Quantum Control of Wave- Particle Duality Robert Mann D. Terno, R. Ionicioiu, T. Jennewein.

Slides:



Advertisements
Similar presentations
Introduction to Quantum Teleportation
Advertisements

1 Taoufik AMRI. Overview 3 Chapter II Quantum Protocols Chapter III Quantum States and Propositions Chapter VI Detector of « Schrödingers Cat » States.
E NTANGLEMENT II by Robert Nemiroff Michigan Tech.
Quantum Correlations in Nuclear Spin Ensembles T. S. Mahesh Indian Institute of Science Education and Research, Pune.
What really happens upon quantum measurement?[n eeds revision] References are more fully listed in my Phys Rev A paperPhys Rev A paper Art Hobson Prof.
Experiments in “Quantum Erasure” and “Delayed Choice” Preventing the simultaneous acquisition of probabilistic and deterministic results for the same result.
Fixing the lower limit of uncertainty in the presence of quantum memory Archan S. Majumdar S. N. Bose National Centre for Basic Sciences, Kolkata Collaborators:
QUANTUM MECHANICS Probability & Uncertainty 1.Probability 2.Uncertainty 3.Double-slit photons.
Quantum Information Stephen M. Barnett University of Strathclyde The Wolfson Foundation.
1 quantum teleportation David Riethmiller 28 May 2007.
Quantum Mechanics 103 Quantum Implications for Computing.
Quantum Potpourri An Attempt to Demonstrate Two Fundamental Quantum Concepts Wave-particle Duality and The Superposition Principle Frank Rioux Department.
Bell inequality & entanglement
Bell’s inequalities and their uses Mark Williamson The Quantum Theory of Information and Computation
Entanglement and Bell’s Inequalities Aaron Michalko Kyle Coapman Alberto Sepulveda James MacNeil Madhu Ashok Brian Sheffler.
Niels Bohr Institute Copenhagen University Eugene PolzikLECTURE 3.
PHYS Quantum Mechanics PHYS Quantum Mechanics Dr Jon Billowes Nuclear Physics Group (Schuster Building, room 4.10)
A lecture series on Relativity Theory and Quantum Mechanics The Relativistic Quantum World University of Maastricht, Sept 24 – Oct 15, 2014 Marcel Merk.
Experimental Quantum Teleportation Quantum systems for Information Technology Kambiz Behfar Phani Kumar.
Study and characterisation of polarisation entanglement JABIR M V Photonic sciences laboratory, PRL.
Copyright 2001 S.D. Personick, All rights reserved Quantum Information Science and Technology Dr. Stewart (“Stu”) Personick Professor, Drexel University.
SCHRODINGER’S CAT Group 1: Sudheer, Venkatesh, Hrudil, Praveen.
Philosophical Interpretations of
Institute of Technical Physics Entanglement – Beamen – Quantum cryptography The weird quantum world Bernd Hüttner CPhys FInstP DLR Stuttgart.
In 1887,when Photoelectric Effect was first introduced by Heinrich Hertz, the experiment was not able to be explained using classical principles.
School of something FACULTY OF OTHER School of Physics and Astronomy FACULTY OF MATHEMATICAL AND PHYSICAL SCIENCES Nonlocality of a single particle Jacob.
University of Gdańsk, Poland
QUANTUM TELEPORTATION
 The Bohr model describes definite electron energy levels within atoms  Bohr’s model only applied to hydrogen – it has been replaced by more sophisticated.
A comparison between Bell's local realism and Leggett-Garg's macrorealism Group Workshop Friedrichshafen, Germany, Sept 13 th 2012 Johannes Kofler.
The Road to Quantum Computing: Boson Sampling Nate Kinsey ECE 695 Quantum Photonics Spring 2014.
Atomic Particles  Atoms are made of protons, neutrons and electrons  % of the atom is empty space  Electrons have locations described.
It’s all done with Mirrors Many of the predictions of quantum mechanics are verified with ordinary matter particles (like electrons), but these experiments.
Physics 2170 – Spring Review 1 Last homework is due tomorrow at 12:50pm Final exam is on Saturday from.
Quantum Dense coding and Quantum Teleportation
1 quantum mysteries again! quantum mysteries again! classical vs. quantum correlations ‘ quantum mechanics is weird” N. Bohr Bell’s inequality? QM VIOLATES.
Early quantum optics Blackbody radiation Planck 1900: EM wave amplitudes/energies work as though they were quantized Photoelectric effect: Einstein.
DUALITY PARTICLE WAVE PARTICLE DUALITY WAVE © John Parkinson.
Frascati 2006, Beatrix C. Hiesmayr Testing QM in Particle Physics by Beatrix C. Hiesmayr Institute for Theoretical Physics University of Vienna Austria.
Wednesday, October 31 Ford Final Chapter (10). Agenda Announce: –Test Wednesday –Office Hours probably busy…better book appt. –Read Chs. 1-3 of Vilekin.
Bell tests with Photons Henry Clausen. Outline:  Bell‘s theorem  Photon Bell Test by Aspect  Loopholes  Photon Bell Test by Weihs  Outlook Photon.
Physics 2170 – Spring Some interesting aspects of quantum mechanics The last homework is due at 12:50pm.
Nonlinear Optics Lab. Hanyang Univ. Chapter 9. Wave-Particle Duality of Light 9.1 What is a Photon ? Whether light consists of particles or waves ? - ~1700,
Quantum Theory of What? What does quantum theory describe?
Uni-Heidelberg Physikalisches Insitut Jian-Wei Pan Multi-Particle Entanglement & It’s Application in Quantum Networks Jian-Wei Pan Lecture Note.
Quantum Theory By: Brian Williams. Blackbody Radiation Around the turn of the 20 th century, physicists were studying the total energy carried by all.
Effective Non-Hermitian Hamiltonian of a pre- and post-selected quantum system Lev Vaidman
Indefinite causal order in quantum mechanics Faculty of Physics, University of Vienna & Institute for Quantum Optics and Quantum Information, Vienna Mateus.
Quantum Weirdness.
Nonlocality test of continuous variable state 17, Jan,2003 QIPI meeting Wonmin Son Queen’s University, Belfast.
Physics Lecture 10 2/22/ Andrew Brandt Monday February 22, 2010 Dr. Andrew Brandt 1.HW4 on ch 5 is due Monday 3/1 2.HW5 on ch 6 will be.
Physics 102: Lecture 22, Slide 1 Hour Exam 3 Monday, April. 18 (one week from today!) –Lectures 14 – 21 –Homework through HW 11 –Discussions through Disc.
What has CP violation to do with nonlocality? by Beatrix C. Hiesmayr Faculty of Physics University of Vienna Austria Spooky action at distance also for.
Quantum Cryptography and Quantum Computing. Cryptography is about a)manipulating information b)transmitting information c)storing information.
Quantum Imaging MURI Kick-Off Meeting Rochester, June 9-10, Entangled state and thermal light - Foundamental and applications.
The Transactional Interpretation: an introduction ©2012 R. E. Kastner.
A1 “BASIC QUANTUM MECHANICS, AND SOME SURPRISING CONSEQUENCES” Anthony J. Leggett Department of Physics University of Illinois at Urbana-Champaign.
Atomic Theory Vocabulary, Models, and Scientists The Discovery of the Atom 440 B. C. to the present.
Quantum Measurements: some technical background “Measurement postulate” “Projection postulate” The two aspects of measurement Density matrices, environments,
Secret keys and random numbers from quantum non locality Serge Massar.
SCHLC- 1 S CHRÖDINGER ’ S C AT AND H ER L ABORATORY C OUSINS A.J. Leggett Dept. of Physics, University of Illinois at Urbana-Champaign 1 st Erwin Schrödinger.
Quantum nonlocality based on finite-speed causal influences
Presented By: Muhammad Imran PhD student (PIEAS)
Early quantum optics Blackbody radiation
Closing the Debates on Quantum Locality and Reality: EPR Theorem, Bell's Theorem, and Quantum Information from the Brown-Twiss Vantage   C. S. Unnikrishnan.
Quantum Teleportation
Double Slit Experiment
Heisenberg Uncertainty
Interference Two possible paths Probability Interference
The Strange World of Quantum Physics
Presentation transcript:

Quantum Control of Wave- Particle Duality Robert Mann D. Terno, R. Ionicioiu, T. Jennewein

Real or Predictive? Quantum Decay of a radioactive nucleus triggers hammer After 1 hour: 50% chance of decay After 1 hour: Either If the cat is really dead or really alive, we can’t predict which Or If we predict the state of the cat, it isn’t really dead or alive

Hidden Variable Theories Perhaps the radioactive nucleus has some (as yet) unseen physical properties (hidden variables) that DEFINITELY PREDICT the REAL state (dead or alive) of the cat Our forced choice between reality and prediction might be because we don’t (yet) know what these hidden variables are

Can we test this? Knowledge of the hidden variables will tell us which of these situations occur for any given setup

Mach-Zender Interferometer phase shift Wave: Ability to produce interference Particle: Inability to produce interference Operational Definitions:

phase shift (a half-silvered mirror) Mach-Zender Interferometer If this beamsplitter is present then the detectors register an phase-dependent interference pattern  photon is a wave If this beamsplitter is absent then the detectors each click half the time  photon is a particle

phase shift (a half-silvered mirror) Delayed Choice Experiment Randomly decide whether or not to insert this 2 nd beamsplitter AFTER the photon has gone through the 1 st beamsplitter Photon can’t “know” beforehand if it is a wave or a particle

Delayed Choice Results 2 nd Beamsplitter removed 2 nd Beamsplitter inserted Jacques, Vincent; et al. (2007) "Experimental Realization of Wheeler's Delayed-Choice Gedanken Experiment". Science 315: 966–968.

Not So Fast! Maybe the insertion (or removal) of the 2 nd beamsplitter modifies the hidden variable of the photon, telling it whether or not it is a wave or a particle BEFORE it reaches the detectors!

Quantum Delayed Choice What if the 2 nd beamsplitter itself is a quantum object? In other words, what would happen if the state of a quantum object (like another photon) determined if the 2 nd beamsplitter were inserted or not?

Quantum Delayed Choice Experiment Equivalent circuit Quantum control R. Ionicioiu & D. Terno Phys. Rev. Lett. 107, (2011)

Implications of Quantum Control Beamsplitter is in an open/closed superposition Temporal order reversed –Photon detected before learning if beamsplitter is open |0> or closed |1> –Wave/particle selection is made after detection Classical control after Quantum control before =

Hidden Variable Explanation? Hidden Variable theories  Photon is “really” a wave or “really” a particle Probability photon is really a particle or really a wave Probability beamsplitter is open or closed, given Probability detector registers, given state of beamsplitter and Probability detector registers and BS is either open or closed HV requires

No (good) HV Explanation The only way this works is if Hidden variable must be PERFECTLY correlated with the beamsplitter! Source randomly emits waves or particles with a probability distribution identical to the ancilla R. Ionicioiu & D. Terno Phys. Rev. Lett. 107, (2011)

What the Quantum DC Expt Predicts Photon is a particle Photon is a wave Photon is a particle/wave phase BS-open BS-closed

What the Quantum DC Expt Measures Photon is a particle Photon is a wave Photon is a particle/wave phase BS-open BS-closed J.S. Tang et.al. Nat. Photonics 6, 600 (2012)

(Un)Predictable (Un)Reality R. Ionicioiu, T. Jennewein, R.B. Mann & D. Terno arXiv L. Celeri, R. GomesR. Ionicioiu, T. Jennewein, R.B. Mann & D. Terno Fnd Phys (in press) Realism and Determinism are NOT compatible! Realism: Photons are either particles or waves (hidden variables determine which is the case) Determinism: The future can be predicted from the past (hidden variables determine how detectors will click) We show

Realism vs. Determinism Measure this first! Ancilla “has no state” before interacting

EPR Control Measure this first! Particle 1 Particle 2 Alice Bob  Our result: There are NO HV models that allow a deterministic AND real solution to the probability requirements

Squeezing out HV Theories? Objective: An HV Theory that is –Deterministic –WPR

Deterministic WPR theory exists 1) Must reproduce QM predictions 2) Adequacy: 3) WPR: Statistics determined by interferometer 4) WPR + Adequacy: 5) Alternative? Conspiracy!

Conspiratorial Determinism  QM Statistics Suppose other statistics: Adequacy Quantum Statistics are reproduced! HV  particle HV  wave

Testing Conspiratorial Determinism

Possible Experimental Outcomes Visibility EPR measurement parameter (determines open/closed beamsplitter) EPR entanglement parameter

Additional Applications CHSH Experiment –Measure the entangled Photons before the choice of direction is made Position/Momentum Complementarity –Fourier transform a continuous-variable state contingent on measurement of entangled ancillae Gravitational Quantum Control –Quantum-controlled COW expt?

Summary Quantum Physics forces a choice between –Realism (objects are definitely waves or particles at any given time) –Predictability (given initial conditions unambiguously determine how detectors will register Is there a way out? –Superluminal communication (signals go faster than light) –Infinite regression (hidden variables for the hidden variables for the hidden variables …)

My Research Group + Friends Aida Ahmadzadegan Wilson Brenna Eric Brown Paulina Corona-Ugalde Keith Ng Marvellous Onuma-Kalu Alexander Smith Aharon Brodutch Eduardo Martin-Martinez Marco Piani