G x, x E x E x E x E x. a a a a. is some matrix element. For a general single photon state. ), applying the operators.

Similar documents
, so the state may be taken to be l S ÅÅÅÅ

In an algebraic expression of the form (1), like terms are terms with the same power of the variables (in this case

Intermediate Applications of Vectors and Matrices Ed Stanek

CHAPTER 7 SYMMETRICAL COMPONENTS AND REPRESENTATION OF FAULTED NETWORKS

ELEC 372 LECTURE NOTES, WEEK 6 Dr. Amir G. Aghdam Concordia University

UNIT #5 SEQUENCES AND SERIES COMMON CORE ALGEBRA II

Schrödinger Equation Via Laplace-Beltrami Operator

APPLICATION OF DIFFERENCE EQUATIONS TO CERTAIN TRIDIAGONAL MATRICES

ALGEBRA II CHAPTER 7 NOTES. Name

Chapter #3 EEE Subsea Control and Communication Systems

Chapter 2 Infinite Series Page 1 of 9

Observations on the Non-homogeneous Quintic Equation with Four Unknowns

, we would have a series, designated as + j 1

10.2 Series. , we get. which is called an infinite series ( or just a series) and is denoted, for short, by the symbol. i i n

( a n ) converges or diverges.

Math 153: Lecture Notes For Chapter 1

2.Decision Theory of Dependence

Note 7 Root-Locus Techniques

Fourier Series and Applications

Sequence and Series of Functions

Chapter #5 EEE Control Systems

Approximations of Definite Integrals

Modified Farey Trees and Pythagorean Triples

Tranformations. Some slides adapted from Octavia Camps

INFINITE SERIES. ,... having infinite number of terms is called infinite sequence and its indicated sum, i.e., a 1

Taylor Polynomials. The Tangent Line. (a, f (a)) and has the same slope as the curve y = f (x) at that point. It is the best

Summer MA Lesson 4 Section P.3. such that =, denoted by =, is the principal square root

MATH 118 HW 7 KELLY DOUGAN, ANDREW KOMAR, MARIA SIMBIRSKY, BRANDEN LASKE

On Almost Increasing Sequences For Generalized Absolute Summability

Laplace s equation in Cylindrical Coordinates

PROGRESSIONS AND SERIES

FOURIER SERIES PART I: DEFINITIONS AND EXAMPLES. To a 2π-periodic function f(x) we will associate a trigonometric series. a n cos(nx) + b n sin(nx),

Linear predictive coding

Certain sufficient conditions on N, p n, q n k summability of orthogonal series

Notes 17 Sturm-Liouville Theory

Chapter 7. , and is unknown and n 30 then X ~ t n

Artificial Intelligence Markov Decision Problems

A Level Mathematics Transition Work. Summer 2018

MASSACHUSETTS INSTITUTE of TECHNOLOGY Department of Mechanical Engineering 2.71/ OPTICS - - Spring Term, 2014

UNIVERSITY OF BRISTOL. Examination for the Degrees of B.Sc. and M.Sci. (Level C/4) ANALYSIS 1B, SOLUTIONS MATH (Paper Code MATH-10006)

Chapter #2 EEE Subsea Control and Communication Systems

Particle in a Box. and the state function is. In this case, the Hermitian operator. The b.c. restrict us to 0 x a. x A sin for 0 x a, and 0 otherwise

Name: Period: Date: 2.1 Rules of Exponents

Definite Integral. The Left and Right Sums

0 otherwise. sin( nx)sin( kx) 0 otherwise. cos( nx) sin( kx) dx 0 for all integers n, k.

The Weierstrass Approximation Theorem

Introduction to Modern Control Theory

The total number of permutations of S is n!. We denote the set of all permutations of S by

THE CONCEPT OF THE ROOT LOCUS. H(s) THE CONCEPT OF THE ROOT LOCUS

EXERCISE a a a 5. + a 15 NEETIIT.COM

Fig. 1. I a. V ag I c. I n. V cg. Z n Z Y. I b. V bg

Numbers (Part I) -- Solutions

Probability and Stochastic Processes: A Friendly Introduction for Electrical and Computer Engineers Roy D. Yates and David J.

A GENERAL METHOD FOR SOLVING ORDINARY DIFFERENTIAL EQUATIONS: THE FROBENIUS (OR SERIES) METHOD

DETERMINANT. = 0. The expression a 1. is called a determinant of the second order, and is denoted by : y + c 1

SUTCLIFFE S NOTES: CALCULUS 2 SWOKOWSKI S CHAPTER 11

5.74 TIME-DEPENDENT QUANTUM MECHANICS

Statistics for Financial Engineering Session 1: Linear Algebra Review March 18 th, 2006

Con Lin Lon+ n. mlfmtm EYE. [ Lm. algebra. get for me 2 : Exercised. follows by. ( Lm Ln. follows forin> o. Ken : Ln IX > Luan -173cm ' sheet 9

20.2. The Transform and its Inverse. Introduction. Prerequisites. Learning Outcomes

ELEG 3143 Probability & Stochastic Process Ch. 5 Elements of Statistics

MORE COMMUTATOR INEQUALITIES FOR HILBERT SPACE OPERATORS

Review of the Riemann Integral

PRIMARY DECOMPOSITION, ASSOCIATED PRIME IDEALS AND GABRIEL TOPOLOGY

Lesson-2 PROGRESSIONS AND SERIES

Discrete Mathematics and Probability Theory Spring 2016 Rao and Walrand Lecture 17

Do the one-dimensional kinetic energy and momentum operators commute? If not, what operator does their commutator represent?

Week 13 Notes: 1) Riemann Sum. Aim: Compute Area Under a Graph. Suppose we want to find out the area of a graph, like the one on the right:

Chap8 - Freq 1. Frequency Response

( ) k ( ) 1 T n 1 x = xk. Geometric series obtained directly from the definition. = 1 1 x. See also Scalars 9.1 ADV-1: lim n.

Chapter 5. The Riemann Integral. 5.1 The Riemann integral Partitions and lower and upper integrals. Note: 1.5 lectures

LEVEL I. ,... if it is known that a 1

MATRIX ALGEBRA, Systems Linear Equations

New data structures to reduce data size and search time

Student Success Center Elementary Algebra Study Guide for the ACCUPLACER (CPT)

g as the function in which for every element x be the set of polynomials of a degree less than or equal to n with , for each i from 0 to n )

Convergence rates of approximate sums of Riemann integrals

ROUTH-HURWITZ CRITERION

Summer Math Requirement Algebra II Review For students entering Pre- Calculus Theory or Pre- Calculus Honors

MA123, Chapter 9: Computing some integrals (pp )

* power rule: * fraction raised to negative exponent: * expanded power rule:

Calculus II Homework: The Integral Test and Estimation of Sums Page 1

POWER SERIES R. E. SHOWALTER

Name Solutions to Test 3 November 8, 2017

Qn Suggested Solution Marking Scheme 1 y. G1 Shape with at least 2 [2]

Graphing Review Part 3: Polynomials

z line a) Draw the single phase equivalent circuit. b) Calculate I BC.

Chem 253A. Crystal Structure. Chem 253B. Electronic Structure

Solutions to Problem Set 7

OXFORD H i g h e r E d u c a t i o n Oxford University Press, All rights reserved.

Double Sums of Binomial Coefficients

Asymptotic Properties of Solutions of Two Dimensional Neutral Difference Systems

1.3 Continuous Functions and Riemann Sums

Proc. of the 8th WSEAS Int. Conf. on Mathematical Methods and Computational Techniques in Electrical Engineering, Bucharest, October 16-17,

Surds, Indices, and Logarithms Radical

General properties of definite integrals

F x = 2x λy 2 z 3 = 0 (1) F y = 2y λ2xyz 3 = 0 (2) F z = 2z λ3xy 2 z 2 = 0 (3) F λ = (xy 2 z 3 2) = 0. (4) 2z 3xy 2 z 2. 2x y 2 z 3 = 2y 2xyz 3 = ) 2

 n. A Very Interesting Example + + = d. + x3. + 5x4. math 131 power series, part ii 7. One of the first power series we examined was. 2!

Motions of Infinite Mass-Spring Systems

Available at Appl. Appl. Math. ISSN: Vol. 4, Issue 1 (June 2009) pp (Previously, Vol. 4, No.

Transcription:

Topic i Qutu Optic d Qutu Ifortio TA: Yuli Mxieko Uiverity of Illioi t Urb-hpig lt updted Februry 6 Proble Set # Quetio With G x, x E x E x E x E x G pqr p q r where G pqr i oe trix eleet For geerl igle photo tte k k k f (with fk ), pplyig the opertor r will ecerily ihilte the tte, ie, Thu, we coclude tht r Now coider ited Altertive view G p r q p q r qr p * qr f j fk jpk k, j * qr j k k jp k, j f f * qr p f f For y tte creted by booic cretio opertor, it i Proof: eigette of the totl uber opertor N k k k N N k N k N Therefore tte with differet uber of re orthogol oider y opertor Ô which ct o oly the two-prticle ubpce jk jk j k k j We c lwy write I j, k j, k ˆ ˆ O IOI O pqr pqr r q p Pge of 8

Topic i Qutu Optic d Qutu Ifortio TA: Yuli Mxieko Uiverity of Illioi t Urb-hpig lt updted Februry 6 Note tht O Tr O ˆ pqr r p q Tr O ˆ p q r where Tr i the trce opertor For deity opertor Ô, we the ee tht it i lwy relted to the orl-ordered expecttio vlue Tr p q r p q r Quetio () For, G d G Thu g (b) For, G d G Thu g / (c) For, G (ote tht ) d G Thu g (d) (i) For A e E where E h d / kt B, G ˆ A A A A A h / kbt A e (ii) oider, Pge of 8

Topic i Qutu Optic d Qutu Ifortio TA: Yuli Mxieko Uiverity of Illioi t Urb-hpig lt updted Februry 6 AA A A G A A A A A A A A A A A A A where we iplicitly dded the ter k G A k kq i ech erie, d ued q q q We therefore hve g Quetio H ~ A H H A () Be plitter effect o the tte: i i H H H ; H H ( H H ) where _ d _ e repectively triio d reflectio r of the be plitter Probbilitie for differet outcoe: Detector (triio r): photo (oly) probbility i ~ A/+A /+A / photo probbility ~ A /*, where the fctor of pper becue of the two reolved photo S=A/+A /+A / Detector h the e probbilitie The coicidece cout:,=a /+ A / ( photo o ech detector) (), A / g, if A S S ( A/ A / A / ) / ( A) (b) Exctly the e ) (c) Up to the order A, HV ~ A H H AV V A A VV VV A HV HV, where oe freedo i tke i the tte ottio HV, for exple, e Pge of 8

Topic i Qutu Optic d Qutu Ifortio TA: Yuli Mxieko Uiverity of Illioi t Urb-hpig lt updted Februry 6 H V d e H V i After be plitter, HV HV H V ( HV H V ) Hece, logouly to ), g () S S, A / A ( A/ ( A / A / / ) A A / / A / ) Quetio () oider it it E ( e e ) i ( )co t ( )i t i( X co t X i t) i Thee two opertor re ocited with phe fctor which ocillte out of phe with ech other by /, d hece clled qudrture opertor (b) co, d iilrly * oider X X i Next, X * X So X X X / Siilrly, d hece X / X X Pge of 8

Topic i Qutu Optic d Qutu Ifortio TA: Yuli Mxieko Uiverity of Illioi t Urb-hpig lt updted Februry 6 Altertive ethod With the diplceet opertor D, or equivletly, D The D, we kow tht D D & D D &, o * * D XD X X X D X D X X X i * X X X X Siilrly we foud X / D X X D X Quetio 5 () i i A ( LO LO LO LO LO LO LO LO A ( LO LO) ) (b) A, e i LO LO ), e i A ( e i e i ), uig tht α i rel, o ll the phe i tke ito ccout i e iφ We lo ued the reltio i i i e d e e e i e i e i NB: e i or e i i thi ce e the e (jut ottio) They both repreet br-vector for the ket-tte e i (c) A e i e i i A ( X ix ) e ( X ix ) e i ) A X co X i Pge 5 of 8

Topic i Qutu Optic d Qutu Ifortio TA: Yuli Mxieko Uiverity of Illioi t Urb-hpig lt updted Februry 6 Quetio 6 () Derivig the followig i otrivil detil re give i the ppedix:! S th r coh r! Note tht the odd uber tte re ot preet oe c be coviced by explicitly expdig the queezig opertor S exp r Perhp, it i obviou tht X X, ice the o-zero tte re ll eve uber tte Oe c lo ee thi directly (uig the reult fro prt (c)), ice X oly deped o ter like d, which equl zero (b) Fortutely, to clculte the vrice we do t eed to del with the ey expreio bove We hll eed to obti the propertie of the queezig opertor logou to tht of the diplceet opertor, ie, A A ivoke the forul e Be B A B A A B The, X S X X S S X S S S,,,!, o S S? r,!!! r r r r coh r ih r S S coh r ih r S X SS X S coh ih coh ih r r r r r r e e e e r, r To proceed, we which iplie tht X e r r / Siilrly, X e / Note tht XX / Pge 6 of 8

Topic i Qutu Optic d Qutu Ifortio TA: Yuli Mxieko Uiverity of Illioi t Urb-hpig lt updted Februry 6 Appedix We hll derive for the followig expreio: r /! e th r coh r! Method (ref Gerry & Kight, Itro Qutu Optic) where cohr d ihr SS S S, d S Fro it we hve!! th r!! where the orliztio coditio require The reiig prt re purely rithetic ivolvig oe pecil erie reltio, d hll be kipped (plee refer to the referece for further detil) Method (ref Brett & Rdore, Method i Theoreticl Qutu Optic ) There i geerl theore: for opertor d tifyig K K K, K K & K, K K, K K K K K K exp exp exp l exp where coh ih, ih coh ih d / K / Here oe c how tht, K / d K / tify the couttio reltio tted bove We put r d The Pge 7 of 8

Topic i Qutu Optic d Qutu Ifortio TA: Yuli Mxieko Uiverity of Illioi t Urb-hpig lt updted Februry 6 r, coh r d th r We therefore hve S r r r which give exp th exp l coh exp th,! S th r coh r! Pge 8 of 8