Quantum teleportation via photonic Faraday rotation Juan-Juan Chen ( 陈娟娟 ) Advisor: Jun-Hong An.

Slides:



Advertisements
Similar presentations
Introduction to Quantum Teleportation
Advertisements

Nanophotonic Devices for Quantum Optics Feb 13, 2013 GCOE symposium Takao Aoki Waseda University.
Separable States can be Used to Distribute Entanglement Toby Cubitt 1, Frank Verstraete 1, Wolfgang Dür 2, and Ignacio Cirac 1 1 Max Planck Institüt für.
Niels Bohr Institute Copenhagen University Quantum memory and teleportation with atomic ensembles Eugene Polzik.

Quantum Entanglement of Rb Atoms Using Cold Collisions ( 韓殿君 ) Dian-Jiun Han Physics Department Chung Cheng University.
Universal Optical Operations in Quantum Information Processing Wei-Min Zhang ( Physics Dept, NCKU )
PG lectures Spontaneous emission. Outline Lectures 1-2 Introduction What is it? Why does it happen? Deriving the A coefficient. Full quantum description.
Superdense coding. How much classical information in n qubits? Observe that 2 n  1 complex numbers apparently needed to describe an arbitrary n -qubit.

Niels Bohr Institute Copenhagen University Eugene PolzikLECTURE 5.
EPR – pair usage in the quantum teleportation The Question was: Is the Quantum Mechanical Description of Reality Actually Complete?
Light-Matter Quantum Interface
Efficient many-party controlled teleportation of multi-qubit quantum information via entanglement Chui-Ping Yang, Shih-I Chu, Siyuan Han Physical Review.
Cavity QED as a Deterministic Photon Source Gary Howell Feb. 9, 2007.
Future Challenges in Long-Distance Quantum Communication Jian-Wei Pan Hefei National Laboratory for Physical Sciences at Microscale, USTC and Physikalisches.
Deterministic teleportation of electrons in a quantum dot nanostructure Deics III, 28 February 2006 Richard de Visser David DiVincenzo (IBM, Yorktown Heights)
Quantum Memory For Teleportation And the Quantum Internet Team: Ahmed Hasan (Undergrad Student) Ken Salit (Graduate Student) Jacob Morzinski (Graduate.
Dogma and Heresy in Quantum Computing DoRon Motter February 18, 2002.
Transfer of entanglement from a Gaussian field to remote qubits Myungshik Kim Queen’s University, Belfast UniMilano 14 December 2004.
PG lectures Spontaneous emission. Outline Lectures 1-2 Introduction What is it? Why does it happen? Deriving the A coefficient. Full quantum description.

Quantum Computation and Quantum Information – Lecture 2 Part 1 of CS406 – Research Directions in Computing Dr. Rajagopal Nagarajan Assistant: Nick Papanikolaou.
Experimental Quantum Teleportation Quantum systems for Information Technology Kambiz Behfar Phani Kumar.
Interfacing quantum optical and solid state qubits Cambridge, Sept 2004 Lin Tian Universität Innsbruck Motivation: ion trap quantum computing; future roads.
ENTANGLEMENT IN SMALL SELF-CONTAINED QUANTUM FRIDGES NICOLAS BRUNNER, RALPH SILVA, PAUL SKRZYPCZYK, MARCUS HUBER NOAH LINDEN & SANDU POPESCU SINGAPORE.
QUANTUM ENTANGLEMENT AND IMPLICATIONS IN INFORMATION PROCESSING: Quantum TELEPORTATION K. Mangala Sunder Department of Chemistry IIT Madras.
Quantum Information, Communication and Computing Jan Kříž Department of physics, University of Hradec Králové Doppler Institute for mathematical physics.
Purdue University Spring 2014 Prof. Yong P. Chen Lecture 16 (3/31/2014) Slide Introduction to Quantum Optics.
Project funded by the Future and Emerging Technologies arm of the IST Programme FET-QIPC -RAMBOQ IST RAMBOQ pRobabilistic gAtes Making Binary.
Paraty, Quantum Information School, August 2007 Antonio Acín ICFO-Institut de Ciències Fotòniques (Barcelona) Quantum Cryptography (III)
Quantum computation with solid state devices - “Theoretical aspects of superconducting qubits” Quantum Computers, Algorithms and Chaos, Varenna 5-15 July.
Jian-Wei Pan Decoherence-free sub-space and quantum error-rejection Jian-Wei Pan Lecture Note 7.
A deterministic source of entangled photons David Vitali, Giacomo Ciaramicoli, and Paolo Tombesi Dip. di Matematica e Fisica and Unità INFM, Università.
Witnessing Quantum Coherence IWQSE 2013, NTU Oct. 15 (2013) Yueh-Nan Chen ( 陳岳男 ) Dep. of Physics, NCKU National Center for Theoretical Sciences (South)
PROPOSAL OF A UNIVERSAL QUANTUM COPYING MACHINE IN CAVITY QED Joanna Gonzalez Miguel Orszag Sergio Dagach Facultad de Física Pontificia Universidad Católica.
PRESENTED BY MIDHUN.T - EC 3 - S 61 TOPIC – QUANTUM TELEPORTATION Presented by - MIDHUN T EC 3, S 6 ROLL NO. 20 Reg no
A Single Photon Source for Photon-atom Interaction Xingxing Xing Centre for Quantum Info. & Quantum Control, Dept. of Physics, Univ. of Toronto CQISC 2006,
School of something FACULTY OF OTHER School of Physics and Astronomy FACULTY OF MATHEMATICAL AND PHYSICAL SCIENCES Putting entanglement to work: Super-dense.
Information Processing by Single Particle Hybrid Entangled States Archan S. Majumdar S. N. Bose National Centre for Basic Sciences Kolkata, India Collaborators:
You Did Not Just Read This or did you?. Quantum Computing Dave Bacon Department of Computer Science & Engineering University of Washington Lecture 3:
Centre for Quantum Physics & Technology, Clarendon Laboratory, University of Oxford. Karl Surmacz (University of Oxford, UK) Efficient Unitary Quantum.
Quantifying quantum discord and Entanglement of Formation via Unified Purifications 岑理相 四川大学 物理科学与技术学院.
Quantum Dense coding and Quantum Teleportation
Bell Measurements and Teleportation. Overview Entanglement Bell states and Bell measurements Limitations on Bell measurements using linear devices Teleportation.
What is Qu antum In formation and T echnology? Prof. Ivan H. Deutsch Dept. of Physics and Astronomy University of New Mexico Second Biannual Student Summer.
1 entanglement-quantum teleportation entanglement-quantum teleportation entanglement (what is it?) quantum teleportation (intuitive & mathematical) ‘ quantum.
Copenhagen interpretation Entanglement - qubits 2 quantum coins 2 spins ( spin “up” or spin “down”) Entangled state many qubits: Entangled state:
Quantum II (PHYS 4410) Lecture 6 Entangled states and quantum teleportation Homework sessions are now Monday 4-6P here. HWK 2 is due Wed. by 5PM.
Efficiency of Multi-Qubit W states in Information Processing Atul Kumar IPQI-2014 IIT Jodhpur
Quantum Entanglement and Distillation in Information Processing Shao-Ming Fei
Efficient measure of scalability Cecilia López, Benjamin Lévi, Joseph Emerson, David Cory Department of Nuclear Science & Engineering, Massachusetts Institute.
Gang Shu  Basic concepts  QC with Optical Driven Excitens  Spin-based QDQC with Optical Methods  Conclusions.
Quantum Computing: An Overview for non-specialists Mikio Nakahara Department of Physics & Research Centre for Quantum Computing Kinki University, Japan.
Mesoscopic Physics Introduction Prof. I.V.Krive lecture presentation Address: Svobody Sq. 4, 61022, Kharkiv, Ukraine, Rooms. 5-46, 7-36, Phone: +38(057)707.
Distillation and determination of unknown two-qubit entanglement: Construction of optimal witness operator Heung-Sun Sim Physics, KAIST ESF conference:
Suggestion for Optical Implementation of Hadamard Gate Amir Feizpour Physics Department Sharif University of Technology.
Quantum Teleportation What does the future hold?.
Quantum Phase Transition of Light: A Renormalization Group Study
Spontaneous Emission in Quantum State
Optical qubits
Quantum Teleportation
Coupled atom-cavity system
Quantum Teleportation
Cavity QED
Spin Many quantum experiments are done with photon polarization instead of electron spin Here is the correspondence between the two And the measurement.
Qubit-induced high-order nonlinear interaction of the polar molecules
Linear Optical Quantum Computing
INTERNATIONAL WORKSHOP ON QUANTUM INFORMATION
Experimental Quantum Teleportation*
Presentation transcript:

Quantum teleportation via photonic Faraday rotation Juan-Juan Chen ( 陈娟娟 ) Advisor: Jun-Hong An

3 Summary 3 Acknowledgments 4 Quantum teleportation via Faraday rotation 1 2 Introduction

 Cavity QED system gives an ideal candidate for QIP. Stationary atoms = static qubits for storing QI; Photons = Flying qubits for transmitting QI. Cavity QED system is perfect interface for the interaction atoms and photons.

 The earlier QT schemes use atoms to transfer QI. Not suitable for long-distance QT. Not easy to keep the QI in the flying atoms. The high-Q condition for the cavities is hard to meet. QT in cavity QED system

 Some schemes use the leaking photons as flying qubits to QT. Advantage: Works in low-Q condition. Disadvantage: Intrinsically probabilistic.

Low-Q cavity Is QT with the photon as flying qubit realizable in this low-Q cavity regime in a deterministic fashion? Condition:. Although the imperfection of the cavity mirror induces the damping of the cavity field, it gives us an efficient injection way of the photon to the cavity.

The Faraday rotation of the J - C model From J.-H. An et al. (2009). Faraday rotation

Figure 3.1: Schematic for teleporting an unknown atomic state from Alice's side to the atoms at Bob's side. The entanglement channel is formed between Bob's atom and the flying photon. The arrows shows the flying direction of the photon, and the bold line denotes a quarter-wave plate. The schematic of our scheme

 The scalability of our scheme. The case of bipartite state The case of tripartite state

Advantages to our schemes : Photons as flying qubits to transmit QI; suitable for long-distance QT. Work in low-Q regime of cavities; the damping of cavity plays active role; Insensitive to atomic spontaneous emission; Only need two-qubit entanglement in multi-qubit QT; Intrinsically deterministic.

Acknowledgments I am firstly greatly indebted to my advisor, Professor Jun-Hong An for his serious patience, careful guidance and assistance to my research work during these three years. At same time I would also like to thank Professor Hong-Gang Luo and collegues of the Center for Interdisciplinary Studies for many valuable and helpful discussions with me. In the last, I can not forget the long-term supports of my parents, mysister to my study.