tems, these solid-state qubits couple to a complex environment which often ...
strong interactions which make solid-state quantum systems attractive can
typically.
Feb 25, 2009 - focus on states that are eigenstates of tenor products of ..... 15: Cluster state stabilizers consistent with the indicated braiding of defects and ...
2. Prof. Dr. Hans-Peter Abicht, Martin-Luther-Universität Halle-Wittenberg, Halle, Germany. 3. ...... D. Hesse, H. Bethge, J. Crystal Growth, 52, 875 (1981). 119.
decay of the so-called free induction signal (Schlichter,. 1992). The free .... the electron transfer takes place via tunneling, the char- ...... Mz(â) = eâÏv2/a2 . (59).
vertical-cavity surface emitting lasers [8] or microsphere lasers [9]. However, the usual ...... in very good approximation as a âthresholdlessâ laser. Thresholdless ...
The basic ideas of the CEF theory (put forward by Bethe in 1929) - the existence of the ...... Dedicated to Hans Albert Bethe, the pioneer of the crystal-field theory,.
Nov 7, 2003 - Abstract. Geometric quantum computation is a scheme to use non-Abelian holonomic operations rather than the conventional dynamic ...
provides a natural capacitive coupling to a solid state charge qubit, represented e.g. by a Josephson junction[4] or a charged double quantum dot[14]. Instead of ...
junction and capacitive coupling, which are already vi- able with current technology. II. JOSEPHSON CHARGE QUBITS. A âJosephson (charge) qubitâ [11, 12] ...
with an equally coupled detector. Keywords: quantum measurement, qubit, quantum noise, quantum feedback, entanglement. 1. INTRODUCTION.
Feb 1, 2008 - a measurement, the system becomes open, and the Schrödinger equation .... case of Schrödinger's cat, one history would include a live cat and ...
Classical and quantum computers both represent informa- tion in the form of ..... for physicists, another class of algorithms looks much more promising: Along the ...
2Department of Physics and Astronomy, University of British Columbia, 6224 Agricultural Road, Vancouver, Canada. 3 Institute of .... ratio Jc/JLR,1 and of the product ÏgateJc, where Ïgate is the time ... lated vs interacting molecules or metallic v
Pauling [1] wrote in his renowned book : `it is now recognized that the .... interaction in hydrogen bonds is still regarded as essentially electrostatic in nature, but.
Coulomb blockade in Quantum Dots. Additional reading complementing the
lecture notes.1. Version: 23/04/2007 - Andreas Fuhrer/Carina Fasth. In the
resonant ...
rare-earth-ion-doped crystals is theoretically analysed taking into account signal-to-noise ratio at the output of the memory device. The crystal. 143Nd3+:Y7LiF4 ...
Sep 27, 2013 - systems where electron spins are used for readout and control [1â10] .... The system is a prototype single node of a larger register, coupled by the electron spins [8, ...... [13] Bell, J. S. On the Einstein Podolsky Rosen Paradox.
Sep 17, 2012 - Yu-Oh proof of quantum contextuality and notations. Explicitly, the .... Science 276, 2012 (1997). 18. Jelezko, F. ... Maze, J. R. et al. Nanoscale ...
designs is to use a gas switch such as a thyratron, ignitron or spark gap. However these devices have limited lifetime, high cost, low repetition rate and high ...
EE 5340 – Semiconductor Device Theory. Contact: Professor ... (A copy of the
Solution Manual is on reserve in the Science and Engineering. Library.) Sample
...
28. The Electrochemical Society Interface • Fall 2006. Nanostructured Solid-State
. Electrochemical Systems. Applications and Challenges by Sangtae Kim.
3 In fact Shor's algorithm strikes the strong Church-Turing thesis, which ..... Assume we have an unsorted list and want to know the largest element, the mean,.
dramatically from the conventional, equal pulse spacing of a Carr-Purcell-Meiboom-Gill (CPMG) multiple spin echo sequence. The UDD sequence was derived ...
form useful in quantum factoring, IBM Research Re- .... Keyes R W and Landauer R 1970 IBM J. Res. ... Knuth D E 1981 The
1 Decoherence of a Josephson Quantum Bit during its Free Evolution: The Quantronium. 1 ... 11 Josephson junction Materials Research Using Phase Qubits. 86.
Quantum Computing in Solid State Systems With 170 Figures
Edited by:
B. Ruggiero Istituto di Cibernetica "E. Caianiello " CNR Italy
P. Delsing Chalmers University of Technology Sweden
C. Granata Istituto di Cibernetica "E. Caianiello " CNR Italy
Y. Pashkin RIKEN/NEC Tsukuba, Japan
P. Silvestrini Seconda Universita di Napoli Italy Under auspices of Regione Campania
Springer
Contents
Preface List of Corresponding Authors 1 Decoherence of a Josephson Quantum Bit during its Free Evolution: The Quantronium 1.1 Introduction 1.2 The Quantronium Circuit and its Decoherence Sources 1.2.1 Principle 1.2.2 Experimental implementation 1.2.3 Decoherence sources 1.2.4 Theoretical relaxation and decoherence rates 1.3 Experimental Characterization of Decoherence During - Free Evolution 1.3.1 Relaxation Time (T1) measurement 1.3.2 Coherence time (T2 and TE) measurements 1.3.3 Discussion 1.4 Conclusion
3 Coupling and Dephasing in Josephson Charge-Phase Qubit with Radio Frequency Readout 3.1 Introduction 3.2 Qubit Parameters and the Model
19 19 20
Contents 3.3 3.4 3.5
Effect of Finite Inductance of the Ring Qubit Dephasing Conclusion
22 24 25
The Josephson Bifurcation Amplifier - for Quantum Measurements 4.1 Introduction 4.2 Theory 4.3 Devices and Setup 4.4 Results 4.5 Conclusion
28 28 29 31 32 36
Current-Controlled coupling - of superconducting charge qubits 5.1 Introduction 5.2 Current-Controlled Coupling of Two Qubits 5.3 Maximum Coupling Strength 5.4 Operating the System 5.5 Coupling via Measurement Junctions 5.6 Extension to Arbitrary Number of Qubits
38 38 38 40 41 41 43
Direct Measurements of Tunable Josephson Plasma Resonance in the L-Set 6.1 Introduction 6.2 The L-Set Circuit 6.3 Plasma Oscillations in L-Set 6.4 Simulation Scheme 6.5 Experiment 6.6 Results and Discussion 6.6.1 Charge detection 6.6.2 Harmonic Oscillations 6.6.3 Switching and nonlinear oscillations
45 45 46 47 48 49 49 49 50 52
Time Domain Analysis of Dynamical Switching in a Josephson Junction 7.1 Introduction 7.2 The Experiment 7.3 The Model 7.4 Results and Discussion 7.5 Summary
54 54 56 57 59 62
Cooper Pair Transistor in a Tunable Environment 8.1 Introduction 8.2 Sample Fabrication and Measurement Techniques 8.3 Squid Arrays Characterization 8.4 Measurement of the CPT
10 Dynamics of a Qubit Coupled to a Harmonic Oscillator 10.1 Introduction 10.2 The System 10.3 Sample Fabrication, Setup and Characterization 10.4 Coupled Dynamics 10.4.1 Spectroscopy 10.4.2 Dynamics 10.5 Using the Coupled Dynamics to Probe the System 10.5.1 Measuring the Oscillator Temperature 10.5.2 Probing the Qubit State 10.6 Conclusion
76 76 77 78 79 79 81 82 82 82 84
11 Josephson junction Materials Research Using Phase Qubits 11.1 Introduction 11.2 Josephson Phase Qubits 11.3 Junction Fabrication Processes 11.3.1 The "Ion Mill Junction Process" 11.3.2 The "Standard Trilayer Junction Process" 11.3.3 The "Evaporated Trilayer Junction Process" 11.4 Josephson Junction and Qubit Characterization 11.4.2 Measurements of Qubit Spectroscopy 11.5 Concluding remarks
86 86 87 88 89 89 89 91 92 93
12 Energy level spectroscopy of a bound vortex-antivortex pair
95
13 Adiabatic Quantum Computation with Flux Qbits 13.1 Introduction 13.2 Adiabatic Quantum Computation 13.3 AQC with an Array of Flux Qbits 13.4 Vertical Two Josephson Junctions Interferometer 13.5 Conclusions
103 103 104 105 106 109
14 Anomalous Thermal Escape in Josephson Systems Perturbed by Microwaves 14.1 Introduction 14.2 Theory 14.3 Experiments and Simulations 14.4 Conclusions
111 111 113 114 117
15 Realization and Characterization of a Squid Flux Qubit with a Direct Readout Scheme 120 15.1 Introduction 120 15.2 The RF Squid Qubit 120 15.3 The Double Squid Qubit 122 15.4 Gradiometric Configuration 122 15.5 Direct Readout Scheme 123
16 A Critique of the Two Level Approximation 16.1 Introduction 16.2 System and Environment 16.3 Density Matrix Solutions 16.3.1 The effect of spectral distribution on Decoherence 16.3.2 The effect of number of levels on Decoherence 16.4 The Photon Number Calculations 16.5 Conclusions and Discussions
127 127 128 129 129 132 132 135
17 Josephson Junction Qubits with Symmetrized Couplings to a Resonant LC Bus 17.1 Introduction 17.2 Josephson Junction Triangular Prism Qubits 17.3 Coupling the Resonant LC Bus to the Qubits 17.3.1 Logical Qubits for a Decoherence Free Subspace 17.3.2 M0lmer-S0rensen Gate 17.4 Circulating Current Patterns for the Qubit States 17.4.1 Initializing the Qubits and the Effect of Critical Current and Geometric Defects 17.4.2 Connecting Buses into a Network 17.5 Conclusions
137 137 138 139 140 140 142
18 Spatial Bose-Einstein Condensation in Josephson Junction Arrays 18.1 Introduction 18.2 Preliminary Studies for Engineering Graph-Shaped Networks 18.3 Fabrication of Comb-Shaped JJNs 18.4 Measurements 18.5 Experimental Implications
147 147 149 150 152 152
19 Cooper Pair Shuttle: A Josephson Quantum Kicked Rotator 19.1 Introduction and System Description 19.2 Classical and Quantum Dynamics 19.3 Fidelity 19.4 The Effect of Noise 19.5 Fidelity Measurement
154 154 155 158 158 161
20 Size Dependence of the Superconductor-Insulator Transition in Josephson Junction Arrays 20.1 Introduction 20.2 Finite-size Effect in the 2DXY Model 20.3 The Effective Hamiltonian 20.4 DMRG 20.5 Spontaneous Symmetry Breaking 20.6 BKT as a SSB 20.7 Conclusions
163 163 164 164 166 166 167 170
143 144 145
Contents
xi
21 Monte Carlo Method for a Superconducting Cooper-Pair-Box Charge Qubit Measured by a Single-Electron Transfer 21.1 Introduction 21.2 Model Hamiltonian 21.3 Measurement records and conditional density matrix 21.4 Stochastic master equation 21.5 Connection to "Partially" Reduced Density Matrix 21.6 Conclusion
171 171 172 173 174 176 178
22 On the Conversion of Ultracold Fermionic Atoms to Bosonic Molecules via Feshbach Resonances 22.1 Introduction 22.2 Initial State Preparation 22.3 General symmetry arguments 22.4 Explaining the Experimental Limited Transfer Efficiency 22.5 Transfer efficiencies above 0.5 22.6 Summary
180 180 181 181 183 185 186
23 Revealing Anisotropy in a Paul Trap Through Berry Phase 23.1 Introduction 23.2 Physical System and Hamiltonian Model 23.3 Calculation of Berry Phase 23.4 Anisotropy vs. Berry Phase Effects 23.5 Conclusions
25 Linear-response conductance of the normal conducting single-electron pump 25.1 Introduction 25.2 Motivation for the Measurements 25.3 Sequential Model 25.4 Experimental Details and Results 25.5 Discussions 25.6 Summary
202 202 203 205 206 208 210
26 Transmission Eigenvalues' Statistics for a Quantum Point Contact 26.1 Introduction 26.2 Model of QPC with Impurities 26.3 Scattering Matrix Elements and Correction to the Conductance 26.4 Distribution function
212 212 213 215 216
Contents 26.4.1 One open channel 26.4.2 Circuit theory 26.5 Conclusions
216 217 218
27 Creating Entangled States between SQUID Rings and Electromagnetic Fields 27.1 Introduction 27.2 Background 27.3 The Hamiltonian's Spectrum 27.4 Rapid Passage 27.5 Towards the Adiabatic Limit 27.6 The Effect of Dissipation 27.7 Conclusions
219 219 220 221 223 223 223 225
28 Frequency Down Conversion and Entanglement 28.1 Introduction 28.2 Entanglement of em Fields via a SQUID Ring 28.3 Entanglement of field modes at similar frequencies 28.3.1 Entanglement of dissimilar input/output frequency field modes 28.4 Energy down Conversion at Higher Frequency Ratios 28.4.1 Factor 5 down conversion 28.5 Larger frequency ratio (factor of 10) down conversion 28.6 Conclusions
228 228 230 231 231 234 234 236 236
29 Entanglement of distant SQUID rings 29.1 Introduction 29.2 Interaction of a Single SQUID Ring with Nonclassical Microwaves 29.3 Interaction of two Distant SQUID Rings with Entangled Microwaves 29.3.1 Microwaves in number states 29.3.2 Microwaves in coherent states 29.3.3 Numerical results 29.4 Discussions
239 239 240 241 242 243 244 245
30 Time Evolution of two distant SQUID rings irradiated with entangled electromagnetic field 30.1 Introduction 30.2 Interaction of Two SQUID Rings with Nonclassical Microwaves 30.3 Discussions
247 247 248 252
31 Phase diagram of dissipative two-dimensional Josephson junction arrays 31.1 Introduction 31.2 Path Integral Monte Carlo for Dissipative Systems 31.3 Josephson Junction Arrays 31.4 Numerical Simulations and Phase Diagram 31.5 Discussion of the Results
254 254 254 256 257 260
32 Persistent currents in a superconductor/normal loop 32.1 Introduction
263 263
Contents 32.2 SNS Junction 32.3 NS Loop
xiii 264 266
33 Josephson junction ladders: a realization of topological order 33.1 Introduction 33.2 Josephson Junction Ladders 33.3 m-reduction Technique 33.4 Topological Order and "Protected" Qubits
271 271 272 274 276
34 Single-electron charge qubit in a double quantum dot 34.1 Introduction 34.2 Charge Qubit in a Double Quantum Dot 34.2.1 Rotation gate and phase-shift gate operation 34.2.2 Decoherence of the system 34.3 Charge Detection of a Double Quantum Dot 34.4 Summary
279 279 280 281 282 284 286
35 Quantum dots for single photon and photon pair technology
37 Spin amplifier for single spin measurement 37.1 Introduction 37.2 Measurement Schemes 37.3 Experimental Demonstration 37.4 Conclusions
306 306 307 308 310
38 Entanglement in quantum-critical spin systems 38.1 Introduction 38.2 The Model 38.3 Linear Chain: Critical Point and Factorized State 38.4 Entanglement Estimators 38.5 Results 38.6 Two-leg Ladder 38.7 Conclusions
313 313 314 315 316 316 319 320
39 Control of nuclear spins by quantum Hall edge channels 39.1 Introduction 39.2 Samples 39.3 Dynamical Nuclear Polarization 39.4 Local and Coherent Control
322 322 322 324 324
xiv
Contents
39.5 Discussion 39.6 Summary 40 Cloning of single photon by high gain amplifier