Lab 1 Entanglement and Bell s Inequalities

Size: px
Start display at page:

Download "Lab 1 Entanglement and Bell s Inequalities"

Transcription

1 Quantum Optics Lab Review Justin Winkler

2 Lab 1 Entanglement and Bell s Inequalities

3 Entanglement Wave-functions are non-separable Measurement of state of one particle alters the state of the other particle Entanglement proposed in EPR paper (1935) Believed this couldn t happen Bell s inequalities show occurrence of entanglement (proposed by J. S. Bell, 1964)

4 Bell s Inequality Inequality does not describe any particular physical quantity Trivially satisfied for classical objects Bell s inequalities allow experimental testing of interpretation of quantum mechanics Bell s theorem no theory of local hidden variables can fully reproduce the predictions of quantum mechanics

5 Theory

6 Measured and Theoretical Probabilities

7 CSHS Inequality Quantum mechanics predicts violation at certain angles, allowing a maximum S value of

8 Experimental Setup

9 Coincident Photon Counts Polarizer A held constant, polarizer B rotated Expected cosine squared dependence

10 Bell s inequality was violated Predicted S = 2.828

11 Additional Results Predicted S = 2.497

12 Lab 2: Single Photon Interference

13 Lab 2 Structure Two Parts Double Slit Diffraction Wave-Particle Duality Single photon diffraction Used attenuated laser source Mach-Zehnder Interferometer Which-way information Also used attenuated laser source

14 Double Slit Diffraction

15 Diffraction Pattern

16 Wave-Particle Duality Light has wave-like and particle-like like properties Wave Diffraction Interference Particle Photoelectric effect Photons Antibunching Single photons are still expected to display interference effects

17 Double Slit Apparatus

18 Double Slit Results 4 orders of attenuation Average of 0.94 meters between photons 0.1 second exposure time

19 Build Up of Interference Pattern Attenuation = 0.8 * 10-5 Photon Separation = 11.7 m 0.5 Seconds 1 Second 5 Seconds

20 Mach-Zehnder Interferometer Light in different paths have orthogonal polarization Presence of which path information is controlled by analyzer polarizer

21 MZ Interferometer Pictures Analyzer Polarizer at 45 (no which way information) Analyzer Polarizer at 90 (which way information present)

22

23 Fringe Visibility Fringe Visibility = Max - Min Max + Min

24 Fringe Visibility Results

25 Lab 3: Confocal Microscope Imaging of Single-Emitter Fluorescence Lab 4: Hanbury Brown & Twiss Setup, Photon Antibunching

26 Single Emitters and Photon Antibunching Attenuated lasers will sometimes produce bunches of photons which cannot be avoided. Single photon source requires single emitter that displays antibunching.

27 Quantum Dots Quantum dot - confines electrons in all directions Colloidal quantum dots - nanocrystals dispersed through a solution We prepared sample slides of colloidal quantum dots through spin coating Also used samples prepared by Luke Brissel

28 Experimental Setup

29 Experimental Setup

30 CCD Imaging

31 Confocal Microscope Scans

32 Scan Close-up

33 Antibunching Histogram

34 Histogram Without Antibunching

35 We Saw Antibunching!

36 Photonic Bandgap Material Photonic Crystals - Spatial periodicity on order of light wavelength Photonic Bandgap - No light passes in certain frequency range Cholesteric Liquid Crystals - Chiral crystals that suppress spontaneous emission in stop band and enhance near band edge.

37 Scan With Photonic Bandgap Material

38 Antibunching With Photonic Bandgap Material

39 Fluorescence Lifetime

40 The End

41 Questions?

42 Phase Shift from BBO Crystals

43 Fringe Visibility Results

44 Delay Characterization ns

45

46 Spontaneous Parametric Down-Conversion

47 SPDC Ring Imaged With CCD Camera

48

49 Single Counts

50 Horizontal Waveplate Alignment

51 Vertical Waveplate Alignment

Quantum Optics and Quantum Information Laboratory Review

Quantum Optics and Quantum Information Laboratory Review Quantum Optics and Quantum Information Laboratory Review Fall 2010 University of Rochester Instructor: Dr. Lukishova Joshua S. Geller Outline Lab 1: Entanglement and Bell s Inequalities Lab 2: Single Photon

More information

Quantum Optics and Quantum Information Laboratory

Quantum Optics and Quantum Information Laboratory Quantum Optics and Quantum Information Laboratory OPT 253, Fall 2011 Institute of Optics University of Rochester Instructor: Dr. Lukishova Jonathan Papa Contents Lab 1: Entanglement and Bell s Inequalities

More information

Quantum and Nano Optics Laboratory. Jacob Begis Lab partners: Josh Rose, Edward Pei

Quantum and Nano Optics Laboratory. Jacob Begis Lab partners: Josh Rose, Edward Pei Quantum and Nano Optics Laboratory Jacob Begis Lab partners: Josh Rose, Edward Pei Experiments to be Discussed Lab 1: Entanglement and Bell s Inequalities Lab 2: Single Photon Interference Labs 3 and 4:

More information

- Presentation - Quantum and Nano-Optics Laboratory. Fall 2012 University of Rochester Instructor: Dr. Lukishova. Joshua A. Rose

- Presentation - Quantum and Nano-Optics Laboratory. Fall 2012 University of Rochester Instructor: Dr. Lukishova. Joshua A. Rose - Presentation - Quantum and Nano-Optics Laboratory Fall 2012 University of Rochester Instructor: Dr. Lukishova Joshua A. Rose Contents Laboratory 1: Entanglement and Bell s Inequalities Laboratory 2:

More information

LAB 3: Confocal Microscope Imaging of single-emitter fluorescence. LAB 4: Hanbury Brown and Twiss setup. Photon antibunching. Roshita Ramkhalawon

LAB 3: Confocal Microscope Imaging of single-emitter fluorescence. LAB 4: Hanbury Brown and Twiss setup. Photon antibunching. Roshita Ramkhalawon LAB 3: Confocal Microscope Imaging of single-emitter fluorescence LAB 4: Hanbury Brown and Twiss setup. Photon antibunching Roshita Ramkhalawon PHY 434 Department of Physics & Astronomy University of Rochester

More information

Lab 3 and 4: Single Photon Source

Lab 3 and 4: Single Photon Source Lab 3 and 4: Single Photon Source By: Justin Deuro, December 10 th, 2009 Abstract We study methods of single photon emission by exciting single colloidal quantum dot (QD) samples. We prepare the single

More information

Confocal Microscopy Imaging of Single Emitter Fluorescence and Hanbury Brown and Twiss Photon Antibunching Setup

Confocal Microscopy Imaging of Single Emitter Fluorescence and Hanbury Brown and Twiss Photon Antibunching Setup 1 Confocal Microscopy Imaging of Single Emitter Fluorescence and Hanbury Brown and Twiss Photon Antibunching Setup Abstract Jacob Begis The purpose of this lab was to prove that a source of light can be

More information

Laboratory 3&4: Confocal Microscopy Imaging of Single-Emitter Fluorescence and Hanbury Brown and Twiss setup for Photon Antibunching

Laboratory 3&4: Confocal Microscopy Imaging of Single-Emitter Fluorescence and Hanbury Brown and Twiss setup for Photon Antibunching Laboratory 3&4: Confocal Microscopy Imaging of Single-Emitter Fluorescence and Hanbury Brown and Twiss setup for Photon Antibunching Jose Alejandro Graniel Institute of Optics University of Rochester,

More information

QUANTUM OPTICS AND QUANTUM INFORMATION TEACHING LABORATORY at the Institute of Optics, University of Rochester

QUANTUM OPTICS AND QUANTUM INFORMATION TEACHING LABORATORY at the Institute of Optics, University of Rochester QUANTUM OPTICS AND QUANTUM INFORMATION TEACHING LABORATORY at the Institute of Optics, University of Rochester Svetlana Lukishova, Luke Bissell, Carlos Stroud, Jr, Anand Kumar Jha, Laura Elgin, Nickolaos

More information

Laboratory 3: Confocal Microscopy Imaging of Single Emitter Fluorescence and Hanbury Brown, and Twiss Setup for Photon Antibunching

Laboratory 3: Confocal Microscopy Imaging of Single Emitter Fluorescence and Hanbury Brown, and Twiss Setup for Photon Antibunching Laboratory 3: Confocal Microscopy Imaging of Single Emitter Fluorescence and Hanbury Brown, and Twiss Setup for Photon Antibunching Jonathan Papa 1, * 1 Institute of Optics University of Rochester, Rochester,

More information

Detection of Single Photon Emission by Hanbury-Brown Twiss Interferometry

Detection of Single Photon Emission by Hanbury-Brown Twiss Interferometry Detection of Single Photon Emission by Hanbury-Brown Twiss Interferometry Greg Howland and Steven Bloch May 11, 009 Abstract We prepare a solution of nano-diamond particles on a glass microscope slide

More information

Confocal Microscope Imaging of Single emitter fluorescence and Observing Photon Antibunching Using Hanbury Brown and Twiss setup. Lab.

Confocal Microscope Imaging of Single emitter fluorescence and Observing Photon Antibunching Using Hanbury Brown and Twiss setup. Lab. Submitted for the partial fulfilment of the course PHY 434 Confocal Microscope Imaging of Single emitter fluorescence and Observing Photon Antibunching Using Hanbury Brown and Twiss setup Lab. 3 and 4

More information

Take that, Bell s Inequality!

Take that, Bell s Inequality! Take that, Bell s Inequality! Scott Barker November 10, 2011 Abstract Bell s inequality was tested using the CHSH method. Entangled photons were produced from two different laser beams by passing light

More information

Lab Experimental observation of singleemitter fluorescence and photon anti-bunching

Lab Experimental observation of singleemitter fluorescence and photon anti-bunching Lab. 3-4. Experimental observation of singleemitter fluorescence and photon anti-bunching Laboratory Report Group, Fall 6 Abstract: Fluorescence from single emitters, such as DiDye molecules and CdSe quantum

More information

Labs 3-4: Single-photon Source

Labs 3-4: Single-photon Source Labs 3-4: Single-photon Source Lab. 3. Confocal fluorescence microscopy of single-emitter Lab. 4. Hanbury Brown and Twiss setup. Fluorescence antibunching 1 Labs 3-4: Single-photon Source Efficiently produces

More information

Joshua S. Geller. Department of Physics and Astronomy, University of Rochester, Rochester NY, 14627

Joshua S. Geller. Department of Physics and Astronomy, University of Rochester, Rochester NY, 14627 LAB 3-4, PHY434. Single Photon Source: Confocal Microscope Imaging of Single-Emitter Fluorescence and Hanbury Brown and Twiss setup for Photon Antibunching Measurements Joshua S. Geller Department of Physics

More information

Confocal Microscope Imaging of Single-Emitter Fluorescence and Photon Antibunching

Confocal Microscope Imaging of Single-Emitter Fluorescence and Photon Antibunching Confocal Microscope Imaging of Single-Emitter Fluorescence and Photon Antibunching By Dilyana Mihaylova Abstract The purpose of this lab is to study different types of single emitters including quantum

More information

Lab 3-4 : Confocal Microscope Imaging of Single-Emitter Fluorescence and Hanbury-Brown and Twiss Set Up, Photon Antibunching

Lab 3-4 : Confocal Microscope Imaging of Single-Emitter Fluorescence and Hanbury-Brown and Twiss Set Up, Photon Antibunching Lab 3-4 : Confocal Microscope Imaging of Single-Emitter Fluorescence and Hanbury-Brown and Twiss Set Up, Photon Antibunching Mongkol Moongweluwan 1 1 Department of Physics and Astronomy, University of

More information

Optical Properties of CdSe Colloidal Quantum Dots and NV-Nanodiamonds

Optical Properties of CdSe Colloidal Quantum Dots and NV-Nanodiamonds Optical Properties of CdSe Colloidal Quantum Dots and NV-Nanodiamonds James MacNeil and Madhu Ashok University of Rochester The Institute of Optics Submitted to Dr. Svetlana Lukishova on 11/20/2013 Abstract:

More information

Quantum Entanglement and Bell s Inequalities Zachary Evans, Joel Howard, Jahnavi Iyer, Ava Dong, and Maggie Han

Quantum Entanglement and Bell s Inequalities Zachary Evans, Joel Howard, Jahnavi Iyer, Ava Dong, and Maggie Han Quantum Entanglement and Bell s Inequalities Zachary Evans, Joel Howard, Jahnavi Iyer, Ava Dong, and Maggie Han Institute of Optics, University of Rochester Opt 101 Meeting, December 4, 2012, Rochester

More information

Entanglement and Bell s Inequalities. Benjamin Feifke, Kara Morse. Professor Svetlana Lukishova

Entanglement and Bell s Inequalities. Benjamin Feifke, Kara Morse. Professor Svetlana Lukishova Entanglement and Bell s Inequalities Benjamin Feifke, Kara Morse Professor Svetlana Lukishova Abstract The purpose of this is experiment was to observe quantum entanglement by calculating Bell s Inequality

More information

Quantum Optics in the Teaching Labs

Quantum Optics in the Teaching Labs Quantum Optics in the Teaching Labs Svetlana Lukishova The Institute of Optics University of Rochester LLE S & T Seminar 17 April 2009 Rochester NY 1 Quantum mechanics has long been found to be among the

More information

Entanglement and Bell s Inequalities Edward Pei. Abstract

Entanglement and Bell s Inequalities Edward Pei. Abstract Entanglement and Bell s Inequalities Edward Pei Abstract The purpose of this laboratory experiment is to verify quantum entanglement of the polarization of two photon pairs. The entanglement of the photon

More information

Lab 2: Single Photon Interference

Lab 2: Single Photon Interference Lab 2: Single Photon Interference Joshua S. Geller Dept. of Physics and Astronomy, University of Rochester, Rochester, NY 14627 Abstract In this lab we exhibit the wave-particle duality of light in the

More information

Lab3-4: Single Photon Source

Lab3-4: Single Photon Source Lab3-4: Single Photon Source Xiaoshu Chen* Department of Mechanical Engineering, University of ochester, NY, 1463 ABSAC n this lab, we studied the quantum dot excitation method of single photon source.

More information

Anti-Bunching from a Quantum Dot

Anti-Bunching from a Quantum Dot Anti-Bunching from a Quantum Dot Gerardo I. Viza 1, 1 Department of Physics and Astronomy, University of Rochester, Rochester, NY 14627 We study the nature of non-classical single emitter light experimentally

More information

Particle-Wave Duality and Which-Way Information

Particle-Wave Duality and Which-Way Information Particle-Wave Duality and Which-Way Information Graham Jensen and Samantha To University of Rochester, Rochester, NY 14627, U.S. September 25, 2013 Abstract Samantha To This experiment aimed to support

More information

Single Photon Sources

Single Photon Sources Single Photon Sources Graham Jensen and Samantha To University of Rochester, Rochester, New York Abstract Graham Jensen: We present the results of an investigation to verify the feasibility of quantum

More information

Laboratory 1: Entanglement & Bell s Inequalities

Laboratory 1: Entanglement & Bell s Inequalities Laboratory 1: Entanglement & Bell s Inequalities Jose Alejandro Graniel Institute of Optics University of Rochester, Rochester, NY 14627, U.S.A Abstract This experiment purpose was to study the violation

More information

Single-photon NV sources. Pauli Kehayias March 16, 2011

Single-photon NV sources. Pauli Kehayias March 16, 2011 Single-photon NV sources 1 Outline Quantum nature of light Photon correlation functions Single-photon sources NV diamond single-photon sources 2 Wave/particle duality Light exhibits wave and particle properties

More information

Quantum optics. Marian O. Scully Texas A&M University and Max-Planck-Institut für Quantenoptik. M. Suhail Zubairy Quaid-i-Azam University

Quantum optics. Marian O. Scully Texas A&M University and Max-Planck-Institut für Quantenoptik. M. Suhail Zubairy Quaid-i-Azam University Quantum optics Marian O. Scully Texas A&M University and Max-Planck-Institut für Quantenoptik M. Suhail Zubairy Quaid-i-Azam University 1 CAMBRIDGE UNIVERSITY PRESS Preface xix 1 Quantum theory of radiation

More information

Lab. 1: Entanglement and Bell s Inequalities. Abstract

Lab. 1: Entanglement and Bell s Inequalities. Abstract December 15, 2008 Submitted for the partial fulfilment of the course PHY 434 Lab. 1: Entanglement and Bell s Inequalities Mayukh Lahiri 1, 1 Department of Physics and Astronomy, University of Rochester,

More information

Innovation and Development of Study Field. nano.tul.cz

Innovation and Development of Study Field. nano.tul.cz Innovation and Development of Study Field Nanomaterials at the Technical University of Liberec nano.tul.cz These materials have been developed within the ESF project: Innovation and development of study

More information

Single Photon Generation & Application

Single Photon Generation & Application Single Photon Generation & Application Photon Pair Generation: Parametric down conversion is a non-linear process, where a wave impinging on a nonlinear crystal creates two new light beams obeying energy

More information

Closing the Debates on Quantum Locality and Reality: EPR Theorem, Bell's Theorem, and Quantum Information from the Brown-Twiss Vantage

Closing the Debates on Quantum Locality and Reality: EPR Theorem, Bell's Theorem, and Quantum Information from the Brown-Twiss Vantage Closing the Debates on Quantum Locality and Reality: EPR Theorem, Bell's Theorem, and Quantum Information from the Brown-Twiss Vantage C. S. Unnikrishnan Fundamental Interactions Laboratory Tata Institute

More information

Supplementary Information: Three-dimensional quantum photonic elements based on single nitrogen vacancy-centres in laser-written microstructures

Supplementary Information: Three-dimensional quantum photonic elements based on single nitrogen vacancy-centres in laser-written microstructures Supplementary Information: Three-dimensional quantum photonic elements based on single nitrogen vacancy-centres in laser-written microstructures Andreas W. Schell, 1, a) Johannes Kaschke, 2 Joachim Fischer,

More information

Experiment 6 - Tests of Bell s Inequality

Experiment 6 - Tests of Bell s Inequality Exp.6-Bell-Page 1 Experiment 6 - Tests of Bell s Inequality References: Entangled photon apparatus for the undergraduate laboratory, and Entangled photons, nonlocality, and Bell inequalities in the undergraduate

More information

Schemes to generate entangled photon pairs via spontaneous parametric down conversion

Schemes to generate entangled photon pairs via spontaneous parametric down conversion Schemes to generate entangled photon pairs via spontaneous parametric down conversion Atsushi Yabushita Department of Electrophysics National Chiao-Tung University? Outline Introduction Optical parametric

More information

Single photons. how to create them, how to see them. Alessandro Cerè

Single photons. how to create them, how to see them. Alessandro Cerè Single photons how to create them, how to see them Alessandro Cerè Intro light is quantum light is cheap let s use the quantum properties of light Little interaction with the environment We can send them

More information

Quantum Entanglement and Bell's Inequalities

Quantum Entanglement and Bell's Inequalities Quantum Entanglement and Bell's Inequalities James Westover University of Rochester In this experiment we produced entangled photons using a pair of BBO crystals. We then proceeded to make measurements

More information

Hong-Ou-Mandel effect with matter waves

Hong-Ou-Mandel effect with matter waves Hong-Ou-Mandel effect with matter waves R. Lopes, A. Imanaliev, A. Aspect, M. Cheneau, DB, C. I. Westbrook Laboratoire Charles Fabry, Institut d Optique, CNRS, Univ Paris-Sud Progresses in quantum information

More information

Comparing quantum and classical correlations in a quantum eraser

Comparing quantum and classical correlations in a quantum eraser Comparing quantum and classical correlations in a quantum eraser A. Gogo, W. D. Snyder, and M. Beck* Department of Physics, Whitman College, Walla Walla, Washington 99362, USA Received 14 February 2005;

More information

Single Photon Generation & Application in Quantum Cryptography

Single Photon Generation & Application in Quantum Cryptography Single Photon Generation & Application in Quantum Cryptography Single Photon Sources Photon Cascades Quantum Cryptography Single Photon Sources Methods to Generate Single Photons on Demand Spontaneous

More information

Quantum physics and the beam splitter mystery

Quantum physics and the beam splitter mystery Quantum physics and François Hénault Institut de Planétologie et d Astrophysique de Grenoble Université Joseph Fourier Centre National de la Recherche Scientifique BP 53, 384 Grenoble France Conf. 957

More information

January 2010, Maynooth. Photons. Myungshik Kim.

January 2010, Maynooth. Photons. Myungshik Kim. January 2010, Maynooth Photons Myungshik Kim http://www.qteq.info Contents Einstein 1905 Einstein 1917 Hanbury Brown and Twiss Light quanta In 1900, Max Planck was working on black-body radiation and suggested

More information

Lamps, lasers and detectors - Misconceptions i in the interpretation i of

Lamps, lasers and detectors - Misconceptions i in the interpretation i of Lamps, lasers and detectors - Misconceptions i in the interpretation i of classical experiments on light Karl Otto Greulich Fritz Lipmann Institute Beutenbergstr. 11 D07745 Jena Germany kog fli@leibniz.de

More information

Interference, Complementarity, Entanglement and all that Jazz

Interference, Complementarity, Entanglement and all that Jazz nterference, Complementarity, Entanglement and all that Jazz Mark Beck Dept. of Physics, Whitman College With lots of help from: Faculty: obert Davies (Seattle U) Students: Ashifi ogo, William Snyder,

More information

Distribution of Delay Times in Laser Excited CdSe-ZnS Core-Shell Quantum Dots

Distribution of Delay Times in Laser Excited CdSe-ZnS Core-Shell Quantum Dots Distribution of Delay Times in Laser Excited CdSe-ZnS Core-Shell Quantum Dots Andrei Vajiac Indiana University South Bend Mathematics, Computer Science Advisor: Pavel Frantsuzov, Physics Abstract This

More information

Timeline: Bohm (1951) EPR (1935) CHSH (1969) Bell (1964) Theory. Freedman Clauser (1972) Aspect (1982) Weihs (1998) Weinland (2001) Zeilinger (2010)

Timeline: Bohm (1951) EPR (1935) CHSH (1969) Bell (1964) Theory. Freedman Clauser (1972) Aspect (1982) Weihs (1998) Weinland (2001) Zeilinger (2010) 1.EPR paradox 2.Bohm s version of EPR with spin ½ particles 3.Entangled states and production 4.Derivation of CHSH inequality - S parameter for mixed and entangled state 5. Loopholes 6.Experiments confirming

More information

Top Le# side TEST Right side bo.om

Top Le# side TEST Right side bo.om Top bo.om e# side TEST Right side Correlation functions in optics and quantum optics, 2 University of Science and Technology of China Hefei, China July 2018 Luis A. Orozco www.jqi.umd.edu The slides of

More information

Top Le# side TEST Right side bo.om

Top Le# side TEST Right side bo.om Top bo.om e# side TEST Right side Correlation functions in optics and quantum optics, 4 University of Science and Technology of China Hefei, China Luis A. Orozco www.jqi.umd.edu The slides of the course

More information

Where are the Fringes? (in a real system) Div. of Amplitude - Wedged Plates. Fringe Localisation Double Slit. Fringe Localisation Grating

Where are the Fringes? (in a real system) Div. of Amplitude - Wedged Plates. Fringe Localisation Double Slit. Fringe Localisation Grating Where are the Fringes? (in a real system) Fringe Localisation Double Slit spatial modulation transverse fringes? everywhere or well localised? affected by source properties: coherence, extension Plane

More information

Correlation functions in optics and quantum optics, 4

Correlation functions in optics and quantum optics, 4 Correlation functions in optics and quantum optics, 4 State Key Laboratory of Precision Spectroscopy East China Normal University, Shanghai, China Luis A. Orozco www.jqi.umd.edu The slides of the course

More information

Quantum Optics and Quantum Information Teaching Laboratories at the Institute of Optics, University of Rochester Svetlana G.

Quantum Optics and Quantum Information Teaching Laboratories at the Institute of Optics, University of Rochester Svetlana G. Quantum Optics and Quantum Information Teaching Laboratories at the Institute of Optics University of Rochester Svetlana G. Lukishova OU-Tulsa Schusterman Center Seminar 4 September 00 Tulsa OK Quantum

More information

Erwin Schrödinger and his cat

Erwin Schrödinger and his cat Erwin Schrödinger and his cat How to relate discrete energy levels with Hamiltonian described in terms of continгous coordinate x and momentum p? Erwin Schrödinger (887-96) Acoustics: set of frequencies

More information

Quantum information processing using linear optics

Quantum information processing using linear optics Quantum information processing using linear optics Karel Lemr Joint Laboratory of Optics of Palacký University and Institute of Physics of Academy of Sciences of the Czech Republic web: http://jointlab.upol.cz/lemr

More information

Correlation functions in optics; classical and quantum 2. TUW, Vienna, Austria, April 2018 Luis A. Orozco

Correlation functions in optics; classical and quantum 2. TUW, Vienna, Austria, April 2018 Luis A. Orozco Correlation functions in optics; classical and quantum 2. TUW, Vienna, Austria, April 2018 Luis A. Orozco www.jqi.umd.edu Correlations in optics Reference that includes pulsed sources: Zheyu Jeff Ou Quantum

More information

Testing The Existence of Single Photons

Testing The Existence of Single Photons Testing The Existence of Single Photons Quynh Nguyen and Asad Khan Method of Experimental Physics Project, University of Minnesota. (Dated: 12 May 2014) We demonstrated the existence of single photon by

More information

Lecture 0. NC State University

Lecture 0. NC State University Chemistry 736 Lecture 0 Overview NC State University Overview of Spectroscopy Electronic states and energies Transitions between states Absorption and emission Electronic spectroscopy Instrumentation Concepts

More information

arxiv:quant-ph/ v1 13 Jun 2001

arxiv:quant-ph/ v1 13 Jun 2001 A double-slit quantum eraser arxiv:quant-ph/1678v1 13 Jun 1 S. P. Walborn 1, M. O. Terra Cunha 1,, S. Pádua 1, and C. H. Monken 1 1 Departamento de Física, Universidade Federal de Minas Gerais, Caixa Postal

More information

Ultrafast Dynamics and Single Particle Spectroscopy of Au-CdSe Nanorods

Ultrafast Dynamics and Single Particle Spectroscopy of Au-CdSe Nanorods Supporting Information Ultrafast Dynamics and Single Particle Spectroscopy of Au-CdSe Nanorods G. Sagarzazu a, K. Inoue b, M. Saruyama b, M. Sakamoto b, T. Teranishi b, S. Masuo a and N. Tamai a a Department

More information

Model Answer (Paper code: AR-7112) M. Sc. (Physics) IV Semester Paper I: Laser Physics and Spectroscopy

Model Answer (Paper code: AR-7112) M. Sc. (Physics) IV Semester Paper I: Laser Physics and Spectroscopy Model Answer (Paper code: AR-7112) M. Sc. (Physics) IV Semester Paper I: Laser Physics and Spectroscopy Section I Q1. Answer (i) (b) (ii) (d) (iii) (c) (iv) (c) (v) (a) (vi) (b) (vii) (b) (viii) (a) (ix)

More information

arxiv:quant-ph/ v3 20 Apr 2005

arxiv:quant-ph/ v3 20 Apr 2005 Controlling the Spontaneous Emission Rate of Single Quantum Dots in a 2D Photonic Crystal Dirk Englund, 1 David Fattal, 1 Edo Waks, 1 Glenn Solomon, 1,2 Bingyang Zhang, 1 Toshihiro Nakaoka, 3 Yasuhiko

More information

Complete all the identification fields below or 10% of the lab value will be deduced from your final mark for this lab.

Complete all the identification fields below or 10% of the lab value will be deduced from your final mark for this lab. Physical optics Identification page Instructions: Print this page and the following ones before your lab session to prepare your lab report. Staple them together with your graphs at the end. If you forgot

More information

Path Entanglement. Liat Dovrat. Quantum Optics Seminar

Path Entanglement. Liat Dovrat. Quantum Optics Seminar Path Entanglement Liat Dovrat Quantum Optics Seminar March 2008 Lecture Outline Path entangled states. Generation of path entangled states. Characteristics of the entangled state: Super Resolution Beating

More information

Theory and Experiment

Theory and Experiment Theory and Experiment Mark Beck OXPORD UNIVERSITY PRESS Contents Table of Symbols Preface xiii xix 1 MATHEMATICAL PRELIMINARIES 3 1.1 Probability and Statistics 3 1.2 LinearAlgebra 9 1.3 References 17

More information

Lab 2: Mach Zender Interferometer Overview

Lab 2: Mach Zender Interferometer Overview Lab : Mach Zender Interferometer Overview Goals:. Study factors that govern the interference between two light waves with identical amplitudes and frequencies. Relative phase. Relative polarization. Learn

More information

Spectroscopic Instruments

Spectroscopic Instruments Spectroscopic Instruments 95 Spectroscopic Instruments by division of amplitude Mach-Zehnder (division of amplitude) Michelson Fringe localisation LIGO Fabry-Perot (FPI) Multi-layer coatings 96 Mach-Zehnder

More information

Quantum Physics in the Nanoworld

Quantum Physics in the Nanoworld Hans Lüth Quantum Physics in the Nanoworld Schrödinger's Cat and the Dwarfs 4) Springer Contents 1 Introduction 1 1.1 General and Historical Remarks 1 1.2 Importance for Science and Technology 3 1.3 Philosophical

More information

Double-Slit Interference

Double-Slit Interference Double-Slit Interference 1. Objectives. The objective of this laboratory is to verify the double-slit interference relationship. 2. Theory. a. When monochromatic, coherent light is incident upon a double

More information

Entangled photon pairs from radiative cascades in semiconductor quantum dots

Entangled photon pairs from radiative cascades in semiconductor quantum dots Early View publication on www.interscience.wiley.com (issue and page numbers not yet assigned; citable using Digital Object Identifier DOI Original phys. stat. sol. (b, 1 5 (26 / DOI 1.12/pssb.267152 Entangled

More information

Two-photon double-slit interference experiment

Two-photon double-slit interference experiment 1192 J. Opt. Soc. Am. B/Vol. 15, No. 3/March 1998 C. K. Hong and T. G. Noh Two-photon double-slit interference experiment C. K. Hong and T. G. Noh Department of Physics, Pohang University of Science and

More information

Generation of single photons and correlated photon pairs using InAs quantum dots

Generation of single photons and correlated photon pairs using InAs quantum dots Fortschr. Phys. 52, No. 2, 8 88 (24) / DOI.2/prop.2488 Generation of single photons and correlated photon pairs using InAs quantum dots C. Santori,2, D. Fattal, J. Vuckovic, G. S. Solomon, and Y. Yamamoto,3,

More information

A Study of the Phenomenon of Spontaneous Parametric Down-Conversion

A Study of the Phenomenon of Spontaneous Parametric Down-Conversion A Study of the Phenomenon of Spontaneous Parametric Down-Conversion Paroma Palchoudhuri Physics Department, The College of Wooster, Wooster, Ohio 44691, USA (Dated: December 1, 214) The phenomenon of type-i

More information

Contents Classical and Quantum Interference and Coherence Quantum Interference in Atomic Systems: Mathematical Formalism

Contents Classical and Quantum Interference and Coherence Quantum Interference in Atomic Systems: Mathematical Formalism 1 Classical and Quantum Interference and Coherence... 1 1.1 ClassicalInterferenceandOpticalInterferometers... 2 1.1.1 Young sdoubleslitinterferometer... 2 1.1.2 First-OrderCoherence... 4 1.1.3 WelcherWegProblem...

More information

PHY3902 PHY3904. Photon Entanglement. Laboratory protocol

PHY3902 PHY3904. Photon Entanglement. Laboratory protocol HY390 HY390 hoton ntanglement Laboratory protocol Goals. Learn how to create and detect pairs of photons entangled in polarization.. Test the lauser Horne Shimony and Holt version of the Bell inequality

More information

Quantum correlations and atomic speckle

Quantum correlations and atomic speckle Quantum correlations and atomic speckle S. S. Hodgman R. G. Dall A. G. Manning M. T. Johnsson K. G. H. Baldwin A. G. Truscott ARC Centre of Excellence for Quantum-Atom Optics, Research School of Physics

More information

Quantum Cryptography in Full Daylight Ilja Gerhardt, Matthew P. Peloso, Caleb Ho, Antía Ilja Gerhardt Lamas-Linares and Christian Kurtsiefer

Quantum Cryptography in Full Daylight Ilja Gerhardt, Matthew P. Peloso, Caleb Ho, Antía Ilja Gerhardt Lamas-Linares and Christian Kurtsiefer Centre for Quantum Technologies, Singapore QUANTUM OPTICS Entanglement-based Free Space Quantum Cryptography in Full Daylight, Matthew P. Peloso, Caleb Ho, Antía Lamas-Linares and Christian Kurtsiefer

More information

Experimental realisation of the weak measurement process

Experimental realisation of the weak measurement process Experimental realisation of the weak measurement process How do you do a strong and weak measurement. Two experiments using photons - Modified Stern-Gerlach - Youngs s 2-slit experiment Preliminary thoughts

More information

Bell s inequality Experimental exercise

Bell s inequality Experimental exercise Bell s inequality Experimental exercise Introduction Purposes of the lab Besides familiarizing yourselves with the important concept of Bell s inequality in relation to the Einstein- Podolsky-Rosen arguments

More information

Single Semiconductor Nanostructures for Quantum Photonics Applications: A solid-state cavity-qed system with semiconductor quantum dots

Single Semiconductor Nanostructures for Quantum Photonics Applications: A solid-state cavity-qed system with semiconductor quantum dots The 3 rd GCOE Symposium 2/17-19, 19, 2011 Tohoku University, Sendai, Japan Single Semiconductor Nanostructures for Quantum Photonics Applications: A solid-state cavity-qed system with semiconductor quantum

More information

PROCEEDINGS OF SPIE. Event: 14th Conference on Education and Training in Optics and Photonics, ETOP 2017, 2017, Hangzhou, China

PROCEEDINGS OF SPIE. Event: 14th Conference on Education and Training in Optics and Photonics, ETOP 2017, 2017, Hangzhou, China PROCEEDINGS OF SPIE SPIEDigitalLibrary.org/conference-proceedings-of-spie Quantum optics and nano-optics teaching laboratory for the undergraduate curriculum: teaching quantum mechanics and nanophysics

More information

Alpha Immersion Hands- on Ac4vi4es. Kiko Galvez Colgate University 2015

Alpha Immersion Hands- on Ac4vi4es. Kiko Galvez Colgate University 2015 lpha Immersion Hands- on c4vi4es Kiko Galvez Colgate University 2015 1 c4vity I (Tuesday M) - Basic lignment Goal: To get hands- on experience with op4cal alignments. Materials: 2 x5 op4cal breadboard

More information

Annual Report:

Annual Report: Annual Report: 0633621 Annual Report for Period:06/2008-05/2009 Submitted on: 05/28/2009 Principal Investigator: Stroud, Carlos R. Award ID: 0633621 Organization: University of Rochester Submitted By:

More information

Bunching-Antibunching of Quantum Particles From Astronomy to AMO. Indu Satija George Mason

Bunching-Antibunching of Quantum Particles From Astronomy to AMO. Indu Satija George Mason Bunching-Antibunching of Quantum Particles From Astronomy to AMO Indu Satija George Mason What is the most beautiful experiment in physics? This is the question that Robert Crease asked Physics World readers

More information

AP/P387 Note2 Single- and entangled-photon sources

AP/P387 Note2 Single- and entangled-photon sources AP/P387 Note Single- and entangled-photon sources Single-photon sources Statistic property Experimental method for realization Quantum interference Optical quantum logic gate Entangled-photon sources Bell

More information

Liquid Crystals Reviews Publication details, including instructions for authors and subscription information:

Liquid Crystals Reviews Publication details, including instructions for authors and subscription information: This article was downloaded by: [University of Rochester] On: 23 February 2015, At: 13:21 Publisher: Taylor & Francis Informa Ltd Registered in England and Wales Registered Number: 1072954 Registered office:

More information

31 st International Free Electron Laser Conference

31 st International Free Electron Laser Conference FHI-BERLIN ASG at CFEL MAX-PLANCK-GESELLSCHAFT 3 st International Free Electron Laser Conference 3 rd - 8 th August, 009 BT Convention Centre Liverpool, UK Evidence for Position Based Entanglement in Auger

More information

Two Dimensional SR-Interferometer at PETRA III. Artem Novokshonov DESY, Tomsk Polytechnic University

Two Dimensional SR-Interferometer at PETRA III. Artem Novokshonov DESY, Tomsk Polytechnic University Two Dimensional SR-Interferometer at PETRA III Artem Novokshonov DESY, Tomsk Polytechnic University First Part: Two Dimensional Interferometer at Petra III Interferometer principal Schematic of the Interferometer

More information

How to use the simulator

How to use the simulator How to use the simulator Overview The application allows for the exploration of four quantum circuits in all. Each simulator grants the user a large amount of freedom in experments they wish to conduct.

More information

Violation of Bell Inequalities

Violation of Bell Inequalities Violation of Bell Inequalities Philipp Kurpiers and Anna Stockklauser 5/12/2011 Quantum Systems for Information Technology Einstein-Podolsky-Rosen paradox (1935) Goal: prove that quantum mechanics is incomplete

More information

SUPPLEMENTARY INFORMATION

SUPPLEMENTARY INFORMATION Supplementary Information Speckle-free laser imaging using random laser illumination Brandon Redding 1*, Michael A. Choma 2,3*, Hui Cao 1,4* 1 Department of Applied Physics, Yale University, New Haven,

More information

Problem Solving. radians. 180 radians Stars & Elementary Astrophysics: Introduction Press F1 for Help 41. f s. picture. equation.

Problem Solving. radians. 180 radians Stars & Elementary Astrophysics: Introduction Press F1 for Help 41. f s. picture. equation. Problem Solving picture θ f = 10 m s =1 cm equation rearrange numbers with units θ factors to change units s θ = = f sinθ fθ = s / cm 10 m f 1 m 100 cm check dimensions 1 3 π 180 radians = 10 60 arcmin

More information

Analysis of photon flux distribution of type-Ⅱ SPDC for highly efficient entangled source adjustment

Analysis of photon flux distribution of type-Ⅱ SPDC for highly efficient entangled source adjustment Analysis of photon flux distribution of type-Ⅱ SPDC for highly efficient entangled source adjustment Ziyi Wang 1, Heying Wang 1, Wenbo Sun 1,* 1Physics Department, Tsinghua University, Beijing 100084,

More information

3. Excitation and Detection of Fluorescence

3. Excitation and Detection of Fluorescence 3. Excitation and Detection of Fluorescence In this chapter, we examine key experimental components and methods to observe weakly fluorescing objects. We consider in turn the excitation source, the detectors,

More information

Quantum Optics in Photonic Crystals. Peter Lodahl Dept. of Communications, Optics & Materials (COM) Technical University of Denmark

Quantum Optics in Photonic Crystals. Peter Lodahl Dept. of Communications, Optics & Materials (COM) Technical University of Denmark Quantum Optics in Photonic Crystals Peter Lodahl Dept. of Communications, Optics & Materials (COM) Technical University of Denmark Acknowledgements AMOLF Institute Amsterdam / University of Twente Ivan

More information

PHY410 Optics Exam #3

PHY410 Optics Exam #3 PHY410 Optics Exam #3 NAME: 1 2 Multiple Choice Section - 5 pts each 1. A continuous He-Ne laser beam (632.8 nm) is chopped, using a spinning aperture, into 500 nanosecond pulses. Compute the resultant

More information

Entanglement Enabled Intensity Interferometry

Entanglement Enabled Intensity Interferometry MIT-CTP-464 Entanglement Enabled Intensity Interferometry Jordan Cotler and Frank Wilczek,. Center for Theoretical Physics, MIT, Cambridge MA 039 USA. Origins Project, Arizona State University, Tempe AZ

More information

Spectroscopy of. Semiconductors. Luminescence OXFORD IVAN PELANT. Academy ofsciences of the Czech Republic, Prague JAN VALENTA

Spectroscopy of. Semiconductors. Luminescence OXFORD IVAN PELANT. Academy ofsciences of the Czech Republic, Prague JAN VALENTA Luminescence Spectroscopy of Semiconductors IVAN PELANT Institute ofphysics, v.v.i. Academy ofsciences of the Czech Republic, Prague JAN VALENTA Department of Chemical Physics and Optics Charles University,

More information

Novel Cascaded Ultra Bright Pulsed Source of Polarization Entangled Photons

Novel Cascaded Ultra Bright Pulsed Source of Polarization Entangled Photons Novel Cascaded Ultra Bright Pulsed Source of Polarization Entangled Photons G. Bitton, W.P. Grice, J. Moreau 1, and L. Zhang 2 Center for Engineering Science Advanced Research, Computer Science and Mathematics

More information