Repetition: Refractive Index
|
|
- Beatrix Golden
- 6 years ago
- Views:
Transcription
1 Repetitio: Refractive Idex (ω) κ(ω) 1 0 ω 0 ω 0 The real part of the refractive idex correspods to refractive idex, as it appears i Sellius law of refractio. The imagiary part correspods to the absorptio of eergy i the medium.
2 Repetitio: Optics - Coservatio Law For optics the followig coservatio law is valid: T + R + A + S = 1 T Trasmissio R Reflectio A Absorptio S Scatterig For geometric optics the refractio idex ca be cosidered as frequecy idepedet.
3 Repetitio: Optics - Iterfaces Reflectio: α = α α β α' 1 Refractio: si si α β = 1 Wavelegth: λ i = λ Vak i
4 Repetitio: Fresel's Equatios Media, idices of refractio 1,, perpedicular impigemet, i. e.: ϕ 1 = ϕ = 0 Reflectio: 1 1 k p k r r + = = Trasmissio: 1 1 k p k t t + = =
5 Repetitio: Optical Film Thickess Electromagetic radiatio passes from Vacuum ito a Medium with refractive idex : Frequecy ω: Wavelegth λ: ω = ω Vak λ = λ Vak If a film thickess is give as the moltiple of a wavelegth, λ is meat. This film thickess is called optical film thickess", d opt. It is: d Opt = d
6 Repetitio: Reflectio Suppressio 0 1 t 0 t 1 0 < 1 1 > d d = λ/4 λ Itesities of reflected radiatio: 0 1 r 0 r 1 1 r r I I ) ( ) ( I ) ( ) ( I = = + = + = Amplitude requiremet
7 Repetitio: Sigle Layer o absorptio, ifiite thickess absorptio, fiite thickess, reflexio at lower iterface Trasmitted itesity [%] d=100 m = =1.5 1 =1.57 0,4 0,5 0,6 0,7 0,8 Wavelegth [µm]
8 Repetitio: Reflectio Ehacemet I
9 Repetitio: Reflectio Ehacemet II A dielectric mirror cosists of a multilayer made from λ/4-coatigs with alteratig high (H) ad low (L) idices of refractio.
10 Magetic Properties I Motivatio: permaet data storage Logitudial Recordig Perpedicular Recordig
11 Magetic Properties II Motivatio: volatile data storage Spi Valve Magetic Radom Access Memory (MRAM)
12 Switchig "Switchig" of a magetic elemet meas the complete reversal of the magetizatio M by a exteral field H. To achieve this, the total eergy E of the elemet which results from M ud H has to be miimized. Eergy cotributios: Exteral field Stray field Aisotropy Exchage eergy Domai walls
13 Eergy Cotributios Grafik: Arbeitsgruppe Mikromagetismus, T. Schrefl
14 Eergy Cosideratio I Focus o the followig eergy cotributios: Exteral field Aisotropy Magetically aisotropic medium: z y easy directio H M x Magetizatio cosidered to rotate coheretly!
15 Eergy Cosideratio II Total magetic eergy (referred to uit volume); aisotropy costat K: z y easy directio M x E r r = M H + K si θ = M H H cos( φ θ) + K si θ = = M H x cosθ M H y si θ + K si θ Aditio theorem cos( φ θ) = cosθ cosφ + si θ si φ H x = H cosφ H y = H si φ
16 Magetic Reversal I H parallel to easy directio: M x K K M M H x A hysteresis loop is observable. H K = K M Exteral Coercitivity H K
17 Magetic Reversal II H perpedicular to easy directio: M y K K M M H y There is o hysteresis loop. M turs cotiously. Each itermediate positio is stable.
18 Further Cosideratios Magetic reversal may ot occur via coheret rotatio of M ia all cases. Further iflueces: Domai ucleatio Domai wall mobility Volume of magetized regios Superparamagetic limit: Volumia of magetized regios (bit size) ca become so small, that the aisotropy eergy ca be surpassed by thermal fluctuatios istability
19 Superparamagetic Limit Estimate: Typical aisotropy eergies: E Ais = J m 3 Thermal eergy withi a grai of volume V: 3 k B T k B T = EAis V V = l = l = 3 E T = 300K : l = m Ais k E B T Ais
20 Giat Mageto Resistace (GMR) Mageto Resistace is the pheomeo that the electric resistivity ca be iflueced by the directio of the magetizatio. The effect is based o differet scatterig probabilities betwee electros of equal ad opposite spis. It has extremely importat techological ad scietific applicatios (Nobel prize 007!): Hard disk readig heads Spi valves
21 Chemical Compositio For the chemical aalysis of thi filmsas well as for the aalysis of the surface of bulk materials a wide rade of physical aalysis methds is available. Most of these methods are based o the followig priciple: + Bombardemet of the material with probe particles + Detectio of the geerated radiatio or of the geerated particles Oly electro optic methods (TEM, LEED, RHEED) ad scaig probe methods (STM, AFM,...) do ot ecessarily ivolve this priciple.
22 Physical Aalytics - Survey
23 Electro Beam Micro Aalysis Iteractio volumes: Backscattered electros: approx. 1-5µm ejectio depth Secodary electros: ear surace regio Auger electros: approx. 10 m ejectio depth X-rays: approx. 1-5µm ejectio depth
24 Auger Electro Spectroscopy (AES) Characteristics: + Surface sesitive (ejectio depth 1 10 m) + Sesitive to light elemets + Sesitivity limit: approx. 0.1 At%
25 Eergy Cispersive X-Ray Aalysis (EDX) Ejectio volume Surface effects EDX-spectrum Nachweisgreze: ca. 0.1 At%
26 XPS, UPS Photoelectro spectroscopy by excitatio with X-rays (XPS) or UV-radiatio (UPS) Observable properties: + Electro work fuctio + Desity of states
27 EELS Electro Eergy Loss Spectroscopy Characteristics: + High lateral resolutio (TEM) + Sesitivity limit: ca. 1 At% + Possibility of local chemical mappig
28 SIMS, SNMS Secodary Io Mass Spectroscopy (SIMS) or Secodary Neutral Mass Spectroscopy (SNMS): Mass spectroscopy of directly sputtered ios (SIMS) or post ioized eutrals (SNMS): Characteristics: Cautio: Ioizatio cross sectio withi the bulk does ot correspod to the oe of a sigle atom " matrix effect " + High chemical sesitivity (mass spectroscopy) + Quatificatio possible (SNMS) + Sesitivity limit: ppm
29 LEISS Low Eergy Io Surface Spectroscopy Characteristics: + High surface sesitivity (1. Moolayer) + Absolute quatificatio possible (simple collisio mechaism)
30 GDOS Glow Discharge Optical Spectroscopy Characteristics: + Fast depth profilgg + Good chemical sesitivity + Reasoable quatificatio possible (Spectroscopy)
31 RBS Rutherford Backscatterig Characteristics: + No destructive depth aalysis + Quatificatio possible (Coulomb potetial)
32 LEED Low Eergy Electro Diffractio W(100) 45 ev 145 ev Characteristics: + Surface sesitive + Yields surface crystallography ad adsorbate positios
33 RHEED Reflected High Eergy Electro Diffractio Ideal situatio: Characteristics: + Surface sesitive + Yields detailed iformatios about growth modes (Layer By Layer/rougheig/stochastic)
Repetition: Micro Hardness
Repetitio: Micro Hardess Defied by the residual deformatio of a material due to the peetratio of a (ideally) udeformable test body. Test body material: + Diamod Test body geometries: + Vicers: Pyramid
More informationPHYS-3301 Lecture 7. CHAPTER 4 Structure of the Atom. Rutherford Scattering. Sep. 18, 2018
CHAPTER 4 Structure of the Atom PHYS-3301 Lecture 7 4.1 The Atomic Models of Thomso ad Rutherford 4.2 Rutherford Scatterig 4.3 The Classic Atomic Model 4.4 The Bohr Model of the Hydroge Atom 4.5 Successes
More informationRay Optics Theory and Mode Theory. Dr. Mohammad Faisal Dept. of EEE, BUET
Ray Optics Theory ad Mode Theory Dr. Mohammad Faisal Dept. of, BUT Optical Fiber WG For light to be trasmitted through fiber core, i.e., for total iteral reflectio i medium, > Ray Theory Trasmissio Ray
More informationOptics. n n. sin. 1. law of rectilinear propagation 2. law of reflection = 3. law of refraction
Optics What is light? Visible electromagetic radiatio Geometrical optics (model) Light-ray: extremely thi parallel light beam Usig this model, the explaatio of several optical pheomea ca be give as the
More informationThin Film Interference
DVCED UDERGRDUTE LORTORY EXPERIMET 3, FILM Thi Film Iterferece Refereces updated by arbara Chu, ugust 6 Revisio: March 6 by Yi Chai Origial y: Jaso Harlow, 6 1. Itroductio The iterferece of reflected waves
More informationa b c d e f g h Supplementary Information
Supplemetary Iformatio a b c d e f g h Supplemetary Figure S STM images show that Dark patters are frequetly preset ad ted to accumulate. (a) mv, pa, m ; (b) mv, pa, m ; (c) mv, pa, m ; (d) mv, pa, m ;
More informationHydrogen (atoms, molecules) in external fields. Static electric and magnetic fields Oscyllating electromagnetic fields
Hydroge (atoms, molecules) i exteral fields Static electric ad magetic fields Oscyllatig electromagetic fields Everythig said up to ow has to be modified more or less strogly if we cosider atoms (ad ios)
More informationINF-GEO Solutions, Geometrical Optics, Part 1
INF-GEO430 20 Solutios, Geometrical Optics, Part Reflectio by a symmetric triagular prism Let be the agle betwee the two faces of a symmetric triagular prism. Let the edge A where the two faces meet be
More informationScattering at an Interface:
8/9/08 Course Istructor Dr. Raymod C. Rumpf Office: A 337 Phoe: (95) 747 6958 E Mail: rcrumpf@utep.edu EE 4347 Applied Electromagetics Topic 3h Scatterig at a Iterface: Phase Matchig & Special Agles Phase
More information6.1 Analysis of frequency selective surfaces
6.1 Aalysis of frequecy selective surfaces Basic theory I this paragraph, reflectio coefficiet ad trasmissio coefficiet are computed for a ifiite periodic frequecy selective surface. The attetio is tured
More informationWaves and rays - II. Reflection and transmission. Seismic methods: Reading: Today: p Next Lecture: p Seismic rays obey Snell s Law
Seismic methods: Waves ad rays - II Readig: Today: p7-33 Net Lecture: p33-43 Reflectio ad trasmissio Seismic rays obey Sell s Law (just like i optics) The agle of icidece equals the agle of reflectio,
More informationMaxwell's Equations in Media and Their Solution *
Maxwell's Equatios i Media ad heir Solutio * ao Zhag College of Nuclear Sciece ad echology, Beijig Normal Uiversity, Beijig 1875 taozhag@bu.edu.c Abstract Magetic field magetizatio, polarizatio ad iduced
More informationPHYS-3301 Lecture 3. EM- Waves behaving like Particles. CHAPTER 3 The Experimental Basis of Quantum. CHAPTER 3 The Experimental Basis of Quantum
CHAPTER 3 The Experimetal Basis of Quatum PHYS-3301 Lecture 3 Sep. 4, 2018 3.1 Discovery of the X Ray ad the Electro 3.2 Determiatio of Electro Charge 3.3 Lie Spectra 3.4 Quatizatio 3.5 Blackbody Radiatio
More informationPhysics 102 Exam 2 Spring Last Name: First Name Network-ID
Physics Exam Sprig 4 Last Name: First Name Network-ID Discussio Sectio: Discussio TA Name: This is a opportuity to improve your scaled score for hour exam. You must tur it i durig lecture o Wedesday April
More informationLecture 3-7 Semiconductor Lasers.
Laser LED Stimulated emissio Spotaeous emissio Laser I th I Typical output optical power vs. diode curret (I) characteristics ad the correspodig output spectrum of a laser diode.?1999 S.O. Kasap, Optoelectroics
More informationCork Institute of Technology Bachelor of Science (Honours) in Applied Physics and Instrumentation-Award - (NFQ Level 8)
ork Istitute of Techology Bachelor of Sciece (Hoours) i Applied Physics ad Istrumetatio-Award - (NFQ Level 8) Istructios Aswer Four questios, at least TWO questios from each Sectio. Use separate aswer
More informationElectrical Resistance
Electrical Resistace I + V _ W Material with resistivity ρ t L Resistace R V I = L ρ Wt (Uit: ohms) where ρ is the electrical resistivity Addig parts/billio to parts/thousad of dopats to pure Si ca chage
More informationEE 485 Introduction to Photonics Photon Optics and Photon Statistics
Itroductio to Photoics Photo Optics ad Photo Statistics Historical Origi Photo-electric Effect (Eistei, 905) Clea metal V stop Differet metals, same slope Light I Slope h/q ν c/λ Curret flows for λ < λ
More informationREFLECTION AND REFRACTION
REFLECTION AND REFRACTION REFLECTION AND TRANSMISSION FOR NORMAL INCIDENCE ON A DIELECTRIC MEDIUM Assumptios: No-magetic media which meas that B H. No dampig, purely dielectric media. No free surface charges.
More informationBohr s Atomic Model Quantum Mechanical Model
September 7, 0 - Summary - Itroductio to Atomic Theory Bohr s Atomic Model Quatum Mechaical Model 3- Some Defiitio 3- Projects Temperature Pressure Website Subject Areas Plasma is a Mixture of electros,
More informationMULTIPLE SCATTERING OF PHOTONS USING THE BOLTZMANN TRANSPORT EQUATION
MULTIPLE SCATTERING OF PHOTONS USING THE BOLTZMANN TRANSPORT EQUATION Jorge E. Feradez Laboratory of Motecuccolio-DIENCA INFN, INFM & Alma Mater Studiorum - Uiversity of Bologa ICXOM-18, Frascati 25-30
More informationName Solutions to Test 2 October 14, 2015
Name Solutios to Test October 4, 05 This test cosists of three parts. Please ote that i parts II ad III, you ca skip oe questio of those offered. The equatios below may be helpful with some problems. Costats
More informationPHYS-3301 Lecture 5. CHAPTER 3 The Experimental Basis of Quantum. 3.8: Compton Effect. 3.8: Compton Effect. Sep. 11, 2018
CHAPTER 3 The Experimetal Basis of Quatum PHYS-3301 Lecture 5 Sep. 11, 2018 3.1 Discovery of the X Ray ad the Electro 3.2 Determiatio of Electro Charge 3.3 Lie Spectra 3.4 Quatizatio 3.5 Blackbody Radiatio
More informationSemiconductors. PN junction. n- type
Semicoductors. PN juctio We have reviously looked at the electroic roerties of itrisic, - tye ad - time semicoductors. Now we will look at what haes to the electroic structure ad macroscoic characteristics
More informationChapter 2 Motion and Recombination of Electrons and Holes
Chapter 2 Motio ad Recombiatio of Electros ad Holes 2.1 Thermal Eergy ad Thermal Velocity Average electro or hole kietic eergy 3 2 kt 1 2 2 mv th v th 3kT m eff 3 23 1.38 10 JK 0.26 9.1 10 1 31 300 kg
More information[ ] sin ( ) ( ) = 2 2 ( ) ( ) ( ) ˆ Mechanical Spectroscopy II
Solid State Pheomea Vol. 89 (003) pp 343-348 (003) Tras Tech Publicatios, Switzerlad doi:0.408/www.scietific.et/ssp.89.343 A New Impulse Mechaical Spectrometer to Study the Dyamic Mechaical Properties
More informationThe power of analytical spectroscopy
The power of aalytical spectroscopy Daiila et al. J. Rama Spectr. 33, 807 (00) Reflected light Red lake varish UV light Rama spectrum Lead white ciabar Caput mortuum Byzatie Ico (AD Our 534), Lady, Our
More informationEECS130 Integrated Circuit Devices
EECS130 Itegrated Circuit Devices Professor Ali Javey 9/04/2007 Semicoductor Fudametals Lecture 3 Readig: fiish chapter 2 ad begi chapter 3 Aoucemets HW 1 is due ext Tuesday, at the begiig of the class.
More informationIntrinsic Carrier Concentration
Itrisic Carrier Cocetratio I. Defiitio Itrisic semicoductor: A semicoductor material with o dopats. It electrical characteristics such as cocetratio of charge carriers, deped oly o pure crystal. II. To
More informationEpsilons Near Zero limits in the Mie scattering theory
Epsilos Near Zero limits i the Mie scatterig theory M. Tagviashvili * Adroikashvili Istitute of Physics, 6 Tamarashvili st, 77, Tbilsi, Georgia * madoa.tagviashvili@grt.ge Abstract: The classical Mie theory
More informationModeling of Plasmas and Neutrals Including Plasma-Wall Interaction for Long Term Tokamak Operation
odelig of Plasmas ad Neutrals Icludig Plasma-Wall Iteractio for Log Term Tokamak Operatio Akiyoshi Hatayama 1, Kousuke Okamoto 1, Ryoko Tatsumi 1, Kazuhiro. Abe 1, ad Kazuaki Haada 2 1. Backgroud/otivatio
More information3 and 4 NSW PHYSICS Module 3 Module 4
Q 3 S C I S Y Ques t d a s io H P NSW er w s ad 4 ics m a ody m r e d Th etism a s g e v a 3 Wa icity ad M tr c e l E 4 le u d o M le u d o M Bria Shadwick s 2018 First published 2018 Private Bag 7023
More informationLecture 6. Semiconductor physics IV. The Semiconductor in Equilibrium
Lecture 6 Semicoductor physics IV The Semicoductor i Equilibrium Equilibrium, or thermal equilibrium No exteral forces such as voltages, electric fields. Magetic fields, or temperature gradiets are actig
More informationIntroduction to Semiconductor Devices and Circuit Model
Itroductio to Semicoductor Devices ad Circuit Model Readig: Chater 2 of Howe ad Sodii Electrical Resistace I + V _ W homogeeous samle t L Resistace R V I L = ρ Wt (Uits: Ω) where ρ is the resistivity (Uits:
More informationA Brief Introduction to the Physical Basis for Electron Spin Resonance
A Brief Itroductio to the Physical Basis for Electro Spi Resoace I ESR measuremets, the sample uder study is exposed to a large slowly varyig magetic field ad a microwave frequecy magetic field orieted
More informationFinite-Difference Time-Domain Simulation of Light Propagation in 2D Periodic and Quasi-Periodic Photonic Structures
JNS 3 (213) 359-364 Fiite-Differece Time-Domai Simulatio of Light Propagatio i 2D Periodic ad Quasi-Periodic Photoic Structures N. Dadashadeh a,b*, O.G. Romaov b a Islamic Aad Uiversity of Hadishahr, Hadishahr,
More informationPhysics Methods in Art and Archaeology
Physics Methods i Art ad Archaeology Michael Wiescher PHYS 78 Archaeologist i the 90ties Somewhere i South America 80 years later --- i the Valley of the Kigs, gypt Physics Tools & Techology Dager & Adveture
More informationThere are 7 crystal systems and 14 Bravais lattices in 3 dimensions.
EXAM IN OURSE TFY40 Solid State Physics Moday 0. May 0 Time: 9.00.00 DRAFT OF SOLUTION Problem (0%) Itroductory Questios a) () Primitive uit cell: The miimum volume cell which will fill all space (without
More informationBasic Concepts of Electricity. n Force on positive charge is in direction of electric field, negative is opposite
Basic Cocepts of Electricity oltage E Curret I Ohm s Law Resistace R E = I R 1 Electric Fields A electric field applies a force to a charge Force o positive charge is i directio of electric field, egative
More informationDESCRIPTION OF THE SYSTEM
Sychroous-Serial Iterface for absolute Ecoders SSI 1060 BE 10 / 01 DESCRIPTION OF THE SYSTEM TWK-ELEKTRONIK GmbH D-001 Düsseldorf PB 1006 Heirichstr. Tel +9/11/6067 Fax +9/11/6770 e-mail: ifo@twk.de Page
More informationCharacterization and Simulation of HF Propagation in a realistic disturbed and horizontally inhomogeneous Ionosphere
Characterizatio ad Simulatio of HF Propagatio i a realistic disturbed ad horizotally ihomogeeous Ioosphere Vadim E. Gherm ad Nikolay N.Zerov Departmet of Radiophysics Uiversity of St.Petersburg St.Petersburg
More informationChapter 2 Motion and Recombination of Electrons and Holes
Chapter 2 Motio ad Recombiatio of Electros ad Holes 2.1 Thermal Motio 3 1 2 Average electro or hole kietic eergy kt mv th 2 2 v th 3kT m eff 23 3 1.38 10 JK 0.26 9.1 10 1 31 300 kg K 5 7 2.310 m/s 2.310
More informationLecture III-2: Light propagation in nonmagnetic
A. La Rosa Lecture Notes ALIED OTIC Lecture III2: Light propagatio i omagetic materials 2.1 urface ( ), volume ( ), ad curret ( j ) desities produced by arizatio charges The objective i this sectio is
More informationCHM 424 EXAM 2 - COVER PAGE FALL
CHM 44 EXAM - COVER PAGE FALL 007 There are six umbered pages with five questios. Aswer the questios o the exam. Exams doe i ik are eligible for regrade, those doe i pecil will ot be regraded. coulomb
More informationOblique frozen modes in periodic layered media
PHYSICAL REVIEW E 68, 036609 2003 Oblique froze modes i periodic layered media A. Figoti ad I. Vitebskiy Departmet of Mathematics, Uiversity of Califoria, Irvie, Irvie, Califoria 92697, USA Received 9
More informationRecent Experimental Results in ADITYA Tokamak
Recet Experimetal Results i ADITYA Tokamak R. Jha ad the ADITYA Team Istitute for Plasma Research, Bhat, Gadhiagar-382 428, INDIA e-mail:rjha@ipr.res.i Abstract. Recet studies o measuremets of edge turbulece
More informationABSTRACT 1. INTRODUCTION
Iwamura, Y., T. Itoh, ad M. SakaNo. Nuclear Products ad Their Time Depedece Iduced by Cotiuous Diffusio of Deuterium Through Multi-layer Palladium Cotaiig Low Work Fuctio Material. i 8th Iteratioal Coferece
More information3/21/2017. Commuting and Non-commuting Operators Chapter 17. A a
Commutig ad No-commutig Operators Chapter 17 Postulate 3. I ay measuremet of the observable associated with a operator A the oly values that will ever be observed are the eige values, a, which satisfy
More informationSignal Processing in Mechatronics
Sigal Processig i Mechatroics Zhu K.P. AIS, UM. Lecture, Brief itroductio to Sigals ad Systems, Review of Liear Algebra ad Sigal Processig Related Mathematics . Brief Itroductio to Sigals What is sigal
More informationPhys 102 Lecture 25 The quantum mechanical model of light
Phys 102 Lecture 25 The quatum mechaical model of light 1 Recall last time Problems with classical physics Stability of atoms Atomic spectra Photoelectric effect Quatum model of the atom Bohr model oly
More informationQuantum Annealing for Heisenberg Spin Chains
LA-UR # - Quatum Aealig for Heiseberg Spi Chais G.P. Berma, V.N. Gorshkov,, ad V.I.Tsifriovich Theoretical Divisio, Los Alamos Natioal Laboratory, Los Alamos, NM Istitute of Physics, Natioal Academy of
More informationPhysics 201 Final Exam December
Physics 01 Fial Exam December 14 017 Name (please prit): This test is admiistered uder the rules ad regulatios of the hoor system of the College of William & Mary. Sigature: Fial score: Problem 1 (5 poits)
More informationIntroduction to Signals and Systems, Part V: Lecture Summary
EEL33: Discrete-Time Sigals ad Systems Itroductio to Sigals ad Systems, Part V: Lecture Summary Itroductio to Sigals ad Systems, Part V: Lecture Summary So far we have oly looked at examples of o-recursive
More informationFree Space Optical Wireless Communications under Turbulence Channel Effect
IOSR Joural of Electroics ad Commuicatio Egieerig (IOSR-JECE) e-issn: 78-834,p- ISSN: 78-8735.Volume 9, Issue 3, Ver. III (May - Ju. 014), PP 01-08 Free Space Optical Wireless Commuicatios uder Turbulece
More informationSOLUTIONS: ECE 606 Homework Week 7 Mark Lundstrom Purdue University (revised 3/27/13) e E i E T
SOUIONS: ECE 606 Homework Week 7 Mark udstrom Purdue Uiversity (revised 3/27/13) 1) Cosider a - type semicoductor for which the oly states i the badgap are door levels (i.e. ( E = E D ). Begi with the
More informationImproved Perfectly Matched Layers for Acoustic Radiation and Scattering Problems
Excerpt from the Proceedigs of the COMSOL Coferece 2008 Haover Improved Perfectly Matched Layers for Acoustic Radiatio ad Scatterig Problems Mario Zampolli *,1, Nils Malm 2, Alessadra Tesei 1 1 NURC NATO
More informationCSIR-UGC-NET/JRF Jue 0 CSIR-UGC NET/JRF JUNE - 0 PHYSICAL SCIENCES BOOKLET - [A] PART - B. A particle of uit mass moves i a potetial V x b ax, where a ad b are positive costats. x The agular frequecy of
More informationWave Motion
Wave Motio Wave ad Wave motio: Wave is a carrier of eergy Wave is a form of disturbace which travels through a material medium due to the repeated periodic motio of the particles of the medium about their
More informationExperimental Fact: E = nhf
CHAPTR 3 The xperimetal Basis of Quatum PHYS-3301 Lecture 4 Sep. 6, 2018 3.1 Discovery of the X Ray ad the lectro 3.2 Determiatio of lectro Charge 3.3 Lie Spectra 3.4 Quatizatio 3.5 Blackbody Radiatio
More informationEE / EEE SAMPLE STUDY MATERIAL. GATE, IES & PSUs Signal System. Electrical Engineering. Postal Correspondence Course
Sigal-EE Postal Correspodece Course 1 SAMPLE STUDY MATERIAL Electrical Egieerig EE / EEE Postal Correspodece Course GATE, IES & PSUs Sigal System Sigal-EE Postal Correspodece Course CONTENTS 1. SIGNAL
More informationNATIONAL UNIVERSITY OF SINGAPORE
NATIONAL UNIVERSITY OF SINGAPORE PC4 Physics II (Semester I: AY 008-09, 6 November) Time Allowed: Hours INSTRUCTIONS TO CANDIDATES This examiatio paper comprises EIGHT (8) prited pages with FIVE (5) short
More informationSolid State Device Fundamentals
Solid State Device Fudametals ENS 345 Lecture Course by Alexader M. Zaitsev alexader.zaitsev@csi.cuy.edu Tel: 718 982 2812 4N101b 1 Thermal motio of electros Average kietic eergy of electro or hole (thermal
More informationSection 19. Dispersing Prisms
Sectio 9 Dispersig Prisms 9- Dispersig Prism 9- The et ray deviatio is the sum of the deviatios at the two surfaces. The ray deviatio as a fuctio of the iput agle : si si si cossi Prism Deviatio - Derivatio
More informationSection 19. Dispersing Prisms
19-1 Sectio 19 Dispersig Prisms Dispersig Prism 19-2 The et ray deviatio is the sum of the deviatios at the two surfaces. The ray deviatio as a fuctio of the iput agle : 1 2 2 si si si cossi Prism Deviatio
More informationIntroduction of Surface Acoustic Wave (SAW) Devices
April, 018 Itroductio of Surface Acoustic Wave (SAW) Devices Part 6: D Propagatio ad Waveguide Ke-a Hashimoto Chiba Uiversit k.hashimoto@ieee.org http://www. te.chiba-u. jp/~ke Cotets Wavevector ad Diffractio
More informationObservation of Landau levels on nitrogen-doped flat graphite. surfaces without external magnetic fields
Supplemetary Iformatio Observatio of Ladau levels o itroge-doped flat graphite surfaces without exteral magetic fields Takahiro Kodo,, oghui Guo, Taishi Shikao, Tetsuya Suzuki, Masataka Sakurai, Susumu
More informationProblem 1. Problem Engineering Dynamics Problem Set 9--Solution. Find the equation of motion for the system shown with respect to:
2.003 Egieerig Dyamics Problem Set 9--Solutio Problem 1 Fid the equatio of motio for the system show with respect to: a) Zero sprig force positio. Draw the appropriate free body diagram. b) Static equilibrium
More informationTotal Internal Reflection Ellipsometry with Transition Layer
168 Total Iteral Reflectio Ellipsometry with Trasitio Layer Jaroslav Vlček*, Jaromír Pištora b, Odřej Bárta c, Tomuo Yamaguchi d VOL. 1, NO. 1, JUNE 26 *Departmet of Mathematics, b Departmet of Physics,
More informationPhoton Scanning Tunneling Microscope: Detection of Evanescent Waves
Photo Scaig Tuelig Microscope: Detectio of Evaescet Waves N. Aderso, J. DeGroote, ad M. A. Ladau Istitute of Optics, Uiversity of Rochester, Rochester NY 460 Opt59 Dec 003 Abstract: We report the formatio
More informationExercises and Problems
HW Chapter 4: Oe-Dimesioal Quatum Mechaics Coceptual Questios 4.. Five. 4.4.. is idepedet of. a b c mu ( E). a b m( ev 5 ev) c m(6 ev ev) Exercises ad Problems 4.. Model: Model the electro as a particle
More informationAccuracy of TEXTOR He-beam diagnostics
Accuracy of TEXTOR He-beam diagostics O. Schmitz, I.L.Beigma *, L.A. Vaishtei *, A. Pospieszczyk, B. Schweer, M. Krychoviak, U. Samm ad the TEXTOR team Forschugszetrum Jülich,, Jülich, Germay *Lebedev
More informationSECTION 2 Electrostatics
SECTION Electrostatics This sectio, based o Chapter of Griffiths, covers effects of electric fields ad forces i static (timeidepedet) situatios. The topics are: Electric field Gauss s Law Electric potetial
More informationDamped Vibration of a Non-prismatic Beam with a Rotational Spring
Vibratios i Physical Systems Vol.6 (0) Damped Vibratio of a No-prismatic Beam with a Rotatioal Sprig Wojciech SOCHACK stitute of Mechaics ad Fudametals of Machiery Desig Uiversity of Techology, Czestochowa,
More information1 Adiabatic and diabatic representations
1 Adiabatic ad diabatic represetatios 1.1 Bor-Oppeheimer approximatio The time-idepedet Schrödiger equatio for both electroic ad uclear degrees of freedom is Ĥ Ψ(r, R) = E Ψ(r, R), (1) where the full molecular
More informationSystems of Particles: Angular Momentum and Work Energy Principle
1 2.003J/1.053J Dyamics ad Cotrol I, Sprig 2007 Professor Thomas Peacock 2/20/2007 Lecture 4 Systems of Particles: Agular Mometum ad Work Eergy Priciple Systems of Particles Agular Mometum (cotiued) τ
More informationReliability and Queueing
Copyright 999 Uiversity of Califoria Reliability ad Queueig by David G. Messerschmitt Supplemetary sectio for Uderstadig Networked Applicatios: A First Course, Morga Kaufma, 999. Copyright otice: Permissio
More informationFYS Vår 2016 (Kondenserte fasers fysikk)
FYS3410 - Vår 2016 (Kodeserte fasers fysikk) http://www.uio.o/studier/emer/matat/fys/fys3410/v16/idex.html Pesum: Itroductio to Solid State Physics by Charles Kittel (Chapters 1-9 ad 17, 18, 20) Adrej
More informationPolariton resonances in multilayered piezoelectric superlattices
Joural of Physics: Coferece Series PAPER OPEN ACCESS Polarito resoaces i multilayered piezoelectric superlattices To cite this article: D Piliposya 218 J. Phys.: Cof. Ser. 991 1265 View the article olie
More informationOptical Devices for High Speed Communication Systems. Lecture Notes
Optical Devices for High Speed Commuicatio Systems Lecture Notes Optoelectroic Devices & Commuicatio Networks Motreal λ λ Switch λ 3 WDM Amplifier λ Add/Drop WDM λ Ottawa Toroto λ λ 3 WDM Switch Amplifier
More informationLecture 9: Diffusion, Electrostatics review, and Capacitors. Context
EECS 5 Sprig 4, Lecture 9 Lecture 9: Diffusio, Electrostatics review, ad Capacitors EECS 5 Sprig 4, Lecture 9 Cotext I the last lecture, we looked at the carriers i a eutral semicoductor, ad drift currets
More information1.3 Convergence Theorems of Fourier Series. k k k k. N N k 1. With this in mind, we state (without proof) the convergence of Fourier series.
.3 Covergece Theorems of Fourier Series I this sectio, we preset the covergece of Fourier series. A ifiite sum is, by defiitio, a limit of partial sums, that is, a cos( kx) b si( kx) lim a cos( kx) b si(
More informationLecture # 07: Flow Visualization techniques: Shadowgraph and Schlieren
AerE 311L & AerE343L Lecture Notes Lecture # 07: Flow Visualizatio techiques: Shadowgraph ad Schliere Dr. Hui H Hu Departmet of Aerospace Egieerig owa State Uiversity Ames, owa 50011, U.S.A AerE311L: Lab#01
More informationPHYS-3301 Lecture 9. CHAPTER 5 Wave Properties of Matter and Quantum Mechanics I. 5.3: Electron Scattering. Bohr s Quantization Condition
CHAPTER 5 Wave Properties of Matter ad Quatum Mecaics I PHYS-3301 Lecture 9 Sep. 5, 018 5.1 X-Ray Scatterig 5. De Broglie Waves 5.3 Electro Scatterig 5.4 Wave Motio 5.5 Waves or Particles? 5.6 Ucertaity
More informationHashing and Amortization
Lecture Hashig ad Amortizatio Supplemetal readig i CLRS: Chapter ; Chapter 7 itro; Sectio 7.. Arrays ad Hashig Arrays are very useful. The items i a array are statically addressed, so that isertig, deletig,
More informationChapter If n is odd, the median is the exact middle number If n is even, the median is the average of the two middle numbers
Chapter 4 4-1 orth Seattle Commuity College BUS10 Busiess Statistics Chapter 4 Descriptive Statistics Summary Defiitios Cetral tedecy: The extet to which the data values group aroud a cetral value. Variatio:
More informationCh.20 SPECTROPHOTOMETERS
Ch.20 SPECTROPHOTOMETERS 20. P Absorbace o Po A log logt ( 0 ~ ) P P Sigle beam spectrophotometer icoveiet Double beam spectrophoptometer correct automatically the chages of source itesity, det. Respose
More informationOPTIMAL PIECEWISE UNIFORM VECTOR QUANTIZATION OF THE MEMORYLESS LAPLACIAN SOURCE
Joural of ELECTRICAL EGIEERIG, VOL. 56, O. 7-8, 2005, 200 204 OPTIMAL PIECEWISE UIFORM VECTOR QUATIZATIO OF THE MEMORYLESS LAPLACIA SOURCE Zora H. Perić Veljo Lj. Staović Alesadra Z. Jovaović Srdja M.
More informationGeometrical optics limit of stochastic electromagnetic fields
PHYSICAL REVIEW A 77, 043831 2008 Geometrical optics limit of stochastic electromagetic fields Robert W. Schooover, Adam M. Zysk,* ad P. Scott Carey Departmet of Electrical ad Computer Egieerig ad The
More informationChem Discussion #13 Chapter 10. Correlation diagrams for diatomic molecules. Key
Chem 101 017 Discussio #13 Chapter 10. Correlatio diagrams for diatomic molecules. Key 1. Below is a plot of the first 10 ioizatio eergies for a sigle atom i 3 rd row of the periodic table. The x- axis
More information3. Magnetism. p e ca (3.3) H = B = (0, 0, B), p p e c A( r), (3.1) A = 1 2 ( B r) = 1 ( By, Bx, 0) = p 2 e (
3 Magetism 31 Couplig of matter to a magetic field: Diamagetism ad paramagetism A exteral magetic field ca couple to matter ad electros i two differet ways we cosider the o-relativistic case: 1 through
More informationNotes The Incremental Motion Model:
The Icremetal Motio Model: The Jacobia Matrix I the forward kiematics model, we saw that it was possible to relate joit agles θ, to the cofiguratio of the robot ed effector T I this sectio, we will see
More informationAcknowledgments. Line Resolved Spectra. Outline. Continuum Processes ATOMIC PROCESSES IN. Spectral Line Intensities. Spectral Line Intensities (2/2)
ATOMIC PROCESSES IN PLASMAS IAEA Advaced School o Plasma Spectroscopy ICTP, March 2015 Ackowledgmets I am greatly idebted to Prof. J. L. Schwob from whom I leared most of what I kow about laboratory plasma
More informationQuantum well states Alkali metals plasmons
SHG from thi films Quatum well states Alkali metals plasmos Wede shaped metal film AFM sca of A/Si()7 7 The wede shaped metal film is deposited by slowly movi the sample up ito the shadow of a fixed shield.
More informationAnalysis of composites with multiple rigid-line reinforcements by the BEM
Aalysis of composites with multiple rigid-lie reiforcemets by the BEM Piotr Fedeliski* Departmet of Stregth of Materials ad Computatioal Mechaics, Silesia Uiversity of Techology ul. Koarskiego 18A, 44-100
More information3. Magnetism. = e2. = erg = 2 Ry = 27.2 ev. E 0 = me4 H = p p e c A( r), (3.1) B = (0, 0, B), A = 1 2 ( B r) = 1 ( By, Bx, 0) = p 2 e (
The eergy scale is give i 3 Magetism E 0 = me4 h = e a 0 = 043 10 10 erg = Ry = 7 ev 31 Couplig of matter to a magetic field: Diamagetism ad paramagetism A exteral magetic field ca couple to matter ad
More informationSection 7. Gaussian Reduction
7- Sectio 7 Gaussia eductio Paraxial aytrace Equatios eractio occurs at a iterace betwee two optical spaces. The traser distace t' allows the ray height y' to be determied at ay plae withi a optical space
More informationPhysics 232 Gauge invariance of the magnetic susceptibilty
Physics 232 Gauge ivariace of the magetic susceptibilty Peter Youg (Dated: Jauary 16, 2006) I. INTRODUCTION We have see i class that the followig additioal terms appear i the Hamiltoia o addig a magetic
More informationComplex Analysis Spring 2001 Homework I Solution
Complex Aalysis Sprig 2001 Homework I Solutio 1. Coway, Chapter 1, sectio 3, problem 3. Describe the set of poits satisfyig the equatio z a z + a = 2c, where c > 0 ad a R. To begi, we see from the triagle
More informationEF 152 Exam #2, Spring 2016 Page 1 of 6
EF 152 Exam #2, Sprig 2016 Page 1 of 6 Name: Sectio: Istructios Sit i assiged seat; failure to sit i assiged seat results i a 0 for the exam. Do ot ope the exam util istructed to do so. Do ot leave if
More informationREFLECTION AND REFRACTION
RFLCTON AND RFRACTON We ext ivestigate what happes whe a light ray movig i oe medium ecouters aother medium, i.e. the pheomea of reflectio ad refractio. We cosider a plae M wave strikig a plae iterface
More information