Quantum Electron Optics Electron Entanglement

Slides:



Advertisements
Similar presentations
Scanning tunnelling spectroscopy
Advertisements

NOKIA MEETING1 APS MARCH MEETING 2007 Denver, Colorado LATEST IN GRAPHENE RESEARCH Mikko Paalanen Low Temperature Laboratory Helsinki.
Nanostructures on ultra-clean two-dimensional electron gases T. Ihn, C. Rössler, S. Baer, K. Ensslin C. Reichl and W. Wegscheider.
Spectroscopy at the Particle Threshold H. Lenske 1.
Signatures of Tomonaga-Luttinger liquid behavior in shot noise of a carbon nanotube Patrik Recher, Na Young Kim, and Yoshihisa Yamamoto Institute of Industrial.
Probing Superconductors using Point Contact Andreev Reflection Pratap Raychaudhuri Tata Institute of Fundamental Research Mumbai Collaborators: Gap anisotropy.
Quantum Coherent Nanoelectromechanics Robert Shekhter Leonid Gorelik and Mats Jonson University of Gothenburg / Heriot-Watt University / Chalmers Univ.
Dynamical response of nanoconductors: the example of the quantum RC circuit Christophe Mora Collaboration with Audrey Cottet, Takis Kontos, Michele Filippone,
High Temperature Superconductivity: D. Orgad Racah Institute, Hebrew University, Jerusalem Stripes: What are they and why do they occur Basic facts concerning.
Concepts in High Temperature Superconductivity
Chaos and interactions in nano-size metallic grains: the competition between superconductivity and ferromagnetism Yoram Alhassid (Yale) Introduction Universal.
Laterally confined Semiconductor Quantum dots Martin Ebner and Christoph Faigle.
Full counting statistics of incoherent multiple Andreev reflection Peter Samuelsson, Lund University, Sweden Sebastian Pilgram, ETH Zurich, Switzerland.
14. April 2003 Quantum Mechanics on the Large Scale Banff, Alberta 1 Relaxation and Decoherence in Quantum Impurity Models: From Weak to Strong Tunneling.
5/2/2007Cohen Group Meeting1 Luttinger Liquids Kevin Chan Cohen Group Meeting May 2, 2007.
Center for Quantum Information ROCHESTER HARVARD CORNELL STANFORD RUTGERS LUCENT TECHNOLOGIES Entanglement and Memory-Force Bound States Beyond Bell Pairing.
Introduction to the Kondo Effect in Mesoscopic Systems.
BOSTON UNIVERSITY PHYSICS DEPARTMENT Nano-spectroscopy of Individual Single Walled Carbon Nanotubes AFM image 1um Measure single, unperturbed nanotube.
© 2010 Eric Pop, UIUCECE 598EP: Hot Chips Conductance Quantization One-dimensional ballistic/coherent transport Landauer theory The role of contacts Quantum.
Markus Büttiker University of Geneva Haifa, Jan. 12, 2007 Mesoscopic Capacitors.
Antiferomagnetism and triplet superconductivity in Bechgaard salts
Electron Entanglement via interactions in a quantum dot Gladys León 1, Otto Rendon 2, Horacio Pastawski 3, Ernesto Medina 1 1 Centro de Física, Instituto.
Ballistic and quantum transports in carbon nanotubes.
Superconducting Qubits Kyle Garton Physics C191 Fall 2009.
Five-Lecture Course on the Basic Physics of Nanoelectromechanical Devices Lecture 1: Introduction to nanoelectromechanical systems (NEMS) Lecture 2: Electronics.
Single Photon Emitters and their use in Quantum Cryptography Presentation by: Bram Slachter Supervision: Dr. Ir. Caspar van der Wal.
System and definitions In harmonic trap (ideal): er.
Spin and Charge Pumping in an Interacting Quantum Wire R. C., N. Andrei (Rutgers University, NJ), Q. Niu (The University of Texas, Texas) Quantum Pumping.
Electron coherence in the presence of magnetic impurities
Radiation induced photocurrent and quantum interference in n-p junctions. M.V. Fistul, S.V. Syzranov, A.M. Kadigrobov, K.B. Efetov.
An Introduction to Carbon Nanotubes
Gerousis Toward Nano-Networks and Architectures C. Gerousis and D. Ball Department of Physics, Computer Science and Engineering Christopher Newport University.
Carbon Nanotube Intramolecular Junctions. Nanotubes A graphene sheet with a hexagonal lattice…
„To bunch or not to bunch” Tóvári Endre Journal Club márc. 8. Coherence and Indistinguishability of Single Electrons Emitted by Independent Sources.
Chap. 41: Conduction of electricity in solids Hyun-Woo Lee.
Supercurrent through carbon-nanotube-based quantum dots Tomáš Novotný Department of Condensed Matter Physics, MFF UK In collaboration with: K. Flensberg,
Electronic States and Transport in Quantum dot Ryosuke Yoshii YITP Hayakawa Laboratory.
L4 ECE-ENGR 4243/ FJain 1 Derivation of current-voltage relation in 1-D wires/nanotubes (pp A) Ballistic, quasi-ballistic transport—elastic.
NSF- NIRT: "Surface State Engineering" Charge Storage and Conduction in Organo-Silicon Heterostructures as a Basis for Nanoscale Devices John C. Bean (PI)
Wigner molecules in carbon-nanotube quantum dots Massimo Rontani and Andrea Secchi S3, Istituto di Nanoscienze – CNR, Modena, Italy.
Gang Shu  Basic concepts  QC with Optical Driven Excitens  Spin-based QDQC with Optical Methods  Conclusions.
Quantum Noise of a Carbon Nanotube Quantum Dot in the Kondo Regime Exp : J. Basset, A.Yu. Kasumov, H. Bouchiat and R. Deblock Laboratoire de Physique des.
An introduction to the theory of Carbon nanotubes A. De Martino Institut für Theoretische Physik Heinrich-Heine Universität Düsseldorf, Germany.
1 Realization of qubit and electron entangler with NanoTechnology Emilie Dupont.
Measuring Quantum Coherence in the Cooper-Pair Box
Current noise in 1D electron systems ISSP International Summer School August 2003 Björn Trauzettel Albert-Ludwigs-Universität Freiburg, Germany [Chung.
Charge pumping in mesoscopic systems coupled to a superconducting lead
Kondo effect in a quantum dot without spin Hyun-Woo Lee (Postech) & Sejoong Kim (Postech  MIT) References: H.-W. Lee & S. Kim, cond-mat/ P. Silvestrov.
Spin-orbit interaction in semiconductor quantum dots systems
Nanoelectronics Part II Single-Electron and Few-Electron Phenomena and Devices Chapter 6 Tunnel Junctions and Applications of Tunneling
Electronic transport in one-dimensional wires Akira Furusaki (RIKEN)
Basics of edge channels in IQHE doing physics with integer edge channels studies of transport in FQHE regime deviations from the ‘accepted’ picture Moty.
The Center for Ultracold Atoms at MIT and Harvard Strongly Correlated Many-Body Systems Theoretical work in the CUA Advisory Committee Visit, May 13-14,
제 4 장 Metals I: The Free Electron Model Outline 4.1 Introduction 4.2 Conduction electrons 4.3 the free-electron gas 4.4 Electrical conductivity 4.5 Electrical.
Quasiparticle Excitations and Optical Response of Bulk and Reduced-Dimensional Systems Steven G. Louie Department of Physics, University of California.
Capri Spring School, April 8, 2006
Fractional Berry phase effect and composite particle hole liquid in partial filled LL Yizhi You KITS, 2017.
Characterization of CNT using Electrostatic Force Microscopy
Lecture 7 DFT Applications
Electrons in a Crystal Chapter 6: 3
RESONANT TUNNELING IN CARBON NANOTUBE QUANTUM DOTS
Introduction to Nanoheat; Aspel group
Experimental Evidences on Spin-Charge Separation
Christian Scheller
Density of States (DOS)
Full Current Statistics in Multiterminal Mesoscopic Conductors
Quantum Computing: the Majorana Fermion Solution
Density of States (DOS)
Tunneling through a Luttinger dot
Density of States (DOS)
Presentation transcript:

Quantum Electron Optics Electron Entanglement Center for Quantum Information ROCHESTER HARVARD CORNELL STANFORD RUTGERS LUCENT TECHNOLOGIES Quantum Electron Optics and Electron Entanglement Na Young Kim (Stanford, AP) Manuel Aranzana (ENS) William D. Oliver (Stanford, EE) Leo Di Carlo (Harvard) Fumiko Yamaguchi (Stanford, AP/EE) Gwendal Feve (ENS) Yoshihisa Yamamoto (Stanford, AP/EE) Jungsang Kim (Lucent) Robert Liu (UCSF) Jing Kong (Stanford, Chem) Xavier Maitre (CNRS) Hongjie Dai (Stanford, Chem)

Electron Entanglement via a Quantum Dot Single electron tunneling suppressed by energy conservation EL = ER1 = ER2 Two-electron virtual tunneling is allowed EL1 + EL2 = ER1 + ER2 Only singlet-state remains at output: indistinguishability and Fermi statistics including Pauli Exclusion Principle Non-linearity: Coulomb charging energy U Optical analogy: Chi-(3) four-wave mixing process L R2 R1 VL VR1 VR2 ER1 Ed U ER2 X EL1 EL2 W. D. Oliver et al., PRL 88, 037901 (2002)

Noise Suppression in Carbon Nanotubes Experimental Fano factor (noise suppresion) LED/PD CNT 200 nm SWCNT R = 17.4 kW 400 800 1200 1600 I PD (nA) , 50 150 200 250 S (arb. units) SCNT = 0.17 (2eI) Elastic scattering: 1-T (transparent contacts) ST = 2eI(1-T) = 0.63 (2eI) Remainder of suppression: LL parameter g S = 2e*IB = 2 (ge) I(1-T) = g (1-T) 2eI g, elastic scattering yield noise suppression CNT: g = 0.2 ~ 0.3 theory, g = 0.28 expt SCNT = g(1-T) 2eI= 0.17 (2eI)

Integrated CNT / SC Structures for Electron Entanglement CNT as a quantum dot (0D) structure ~20 nm Easy to make strong tunnel barriers Strong confinement w/out surface depletion effect Very small CNT quantum dot entangler CNT as a quantum wire (1D) structure “Ideal” 1D channel, minimize intermode coupling Reduced scattering phase space (cf., 2D leads) “interconnect” with long mean free path (?) Caveat: LL quasi-particle not free electron (cf., Fermi Liquid) collective excitation (CDW, SDW) TBD: how does this effect entanglement ?? CNT as 0D and 1D structure “Kinks”, CNT overlap, AFM tip, etc. create tunnel barrier

Future Directions Theory of regulated entangled pair generation “unitary limit” of conductance with resonant biasing ….. “natural regulation” turnstile-like operation ….. “engineered regulation” Luttinger Liquid theory Experimental demonstration of electron entangler Integrated semiconductor / CNT structure Bunching / Anti-bunching experiment Noise Properties of the 0.7 Structure HBT-type Experiment: shows noise suppression one channel in unitary limit one channel partially conducting Collision experiment: spin polarized vs. unpolarized 0.8 -0.1 -0.2 0.6 3 1 2 4 -0.3 Conductance (G/GQ) Normalized xcov 0.4 -0.4 -0.5 0.2 -0.6 -0.7 -2.9 -2.8 -2.7 -2.6 -2.5 Gate Voltage (V)