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Schrödinger’s Rainbow: The Renaissance in Quantum Optical Interferometry Jonathan P. Dowling Quantum Science & Technologies (QST) Group Hearne Institute.

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Presentation on theme: "Schrödinger’s Rainbow: The Renaissance in Quantum Optical Interferometry Jonathan P. Dowling Quantum Science & Technologies (QST) Group Hearne Institute."— Presentation transcript:

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2 Schrödinger’s Rainbow: The Renaissance in Quantum Optical Interferometry Jonathan P. Dowling Quantum Science & Technologies (QST) Group Hearne Institute for Theoretical Physics Louisiana State University http://quantum.phys.lsu.edu

3 Table of Contents Quantum Technologies Schrödinger’s Cat and All That Quantum Light—Over the Rainbow Putting Entangled Light to Work The Yellow-Brick Roadmap

4 Quantum Technology: The Second Quantum Revolution JP Dowling & GJ Milburn, Phil. Transactions of the Royal Soc. of London Quantum Mechanical Systems Pendulums Cantilevers Phonons Coherent Quantum Electronics Superconductors Excitons Spintronics Quantum Optics Ion Traps Cavity QED Linear Optics Quantum Atomics Bose-Einstein Atomic Coherence Ion Traps Quantum Information Processing

5 Schrödinger’s Cat and All That

6 Schrödinger’s Cat Revisited

7 Quantum Kitty Review A sealed and insulated box (A) contains a radioactive source (B) which has a 50% chance during the course of the "experiment" of triggering Geiger counter (C) which activates a mechanism (D) causing a hammer to smash a flask of prussic acid (E) and killing the cat (F). An observer (G) must open the box in order to collapse the state vector of the system into one of the two possible states. A second observer (H) may be needed to collapse the state vector of the larger system containing the first observer (G) and the apparatus (A-F). And so on...

8 Paradox? What Paradox!? (1.) The State of the Cat is “Entangled” with That of the Atom. (2.) The Cat is in a Simultaneous Superposition of Dead & Alive. (3.) Observers are Required to “Collapse” the Cat to Dead or Alive

9 Quantum Entanglement “Quantum entanglement is the characteristic trait of quantum mechanics, the one that enforces its entire departure from classical lines of thought.” — Erwin Schrödinger

10 Conservation of Classical Angular Momentum A B

11 Conservation of Quantum Spin Entangled David Bohm A B

12 Einstein, Podolsky, Rosen (EPR) Paradox Albert EinsteinBoris Podolsky “If, without in any way disturbing a system, we can predict with certainty... the value of a physical quantity, then there exists an element of physical reality corresponding to this physical quantity." Nathan Rosen

13 Hidden Variable Theory + ABAB Can the Spooky, Action-at-a-distance Predictions (Entanglement) of Quantum Mechanics… + ABAB …Be Replaced by Some Sort of Local, Statistical, Classical (Hidden Variable) Theory?

14 NO!—Bell’s Inequality The physical predictions of quantum theory disagree with those of any local (classical) hidden-variable theory! John Bell

15 Clauser (1978) & Aspect (1982) Experiments John Clauser Alain Aspect V= Vertical Polarization H = Horizontal Polarization H A V B  V A H B AB H VH V Two-Photon Atomic Decay

16 Quantum Light—Over the Rainbow

17 Parametric Downconversion: Type I

18 UV Pump Signal B Idler A Degenerate (Entangled) Case:  s =  i  s,  s, k s A  i,  i, k s B  i,  i, k i A  s,  s, k s B Type I Photon Pairs

19 Parametric Downconversion: Type I

20 A B Parametric Downconversion: Type II H A V B  V A H B Degenerate (Entangled) Case:  s =  i

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22 Putting Entangled Light to Work

23 Tests of Bell’s Inequalities at Innsbruck Anton Zeilinger Alice Bob Type II Downcoversion

24 Quantum Teleportation

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26 Teleportation Experiment at Innsbruck Bell State Analysis EPR Source Experiment

27 NIST Heralded Photon Absolute Light Source Output characteristics : photon #  known photon timing  known wavelength  known direction  known polarization  known Alan Migdall

28 Detector to be Calibrated Trigger or “Herald” Detector Detector Quantum Efficiency Scheme No External Standards Needed!

29 Black Box Generates arbitrary Entangled States QWP HWP PBS Detector This setup allows measurement of an arbitrary polarization state in each arm. Any two-photon tomography requires 16 of these measurements. Examples Arm 1 Arm 2 H V H R D D Characterizing Two-Photon Entanglement Paul Kwiat U. Illinois Kwiat Super-Bright Source

30 Characterization of Entangled States Werner States

31 Bob and “Charly” Share Random Crypto Key Quantum Cryptography at University of Geneva System Under Lake Geneva Nicolas Gisin

32 New York Times

33 The Hong-Ou-Mandel Effect Leonard Mandel

34 Classical One-Photon Absorption — Classical Two-Photon Absorption — Quantum Two-Photon Absorption — Quantum Peak Is Narrower and Spacing is HALVED! Quantum Peak Is Narrower and Spacing is HALVED! Quantum Optical Lithography

35 squeezed vacuum : OPA + 0.92 0.08 coherent beam wave plate R=0.92 33cm lens f=3cm 3.3cm Image of the wave plate plane with waist=300  m Displacement Measurements and Gravity Waves Hans Bachor Australian National University

36 Quantum Clock Synchronization Entangled Photons Can Synchronize Past the Turbulent Atmosphere! Seth Lloyd MIT A B

37 Quantum Computing Quantum Controlled-NOT Gate using and Entangled-Light Source, Beam Splitters, and Detectors. Entangled Photons are a Resource for Scalable Quantum Computation! E. Knill, R. Laflamme and G. Milburn, Nature 409, 46, (2001) Gerard Milburn University Of Queensland

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39 Computing CommunicationsClock SynchronizationImaging SensorsMetrology The Yellow-Brick Roadmap


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