Slides:



Advertisements
Similar presentations
Today’s summary Polarization Energy / Poynting’s vector
Advertisements

Matrix Representation
Net vibration at point P:
Introduction to Quantum Information Processing CS 467 / CS 667 Phys 467 / Phys 767 C&O 481 / C&O 681 Lecture 11 (2005) Richard Cleve DC 3524
Chapters 14 & 18: Matrix methods. Welcome to the Matrix.
Properties of Multilayer Optics An Investigation of Methods of Polarization Analysis for the ICS Experiment at UCLA 8/4/04 Oliver Williams.
Physics 1402: Lecture 33 Today’s Agenda Announcements: –Midterm 2: graded after Thanks Giving –Homework 09: Friday December 4 Optics –interference.
Optically polarized atoms
Dirac Notation and Spectral decomposition
Chapter 18 Superposition and Standing Waves. Waves vs. Particles Waves are very different from particles. Particles have zero size.Waves have a characteristic.
Chapter 5 Jones Calculus and Its Application to Birefringent Optical Systems Lecture 1 Wave plates Wave plates (retardation plates) are optical elements.
Lecture 15 Interference Chp. 35
States, operators and matrices Starting with the most basic form of the Schrödinger equation, and the wave function (  ): The state of a quantum mechanical.
OPTICAL MINERALOGY Dr. AZZA RAGAB.
Lecture 15 Interference Chp. 35 Topics –Interference from thin films –Due to the wave nature of light –Change in wavelength and phase change in a medium.
CHAPTER 37 : INTERFERENCE OF LIGHT WAVES
EXAMPLE Young’s double-slit experiment is performed with 589-nm light and a distance of 2.00 m between the slits and the screen. The tenth interference.
ConcepTest 22.5 Heat Insulation
Chapter 24 Wave Optics. General Physics Review – waves T=1/f period, frequency T=1/f period, frequency v = f velocity, wavelength v = f velocity, wavelength.

Quantum One: Lecture Representation Independent Properties of Linear Operators 3.
Silicon chip birefringence
Interference in Thin Films, final
Doc.: IEEE /0431r0 Submission April 2009 Alexander Maltsev, Intel CorporationSlide 1 Polarization Model for 60 GHz Date: Authors:
Lecture Nine: Interference of Light Waves: I
Electromagnetic waves: Reflection, Refraction and Interference
Reflection and Refraction A short overview. Plane wave A plane wave can be written as follows: Here A represent the E or B fields, q=i,r,t and j=x,y,z.
Fundamental Physics II PETROVIETNAM UNIVERSITY FACULTY OF FUNDAMENTAL SCIENCES Vungtau, 2013 Phamj Hong Quang
8.4.2 Quantum process tomography 8.5 Limitations of the quantum operations formalism 量子輪講 2003 年 10 月 16 日 担当:徳本 晋
Angular Momentum Classical radius vector from origin linear momentum determinant form of cross product Copyright – Michael D. Fayer, 2007.
Conditions for Interference
Polarization Jones vector & matrices
Initially in medium with lower nInitially in medium with higher n Reflection at interfacePhase shift of πNo phase shift Transmission at interfaceNo phase.
Chapter 4 Two-Level Systems, Spin. Two-level systems Let us start with the simplest non-trivial state space, with only two dimensions Despite its simplicity,
GEOMETRICAL OPTICS. Laws of Reflection Laws of Refraction.
Chapter 9 Spin. Total angular momentum Let us recall key results for the total angular momentum 6.B.2 6.C.1.
6  When waves are combined in systems with boundary conditions, only certain allowed frequencies can exist. › We say the frequencies are quantized.
Chapter 24 Wave Optics. Young’s Double Slit Experiment Thomas Young first demonstrated interference in light waves from two sources in Light is.
Silicon chip birefringence. Jones Matrix JM for linear polarizer Horizontal transmission (trans. axis along x) Vertical transmission (trans. axis along.
Chapter 5 Jones Calculus and Its Application to Birefringent Optical Systems Lecture 1 Wave plates Wave plates (retardation plates) are optical elements.
17. Electromagnetic waves
Today’s agenda: Thin Film Interference.
Interference of Light Waves
Angular Momentum Classical radius vector from origin linear momentum
Light Waves in 2D SPH4U.
Quantum One.
QM1 Concept Test 9.1 Consider the following statements for the product space of two spin systems:
Quantum Two.
2-D Geometry.
Announcements I should have exams back to you on Fri.
PRISMS – one of the e.g. of optical instrumentation
Quantum One.
Interference of Light Waves
Chapter 4 Two-Level Systems.
Reflection Refractive index Snell's law Optical power Lens equation
DIRECT STIFFNESS METHOD FOR TRUSSES:
QM1 Concept test 8.1 If the total spin quantum number for the system is
QM1 Concept Test 9.1 Consider the following statements for the product space of a two spin-1/2 system:
Choose all of the following observables for which it will be convenient to use the coupled representation to find the probabilities of different outcomes.
Handout 4 : Electron-Positron Annihilation
Maths for Signals and Systems Linear Algebra in Engineering Lectures 13 – 14, Tuesday 8th November 2016 DR TANIA STATHAKI READER (ASSOCIATE PROFFESOR)
Polarization Superposition of plane waves
Matrix treatment of polarization
Light and Lenses While Mirrors involve the reflection of light and the images we see, Lenses involve another property of light, refraction, or the effects.
Categories of Optical Elements that modify states of polarization:
DR MOHAMAD HALIM ABD. WAHID School of Microelectronic Engineering
A water wave is incident on a breakwater as sketched below
Linear Vector Space and Matrix Mechanics
QM2 Concept Test 10.1 Consider the Hamiltonian
Presentation transcript:

𝐿 𝑈 𝐿 𝑈 𝐿 𝑈 Figure 1 Figure 2 Figure 3 For all of the following questions, Assume that the source emits a highly collimated stream of photons (photons emitted as a single ray having an infinitesimally small width). “Which-path” information is known when each detector D1 and D2 shown below can only project the component of the photon state from the U path or the L path. Choose a basis in which the state of the photon from the source towards BS1 can be represented by 𝑈 = 1 0 (see Figure 1) or 𝐿 = 0 1 (see figure 2) inside the MZI is represented by 𝑈 = 1 0 along the upper path state and 𝐿 = 0 1 along the lower path state (see Figure 3). propagating towards detector D1 is represented as path state 𝑈 = 1 0 and the state of the photon propagating towards detector D2 is represented as path state 𝐿 = 0 1 (see Figure 3). 𝐿 𝑈 𝐿 𝑈 𝐿 𝑈 Figure 1 Figure 2 Figure 3

Summary of phase shifts   Initially in medium with lower n Initially in medium with higher n Reflection at interface Phase shift of π No phase shift Transmission at interface Propagation through a medium Phase shift depending on thickness and refractive index 𝑛 of medium

The matrix corresponding to BS1 is [BS1]= 1 2 −1 1 −1 1 Choose all of the following statements that are correct about the matrix representation of the operator corresponding to BS1. Assume that the basis vectors are in the order 𝑈 , 𝐿 . The matrix corresponding to BS1 is [BS1]= 1 2 −1 1 −1 1 The matrix corresponding to BS1 is [BS1]= 1 2 −1 1 1 1 BS1 evolves the photon state from the source shown into a superposition of the U and L path states. The matrix corresponding to the operator BS1 should incorporate a negative sign due to the BS1 operator causing a reflection in the upper path inside MZI and should have no sign change due to BS1 causing transmission to the lower path inside MZI. I only B. II only C. III only D. I and III only E. II and III only   𝐿 𝑈 𝑈 𝐿

I only B. II only C. III only D. I and III only E. II and III only Choose all of the following statements that are correct about the matrix representation of the operator corresponding to BS2. Assume that the basis vectors are in the order 𝑈 , 𝐿 to construct the matrices. 𝑈 𝐵𝑆2 𝐿 =− 1 2 𝐿 𝐵𝑆2 𝐿 =− 1 2 The matrix corresponding to operator BS2 should incorporate a negative sign due to the BS2 operator causing a reflection of the lower path state inside MZI to upper path state towards D1. I only B. II only C. III only D. I and III only E. II and III only 𝐿 𝑈 𝑈 𝐿

I only B. II only C. III only D. I and III only E. II and III only Choose all of the following statements that are correct about the matrix representation of the mirror operators. Assume that the basis vectors are in the order 𝑈 , 𝐿 to construct the matrices. [M1]= 1 0 0 −1 𝐿 𝑀2 𝑈 =1 The mirror operators corresponding to Mirror 1 and Mirror 2 operate on two different components of photon state, i.e., the upper path state and lower path state of the photon. Therefore, the mirror operators [M1] and [M2] commute and we can combine the mirror operators to find the net effect of the mirrors on the photon state, i.e., [M]=[M1][M2]. I only B. II only C. III only D. I and III only E. II and III only 𝐿 𝑈 𝑈 𝐿

I only B. I and II only C. I and III only D. II and III only Choose all of the following statements that are correct about the matrix representation of the phase shifter operator that introduces a phase shift of 𝜑 𝑃𝑆 to the component of the photon state in the U path. Assume that the basis vectors are in the order 𝑈 , 𝐿 to construct the matrices. 𝑃𝑆 𝑈 = 𝑒 𝑖𝜑 𝑃𝑆 0 0 1 The operator corresponding to a phase shifter in the upper path does NOT affect the lower path state (it is equivalent to an identity operator in the lower path). The operator corresponding to a phase shifter in the upper path is a time evolution operator and must be a unitary operator to preserve the norm of the photon state. I only B. I and II only C. I and III only D. II and III only E. All of the above Phase shifter 𝐿 𝑈 𝑈 𝐿

Choose all of the following statements that are true about the operators corresponding to BS1, BS2, the mirrors, and the phase shifter. Note: If an operator 𝑈 is Hermitian, then 𝑈= 𝑈 † = 𝑈 𝑇 ∗ . If an operator 𝑈 is unitary, then 𝑈 † 𝑈= 𝐼 , where 𝐼 is the identity operator. The operators corresponding to BS1, BS2, the mirrors, and the phase shifter are Hermitian operators because they satisfy the condition 𝑈= 𝑈 † . The operators corresponding to BS1, BS2, the mirrors, and the phase shifter are Hermitian operators because they correspond to physical observables. The operators corresponding to BS2, BS2, the mirrors, and the phase shifter are unitary because they are all time evolution operators and must preserve the norm of the state. A. III only B. I and II only C. I and III only D. II and III only E. all of the above 𝐿 𝑈 𝑈 𝐿

The probability that detector D1 clicks is 𝑈 Ψ . Choose all of the following statements that are correct about the the photon at the detector for the setup shown below. The photon originates from the source in the initial state 𝑈 (see figure below). The final state of the photon before it is detected by a detector is Ψ = 1 2 1+ 𝑒 𝑖 𝜑 𝑃𝑆 1− 𝑒 𝑖 𝜑 𝑃𝑆 , where 𝜑 𝑃𝑆 is the phase shift of the phase shifter. The probability that detector D1 clicks is 𝑈 Ψ . “Which-path” information is unknown because each detector D1 and D2 can project both components of the photon state along the U path or the L path. There is interference displayed at the detectors and the probability that detector D1 or D2 clicks depends on 𝜑 𝑃𝑆 . A. I only B. I and II only C. I and III only D. II and III only E. all of the above 𝐿 𝑈 𝑈 𝐿

Choose all of the following statements that are correct about the photon for the setup shown below (BS2 is removed from the setup). The photon originates from the source in the initial state 𝑈 (see figure below). The final state of the photon before it is detected by a detector D1 or D2 is Ψ = 1 2 1 −𝑒 𝑖 𝜑 𝑃𝑆 , where 𝜑 𝑃𝑆 is the phase shift of the phase shifter. The probability that detector D1 registers a photon is 1 2 . “Which-path” information is known because each detector D1 and D2 can only project the component of the photon state along the U path or the L path. There is interference displayed at detector D2 and probability of the detector D2 clicking, 𝐿 Ψ 2 , depends on the phase shift of the phase shifter 𝜑 𝑃𝑆 . A. I only B. I and II only C. I and III only D. II and III only E. all of the above

For all of the following questions, we will now include the polarization state of the single photon along with the path state. Choose a basis in which the polarization state of the vertically polarized photon is represented as 𝑉 = 1 0 and the polarization state of the horizontally polarized photon is represented as 𝐻 = 0 1 . We will always use the following convention for the order of the basis vectors when determining all the 4×4 matrices corresponding to the optical elements (BS1, BS2, mirrors, phase shifter, and polarizers) in the product space: 𝑈 𝑉 , 𝑈𝐻 , 𝐿 𝑉 , 𝐿 𝐻 .

Choose all of the following statements that are correct about the matrix representation of BS1 in the 4×4 product space involving both photon path states and polarization states. Assume that basis vectors are chosen in the order 𝑈 𝑉 , 𝑈𝐻 , 𝐿 𝑉 , 𝐿 𝐻 . The BS1 operator affects the polarization state of the single photons. If the BS1 matrix in the 2×2 space involving only the photon path states is given as follows, then the [BS1] matrix in the 4×4 product space involving both photon path states and polarization states is represented by 𝐵𝑆1 = 1 2 −1 1 1 1 → 𝐵𝑆1 = 1 2 −1 0 1 0 0 −1 0 1 1 0 1 0 0 1 0 1 III. The matrix elements of BS1 that mix different polarizations, e.g., 𝑈𝐻 𝐵𝑆2 𝑈𝑉 and 𝑈𝐻 𝐵𝑆2 𝐿𝑉 , are 0. A. I only B. I and II only C. I and III only D. II and III only E. all of the above

Which one of the following matrices is the correct matrix representation of BS2 in the 4×4 product space involving both single photon path states and polarization states? Assume that basis vectors are chosen in the order 𝑈 𝑉 , 𝑈𝐻 , 𝐿 𝑉 , 𝐿 𝐻 . Hint: The matrix representation of BS2 in the 2×2 space involving only the single photon path states is [BS2]= 1 2 1 −1 1 1 . 𝐵𝑆2 = 1 2 1 0 −1 0 0 1 0 1 1 0 1 0 0 1 0 1 𝐵𝑆2 = 1 2 1 0 1 0 0 1 0 1 1 0 −1 0 0 1 0 −1 𝐵𝑆2 = 1 2 1 0 −1 0 0 1 0 −1 1 0 1 0 0 1 0 1 D. 𝐵𝑆2 = 1 2 1 0 1 0 0 1 0 −1 1 0 1 0 0 1 0 1 E. 𝐵𝑆2 = 1 2 1 0 1 0 0 1 0 1 1 0 1 0 0 1 0 1

The normalized state of a +45° polarized photon (not taking into account path states) can be written as an equal superposition of the states 𝑉 and 𝐻 as follows: 45° = 1 2 𝑉 + 𝐻 = 1 2 1 0 + 0 1 = 1 2 1 1 . Which one of the following represents the state of a + 45° polarized photon emitted from the source shown below? 𝑈 ⊗ 45° = 1 2 2 1 𝑈 ⊗ 45° = 1 2 1 0 1 0 𝑈 ⊗ 45° = 1 2 1 0 0 0 D. 𝑈 ⊗ 45° = 1 2 0 1 1 0 E. 𝑈 ⊗ 45° = 1 2 1 1 0 0 source