptic effect Electrooptic effect: example of a KDP Pockels cell Liquid
More informationLecture #16. Spatial Transforms. Lecture 16 1
ECE 53 1 st Century Electromagnetics Instructor: Office: Phone: E Mail: Dr. Raymond C. Rumpf A 337 (915) 747 6958 rcrumpf@utep.edu Lecture #16 Spatial ransforms Lecture 16 1 Lecture Outline ransformation
More information16. More About Polarization
16. More About Polarization Polarization control Wave plates Circular polarizers Reflection & polarization Scattering & polarization Birefringent materials have more than one refractive index A special
More informationProblem Set 2 Due Tuesday, September 27, ; p : 0. (b) Construct a representation using five d orbitals that sit on the origin as a basis: 1
Problem Set 2 Due Tuesday, September 27, 211 Problems from Carter: Chapter 2: 2a-d,g,h,j 2.6, 2.9; Chapter 3: 1a-d,f,g 3.3, 3.6, 3.7 Additional problems: (1) Consider the D 4 point group and use a coordinate
More informationChapter 9 Electro-Optics
Chapter 9 Electro-Optics Gabriel Popescu University of Illinois at Urbana Champaign Beckman Institute Quantitative Light Imaging Laboratory http://light.ece.uiuc.edu Principles of Optical Imaging Electrical
More informationLecture 4: Anisotropic Media. Dichroism. Optical Activity. Faraday Effect in Transparent Media. Stress Birefringence. Form Birefringence
Lecture 4: Anisotropic Media Outline Dichroism Optical Activity 3 Faraday Effect in Transparent Media 4 Stress Birefringence 5 Form Birefringence 6 Electro-Optics Dichroism some materials exhibit different
More informationBrewster Angle and Total Internal Reflection
Lecture 4: Polarization Outline 1 Polarized Light in the Universe 2 Brewster Angle and Total Internal Reflection 3 Descriptions of Polarized Light 4 Polarizers 5 Retarders Christoph U. Keller, Utrecht
More informationOPTI 501, Electromagnetic Waves (3)
OPTI 501, Electromagnetic Waves (3) Vector fields, Maxwell s equations, electromagnetic field energy, wave equations, free-space solutions, box modes, Fresnel equations, scalar and vector potentials, gauge
More informationLECTURE 3 DIRECT PRODUCTS AND SPECTROSCOPIC SELECTION RULES
SYMMETRY II. J. M. GOICOECHEA. LECTURE 3 1 LECTURE 3 DIRECT PRODUCTS AND SPECTROSCOPIC SELECTION RULES 3.1 Direct products and many electron states Consider the problem of deciding upon the symmetry of
More informationGrading. Class attendance: (1 point/class) x 9 classes = 9 points maximum Homework: (10 points/hw) x 3 HW = 30 points maximum
Grading Class attendance: (1 point/class) x 9 classes = 9 points maximum Homework: (10 points/hw) x 3 HW = 30 points maximum Maximum total = 39 points Pass if total >= 20 points Fail if total
More information(Introduction) Linear Optics and Nonlinear Optics
18. Electro-optics (Introduction) Linear Optics and Nonlinear Optics Linear Optics The optical properties, such as the refractive index and the absorption coefficient are independent of light intensity.
More informationGY 302: Crystallography & Mineralogy
UNIVERSITY OF SOUTH ALABAMA GY 302: Crystallography & Mineralogy Lecture 7a: Optical Mineralogy (two day lecture) Instructor: Dr. Douglas Haywick This Week s Agenda 1. Properties of light 2. Minerals and
More informationTensor Visualization. CSC 7443: Scientific Information Visualization
Tensor Visualization Tensor data A tensor is a multivariate quantity Scalar is a tensor of rank zero s = s(x,y,z) Vector is a tensor of rank one v = (v x,v y,v z ) For a symmetric tensor of rank 2, its
More information3 Constitutive Relations: Macroscopic Properties of Matter
EECS 53 Lecture 3 c Kamal Sarabandi Fall 21 All rights reserved 3 Constitutive Relations: Macroscopic Properties of Matter As shown previously, out of the four Maxwell s equations only the Faraday s and
More informationBrewster Angle and Total Internal Reflection
Lecture 5: Polarization Outline 1 Polarized Light in the Universe 2 Brewster Angle and Total Internal Reflection 3 Descriptions of Polarized Light 4 Polarizers 5 Retarders Christoph U. Keller, Leiden University,
More informationLight matter interaction. Ground state spherical electron cloud. Excited state : 4 quantum numbers n principal (energy)
Light matter interaction Hydrogen atom Ground state spherical electron cloud Excited state : 4 quantum numbers n principal (energy) L angular momentum, 2,3... L L z projection of angular momentum S z projection
More informationChemistry 431. NC State University. Lecture 17. Vibrational Spectroscopy
Chemistry 43 Lecture 7 Vibrational Spectroscopy NC State University The Dipole Moment Expansion The permanent dipole moment of a molecule oscillates about an equilibrium value as the molecule vibrates.
More informationPreliminary Topics in EM
ECE 53 1 st Century Electromagnetics Instructor: Office: Phone: E Mail: Dr. Raymond C. Rumpf A 337 (915) 747 6958 rcrumpf@utep.edu Lecture #1 Preliminary Topics in EM Lecture 1 1 Lecture Outline Maxwell
More informationRotational Raman Spectroscopy
Rotational Raman Spectroscopy If EM radiation falls upon an atom or molecule, it may be absorbed if the energy of the radiation corresponds to the separation of two energy levels of the atoms or molecules.
More informationElectromagnetic Waves Across Interfaces
Lecture 1: Foundations of Optics Outline 1 Electromagnetic Waves 2 Material Properties 3 Electromagnetic Waves Across Interfaces 4 Fresnel Equations 5 Brewster Angle 6 Total Internal Reflection Christoph
More information8. Propagation in Nonlinear Media
8. Propagation in Nonlinear Media 8.. Microscopic Description of Nonlinearity. 8... Anharmonic Oscillator. Use Lorentz model (electrons on a spring) but with nonlinear response, or anharmonic spring d
More informationSynthesizing Geometries for 21st Century Electromagnetics
ECE 5322 21 st Century Electromagnetics Instructor: Office: Phone: E Mail: Dr. Raymond C. Rumpf A 337 (915) 747 6958 rcrumpf@utep.edu Lecture #18b Synthesizing Geometries for 21st Century Electromagnetics
More informationCHAPTER 9 FUNDAMENTAL OPTICAL PROPERTIES OF SOLIDS
CHAPTER 9 FUNDAMENTAL OPTICAL PROPERTIES OF SOLIDS Alan Miller Department of Physics and Astronomy Uni ersity of St. Andrews St. Andrews, Scotland and Center for Research and Education in Optics and Lasers
More informationSummary of Beam Optics
Summary of Beam Optics Gaussian beams, waves with limited spatial extension perpendicular to propagation direction, Gaussian beam is solution of paraxial Helmholtz equation, Gaussian beam has parabolic
More informationChiroptical Spectroscopy
Chiroptical Spectroscopy Theory and Applications in Organic Chemistry Lecture 2: Polarized light Masters Level Class (181 041) Mondays, 8.15-9.45 am, NC 02/99 Wednesdays, 10.15-11.45 am, NC 02/99 28 Electromagnetic
More information3D PRINTING OF ANISOTROPIC METAMATERIALS
Progress In Electromagnetics Research Letters, Vol. 34, 75 82, 2012 3D PRINTING OF ANISOTROPIC METAMATERIALS C. R. Garcia 1, J. Correa 1, D. Espalin 2, J. H. Barton 1, R. C. Rumpf 1, *, R. Wicker 2, and
More informationElectromagnetic Waves
Electromagnetic Waves Our discussion on dynamic electromagnetic field is incomplete. I H E An AC current induces a magnetic field, which is also AC and thus induces an AC electric field. H dl Edl J ds
More informationProblem Set 2 Due Thursday, October 1, & & & & # % (b) Construct a representation using five d orbitals that sit on the origin as a basis:
Problem Set 2 Due Thursday, October 1, 29 Problems from Cotton: Chapter 4: 4.6, 4.7; Chapter 6: 6.2, 6.4, 6.5 Additional problems: (1) Consider the D 3h point group and use a coordinate system wherein
More informationElectromagnetic fields and waves
Electromagnetic fields and waves Maxwell s rainbow Outline Maxwell s equations Plane waves Pulses and group velocity Polarization of light Transmission and reflection at an interface Macroscopic Maxwell
More informationLiquid Crystals IAM-CHOON 1(1100 .,4 WILEY 2007 WILEY-INTERSCIENCE A JOHN WILEY & SONS, INC., PUBLICATION. 'i; Second Edition. n z
Liquid Crystals Second Edition IAM-CHOON 1(1100.,4 z 'i; BICENTCNNIAL 1 8 0 7 WILEY 2007 DICENTENNIAL n z z r WILEY-INTERSCIENCE A JOHN WILEY & SONS, INC., PUBLICATION Contents Preface xiii Chapter 1.
More informationTypical anisotropies introduced by geometry (not everything is spherically symmetric) temperature gradients magnetic fields electrical fields
Lecture 6: Polarimetry 1 Outline 1 Polarized Light in the Universe 2 Fundamentals of Polarized Light 3 Descriptions of Polarized Light Polarized Light in the Universe Polarization indicates anisotropy
More informationLecture 7. Properties of Materials
MIT 3.00 Fall 2002 c W.C Carter 55 Lecture 7 Properties of Materials Last Time Types of Systems and Types of Processes Division of Total Energy into Kinetic, Potential, and Internal Types of Work: Polarization
More informationPhotonic/Plasmonic Structures from Metallic Nanoparticles in a Glass Matrix
Excerpt from the Proceedings of the COMSOL Conference 2008 Hannover Photonic/Plasmonic Structures from Metallic Nanoparticles in a Glass Matrix O.Kiriyenko,1, W.Hergert 1, S.Wackerow 1, M.Beleites 1 and
More informationOPTI 511L Fall A. Demonstrate frequency doubling of a YAG laser (1064 nm -> 532 nm).
R.J. Jones Optical Sciences OPTI 511L Fall 2017 Experiment 3: Second Harmonic Generation (SHG) (1 week lab) In this experiment we produce 0.53 µm (green) light by frequency doubling of a 1.06 µm (infrared)
More informationNumerical Simulation of Nonlinear Electromagnetic Wave Propagation in Nematic Liquid Crystal Cells
Numerical Simulation of Nonlinear Electromagnetic Wave Propagation in Nematic Liquid Crystal Cells N.C. Papanicolaou 1 M.A. Christou 1 A.C. Polycarpou 2 1 Department of Mathematics, University of Nicosia
More informationJones calculus for optical system
2/14/17 Electromagnetic Processes In Dispersive Media, Lecture 6 1 Jones calculus for optical system T. Johnson Key concepts in the course so far What is meant by an electro-magnetic response? What characterises
More information12. Nonlinear optics I
1. Nonlinear optics I What are nonlinear-optical effects and why do they occur? Maxwell's equations in a medium Nonlinear-optical media Second-harmonic generation Conservation laws for photons ("Phasematching")
More informationLecture 8. Stress Strain in Multi-dimension
Lecture 8. Stress Strain in Multi-dimension Module. General Field Equations General Field Equations [] Equilibrium Equations in Elastic bodies xx x y z yx zx f x 0, etc [2] Kinematics xx u x x,etc. [3]
More informationSymmetry. 2-D Symmetry. 2-D Symmetry. Symmetry. EESC 2100: Mineralogy 1. Symmetry Elements 1. Rotation. Symmetry Elements 1. Rotation.
Symmetry a. Two-fold rotation = 30 o /2 rotation a. Two-fold rotation = 30 o /2 rotation Operation Motif = the symbol for a two-fold rotation EESC 2100: Mineralogy 1 a. Two-fold rotation = 30 o /2 rotation
More information+ f f n x n. + (x)
Math 255 - Vector Calculus II Notes 14.5 Divergence, (Grad) and Curl For a vector field in R n, that is F = f 1, f 2,..., f n, where f i is a function of x 1, x 2,..., x n, the divergence is div(f) = f
More informationElectromagnetic Wave Propagation Lecture 8: Propagation in birefringent media
Electromagnetic Wave Propagation Lecture 8: Propagation in birefringent media Daniel Sjöberg Department of Electrical and Information Technology September 27, 2012 Outline 1 Introduction 2 Maxwell s equations
More informationLecture Outline. Scattering at an Interface Sunrises & Sunsets Rainbows Polarized Sunglasses 8/9/2018. EE 4347 Applied Electromagnetics.
Course Instructor Dr. Raymond C. Rumpf Office: A 337 Phone: (915) 747 6958 E Mail: rcrumpf@utep.edu EE 4347 Applied Electromagnetics Topic 3i Scattering at an Interface: Examples Examples These notes may
More informationPOLARISATION. We have not really discussed the direction of the Electric field other that that it is perpendicular to the direction of motion.
POLARISATION Light is a transverse electromagnetic wave. We have not really discussed the direction of the Electric field other that that it is perpendicular to the direction of motion. If the E field
More informationMicroscopic-Macroscopic connection. Silvana Botti
relating experiment and theory European Theoretical Spectroscopy Facility (ETSF) CNRS - Laboratoire des Solides Irradiés Ecole Polytechnique, Palaiseau - France Temporary Address: Centre for Computational
More informationRotational Motion. Chapter 4. P. J. Grandinetti. Sep. 1, Chem P. J. Grandinetti (Chem. 4300) Rotational Motion Sep.
Rotational Motion Chapter 4 P. J. Grandinetti Chem. 4300 Sep. 1, 2017 P. J. Grandinetti (Chem. 4300) Rotational Motion Sep. 1, 2017 1 / 76 Angular Momentum The angular momentum of a particle with respect
More informationPhysics 742 Graduate Quantum Mechanics 2 Midterm Exam, Spring [15 points] A spinless particle in three dimensions has potential 2 2 2
Physics 74 Graduate Quantum Mechanics Midterm Exam, Spring 4 [5 points] A spinless particle in three dimensions has potential V A X Y Z BXYZ Consider the unitary rotation operator R which cyclically permutes
More informationChiroptical Spectroscopy
Chiroptical Spectroscopy Theory and Applications in Organic Chemistry Lecture 3: (Crash course in) Theory of optical activity Masters Level Class (181 041) Mondays, 8.15-9.45 am, NC 02/99 Wednesdays, 10.15-11.45
More informationRotational motion of a rigid body spinning around a rotational axis ˆn;
Physics 106a, Caltech 15 November, 2018 Lecture 14: Rotations The motion of solid bodies So far, we have been studying the motion of point particles, which are essentially just translational. Bodies with
More informationChem8028(1314) - Spin Dynamics: Spin Interactions
Chem8028(1314) - Spin Dynamics: Spin Interactions Malcolm Levitt see also IK m106 1 Nuclear spin interactions (diamagnetic materials) 2 Chemical Shift 3 Direct dipole-dipole coupling 4 J-coupling 5 Nuclear
More informationModern Optics Prof. Partha Roy Chaudhuri Department of Physics Indian Institute of Technology, Kharagpur
Modern Optics Prof. Partha Roy Chaudhuri Department of Physics Indian Institute of Technology, Kharagpur Lecture 09 Wave propagation in anisotropic media (Contd.) So, we have seen the various aspects of
More informationChapter 6. Polarization Optics
Chapter 6. Polarization Optics 6.1 Polarization of light 6. Reflection and refraction 6.3 Optics of anisotropic media 6.4 Optical activity and magneto-optics 6.5 Optics of liquid crystals 6.6 Polarization
More informationCSE 167: Introduction to Computer Graphics Lecture #2: Linear Algebra Primer
CSE 167: Introduction to Computer Graphics Lecture #2: Linear Algebra Primer Jürgen P. Schulze, Ph.D. University of California, San Diego Fall Quarter 2016 Announcements Monday October 3: Discussion Assignment
More informationLeft-handed materials: Transfer matrix method studies
Left-handed materials: Transfer matrix method studies Peter Markos and C. M. Soukoulis Outline of Talk What are Metamaterials? An Example: Left-handed Materials Results of the transfer matrix method Negative
More informationLagrange Multipliers
Optimization with Constraints As long as algebra and geometry have been separated, their progress have been slow and their uses limited; but when these two sciences have been united, they have lent each
More informationMaxwell s Equations:
Course Instructor Dr. Raymond C. Rumpf Office: A-337 Phone: (915) 747-6958 E-Mail: rcrumpf@utep.edu Maxwell s Equations: Terms & Definitions EE-3321 Electromagnetic Field Theory Outline Maxwell s Equations
More informationIf the symmetry axes of a uniform symmetric body coincide with the coordinate axes, the products of inertia (Ixy etc.
Prof. O. B. Wright, Autumn 007 Mechanics Lecture 9 More on rigid bodies, coupled vibrations Principal axes of the inertia tensor If the symmetry axes of a uniform symmetric body coincide with the coordinate
More informationTheoretische Physik 2: Elektrodynamik (Prof. A-S. Smith) Home assignment 9
WiSe 202 20.2.202 Prof. Dr. A-S. Smith Dipl.-Phys. Ellen Fischermeier Dipl.-Phys. Matthias Saba am Lehrstuhl für Theoretische Physik I Department für Physik Friedrich-Alexander-Universität Erlangen-Nürnberg
More informationNon-linear Optics III (Phase-matching & frequency conversion)
Non-linear Optics III (Phase-matching & frequency conversion) P.E.G. Baird MT 011 Phase matching In lecture, equation gave an expression for the intensity of the second harmonic generated in a non-centrosymmetric
More informationpolarisation of Light
Basic concepts to understand polarisation of Light Polarization of Light Nature of light: light waves are transverse in nature i. e. the waves propagates in a direction perpendicular to the direction of
More informationFORTH. Essential electromagnetism for photonic metamaterials. Maria Kafesaki. Foundation for Research & Technology, Hellas, Greece (FORTH)
FORTH Essential electromagnetism for photonic metamaterials Maria Kafesaki Foundation for Research & Technology, Hellas, Greece (FORTH) Photonic metamaterials Metamaterials: Man-made structured materials
More informationCSE 167: Introduction to Computer Graphics Lecture #2: Linear Algebra Primer
CSE 167: Introduction to Computer Graphics Lecture #2: Linear Algebra Primer Jürgen P. Schulze, Ph.D. University of California, San Diego Spring Quarter 2016 Announcements Project 1 due next Friday at
More informationAbsorption suppression in photonic crystals
PHYSICAL REVIEW B 77, 442 28 Absorption suppression in photonic crystals A. Figotin and I. Vitebskiy Department of Mathematics, University of California at Irvine, Irvine, California 92697, USA Received
More informationOmm Al-Qura University Dr. Abdulsalam Ai LECTURE OUTLINE CHAPTER 3. Vectors in Physics
LECTURE OUTLINE CHAPTER 3 Vectors in Physics 3-1 Scalars Versus Vectors Scalar a numerical value (number with units). May be positive or negative. Examples: temperature, speed, height, and mass. Vector
More informationLinear Algebra. Chapter 8: Eigenvalues: Further Applications and Computations Section 8.2. Applications to Geometry Proofs of Theorems.
Linear Algebra Chapter 8: Eigenvalues: Further Applications and Computations Section 8.2. Applications to Geometry Proofs of Theorems May 1, 2018 () Linear Algebra May 1, 2018 1 / 8 Table of contents 1
More informationPolarimetry in the E-ELT era. Polarized Light in the Universe. Descriptions of Polarized Light. Polarizers. Retarders. Fundamentals of Polarized Light
Polarimetry in the E-ELT era Fundamentals of Polarized Light 1 Polarized Light in the Universe 2 Descriptions of Polarized Light 3 Polarizers 4 Retarders Christoph U. Keller, Leiden University, keller@strw.leidenuniv.nl
More information2.4 Properties of the nonlinear susceptibilities
2.4 Properties of the nonlinear susceptibilities 2.4.1 Physical fields are real 2.4.2 Permutation symmetry numbering 1 to n arbitrary use symmetric definition 1 2.4.3 Symmetry for lossless media two additional
More informationUniformity of the Universe
Outline Universe is homogenous and isotropic Spacetime metrics Friedmann-Walker-Robertson metric Number of numbers needed to specify a physical quantity. Energy-momentum tensor Energy-momentum tensor of
More informationPolarization of Light and Birefringence of Materials
Polarization of Light and Birefringence of Materials Ajit Balagopal (Team Members Karunanand Ogirala, Hui Shen) ECE 614- PHOTONIC INFORMATION PROCESSING LABORATORY Abstract-- In this project, we study
More informationMechanics of Earthquakes and Faulting
Mechanics of Earthquakes and Faulting www.geosc.psu.edu/courses/geosc508 Surface and body forces Tensors, Mohr circles. Theoretical strength of materials Defects Stress concentrations Griffith failure
More informationTechnische Universität Graz. Institute of Solid State Physics. 22. Crystal Physics
Technische Universität Graz Institute of Solid State Physics 22. Crystal Physics Jan. 7, 2018 Hall effect / Nerst effect Technische Universität Graz Institute of Solid State Physics Crystal Physics Crystal
More informationCrystal Relaxation, Elasticity, and Lattice Dynamics
http://exciting-code.org Crystal Relaxation, Elasticity, and Lattice Dynamics Pasquale Pavone Humboldt-Universität zu Berlin http://exciting-code.org PART I: Structure Optimization Pasquale Pavone Humboldt-Universität
More informationApplied Nonlinear Optics. David C. Hutchings Dept. of Electronics and Electrical Engineering University of Glasgow
Applied Nonlinear Optics David C. Hutchings Dept. of Electronics and Electrical Engineering University of Glasgow ii Preface This course will cover aspects of birefringence, the electro-optic effect and
More information6.730 Physics for Solid State Applications
6.730 Physics for Solid State Applications Lecture 5: Specific Heat of Lattice Waves Outline Review Lecture 4 3-D Elastic Continuum 3-D Lattice Waves Lattice Density of Modes Specific Heat of Lattice Specific
More informationPEAT SEISMOLOGY Lecture 2: Continuum mechanics
PEAT8002 - SEISMOLOGY Lecture 2: Continuum mechanics Nick Rawlinson Research School of Earth Sciences Australian National University Strain Strain is the formal description of the change in shape of a
More informationOPTI510R: Photonics. Khanh Kieu College of Optical Sciences, University of Arizona Meinel building R.626
OPTI510R: Photonics Khanh Kieu College of Optical Sciences, University of Arizona kkieu@optics.arizona.edu Meinel building R.626 Important announcements Homework #2 is due Feb. 12 Mid-term exam Feb 28
More informationLayer-Inversion Zones in Angular Distributions of Luminescence and Absorption Properties in Biaxial Crystals
Materials 2010, 3, 2474-2482; doi:10.3390/ma3042474 Article OPEN ACCESS materials ISSN 1996-1944 www.mdpi.com/jonal/materials Layer-Inversion Zones in Angular Distributions of Luminescence and Absorption
More informationLight for which the orientation of the electric field is constant although its magnitude and sign vary in time.
L e c t u r e 8 1 Polarization Polarized light Light for which the orientation of the electric field is constant although its magnitude and sign vary in time. Imagine two harmonic, linearly polarized light
More information