Condensed Matter Physics CEG - Science and microwaves26th Jan 2004 Electronic properties of HTS and novel superconductors Intrinsic Josephson Tunnelling.

Slides:



Advertisements
Similar presentations
Single Electron Devices Single-electron Transistors
Advertisements

1 Quantum Enabling Technology Materials Research for Superconducting Quantum Computing Materials P.I. - D. P. Pappas Affiliates: Jeff Kline Fabio da Silva.
STM/S Imaging Studies in the Vortex State Anjan K. Gupta Physics Department, IIT, Kanpur (Tutorial, IVW10 at TIFR)
THE UNIVERSITY OF ALABAMA CENTER FOR MATERIALS FOR INFORMATION TECHNOLOGY An NSF Science and Engineering Center Quantum Design PPMS T: 350mK K H:
Electrical Techniques MSN506 notes. Electrical characterization Electronic properties of materials are closely related to the structure of the material.
OUTLINE Introduction „Tera-to-Nano“: Our Novel Near-Field Antenna 80 GHz CW Frequency Domain Measurements Picosecond Pulse Time Domain Measurements 2D.
Materials Science in Quantum Computing. Materials scientist view of qubit Materials –SiOx sub substrate –Superconductor (Al,Nb) –SiO x dielectric –Al0.
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.
Coherent Quantum Phase Slip Oleg Astafiev NEC Smart Energy Research Laboratories, Japan and The Institute of Physical and Chemical Research (RIKEN), Japan.
EE 403 (or 503) Introduction to plasma Processing Fall 2011 Title of the project Your name.
HTS Qubits and JJ's using BSCCO Design and Fabrication of HTS Qubits using BSCCO Suzanne Gildert.
Josephson Junctions, What are they?
Microwave Spectroscopy of the radio- frequency Cooper Pair Transistor A. J. Ferguson, N. A. Court & R. G. Clark Centre for Quantum Computer Technology,
What NEC Did Engineered a two-state system Initialized the system Formed a superposition state Allowed the system to evolve Stopped the evolution Read.
UNIVERSITY OF NOTRE DAME Xiangning Luo EE 698A Department of Electrical Engineering, University of Notre Dame Superconducting Devices for Quantum Computation.
The Three Hallmarks of Superconductivity
Submicron structures 26 th January 2004 msc Condensed Matter Physics Photolithography to ~1 μm Used for... Spin injection Flux line dynamics Josephson.
9. Semiconductors Optics Absorption and gain in semiconductors Principle of semiconductor lasers (diode lasers) Low dimensional materials: Quantum wells,
Electron Scattering Length - Mean Free Path – le - Avg. distance between scattering Si - ~ 5nm; GaAs - ~ 100 nm Electrical Resistance is closely related.
Robustness of Topological Superconductivity in Proximity-Coupled Topological Insulator Nanoribbons Tudor D. Stanescu West Virginia University Collaborators:
Josephson effect (see also hand-out) In 1962 Josephson predicted Cooper-pairs can tunnel through a weak link at zero voltage difference. Current in junction.
Metamaterial Emergence of novel material properties Ashida Lab Masahiro Yoshii PRL 103, (2009)
Superconducting Qubits Kyle Garton Physics C191 Fall 2009.
Condensed Matter Physics Big Facility Physics26th Jan 2004 Sub Heading “Big Facility” Physics in Grenoble ESRF: X-rays ILL: neutrons.
Implementation of a wideband phase shifter for phased array antennas MSc/M-Tech Electrical Engineering FSATIE/CPUT Vernon Davids Supervised by Dr. R. R.
Physical Phenomena for TeraHertz Electronic Devices
Chernogolovka, October 2009 Nolinear nonequilibrium phenomena in stacked junctions Vladimir Krasnov Experimental Condensed Matter Physics Fysikum, AlbaNova,
J. R. Kirtley et al., Phys. Rev. Lett. 76 (1996),
M.Hangyo,M.Tani,and T.Nagashima TERAHERTZ TIME-DOMAIN SPECTROSCOPY OF SOLIDS: A REVIEW International Journal of Infrared and Millimeter Waves,Vol. 26,
@Nagoya U. Sept. 5, 2009 Naoto Nagaosa Department of Applied Physics
Applications of Quantum Physics
ECE & TCOM 590 Microwave Transmission for Telecommunications Introduction to Microwaves January 29, 2004.
Materials World Network: Understanding & controlling optical excitations in individual hybrid nanostructures Gregory J. Salamo, University of Arkansas,
441 Chem Introduction to Spectroscopy CH-1 1. Introduction to Spectroscopy Set of methods where interaction of electromagnetic radiation with chemical.
Unconventional superconductivity Author: Jure Kokalj Mentor: prof. dr. Peter Prelovšek.
EPR OF QUASIPARTICLES BY FLUCTUATIONS OF COOPER PAIRS Jan Stankowski Institute of Molecular Physics, Polish Academy of Sciences Kazimierz Dolny 2005.
Noise and decoherence in the Josephson Charge Qubits Oleg Astafiev, Yuri Pashkin, Tsuyoshi Yamamoto, Yasunobu Nakamura, Jaw-Shen Tsai RIKEN Frontier Research.
Development of an Antenna-coupled Al Superconducting Tunnel Junction for a detection of cosmic microwave background B-mode polarization H. Ishino 4, M.
DC-squid for measurements on a Josephson persistent-current qubit Applied Physics Quantum Transport Group Alexander ter Haar May 2000 Supervisors: Ir.
Anisotropic Superconductivity in  -(BDA-TTP) 2 SbF 6 : STM Spectroscopy K. Nomura Department of Physics, Hokkaido University, Japan ECRYS-2008, Cargese.
1 H. Hayano for the ATF collaboration Low Emittance Beam Generation in ATF H. Hayano for the ATF collaboration BPM electronics improvement emittance tuning.
Postdoctoral research assistant discussion. The Topological Protected and Non-Equilibrium States (TOPNES) program gathers many scientists, grouped at.
Simulating current voltage characteristics in Intrinsic Josephson junctions M. Hromnik Yu. M. Shukrinov M Gaafar BLTP, JINR, Dubna , Russia.
Two Level Systems in Phase Qubits: Tunnel Barriers & Wiring Dielectrics Jeff Kline March 6, 2008.
Fundamentals of Transmission channels
Strontium Ruthenate Rachel Wooten Solid State II Elbio Dagotto
Institute of Physics Founded : 1993 Goals : –fundamental research in physics –graduate study Faculty: 11 Post doctors: 10 Assistant: 4 Students: Master.
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.
Measuring Quantum Coherence in the Cooper-Pair Box
An atomic Fermi gas near a p-wave Feshbach resonance
K. Gireesan1, T. S. Radhakrishnan1, Joseph Bensigh3, S
LLNL-PRES This work was performed under the auspices of the U.S. Department of Energy by Lawrence Livermore National Laboratory under Contract DE-AC52-07NA27344.
Superconductivity, Josephson Junctions, and squids
POLAR CLUSTERS IN: PLZT PSN-PMN-PZN SBN Mesoporous molecular sieves Conclusions.
Saptarshi Das, PhD 2. Adjunct Birck Research Scholar Birck Nanotechnology Center Purdue University West Lafayette, Indiana Post-doctoral Research.
Many-Body Effects in a Frozen Rydberg Gas Feng zhigang
Resonant Zener tunnelling via zero-dimensional states in a narrow gap InAsN diode Davide Maria Di Paola School of Physics and Astronomy The University.
Quantum mechanics in electronics
Unbound States A review on calculations for the potential step.
Circuit QED Experiment
BCS THEORY BCS theory is the first microscopic theory of superconductivity since its discovery in It explains, The interaction of phonons and electrons.
Superconducting Electromagnetic
Microwaves for Qubits on Helium
Evidence for fully gapped superconductivity from microwave penetration depth measurements in PrFeAsO1-y single crystals K. Hashimoto1, T. Shibauchi1,
شيمی تجزيه دستگاهی Instrumental Analysis, Second edition, Gary D.Christian and James E.O , Reily درس شيمی تجزيه دستگاهی ـ 3 واحد ـ رشته شيمی و شيمی.
Josephson supercurrent through a topological insulator surface state
Capacitors (Condenser)
Nuclear Magnetic Resonance Spectroscopy
Strong Coupling of a Spin Ensemble to a Superconducting Resonator
Quantum complexity in condensed matter physics
Presentation transcript:

Condensed Matter Physics CEG - Science and microwaves26th Jan 2004 Electronic properties of HTS and novel superconductors Intrinsic Josephson Tunnelling between atomic layers in HTS Fundamental physics + “blue sky” applications (THz spectroscopy, single-electron and quantum devices) microwave properties Fundamental physics + immediate applications Close synergy with “Emerging Device Technologies” –EE CMP includes - “Emerging Device Physics” introduction

Condensed Matter Physics CEG - Science and microwaves26th Jan 2004 Intrinsic Josephson Tunnelling between atomic layers in HTS Birmingham early SQUID measurements confirmed electron-pairing in d-wave HTS also first HTS quantum devices and microwave applications Cooper pairs excitations volts current volts 2  - energy gap Ij sin  Intrinsic tunnelling

Condensed Matter Physics CEG - Science and microwaves26th Jan 2004 Intrinsic Josephson Junction Tunnelling in BSCCO BSCCO-2212 Bi 2 Sr 2 CaCu 2 O 8 electrical anisotropy ~10 5 quasi-2d HTc superconductor d-wave l =2 Cooper pairs Energy gap  (T,B)  (  )~ cos2   line nodes - gap 0 inter-layer quantum tunnnelling BSCCO xtal

Condensed Matter Physics CEG - Science and microwaves26th Jan 2004 BSSCO cleaves atomically flat ~ mm Ion beam and chemical photolithography 10 – 50  m mesa structures 4-point VI measurements across 1-50 atomic layers atomically defined intrinsic JJs Mesa structures

Condensed Matter Physics CEG - Science and microwaves26th Jan 2004 Birmingham measurements Intrinsic tunnelling across individual atomic layers 10 Josephson junctions in series d-wave Cooper pair and quasi-particle tunnelling 4-point IV measurements 20 ns resolution tunnelling dynamics. Measurement expertise x x x x x

Condensed Matter Physics CEG - Science and microwaves26th Jan 2004 Future - quantum physics of atomically-defined structures Intrinsic single-electron array devices Intrinsic Coulomb-blockade array structures Quantum coherence/computing – Q-bits Also THz spectroscopy (ac Josephson) ~ 100 nm HTS mesa (FIB -Nature + Nano-technology in Engineering) 1 nm Quantum devices Charging energy e 2 /2C >> kT Resistance/junction > R quantum = h/e 2

Condensed Matter Physics CEG - Science and microwaves26th Jan 2004 Spintronics on individual atomic layers with Chris Muirhead and Mark Colclough Spintronics(2) V Measure changes in T c and Josephson current on the top atomic plane

Condensed Matter Physics CEG - Science and microwaves26th Jan 2004 Birmingham facility is unique Very high resolution/sensitivity MHz - 40 GHz 50 mK to room temperature B up to 16T Low T - T c often ~ 1K High B - Hc 2 often ~ 10T Microwave physics -HTS and other novel s/c existing 5-year portfolio programme CEG, Dr Rod Ormeno and Tim Barraclough Microwaves

Condensed Matter Physics CEG - Science and microwaves26th Jan 2004 What do microwaves tell us? Complex conductivity  =  1 + i  2 “normal” electrons s/c electrons Penetration and losses B(r) ~ exp(-x/   wave penetration and losses

Condensed Matter Physics CEG - Science and microwaves26th Jan 2004 Novel dielectric resonator and typical data Sr 2 RuO 4 p-wave s/c Cavity measurements Position and width to 50Hz in 10GHz 0 1K Measure resonant frequency shifts and Q-values - sub 1mm single crystals

Condensed Matter Physics CEG - Science and microwaves26th Jan 2004 novel materials -novel pairing- novel physics heavy fermions UPt 3, CeCoIn 5 pairing ? Strontium Ruthenate p-wave HTc d-wave pairing Organic s/c  -(ET) 2 Cu(SCN) 2 pairing ? MgB 2 Tc~38K s-wave, but 2 energy gaps Also conventional s/c T meas < 1K h  > kT B measurements Novel materials

Condensed Matter Physics CEG - Science and microwaves26th Jan 2004 EE - Emerging Device Technologies Group Prof Mike Lancaster, Dr Tim Jackson, Dr Anton Velichko + 4 others Close synergy in research non-linear properties, spin-injection tuning of filters, ferrites, ferro-electrics,dielectrics continued collaboration involving frontier physics EPSRC views collaboration as a major Birmingham strength Birmingham Microwave programme Physics - fundamental science Electrical Engineering – applications filters for mobile communications front-end filters for radio astronomy - Jodrell Bank Telescope delay lines and signal processing tuneable filters with ferroelectrics Synergy with EE

Condensed Matter Physics CEG - Science and microwaves26th Jan 2004