Superconducting devices based on coherent operation of Josephson junction arrays above 77K

Size: px
Start display at page:

Download "Superconducting devices based on coherent operation of Josephson junction arrays above 77K"

Transcription

1 Electronic Devices, Invited talk, ISS 2017, Tokyo, Japan Superconducting devices based on coherent operation of Josephson junction arrays above 77K Boris Chesca Physics Department, Loughborough University, UK Collaborators Loughborough University Experimental: PhD/postdoc, Daniel John Dr. Marat Gaifullin Master students: Matthew Kemp, Jeffrey Brown, Richard Pollett Theory: PhD Jonathan Cox, Prof. Sergey Savelev Nottingham University: Christopher Mellor 1

2 Outline 77 K better than 4.2 K First flux-flow microwave 77K Josephson vortex-flow transistors with record 77K reversible flux-flow ratchets 2

3 77 K better than 4.2 K 3

4 SQUID SQUID arrays N SQUID array B. Chesca, American Institute of Physics, press release October 2015: Noise Array = N 1/2 Noise SQUID V Array = N V SQUID [ ] Array N 1/2 ]SQUID [ Noise 1 Noise = V V flux coherent & non-interacting SQUID array 4

5 V Array = N V SQUID, small arrays (N=10) V Array = N V SQUID true for 2 SQUIDs 2 SQUIDs 1 SQUID V Array = N V SQUID NOT true for 10 SQUIDs! 10 SQUIDs 1 SQUID Chiu-Hsien Wu et al, J. Appl. Phys. 100, (2006); 5

6 V Array = N V SQUID, small arrays (N=10) V Array = N V SQUID true for 10 SQUIDs but SQUIDs are too large; this design is not suitable for large N! C. H. Wu et al, Supercond. Sci. Technol. 19, S246 (2006) 6

7 Large SQUID arrays (N=484, 770) B. Chesca, D. John, C. Mellor, Appl. Phys. Lett. 107, (2015) International Patent, PCT: B. Chesca, D. John, WO A1(2017) 7

8 SQUID 77K better than 4.2 K -5 Voltage V, mv series SQUID array T=83K, V max =6.8 mv (b) -172 A -212 A Applied magnetic field B, T 10 S 1/2 ( Hz1/2 ) K K 1/N 1/2 Max ( V), mv Number of SQUIDs Number of SQUIDs 5 HTS 77 K nano-hts 4.2 K LTS 4.2 K B. Chesca, D. John, C. Mellor, Appl. Phys. Lett. 107, (2015); D. Castelvecchi and B. Chesca, Nature, Research Highlights 526, 613 (2015). 8

9 First flux-flow microwave 77K 9

10 10x10 JJ array as tunable microwave 4.2K GHz P. A. A. Booi, and S. P. Benz, Appl. Phys. Lett. 64, 2163 (1994) 10

11 Flux-flow resonances in asymmetric 440 JJ arrays B-field tunable power of about 0.1 µw within the range (1.5-25) 77K 1.0 P=0.5(I I step /I c ) 2 R N /N Flux-flow resonances T=77K, 15 IVCs Current, I (ma) 0.5 m=2 asymmetric array 22 x 20 JJ B YBCO (a) set of 20 JJ 20 m Voltage, V ( V) B. Chesca, D. John, C. Mellor, Supercond. Sci. Technol. 27, (2014) I V 11

12 Flux-flow resonances in asymmetric 440 JJ arrays 1.0 Array of 22 x 20 JJ T=84 K IVCs: 1-16 m=1 Current (ma) 0.5 m=3 m=4 Voltage, V/I C R N m=4 m=1 m=4 m= (b) ex Voltage ( V) B. Chesca, D. John, C. Mellor, Supercond. Sci. Technol. 27, (2014) 12

13 Josephson vortex-flow transistors (JVFT) with record 77K 13

14 Previous JVFT designs: asymmetrical bias current Small symmetrical arrays (6JJ), maximum current 77K: 3.5 R. Gross, et.al, Appl. Supercond. 3, 443 (1995) 14

15 1.0 4 IEEE/CSC & ESAS SUPERCONDUCTIVITY NEWS FORUM (global edition), February Anomalous flux-flow in large asymmetric arrays Large asymmetrical arrays (440 JJ) maximum current 77K: Current (ma) g max =0.28mA/15 A=19 Maximum Current Gain Parallel array of 22 x 20 JJ T=77K Voltage ( V) gmax (T) Temperature (K) B. Chesca, D. John, C. Mellor, Appl. Phys. Lett. 103, (2013) 15

16 Current amplification in large asymmetric arrays Critical Current, I c (ma) Parallel array of 22 x 20 JJ T=77 K g max = V -0.2 V -0.3 V -0.4 V -0.5 V -0.6 V -0.7 V Critical Current, I c (ma) Parallel array of 22 x 20 JJ T=77 K 0.7 V 0.6 V 0.5 V 0.4 V 0.3 V 0.2 V 0.1 V g max = (b) 0.4 (a) Control Current, I ctrl (ma) Control Current, I ctrl (ma) B. Chesca, D. John, C. Mellor, Appl. Phys. Lett. 103, (2013) 16

17 Reversible flux-flow ratchets 17

18 Which ratchet? 100% Symmetric J c, asymmetric A 10 JJ array Simulations (a) Symmetric j c & A Asymmetric j c & A Asymmetric J c, symmetric A Magnetic Field, 0 /S 1 B. Chesca, D. John, R. Pollett, M. Gaifullin, J. Cox, C. Mellor, S. Savelev, Appl. Phys. Lett. 111, (2017). 18

19 Reversible flux-flow ratchets ex JJ array, sample A T=89K 40 I=-100 A, 100 A, sample A 20 0 Voltage, V I, A T=89K B=4 T V, V I, A T=89K 221 IVs -300 B=(-37 T, 37 T) V, V B, T I=-100 A, 100 A, sample B A -100 A B, T B, T B. Chesca, D. John, R. Pollett, M. Gaifullin, J. Cox, C. Mellor, S. Savelev, Appl. Phys. Lett. 111, (2017). 19

20 Conclusions Remarkable performances shown by very large arrays-based 77K series arrays: magnetometers asymmetric parallel arrays: flux-flow microwave generators transistors reversible ratchets Great potential to replace single-jj or single-squid based 4.2K performance can be further improved by optimization 20

Large scale 2D SQIF arrays

Large scale 2D SQIF arrays Large scale 2D SQIF arrays Shane T Keenan CSIRO, Sydney, Australia EUCAS, 18 th September 2017 E Mitchell, K Hannam, J Lazar, C Lewis, A Grancea, K Wilson, B Vasilevski, W Purches and C Foley MANUFACTURING

More information

Superconducting Flux Qubits: The state of the field

Superconducting Flux Qubits: The state of the field Superconducting Flux Qubits: The state of the field S. Gildert Condensed Matter Physics Research (Quantum Devices Group) University of Birmingham, UK Outline A brief introduction to the Superconducting

More information

Final Report. Superconducting Qubits for Quantum Computation Contract MDA C-A821/0000

Final Report. Superconducting Qubits for Quantum Computation Contract MDA C-A821/0000 Final Report Superconducting Qubits for Quantum Computation Contract MDA904-98-C-A821/0000 Project Director: Prof. J. Lukens Co-project Director: Prof. D. Averin Co-project Director: Prof. K. Likharev

More information

Title. Author(s)Terauchi, N.; Noguchi, S.; Igarashi, H. CitationPhysica C: Superconductivity, 471(21-22): Issue Date Doc URL.

Title. Author(s)Terauchi, N.; Noguchi, S.; Igarashi, H. CitationPhysica C: Superconductivity, 471(21-22): Issue Date Doc URL. Title Magnetic shield effect simulation of superconducting magnetometer Author(s)Terauchi, N.; Noguchi, S.; Igarashi, H. CitationPhysica C: Superconductivity, 471(21-22): 1253-1257 Issue Date 2011-11 Doc

More information

Self-Induced Resonances in Asymmetric Superconducting Quantum Interference Devices

Self-Induced Resonances in Asymmetric Superconducting Quantum Interference Devices Vol. 114 (2008) ACTA PHYSICA POLONICA A No. 1 Proceedings of the XIII National School of Superconductivity, L adek Zdrój 2007 Self-Induced Resonances in Asymmetric Superconducting Quantum Interference

More information

Superconducting Metamaterials

Superconducting Metamaterials Superconducting Metamaterials P. Jung 1, S. Butz 1, N. Maleeva 1,2, A. Averkin 2, N. Abramov 2, K. Shulga 2,3 V. P. Koshelets 2,4, L. V. Filippenko 2,4, V. Chichkov 2 A. Karpov 2, S. V. Shitov 2,4, V.

More information

Principles and Applications of Superconducting Quantum Interference Devices (SQUIDs)

Principles 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 information

M.C. Escher. Angels and devils (detail), 1941

M.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 information

The Nanotube SQUID. uhu,, M. Monthioux,, V. Bouchiat, W. Wernsdorfer, CEMES-Toulouse, CRTBT & LLN Grenoble

The Nanotube SQUID. uhu,, M. Monthioux,, V. Bouchiat, W. Wernsdorfer, CEMES-Toulouse, CRTBT & LLN Grenoble The Nanotube SQUID J.-P. Cleuziou,, Th. Ondarçuhu uhu,, M. Monthioux,, V. Bouchiat, W. Wernsdorfer, CEMES-Toulouse, CRTBT & LLN Grenoble Outline Sample fabrication Proximity effect in CNT The CNT superconducting

More information

QIC 890/891, Module 4: Microwave Parametric Amplification in Superconducting Qubit Readout experiments

QIC 890/891, Module 4: Microwave Parametric Amplification in Superconducting Qubit Readout experiments QIC 890/891, Module 4: Microwave Parametric Amplification in Superconducting Qubit Readout experiments 1 Instructor: Daryoush Shiri Postdoctoral fellow, IQC IQC, June 2015, WEEK-2 2 Parametric Amplifiers

More information

Superconducting Nanowire Single Photon Detector. for Quantum Information SNSPD for QI. Lixing You. Dept of Phys., UC Berkeley

Superconducting Nanowire Single Photon Detector. for Quantum Information SNSPD for QI. Lixing You. Dept of Phys., UC Berkeley ISS 2015 28th International Symposium on Superconductivity November 16-18, 2015 Superconducting Nanowire Single Photon Detector for Quantum Information SNSPD for QI Lixing You 1 Shanghai Center for SuperConductivity

More information

Electric transport measurements of thin film high-tc superconductor bicrystal grain boundary Josephson junctions

Electric transport measurements of thin film high-tc superconductor bicrystal grain boundary Josephson junctions Loughborough University Institutional Repository Electric transport measurements of thin film high-tc superconductor bicrystal grain boundary Josephson junctions This item was submitted to Loughborough

More information

Superconducting Qubits

Superconducting Qubits Superconducting Qubits Fabio Chiarello Institute for Photonics and Nanotechnologies IFN CNR Rome Lego bricks The Josephson s Lego bricks box Josephson junction Phase difference Josephson equations Insulating

More information

Strong tunable coupling between a charge and a phase qubit

Strong tunable coupling between a charge and a phase qubit Strong tunable coupling between a charge and a phase qubit Wiebke Guichard Olivier Buisson Frank Hekking Laurent Lévy Bernard Pannetier Aurélien Fay Ioan Pop Florent Lecocq Rapaël Léone Nicolas Didier

More information

Dynamical Casimir effect in superconducting circuits

Dynamical 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 information

Non-linear driving and Entanglement of a quantum bit with a quantum readout

Non-linear driving and Entanglement of a quantum bit with a quantum readout Non-linear driving and Entanglement of a quantum bit with a quantum readout Irinel Chiorescu Delft University of Technology Quantum Transport group Prof. J.E. Mooij Kees Harmans Flux-qubit team visitors

More information

Theory for investigating the dynamical Casimir effect in superconducting circuits

Theory for investigating the dynamical Casimir effect in superconducting circuits Theory for investigating the dynamical Casimir effect in superconducting circuits Göran Johansson Chalmers University of Technology Gothenburg, Sweden International Workshop on Dynamical Casimir Effect

More information

Direct Measurement of Penetration Length in Ultra-Thin and/or Mesoscopic Superconducting Structures

Direct Measurement of Penetration Length in Ultra-Thin and/or Mesoscopic Superconducting Structures Direct Measurement of Penetration Length in Ultra-Thin and/or Mesoscopic Superconducting Structures L. Hao National Physical Laboratory, Teddington, TW11 0LW, United Kingdom; J.C. Macfarlane Department

More information

Quantum Optics with Propagating Microwaves in Superconducting Circuits. Io-Chun Hoi 許耀銓

Quantum 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 information

Chapter 5 Nanomanipulation. Chapter 5 Nanomanipulation. 5.1: With a nanotube. Cutting a nanotube. Moving a nanotube

Chapter 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 information

Testing axion physics in a Josephson junction environment

Testing axion physics in a Josephson junction environment Testing axion physics in a Josephson junction environment Christian Beck Queen Mary, University of London 1 Testing axion physics in a Josephson junction environment Christian Beck Queen Mary, University

More information

Fabio Chiarello IFN-CNR Rome, Italy

Fabio Chiarello IFN-CNR Rome, Italy Italian National Research Council Institute for Photonics and Nanotechnologies Elettronica quantistica con dispositivi Josephson: dagli effetti quantistici macroscopici al qubit Fabio Chiarello IFN-CNR

More information

From Last Time. Partially full bands = metal Bands completely full or empty = insulator / seminconductor

From 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 information

Cryogenic memory element based on a single Abrikosov vortex

Cryogenic memory element based on a single Abrikosov vortex Cryogenic memory element based on a single Abrikosov vortex Vladimir Krasnov, T. Golod and A. Iovan Experimental Condensed Matter Physics Group Department of Physics Stockholm University AlbaNova University

More information

Coherent Coupling between 4300 Superconducting Flux Qubits and a Microwave Resonator

Coherent 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 information

The Influence of the Second Harmonic in the Current-Phase Relation on the Voltage-Current Characteristic of high T C DC SQUID

The Influence of the Second Harmonic in the Current-Phase Relation on the Voltage-Current Characteristic of high T C DC SQUID The Influence of the Second Harmonic in the Current-Phase Relation on the Voltage-Current Characteristic of high T C DC SQUID Ya. S. Greenberg 1,*, I. L. Novikov 1, V. Schultze 2, H.-G. Meyer 2 1 Novosibirsk

More information

Curriculum Vitae. Shkolnykov Vladyslav, MPhys.

Curriculum Vitae. Shkolnykov Vladyslav, MPhys. Curriculum Vitae Personal Data Shkolnykov Vladyslav, MPhys. Date of birth 8 November, 1991 Residence Reutestrasse 104, 78467 Konstanz, Germany Citizenship Ukraine Marital status single Tel. +49 (162) 544-20-98

More information

FYSZ 460 Advanced laboratory work: Superconductivity and high T C superconductor Y 1 Ba 2 Cu 3 O 6+y

FYSZ 460 Advanced laboratory work: Superconductivity and high T C superconductor Y 1 Ba 2 Cu 3 O 6+y FYSZ 460 Advanced laboratory work: Superconductivity and high T C superconductor Y 1 Ba 2 Cu 3 O 6+y Laboratory Instructions Minna Nevala minna.nevala@phys.jyu.fi November 15, 2010 Contents 1 Introduction

More information

Superconducting qubits (Phase qubit) Quantum informatics (FKA 172)

Superconducting 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 information

Design Considerations for Integrated Semiconductor Control Electronics for a Large-scale Solid State Quantum Processor

Design Considerations for Integrated Semiconductor Control Electronics for a Large-scale Solid State Quantum Processor Design Considerations for Integrated Semiconductor Control Electronics for a Large-scale Solid State Quantum Processor Hendrik Bluhm Andre Kruth Lotte Geck Carsten Degenhardt 1 0 Ψ 1 Quantum Computing

More information

Supercondcting Qubits

Supercondcting 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 information

phys4.20 Page 1 - the ac Josephson effect relates the voltage V across a Junction to the temporal change of the phase difference

phys4.20 Page 1 - the ac Josephson effect relates the voltage V across a Junction to the temporal change of the phase difference Josephson Effect - the Josephson effect describes tunneling of Cooper pairs through a barrier - a Josephson junction is a contact between two superconductors separated from each other by a thin (< 2 nm)

More information

Nonlinear multilevel dynamics of a coupled SQUID ring-resonator system in the hysteretic regime

Nonlinear multilevel dynamics of a coupled SQUID ring-resonator system in the hysteretic regime Loughborough University Institutional Repository Nonlinear multilevel dynamics of a coupled SQUID ring-resonator system in the hysteretic regime This item was submitted to Loughborough University's Institutional

More information

Exploring parasitic Material Defects with superconducting Qubits

Exploring parasitic Material Defects with superconducting Qubits Exploring parasitic Material Defects with superconducting Qubits Jürgen Lisenfeld, Alexander Bilmes, Georg Weiss, and A.V. Ustinov Physikalisches Institut, Karlsruhe Institute of Technology, Karlsruhe,

More information

A TES Bolometer for THz FT-Spectroscopy

A TES Bolometer for THz FT-Spectroscopy A TES Bolometer for THz FT-Spectroscopy M. Kehrt, J. Beyer, C. Monte, J. Hollandt Physikalisch-Technische Bundesanstalt Abbestraße 2-12, Berlin, Germany E-Mail: Mathias.Kehrt@PTB.de Abstract - We recently

More information

nano Josephson junctions Quantum dynamics in

nano Josephson junctions Quantum dynamics in Permanent: Wiebke Guichard Olivier Buisson Frank Hekking Laurent Lévy Cécile Naud Bernard Pannetier Quantum dynamics in nano Josephson junctions CNRS Université Joseph Fourier Institut Néel- LP2MC GRENOBLE

More information

Eli Levenson-Falk CURRICULUM VITAE

Eli Levenson-Falk CURRICULUM VITAE Eli Levenson-Falk CURRICULUM VITAE Department of Physics and Astronomy elevenso@usc.edu (213) 740-0163 Updated 10/1/2018 RESEACH INTERESTS My research focuses on the development and use of superconducting

More information

SPECTRUM of electromagnetic radiation from a type-ii

SPECTRUM of electromagnetic radiation from a type-ii IEEE TRANSACTIONS ON APPLIED SUPERCONDUCTIVITY, VOL. 19, NO. 4, AUGUST 2009 3653 A Superconductor THz Modulator Based on Vortex Flux Flow Farrokh Sarreshtedari, Mehdi Hosseini, Hamid Reza Chalabi, Ali

More information

Zero-biased YBCO detectors for the real-time observation of coherent synchrotron radiation

Zero-biased YBCO detectors for the real-time observation of coherent synchrotron radiation Zero-biased YBCO detectors for the real-time observation of KSETA Plenary Workshop, 13-15 February 217, Durbach J. Raasch Institut für Mikro- und Nanoelektronische Systeme (IMS) KIT University of the State

More information

Spin-torque nano-oscillators trends and challenging

Spin-torque nano-oscillators trends and challenging Domain Microstructure and Dynamics in Magnetic Elements Heraklion, Crete, April 8 11, 2013 Spin-torque nano-oscillators trends and challenging N H ext S Giovanni Finocchio Department of Electronic Engineering,

More information

Molecular prototypes for spin-based CNOT and SWAP quantum logic gates

Molecular prototypes for spin-based CNOT and SWAP quantum logic gates Bellaterra: anuary 2011 Architecture & Design of Molecule Logic Gates and Atom Circuits Molecular prototypes for spin-based CNOT and SWAP quantum logic gates Fernando LUIS Instituto de Ciencia de Materiales

More information

Measuring heat current and its fluctuations in superconducting quantum circuits

Measuring heat current and its fluctuations in superconducting quantum circuits Measuring heat current and its fluctuations in superconducting quantum circuits Bayan Karimi QTF Centre of Excellence, Department of Applied Physics, Aalto University, Finland Supervisor: Jukka P. Pekola

More information

The Quantum Supremacy Experiment

The Quantum Supremacy Experiment The Quantum Supremacy Experiment John Martinis, Google & UCSB New tests of QM: Does QM work for 10 15 Hilbert space? Does digitized error model also work? Demonstrate exponential computing power: Check

More information

Vortex matter in HTS Grain Boundary Josephson Junctions: Intrinsic and Extrinsic d-wave Effects

Vortex matter in HTS Grain Boundary Josephson Junctions: Intrinsic and Extrinsic d-wave Effects Vortex matter in HTS Grain Boundary Josephson Junctions: Intrinsic and Extrinsic d-wave Effects Francesco Tafuri INFM Coherentia Seconda Università di Napoli In collaboration with: J. Kirtley and C. Tsuei,

More information

LECTURE 2: Thermometry

LECTURE 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 information

QuAMP Towards large scale quantum informa4on processing: Sta4c magne4c field gradient quantum gates and microfabricated ion traps

QuAMP Towards large scale quantum informa4on processing: Sta4c magne4c field gradient quantum gates and microfabricated ion traps QuAMP 2013 Towards large scale quantum informa4on processing: Sta4c magne4c field gradient quantum gates and microfabricated ion traps Kim Lake University of Sussex Talk Outline Ion Trapping and Ytterbium

More information

Modern Physics for Scientists and Engineers International Edition, 4th Edition

Modern 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 information

Post Von Neumann Computing

Post Von Neumann Computing Post Von Neumann Computing Matthias Kaiserswerth Hasler Stiftung (formerly IBM Research) 1 2014 IBM Corporation Foundation Purpose Support information and communication technologies (ICT) to advance Switzerland

More information

Status of 2G HTS Wire Production at SuperOx

Status of 2G HTS Wire Production at SuperOx Status of 2G HTS Wire Production at SuperOx Sergey Samoilenkov SuperOx, Moscow, Russia 1 Outline About SuperOx 2G HTS wire characteristics New customization options for 2G HTS wire Development for applications

More information

Aspects of of Intrinsic Josephson Tunneling

Aspects of of Intrinsic Josephson Tunneling Aspects of of Intrinsic Josephson Tunneling D. Winkler, 1,2 A. Yurgens, 1 V.M. Krasnov, 1 Y.S. Sudershan, 1 T. Claeson, 1 E. J. Tarte, 3 M.G. Blamire 3 Chalmers University of Technology and Göteborg University

More information

Interplay between static and dynamic properties of semifluxons in Y Ba 2 Cu 3 O 7 δ 0 π Josephson junctions

Interplay between static and dynamic properties of semifluxons in Y Ba 2 Cu 3 O 7 δ 0 π Josephson junctions Interplay between static and dynamic properties of semifluxons in Y Ba 2 Cu 3 O 7 δ 0 π Josephson junctions K. Cedergren 1, J.R. Kirtley 2, T. Bauch 1, G. Rotoli 3, A. Troeman 4, H. Hilgenkamp 4, F. Tafuri

More information

Nanoelectronics 08. Atsufumi Hirohata Department of Electronics. Quick Review over the Last Lecture E = 2m 0 a 2 ξ 2.

Nanoelectronics 08. Atsufumi Hirohata Department of Electronics. Quick Review over the Last Lecture E = 2m 0 a 2 ξ 2. Nanoelectronics 08 Atsufumi Hirohata Department of Electronics 09:00 Tuesday, 6/February/2018 (P/T 005) Quick Review over the Last Lecture 1D quantum well : E = 2 2m 0 a 2 ξ 2 ( Discrete states ) Quantum

More information

Superconducting Resonators and Their Applications in Quantum Engineering

Superconducting 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 information

Quantum dynamics in Josephson junction circuits Wiebke Guichard Université Joseph Fourier/ Néel Institute Nano Department Equipe Cohérence quantique

Quantum dynamics in Josephson junction circuits Wiebke Guichard Université Joseph Fourier/ Néel Institute Nano Department Equipe Cohérence quantique Quantum dynamics in Josephson junction circuits Wiebke Guichard Université Joseph Fourier/ Néel Institute Nano Department Equipe Cohérence quantique Josephson junction team Olivier Buisson, Bernard Pannetier,

More information

Lectures of ENVIRONMENTAL ELECTRICAL SCIENCE

Lectures of ENVIRONMENTAL ELECTRICAL SCIENCE Lectures of ENVIRONMENTAL ELECTRICAL SCIENCE CEI EN 50366 Standard Presentation edited by: Prof. Alvise Maschio Department of Industrial Engineering University of Padova 12/9/13 1/11 Index of lecture 19

More information

Sub-Boltzmann Transistors with Piezoelectric Gate Barriers

Sub-Boltzmann Transistors with Piezoelectric Gate Barriers Sub-Boltzmann Transistors with Piezoelectric Gate Barriers Raj Jana, Gregory Snider, Debdeep Jena Electrical Engineering University of Notre Dame 29 Oct, 2013 rjana1@nd.edu Raj Jana, E3S 2013, Berkeley

More information

Coherent oscillations in a charge qubit

Coherent oscillations in a charge qubit Coherent oscillations in a charge qubit The qubit The read-out Characterization of the Cooper pair box Coherent oscillations Measurements of relaxation and decoherence times Tim Duty, Kevin Bladh, David

More information

2015 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 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 information

Superconducting Qubits. Nathan Kurz PHYS January 2007

Superconducting 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 information

November 16, 2015 ISS 2015 (Funabori, Tokyo) Road to Higher T. S. Uchida, Univ of Tokyo, 2. AIST, Tsukuba, 3. IOP-CAS, Beijing

November 16, 2015 ISS 2015 (Funabori, Tokyo) Road to Higher T. S. Uchida, Univ of Tokyo, 2. AIST, Tsukuba, 3. IOP-CAS, Beijing Road to Higher T November 16, 2015 ISS 2015 (Funabori, Tokyo) S. Uchida, 1 Univ of Tokyo, 2 AIST, Tsukuba, 3 IOP-CAS, Beijing T c stopped rising in 1993 (more than 20 years silence ), but signatures of

More information

Configuration-induced vortex motion in type II superconducting films with periodic magnetic dot arrays

Configuration-induced vortex motion in type II superconducting films with periodic magnetic dot arrays Configuration-induced vortex motion in type II superconducting films with periodic magnetic dot arrays Qinghua Chen Prof. Shi Xue Dou 1 Outline: I. An Introduction of superconductor II. Overview of vortex

More information

CONTENTS. Contributors. Preface HTS APPLICATIONS: PRESENT AND FUTURE PROSPECTS. Pascal TIXADOR

CONTENTS. Contributors. Preface HTS APPLICATIONS: PRESENT AND FUTURE PROSPECTS. Pascal TIXADOR CONTENTS Contributors Preface v xi HTS APPLICATIONS: PRESENT AND FUTURE PROSPECTS Pascal TIXADOR Introduction 1 Required Elements 2 LTS Applications 5 HTS Applications 8 General Conclusions 30 References

More information

Superconductivity at nanoscale

Superconductivity 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 information

Large-scale Simulation for a Terahertz Resonance Superconductor Device

Large-scale Simulation for a Terahertz Resonance Superconductor Device Large-scale Simulation for a Terahertz Resonance Superconductor Device Project Representative Masashi Tachiki Research Organization for Information Science and Technology Authors Mikio Iizuka 1, Masashi

More information

Vortices in Classical Systems

Vortices in Classical Systems Vortices in Classical Systems 4 He-II vortices: Vortices in Quantum Systems STM of NbSe 2 vortices: G. A. Williams, R. E. Packard, Hess PRL (1989). Phys. Rev. Lett. 33, 280 (1974) Pan, Hudson, Davis, RSI

More information

single-electron electron tunneling (SET)

single-electron electron tunneling (SET) single-electron electron tunneling (SET) classical dots (SET islands): level spacing is NOT important; only the charging energy (=classical effect, many electrons on the island) quantum dots: : level spacing

More information

arxiv: v1 [cond-mat.supr-con] 23 Sep 2011

arxiv: v1 [cond-mat.supr-con] 23 Sep 2011 Modeling and Simulation of a Microstrip-SQUID Amplifier G.P. Berman a, O.O. Chumak b, D.I. Kamenev a, D. Kinion c, and V.I. Tsifrinovich d a Theoretical Division, Los Alamos National Laboratory, Los Alamos,

More information

Александр Баланов

Александр Баланов a.balanov@lboro.ac.uk Александр Баланов a.balanov@lboro.ac.uk Collaborators M.T. Greenaway (University of Nottingham, UK) T.M. Fromhold (University of Nottingham, UK) A.O. Selskii (Saratov State University,

More information

The New IMP(F) - F4 unified. Nanoscale Science and Technology

The New IMP(F) - F4 unified. Nanoscale Science and Technology IMP(F) - Nanoscale Science and Technology The New IMP(F) - F4 unified International Master s Programme in Nanoscale Science and Technology 2002/2003 Göran Wendin, MINA/MC2 What sizes are we talking about?

More information

Electrical quantum engineering with superconducting circuits

Electrical 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 information

Quantum Technologies CCEM Workshop March 23 rd, 2017

Quantum Technologies CCEM Workshop March 23 rd, 2017 Quantum Technologies CCEM Workshop March 23 rd, 2017 JT Janssen Welcome to the National Physical Laboratory The first quantum revolution h V n f 2 e 1 The second quantum revolution Superposition Entanglement

More information

Topologicaly protected abelian Josephson qubits: theory and experiment.

Topologicaly protected abelian Josephson qubits: theory and experiment. Topologicaly protected abelian Josephson qubits: theory and experiment. B. Doucot (Jussieu) M.V. Feigelman (Landau) L. Ioffe (Rutgers) M. Gershenson (Rutgers) Plan Honest (pessimistic) review of the state

More information

Noise effects and thermally induced switching errors in Josephson junctions

Noise effects and thermally induced switching errors in Josephson junctions 3479 Noise effects and thermally induced switching errors in Josephson junctions Andrey L. Pankratov 1 and Bernardo Spagnolo 2 1 Institute for Physics of Microstructures of RAS, Nizhny Novgorod, Russia

More information

Prospective performance of graphene HEB for ultrasensitive detection of sub-mm radiation

Prospective performance of graphene HEB for ultrasensitive detection of sub-mm radiation Prospective performance of graphene HEB for ultrasensitive detection of sub-mm radiation Boris S. Karasik 1, Christopher B. McKitterick 2, and Daniel E. Prober 2 1 Jet Propulsion Laboratory, California

More information

From SQUID to Qubit Flux 1/f Noise: The Saga Continues

From SQUID to Qubit Flux 1/f Noise: The Saga Continues From SQUID to Qubit Flux 1/f Noise: The Saga Continues Fei Yan, S. Gustavsson, A. Kamal, T. P. Orlando Massachusetts Institute of Technology, Cambridge, MA T. Gudmundsen, David Hover, A. Sears, J.L. Yoder,

More information

Energy harvesting in nanoelectronic devices. Technische Physik, Universität Würzburg, Germany

Energy harvesting in nanoelectronic devices. Technische Physik, Universität Würzburg, Germany Energy harvesting in nanoelectronic devices Lukas Worschech Technische Physik, Universität Würzburg, Germany Energy harvesting with nanoelectronics Energy harvesting: Energy provider+transducer+rectifier

More information

Title. Author(s)Hatta, E.; Nagao, J.; Mukasa, K. CitationJournal of Applied Physics, 79(3): Issue Date Doc URL. Rights.

Title. Author(s)Hatta, E.; Nagao, J.; Mukasa, K. CitationJournal of Applied Physics, 79(3): Issue Date Doc URL. Rights. Title Tunneling through a narrow-gap semiconductor with di Author(s)Hatta, E.; Nagao, J.; Mukasa, K. CitationJournal of Applied Physics, 79(3): 1511-1514 Issue Date 1996-02-01 Doc URL http://hdl.handle.net/2115/5716

More information

Excess Noise in TESs A comparison between theories.

Excess Noise in TESs A comparison between theories. Space Research Centre Excess Noise in TESs A comparison between theories Daniel Brandt, George W. Fraser, Stephen Smith www.src.le.ac.uk Introduction Excess Noise Theories Experiments have shown that the

More information

Chapter 10. Superconducting Quantum Circuits

Chapter 10. Superconducting Quantum Circuits AS-Chap. 10-1 Chapter 10 Superconducting Quantum Circuits AS-Chap. 10-2 10.1 Fabrication of JJ for quantum circuits AS-Chap. 10-3 Motivation Repetition Current-phase and voltage-phase relation are classical,

More information

Quantum physics in quantum dots

Quantum 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 information

Broadband ESR from 500 MHz to 40 GHz using superconducting coplanar waveguides

Broadband ESR from 500 MHz to 40 GHz using superconducting coplanar waveguides Broadband ESR from 500 MHz to 40 GHz using superconducting coplanar waveguides Martin Dressel 1. Physikalisches Institut, Universität Stuttgart, Germany Outline 1. Introduction ESR resonators 2. Strip

More information

Introduction 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 Introduction to Superconductivity Superconductivity was discovered in 1911 by Kamerlingh Onnes. Zero electrical resistance Meissner Effect Magnetic field expelled. Superconducting surface current ensures

More information

This is an electronic reprint of the original article. This reprint may differ from the original in pagination and typographic detail.

This is an electronic reprint of the original article. This reprint may differ from the original in pagination and typographic detail. Powered by TCPDF (www.tcpdf.org) This is an electronic reprint of the original article. This reprint may differ from the original in pagination and typographic detail. Author(s): Title: Kemppinen, Antti

More information

III. Address Department of Physics, Iran University of Science & Technology, Tehran, P.O.Box: 16345, IRAN.

III. Address Department of Physics, Iran University of Science & Technology, Tehran, P.O.Box: 16345, IRAN. Curriculum Vitae I. Personal Last Name: Namiranian First Name: Afshin Date of Birth: 04.10.1969 (12/Mehr/1348) Place of birth: Tehran, IRAN Nationality: Iranian Marital status: Married, having two children

More information

Microwaves for quantum simulation in superconducting circuits and semiconductor quantum dots

Microwaves for quantum simulation in superconducting circuits and semiconductor quantum dots Microwaves for quantum simulation in superconducting circuits and semiconductor quantum dots Christopher Eichler - 29.01. 2016 ScaleQIT Conference, Delft In collaboration with: C. Lang, J. Mlynek, Y. Salathe,

More information

Charge spectrometry with a strongly coupled superconducting single-electron transistor

Charge spectrometry with a strongly coupled superconducting single-electron transistor PHYSICAL REVIEW B, VOLUME 64, 245116 Charge spectrometry with a strongly coupled superconducting single-electron transistor C. P. Heij, P. Hadley, and J. E. Mooij Applied Physics and Delft Institute of

More information

SUPPLEMENTARY INFORMATION

SUPPLEMENTARY INFORMATION Collapse of superconductivity in a hybrid tin graphene Josephson junction array by Zheng Han et al. SUPPLEMENTARY INFORMATION 1. Determination of the electronic mobility of graphene. 1.a extraction from

More information

Qubits: Supraleitende Quantenschaltungen. (i) Grundlagen und Messung

Qubits: Supraleitende Quantenschaltungen. (i) Grundlagen und Messung Braunschweiger Supraleiter-Seminar Seminar Qubits: Supraleitende Quantenschaltungen (i) Grundlagen und Messung Jens Könemann, Bundesallee 100, 38116 Braunschweig Q Φ 26. Mai 0/ 16 Braunschweiger Supraleiter-Seminar

More information

Circuit Quantum Electrodynamics. Mark David Jenkins Martes cúantico, February 25th, 2014

Circuit 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 information

A Radio For Hidden Photon Dark Matter

A Radio For Hidden Photon Dark Matter A Radio For Hidden Photon Dark Matter Saptarshi Chaudhuri Stanford University LTD-16 July 22, 2015 Co-Authors: Kent Irwin, Peter Graham, Harvey Moseley, Betty Young, Dale Li, Hsiao-Mei Cho, Surjeet Rajendran,

More information

R. McDermott Publications

R. McDermott Publications R. McDermott Publications 1. R. McDermott, M. G. Vavilov, B. L. T. Plourde, F. K. Wilhelm, P. J. Liebermann, O. A. Mukhanov, and T. A. Ohki, Quantum Classical Interface Based on Single Flux Quantum Digital

More information

dc-squid current sensors for the readout of high-resolution Metallic Magnetic Calorimeters J. Beyer for MetroBeta consortium

dc-squid current sensors for the readout of high-resolution Metallic Magnetic Calorimeters J. Beyer for MetroBeta consortium dc-squid current sensors for the readout of high-resolution Metallic Magnetic Calorimeters J. Beyer for MetroBeta consortium IWSSD AIST Tsukuba Nov 2016 The unit of activity - Bq - of b-emitters MMCs /SQUIDs

More information

Superconductivity in pictures

Superconductivity in pictures Superconductivity in pictures Alexey Bezryadin Department of Physics University of Illinois at Urbana-Champaign Superconductivity observation Electrical resistance of some metals drops to zero below a

More information

AS mentioned in [1], the drift of a levitated/suspended body

AS mentioned in [1], the drift of a levitated/suspended body IEEE TRANSACTIONS ON APPLIED SUPERCONDUCTIVITY, VOL. 17, NO. 3, SEPTEMBER 2007 3803 Drift of Levitated/Suspended Body in High-T c Superconducting Levitation Systems Under Vibration Part II: Drift Velocity

More information

in this web service Cambridge University Press

in this web service Cambridge University Press BROWNIAN RATCHETS Illustrating the development of Brownian ratchets, from their foundations, to their role in the description of life at the molecular scale and in the design of artificial nano-machinery,

More information

Free Electron Laser. Project report: Synchrotron radiation. Sadaf Jamil Rana

Free Electron Laser. Project report: Synchrotron radiation. Sadaf Jamil Rana Free Electron Laser Project report: Synchrotron radiation By Sadaf Jamil Rana History of Free-Electron Laser (FEL) The FEL is the result of many years of theoretical and experimental work on the generation

More information

Dispersive Readout, Rabi- and Ramsey-Measurements for Superconducting Qubits

Dispersive Readout, Rabi- and Ramsey-Measurements for Superconducting Qubits Dispersive Readout, Rabi- and Ramsey-Measurements for Superconducting Qubits QIP II (FS 2018) Student presentation by Can Knaut Can Knaut 12.03.2018 1 Agenda I. Cavity Quantum Electrodynamics and the Jaynes

More information

Superconducting Quantum Interference Devices for Current Sensing and Thermometry in the Millikelvin Range

Superconducting Quantum Interference Devices for Current Sensing and Thermometry in the Millikelvin Range Cryoconference 2010 Superconducting Quantum Interference Devices for Current Sensing and Thermometry in the Millikelvin Range J.-H. Storm, J. Beyer, D.Drung,Th.Schurig Physikalisch-Technische Bundesanstalt

More information

A Superconducting Quantum Simulator for Topological Order and the Toric Code. Michael J. Hartmann Heriot-Watt University, Edinburgh qlightcrete 2016

A Superconducting Quantum Simulator for Topological Order and the Toric Code. Michael J. Hartmann Heriot-Watt University, Edinburgh qlightcrete 2016 A Superconducting Quantum Simulator for Topological Order and the Toric Code Michael J. Hartmann Heriot-Watt University, Edinburgh qlightcrete 2016 Topological Order (in 2D) A 2-dimensional physical system

More information

CIRCUIT QUANTUM ELECTRODYNAMICS WITH ELECTRONS ON HELIUM

CIRCUIT 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