Emergent Majorana Fermion in Cavity QED Lattice

Slides:



Advertisements
Similar presentations
Chiral Tunneling and the Klein Paradox in Graphene M. I. Katsnelson, K
Advertisements

Quantum Theory of Collective Atomic Recoil in Ring Cavities
APRIL 2010 AARHUS UNIVERSITY Simulation of probed quantum many body systems.
Quantum Computer Implementations
Zero-Phonon Line: transition without creation or destruction of phonons Phonon Wing: at T = 0 K, creation of one or more phonons 7. Optical Spectroscopy.
Vibrational Spectroscopy of Cold Molecular Ions Ncamiso Khanyile Ken Brown Lab School of Chemistry and Biochemistry June 2014.
Entanglement of Movable Mirrors in a Correlated Emission Laser
Quantum “disordering” magnetic order in insulators, metals, and superconductors HARVARD Talk online: sachdev.physics.harvard.edu Perimeter Institute, Waterloo,
Dynamics of Vibrational Excitation in the C 60 - Single Molecule Transistor Aniruddha Chakraborty Department of Inorganic and Physical Chemistry Indian.
Quantum Entanglement of Rb Atoms Using Cold Collisions ( 韓殿君 ) Dian-Jiun Han Physics Department Chung Cheng University.
L. Besombes et al., PRL93, , 2004 Single exciton spectroscopy in a semimagnetic nanocrystal J. Fernández-Rossier Institute of Materials Science,
Fermions without Fermi Fields RC Ball Department of Physics University of Warwick Fermions can emerge as the elementary excitations of generalised spin.
Strongly Correlated Systems of Ultracold Atoms Theory work at CUA.
Jordan-Wigner Transformation and Topological characterization of quantum phase transitions in the Kitaev model Guang-Ming Zhang (Tsinghua Univ) Xiaoyong.
IMT INSTITUT DE MICROTECHNIQUE NEUCHÂTEL Optical cavity with high quality factor Q Photonic crystals course final presentation Karin Söderström.
Fractional Quantum Hall states in optical lattices Anders Sorensen Ehud Altman Mikhail Lukin Eugene Demler Physics Department, Harvard University.
Cavity QED as a Deterministic Photon Source Gary Howell Feb. 9, 2007.
Guillermina Ramirez San Juan
Interference of fluctuating condensates Anatoli Polkovnikov Harvard/Boston University Ehud Altman Harvard/Weizmann Vladimir Gritsev Harvard Mikhail Lukin.
Robustness of Topological Superconductivity in Proximity-Coupled Topological Insulator Nanoribbons Tudor D. Stanescu West Virginia University Collaborators:
Carrier Wave Rabi Flopping (CWRF) Presentation by Nathan Hart Conditions for CWRF: 1.There must exist a one photon resonance with the ground state 2.The.
PG lectures Spontaneous emission. Outline Lectures 1-2 Introduction What is it? Why does it happen? Deriving the A coefficient. Full quantum description.
Guillaume TAREL, PhC Course, QD EMISSION 1 Control of spontaneous emission of QD using photonic crystals.
Topological superconductor to Anderson localization transition in one-dimensional incommensurate lattices 蔡小明
Bose-Einstein Condensate Fundaments, Excitation and Turbulence Vanderlei Salvador Bagnato Instituto de Física de São Carlos – Universidade de São Paulo.
Decoherence issues for atoms in cavities & near surfaces Peter Knight, Imperial College London work with P K Rekdal,Stefan Scheel, Almut Beige, Jiannis.
EXPLORING NATURE WITH A QUANTUM SIMULATOR
Strongly correlated phenomena in cavity QED Fernando G.S.L. Brandão 1,2 Michael J. Hartmann 1,2 Martin B. Plenio 1,2 1 Institute for Mathematical Sciences,
Han Pu Rice University Collaborators: Lei Jiang (NIST/JQI) Hui Hu, Xia-Ji Liu (Swinburne) Yan Chen (Fudan U.) 2013 Hangzhou Workshop on Quantum Matter.
M.T. Bell et al., Quantum Superinductor with Tunable Non-Linearity, Phys. Rev. Lett. 109, (2012). Many Josephson circuits intended for quantum computing.
@Nagoya U. Sept. 5, 2009 Naoto Nagaosa Department of Applied Physics
Composite Fermion Groundstate of Rashba Spin-Orbit Bosons Alex Kamenev Fine Theoretical Physics Institute, School of Physics & Astronomy, University of.
Christine Muschik and J. Ignacio Cirac Entanglement generated by Dissipation Max-Planck-Institut für Quantenoptik Hanna Krauter, Kasper Jensen, Jonas Meyer.
Dynamics of phase transitions in ion traps A. Retzker, A. Del Campo, M. Plenio, G. Morigi and G. De Chiara Quantum Engineering of States and Devices: Theory.
Wave Packet Echo in Optical Lattice and Decoherence Time Chao Zhuang U(t) Aug. 15, 2006 CQISC2006 University of Toronto.
Correlated States in Optical Lattices Fei Zhou (PITP,UBC) Feb. 1, 2004 At Asian Center, UBC.
Strong coupling between a metallic nanoparticle and a single molecule Andi Trügler and Ulrich Hohenester Institut für Physik, Univ. Graz
Drude weight and optical conductivity of doped graphene Giovanni Vignale, University of Missouri-Columbia, DMR The frequency of long wavelength.
VORTICES IN BOSE-EINSTEIN CONDENSATES TUTORIAL R. Srinivasan IVW 10, TIFR, MUMBAI 8 January 2005 Raman Research Institute, Bangalore.
Gang Shu  Basic concepts  QC with Optical Driven Excitens  Spin-based QDQC with Optical Methods  Conclusions.
QUEST - Centre for Quantum Engineering and Space-Time Research Multi-resonant spinor dynamics in a Bose-Einstein condensate Jan Peise B. Lücke, M.Scherer,
Transverse optical mode in a 1-D chain J. Goree, B. Liu & K. Avinash.
Atoms in optical lattices and the Quantum Hall effect Anders S. Sørensen Niels Bohr Institute, Copenhagen.
Plasmonic vector near-field for composite interference, SPP switch and optical simulator Tao Li(李涛) National Laboratory of Solid State.
Topology induced emergent dynamic gauge theory in an extended Kane-Mele-Hubbard model Xi Luo January 5, 2015 arXiv:
Spin-orbital effects in frustrated antiferromagnets Oleg A. Starykh, University of Utah, DMR Electron spin resonance (ESR) measures absorption.
Gilles Montambaux, Orsay Les graphènes artificiels, des microondes aux atomes froids TexPoint fonts used in EMF. Read the TexPoint manual before you delete.
Exact ground states of a frustrated 2D magnet: deconfined fractional excitations at a first order quantum phase transition Cristian D. Batista and Stuart.
Aiming at Quantum Information Processing on an Atom Chip Caspar Ockeloen.
The Puzzling Boundaries of Topological Quantum Matter Michael Levin Collaborators: Chien-Hung Lin (University of Chicago) Chenjie Wang (University of Chicago)
C 60 - Single Molecule Transistor Aniruddha Chakraborty Indian Institute of Technology Mandi, Mandi , Himachal Pradesh, India.
Topological physics with a BEC: geometric pumping and edge states Hsin-I Lu with Max Schemmer, Benjamin K. Stuhl, Lauren M. Aycock, Dina Genkina, and Ian.
Dirac’s inspiration in the search for topological insulators
1 Vortex configuration of bosons in an optical lattice Boulder Summer School, July, 2004 Congjun Wu Kavli Institute for Theoretical Physics, UCSB Ref:
QUANTUM PHYSICS BY- AHRAZ, ABHYUDAI AND AKSHAY LECTURE SECTION-5 GROUP NO. 6.
Jiří Minář Centre for Quantum Technologies
B3 Correlations in antiferromagnets
Photo-induced topological phase transitions in ultracold fermions
Search for Novel Quantum Phases in
Spin-Orbit Coupling Effects in Bilayer and Optical Lattice Systems
Quantum Phase Transition of Light: A Renormalization Group Study
BOSE-EINSTEIN CONDENSATES A REVIEW OF EXPERIMENTAL RESULTS
Remote tuning of an optical resonator
Topological Insulators
On the collapses and revivals in the Rabi Hamiltonian
Strong coupling of a superradiant spin ensemble B. C. Rose, A. M
Strong Coupling of a Spin Ensemble to a Superconducting Resonator
Majorana Spin Diagnostics
Quantum Computing: the Majorana Fermion Solution
SOC Fermi Gas in 1D Optical Lattice —Exotic pairing states and Topological properties 中科院物理研究所 胡海平 Collaborators : Chen Cheng, Yucheng Wang, Hong-Gang.
Presentation transcript:

Emergent Majorana Fermion in Cavity QED Lattice Dr. Sujit Sarkar Poornaprajna Institute of Scientific Research, Bangalore-560 080 Acknowledgement: Raman Research Institute Library And CCMT of Phys. Dept of IISc Bangalore

Out Line of the Talk: (1). What is Majorana Fermion? (2). What is Optical Cavity QED? (3). Motivation. (4). Interesting Experiments. (5). Model Hamiltonians. (6). Results and Discussions. (7). Conclusions.

Majorana Fermion?

Majorana Fermions in Quantum Condensed Matter System (1). QH system with filling fraction 5/2. (2). Kitaev: Majorana Fermions modes in one dimensional model. (3). Edge state of 1D system: Electrostatic defect lines in superconductor and quasi one dimensional superconductor. (4). Cold atoms trapped in one-dimension. (5). Topological quantum computation. What is about Cavity QED?

Majorana Fermion in Superconductor

Motivation: (1). Interesting Experimental Findings. (2). Application of Quantum Many Body Physics and Quantum Field Theoretical Aspects in Cavity QED.

Light Crystallization:

Reference: Matrin B Plenio et al. (1) Reference: Matrin B Plenio et al. (1). Laser and Photonics Reviews, August 19, 2008. (2). Phys. Rev. Lett 99, 103601 (2007). (3). Phys. Rev. Lett 99, 160501 (2007). (4). Nature Physics 2, 849 (2006).

Effective Spin Model

o0

Luttinger Liquid Physics Intrinsic in Cavity QED Lattice

Cavity QED Lattice Physics in XY Model

Conclusions: (1). We express cavity QED lattice system in integrable quantum spin system. (2). Elementary excitation of the cavity QED lattice is the Majorana fermions. (3). We have derived the Dirac equation for the cavity QED lattice and the condition for the massless excitations. (4). We have derived the condition in terms of Rabi frequency oscillations and coupling strengths where the physics of Transverse Ising model and anisotropic XY model are the same.

Thank You