QUANTUM ELECTRONICS ON THE TRAY* *Sur le plateau (de Saclay)
|
|
- Malcolm Walsh
- 6 years ago
- Views:
Transcription
1 QUANTUM ELECTRONIC ON THE TRAY* *ur le plateau (de aclay)
2 Goal: Reveal the quantum behavior of electrons
3 everal ways of revealing the quantum behavior of electrons 1 Interference experiments of coherent electron waves B 2 Particle-in-a box quantum energy levels of artificial atoms 3 Interaction via exchange of light quanta with environment?
4 Interference of electrons in vacuum Change phase with Aharonov Bohm flux In an electron microscope Detector Interference pattern builds up on detector. What about in solids? 4
5 Electron interference in solids? Does disorder destroy interference? Defects What modulates electron interference? Aharonov Bohm flux modulates the phase: j =-2p F/F 0 F=B creen? creen=resistance Constructive or desctructive interference determine electric 5 transmission
6 R ( ) Electron interference in micron-size rings F=B Magnetic flux modulates transmission Ring in a two dimensional electron «gas» (D. Mailly, LPN Marcoussis) micron A (small) fraction of resistance is modulated by a magnetic field! 6400 T=0.05 Kelvin champ magnétique B (Gauss) 6
7 Much more than resistance: all quantum properties are modulated by magnetic flux F ext E j =-2p F ext /F 0 0 p 2 2p j Phase dependent electron spectrum Consequence= persistent current in ring (non superconducting), I persistent =-de/df Contactless detection of these currents: Mesoscopic Physics Group, LP Orsay (H. Bouchiat)
8 Interference between 1D Quantum Hall edge states Disordered 2D conductor in zero magnetic field Many diffusive trajectories Disordered 2D conductor in high magnetic field B Quantum Hall edge states Propagate ballistically, as if no disorder uantum Hall edge states perfect for interference experiments
9 Interference between 1D Quantum Hall edge states Mach Zender interferometer in a 2D «electron gas» B Ballistic Quantum Hall edge states Quantum interference over several tens of micrometers. Can change length of path with V G NanoElectronics group, PEC, CEA aclay Quantum Transport group, LPN Marcoussis What limits interference: interaction between edge states (many body, not independent)?
10 Density of states x occupation Another way to control phase: use superconductors uperconductors have a fixed phase Macroscopic wavefunction y BC =De ij Cooper pairs +k, -k, A gap D in the spectrum, and R=0 Energy Empty quasiparticle states D 0 -D No single particle states at low energy: only paired electrons Occupied quasiparticle states
11 Two superconductors impose interesting boundary conditions: a gap and a phase difference,j 1 Disordered non wire,j 2 Phase difference controls all properties of junction
12 uperconductors impose phase difference and induce entanglement between pairs of electrons,j 1 Disordered non wire,j 2 A phase dependent gap appears due to quantum interference gap No gap gap p 2p j 0 p 2p j Phase dependent spectrum with gap due to entanglement of pairs of electrons: upercurrent
13 Pair correlations induced in all sorts of conductors metals Ferromagnets Meso group LP Orsay;,D,De ij 1 DNA Au, Cu, Ag graphene,d Molecules with spins,j 1,j 2 carbon nanotube A single atom! N2 group LP Orsay; Quantronics group CEA aclay; Theory group LP Orsay; Theory group Polythechnique
14 Guessing game What s what? Physique mésoscopique LP Orsay Physique mésoscopique LP Orsay 300 nm Quantronique CEA aclay 1 mm
15 2 Particle-in-a box quantum energy levels of artificial atoms Carbon nanotubes: 2 levels! Meso group LP Orsay Transport via orbitals of real atoms Quantronics group CEA aclay Discrete levels in electron box Quantum dots: a small electron box Quantum Transport, LPN Marcoussis Questions: Probe quantum states of these systems. Magnetism, superconductivity, correlations via such a small number of channels?
16 2 Particle-in-a box quantum energy levels of artificial atoms Classical Just two levels: Form a quantum bit In practice, quantum bits = artificial atoms made of superconductors Quantronics group CEA aclay
17 Example of processor with two qbits Qubit= Jonction Josephson + Capacitor Quantronics group, aclay
18 3 Interaction via electromagnetic (light) quanta with environment? Current fluctuations in conductor : NOIE Intrinsic noise reveals transport properties of conductor : Low frequency: can reveal discreteness of electron charge and statistics High frequency (>1 GHz: hw>>k B T), realm of quantum optics: Electronic fluctuations within conductor can be seen as photons. Photon frequency= knob to probe dynamics and energy of conductor. Entanglement of emitted photons? Difference between emission and absorption? Reveal dynamics of systems and energy spectrum Can outer circuit modify (via photon exchange) electronic fluctuations?
19 Interaction via electromagnetic (light) quanta with environment? Emission w<0 Mesoscopic system Absorption w>0 insulator On-chip quantum detector (counts photons, up to 100 GHz) Meso group LP Orsay Theory group LP Orsay Detect very high frequency noise of quantum system. ensitive to difference between emission and absorption (hw>>kt ) Reveal dynamics of systems and energy spectrum
20 Interaction via electromagnetic (light) quanta with environment? electrons photons Mesoscopic system Quantum transport, LPN Marcoussis Quantronics, CEA aclay NanoElectronics, CEA aclay Impedance Z(w) Circuit in which system is embedded can change (via photon exchange) resistance of mesoscopic system!
21 Interaction via electromagnetic (light) quanta with environment? Current fluctuations generate photons: Detection via rf circuit or optical detection NanoElectronics, CEA aclay N2, LP Orsay Measure both electron transport and photon emission from quantum circuit (correlation)
22 Theory group (LP Orsay) G. Montambaux I. afi P. imon C. Bena J.N. Fuchs M. Gabay Quantum Transport (LPN Marcoussis) F. Pierre A. Anthore D. Mailly Meso group (LP Orsay) H. Bouchiat R. Deblock M. Ferrier. Guéron A. Kasumov N2 (LP Orsay) J. Gabelli M. Aprili C. Quay Theory (X) A. Georges K. LeHur Quantronics (CEA aclay) D. Estève H. Pothier C. Urbina P. Berthet D. Vion P. Joyez NanoElectronic (CEA aclay) P. Roche C. Glattli F. Portier
The Physics of Nanoelectronics
The Physics of Nanoelectronics Transport and Fluctuation Phenomena at Low Temperatures Tero T. Heikkilä Low Temperature Laboratory, Aalto University, Finland OXFORD UNIVERSITY PRESS Contents List of symbols
More informationINTRODUCTION À LA PHYSIQUE MÉSOSCOPIQUE: ÉLECTRONS ET PHOTONS INTRODUCTION TO MESOSCOPIC PHYSICS: ELECTRONS AND PHOTONS
Chaire de Physique Mésoscopique Michel Devoret Année 2007, Cours des 7 et 14 juin INTRODUCTION À LA PHYSIQUE MÉSOSCOPIQUE: ÉLECTRONS ET PHOTONS INTRODUCTION TO MESOSCOPIC PHYSICS: ELECTRONS AND PHOTONS
More informationSupercondcting Qubits
Supercondcting Qubits Patricia Thrasher University of Washington, Seattle, Washington 98195 Superconducting qubits are electrical circuits based on the Josephson tunnel junctions and have the ability to
More informationStrong back-action of a linear circuit on a single electronic quantum channel F. PIERRE
Strong back-action of a linear circuit on a single electronic quantum channel F. PIERRE F. Parmentier, A. Anthore, S. Jézouin, H. le Sueur, U. Gennser, A. Cavanna, D. Mailly Laboratory for Photonics &
More informationIntroduction to Superconductivity. Superconductivity was discovered in 1911 by Kamerlingh Onnes. Zero electrical resistance
Introduction to Superconductivity Superconductivity was discovered in 1911 by Kamerlingh Onnes. Zero electrical resistance Meissner Effect Magnetic field expelled. Superconducting surface current ensures
More informationINTRODUCTION À LA PHYSIQUE MÉSOSCOPIQUE: ÉLECTRONS ET PHOTONS INTRODUCTION TO MESOSCOPIC PHYSICS: ELECTRONS AND PHOTONS
Chaire de Physique Mésoscopique Michel Devoret Année 2007, Cours des 7 et 14 juin INTRODUCTION À LA PHYSIQUE MÉSOSCOPIQUE: ÉLECTRONS ET PHOTONS INTRODUCTION TO MESOSCOPIC PHYSICS: ELECTRONS AND PHOTONS
More informationQUANTUM- CLASSICAL ANALOGIES
D. Dragoman M. Dragoman QUANTUM- CLASSICAL ANALOGIES With 78 Figures ^Ü Springer 1 Introduction 1 2 Analogies Between Ballistic Electrons and Electromagnetic Waves 9 2.1 Analog Parameters for Ballistic
More informationQuantum Noise Measurement of a Carbon Nanotube Quantum dot in the Kondo Regime
Quantum Noise Measurement of a Carbon Nanotube Quantum dot in the Kondo Regime J. Basset, 1 A.Yu. Kasumov, 1 C.P. Moca, G. Zarand,, 3 P. Simon, 1 H. Bouchiat, 1 and R. Deblock 1 1 Laboratoire de Physique
More informationRéunion erc. Gwendal Fève. Panel PE3 12 mn presentation 12 mn questions
Réunion erc Gwendal Fève Panel PE3 12 mn presentation 12 mn questions Electron quantum optics in quantum Hall edge channels Gwendal Fève Laboratoire Pierre Aigrain, Ecole Normale Supérieure-CNRS Professor
More informationDynamical Casimir effect in superconducting circuits
Dynamical Casimir effect in superconducting circuits Dynamical Casimir effect in a superconducting coplanar waveguide Phys. Rev. Lett. 103, 147003 (2009) Dynamical Casimir effect in superconducting microwave
More informationDistributing Quantum Information with Microwave Resonators in Circuit QED
Distributing Quantum Information with Microwave Resonators in Circuit QED M. Baur, A. Fedorov, L. Steffen (Quantum Computation) J. Fink, A. F. van Loo (Collective Interactions) T. Thiele, S. Hogan (Hybrid
More informationSuperconductivity. S2634: Physique de la matière condensée & nano-objets. Miguel Anía Asenjo Alexandre Le Boité Christine Lingblom
Superconductivity S2634: Physique de la matière condensée & nano-objets Miguel Anía Asenjo Alexandre Le Boité Christine Lingblom 1 What is superconductivity? 2 Superconductivity Superconductivity generally
More informationFrom Last Time. Partially full bands = metal Bands completely full or empty = insulator / seminconductor
From Last Time Solids are large numbers of atoms arranged in a regular crystal structure. Each atom has electron quantum states, but interactions shift the energies. End result is each type atomic electron
More information2015 AMO Summer School. Quantum Optics with Propagating Microwaves in Superconducting Circuits I. Io-Chun, Hoi
2015 AMO Summer School Quantum Optics with Propagating Microwaves in Superconducting Circuits I Io-Chun, Hoi Outline 1. Introduction to quantum electrical circuits 2. Introduction to superconducting artificial
More informationSemiclassical formulation
The story so far: Transport coefficients relate current densities and electric fields (currents and voltages). Can define differential transport coefficients + mobility. Drude picture: treat electrons
More informationDetecting noise with shot noise: a new on-chip photon detector
Detecting noise with shot noise: a new on-chip photon detector Y. Jompol 1,,, P. Roulleau 1,, T. Jullien 1, B. Roche 1, I. Farrer 2, D.A. Ritchie 2, and D. C. Glattli 1 1 Nanoelectronics Group, Service
More informationQuantum Noise of a Carbon Nanotube Quantum Dot in the Kondo Regime
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 Solides Orsay (France) Theory : P. Simon (LPS),
More informationSuperconducting Qubits. Nathan Kurz PHYS January 2007
Superconducting Qubits Nathan Kurz PHYS 576 19 January 2007 Outline How do we get macroscopic quantum behavior out of a many-electron system? The basic building block the Josephson junction, how do we
More informationWhat is Quantum Transport?
What is Quantum Transport? Branislav K. Nikolić Department of Physics and Astronomy, University of Delaware, U.S.A. http://www.physics.udel.edu/~bnikolic Semiclassical Transport (is boring!) Bloch-Boltzmann
More informationSuperconducting qubits (Phase qubit) Quantum informatics (FKA 172)
Superconducting qubits (Phase qubit) Quantum informatics (FKA 172) Thilo Bauch (bauch@chalmers.se) Quantum Device Physics Laboratory, MC2, Chalmers University of Technology Qubit proposals for implementing
More informationM.C. Escher. Angels and devils (detail), 1941
M.C. Escher Angels and devils (detail), 1941 1 Coherent Quantum Phase Slip: Exact quantum dual to Josephson Tunneling (Coulomb blockade is a partial dual) Degree of freedom in superconductor: Phase and
More informationCircuit Quantum Electrodynamics. Mark David Jenkins Martes cúantico, February 25th, 2014
Circuit Quantum Electrodynamics Mark David Jenkins Martes cúantico, February 25th, 2014 Introduction Theory details Strong coupling experiment Cavity quantum electrodynamics for superconducting electrical
More informationDemonstration of conditional gate operation using superconducting charge qubits
Demonstration of conditional gate operation using superconducting charge qubits T. Yamamoto, Yu. A. Pashkin, * O. Astafiev, Y. Nakamura, & J. S. Tsai NEC Fundamental Research Laboratories, Tsukuba, Ibaraki
More informationCONDUCTIVITY AND INDUCED SUPERCONDUCTIVITY IN DNA
CONDUCTIVITY AND INDUCED SUPERCONDUCTIVITY IN DNA A.Yu. Kasumov 1,2, K.Tsukagoshi 1,3, M. Kawamura 1, T. Kobayashi 1, Y.Aoyagi 1,4, V.T. Volkov 2, Yu.A. Kasumov 2, D.V. Klinov 5, M. Kociak 6, P.-E. Roche
More informationSuperconductivity at nanoscale
Superconductivity at nanoscale Superconductivity is the result of the formation of a quantum condensate of paired electrons (Cooper pairs). In small particles, the allowed energy levels are quantized and
More informationSuperconductivity and the BCS theory
Superconductivity and the BCS theory PHY 313 - Statistical Mechanics Syed Ali Raza Roll no: 2012-10-0124 LUMS School of Science and Engineering Monday, December, 15, 2010 1 Introduction In this report
More informationSingle Electron Transistor (SET)
Single Electron Transistor (SET) e - e - dot C g V g A single electron transistor is similar to a normal transistor (below), except 1) the channel is replaced by a small dot. 2) the dot is separated from
More informationModern Physics for Scientists and Engineers International Edition, 4th Edition
Modern Physics for Scientists and Engineers International Edition, 4th Edition http://optics.hanyang.ac.kr/~shsong 1. THE BIRTH OF MODERN PHYSICS 2. SPECIAL THEORY OF RELATIVITY 3. THE EXPERIMENTAL BASIS
More informationPrinciples and Applications of Superconducting Quantum Interference Devices (SQUIDs)
Principles and Applications of Superconducting Quantum Interference Devices (SQUIDs) PHY 300 - Junior Phyics Laboratory Syed Ali Raza Roll no: 2012-10-0124 LUMS School of Science and Engineering Thursday,
More informationEnergy Levels Zero energy. From Last Time Molecules. Today. n- and p-type semiconductors. Energy Levels in a Metal. Junctions
Today From Last Time Molecules Symmetric and anti-symmetric wave functions Lightly higher and lower energy levels More atoms more energy levels Conductors, insulators and semiconductors Conductors and
More informationLECTURE 2: Thermometry
LECTURE 2: Thermometry Tunnel barrier Examples of aluminium-oxide tunnel barriers Basics of tunnel junctions E 1 2 Tunneling from occupied states to empty states V Metal Insulator Metal (NIN) tunnel junction
More informationQuantum Optics. Manipulation of «simple» quantum systems
Quantum Optics Manipulation of «simple» quantum systems Antoine Browaeys Institut d Optique, Palaiseau, France Quantum optics = interaction atom + quantum field e g ~ 1960: R. Glauber (P. Nobel. 2005),
More informationChapter 5 Nanomanipulation. Chapter 5 Nanomanipulation. 5.1: With a nanotube. Cutting a nanotube. Moving a nanotube
Objective: learn about nano-manipulation techniques with a STM or an AFM. 5.1: With a nanotube Moving a nanotube Cutting a nanotube Images at large distance At small distance : push the NT Voltage pulse
More informationSuperconductors: Quantum circuits
Superconductors: Quantum circuits J. J. García-Ripoll IFF, CSIC Madrid (20-4-2009) Mesoscopic QIPC Small systems So far we have only seen small systems to store and process QI Individual atoms As trapped
More informationQuantum Optics with Propagating Microwaves in Superconducting Circuits. Io-Chun Hoi 許耀銓
Quantum Optics with Propagating Microwaves in Superconducting Circuits 許耀銓 Outline Motivation: Quantum network Introduction to superconducting circuits Quantum nodes The single-photon router The cross-kerr
More informationSCIENTIFIC PRODUCTION
SCIENTIFIC PRODUCTION 0. SUMMARY - Highlights: 2 Nature, 2 Science, 3 Nature physics, 2 Nature Communications as principal investigator (PI) ; 13 PRL as PI or among first authors ; 1 monograph ; 2 articles
More informationQuantum physics in quantum dots
Quantum physics in quantum dots Klaus Ensslin Solid State Physics Zürich AFM nanolithography Multi-terminal tunneling Rings and dots Time-resolved charge detection Moore s Law Transistors per chip 10 9
More informationTDGL Simulation on Dynamics of Helical Vortices in Thin Superconducting Wires in the Force-Free Configuration
5th International Workshop on Numerical Modelling of High-Temperature Superconductors, 6/15-17/2016, Bologna, Italy TDGL Simulation on Dynamics of Helical Vortices in Thin Superconducting Wires in the
More informationLecture 2, March 1, 2018
Lecture 2, March 1, 2018 Last week: Introduction to topics of lecture Algorithms Physical Systems The development of Quantum Information Science Quantum physics perspective Computer science perspective
More informationSuperinsulator: a new topological state of matter
Superinsulator: a new topological state of matter M. Cristina Diamantini Nips laboratory, INFN and Department of Physics and Geology University of Perugia Coll: Igor Lukyanchuk, University of Picardie
More informationHybrid Quantum Circuit with a Superconducting Qubit coupled to a Spin Ensemble
Hybrid Quantum Circuit with a Superconducting Qubit coupled to a Spin Ensemble, Cécile GREZES, Andreas DEWES, Denis VION, Daniel ESTEVE, & Patrice BERTET Quantronics Group, SPEC, CEA- Saclay Collaborating
More informationQuantum Theory of Matter
Quantum Theory of Matter Overview Lecture Derek Lee Imperial College London January 2007 Outline 1 Course content Introduction Superfluids Superconductors 2 Course Plan Resources Outline 1 Course content
More informationShort Course in Quantum Information Lecture 8 Physical Implementations
Short Course in Quantum Information Lecture 8 Physical Implementations Course Info All materials downloadable @ website http://info.phys.unm.edu/~deutschgroup/deutschclasses.html Syllabus Lecture : Intro
More information400 nm Solid State Qubits (1) Daniel Esteve GROUP. SPEC, CEA-Saclay
400 nm Solid State Qubits (1) S D Daniel Esteve QUAN UM ELECT RONICS GROUP SPEC, CEA-Saclay From the Copenhagen school (1937) Max Planck front row, L to R : Bohr, Heisenberg, Pauli,Stern, Meitner, Ladenburg,
More informationCircuit QED: A promising advance towards quantum computing
Circuit QED: A promising advance towards quantum computing Himadri Barman Jawaharlal Nehru Centre for Advanced Scientific Research Bangalore, India. QCMJC Talk, July 10, 2012 Outline Basics of quantum
More informationCharging and Kondo Effects in an Antidot in the Quantum Hall Regime
Semiconductor Physics Group Cavendish Laboratory University of Cambridge Charging and Kondo Effects in an Antidot in the Quantum Hall Regime M. Kataoka C. J. B. Ford M. Y. Simmons D. A. Ritchie University
More informationLecture 26: Nanosystems Superconducting, Magnetic,. What is nano? Size
Lecture 26: Nanosystems Superconducting, Magnetic,. What is nano? Size Quantum Mechanics Structure Properties Recall discussion in Lecture 21 Add new ideas Physics 460 F 2006 Lect 26 1 Outline Electron
More information10 Supercondcutor Experimental phenomena zero resistivity Meissner effect. Phys463.nb 101
Phys463.nb 101 10 Supercondcutor 10.1. Experimental phenomena 10.1.1. zero resistivity The resistivity of some metals drops down to zero when the temperature is reduced below some critical value T C. Such
More informationScanning Gate Microscopy (SGM) of semiconductor nanostructures
Scanning Gate Microscopy (SGM) of semiconductor nanostructures H. Sellier, P. Liu, B. Sacépé, S. Huant Dépt NANO, Institut NEEL, Grenoble, France B. Hackens, F. Martins, V. Bayot UCL, Louvain-la-Neuve,
More informationMartes Cuánticos. Quantum Capacitors. (Quantum RC-circuits) Victor A. Gopar
Martes Cuánticos Quantum Capacitors (Quantum RC-circuits) Victor A. Gopar -Universal resistances of the quantum resistance-capacitance circuit. Nature Physics, 6, 697, 2010. C. Mora y K. Le Hur -Violation
More informationDissipation in Transmon
Dissipation in Transmon Muqing Xu, Exchange in, ETH, Tsinghua University Muqing Xu 8 April 2016 1 Highlight The large E J /E C ratio and the low energy dispersion contribute to Transmon s most significant
More information6.763 Applied Superconductivity Lecture 1
6.763 Applied Superconductivity Lecture 1 Terry P. Orlando Dept. of Electrical Engineering MIT September 4, 2003 Outline What is a Superconductor? Discovery of Superconductivity Meissner Effect Type I
More informationQUANTUM TECHNOLOGIES: THE SECOND QUANTUM REVOLUTION* Jonathan P. Dowling
QUANTUM TECHNOLOGIES: THE SECOND QUANTUM REVOLUTION* Jonathan P. Dowling Quantum Science & Technologies Group Hearne Institute for Theoretical Physics Louisiana State University http://quantum.phys.lsu.edu
More informationLecture 3. Shot noise correlations: The two-particle Aharonv-Bohm effect. Markus Buttiker University of Geneva
Lecture 3 Shot noise correlations: The two-particle haronv-bohm effect 1 6 1 C 3 B 8 5 4 D 3 4 7 Markus Buttiker University of Geneva IV-th Windsor Summer School on Condensed Matter Theory, organized by
More information1 P a g e h t t p s : / / w w w. c i e n o t e s. c o m / Physics (A-level)
1 P a g e h t t p s : / / w w w. c i e n o t e s. c o m / Physics (A-level) Electromagnetic induction (Chapter 23): For a straight wire, the induced current or e.m.f. depends on: The magnitude of the magnetic
More informationHall Effect Gyrators and Circulators David DiVincenzo Quantum Technology - Chalmers
Hall Effect Gyrators and Circulators David DiVincenzo 14.12.2016 Quantum Technology - Chalmers G. Viola and D. P. DiVincenzo, Hall Effect Gyrators and Circulators, Phys. Rev. X 4, 021019 (2014). S. Bosco,
More informationMesoscopic quantum measurements
Mesoscopic quantum measurements D.V. Averin Department of Physics and Astronomy SUNY Stony Brook A. Di Lorentzo K. Rabenstein V.K. Semenov D. Shepelyanskii E.V. Sukhorukov Summary α β Example of the trivial
More informationQuantum dots and Majorana Fermions Karsten Flensberg
Quantum dots and Majorana Fermions Karsten Flensberg Center for Quantum Devices University of Copenhagen Collaborator: Martin Leijnse and R. Egger M. Kjærgaard K. Wölms Outline: - Introduction to Majorana
More informationSuperconductivity. The Discovery of Superconductivity. Basic Properties
Superconductivity Basic Properties The Discovery of Superconductivity Using liquid helium, (b.p. 4.2 K), H. Kamerlingh Onnes found that the resistivity of mercury suddenly dropped to zero at 4.2 K. H.
More informationDemonstration Some simple theoretical models Materials How to make superconductors Some applications
Superconductivity Demonstration Some simple theoretical models Materials How to make superconductors Some applications How do we show superconductivity? Superconductors 1. have an electrical resistivity
More informationElectronic Quantum Transport in Mesoscopic Semiconductor Structures
Thomas Ihn Electronic Quantum Transport in Mesoscopic Semiconductor Structures With 90 Illustrations, S in Full Color Springer Contents Part I Introduction to Electron Transport l Electrical conductance
More informationQuantum Physics & From Ideas to Implementation. Underlying concepts in the syllabus
Quantum Physics & From Ideas to Implementation Underlying concepts in the syllabus 1 1 What is Quantum Physics? Wave-particle duality Tells us that energy comes in packets, particles are wave-like. Systems
More informationQuantum Photonic Integrated Circuits
Quantum Photonic Integrated Circuits IHFG Hauptseminar: Nanooptik und Nanophotonik Supervisor: Prof. Dr. Peter Michler 14.07.2016 Motivation and Contents 1 Quantum Computer Basics and Materials Photon
More informationExciting Andreev pairs in a superconducting atomic. contact
Exciting Andreev pairs in a superconducting atomic contact L. Bretheau, 1* Ç. Ö. Girit, 1* H. Pothier, 1 D. Esteve 1 and C. Urbina 1 1 Quantronics Group, Service de Physique de l État Condensé (CNRS, URA
More informationLet's Build a Quantum Computer!
Let's Build a Quantum Computer! 31C3 29/12/2014 Andreas Dewes Acknowledgements go to "Quantronics Group", CEA Saclay. R. Lauro, Y. Kubo, F. Ong, A. Palacios-Laloy, V. Schmitt PhD Advisors: Denis Vion,
More informationSolid Surfaces, Interfaces and Thin Films
Hans Lüth Solid Surfaces, Interfaces and Thin Films Fifth Edition With 427 Figures.2e Springer Contents 1 Surface and Interface Physics: Its Definition and Importance... 1 Panel I: Ultrahigh Vacuum (UHV)
More informationSuperconducting Resonators and Their Applications in Quantum Engineering
Superconducting Resonators and Their Applications in Quantum Engineering Nov. 2009 Lin Tian University of California, Merced & KITP Collaborators: Kurt Jacobs (U Mass, Boston) Raymond Simmonds (Boulder)
More informationQuantum transport in nanoscale solids
Quantum transport in nanoscale solids The Landauer approach Dietmar Weinmann Institut de Physique et Chimie des Matériaux de Strasbourg Strasbourg, ESC 2012 p. 1 Quantum effects in electron transport R.
More informationVienna Doctoral School in Physics
Vienna Doctoral School in Physics You? Hearings in Vienna: 22& 23 February 2018 Aerosol Physics Prof. Bernadett Weinzierl Atmospheric and Aerosol Physics Position 1 Airborne measurements of the complex
More informationSuperconductivity. Introduction. Final project. Statistical Mechanics Fall Mehr Un Nisa Shahid
1 Final project Statistical Mechanics Fall 2010 Mehr Un Nisa Shahid 12100120 Superconductivity Introduction Superconductivity refers to the phenomenon of near-zero electric resistance exhibited by conductors
More informationProximity dc squids in the long-junction limit
Proximity dc squids in the long-junction limit L. Angers, F. Chiodi, G. Montambaux, M. Ferrier, S. Guéron, and H. Bouchiat Laboratoire de Physique des Solides, Université Paris-Sud, CNRS, UMR 852, F-945
More informationPHYS 3313 Section 001 Lecture #21 Monday, Nov. 26, 2012
PHYS 3313 Section 001 Lecture #21 Monday, Nov. 26, 2012 Superconductivity Theory, The Cooper Pair Application of Superconductivity Semi-Conductor Nano-technology Graphene 1 Announcements Your presentations
More informationElectronic and Optoelectronic Properties of Semiconductor Structures
Electronic and Optoelectronic Properties of Semiconductor Structures Jasprit Singh University of Michigan, Ann Arbor CAMBRIDGE UNIVERSITY PRESS CONTENTS PREFACE INTRODUCTION xiii xiv 1.1 SURVEY OF ADVANCES
More informationScanning gate microscopy and individual control of edge-state transmission through a quantum point contact
Scanning gate microscopy and individual control of edge-state transmission through a quantum point contact Stefan Heun NEST, CNR-INFM and Scuola Normale Superiore, Pisa, Italy Coworkers NEST, Pisa, Italy:
More informationUnconventional electron quantum optics in condensed matter systems
Unconventional electron quantum optics in condensed matter systems Dario Ferraro Centre de Physique Théorique, Marseille nanoqt-2016, Kyiv, October 10, 2016 In collaboration with: J. Rech, T. Jonckheere,
More informationEntanglement Control of Superconducting Qubit Single Photon System
: Quantum omputing Entanglement ontrol of Superconducting Qubit Single Photon System Kouichi Semba Abstract If we could achieve full control of the entangled states of a quantum bit (qubit) interacting
More informationQuantum computation with superconducting qubits
Quantum computation with superconducting qubits Project for course: Quantum Information Ognjen Malkoc June 10, 2013 1 Introduction 2 Josephson junction 3 Superconducting qubits 4 Circuit and Cavity QED
More informationNews from NBIA. Condensed Matter Physics: from new materials to quantum technology. time. Mark Rudner
News from NBIA Condensed Matter Physics: from new materials to quantum technology Mark Rudner time ~100 years after Bohr, the basic laws and players are established 1913 2013 Image from www.periodni.com
More informationUnit V Superconductivity Engineering Physics
1. Superconductivity ertain metals and alloys exhibit almost zero resistivity (i.e. infinite conductivity), when they are cooled to sufficiently low temperatures. This effect is called superconductivity.
More informationElectrical quantum engineering with superconducting circuits
1.0 10 0.8 01 switching probability 0.6 0.4 0.2 00 P. Bertet & R. Heeres SPEC, CEA Saclay (France), Quantronics group 11 0.0 0 100 200 300 400 swap duration (ns) Electrical quantum engineering with superconducting
More informationPhysics of Low-Dimensional Semiconductor Structures
Physics of Low-Dimensional Semiconductor Structures Edited by Paul Butcher University of Warwick Coventry, England Norman H. March University of Oxford Oxford, England and Mario P. Tosi Scuola Normale
More informationRecent experimental studies of electron dephasing in metal and semiconductor mesoscopic structures
INSTITUTE OF PHYSICS PUBLISHING JOURNAL OF PHYSICS: CONDENSED MATTER J. Phys.: Condens. Matter 14 (2002) R501 R596 PII: S0953-8984(02)16903-7 TOPICAL REVIEW Recent experimental studies of electron dephasing
More informationMesoscopic Nano-Electro-Mechanics of Shuttle Systems
* Mesoscopic Nano-Electro-Mechanics of Shuttle Systems Robert Shekhter University of Gothenburg, Sweden Lecture1: Mechanically assisted single-electronics Lecture2: Quantum coherent nano-electro-mechanics
More informationSuperconducting quantum bits. Péter Makk
Superconducting quantum bits Péter Makk Qubits Qubit = quantum mechanical two level system DiVincenzo criteria for quantum computation: 1. Register of 2-level systems (qubits), n = 2 N states: eg. 101..01>
More informationSingle Electron Transistor (SET)
Single Electron Transistor (SET) SET: e - e - dot A single electron transistor is similar to a normal transistor (below), except 1) the channel is replaced by a small dot. C g 2) the dot is separated from
More informationIs Quantum Mechanics the Whole Truth?* A.J. Leggett. University of Illinois at Urbana-Champaign
Is Quantum Mechanics the Whole Truth?* A6S1 A.J. Leggett University of Illinois at Urbana-Champaign 1. Why bother? 2. What are we looking for? 3. What have we seen so far? 4. Where do we go from here?
More informationwe can said that matter can be regarded as composed of three kinds of elementary particles; proton, neutron (no charge), and electron.
Physics II we can said that matter can be regarded as composed of three kinds of elementary particles; proton, neutron (no charge), and electron. Particle Symbol Charge (e) Mass (kg) Proton P +1 1.67
More informationRabi oscillations, Ramsey fringes and spin echoes in an electrical circuit
Fortschr. Phys. 51, No. 4 5, 462 468 (2003) / DOI 10.1002/prop.200310063 Rabi oscillations, Ramsey fringes and spin echoes in an electrical circuit D. Vion 1, A. Aassime 1, A. Cottet 1,P.Joyez 1, H. Pothier
More informationSolid State Device Fundamentals
Solid State Device Fundamentals ENS 345 Lecture Course by Alexander M. Zaitsev alexander.zaitsev@csi.cuny.edu Tel: 718 982 2812 Office 4N101b 1 Outline - Goals of the course. What is electronic device?
More informationJosephson currents in two dimensional mesoscopic ballistic conductors Heida, Jan Peter
University of Groningen Josephson currents in two dimensional mesoscopic ballistic conductors Heida, Jan Peter IMPORTANT NOTE: You are advised to consult the publisher's version (publisher's PDF) if you
More information2426 Required Topics (May 4, 2012 draft) Halliday, FUNDAMENTALS OF PHYSICS, 9e Required topics are in bold text. Optional topics are in normal text.
2426 Required Topics (May 4, 2012 draft) Halliday, FUNDAMENTALS OF PHYSICS, 9e Required topics are in bold text. Optional topics are in normal text. Chapter 21 Electric Charge 21-1 What Is Physics? 21-2
More informationFrom Last Time Important new Quantum Mechanical Concepts. Atoms and Molecules. Today. Symmetry. Simple molecules.
Today From Last Time Important new Quantum Mechanical Concepts Indistinguishability: Symmetries of the wavefunction: Symmetric and Antisymmetric Pauli exclusion principle: only one fermion per state Spin
More informationCorrelated 2D Electron Aspects of the Quantum Hall Effect
Correlated 2D Electron Aspects of the Quantum Hall Effect Magnetic field spectrum of the correlated 2D electron system: Electron interactions lead to a range of manifestations 10? = 4? = 2 Resistance (arb.
More informationQuantum phase slip junctions
Quantum phase slip junctions J.E. Mooij* and Yu.V. Nazarov Kavli Institute of Nanoscience Delft University of Technology 68 CJ Delft, The Netherlands *e-mail: j.e.mooij@tnw.tudelft.nl abstract For a superconductor,
More informationCoherent Coupling between 4300 Superconducting Flux Qubits and a Microwave Resonator
: A New Era in Quantum Information Processing Technologies Coherent Coupling between 4300 Superconducting Flux Qubits and a Microwave Resonator Yuichiro Matsuzaki, Kosuke Kakuyanagi, Hiraku Toida, Hiroshi
More informationINTRODUCTION TO SUPERCONDUCTING QUBITS AND QUANTUM EXPERIENCE: A 5-QUBIT QUANTUM PROCESSOR IN THE CLOUD
INTRODUCTION TO SUPERCONDUCTING QUBITS AND QUANTUM EXPERIENCE: A 5-QUBIT QUANTUM PROCESSOR IN THE CLOUD Hanhee Paik IBM Quantum Computing Group IBM T. J. Watson Research Center, Yorktown Heights, NY USA
More informationExploring the quantum dynamics of atoms and photons in cavities. Serge Haroche, ENS and Collège de France, Paris
Exploring the quantum dynamics of atoms and photons in cavities Serge Haroche, ENS and Collège de France, Paris Experiments in which single atoms and photons are manipulated in high Q cavities are modern
More informationElectron counting with quantum dots
Electron counting with quantum dots Klaus Ensslin Solid State Physics Zürich with S. Gustavsson I. Shorubalko R. Leturcq T. Ihn A. C. Gossard Time-resolved charge detection Single photon detection Time-resolved
More informationBEC meets Cavity QED
BEC meets Cavity QED Tilman Esslinger ETH ZürichZ Funding: ETH, EU (OLAQUI, Scala), QSIT, SNF www.quantumoptics.ethz.ch Superconductivity BCS-Theory Model Experiment Fermi-Hubbard = J cˆ ˆ U nˆ ˆ i, σ
More informationCIRCUIT QUANTUM ELECTRODYNAMICS WITH ELECTRONS ON HELIUM
CIRCUIT QUANTUM ELECTRODYNAMICS WITH ELECTRONS ON HELIUM David Schuster Assistant Professor University of Chicago Chicago Ge Yang Bing Li Michael Geracie Yale Andreas Fragner Rob Schoelkopf Useful cryogenics
More information