16. Dielectrics / Metals

Size: px
Start display at page:

Download "16. Dielectrics / Metals"

Transcription

1 Technische Universität Graz Institute of Solid State Physics 16. Dielectrics / Metals Nov. 26, 2018

2 Dielectrics Dielectrics used as electrical insulators should not conduct. Large breakdown field. Low AC losses. Sometimes a low dielectric constant is desired (CMOS interconnects) Sometimes a high dielectric constant is desired (supercapacitors).

3 Breakdown field Typically V/cm

4 AC losses - loss tangent In an ideal capacitor, current leads voltage by 90 o. Because the dielectric constant is complex, in real materials current leads voltage by 90 o -. Power loss = 2 1V0 tan 2 Becomes more of an issue at high frequencies (microwaves) 0 0

5 Loss tangent

6 Polarizability Overdamped modes Orientation polarizability Space charge polarizability Underdamped modes Ionic polarizability Electronic polarizability

7 Orientation (dipolar) Polarizability For materials (gases, liquids, solids) with a permanent dipole moment. The theory is very similar to paramagnetism. 1 T Curie law

8 Orientation Polarizability Ion jumps. doubly ionized

9 Water Schematic dielectric function of water from Wikipedia Source: Classical Electrodynamics, J.D. Jackson

10 Ionic Polarizability Displacement of ions of opposite sign. Only in ionic substances. This is an underdamped mode in the infrared.

11 Electronic polarizability (all materials) P Np N E dipole moments density polarizability

12 Polarizability Kittel

13 Inter- and intraband transitions When the bands are parallel, there is a peak in the absorption (") E ( k) E ( k) c v Optical spectroscopy has developed into the most important experimental tool for band structure determination. - Kittel

14 Ashcroft and Mermin

15 Dielectric function of BaTiO3

16 Dielectric function of silicon absorption ( ) n( ) ik( ) refractive index n 4 fk c extinction K

17 AC Conductivity For constant voltage, conductors conduct and insulators don't. For low ac voltages in a conductor, electric field and the electron velocity are inphase, electric field and electron position are out-of-phase. For low ac voltages in an insulator, electric field and the electron position are inphase, electric field and electron velocity are out-of-phase. At high (optical) frequencies the in-phase and out-of-phase component of the response is described by the dielectric function.

18 Conductivity / Dielectric function Harmonic dependence,, v v e x x e E E e i t i t i t v i x 0 0 P nex E E j nev inex E E E i i 0 Below about 100 GHz the frequency dependent conductivity is normally used. Above about 100 GHz the dielectric function is used (optical experiments).

19 Diffusive transport (low frequencies) v F ma ee m d e sc E v m E v e d d sc sc m e ne 2 ne m

20 Diffusive metal The current is related to the electric field j E n nm m v E n nm m Steady state solution The differential equation that describes how the velocity changes in time is: Inertial term m dv() t ev() t dt ee() t The impulse response function : 1 et g ( t) exp t 0 m m

21 Diffusive metal The differential equation is: m dv() t ev() t dt ee() t Assume a harmonic solution E()e it, v()e it i m 1 v( ) E( ) e v E 1 i m 1 1 1i 1 i 2 2 e 1 1 ne j ne v i E E m e Scattering time low ne high ine m 2

22 Diffusive metal ne 1 i 2 2 i0 i0 1 ne i i 1p p 2 ne m 0 Take the limit as goes to infinity 2 p for 0 for 0

23 low frequency metal / high frequency insulator Ibach & Lueth Aluminum ITO Conducting transparent contacts for LEDs and Solar cells Windows that reflect infrared 2 p 2 ne m 0 Reflection of radio waves from ionosphere

24

25

26 Ellipsometry n sin n sin

27 Ellipsometry Ellipsometry measures the change of polarization upon reflection. The measured signal depends on the thickness and the dielectric constant.

28 Ellipsometry The ratio of the two reflected polarizations is insensitive to instabilities of light source or atmospheric absorption.

Lecture contents Review: Few concepts from physics Electric field

Lecture contents Review: Few concepts from physics Electric field 1 Lecture contents Review: Few concepts from physics Electric field Coulomb law, Gauss law, Poisson equation, dipole, capacitor Conductors and isolators 1 Electric current Dielectric constant Overview

More information

Dielectric Materials: Properties and Applications

Dielectric Materials: Properties and Applications Dielectric Materials: Properties and Applications Content 1. Dielectrics : Properties 2. Fundamental definitions and Properties of electric dipole 3. Various polarization mechanisms involved in dielectric

More information

Polarization. D =e i E=k i e o E =e o E+ P

Polarization. D =e i E=k i e o E =e o E+ P Dielectrics Polarization a perfect insulator or a dielectric is the material with no free charge carriers. if an electric field, E, is applied to the insulator no charge flow. However in the presence of

More information

Basics of electromagnetic response of materials

Basics of electromagnetic response of materials Basics of electromagnetic response of materials Microscopic electric and magnetic field Let s point charge q moving with velocity v in fields e and b Force on q: F e F qeqvb F m Lorenz force Microscopic

More information

INTERACTION OF LIGHT WITH MATTER

INTERACTION OF LIGHT WITH MATTER INTERACTION OF LIGHT WITH MATTER Already.the speed of light can be related to the permittivity, ε and the magnetic permeability, µ of the material by Rememberε = ε r ε 0 and µ = µ r µ 0 where ε 0 = 8.85

More information

Class 6 : Insulating Materials

Class 6 : Insulating Materials Class 6 : Insulating Materials What is an insulator? Electric dipoles Polarization of an insulator, and how it modifies electric field Electric displacement Boundary conditions for E Recap (1) Maxwell

More information

Chapter 2. Dielectric Theories

Chapter 2. Dielectric Theories Chapter Dielectric Theories . Dielectric Theories 1.1. Introduction Measurements of dielectric properties of materials is very important because it provide vital information regarding the material characteristics,

More information

PHYSICS OF THE SPACE ENVIRONMENT

PHYSICS OF THE SPACE ENVIRONMENT PHYSICS OF THE SPACE ENVIRONMENT PHYS/EATS 380 Winter 006 Notes Set 6 Ionospheric Electron Densities The D, E, F1 and F Layers With the advent of radio communication in the early part of the last century

More information

Chap. 7. Dielectric Materials and Insulation

Chap. 7. Dielectric Materials and Insulation Chap. 7. Dielectric Materials and Insulation - The parallel plate capacitor with free space as an insulator: - The electric dipole moment for a pair of opposite changes +Q and -Q separated by a finite

More information

Advanced Vitreous State The Physical Properties of Glass

Advanced Vitreous State The Physical Properties of Glass Advanced Vitreous State The Physical Properties of Glass Dielectric Properties of Glass Lecture 1: Dielectric in Static Field Himanshu Jain Department of Materials Science & Engineering Lehigh University,

More information

MME 467: Ceramics for Advanced Applications

MME 467: Ceramics for Advanced Applications MME 467: Ceramics for Advanced Applications Lecture 26 Dielectric Properties of Ceramic Materials 2 1. Barsoum, Fundamental Ceramics, McGraw-Hill, 2000, pp.513 543 2. Richerson, Modern Ceramic Engineering,

More information

CHAPTER 6 DIELECTRIC AND CONDUCTIVITY STUDIES OF ZIRCONIUM TIN TITANATE (ZST)

CHAPTER 6 DIELECTRIC AND CONDUCTIVITY STUDIES OF ZIRCONIUM TIN TITANATE (ZST) 123 CHAPTER 6 DIELECTRIC AND CONDUCTIVITY STUDIES OF ZIRCONIUM TIN TITANATE (ZST) 6.1 INTRODUCTION We know that zirconium tin titanate ceramics are mostly used in microwave frequency applications. Previous

More information

UNIT I CONDUCTING MATERIALS 1. What are the merits of classical free electron theory? (i) It is used to verify Ohm s law. (ii) It is used to explain electrical and thermal conductivities of metals. (iii)

More information

Lecture 3: Optical Properties of Insulators, Semiconductors, and Metals. 5 nm

Lecture 3: Optical Properties of Insulators, Semiconductors, and Metals. 5 nm Metals Lecture 3: Optical Properties of Insulators, Semiconductors, and Metals 5 nm Course Info Next Week (Sept. 5 and 7) no classes First H/W is due Sept. 1 The Previous Lecture Origin frequency dependence

More information

Lecture 21 Reminder/Introduction to Wave Optics

Lecture 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 information

Chemistry 24b Lecture 23 Spring Quarter 2004 Instructor: Richard Roberts. (1) It induces a dipole moment in the atom or molecule.

Chemistry 24b Lecture 23 Spring Quarter 2004 Instructor: Richard Roberts. (1) It induces a dipole moment in the atom or molecule. Chemistry 24b Lecture 23 Spring Quarter 2004 Instructor: Richard Roberts Absorption and Dispersion v E * of light waves has two effects on a molecule or atom. (1) It induces a dipole moment in the atom

More information

10. Optics of metals - plasmons

10. Optics of metals - plasmons 1. Optics of metals - plasmons Drude theory at higher frequencies The Drude scattering time corresponds to the frictional damping rate The ultraviolet transparency of metals Interface waves - surface plasmons

More information

Atoms & Their Interactions

Atoms & Their Interactions Lecture 2 Atoms & Their Interactions Si: the heart of electronic materials Intel, 300mm Si wafer, 200 μm thick and 48-core CPU ( cloud computing on a chip ) Twin Creeks Technologies, San Jose, Si wafer,

More information

iclicker A metal ball of radius R has a charge q. Charge is changed q -> - 2q. How does it s capacitance changed?

iclicker A metal ball of radius R has a charge q. Charge is changed q -> - 2q. How does it s capacitance changed? 1 iclicker A metal ball of radius R has a charge q. Charge is changed q -> - 2q. How does it s capacitance changed? q A: C->2 C0 B: C-> C0 C: C-> C0/2 D: C->- C0 E: C->-2 C0 2 iclicker A metal ball of

More information

Solution Set 2 Phys 4510 Optics Fall 2014

Solution Set 2 Phys 4510 Optics Fall 2014 Solution Set Phys 4510 Optics Fall 014 Due date: Tu, September 16, in class Scoring rubric 4 points/sub-problem, total: 40 points 3: Small mistake in calculation or formula : Correct formula but calculation

More information

EC 577 / MS 577: Electrical Optical and Magnetic Properties of Materials Professor Theodore. D. Moustakas Fall Semester 2012

EC 577 / MS 577: Electrical Optical and Magnetic Properties of Materials Professor Theodore. D. Moustakas Fall Semester 2012 EC 577 / MS 577: Electrical Optical and Magnetic Properties of Materials Professor Theodore. D. Moustakas Fall Semester 2012 Office: 8 St. Mary s Street, Room no: 835 Phone: 353-5431 e-mail: tdm@bu.edu

More information

AML 883 Properties and selection of engineering materials

AML 883 Properties and selection of engineering materials AML 883 Properties and selection of engineering materials LECTURE 17. Electrical properties M P Gururajan Email: guru.courses@gmail.com Room No. MS 207/A 3 Phone: 1340 Types of electric behaviour Conduction

More information

Properties of Materials

Properties of Materials Tao Deng, dengtao@sjtu.edu.cn 1 1896 1920 1987 2006 Properties of Materials Chapter 3 Electrical Properties of Materials Tao Deng 3.1.4.4 The superconducting tunneling effect (Josephson effect) Tao Deng,

More information

Infrared Spectroscopy

Infrared Spectroscopy Infrared Spectroscopy The Interaction of Light with Matter Electric fields apply forces to charges, according to F = qe In an electric field, a positive charge will experience a force, but a negative charge

More information

The Electromagnetic Properties of Materials

The Electromagnetic Properties of Materials The Electromagnetic Properties of Materials Electrical conduction Metals Semiconductors Insulators (dielectrics) Superconductors Magnetic materials Ferromagnetic materials Others Photonic Materials (optical)

More information

Absorption and scattering

Absorption and scattering Absorption and scattering When a beam of radiation goes through the atmosphere, it encounters gas molecules, aerosols, cloud droplets, and ice crystals. These objects perturb the radiation field. Part

More information

ESO 205 Nature and Properties of Materials

ESO 205 Nature and Properties of Materials Dielectric Materials Topics to discuss Principles of dielectrics Dielectrics Loss and Breakdown Polarizations Frequency dependence Ferro-, Piezo- and Pyro- electrics ESO 205 Nature and Properties of Materials

More information

Dielectrics 9.1 INTRODUCTION 9.2 DIELECTRIC CONSTANT

Dielectrics 9.1 INTRODUCTION 9.2 DIELECTRIC CONSTANT 9 Dielectrics 9.1 INTRODUCTION A dielectric is an insulating material in which all the electrons are tightly bound to the nuclei of the atoms and there are no free electrons available for the conduction

More information

Energy Stored in Capacitors

Energy Stored in Capacitors Energy Stored in Capacitors U = 1 2 qv q = CV U = 1 2 CV 2 q 2 or U = 1 2 C 37 Energy Density in Capacitors (1) We define the, u, as the electric potential energy per unit volume Taking the ideal case

More information

Electrical Properties

Electrical Properties Electrical Properties Electrical Conduction R Ohm s law V = IR I l Area, A V where I is current (Ampere), V is voltage (Volts) and R is the resistance (Ohms or ) of the conductor Resistivity Resistivity,

More information

The electronic structure of materials 1

The electronic structure of materials 1 Quantum mechanics 2 - Lecture 9 December 18, 2013 1 An overview 2 Literature Contents 1 An overview 2 Literature Electronic ground state Ground state cohesive energy equilibrium crystal structure phase

More information

CBSE QUESTION PAPER. PHYSICS (Theory)

CBSE QUESTION PAPER. PHYSICS (Theory) CBSE QUESTION PAPER PHYSICS (Theory) Time allowed : 3 hours Maximum Marks : 70 General Instructions: (i) (ii) (iii) All questions are compulsory. There are 30 questions in total. Questions 1 to 8 carry

More information

Quantum Condensed Matter Physics Lecture 1

Quantum Condensed Matter Physics Lecture 1 Quantum Condensed Matter Physics Lecture 1 David Ritchie QCMP Lent/Easter 2017 http://www.sp.phy.cam.ac.uk/drp2/home 1.1 Quantum Condensed Matter Physics: synopsis (1) 1. Classical and Semi-classical models

More information

OPTICAL Optical properties of multilayer systems by computer modeling

OPTICAL Optical properties of multilayer systems by computer modeling Workshop on "Physics for Renewable Energy" October 17-29, 2005 301/1679-15 "Optical Properties of Multilayer Systems by Computer Modeling" E. Centurioni CNR/IMM AREA Science Park - Bologna Italy OPTICAL

More information

Lesson 3. Electric Potential. Capacitors Current Electricity

Lesson 3. Electric Potential. Capacitors Current Electricity Electric Potential Lesson 3 Potential Differences in a Uniform Electric Field Electric Potential and Potential Energy The Millikan Oil-Drop Experiment Capacitors Current Electricity Ohm s Laws Resistance

More information

Study Unit 5 INTERACTION OF ELECTROMAGNETIC WAVES WITH SUBSTANCE Dispersion of light

Study Unit 5 INTERACTION OF ELECTROMAGNETIC WAVES WITH SUBSTANCE Dispersion of light Study Unit 5 INTERACTION OF ELECTROMAGNETIC WAVES WITH SUBSTANCE 5.1. Dispersion of light We know that visible light consists of electromagnetic waves with the lengths band of 4 76 nm (corresponding frequency

More information

Physics (Theory) There are 30 questions in total. Question Nos. 1 to 8 are very short answer type questions and carry one mark each.

Physics (Theory) There are 30 questions in total. Question Nos. 1 to 8 are very short answer type questions and carry one mark each. Physics (Theory) Time allowed: 3 hours] [Maximum marks:70 General Instructions: (i) All questions are compulsory. (ii) (iii) (iii) (iv) (v) There are 30 questions in total. Question Nos. to 8 are very

More information

ELECTRODYNAMICS OF CONTINUOUS MEDIA

ELECTRODYNAMICS OF CONTINUOUS MEDIA ELECTRODYNAMICS OF CONTINUOUS MEDIA by L. D. LANDAU and E. M. LIFSHITZ Institute of Physical Problems, USSR Academy of Sciences Volume 8 of Course of Theoretical Physics Translated from the Russian by

More information

Scattering cross-section (µm 2 )

Scattering cross-section (µm 2 ) Supplementary Figures Scattering cross-section (µm 2 ).16.14.12.1.8.6.4.2 Total scattering Electric dipole, a E (1,1) Magnetic dipole, a M (1,1) Magnetic quardupole, a M (2,1). 44 48 52 56 Wavelength (nm)

More information

Maxwell s Equations:

Maxwell 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 information

5/1/2011 V R I. = ds. by definition is the ratio of potential difference of the wire ends to the total current flowing through it.

5/1/2011 V R I. = ds. by definition is the ratio of potential difference of the wire ends to the total current flowing through it. Session : Fundamentals by definition is the ratio of potential difference of the wire ends to the total current flowing through it. V R I E. dl L = σ E. ds A R = L σwt W H T At high frequencies, current

More information

THREE MAIN LIGHT MATTER INTERRACTION

THREE MAIN LIGHT MATTER INTERRACTION Chapters: 3and 4 THREE MAIN LIGHT MATTER INTERRACTION Absorption: converts radiative energy into internal energy Emission: converts internal energy into radiative energy Scattering; Radiative energy is

More information

Electronic Properties of Materials An Introduction for Engineers

Electronic Properties of Materials An Introduction for Engineers Rolf E. Hummel Electronic Properties of Materials An Introduction for Engineers With 219 Illustrations Springer-Verlag Berlin Heidelberg New York Tokyo Contents PARTI Fundamentals of Electron Theory CHAPTER

More information

Thin Film Bi-based Perovskites for High Energy Density Capacitor Applications

Thin Film Bi-based Perovskites for High Energy Density Capacitor Applications ..SKELETON.. Thin Film Bi-based Perovskites for High Energy Density Capacitor Applications Colin Shear Advisor: Dr. Brady Gibbons 2010 Table of Contents Chapter 1 Introduction... 1 1.1 Motivation and Objective...

More information

Radar sensing of Wake Vortices in clear air

Radar sensing of Wake Vortices in clear air 1 Radar sensing of Wake Vortices in clear air a feasibility study V. Brion*, N. Jeannin** Wakenet workshop, 15-16 may 2013, DGAC STAC, Bonneuil-Sur-Marne *Onera Paris **Onera Toulouse 2 Introduction In-house

More information

Radiation in the Earth's Atmosphere. Part 1: Absorption and Emission by Atmospheric Gases

Radiation in the Earth's Atmosphere. Part 1: Absorption and Emission by Atmospheric Gases Radiation in the Earth's Atmosphere Part 1: Absorption and Emission by Atmospheric Gases Electromagnetic Waves Electromagnetic waves are transversal. Electric and magnetic fields are perpendicular. In

More information

ECE 340 Lecture 6 : Intrinsic and Extrinsic Material I Class Outline:

ECE 340 Lecture 6 : Intrinsic and Extrinsic Material I Class Outline: ECE 340 Lecture 6 : Intrinsic and Extrinsic Material I Class Outline: Effective Mass Intrinsic Material Extrinsic Material Things you should know when you leave Key Questions What is the physical meaning

More information

van Quantum tot Molecuul

van Quantum tot Molecuul 10 HC10: Molecular and vibrational spectroscopy van Quantum tot Molecuul Dr Juan Rojo VU Amsterdam and Nikhef Theory Group http://www.juanrojo.com/ j.rojo@vu.nl Molecular and Vibrational Spectroscopy Based

More information

we can said that matter can be regarded as composed of three kinds of elementary particles; proton, neutron (no charge), and electron.

we can said that matter can be regarded as composed of three kinds of elementary particles; proton, neutron (no charge), and electron. Physics II we can said that matter can be regarded as composed of three kinds of elementary particles; proton, neutron (no charge), and electron. Particle Symbol Charge (e) Mass (kg) Proton P +1 1.67

More information

Optical Spectroscopies of Thin Films and Interfaces. Dietrich R. T. Zahn Institut für Physik, Technische Universität Chemnitz, Germany

Optical Spectroscopies of Thin Films and Interfaces. Dietrich R. T. Zahn Institut für Physik, Technische Universität Chemnitz, Germany Optical Spectroscopies of Thin Films and Interfaces Dietrich R. T. Zahn Institut für Physik, Technische Universität Chemnitz, Germany 1. Introduction 2. Vibrational Spectroscopies (Raman and Infrared)

More information

PHYSICS ADMISSIONS TEST Thursday, 2 November Time allowed: 2 hours

PHYSICS ADMISSIONS TEST Thursday, 2 November Time allowed: 2 hours PHYSICS ADMISSIONS TEST Thursday, 2 November 2017 Time allowed: 2 hours For candidates applying to Physics, Physics and Philosophy, Engineering, or Materials Total 23 questions [100 Marks] Answers should

More information

Magnetic Materials. 1. Magnetization 2. Potential and field of a magnetized object

Magnetic Materials. 1. Magnetization 2. Potential and field of a magnetized object Magnetic Materials 1. Magnetization 2. Potential and field of a magnetized object 3. H-field 4. Susceptibility and permeability 5. Boundary conditions 6. Magnetic field energy and magnetic pressure 1 Magnetic

More information

Preface to the Second Edition. Preface to the First Edition

Preface to the Second Edition. Preface to the First Edition Contents Preface to the Second Edition Preface to the First Edition iii v 1 Introduction 1 1.1 Relevance for Climate and Weather........... 1 1.1.1 Solar Radiation.................. 2 1.1.2 Thermal Infrared

More information

Supplementary Figure S1 SEM and optical images of Si 0.6 H 0.4 colloids. a, SEM image of Si 0.6 H 0.4 colloids. b, The size distribution of Si 0.

Supplementary Figure S1 SEM and optical images of Si 0.6 H 0.4 colloids. a, SEM image of Si 0.6 H 0.4 colloids. b, The size distribution of Si 0. Supplementary Figure S1 SEM and optical images of Si 0.6 H 0.4 colloids. a, SEM image of Si 0.6 H 0.4 colloids. b, The size distribution of Si 0.6 H 0.4 colloids. The standard derivation is 4.4 %. Supplementary

More information

THE EFFECT OF REVERSAL ON CAPACITOR LIFE

THE EFFECT OF REVERSAL ON CAPACITOR LIFE GENERAL ATOMICS ENERGY PRODUCTS Engineering Bulletin 96-004 THE EFFECT OF REVERSAL ON CAPACITOR LIFE November 2003 2003 Sorrento Electronics, Inc. Capacitor Engineering Department General Atomics Energy

More information

PHYSICS Course Structure Units Topics Marks Electrostatics Current Electricity III Magnetic Effect of Current & Magnetism

PHYSICS Course Structure Units Topics Marks Electrostatics Current Electricity III Magnetic Effect of Current & Magnetism PHYSICS Course Structure Units Topics Marks I Chapter 1 Chapter 2 II Chapter 3 III Chapter 4 Chapter 5 IV Chapter 6 Chapter 7 V Chapter 8 VI Chapter 9 Electrostatics Electric Charges and Fields Electrostatic

More information

EELE 3332 Electromagnetic II Chapter 9. Maxwell s Equations. Islamic University of Gaza Electrical Engineering Department Dr.

EELE 3332 Electromagnetic II Chapter 9. Maxwell s Equations. Islamic University of Gaza Electrical Engineering Department Dr. EELE 3332 Electromagnetic II Chapter 9 Maxwell s Equations Islamic University of Gaza Electrical Engineering Department Dr. Talal Skaik 2012 1 Review Electrostatics and Magnetostatics Electrostatic Fields

More information

Electrical and Electronics Engineering Materials

Electrical and Electronics Engineering Materials Electrical and Electronics Engineering Materials G.K. Banerjee Electrical and Electronics Engineering Materials Electrical and Electronics Engineering Materials G.K. Banerjee Professor and Head Department

More information

Lecture 2 Notes, Electromagnetic Theory II Dr. Christopher S. Baird, faculty.uml.edu/cbaird University of Massachusetts Lowell

Lecture 2 Notes, Electromagnetic Theory II Dr. Christopher S. Baird, faculty.uml.edu/cbaird University of Massachusetts Lowell Lecture Notes, Electromagnetic Theory II Dr. Christopher S. Baird, faculty.uml.edu/cbaird University of Massachusetts Lowell 1. Dispersion Introduction - An electromagnetic wave with an arbitrary wave-shape

More information

Dielectric Properties of Solids

Dielectric Properties of Solids Dielectric Properties of Solids Electric polarization In an insulator the electrons are so tightly bound that at ordinary temperatures they cannot be dislodged either by thermal vibrations or with ordinary

More information

Physics 9e/Cutnell. correlated to the. College Board AP Physics 2 Course Objectives

Physics 9e/Cutnell. correlated to the. College Board AP Physics 2 Course Objectives correlated to the College Board AP Physics 2 Course Objectives Big Idea 1: Objects and systems have properties such as mass and charge. Systems may have internal structure. Enduring Understanding 1.A:

More information

Probing the dynamics of biomolecules in liquid water by terahertz spectroscopy

Probing the dynamics of biomolecules in liquid water by terahertz spectroscopy Probing the dynamics of biomolecules in liquid water by terahertz spectroscopy Nguyen Quang Vinh Institute for Terahertz Science and technology Physics Department, UC Santa Barbara Spectroscopy probes

More information

Supplementary Information

Supplementary Information 1 Supplementary Information 3 Supplementary Figures 4 5 6 7 8 9 10 11 Supplementary Figure 1. Absorbing material placed between two dielectric media The incident electromagnetic wave propagates in stratified

More information

Electronic Devices & Circuits

Electronic Devices & Circuits Electronic Devices & Circuits For Electronics & Communication Engineering By www.thegateacademy.com Syllabus Syllabus for Electronic Devices Energy Bands in Intrinsic and Extrinsic Silicon, Carrier Transport,

More information

COLLEGE PHYSICS Chapter 19 ELECTRIC POTENTIAL AND ELECTRIC FIELD

COLLEGE PHYSICS Chapter 19 ELECTRIC POTENTIAL AND ELECTRIC FIELD COLLEGE PHYSICS Chapter 19 ELECTRIC POTENTIAL AND ELECTRIC FIELD Electric Potential Energy and Electric Potential Difference It takes work to move a charge against an electric field. Just as with gravity,

More information

Optical and Photonic Glasses. Lecture 37. Non-Linear Optical Glasses I - Fundamentals. Professor Rui Almeida

Optical and Photonic Glasses. Lecture 37. Non-Linear Optical Glasses I - Fundamentals. Professor Rui Almeida Optical and Photonic Glasses : Non-Linear Optical Glasses I - Fundamentals Professor Rui Almeida International Materials Institute For New Functionality in Glass Lehigh University Non-linear optical glasses

More information

ATMO 551a Fall Resonant Electromagnetic (EM) Interactions in Planetary atmospheres. Electron transition between different electron orbits

ATMO 551a Fall Resonant Electromagnetic (EM) Interactions in Planetary atmospheres. Electron transition between different electron orbits Resonant Electromagnetic (EM) Interactions in Planetary atmospheres There are three classes of energy states that interact with EM radiation that we are interested in to understand how light (EM radiation)

More information

Physikalisches Praktikum für Fortgeschrittene 1 Dielectric Constant Assistent: Herr Dr. M. Ghatkesar by Therese Challand theres.

Physikalisches Praktikum für Fortgeschrittene 1 Dielectric Constant Assistent: Herr Dr. M. Ghatkesar by Therese Challand theres. Physikalisches Praktikum für Fortgeschrittene 1 Dielectric Constant Assistent: Herr Dr. M. Ghatkesar by Therese Challand theres.challand stud.unibas.ch Contents 1 Theory 1 1.1 Introduction............................

More information

AML 883 Properties and selection of engineering materials

AML 883 Properties and selection of engineering materials AML 883 Properties and selection of engineering materials LECTURE 18. Electrical properties and design for their exploitation M P Gururajan Email: guru.courses@gmail.com Room No. MS 207/A 3 Phone: 1340

More information

Intrinsic Semiconductors

Intrinsic Semiconductors Technische Universität Graz Institute of Solid State Physics Intrinsic Semiconductors ermi function f(e) is the probability that a state at energy E is occupied. f( E) 1 E E 1 exp kt B ermi energy The

More information

PHY102 Electricity Course Summary

PHY102 Electricity Course Summary TOPIC 1 ELECTOSTTICS PHY1 Electricity Course Summary Coulomb s Law The magnitude of the force between two point charges is directly proportional to the product of the charges and inversely proportional

More information

Microwave Loss Reduction in Cryogenically Cooled Conductors R. Finger and A. R. Kerr

Microwave Loss Reduction in Cryogenically Cooled Conductors R. Finger and A. R. Kerr NATIONAL RADIO ASTRONOMY OBSERVATORY ELECTRONICS DIVISION INTERNAL REPORT NO. 321 Microwave Loss Reduction in Cryogenically Cooled Conductors R. Finger and A. R. Kerr July 3, 2008 NATIONAL RADIO ASTRONOMY

More information

The Dielectric Function of a Metal ( Jellium )

The Dielectric Function of a Metal ( Jellium ) The Dielectric Function of a Metal ( Jellium ) Total reflection Plasma frequency p (10 15 Hz range) Why are Metals Shiny? An electric field cannot exist inside a metal, because metal electrons follow the

More information

Units (Different systems of units, SI units, fundamental and derived units)

Units (Different systems of units, SI units, fundamental and derived units) Physics: Units & Measurement: Units (Different systems of units, SI units, fundamental and derived units) Dimensional Analysis Precision and significant figures Fundamental measurements in Physics (Vernier

More information

Chapter 17 Electric Potential

Chapter 17 Electric Potential Chapter 17 Electric Potential Units of Chapter 17 Electric Potential Energy and Potential Difference Relation between Electric Potential and Electric Field Equipotential Lines The Electron Volt, a Unit

More information

Chapter 14: Electric Fields and Matter

Chapter 14: Electric Fields and Matter Chapter 14: Electric Fields and Matter We extend the concepts of charge and electric fields due to point particles (and dipoles) to macroscopic objects In terms of their response to electric fields, we

More information

1) Introduction 2) Photo electric effect 3) Dual nature of matter 4) Bohr s atom model 5) LASERS

1) Introduction 2) Photo electric effect 3) Dual nature of matter 4) Bohr s atom model 5) LASERS 1) Introduction 2) Photo electric effect 3) Dual nature of matter 4) Bohr s atom model 5) LASERS 1. Introduction Types of electron emission, Dunnington s method, different types of spectra, Fraunhoffer

More information

Wavelength Dependent Microwave Devices Based on Metamaterial Technology. Professor Bal Virdee BSc(Eng) PhD CEng FIET

Wavelength Dependent Microwave Devices Based on Metamaterial Technology. Professor Bal Virdee BSc(Eng) PhD CEng FIET Wavelength Dependent Microwave Devices Based on Metamaterial Technology by Professor Bal Virdee BSc(Eng) PhD CEng FIET EM response of materials are determined by the spatial distribution of its atoms and

More information

Radiation processes and mechanisms in astrophysics I. R Subrahmanyan Notes on ATA lectures at UWA, Perth 18 May 2009

Radiation processes and mechanisms in astrophysics I. R Subrahmanyan Notes on ATA lectures at UWA, Perth 18 May 2009 Radiation processes and mechanisms in astrophysics I R Subrahmanyan Notes on ATA lectures at UWA, Perth 18 May 009 Light of the night sky We learn of the universe around us from EM radiation, neutrinos,

More information

1.9.5 Stoichiometry, Nonstoichiometry, and Defect Structures 75

1.9.5 Stoichiometry, Nonstoichiometry, and Defect Structures 75 Chapter 1 Elementary Materials Science Concepts 3 1.1 Atomic Structure and Atomic Number 3 1.2 Atomic Mass and Mole 8 1.3 Bonding and Types of Solids 9 1.3.1 Molecules and General Bonding Principles 9

More information

Skoog Chapter 6 Introduction to Spectrometric Methods

Skoog Chapter 6 Introduction to Spectrometric Methods Skoog Chapter 6 Introduction to Spectrometric Methods General Properties of Electromagnetic Radiation (EM) Wave Properties of EM Quantum Mechanical Properties of EM Quantitative Aspects of Spectrochemical

More information

Plasmonics. The long wavelength of light ( μm) creates a problem for extending optoelectronics into the nanometer regime.

Plasmonics. The long wavelength of light ( μm) creates a problem for extending optoelectronics into the nanometer regime. Plasmonics The long wavelength of light ( μm) creates a problem for extending optoelectronics into the nanometer regime. A possible way out is the conversion of light into plasmons. They have much shorter

More information

ELECTRICAL PROPERTIES

ELECTRICAL PROPERTIES ELECTRICAL PROPERTIES Introduction The objective of this chapter is to explore the electrical properties of materials, i.e. their responses to an applied electric field. We begin with the phenomenon of

More information

JFET/MESFET. JFET: small gate current (reverse leakage of the gate-to-channel junction) More gate leakage than MOSFET, less than bipolar.

JFET/MESFET. JFET: small gate current (reverse leakage of the gate-to-channel junction) More gate leakage than MOSFET, less than bipolar. JFET/MESFET JFET: small gate current (reverse leakage of the gate-to-channel junction) More gate leakage than MOSFET, less than bipolar. JFET has higher transconductance than the MOSFET. Used in low-noise,

More information

1 Physics Level I. Concepts Competencies Essential Questions Standards / Eligible Content

1 Physics Level I. Concepts Competencies Essential Questions Standards / Eligible Content Math Review Concepts Competencies Essential Questions Standards / Eligible A. Math Review 1. Accuracy & Precision 2. Quantitative Measurement 3. Scientific Notation 4. Algebraic Distributing & Factoring

More information

Advanced Prop. of Materials: What else can we do?

Advanced Prop. of Materials: What else can we do? 1.021, 3.021, 10.333, 22.00 : Introduction to Modeling and Simulation : Spring 2011 Part II Quantum Mechanical Methods : Lecture 6 Advanced Prop. of Materials: What else can we do? Jeffrey C. Grossman

More information

AML 883 Properties and selection of engineering materials

AML 883 Properties and selection of engineering materials AML 883 Properties and selection of engineering materials LECTURE 20. Origin of electrical properties M P Gururajan Email: guru.courses@gmail.com Room No. MS 207/A 3 Phone: 1340 What is the Big Bang Channel?

More information

Technische Universität Graz. Institute of Solid State Physics. 11. MOSFETs

Technische Universität Graz. Institute of Solid State Physics. 11. MOSFETs Technische Universität Graz Institute of Solid State Physics 11. MOSFETs Dec. 12, 2018 Gradual channel approximation accumulation depletion inversion http://lampx.tugraz.at/~hadley/psd/l10/gradualchannelapprox.php

More information

Electricity & Magnetism Study Questions for the Spring 2018 Department Exam December 4, 2017

Electricity & Magnetism Study Questions for the Spring 2018 Department Exam December 4, 2017 Electricity & Magnetism Study Questions for the Spring 2018 Department Exam December 4, 2017 1. a. Find the capacitance of a spherical capacitor with inner radius l i and outer radius l 0 filled with dielectric

More information

CIRCUIT ELEMENT: CAPACITOR

CIRCUIT ELEMENT: CAPACITOR CIRCUIT ELEMENT: CAPACITOR PROF. SIRIPONG POTISUK ELEC 308 Types of Circuit Elements Two broad types of circuit elements Ati Active elements -capable of generating electric energy from nonelectric energy

More information

Supporting Information

Supporting Information Supporting Information Improved Working Model for Interpreting the Excitation Wavelength- and Fluence-Dependent Response in Pulsed aser-induced Size Reduction of Aqueous Gold Nanoparticles Daniel Werner

More information

Overview. Sensors? Commonly Detectable Phenomenon Physical Principles How Sensors Work? Need for Sensors Choosing a Sensor Examples

Overview. Sensors? Commonly Detectable Phenomenon Physical Principles How Sensors Work? Need for Sensors Choosing a Sensor Examples Intro to Sensors Overview Sensors? Commonly Detectable Phenomenon Physical Principles How Sensors Work? Need for Sensors Choosing a Sensor Examples Sensors? American National Standards Institute A device

More information

Physics II (PH2223) Physics for Scientists and Engineers, with Modern Physics, 4th edition, Giancoli

Physics II (PH2223) Physics for Scientists and Engineers, with Modern Physics, 4th edition, Giancoli Physics II (PH2223) Physics for Scientists and Engineers, with Modern Physics, 4th edition, Giancoli Topics Covered Electric Charge & Electric Field Electric Potential Capacitance, Dielectric, Electric

More information

ELSEVIER FIRST PROOFS

ELSEVIER FIRST PROOFS OPTICAL MATERIALS / Measurement of Optical Properties of Solids 1 OPTICAL MATERIALS A0005 S0005 P0005 P0010 S0010 P0015 Measurement of Optical Properties of Solids P Lucas, University of Arizona, Tucson,

More information

Stopping, blooming, and straggling of directed energetic electrons in hydrogenic and arbitrary-z plasmas

Stopping, blooming, and straggling of directed energetic electrons in hydrogenic and arbitrary-z plasmas Stopping, blooming, and straggling of directed energetic electrons in hydrogenic and arbitrary-z plasmas This model Monte Carlo 1 MeV e 1 MeV e C. K. Li and R. D. Petrasso MIT 47th Annual Meeting of the

More information

2A: Absorbing Materials Pt-by-Pt and GenOsc

2A: Absorbing Materials Pt-by-Pt and GenOsc 2014 J.A. Woollam Co., Inc. www.jawoollam.com 1 2A: Absorbing Materials Pt-by-Pt and GenOsc Nina Hong U Penn, February 2014 2014 J.A. Woollam Co., Inc. www.jawoollam.com 2 Pt-by-Pt Fit UV Absorbing Films

More information

Chapter 10: Air Breakdown

Chapter 10: Air Breakdown ELECTOMAGNETIC COMPATIBILITY HANDBOOK 1 Chapter 10: Air Breakdown 10.1 How is a silicon controlled rectifier (SC) similar to the breakdown of a gas? 10.S By comparing to an actual Paschen curve for air

More information

Molecular spectroscopy

Molecular spectroscopy Molecular spectroscopy Origin of spectral lines = absorption, emission and scattering of a photon when the energy of a molecule changes: rad( ) M M * rad( ' ) ' v' 0 0 absorption( ) emission ( ) scattering

More information

Introduction to Electromagnetic Radiation and Radiative Transfer

Introduction to Electromagnetic Radiation and Radiative Transfer Introduction to Electromagnetic Radiation and Radiative Transfer Temperature Dice Results Visible light, infrared (IR), ultraviolet (UV), X-rays, γ-rays, microwaves, and radio are all forms of electromagnetic

More information

SOLID STATE PHYSICS AND MATERIAL SCIENCE

SOLID STATE PHYSICS AND MATERIAL SCIENCE M.Sc. (FINAL) PAPER II BLOCK I SOLID STATE PHYSICS AND MATERIAL SCIENCE Writer: Editor: Dr. Meetu Singh Dr. Purnima Swarup Khare SOLID STATE PHYSICS AND MATERIAL SCIENCE Unit -1 Unit- Unit-3 Lattice dynamics

More information