What NEC Did Engineered a two-state system Initialized the system Formed a superposition state Allowed the system to evolve Stopped the evolution Read.

Slides:



Advertisements
Similar presentations
Demonstration of conditional gate operation using superconducting charge qubits T. Yamamoto, Yu. A. Pashkin, O. Astafiev, Y. Nakamura & J. S. Tsai Presented.
Advertisements

Fractionalization in condensed matter systems (pre-Majorana days)
Technological issues of superconducting charge qubits Oleg Astafiev Tsuyoshi Yamamoto Yasunobu Nakamura Jaw-Shen Tsai Dmitri Averin NEC Tsukuba - SUNY.
Materials Science in Quantum Computing. Materials scientist view of qubit Materials –SiOx sub substrate –Superconductor (Al,Nb) –SiO x dielectric –Al0.
1 SQUID and Josephson Devices By : Yatin Singhal.
Chapter 28 Direct Current Circuits TexPoint fonts used in EMF. Read the TexPoint manual before you delete this box.: AAAAAA.
Electron Tunneling and the Josephson Effect. Electron Tunneling through an Insulator.
Superconducting transport  Superconducting model Hamiltonians:  Nambu formalism  Current through a N/S junction  Supercurrent in an atomic contact.
Operating in Charge-Phase Regime, Ideal for Superconducting Qubits M. H. S. Amin D-Wave Systems Inc. THE QUANTUM COMPUTING COMPANY TM D-Wave Systems Inc.,
Quantum Mechanics 102 Tunneling and its Applications.
Status of Experiments on Charge- and Flux- Entanglements October 18, 2002, Workshop on Quantum Information Science 中央研究院 物理研究所 陳啟東.
Josephson Junctions, What are they?
P460 - operators and H.O.1 Operator methods in Quantum Mechanics Section 6-1 outlines some formalism – don’t get lost; much you understand define ket and.
Quantum Hall Effect Jesse Noffsinger Group Meeting Talk (As required by the Governor of the State of California) April 17, 2007.
UNIVERSITY OF NOTRE DAME Xiangning Luo EE 698A Department of Electrical Engineering, University of Notre Dame Superconducting Devices for Quantum Computation.
SQUID Based Quantum Bits James McNulty. What’s a SQUID? Superconducting Quantum Interference Device.
EECS 40 Spring 2003 Lecture 3W. G. Oldham and S. Ross 1 Lecture 3 Definitions: Circuits, Nodes, Branches Kirchoff’s Voltage Law (KVL) Kirchoff’s Current.
1 Faraday’s Law of Induction If C is a stationary closed curve and S is a surface spanning C then The changing magnetic flux through S induces a non-electrostatic.
Week 04, Day 2 W10D2 DC Circuits Today’s Reading Assignment W10D2 DC Circuits & Kirchhoff’s Loop Rules Course Notes: Sections Class 09 1.
Superconducting Qubits Kyle Garton Physics C191 Fall 2009.
Electrical Engineering for Civil Engineer Dr. Basim Zafar Spring 2013 EE for CE Course Outlines MID TERM I Dr. Basim Zafar.
Quantum computation with solid state devices - “Theoretical aspects of superconducting qubits” Quantum Computers, Algorithms and Chaos, Varenna 5-15 July.
What is meant by the term “ground state”? It is the lowest energy state that an electron can occupy.
1 PHY 712 Electrodynamics 9-9:50 AM MWF Olin 103 Plan for Lecture 34: Special Topics in Electrodynamics: Electromagnetic aspects of superconductivity 
Physics 2170 – Spring Quantum tunneling: STM & electric shock Homework set 12 is due Wednesday. Clicker.
Electricity & Magnetism Static, Currents, & Electro Magnets Motors & Generators.
Radiation induced photocurrent and quantum interference in n-p junctions. M.V. Fistul, S.V. Syzranov, A.M. Kadigrobov, K.B. Efetov.
SQUIDs (Superconducting QUantum Interference Devices)
Power Dissipation Bounds and Models for Quantum-dot Cellular Automata Circuits Saket Srivastava*, Sudeep Sarkar # and Sanjukta Bhanja* * Electrical Engineering,
Operators A function is something that turns numbers into numbers An operator is something that turns functions into functions Example: The derivative.
Type I and Type II superconductivity
D.Giuliano (Cosenza), P. Sodano (Perugia) Local Pairing of Cooper pairs in Josephson junction networks Obergurgl, June 2010.
(=“P B ”) (=“P C ”) (=“P B or C ”). NEITHER B NOR C “SELECTED”…. BY EACH INDIVIDUAL ATOM !
Exam 2: Review Session CH 24–28
Noise and decoherence in the Josephson Charge Qubits Oleg Astafiev, Yuri Pashkin, Tsuyoshi Yamamoto, Yasunobu Nakamura, Jaw-Shen Tsai RIKEN Frontier Research.
Quantum computation with solid state devices - “Theoretical aspects of superconducting qubits” Quantum Computers, Algorithms and Chaos, Varenna 5-15 July.
DC-squid for measurements on a Josephson persistent-current qubit Applied Physics Quantum Transport Group Alexander ter Haar May 2000 Supervisors: Ir.
Introduction to Josephson Tunneling and Macroscopic Quantum Tunneling
Exam 2: Review Session CH 25–28
Syllabus Resistor Inductor Capacitor Voltage and Current Sources
The review of modern physics has given us a description of nature. Waves are described with a wave equation. Particles are described with particle equations.
 a German physicist  fields of study are electrical circuits, spectroscopy, and the emission of black-body radiation by heated objects  discovered.
Simulating current voltage characteristics in Intrinsic Josephson junctions M. Hromnik Yu. M. Shukrinov M Gaafar BLTP, JINR, Dubna , Russia.
Sid Nb device fabrication Superconducting Nb thin film evaporation Evaporate pure Nb to GaAs wafer and test its superconductivity (T c ~9.25k ) Tc~2.5K.
Scanning Tunneling Microsopy Basics Transmission coefficient critically dependent on the distance btw. tip & surf. Electron energy level densities Electron.
Measuring Quantum Coherence in the Cooper-Pair Box
Introduction to Quantum Mechanics
P460 - operators and H.O.1 Operator methods in Quantum Mechanics Section 6-1 outlines some formalism – don’t get lost; much you understand define ket and.
The rf-SQUID Quantum Bit
Modern Physics lecture 4. The Schroedinger Equation As particles are described by a wave function, we need a wave equation for matter waves As particles.
Subharmonic gap Structures
Principles of Quantum Mechanics P1) Energy is quantized The photoelectric effect Energy quanta E = h  where h = J-s.
By ARKA DUTTA ECE HERITAGE INSTITUTE OF TECHNOLOGY, KOLKATA
Superconductivity, Josephson Junctions, and squids
Quantum dynamics in nano Josephson junctions Equipe cohérence quantique CNRS – Université Joseph Fourier Institut Néel GRENOBLE Wiebke Guichard Olivier.
Unbound States A review on calculations for the potential step.
Coyright(c) by L.R.Linares, 2003.
Superconducting Qubits
BCS THEORY BCS theory is the first microscopic theory of superconductivity since its discovery in It explains, The interaction of phonons and electrons.
Effects of Magnetic Fields and Producing Current
PHYS274 Quantum Mechanics VII
PES 1000 – Physics in Everyday Life
Design and Realization of Decoherence-Free
Devil physics The baddest class on campus IB Physics
Modern Physics Photoelectric Effect Bohr Model for the Atom
Electricity & Magnetism
Joseph Fourier ( ).
Special Topics in Electrodynamics:
Cavity Quantum Electrodynamics for Superconducting Electrical Circuits
Do Now (3B/4B) Take-out: Be ready to review p. 12 at the bell! Paper
Presentation transcript:

What NEC Did Engineered a two-state system Initialized the system Formed a superposition state Allowed the system to evolve Stopped the evolution Read out the final state

The Box The box is 700x50x15nm; It has about 10 8 conduction electrons. e 2 /2C = 117  V; T=30mK, so kT = 3  V; for aluminum,  =230  V

Scope of Talk Tunneling The wave function Josephson’s equations and the squid The Cooper pair box Schrodinger equation solution Josephson quasiparticle current

Tunneling

Josephson’s Equations

Energy in a Junction. Finally, where

Squid Figure 6.1: Schematic of a two-junction squid. Current enters at the top, splits into two branches, and recombines at the bottom. The junctions are at a-b and d-c. A magnetic field B threads the loop formed by the two branches. The integration path is denoted C.

Energy of a Squid

Cooper Pair Box VgVg Box Capacitor Junction RjRj CgCg Box,  CjCj VgVg

Energy of the Box

Hamiltonian To arrive at the quantum mechanical Hamiltonian, note that These two exponents are just raising and lowering operators. H can be rewritten:

Hamiltonian For our system, we can safely consider only the two lowest energy states, In that case,

Josephson Quasiparticle Current Figure 9.1: The double junction Cooper pair box. Junction 2 has very high impedance, has very low critical current, and is voltage biased. Capacitor Junctions VgVg VbVb Box 1 2 V b =650  V, E C =117  V, and R 2 =30M   qp =1.6 x 10 8 sec -1, the lifetime is about 6ns. (Averin and Aleshkin)