Degree of polarization in quantum optics UCMUCM Luis L. Sánchez-Soto, E. C. Yustas Universidad Complutense. Madrid. Spain Andrei B. Klimov Universidad.

Slides:



Advertisements
Similar presentations
Optics, Eugene Hecht, Chpt. 8
Advertisements

Today’s summary Polarization Energy / Poynting’s vector
II Escuela de Optica Biomedica, Puebla, 2011 Use of polarized light imaging and sensing in the clinical setting Jessica C. Ramella-Roman, PhD.
Chapter 1 Electromagnetic Fields
PHY 042: Electricity and Magnetism Magnetic field in Matter Prof. Hugo Beauchemin 1.
Bose systems: photons, phonons & magnons Photons* and Planck’s black body radiation law
Nonlinear Optics Lab. Hanyang Univ. Chapter 8. Semiclassical Radiation Theory 8.1 Introduction Semiclassical theory of light-matter interaction (Ch. 6-7)
1 Experimental Determination of Crystal Structure Introduction to Solid State Physics
Emergence of Quantum Mechanics from Classical Statistics.
Representation of synchrotron radiation in phase space Ivan Bazarov 1.
Chapters 14 & 18: Matrix methods. Welcome to the Matrix.
Polarization Jones vector & matrices
PHY 042: Electricity and Magnetism Electric field in Matter Prof. Hugo Beauchemin 1.
Evan Walsh Mentors: Ivan Bazarov and David Sagan August 13, 2010.
Analyse de la cohérence en présence de lumière partiellement polarisée François Goudail Laboratoire Charles Fabry de l’Institut d’Optique, Palaiseau (France)
Light and Matter Tim Freegarde School of Physics & Astronomy University of Southampton Controlling light with matter.
Statistical Models in Optical Communications
Polarization Measurements
Optically polarized atoms
Quantum Mechanics from Classical Statistics. what is an atom ? quantum mechanics : isolated object quantum mechanics : isolated object quantum field theory.
Chapter 33 Electromagnetic Waves
March 2, 2011 Fill in derivation from last lecture Polarization of Thomson Scattering No class Friday, March 11.
Lecture 14 (11/13/2006) Analytical Mineralogy Part 1: Nature of Light Introduction to Optical Mineralogy.
School of Physics & Astronomy FACULTY OF MATHEMATICAL & PHYSICAL SCIENCE Parallel Transport & Entanglement Mark Williamson 1, Vlatko Vedral 1 and William.
Chapter 33. Electromagnetic Waves What is Physics? Maxwell's Rainbow The Traveling Electromagnetic Wave, Qualitatively The Traveling.
1 Chapter 4: Polarization of light 2 Preliminaries and definitions Preliminaries and definitions Plane-wave approximation: E(r,t) and B(r,t) are uniform.
Review: Laws of Reflection and Refraction
A Study of The Applications of Matrices and R^(n) Projections By Corey Messonnier.
The Hong Kong Polytechnic University Optics II----by Dr.H.Huang, Department of Applied Physics1 Light Waves Nature of Light: Light can be viewed as both.
Photon angular momentum and geometric gauge Margaret Hawton, Lakehead University Thunder Bay, Ontario, Canada William Baylis, U. of Windsor, Canada.
1 ECE 480 Wireless Systems Lecture 3 Propagation and Modulation of RF Waves.
Chang-Kui Duan, Institute of Modern Physics, CUPT 1 Harmonic oscillator and coherent states Reading materials: 1.Chapter 7 of Shankar’s PQM.
Supervisor: Prof K. Abramski States of polarization of chosen fiber elements.
Geometrical Optics LL2 Section 53. Local propagation vector is perpendicular to wave surface Looks like a plane wave if amplitude and direction are ~constant.
Lecture/Lab: Interaction of light with particles. Mie’s solution.
Doc.: IEEE /0431r0 Submission April 2009 Alexander Maltsev, Intel CorporationSlide 1 Polarization Model for 60 GHz Date: Authors:
Review of Basic Polarization Optics for LCDs Module 4.
Electromagnetic Waves
1 Chapter 2: Geometric Camera Models Objective: Formulate the geometrical relationships between image and scene measurements Scene: a 3-D function, g(x,y,z)
Polarization descriptions of quantized fields Anita Sehat, Jonas Söderholm, Gunnar Björk Royal Institute of Technology Stockholm, Sweden Pedro Espinoza,
DYNAMICS OF OPEN Q-SYSTES FROM A PERSPECTIVE OF QIT IMS, Imperial College, London, 18 January 2007 Vladimír Bužek Research Center for Quantum Information.
Electromagnetism Around 1800 classical physics knew: - 1/r 2 Force law of attraction between positive & negative charges. - v ×B Force law for a moving.
Chapter 3 Polarization of Light Waves
Polarization Jones vector & matrices
PHYS 408 Applied Optics (Lecture 4) JAN-APRIL 2016 EDITION JEFF YOUNG AMPEL RM 113.
Density matrix and its application. Density matrix An alternative of state-vector (ket) representation for a certain set of state-vectors appearing with.
1 Optics of LC displays. 2 Chap.2 Polarization of optical waves.
Hale COLLAGE (CU ASTR-7500) “Topics in Solar Observation Techniques” Lecture 3: Basic concepts in radiative transfer & polarization Spring 2016, Part 1.
Phys 102 – Lecture 16 Electromagnetic wave energy & polarization.
Shanxi University Atomic Physics Chapter 7 The interaction of atoms with radiation Atomic Physics.
Dollan, Laihem, Lohse, Schälicke, Stahl 1 Monte Carlo based studies of polarized positrons source for the International Linear Collider (ILC)
Sect. 4.5: Cayley-Klein Parameters 3 independent quantities are needed to specify a rigid body orientation. Most often, we choose them to be the Euler.
7. Electromagnetic Waves 7A. Plane Waves Consider Maxwell’s Equations with no sources We are going to search for waves of the form To make things as general.
Einstein’s coefficients represent a phenomenological description of the matter-radiation interaction Prescription for computing the values of the A and.
EE231 Introduction to Optics: Basic EM Andrea Fratalocchi ( slide 1 EE 231 Introduction to Optics Review of basic EM concepts Andrea.
Raman Effect The Scattering of electromagnetic radiation by matter with a change of frequency.
Fluctuation properties of chaotic light
Chapter 1 Electromagnetic Fields
Coherent and squeezed states of the radiation field
Review: Laws of Reflection and Refraction
Polarization in spectral lines
Еugene Grichuk, Margarita Kuzmina, Eduard Manykin
Review of basic EM concepts
Polarization P47 – Optics: Unit 5.
Ordinary light versus polarized light
Review of basic EM concepts
Optics 430/530, week I Introduction E&M description
Chapter 33 Electromagnetic Waves
Jaynes-Cummings Hamiltonian
Presentation transcript:

Degree of polarization in quantum optics UCMUCM Luis L. Sánchez-Soto, E. C. Yustas Universidad Complutense. Madrid. Spain Andrei B. Klimov Universidad de Guadalajara. Jalisco. Mexico Gunnar Björk, Jonas Söderholm Royal Institute of Technology. Stockholm. Sweden. Quantum Optics II. Cozumel 2004

Outline Classical description of polarization. Quantum description of polarization. Classical degree of polarization. Quantum assessment of the degree of polarization. UCMUCM

Classical description of polarization Monochromatic plane wave in a linear, homogeneous, isotropic medium E 0 is a complex vector that characterizes the state of polarization linear-polarization basis: (e H, e V ) circular-polarization basis: (e +, e - ) UCMUCM

Stokes parameters Operational interpretation UCMUCM

The Poincaré sphere Coherence vector Poincaré sphere UCMUCM

Transformations on the Poincaré sphere Polarization transformations corresponding transformations in the Poincaré sphere UCMUCM

Transformations on the Poincaré sphere Examples A differential phase shift induces a rotation about Z A geometrical rotation of angle  /2 induces a rotation about Y of angle  UCMUCM

Quantum fields One goes to the quantum version by replacing classical amplitudes by bosonic operators Stokes parameters appear as average values of Stokes operators s is the polarization (Bloch) vector The electric field vector never describes a definite ellipse! UCMUCM

Classical degree of polarization Classical definition of the degree of polarization Distance from the point to the origin (fully unpolarized state)! Problems It is defined solely in terms of the first moment of the Stokes operators. There are states with P=0 that cannot be regarded as unpolarized. P does not reflect the lack of perfect polarization for any quantum state. P=1 for SU(2) coherent states (and this includes the two-mode vacuum). UCMUCM

A new proposal of degree of polarization SU(2) coherent states associated Q function Q function for unpolarized light UCMUCM A. Luis, Phys. Rev. A 66, (2002).

A new proposal of degree of polarization Distance to the unpolarized state Definition Advantages Invariant under polarization transformations. The only states with P =0 are unpolarized states. P depends on the all the moments of the Stokes operators. Measures the spread of the Q function (i.e., localizability) UCMUCM A. Luis, Phys. Rev. A 66, (2002).

Examples: SU(2) coherent states Remarks: =1 for all N. The case N=0 is the two-mode vacuum with = 0. In the limit of high intensity tend to be fully polarized UCMUCM

Examples: number states Remarks: For classically they would be unpolarized! The number states tend to be polarized when their intensity increases. UCMUCM

Examples: phase states UCMUCM

Drawbacks is intrinsically semiclassical. The concept of distance is not well defined. There is no physical prescription of unpolarized light. States in the same excitation manifold can have quite different polarization degrees. UCMUCM

Unpolarized light: classical vs. quantum Classically, unpolarized light is the origin of the Poincaré sphere: Physical requirements: Rotational invariance Left-right symmetry Retardation invariance The vacuum is the only pure state that is unpolarized! UCMUCM

Alternative degrees of polarization Idea: Distance of the density matrix to the unpolarized density matrix Hilbert-Schmidt distance Advantages The quantum definition closest to the classical one. Invariant under polarization transformations. Feasible Related to the fidelity respect the fully unpolarized state. UCMUCM

A new degree of polarization (I) Any state can be expressed as Main hypothesis: The depolarized state corresponding to  is UCMUCM

Properties of the depolarized state The depolarized state depends on the initial state. The depolarized state in each su(2) invariant subspace is random The extension to entangled or mixed states is trivial. UCMUCM

Example States then UCMUCM

A new degree of polarization (II) Definition: Pure states UCMUCM

Examples For any pure state in the N+1 invariant subspace Quadrature coherent states in both polarization modes UCMUCM

Conclusions Quantum optics entails polarization states that cannot be suitably described by the classical formalism based on the Stokes parameters. A quantum degree of polarization can be defined as the distance between the density operator and the density operator representing unpolarized light. Correlations and the degree of polarization can be seen as complementary. UCMUCM