INTRIQ. Coherent Manipulation of single nuclear spin

Size: px
Start display at page:

Download "INTRIQ. Coherent Manipulation of single nuclear spin"

Transcription

1 INTRIQ Coherent Manipulation of single nuclear spin Clément Godfrin Eva Dupont Ferrier Michel Pioro-Ladrière K. Ferhat (Inst. Néel) R. Ballou (Inst. Néel) M. Ruben (KIT) W. Wernsdorfer (KIT) F. Balestro (Inst. Néel) INTRIQ 18 Bromont 1

2 Introduction Qubit Superconducting circuits Nature 453, 131 Quantum dots + 1/ NV center Nature 491, 46 Nature 4, 766 1/ PRL 9, P in silicon Nature 489, 541 INTRIQ 18 Bromont

3 Introduction Qudit + 3/ + 1/ - Fundamental investigation (Bell inequality, Chaos dynamics ) - Quantum information (error correction, simulation, algorithm, cryptography ) 1/ 3/ INTRIQ 18 Bromont 3

4 Conductance (ns) Introduction Molecular magnet Terbium electronic spin Terbium nuclear spin +6 or 6 Terbium double-decker (TbPc ) transistor GHz 3.13 GHz.45 GHz Conductance value Direct read-out Conductance jump position Indirect read-out 1 4 Time Godfrin et al ACS Nano Vincent et al Nature INTRIQ 18 Bromont 4

5 Outline Two-level coherent manipulation Qudit to probe Berry s phase Quantum gate phase INTRIQ 18 Bromont 5

6 Two-level coherent manipulation + 3/ Qubit + 1/ 1/ 3/ INTRIQ 18 Bromont 6

7 Qubit Pulse Energy : E Population : α β Phase : ρ Coupling : g Amplitude : A Frequency : f Length : τ Phase : Φ E 1 Ψ = α + βe iρ 1 P = A sin ( π f τ + Φ) INTRIQ 18 Bromont 7

8 Qubit State representation: Bloch Sphere Ω y 1 State dynamic: Hamiltonian Ω x = g A cos(φ) μ N /h Ω y = g A sin(φ) μ N /h δ z = f - E/h δ z Ψ = cos(θ/) + sin(θ/) e iρ 1 Ω x H = h δ z Ω x +iω y Ω x iω y δ z Ψ τ = e ihτ/h Ψ Pulse Energy : E Population : α β Phase : ρ Coupling : g Amplitude : A Frequency : f Length : τ Phase : Φ What we measure What we tune INTRIQ 18 Bromont 8

9 Nuclear Qubit spin dynamic Pulse Ψ = cos(θ/) + sin(θ/) e iρ 1 1 (ns) (ns) INTRIQ 18 Bromont 9

10 Visibility Visibility Visibility Visibility Visibility Visibility Nuclear spin dynamic + 3/ T 1 = 34 s T =.6 ms 4 τ (ns) Frequency (GHz) + 1/ 1 1 T 1 = 18 s.5.5 T = 1.6 ms T 1 = 34 s T =.4 ms 1/ 3/ Godfrin et al PRL τ (ns) 4 τ (ns) Frequency (GHz) Frequency (GHz) INTRIQ 18 Bromont 1

11 Outline Two-level coherent manipulation Qudit to probe Berry s phase Quantum gate phase INTRIQ 18 Bromont 11

12 Berry s phase Geometric phase accumulation : 1 ) Pulse π with phase α = ) Pulse π with phase α = π + Ω/ 1 1 e iω 1 Ω / INTRIQ 18 Bromont 1

13 Berry s phase Geometric phase accumulation : 1 1 ) Pulse π with α = ) Pulse π with α = π + Ω/ 1 e iω 1 Ω / Phase measurement : Interferometer π, π, α π/, Ω π/, Φ P= cos ( Φ+ α ) Φ INTRIQ 18 Bromont 13

14 Berry s phase π α π π π Φ π, π, α π/, π/, Φ P= cos ( Φ+ α ) INTRIQ 18 Bromont 14

15 Berry s phase α π Φ α π π π Φ π, πτ, π, α πτ, Φ P = cos ( α + Φ ) INTRIQ 18 Bromont 15

16 Berry s phase α 1 π α 3 α 3 π πτ, π, π,α 3 π Τ, P = cos ( α 1 + α 3 ) π π α π, π,α 1 INTRIQ 18 Bromont 16

17 Berry s phase π, π, α +1 π, π, α 3 π, π, α πτ, π Τ, 1 1 π πτ, πτ, Φ 3 π πτ, π Τ, Φ 3 π π, π, α 1 α π α π α 3 π π π π π π π Φ Φ α 1 Godfrin et al, NPJ quant. inf (18) INTRIQ 18 Bromont 17

18 Outline Two-level coherent manipulation Qudit to probe Berry s phase Quantum gate phase INTRIQ 18 Bromont 18

19 iswap Gate 3/ A B 1/ A 1 B 1/ 1 A B 3/ 1 A 1 B U iswap = 1 i i 1 INTRIQ 18 Bromont 19

20 Visibility iswap Gate i ππ 1 1 i π π 3π INTRIQ 18 Bromont

21 Measure iswap phase First measurement: τ = π Create paths +3 π π/ +1 π/ τ Second measurement: τ = 3π 1 3 Godfrin et al, NPJ quant. inf (18) INTRIQ 18 Bromont 1

22 Conclusion Full coherent control of a 4-level single nuclear spin Qudit interferometry Suitable basic block for quantum computing Quantum phase measurement Fundamental physic Quantum computing Multi-level resonance Thank you for your attention Implementation of a Grover s algorithm INTRIQ 18 Bromont

arxiv: v2 [quant-ph] 28 Nov 2017

arxiv: v2 [quant-ph] 28 Nov 2017 Operating Quantum States in Single Magnetic Molecules: Implementation of Grover s Quantum Algorithm arxiv:1710.11229v2 [quant-ph] 28 ov 2017 C. Godfrin, 1, 2 A. Ferhat, 1, 2 R. Ballou, 1 S. Klyatskaya,

More information

Semiconductors: Applications in spintronics and quantum computation. Tatiana G. Rappoport Advanced Summer School Cinvestav 2005

Semiconductors: Applications in spintronics and quantum computation. Tatiana G. Rappoport Advanced Summer School Cinvestav 2005 Semiconductors: Applications in spintronics and quantum computation Advanced Summer School 1 I. Background II. Spintronics Spin generation (magnetic semiconductors) Spin detection III. Spintronics - electron

More information

Towards quantum metrology with N00N states enabled by ensemble-cavity interaction. Massachusetts Institute of Technology

Towards quantum metrology with N00N states enabled by ensemble-cavity interaction. Massachusetts Institute of Technology Towards quantum metrology with N00N states enabled by ensemble-cavity interaction Hao Zhang Monika Schleier-Smith Robert McConnell Jiazhong Hu Vladan Vuletic Massachusetts Institute of Technology MIT-Harvard

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

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

Problem Set # 8 Solutions

Problem Set # 8 Solutions Id: hw.tex,v 1.4 009/0/09 04:31:40 ike Exp 1 MIT.111/8.411/6.898/18.435 Quantum Information Science I Fall, 010 Sam Ocko November 15, 010 Problem Set # 8 Solutions 1. (a) The eigenvectors of S 1 S are

More information

Experimental Realization of Shor s Quantum Factoring Algorithm

Experimental Realization of Shor s Quantum Factoring Algorithm Experimental Realization of Shor s Quantum Factoring Algorithm M. Steffen1,2,3, L.M.K. Vandersypen1,2, G. Breyta1, C.S. Yannoni1, M. Sherwood1, I.L.Chuang1,3 1 IBM Almaden Research Center, San Jose, CA

More information

Superconducting Qubits Lecture 4

Superconducting Qubits Lecture 4 Superconducting Qubits Lecture 4 Non-Resonant Coupling for Qubit Readout A. Blais, R.-S. Huang, A. Wallraff, S. M. Girvin, and R. J. Schoelkopf, PRA 69, 062320 (2004) Measurement Technique Dispersive Shift

More information

Quantum Optics and Quantum Informatics FKA173

Quantum Optics and Quantum Informatics FKA173 Quantum Optics and Quantum Informatics FKA173 Date and time: Tuesday, 7 October 015, 08:30-1:30. Examiners: Jonas Bylander (070-53 44 39) and Thilo Bauch (0733-66 13 79). Visits around 09:30 and 11:30.

More information

INTRODUCTION TO NMR and NMR QIP

INTRODUCTION TO NMR and NMR QIP Books (NMR): Spin dynamics: basics of nuclear magnetic resonance, M. H. Levitt, Wiley, 2001. The principles of nuclear magnetism, A. Abragam, Oxford, 1961. Principles of magnetic resonance, C. P. Slichter,

More information

Quantum Computation with Neutral Atoms

Quantum Computation with Neutral Atoms Quantum Computation with Neutral Atoms Marianna Safronova Department of Physics and Astronomy Why quantum information? Information is physical! Any processing of information is always performed by physical

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

QUANTUM TECHNOLOGIES: THE SECOND QUANTUM REVOLUTION* Jonathan P. Dowling

QUANTUM 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 information

Single Spin Qubits, Qubit Gates and Qubit Transfer with Quantum Dots

Single Spin Qubits, Qubit Gates and Qubit Transfer with Quantum Dots International School of Physics "Enrico Fermi : Quantum Spintronics and Related Phenomena June 22-23, 2012 Varenna, Italy Single Spin Qubits, Qubit Gates and Qubit Transfer with Quantum Dots Seigo Tarucha

More information

Introduction to Cavity QED: fundamental tests and application to quantum information Serge Haroche July 2004

Introduction to Cavity QED: fundamental tests and application to quantum information Serge Haroche July 2004 Introduction to Cavity QED: fundamental tests and application to quantum information Serge Haroche July 2004 A very active research field: Code information in simple systems (atoms, photons..) and use

More information

MolNanoSpin: Spintronique moléculaire avec des molécules-aimants

MolNanoSpin: Spintronique moléculaire avec des molécules-aimants MolNanoSpin: Spintronique moléculaire avec des molécules-aimants W. Wernsdorfer : Institut Néel T. Mallah : Institut de Chimie Moléculaire et des Matériaux d'orsay P. Mialane : Institut Lavoisier Journées

More information

Exploring 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 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 information

Suppression of the low-frequency decoherence by motion of the Bell-type states Andrey Vasenko

Suppression of the low-frequency decoherence by motion of the Bell-type states Andrey Vasenko Suppression of the low-frequency decoherence by motion of the Bell-type states Andrey Vasenko School of Electronic Engineering, Moscow Institute of Electronics and Mathematics, Higher School of Economics

More information

NANOSCALE SCIENCE & TECHNOLOGY

NANOSCALE SCIENCE & TECHNOLOGY . NANOSCALE SCIENCE & TECHNOLOGY V Two-Level Quantum Systems (Qubits) Lecture notes 5 5. Qubit description Quantum bit (qubit) is an elementary unit of a quantum computer. Similar to classical computers,

More information

Coherence and optical electron spin rotation in a quantum dot. Sophia Economou NRL. L. J. Sham, UCSD R-B Liu, CUHK Duncan Steel + students, U Michigan

Coherence and optical electron spin rotation in a quantum dot. Sophia Economou NRL. L. J. Sham, UCSD R-B Liu, CUHK Duncan Steel + students, U Michigan Coherence and optical electron spin rotation in a quantum dot Sophia Economou Collaborators: NRL L. J. Sham, UCSD R-B Liu, CUHK Duncan Steel + students, U Michigan T. L. Reinecke, Naval Research Lab Outline

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

Two-qubit Gate of Combined Single Spin Rotation and Inter-dot Spin Exchange in a Double Quantum Dot

Two-qubit Gate of Combined Single Spin Rotation and Inter-dot Spin Exchange in a Double Quantum Dot Two-qubit Gate of Combined Single Spin Rotation and Inter-dot Spin Exchange in a Double Quantum Dot R. Brunner 1,2, Y.-S. Shin 1, T. Obata 1,3, M. Pioro-Ladrière 4, T. Kubo 5, K. Yoshida 1, T. Taniyama

More information

Developing Quantum Logic Gates: Spin-Resonance-Transistors

Developing Quantum Logic Gates: Spin-Resonance-Transistors Developing Quantum Logic Gates: Spin-Resonance-Transistors H. W. Jiang (UCLA) SRT: a Field Effect Transistor in which the channel resistance monitors electron spin resonance, and the resonance frequency

More information

Electron spins in nonmagnetic semiconductors

Electron spins in nonmagnetic semiconductors Electron spins in nonmagnetic semiconductors Yuichiro K. Kato Institute of Engineering Innovation, The University of Tokyo Physics of non-interacting spins Optical spin injection and detection Spin manipulation

More information

Short Course in Quantum Information Lecture 8 Physical Implementations

Short 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 information

arxiv: v1 [quant-ph] 11 Nov 2014

arxiv: v1 [quant-ph] 11 Nov 2014 Electric dipoles on the Bloch sphere arxiv:1411.5381v1 [quant-ph] 11 Nov 014 Amar C. Vutha Dept. of Physics & Astronomy, York Univerity, Toronto ON M3J 1P3, Canada email: avutha@yorku.ca Abstract The time

More information

Quantum Control of Qubits

Quantum Control of Qubits Quantum Control of Qubits K. Birgitta Whaley University of California, Berkeley J. Zhang J. Vala S. Sastry M. Mottonen R. desousa Quantum Circuit model input 1> 6> = 1> 0> H S T H S H x x 7 k = 0 e 3 π

More information

Homework 3. 1 Coherent Control [22 pts.] 1.1 State vector vs Bloch vector [8 pts.]

Homework 3. 1 Coherent Control [22 pts.] 1.1 State vector vs Bloch vector [8 pts.] Homework 3 Contact: jangi@ethz.ch Due date: December 5, 2014 Nano Optics, Fall Semester 2014 Photonics Laboratory, ETH Zürich www.photonics.ethz.ch 1 Coherent Control [22 pts.] In the first part of this

More information

Experimental Quantum Computing: A technology overview

Experimental Quantum Computing: A technology overview Experimental Quantum Computing: A technology overview Dr. Suzanne Gildert Condensed Matter Physics Research (Quantum Devices Group) University of Birmingham, UK 15/02/10 Models of quantum computation Implementations

More information

Some Introductory Notes on Quantum Computing

Some Introductory Notes on Quantum Computing Some Introductory Notes on Quantum Computing Markus G. Kuhn http://www.cl.cam.ac.uk/~mgk25/ Computer Laboratory University of Cambridge 2000-04-07 1 Quantum Computing Notation Quantum Computing is best

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

Supplementary information for Quantum delayed-choice experiment with a beam splitter in a quantum superposition

Supplementary information for Quantum delayed-choice experiment with a beam splitter in a quantum superposition Supplementary information for Quantum delayed-choice experiment with a beam splitter in a quantum superposition Shi-Biao Zheng 1, You-Peng Zhong 2, Kai Xu 2, Qi-Jue Wang 2, H. Wang 2, Li-Tuo Shen 1, Chui-Ping

More information

Deterministic Coherent Writing and Control of the Dark Exciton Spin using Short Single Optical Pulses

Deterministic Coherent Writing and Control of the Dark Exciton Spin using Short Single Optical Pulses Deterministic Coherent Writing and Control of the Dark Exciton Spin using Short Single Optical Pulses Ido Schwartz, Dan Cogan, Emma Schmidgall, Liron Gantz, Yaroslav Don and David Gershoni The Physics

More information

Quantum Communication & Computation Using Spin Chains

Quantum Communication & Computation Using Spin Chains Quantum Communication & Computation Using Spin Chains Sougato Bose Institute for Quantum Information, Caltech & UCL, London Quantum Computation Part: S. C. Benjamin & S. Bose, quant-ph/02057 (to appear

More information

C/CS/Phys C191 Amplitude Amplification, Quantum Zeno, Vaidman s bomb 11/10/09 Fall 2009 Lecture 22

C/CS/Phys C191 Amplitude Amplification, Quantum Zeno, Vaidman s bomb 11/10/09 Fall 2009 Lecture 22 C/CS/Phys C191 Amplitude Amplification, Quantum Zeno, Vaidman s bomb 11/10/09 Fall 2009 Lecture 22 1 Readings Kaye et al, Ch 83 Nielsen and Chuang: Ch 63-65 Grover s algorithm and amplitude amplification:

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

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

Synthesizing arbitrary photon states in a superconducting resonator

Synthesizing arbitrary photon states in a superconducting resonator Synthesizing arbitrary photon states in a superconducting resonator Max Hofheinz, Haohua Wang, Markus Ansmann, R. Bialczak, E. Lucero, M. Neeley, A. O Connell, D. Sank, M. Weides, J. Wenner, J.M. Martinis,

More information

Superconducting quantum bits. Péter Makk

Superconducting 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 information

Solid-State Spin Quantum Computers

Solid-State Spin Quantum Computers Solid-State Spin Quantum Computers 1 NV-Centers in Diamond P Donors in Silicon Kane s Computer (1998) P- doped silicon with metal gates Silicon host crystal + 31 P donor atoms + Addressing gates + J- coupling

More information

Spin Coherent Phenomena in Quantum Dots Driven by Magnetic Fields

Spin Coherent Phenomena in Quantum Dots Driven by Magnetic Fields Spin Coherent Phenomena in Quantum Dots Driven by Magnetic Fields Gloria Platero Instituto de Ciencia de Materiales (ICMM), CSIC, Madrid, Spain María Busl (ICMM), Rafael Sánchez,Université de Genève Toulouse,

More information

Quantum Information Processing and Quantum Simulation with Ultracold Alkaline-Earth Atoms in Optical Lattices

Quantum Information Processing and Quantum Simulation with Ultracold Alkaline-Earth Atoms in Optical Lattices Quantum Information Processing and Quantum Simulation with Ultracold Alkaline-Earth Atoms in Optical Lattices Alexey Gorshkov California Institute of Technology Mikhail Lukin, Eugene Demler, Cenke Xu -

More information

Josephson qubits. P. Bertet. SPEC, CEA Saclay (France), Quantronics group

Josephson qubits. P. Bertet. SPEC, CEA Saclay (France), Quantronics group Josephson qubits P. Bertet SPEC, CEA Saclay (France), Quantronics group Outline Lecture 1: Basics of superconducting qubits Lecture 2: Qubit readout and circuit quantum electrodynamics Lecture 3: 2-qubit

More information

Quantum computation and quantum information

Quantum computation and quantum information Quantum computation and quantum information Chapter 7 - Physical Realizations - Part 2 First: sign up for the lab! do hand-ins and project! Ch. 7 Physical Realizations Deviate from the book 2 lectures,

More information

INTRODUCTION TO NMR and NMR QIP

INTRODUCTION TO NMR and NMR QIP Books (NMR): Spin dynamics: basics of nuclear magneac resonance, M. H. LeviF, Wiley, 200. The principles of nuclear magneasm, A. Abragam, Oxford, 96. Principles of magneac resonance, C. P. Slichter, Springer,

More information

Itinerant microwave photon detector

Itinerant microwave photon detector Itinerant microwave photon detector Baptiste Royer Arne L. Grimsmo Alexandre Choquette-Poitevin Alexandre Blais November 10, 2017 Intriq meeting, Bromont BR, A.L. Grimsmo, A. Choquette-Poitevin, A. Blais,

More information

Ion trap quantum processor

Ion trap quantum processor Ion trap quantum processor Laser pulses manipulate individual ions row of qubits in a linear Paul trap forms a quantum register Effective ion-ion interaction induced by laser pulses that excite the ion`s

More information

1.0 Introduction to Quantum Systems for Information Technology 1.1 Motivation

1.0 Introduction to Quantum Systems for Information Technology 1.1 Motivation QSIT09.V01 Page 1 1.0 Introduction to Quantum Systems for Information Technology 1.1 Motivation What is quantum mechanics good for? traditional historical perspective: beginning of 20th century: classical

More information

Cavity Quantum Electrodynamics Lecture 2: entanglement engineering with quantum gates

Cavity Quantum Electrodynamics Lecture 2: entanglement engineering with quantum gates DÉPARTEMENT DE PHYSIQUE DE L ÉCOLE NORMALE SUPÉRIEURE LABORATOIRE KASTLER BROSSEL Cavity Quantum Electrodynamics Lecture : entanglement engineering with quantum gates Michel BRUNE Les Houches 003 1 CQED

More information

Mesoscopic field state superpositions in Cavity QED: present status and perspectives

Mesoscopic field state superpositions in Cavity QED: present status and perspectives Mesoscopic field state superpositions in Cavity QED: present status and perspectives Serge Haroche, Ein Bokek, February 21 st 2005 Entangling single atoms with larger and larger fields: an exploration

More information

The Deutsch-Josza Algorithm in NMR

The Deutsch-Josza Algorithm in NMR December 20, 2010 Matteo Biondi, Thomas Hasler Introduction Algorithm presented in 1992 by Deutsch and Josza First implementation in 1998 on NMR system: - Jones, JA; Mosca M; et al. of a quantum algorithm

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

C/CS/Phy191 Problem Set 6 Solutions 3/23/05

C/CS/Phy191 Problem Set 6 Solutions 3/23/05 C/CS/Phy191 Problem Set 6 Solutions 3/3/05 1. Using the standard basis (i.e. 0 and 1, eigenstates of Ŝ z, calculate the eigenvalues and eigenvectors associated with measuring the component of spin along

More information

New schemes for manipulating quantum states using a Kerr cell. Istituto Elettrotecnico Nazionale Galileo Ferraris, Str. delle Cacce 91, I Torino

New schemes for manipulating quantum states using a Kerr cell. Istituto Elettrotecnico Nazionale Galileo Ferraris, Str. delle Cacce 91, I Torino New schemes for manipulating quantum states using a Kerr cell Marco Genovese and C.Novero Istituto Elettrotecnico Nazionale Galileo Ferraris, Str. delle Cacce 91, I-10135 Torino Recently, Quantum Non Demolition

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

Dissipation in Transmon

Dissipation 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 information

Lecture 2, March 2, 2017

Lecture 2, March 2, 2017 Lecture 2, March 2, 2017 Last week: Introduction to topics of lecture Algorithms Physical Systems The development of Quantum Information Science Quantum physics perspective Computer science perspective

More information

Let's Build a Quantum Computer!

Let'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 information

Martes cuántico Zaragoza, 8 th October Atomic and molecular spin qubits. Fernando LUIS Instituto de Ciencia de Materiales de Aragón

Martes cuántico Zaragoza, 8 th October Atomic and molecular spin qubits. Fernando LUIS Instituto de Ciencia de Materiales de Aragón Martes cuántico Zaragoza, 8 th October 2013 Atomic and molecular spin qubits Fernando LUIS Instituto de Ciencia de Materiales de Aragón Outline Quantum information with spins 1 0 Atomic defects in semiconductors

More information

Quantum Optics in Wavelength Scale Structures

Quantum Optics in Wavelength Scale Structures Quantum Optics in Wavelength Scale Structures SFB Summer School Blaubeuren July 2012 J. G. Rarity University of Bristol john.rarity@bristol.ac.uk Confining light: periodic dielectric structures Photonic

More information

Quantum Information Processing with Semiconductor Quantum Dots. slides courtesy of Lieven Vandersypen, TU Delft

Quantum Information Processing with Semiconductor Quantum Dots. slides courtesy of Lieven Vandersypen, TU Delft Quantum Information Processing with Semiconductor Quantum Dots slides courtesy of Lieven Vandersypen, TU Delft Can we access the quantum world at the level of single-particles? in a solid state environment?

More information

2.0 Basic Elements of a Quantum Information Processor. 2.1 Classical information processing The carrier of information

2.0 Basic Elements of a Quantum Information Processor. 2.1 Classical information processing The carrier of information QSIT09.L03 Page 1 2.0 Basic Elements of a Quantum Information Processor 2.1 Classical information processing 2.1.1 The carrier of information - binary representation of information as bits (Binary digits).

More information

400 nm Solid State Qubits (1) Daniel Esteve GROUP. SPEC, CEA-Saclay

400 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 information

Entanglement: concept, measures and open problems

Entanglement: concept, measures and open problems Entanglement: concept, measures and open problems Division of Mathematical Physics Lund University June 2013 Project in Quantum information. Supervisor: Peter Samuelsson Outline 1 Motivation for study

More information

What is possible to do with noisy quantum computers?

What is possible to do with noisy quantum computers? What is possible to do with noisy quantum computers? Decoherence, inaccuracy and errors in Quantum Information Processing Sara Felloni and Giuliano Strini sara.felloni@disco.unimib.it Dipartimento di Informatica

More information

Electron spin coherence exceeding seconds in high-purity silicon

Electron spin coherence exceeding seconds in high-purity silicon Electron spin coherence exceeding seconds in high-purity silicon Alexei M. Tyryshkin, Shinichi Tojo 2, John J. L. Morton 3, H. Riemann 4, N.V. Abrosimov 4, P. Becker 5, H.-J. Pohl 6, Thomas Schenkel 7,

More information

9 Atomic Coherence in Three-Level Atoms

9 Atomic Coherence in Three-Level Atoms 9 Atomic Coherence in Three-Level Atoms 9.1 Coherent trapping - dark states In multi-level systems coherent superpositions between different states (atomic coherence) may lead to dramatic changes of light

More information

Quantum Computing ~ Algorithms. HIO) 0 HIO) 010) = ~(l000) ) ) ))

Quantum Computing ~ Algorithms. HIO) 0 HIO) 010) = ~(l000) ) ) )) Quantum Computing 2. Algorithms C S Vijay and Vishal Gupta Introduction C S Vijay is in the final year of a dual degree program in microelectronics at the Department of Electrical Engineering at lit Mumbai.

More information

Quantum Information NV Centers in Diamond General Introduction. Zlatko Minev & Nate Earnest April 2011

Quantum Information NV Centers in Diamond General Introduction. Zlatko Minev & Nate Earnest April 2011 Quantum Information NV Centers in Diamond General Introduction Zlatko Minev & Nate Earnest April 2011 QIP & QM & NVD Outline Interest in Qubits. Why? Quantum Information Motivation Qubit vs Bit Sqrt(Not)

More information

10.5 Circuit quantum electrodynamics

10.5 Circuit quantum electrodynamics AS-Chap. 10-1 10.5 Circuit quantum electrodynamics AS-Chap. 10-2 Analogy to quantum optics Superconducting quantum circuits (SQC) Nonlinear circuits Qubits, multilevel systems Linear circuits Waveguides,

More information

Problem Set #6 BioE 326B/Rad 226B

Problem Set #6 BioE 326B/Rad 226B . Chemical shift anisotropy Problem Set #6 BioE 26B/Rad 226B 2. Scalar relaxation of the 2 nd kind. 0 imaging 4. NMRD curves Chemical Shift Anisotropy The Hamiltonian a single-spin system in a magnetic

More information

IBM Systems for Cognitive Solutions

IBM Systems for Cognitive Solutions IBM Q Quantum Computing IBM Systems for Cognitive Solutions Ehningen 12 th of July 2017 Albert Frisch, PhD - albert.frisch@de.ibm.com 2017 IBM 1 st wave of Quantum Revolution lasers atomic clocks GPS sensors

More information

Factoring 15 with NMR spectroscopy. Josefine Enkner, Felix Helmrich

Factoring 15 with NMR spectroscopy. Josefine Enkner, Felix Helmrich Factoring 15 with NMR spectroscopy Josefine Enkner, Felix Helmrich Josefine Enkner, Felix Helmrich April 23, 2018 1 Introduction: What awaits you in this talk Recap Shor s Algorithm NMR Magnetic Nuclear

More information

Driving Qubit Transitions in J-C Hamiltonian

Driving Qubit Transitions in J-C Hamiltonian Qubit Control Driving Qubit Transitions in J-C Hamiltonian Hamiltonian for microwave drive Unitary transform with and Results in dispersive approximation up to 2 nd order in g Drive induces Rabi oscillations

More information

Image courtesy of Keith Schwab http://www.lbl.gov/science-articles/archive/afrd Articles/Archive/AFRD-quantum-logic.html http://www.wmi.badw.de/sfb631/tps/dqd2.gif http://qist.lanl.gov/qcomp_map.shtml

More information

Physikalische Chemie IV (Magnetische Resonanz) HS Solution Set 2. Hand out: Hand in:

Physikalische Chemie IV (Magnetische Resonanz) HS Solution Set 2. Hand out: Hand in: Solution Set Hand out:.. Hand in:.. Repetition. The magnetization moves adiabatically during the application of an r.f. pulse if it is always aligned along the effective field axis. This behaviour is observed

More information

Quantum entanglement and its detection with few measurements

Quantum entanglement and its detection with few measurements Quantum entanglement and its detection with few measurements Géza Tóth ICFO, Barcelona Universidad Complutense, 21 November 2007 1 / 32 Outline 1 Introduction 2 Bipartite quantum entanglement 3 Many-body

More information

Coherent manipulation of atomic wavefunctions in an optical lattice. V. V. Ivanov & A. Alberti, M. Schioppo, G. Ferrari and G. M.

Coherent manipulation of atomic wavefunctions in an optical lattice. V. V. Ivanov & A. Alberti, M. Schioppo, G. Ferrari and G. M. Coherent manipulation of atomic wavefunctions in an optical lattice V. V. Ivanov & A. Alberti, M. Schioppo, G. Ferrari and G. M. Tino Group Andrea Alberti Marco Schioppo Guglielmo M. Tino me Gabriele Ferarri

More information

Lecture 11, May 11, 2017

Lecture 11, May 11, 2017 Lecture 11, May 11, 2017 This week: Atomic Ions for QIP Ion Traps Vibrational modes Preparation of initial states Read-Out Single-Ion Gates Two-Ion Gates Introductory Review Articles: D. Leibfried, R.

More information

quantum mechanics is a hugely successful theory... QSIT08.V01 Page 1

quantum mechanics is a hugely successful theory... QSIT08.V01 Page 1 1.0 Introduction to Quantum Systems for Information Technology 1.1 Motivation What is quantum mechanics good for? traditional historical perspective: beginning of 20th century: classical physics fails

More information

Control of quantum two-level systems

Control of quantum two-level systems Control of quantum two-level sstems R. Gross, A. Mar & F. Deppe, Walther-Meißner-Institut (00-03) 0.3 Control of quantum two-level sstems.. General concept AS-Chap. 0 - How to control a qubit? Does the

More information

Lecture 8, April 12, 2017

Lecture 8, April 12, 2017 Lecture 8, April 12, 2017 This week (part 2): Semiconductor quantum dots for QIP Introduction to QDs Single spins for qubits Initialization Read-Out Single qubit gates Book on basics: Thomas Ihn, Semiconductor

More information

Cavity QED with Rydberg Atoms Serge Haroche, Collège de France & Ecole Normale Supérieure, Paris

Cavity QED with Rydberg Atoms Serge Haroche, Collège de France & Ecole Normale Supérieure, Paris Cavity QED with Rydberg Atoms Serge Haroche, Collège de France & Ecole Normale Supérieure, Paris A three lecture course Goal of lectures Manipulating states of simple quantum systems has become an important

More information

Retract. Press down D RG MG LG S. Recess. I-V Converter VNA. Gate ADC. DC Bias. 20 mk. Amplifier. Attenuators. 0.

Retract. Press down D RG MG LG S. Recess. I-V Converter VNA. Gate ADC. DC Bias. 20 mk. Amplifier. Attenuators. 0. a Press down b Retract D RG S c d 2 µm Recess 2 µm.5 µm Supplementary Figure 1 CNT mechanical transfer (a) Schematics showing steps of pressing down and retracting during the transfer of the CNT from the

More information

Optically-controlled controlled quantum dot spins for quantum computers

Optically-controlled controlled quantum dot spins for quantum computers Optically-controlled controlled quantum dot spins for quantum computers David Press Yamamoto Group Applied Physics Department Ph.D. Oral Examination April 28, 2010 1 What could a Quantum Computer do? Simulating

More information

example: e.g. electron spin in a field: on the Bloch sphere: this is a rotation around the equator with Larmor precession frequency ω

example: e.g. electron spin in a field: on the Bloch sphere: this is a rotation around the equator with Larmor precession frequency ω Dynamics of a Quantum System: QM postulate: The time evolution of a state ψ> of a closed quantum system is described by the Schrödinger equation where H is the hermitian operator known as the Hamiltonian

More information

Felix Kleißler 1,*, Andrii Lazariev 1, and Silvia Arroyo-Camejo 1,** 1 Accelerated driving field frames

Felix Kleißler 1,*, Andrii Lazariev 1, and Silvia Arroyo-Camejo 1,** 1 Accelerated driving field frames Supplementary Information: Universal, high-fidelity quantum gates based on superadiabatic, geometric phases on a solid-state spin-qubit at room temperature Felix Kleißler 1,*, Andrii Lazariev 1, and Silvia

More information

From trapped ions to macroscopic quantum systems

From trapped ions to macroscopic quantum systems 7th International Summer School of the SFB/TRR21 "Control of Quantum Correlations in Tailored Matter 21-13 July 2014 From trapped ions to macroscopic quantum systems Peter Rabl Yesterday... Trapped ions:

More information

Quantum Information Processing with Semiconductor Quantum Dots

Quantum Information Processing with Semiconductor Quantum Dots Quantum Information Processing with Semiconductor Quantum Dots slides courtesy of Lieven Vandersypen, TU Delft Can we access the quantum world at the level of single-particles? in a solid state environment?

More information

Lecture 9 Superconducting qubits Ref: Clarke and Wilhelm, Nature 453, 1031 (2008).

Lecture 9 Superconducting qubits Ref: Clarke and Wilhelm, Nature 453, 1031 (2008). Lecture 9 Superconducting qubits Ref: Clarke and Wilhelm, Nature 453, 1031 (2008). Newcomer in the quantum computation area ( 2000, following experimental demonstration of coherence in charge + flux qubits).

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

*WILEY- Quantum Computing. Joachim Stolze and Dieter Suter. A Short Course from Theory to Experiment. WILEY-VCH Verlag GmbH & Co.

*WILEY- Quantum Computing. Joachim Stolze and Dieter Suter. A Short Course from Theory to Experiment. WILEY-VCH Verlag GmbH & Co. Joachim Stolze and Dieter Suter Quantum Computing A Short Course from Theory to Experiment Second, Updated and Enlarged Edition *WILEY- VCH WILEY-VCH Verlag GmbH & Co. KGaA Contents Preface XIII 1 Introduction

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

Quantum computation with superconducting qubits

Quantum 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 information

Introduction to Quantum Mechanics of Superconducting Electrical Circuits

Introduction to Quantum Mechanics of Superconducting Electrical Circuits Introduction to Quantum Mechanics of Superconducting lectrical Circuits What is superconductivity? What is a osephson junction? What is a Cooper Pair Box Qubit? Quantum Modes of Superconducting Transmission

More information

Circuit QED: A promising advance towards quantum computing

Circuit 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 information

P 3/2 P 1/2 F = -1.5 F S 1/2. n=3. n=3. n=0. optical dipole force is state dependent. n=0

P 3/2 P 1/2 F = -1.5 F S 1/2. n=3. n=3. n=0. optical dipole force is state dependent. n=0 (two-qubit gate): tools: optical dipole force P 3/2 P 1/2 F = -1.5 F n=3 n=3 n=0 S 1/2 n=0 optical dipole force is state dependent tools: optical dipole force (e.g two qubits) ω 2 k1 d ω 1 optical dipole

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

Physics is becoming too difficult for physicists. David Hilbert (mathematician)

Physics is becoming too difficult for physicists. David Hilbert (mathematician) Physics is becoming too difficult for physicists. David Hilbert (mathematician) Simple Harmonic Oscillator Credit: R. Nave (HyperPhysics) Particle 2 X 2-Particle wave functions 2 Particles, each moving

More information

Single Microwave-Photon Detector based on Superconducting Quantum Circuits

Single Microwave-Photon Detector based on Superconducting Quantum Circuits 17 th International Workshop on Low Temperature Detectors 19/July/2017 Single Microwave-Photon Detector based on Superconducting Quantum Circuits Kunihiro Inomata Advanced Industrial Science and Technology

More information