Quantum Walks and Phase Transitions in Quadratic Nonlinear Waveguide Arrays

Size: px
Start display at page:

Download "Quantum Walks and Phase Transitions in Quadratic Nonlinear Waveguide Arrays"

Transcription

1 Quatum Walks ad Phase Trasitios i Quadratic Noliear Waveguide Arrays Adrey A. Sukhorukov joit work with Alexader S. Soltsev, Dragomir N. Neshev, Yuri S. Kivshar Noliear Physics Cetre, Australia Natioal Uiversity Frak Setzpfadt, Rolad Schiek, Thomas Pertsch Friedrich-Schiller-Uiversity Jea, Germay Outlie Waveguide arrays i material with quadratic oliearity Secod-harmoic geeratio: Phase trasitio through parametric iteractios; theory ad experimet Spotaeous parametric dowcoversio: Combied photo-pair geeratio ad quatum walks i arrays

2 z Optical arrays de dz - + E + E 0 i +C + = Light tuels betwee s E amplitude at umber C couplig coefficiet Review: Christodoulides, et al., Nature 424, 87 (2003) Periodically poled s i Lithium Niobate Parametric oliear iteractios Liear couplig betwee s Noliear couplig betwee FW ad SH through quadratic oliearity c FW + - period c FW c NL c NL c NL idex profile SH 02 ~750 m FW 00 ~500 m c SH c SH 2

3 Localizatio i quadratic layered structures Statioary (solito) solutios 0exp 0exp2 A z A i z B z B i z Small propagatio costat wide FW drivig force cotrols SH FW ad SH are i phase o staggered SH propagatio costat Large propagatio costat arrow FW drivig FW ad SH are out of phase staggered SH A c A A A B * FW (2) 2 B csh B B A (field) [a.u.] Localizatio & sychroizatio amplitude phase spatial spectrum umber trasverse waveumber =; c FW = c SH = umber (field) [a.u.] umber First theory: Sukhorukov, Kivshar, Bag, Soukoulis, PRE 63, 0665 (200) Experimet: Setzpfadt, Sukhorukov, Neshev, Schiek, Kivshar, Pertsch, PRL 05, (200) FW SH 3

4 Mismatch cotrolled by FW wavelegth Spectral peak aroud i spatial Fourier domai key feature of staggered phase profile Experimetal results 0 s 5 µm period 7 mm log 550 m laser 5.2 ps pulses Experimet: Setzpfadt, Sukhorukov, Neshev, Schiek, Kivshar, Pertsch, PRL 05, (200) Spotaeous Parametric Dow-Coversio Spotaeous Parametric Dow- Coversio (SPDC) is a commo source of etagled photo pairs s i,, k s k i p s i k k k p s i 4

5 Quatum walks of photo pairs sigal detector BBO idler detector array couplig iterface Correlatios of photo pairs at the output of the array coicidece measuremet idler umber Correlated photo pairs a - a 0 at a iput lead to output with o classical aalogy sigal umber Buchig & ati-buchig: sigal & idler photos primarily propagate i the same or opposite directios A. Peruzzo, M. Lobio, J. C. F. Matthews, N. Matsuda, A. Politi, K. Poulios, X.-Q. Zhou, Y. Lahii, N. Ismail, K. Worhoff, et al., Sciece 329, 500 (200). Our work Simultaeous photo-pair geeratio ad quatum walks i array with quadratic oliearity Quatum statistics govered by: quatum walks - couplig to the right ad left photo correlatios i a pair probabilities to geerate the photo pairs at differet spatial locatios Pump stays i iput Degeerate type-i SPDC Soltsev, Sukhorukov, Neshev, Kivshar (20) submitted Itegrated device for ovel classically cotrollable quatum states 5

6 Photo pair correlatios for pump i oe Pump i oe =0 Phase-mismatch is equal to 0 whe for 0 i s idler detector sigal detector coicidece measuremet i real space K-space Real space I real space buchig ad ati-buchig are archieved Phase mismatch ca be cotrolled by pump wavelegth or temperature 2 With icrease of 4 sigle phase mismatch real-space output becomes classical Soltsev, Sukhorukov, Neshev, Kivshar (20) submitted Photo pair correlatios for pump i two s Pump i two eighbourig s with phase shift P I real space buchig ad ati-buchig switchig ca be cotrolled by phase shift P betwee pump waves I s = (0,) =0 = P = 0 P = π i s idler detector sigal detector K-space coicidece measuremet i real space Real space Soltsev, Sukhorukov, Neshev, Kivshar (20) submitted 6

7 Summary Fudametal effects ad future applicatios of quadratic oliear arrays New type of phase trasitio associated with secod-harmoic geeratio due to a iterplay of localizatio ad sychroisatio Theory: Sukhorukov, Kivshar, Bag, Soukoulis, PRE 63, 0665 (200); Experimet i LiNbO 3 : Setzpfadt et al., PRL 05, (200) Novel itegrated device icorporatig spotaeous parametric dow-coversio ad quatum walks photo pair source with strogly oclassical correlatios with simple classical cotrol of photo statistics by shapig the iput pump Soltsev, Sukhorukov, Neshev, Kivshar (20) submitted 7

Coherent control of Rydberg atoms

Coherent control of Rydberg atoms Coheret cotrol of Rydberg atoms Haruka Maeda Departmet of Phys. & Math., Aoyama Gakui Uiversity Why Rydberg atom? Multilevel ladder system What ca we study with Rydberg atom? Microwave multiphoto ioizatio

More information

Steering of bright discrete photovoltaic solitons in lithium niobate waveguide arrays

Steering of bright discrete photovoltaic solitons in lithium niobate waveguide arrays Steerig of bright discrete photovoltaic solitos i lithium iobate waveguide arrays Miluti Stepió', Vladimir Shadarov2, Aleksadra Maluckov3, Feg Che', Daiel Rude', Christia Rüter', ad Detlef Kip1 1 stitute

More information

Quantum Annealing for Heisenberg Spin Chains

Quantum 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 information

36. Nonlinear optics: χ(2) processes

36. Nonlinear optics: χ(2) processes 36. Nonlinear optics: χ() processes The wave equation with nonlinearity Second-harmonic generation: making blue light from red light approximations: SVEA, zero pump depletion phase matching quasi-phase

More information

12. Nonlinear optics I

12. 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 information

Introduction to Signals and Systems, Part V: Lecture Summary

Introduction 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 information

36. Nonlinear optics: (2) processes

36. Nonlinear optics: (2) processes 36. Nonlinear optics: () processes The wave equation with nonlinearity Second-harmonic generation: making blue light from red light approximations: SVEA, zero pump depletion phase matching quasi-phase

More information

Hydrogen (atoms, molecules) in external fields. Static electric and magnetic fields Oscyllating electromagnetic fields

Hydrogen (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 information

Types of Waves Transverse Shear. Waves. The Wave Equation

Types of Waves Transverse Shear. Waves. The Wave Equation Waves Waves trasfer eergy from oe poit to aother. For mechaical waves the disturbace propagates without ay of the particles of the medium beig displaced permaetly. There is o associated mass trasport.

More information

SLAC Summer School on Electron and Photon Beams. Tor Raubenheimer Lecture #3: High Gain FEL s

SLAC Summer School on Electron and Photon Beams. Tor Raubenheimer Lecture #3: High Gain FEL s SLAC Summer School o Electro ad Photo Beams Tor Raubeheimer Lecture #3: High Gai FEL s Outlie Sychrotro radiatio Bedig magets Wigglers ad udulators Iverse Compto scatterig Free Electro Lasers FEL Oscillators

More information

CKM Matrix and CP Violation in Standard Model

CKM Matrix and CP Violation in Standard Model CKM Matrix ad CP Violatio i Stadard Model Origi of CKM Matrix. B meso produc,o at B factories Lecture 13 Shahram Rahatlou Fisica delle Par,celle Elemetari, Ao Accademico 2015-16 http://www.roma1.if.it/people/rahatlou/particelle/

More information

Exponential transient rotating waves and their bifurcations in a ring of unidirectionally coupled bistable Lorenz systems

Exponential transient rotating waves and their bifurcations in a ring of unidirectionally coupled bistable Lorenz systems Available olie at www.sciecedirect.com Procedia IUTAM 5 (2012 ) 283 287 IUTAM Symposium o 50 Years of Chaos: Applied ad Theoretical Expoetial trasiet rotatig waves ad their bifurcatios i a rig of uidirectioally

More information

REGRESSION (Physics 1210 Notes, Partial Modified Appendix A)

REGRESSION (Physics 1210 Notes, Partial Modified Appendix A) REGRESSION (Physics 0 Notes, Partial Modified Appedix A) HOW TO PERFORM A LINEAR REGRESSION Cosider the followig data poits ad their graph (Table I ad Figure ): X Y 0 3 5 3 7 4 9 5 Table : Example Data

More information

LECTURE 14. Non-linear transverse motion. Non-linear transverse motion

LECTURE 14. Non-linear transverse motion. Non-linear transverse motion LETURE 4 No-liear trasverse motio Floquet trasformatio Harmoic aalysis-oe dimesioal resoaces Two-dimesioal resoaces No-liear trasverse motio No-liear field terms i the trajectory equatio: Trajectory equatio

More information

AN OPEN-PLUS-CLOSED-LOOP APPROACH TO SYNCHRONIZATION OF CHAOTIC AND HYPERCHAOTIC MAPS

AN OPEN-PLUS-CLOSED-LOOP APPROACH TO SYNCHRONIZATION OF CHAOTIC AND HYPERCHAOTIC MAPS http://www.paper.edu.c Iteratioal Joural of Bifurcatio ad Chaos, Vol. 1, No. 5 () 119 15 c World Scietific Publishig Compay AN OPEN-PLUS-CLOSED-LOOP APPROACH TO SYNCHRONIZATION OF CHAOTIC AND HYPERCHAOTIC

More information

PHYS-3301 Lecture 10. Wave Packet Envelope Wave Properties of Matter and Quantum Mechanics I CHAPTER 5. Announcement. Sep.

PHYS-3301 Lecture 10. Wave Packet Envelope Wave Properties of Matter and Quantum Mechanics I CHAPTER 5. Announcement. Sep. Aoucemet Course webpage http://www.phys.ttu.edu/~slee/3301/ PHYS-3301 Lecture 10 HW3 (due 10/4) Chapter 5 4, 8, 11, 15, 22, 27, 36, 40, 42 Sep. 27, 2018 Exam 1 (10/4) Chapters 3, 4, & 5 CHAPTER 5 Wave

More information

MIT Department of Chemistry 5.74, Spring 2005: Introductory Quantum Mechanics II Instructor: Professor Andrei Tokmakoff

MIT Department of Chemistry 5.74, Spring 2005: Introductory Quantum Mechanics II Instructor: Professor Andrei Tokmakoff MIT Departmet of Chemistry 5.74, Sprig 5: Itroductory Quatum Mechaics II Istructor: Professor Adrei Tomaoff p. 97 ABSORPTION SPECTRA OF MOLECULAR AGGREGATES The absorptio spectra of periodic arrays of

More information

Ofer Aharony Strings 2004, Paris, France Aharony, Marsano, Minwalla, Papadodimas and Van Raamsdonk, hep-th/ to appear

Ofer Aharony Strings 2004, Paris, France Aharony, Marsano, Minwalla, Papadodimas and Van Raamsdonk, hep-th/ to appear The Decofiemet ad Hagedor Phase Trasitios i Weakly Coupled Large N Gauge Theories Ofer Aharoy Strigs 2004, Paris, Frace Aharoy, Marsao, Miwalla, Papadodimas ad Va Raamsdok, hep-th/0310285 + to appear Outlie

More information

PH 411/511 ECE B(k) Sin k (x) dk (1)

PH 411/511 ECE B(k) Sin k (x) dk (1) Fall-27 PH 4/5 ECE 598 A. La Rosa Homework-3 Due -7-27 The Homework is iteded to gai a uderstadig o the Heiseberg priciple, based o a compariso betwee the width of a pulse ad the width of its spectral

More information

[ ] sin ( ) ( ) = 2 2 ( ) ( ) ( ) ˆ Mechanical Spectroscopy II

[ ] 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 information

arxiv:physics/ v1 [physics.optics] 23 Oct 2006

arxiv:physics/ v1 [physics.optics] 23 Oct 2006 Localized modes ad bistable scatterig i oliear etwork juctios Adrey E. Miroshicheko, Mario I. Molia, ad Yuri S. Kivshar Noliear Physics Cetre, Research School of Physical Scieces ad Egieerig, Australia

More information

Phys 102 Lecture 25 The quantum mechanical model of light

Phys 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 information

The Effects of Substitution on the Optical Properties of poly(p-phenylenevinylene) Derivatives

The Effects of Substitution on the Optical Properties of poly(p-phenylenevinylene) Derivatives Proc. of the 2 d Iteratioal Cof. o ptics ad Laser Applicatios ICLA 7, September -7, Yogyakarta, Idoesia The Effects of Substitutio o the ptical Properties of poly(p-pheyleeviylee) Derivatives A. Bahtiar

More information

Cryptography using dark-bright soliton to generate keys by orthogonal dark-bright soliton pair

Cryptography using dark-bright soliton to generate keys by orthogonal dark-bright soliton pair vol.6,no,03,pp.5- Proc. Schl. IT Tokai Uiv. Vol.xx,No.,0xx,pp.xxx -xxx Paper Paper Cryptography usig dark-bright solito to geerate keys by orthogoal dark-bright solito pair by Xaythavy LOUANGVILAY *, Somsak

More information

Some Features on Entropy Squeezing for Two-Level System with a New Nonlinear Coherent State

Some Features on Entropy Squeezing for Two-Level System with a New Nonlinear Coherent State Joural of Quatum Iformatio Sciece, 4, 4, 7-8 Published Olie March 4 i SciRes. http://www.scirp.org/joural/jqis http://d.doi.org/.436/jqis.4.47 Some Features o Etropy Squeezig for Two-Level System with

More information

The DOA Estimation of Multiple Signals based on Weighting MUSIC Algorithm

The DOA Estimation of Multiple Signals based on Weighting MUSIC Algorithm , pp.10-106 http://dx.doi.org/10.1457/astl.016.137.19 The DOA Estimatio of ultiple Sigals based o Weightig USIC Algorithm Chagga Shu a, Yumi Liu State Key Laboratory of IPOC, Beijig Uiversity of Posts

More information

5.1. Periodic Signals: A signal f(t) is periodic iff for some T 0 > 0,

5.1. Periodic Signals: A signal f(t) is periodic iff for some T 0 > 0, 5. Periodic Sigals: A sigal f(t) is periodic iff for some >, f () t = f ( t + ) i t he smallest value that satisfies the above coditios is called the period of f(t). Cosider a sigal examied over to 5 secods

More information

To the use of Sellmeier formula

To the use of Sellmeier formula To the use of Sellmeier formula by Volkmar Brücker Seior Experte Service (SES) Bo ad HfT Leipzig, Germay Abstract Based o dispersio of pure silica we proposed a geeral Sellmeier formula for various dopats

More information

Cork Institute of Technology Bachelor of Science (Honours) in Applied Physics and Instrumentation-Award - (NFQ Level 8)

Cork 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 information

Chapter 2 Systems and Signals

Chapter 2 Systems and Signals Chapter 2 Systems ad Sigals 1 Itroductio Discrete-Time Sigals: Sequeces Discrete-Time Systems Properties of Liear Time-Ivariat Systems Liear Costat-Coefficiet Differece Equatios Frequecy-Domai Represetatio

More information

Nonequilibrium theory of exciton-polariton condensates. Michiel Wouters

Nonequilibrium theory of exciton-polariton condensates. Michiel Wouters Noequilibrium theory of excito-polarito codesates Michiel Wouters Collaboratio with Iacopo Carusotto Treto, theory) Vicezo Savoa EPFL theory) Cristiao Ciuti Paris 7, theory) Kostatios Lagoudais, Barbara

More information

Analysis Methods for Slab Waveguides

Analysis Methods for Slab Waveguides Aalsis Methods for Slab Waveguides Maxwell s Equatios ad Wave Equatios Aaltical Methods for Waveguide Aalsis: Marcatilis Method Simple Effective Idex Method Numerical Methods for Waveguide Aalsis: Fiite-Elemet

More information

INF-GEO Solutions, Geometrical Optics, Part 1

INF-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 information

17 Phonons and conduction electrons in solids (Hiroshi Matsuoka)

17 Phonons and conduction electrons in solids (Hiroshi Matsuoka) 7 Phoos ad coductio electros i solids Hiroshi Matsuoa I this chapter we will discuss a miimal microscopic model for phoos i a solid ad a miimal microscopic model for coductio electros i a simple metal.

More information

Ray Optics Theory and Mode Theory. Dr. Mohammad Faisal Dept. of EEE, BUET

Ray 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 information

Note: we can take the Real and Imaginary part of the Schrödinger equation and write it in a way similar to the electromagnetic field. p = n!

Note: we can take the Real and Imaginary part of the Schrödinger equation and write it in a way similar to the electromagnetic field. p = n! Quatum Mechaics //8 Staford class with Leoard Susskid. Lecture 5. The ext class i this series has the title Special Relativity ad icludes classical field theory, least actio, Lagragia techiques, tesor

More information

PH 411/511 ECE B(k) Sin k (x) dk (1)

PH 411/511 ECE B(k) Sin k (x) dk (1) Fall-26 PH 4/5 ECE 598 A. La Rosa Homework-2 Due -3-26 The Homework is iteded to gai a uderstadig o the Heiseberg priciple, based o a compariso betwee the width of a pulse ad the width of its spectral

More information

Finite-Difference Time-Domain Method (FDTD)

Finite-Difference Time-Domain Method (FDTD) Computatioal Photoics, Summer Term 04, Abbe School of Photoics, FSU Jea, Prof. Thomas Pertsch Computatioal Photoics Semiar 05, 0 Jue 04 Fiite-Differece Time-Domai Method (FDTD) Lear how to implemet a D

More information

Dr. Radhakant Padhi Asst. Professor Dept. of Aerospace Engineering Indian Institute of Science - Bangalore

Dr. Radhakant Padhi Asst. Professor Dept. of Aerospace Engineering Indian Institute of Science - Bangalore Lecture 0 Coversio Betwee State Space ad Trasfer Fuctio Represetatios i Liear Systems II Dr. Radhakat Padhi Asst. Professor Dept. of Aerospace Egieerig Idia Istitute of Sciece - Bagalore A Alterate First

More information

DIRECTION OF ARRIVAL ESTIMATION

DIRECTION OF ARRIVAL ESTIMATION Research Article DIRECTION OF ARRIVAL ESTIMATION Lalita Gupta, R P Sigh Address for correspodece Dept. of Electroics & Commuicatio Egieerig, Maulaa Azad Natioal Istitute of Techology, Bhopal MP Email:gupta.lalita@gmail.com

More information

Further Exploration of Patterns

Further Exploration of Patterns Further Exploratio of Patters Abstract Quadratic Patters a+b+c 4a+b+c 9a+3b+c 16a+4b+c 5a+5b+c 1 st chage 3a+b 5a+b 7a+b 9a+b d chage a a a 1 Coefficiet of is ( a) a. Costat secod chage, therefore it is

More information

TIME-CORRELATION FUNCTIONS

TIME-CORRELATION FUNCTIONS p. 8 TIME-CORRELATION FUNCTIONS Time-correlatio fuctios are a effective way of represetig the dyamics of a system. They provide a statistical descriptio of the time-evolutio of a variable for a esemble

More information

Bohr s Atomic Model Quantum Mechanical Model

Bohr 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 information

Lecture 25 (Dec. 6, 2017)

Lecture 25 (Dec. 6, 2017) Lecture 5 8.31 Quatum Theory I, Fall 017 106 Lecture 5 (Dec. 6, 017) 5.1 Degeerate Perturbatio Theory Previously, whe discussig perturbatio theory, we restricted ourselves to the case where the uperturbed

More information

Harmonic Quantum Integer

Harmonic Quantum Integer Harmoic Quatum Iteger The hypothesis of this paper is that there is a quatum iteger umber system that is aalogous to the umbers associated with the elemets, the isotopes, or the differet eergy states of

More information

Chapter 4. The Intensity-Dependent Refractive Index

Chapter 4. The Intensity-Dependent Refractive Index Chapter. The Itesity-Depedet Refractive Idex - Third order oliear effect - Mathematical descriptio of the oliear refractive idex - Physical processes that give rise to this effect Referece : R.W. Boyd,

More information

Monte Carlo Optimization to Solve a Two-Dimensional Inverse Heat Conduction Problem

Monte Carlo Optimization to Solve a Two-Dimensional Inverse Heat Conduction Problem Australia Joural of Basic Applied Scieces, 5(): 097-05, 0 ISSN 99-878 Mote Carlo Optimizatio to Solve a Two-Dimesioal Iverse Heat Coductio Problem M Ebrahimi Departmet of Mathematics, Karaj Brach, Islamic

More information

Voltage controlled oscillator (VCO)

Voltage controlled oscillator (VCO) Voltage cotrolled oscillator (VO) Oscillatio frequecy jl Z L(V) jl[ L(V)] [L L (V)] L L (V) T VO gai / Logf Log 4 L (V) f f 4 L(V) Logf / L(V) f 4 L (V) f (V) 3 Lf 3 VO gai / (V) j V / V Bi (V) / V Bi

More information

ANTI-SYNCHRONIZING SLIDING CONTROLLER DESIGN FOR IDENTICAL PAN SYSTEMS

ANTI-SYNCHRONIZING SLIDING CONTROLLER DESIGN FOR IDENTICAL PAN SYSTEMS ANTI-SYNCHRONIZING SLIDING CONTROLLER DESIGN FOR IDENTICAL PAN SYSTEMS Sudarapadia Vaidyaatha Research ad Developmet Cetre, Vel Tech Dr. RR & Dr. SR Techical Uiversity Avadi, Cheai-600 062, Tamil Nadu,

More information

Orthogonal Gaussian Filters for Signal Processing

Orthogonal Gaussian Filters for Signal Processing Orthogoal Gaussia Filters for Sigal Processig Mark Mackezie ad Kiet Tieu Mechaical Egieerig Uiversity of Wollogog.S.W. Australia Abstract A Gaussia filter usig the Hermite orthoormal series of fuctios

More information

PHYS-3301 Lecture 9. CHAPTER 5 Wave Properties of Matter and Quantum Mechanics I. 5.3: Electron Scattering. Bohr s Quantization Condition

PHYS-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 information

PH 425 Quantum Measurement and Spin Winter SPINS Lab 1

PH 425 Quantum Measurement and Spin Winter SPINS Lab 1 PH 425 Quatum Measuremet ad Spi Witer 23 SPIS Lab Measure the spi projectio S z alog the z-axis This is the experimet that is ready to go whe you start the program, as show below Each atom is measured

More information

CS537. Numerical Analysis and Computing

CS537. Numerical Analysis and Computing CS57 Numerical Aalysis ad Computig Lecture Locatig Roots o Equatios Proessor Ju Zhag Departmet o Computer Sciece Uiversity o Ketucky Leigto KY 456-6 Jauary 9 9 What is the Root May physical system ca be

More information

Notes for Lecture 5. 1 Grover Search. 1.1 The Setting. 1.2 Motivation. Lecture 5 (September 26, 2018)

Notes for Lecture 5. 1 Grover Search. 1.1 The Setting. 1.2 Motivation. Lecture 5 (September 26, 2018) COS 597A: Quatum Cryptography Lecture 5 (September 6, 08) Lecturer: Mark Zhadry Priceto Uiversity Scribe: Fermi Ma Notes for Lecture 5 Today we ll move o from the slightly cotrived applicatios of quatum

More information

Numerical Methods in Fourier Series Applications

Numerical Methods in Fourier Series Applications Numerical Methods i Fourier Series Applicatios Recall that the basic relatios i usig the Trigoometric Fourier Series represetatio were give by f ( x) a o ( a x cos b x si ) () where the Fourier coefficiets

More information

ANALYTICAL SOLUTIONS TO SINE-GORDON EQUATION WITH VARIABLE COEFFICIENT

ANALYTICAL SOLUTIONS TO SINE-GORDON EQUATION WITH VARIABLE COEFFICIENT Romaia Reports i Physics, Vol. 66, No., P. 6 73, 4 ANALYICAL SOLUIONS O SINE-GORDON EQUAION WIH VARIABLE COEFFICIEN ZHENGPING YANG, WEI-PING ZHONG,,* Shude Polytechic, Departmet of Electroic ad Iformatio

More information

The Wave Function and Quantum Reality

The Wave Function and Quantum Reality The Wave Fuctio ad Quatum Reality Sha Gao Uit for History ad Philosophy of Sciece & Cetre for Time, SOPHI Uiversity of Sydey, Sydey, NSW 006, Australia Abstract. We ivestigate the meaig of the wave fuctio

More information

EE 435. Lecture 25. Data Converters

EE 435. Lecture 25. Data Converters EE 435 Lecture 5 Data Coverters . Review from last lecture. Basic Operatio of CMFB Block V DD V FB V O1 V O CMFB Circuit V FB V OUT C L M 3 M 4 V OUT V IN M 1 M V IN C L V OXX CMFB Circuit V B M 9 V OXX

More information

Rabi oscillations and stimulated mode conversion on the subwavelength scale

Rabi oscillations and stimulated mode conversion on the subwavelength scale Rabi oscillatios ad stiulated ode coversio o the subwavelegth scale Xiao Zhag, 1,2 Fagwei Ye, 1,2,* Yaroslav V. Kartashov, 3 ad Xiafeg Che 1,2 1 Departet of Physics ad Astrooy, Shaghai Jiao Tog Uiversity,

More information

PHY4905: Nearly-Free Electron Model (NFE)

PHY4905: Nearly-Free Electron Model (NFE) PHY4905: Nearly-Free Electro Model (NFE) D. L. Maslov Departmet of Physics, Uiversity of Florida (Dated: Jauary 12, 2011) 1 I. REMINDER: QUANTUM MECHANICAL PERTURBATION THEORY A. No-degeerate eigestates

More information

NEW IDENTIFICATION AND CONTROL METHODS OF SINE-FUNCTION JULIA SETS

NEW IDENTIFICATION AND CONTROL METHODS OF SINE-FUNCTION JULIA SETS Joural of Applied Aalysis ad Computatio Volume 5, Number 2, May 25, 22 23 Website:http://jaac-olie.com/ doi:.948/252 NEW IDENTIFICATION AND CONTROL METHODS OF SINE-FUNCTION JULIA SETS Jie Su,2, Wei Qiao

More information

CS321. Numerical Analysis and Computing

CS321. Numerical Analysis and Computing CS Numerical Aalysis ad Computig Lecture Locatig Roots o Equatios Proessor Ju Zhag Departmet o Computer Sciece Uiversity o Ketucky Leigto KY 456-6 September 8 5 What is the Root May physical system ca

More information

Introduction of Surface Acoustic Wave (SAW) Devices

Introduction 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 information

Nonlinear Optics and Gap Solitons in Periodic Photonic Structures

Nonlinear Optics and Gap Solitons in Periodic Photonic Structures Nonlinear Optics and Gap Solitons in Periodic Photonic Structures Yuri Kivshar Nonlinear Physics Centre Research School of Physical Sciences and Engineering Australian National University Perspectives

More information

ECE594I Notes set 13: Two-port Noise Parameters

ECE594I Notes set 13: Two-port Noise Parameters C594 otes, M. Rodwell, copyrighted C594 Notes set 13: Two-port Noise Parameters Mark Rodwell Uiversity of Califoria, Sata Barbara rodwell@ece.ucsb.edu 805-893-3244, 805-893-3262 fax Refereces ad Citatios:

More information

DIGITAL MEASUREMENT OF POWER SYSTEM HARMONIC MAGNITUDE AND PHASE ANGLE

DIGITAL MEASUREMENT OF POWER SYSTEM HARMONIC MAGNITUDE AND PHASE ANGLE DIGIL MESUREMEN OF POWER SYSEM HRMONIC MGNIUDE ND PHSE NGLE R Micheletti (, R Pieri ( ( Departmet of Electrical Systems ad utomatio, Uiversity of Pisa, Via Diotisalvi, I-566 Pisa, Italy Phoe +39 5 565,

More information

Infinite Series and Improper Integrals

Infinite Series and Improper Integrals 8 Special Fuctios Ifiite Series ad Improper Itegrals Ifiite series are importat i almost all areas of mathematics ad egieerig I additio to umerous other uses, they are used to defie certai fuctios ad to

More information

a b c d e f g h Supplementary Information

a 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 information

The Quest for Efficiency

The Quest for Efficiency CST8130: Data Structures Algorithm Efficiecy ad the Big-O Created by Rex Woollard Use PageUp ad PageDow to move from scree to scree. Olie use arrow buttos. Click o speaker to play soud. The Quest for Efficiecy

More information

Optical Devices for High Speed Communication Systems. Lecture Notes

Optical 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 information

Toy models for Rayleigh- Taylor instability:

Toy models for Rayleigh- Taylor instability: Toy models for Rayleigh- Taylor istability: Stuart Dalziel Departmet of Applied Mathematics ad Theoretical Physics iversity of Cambridge Iteratioal Workshop o the Physics of Compressible Turbulet Mixig

More information

Physics 201 Final Exam December

Physics 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 information

Filter banks. Separately, the lowpass and highpass filters are not invertible. removes the highest frequency 1/ 2and

Filter banks. Separately, the lowpass and highpass filters are not invertible. removes the highest frequency 1/ 2and Filter bas Separately, the lowpass ad highpass filters are ot ivertible T removes the highest frequecy / ad removes the lowest frequecy Together these filters separate the sigal ito low-frequecy ad high-frequecy

More information

Particle Physics Insights

Particle Physics Insights Ope Access: Full ope access to this ad thousads of other papers at http://www.la-press.com. Particle Physics Isights The Harmoic Neutro Hypothesis: Derivatio of the Mass Equivalets of the Quars from the

More information

Some Nonlinear Equations with Double Solutions: Soliton and Chaos

Some Nonlinear Equations with Double Solutions: Soliton and Chaos Some Noliear Equatios with Double Solutios: Solito a Chaos Yi-Fag Chag Departmet of Physics, Yua Uiversity, Kumig, 659, Chia (E-mail: yifagchag@hotmail.com) Abstract The fuametal characteristics of solito

More information

AIT. Blackbody Radiation IAAT

AIT. Blackbody Radiation IAAT 3 1 Blackbody Radiatio Itroductio 3 2 First radiatio process to look at: radiatio i thermal equilibrium with itself: blackbody radiatio Assumptios: 1. Photos are Bosos, i.e., more tha oe photo per phase

More information

Polariton resonances in multilayered piezoelectric superlattices

Polariton 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 information

Abstract. Donald William Chakeres. Department of Radiology, The Ohio State University, Columbus, OH, USA

Abstract. Donald William Chakeres. Department of Radiology, The Ohio State University, Columbus, OH, USA Joural of Moder Physics, 014, 5, 1670-1683 Published Olie October 014 i SciRes. http://www.scirp.org/joural/jmp http://dx.doi.org/10.436/jmp.014.516167 Predictio ad Derivatio of the Higgs Boso from the

More information

REPORT DOCUMENTATION PAGE Form Approved OMB No

REPORT DOCUMENTATION PAGE Form Approved OMB No REPORT DOCUMENTATION PAGE Form Approved OMB No. 74-188 Public reportig burde for this collectio of iformatio is estimated to average 1 hour per respose, icludig the time for reviewig istructios, searchig

More information

Observation of discrete quadratic surface solitons

Observation of discrete quadratic surface solitons Observation of discrete quadratic surface solitons Georgios A. Siviloglou, Konstantinos G. Makris, Robert Iwanow, Roland Schiek, Demetrios N. Christodoulides and George I. Stegeman College of Optics and

More information

Multiphoton absorption cross section and virtual-state spectroscopy for the entangled n-photon state

Multiphoton absorption cross section and virtual-state spectroscopy for the entangled n-photon state PHYSICAL REVIEW A VOLUME 57, NUMBER 5 MAY 998 Multiphoto absorptio cross sectio ad virtual-state spectroscopy for the etagled -photo state Ja Peřia, Jr.,* Bahaa E. A. Saleh, ad Malvi C. Teich Quatum Imagig

More information

Exercises and Problems

Exercises 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 information

Modified Logistic Maps for Cryptographic Application

Modified Logistic Maps for Cryptographic Application Applied Mathematics, 25, 6, 773-782 Published Olie May 25 i SciRes. http://www.scirp.org/joural/am http://dx.doi.org/.4236/am.25.6573 Modified Logistic Maps for Cryptographic Applicatio Shahram Etemadi

More information

Application of Homotopy Perturbation Method for the Large Angle period of Nonlinear Oscillator

Application of Homotopy Perturbation Method for the Large Angle period of Nonlinear Oscillator Applicatio of Homotopy Perturbatio Method for the Large Agle period of Noliear Oscillator Olayiwola, M. O. Gbolagade A.W., Adesaya A.O. & Akipelu F.O. Departmet of Mathematical Scieces, Faculty of Sciece,

More information

ECONOMIC OPERATION OF POWER SYSTEMS

ECONOMIC OPERATION OF POWER SYSTEMS ECOOMC OEATO OF OWE SYSTEMS TOUCTO Oe of the earliest applicatios of o-lie cetralized cotrol was to provide a cetral facility, to operate ecoomically, several geeratig plats supplyig the loads of the system.

More information

Formation of A Supergain Array and Its Application in Radar

Formation of A Supergain Array and Its Application in Radar Formatio of A Supergai Array ad ts Applicatio i Radar Tra Cao Quye, Do Trug Kie ad Bach Gia Duog. Research Ceter for Electroic ad Telecommuicatios, College of Techology (Coltech, Vietam atioal Uiversity,

More information

CDS 101: Lecture 5.1 Controllability and State Space Feedback

CDS 101: Lecture 5.1 Controllability and State Space Feedback CDS, Lecture 5. CDS : Lecture 5. Cotrollability ad State Space Feedback Richard M. Murray 8 October Goals: Deie cotrollability o a cotrol system Give tests or cotrollability o liear systems ad apply to

More information

Quantum Simulation: Solving Schrödinger Equation on a Quantum Computer

Quantum Simulation: Solving Schrödinger Equation on a Quantum Computer Purdue Uiversity Purdue e-pubs Birc Poster Sessios Birc Naotechology Ceter 4-14-008 Quatum Simulatio: Solvig Schrödiger Equatio o a Quatum Computer Hefeg Wag Purdue Uiversity, wag10@purdue.edu Sabre Kais

More information

Numerical Simulation of Thermomechanical Problems in Applied Mechanics: Application to Solidification Problem

Numerical Simulation of Thermomechanical Problems in Applied Mechanics: Application to Solidification Problem Leoardo Joural of Scieces ISSN 1583-0233 Issue 9, July-December 2006 p. 25-32 Numerical Simulatio of Thermomechaical Problems i Applied Mechaics: Applicatio to Solidificatio Problem Vicet Obiajulu OGWUAGWU

More information

EE 435. Lecture 25. Data Converters. Architectures. Characterization

EE 435. Lecture 25. Data Converters. Architectures. Characterization EE 435 Lecture 5 Data Coverters Architectures Characterizatio . eview from last lecture. Data Coverters Types: A/D (Aalog to Digital) Coverts Aalog Iput to a Digital Output D/A (Digital to Aalog) Coverts

More information

Zeros of Polynomials

Zeros of Polynomials Math 160 www.timetodare.com 4.5 4.6 Zeros of Polyomials I these sectios we will study polyomials algebraically. Most of our work will be cocered with fidig the solutios of polyomial equatios of ay degree

More information

Problem Set # 5 Solutions

Problem Set # 5 Solutions MIT./8.4/6.898/8.435 Quatum Iformatio Sciece I Fall, 00 Sam Ocko October 5, 00 Problem Set # 5 Solutios. Most uitar trasforms are hard to approimate. (a) We are dealig with boolea fuctios that take bits

More information

Free Space Optical Wireless Communications under Turbulence Channel Effect

Free 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 information

Experimental and theoretical problems:

Experimental and theoretical problems: Workshop o Nuclear Physics, Beijig, September 211 2 t p 6 He 5 H Experimetal ad theoretical problems: We ca ot rely o the theory predictios Reactio mechaism affects the shape of the spectra The overlappig

More information

Map as Outcomes of Processes. Outline. Map as Outcomes of Processes

Map as Outcomes of Processes. Outline. Map as Outcomes of Processes Map as Outcomes of Processes Outlie Defiitios: processes & patters A Startig poit: Complete Spatial Radomess More defiitio: Statioary Map as Outcomes of Processes The basic assumptio of Spatial Aalysis:

More information

A Brief Introduction to the Physical Basis for Electron Spin Resonance

A 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 information

Lecture 3. Digital Signal Processing. Chapter 3. z-transforms. Mikael Swartling Nedelko Grbic Bengt Mandersson. rev. 2016

Lecture 3. Digital Signal Processing. Chapter 3. z-transforms. Mikael Swartling Nedelko Grbic Bengt Mandersson. rev. 2016 Lecture 3 Digital Sigal Processig Chapter 3 z-trasforms Mikael Swartlig Nedelko Grbic Begt Madersso rev. 06 Departmet of Electrical ad Iformatio Techology Lud Uiversity z-trasforms We defie the z-trasform

More information

Discrete gap solitons in a diffraction-managed waveguide array

Discrete gap solitons in a diffraction-managed waveguide array Uiversity of Massachusetts Amherst ScholarWorks@UMass Amherst Mathematics ad Statistics Departmet Faculty ublicatio Series Mathematics ad Statistics Discrete gap solitos i a diffractio-maaged waveguide

More information

Vibrational Spectroscopy 1

Vibrational Spectroscopy 1 Applied Spectroscopy Vibratioal Spectroscopy Recommeded Readig: Bawell ad McCash Chapter 3 Atkis Physical Chemistry Chapter 6 Itroductio What is it? Vibratioal spectroscopy detects trasitios betwee the

More information

. (24) If we consider the geometry of Figure 13 the signal returned from the n th scatterer located at x, y is

. (24) If we consider the geometry of Figure 13 the signal returned from the n th scatterer located at x, y is .5 SAR SIGNA CHARACTERIZATION I order to formulate a SAR processor we first eed to characterize the sigal that the SAR processor will operate upo. Although our previous discussios treated SAR cross-rage

More information