DIRECT OBSERVATION OF JOSEPHSON VORTICES

Slides:



Advertisements
Similar presentations
Superconductors. Gor’kov and Eliashberg found the time- dependent G-L equations using microscopic theory: These equations are solved numerically Model.
Advertisements

Josepson Current in Four-Terminal Superconductor/Exciton- Condensate/Superconductor System S. Peotta, M. Gibertini, F. Dolcini, F. Taddei, M. Polini, L.
Probing Superconductors using Point Contact Andreev Reflection Pratap Raychaudhuri Tata Institute of Fundamental Research Mumbai Collaborators: Gap anisotropy.
STM/S Imaging Studies in the Vortex State Anjan K. Gupta Physics Department, IIT, Kanpur (Tutorial, IVW10 at TIFR)
Superconducting Quantum Interference Device SQUID C. P. Sun Department of Physics National Sun Yat Sen University.
Electrical Techniques MSN506 notes. Electrical characterization Electronic properties of materials are closely related to the structure of the material.
High-T c Superconductor Surface State 15/20/2015 Group member: 陈玉琴、郭亚光、贾晓萌、刘俊义、刘晓雪 彭星星、王建力、王鹏捷 ★ 、喻佳兵 ★ :Group Leader & Speaker.
1 SQUID and Josephson Devices By : Yatin Singhal.
1 Ferromagnetic Josephson Junction and Spin Wave Resonance Nagoya University on September 5,2009 Sadamichi Maekawa (IMR, Tohoku University) Co-workers:
Electron Tunneling and the Josephson Effect. Electron Tunneling through an Insulator.
“… at each new level of complexity, entirely new properties appear, and the understanding of this behavior requires research which I think is as fundamental.
Heat conduction by photons through superconducting leads W.Guichard Université Joseph Fourier and Institut Neel, Grenoble, France M. Meschke, and J.P.
Insights into quantum matter from new experiments Detecting new many body states will require: Atomic scale resolution of magnetic fields Measuring and.
ECRYS 2011 Confinement-Induced Vortex Phases in Superconductors Institut des Nanosciences de Paris INSP, CNRS, Université Pierre et Marie Curie Paris 6,
Phase Diagram of a Point Disordered Model Type-II Superconductor Peter Olsson Stephen Teitel Umeå University University of Rochester IVW-10 Mumbai, India.
SQUID Based Quantum Bits James McNulty. What’s a SQUID? Superconducting Quantum Interference Device.
Submicron structures 26 th January 2004 msc Condensed Matter Physics Photolithography to ~1 μm Used for... Spin injection Flux line dynamics Josephson.
VORTEX MATTER IN SUPERCONDUCTORS WITH FERROMAGNETIC DOT ARRAYS Margriet J. Van Bael Martin Lange, Victor V. Moshchalkov Laboratorium voor Vaste-Stoffysica.
Superconductors: Basic Concepts Daniel Shantsev AMCS group Department of Physics University of Oslo History Superconducting materials Properties Understanding.
Superconducting Qubits Kyle Garton Physics C191 Fall 2009.
J. R. Kirtley et al., Phys. Rev. Lett. 76 (1996),
1 PHY 712 Electrodynamics 9-9:50 AM MWF Olin 103 Plan for Lecture 34: Special Topics in Electrodynamics: Electromagnetic aspects of superconductivity 
I. Grigorieva, L. Vinnikov, A. Geim (Manchester) V. Oboznov, S. Dubonos (Chernogolovka)
SQUIDs (Superconducting QUantum Interference Devices)
Type I and Type II superconductivity
Complex Epitaxial Oxides: Synthesis and Scanning Probe Microscopy Goutam Sheet, 1 Udai Raj Singh, 2 Anjan K. Gupta, 2 Ho Won Jang, 3 Chang-Beom Eom 3 and.
Lecture 3. Granular superconductors and Josephson Junction arrays Plan of the Lecture 1). Superconductivity in a single grain 2) Granular superconductors:
Superconducting vortex avalanches D. Shantsev Åge A. F. Olsen, D. Denisov, V. Yurchenko, Y. M. Galperin, T. H. Johansen AMCS (COMPLEX) group Department.
Supercurrent through carbon-nanotube-based quantum dots Tomáš Novotný Department of Condensed Matter Physics, MFF UK In collaboration with: K. Flensberg,
Electron-Phonon Interaction and Disorder: Nanoscale Interference in Transport Phenomena Andrei Sergeyev, SUNY at Buffalo, DMR Thermomagnetic vortex.
Michael Browne 11/26/2007.
Electrical Transport in Thin Film Nanostructures Hanno H. Weitering, The University of Tennessee, DMR Competing periodicities in a single atom.
Dendritic Thermo-magnetic Instability in Superconductors Daniel V. Shantsev AMCS group, Department of Physics, UiO Collaboration: D. V. Denisov, A.A.F.Olsen,
Practice of students from ARAB REPUBLIC OF EGYPT 2009
Spin Readout with Superconducting Circuits April 27 th, 2011 N. Antler R. Vijay, E. Levenson-Falk, I. Siddiqi.
DC-squid for measurements on a Josephson persistent-current qubit Applied Physics Quantum Transport Group Alexander ter Haar May 2000 Supervisors: Ir.
RF breakdown in multilayer coatings: a possibility to break the Nb monopoly Alex Gurevich National High Magnetic Field Laboratory, Florida State University.
Nanoscience and Engineering in Superconductivity (NES - ESF) Mid-term evaluation report presented to the 32nd PESC Plenary Meeting of the ESF Victor V.
Tunneling Spectroscopy and Vortex Imaging in Boron-doped Diamond
I NTERLAYER E XCHANGE C OUPLING, P AIR B REAKING & 2D V ORTEX D YNAMICS IN F ERROMAGNET - S UPERCONDUCTOR H ETEROSTRUCTURES R. C. B UDHANI Indian Institute.
R OLE OF D ISORDER IN S UPERCONDUCTING T RANSITION Sudhansu S. Mandal IACS, Kolkata HRI 1.
Sid Nb device fabrication Superconducting Nb thin film evaporation Evaporate pure Nb to GaAs wafer and test its superconductivity (T c ~9.25k ) Tc~2.5K.
Vortex Solution in Holographic Two-Band Superconductor
Nikolai Kopnin Theory Group Dynamics of Superfluid 3 He and Superconductors.
Electrical Transport in Thin Film Nanostructures Hanno H. Weitering, The University of Tennessee, DMR Understanding and control of electrical conductivity.
K.M.Shahabasyan, M. K. Shahabasyan,D.M.Sedrakyan
1 PHY 712 Electrodynamics 10-10:50 AM MWF Olin 107 Plan for Lecture 33: Special Topics in Electrodynamics: 1.Electromagnetic aspects of superconductivity.
1 Non-uniform superconductivity in superconductor/ferromagnet nanostructures A. Buzdin Institut Universitaire de France, Paris and Condensed Matter Theory.
Why Make Holes in Superconductors? Saturday Morning Physics December 6, 2003 Dr. Sa-Lin Cheng Bernstein.
Superconductivity and Superfluidity The Pippard coherence length In 1953 Sir Brian Pippard considered 1. N/S boundaries have positive surface energy 2.
Pinning Effect on Niobium Superconducting Thin Films with Artificial Pinning Centers. Lance Horng, J. C. Wu, B. H. Lin, P. C. Kang, J. C. Wang, and C.
K. Gireesan1, T. S. Radhakrishnan1, Joseph Bensigh3, S
Subharmonic gap Structures
Superconductivity: approaching the century jubilee A.A.Varlamov Institute of Superconductivity and Innovative Materials SPIN-CNR, Italy.
Superconductivity, Josephson Junctions, and squids
Superconducting materials have an electrical resistance of zero, and so can carry large electrical currents without power dissipation or heat generation.
WHAT IS SUPERCONDUCTIVITY?? For some materials, the resistivity vanishes at some low temperature: they become superconducting. Superconductivity is the.
Super Conductivity Josephsen Junctions And SQUIDS
Unbound States A review on calculations for the potential step.
Superconducting Qubits
BCS THEORY BCS theory is the first microscopic theory of superconductivity since its discovery in It explains, The interaction of phonons and electrons.
STM Conference Talk: Dirk Sander
Topological Phase transitions and Topological phases of matter
Experimental Evidences on Spin-Charge Separation
High Temperature Superconductivity
Special Topics in Electrodynamics:
The Metal-Insulator Transition
Arian Lalezari 22 September 2004 Modeling in Applied Math
Presentation transcript:

DIRECT OBSERVATION OF JOSEPHSON VORTICES Young Scientist Contest 2016 of the Belgian Physical Society DIRECT OBSERVATION OF JOSEPHSON VORTICES presented by Lise SERRIER-GARCIA Lise SERRIER-GARCIA, Tristan CREN, Dimitri RODITCHEV, François DEBONTRIDDER, Christophe BRUN, Juan Carlos CUEVAS, Vagner H. L. BESSA, Milorad MILOŠEVIĆ Institute for Nanoscale Physics and Chemistry, Leuven, Belgium Institut des Nanosciences de Paris, CNRS-UPMC, Paris, France, Departamento de Física Teórica de la Materia Condensada, Universidad Autónoma de Madrid, SPAIN Departement Fysica, Universiteit Antwerpen, BELGIUM

The supercurrent is zero at each step of quantum flux. JOSEPHSON EFFECT 𝐼 𝑚𝑎𝑥 𝐼 𝑐 superconductor tunneling barrier Superconducting Quantum Interference Device (SQUID) A very sensitive sensor of extremely subtle magnetic fields magnetic field 𝐼 𝑚𝑎𝑥 𝐼 𝑐 = sin Δ𝜑 =sin⁡( 𝜙 𝜙 0 ) magnetic flux: 𝜙= 𝐵 𝑆 quantum flux: 𝜙 0 = ℎ 2𝑒 The supercurrent is zero at each step of quantum flux. 2

SUPERCONDUCTING ELECTRODES Si Pb 𝑏𝑎𝑖𝑠 𝑣𝑜𝑙𝑡𝑎𝑔𝑒 𝑐𝑢𝑟𝑟𝑒𝑛𝑡 STM Non-superconducting metal Superconductor Insulator 𝐶∝ 𝜌 𝑛 𝑒𝑉 ℜ𝑒 𝑒𝑉 𝑒𝑉 2 − ∆ 2 at T = 0 normalized conductance 𝑇=0.3 𝐾 𝑇 𝑐 =7 𝐾 Bias voltage (mV) Using scanning tunneling spectroscopy, we directly access to the local electronic density of states. 3

NANOSTRUCTURES CONTROLLED BY PREPARATION CONDITIONS 1 x 1 µm² 2 x 2 µm² 1 x 1 µm² J. Phys. Chem C 119 12651 (2015) The lead on silicon growth follows a self-organisation. Temperature, pressure, quality and amount of lead determine the nanostructures. 4

BUILDING A JOSEPHSON JUNCTION 𝜉 𝑛 ≈15 𝑛𝑚 nanostructure What? 4 𝜉 𝑛 ≈15 𝑛𝑚 thickness (nm) topography conductance nanostructure Phys Rev Lett 110 157003 (2013) Bias voltage (mV) Superconductivity is not limited to the nanostructures. 5

JOSEPHSON JUNCTION The distance is reduced to few tens of nanometer superconductor d≈45 𝑛𝑚 Josephson junction 1 conductance conductance conductance map superconductor Bias voltage (mV) The distance is reduced to few tens of nanometer creating a Josephson junction. 6

JOSEPHSON JUNCTIONS WITH MAGNETIC FIELD non-supercodnucting metal superconductors magnetic field 1 x 1 µm² 5 thickness (nm) topography Array of Josephson junctions. 7

ABRIKOSOV AND JOSEPSHON VORTICES Nat Phys 11 332-337 (2015) 1 x 1 µm2 magnetic field 0 mT 180 mT 60 mT 120 mT 1 conductance 8

THE GINZBURG-LANDAU EQUATIONS Minimizing the free energy of the Ginzburg-Landau theory… 𝑓 𝑟 =𝑎 𝛹(𝑟) 2 + 𝑏 2 𝛹(𝑟) 4 + 1 2 𝑚 ∗ ℏ 𝑖 𝛻−2𝑒 𝐴 𝑟 𝛹 𝑟 + µ 0 2 𝐵 𝑟 2 Condensation Kinetic Magnetic Phys Rev E 86 056709 (2012) Nat Phys 11 332-337 (2015) Phys Rev B 65 104515 (2002) 𝐻 Current 𝑗 𝑟 Phase 𝜑 𝑟 Amplitude |Ψ 𝑟 | … to simulate the Abrikosov vortices. 9

SIMULATING THE SUPERCONDUCTORS… Abrikosov vortex Josephson junction 500 x 500 nm2 H = 120 mT Nat Phys 11 332-337 (2015) 1 2π amplitude |ψ| phase ϕ Ginzburg-Landau equations describe the superconductivity in the nanostructures but not in the Josephson junctions. 10

… SIMULATING THE JOSEPHSON EFFECT… Phase ϕ Interference pattern J Superconductor 1 Josephson junction Superconductor ∆𝜑 𝑖𝑛𝑣 =𝜑 𝑟 𝑎 −𝜑 𝑟 𝑏 − 2𝑒 ħ 𝑟 𝑏 𝑟 𝑎 𝐴 . 𝑑𝑙 𝐽 𝒓 = 𝜓 0 𝑒 − 𝒓− 𝒓 𝒂 2 𝜉 𝑛 2 + 𝜓 0 𝑒 − 𝒓− 𝒓 𝑏 2 𝜉 𝑛 2 + 2 𝜓 0 2 sin ∆𝜑 𝑖𝑛𝑣 𝒓 + 𝜑 0 11

Simulations and experiments are in very good agreement. … TO SIMULATE THE JOSEPSHON VORTICES Josephson vortex 500 x 500 nm2 H = 120 mT Nat Phys 11 332-337 (2015) 1 1 superconductivity conductance Simulations and experiments are in very good agreement. 12

JOSEPSHON VORTICES IN ELECTRONIC CIRCUITS Nat Phys 11 332-337 (2015) 𝐼 1 𝐼 2 𝐼 Josephson vortices can be induced by supercurrents instead of magnetic field. 13

THANK YOU FOR YOUR ATTENTION!

JOSEPSHON VORTICES AS REAL VORTICES? 1 1 Currents Superconducting correlations 𝑐 𝒅𝒍 𝑱= 𝑒 ∗ 𝑚 ∗ 𝑐 𝒅𝒍 𝛹 𝒓 2 ħ𝛁𝜑 𝒓 − 𝑒 ∗ 𝑨 𝒓 𝟎 = ħ 𝐿 2𝜋 − 2𝑒 𝐵𝑆 ⇔ 𝐵𝑆=𝐿 𝛷 0 a Josephson vortex corresponds to a quanta of magnetic flux.

Josephson vortex cores have a normal state. AN ELECTRONIC DENSITY OF STATES! superconductor Josephson junction normal layer Abrikosov vortex Josephson vortex x x x x x Josephson vortex cores have a normal state.

ABRIKOSOV VORTICES supercurrents vortex core magnetic field vortices in superconductors An Abrikosov vortex has: a normal core, supercurrents around it, one quantum of magnetic flux.