Nonlinear kinetic inductance in TiN/NbTiN microresonators and Transmission lines. Peter Day Byeong-Ho Eom Rick Leduc Jonas Zmuidzinas

Evaluation of kinetic-inductance nonlinearity in a singlecrystal NbTiN-based coplanar waveguide

Proc. 14th Int. Conf. on Global Research and Education, Inter-Academia 2015 2016 The Japan Society of Applied Physics Evaluation of kinetic-inductance nonlinearity in a singlecrystal NbTiN-based coplanar

Nonlinear Oscillators and Vacuum Squeezing

Nonlinear Oscillators and Vacuum Squeezing David Haviland Nanosturcture Physics, Dept. Applied Physics, KTH, Albanova Atom in a Cavity Consider only two levels of atom, with energy separation Atom drifts

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

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

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

Design and Characterisation of Titanium Nitride Subarrays of Kinetic Inductance Detectors for Passive Terahertz Imaging

https://doi.org/10.1007/s10909-018-2023-z Design and Characterisation of Titanium Nitride Subarrays of Kinetic Inductance Detectors for Passive Terahertz Imaging Dmitry Morozov 1 Simon M. Doyle 2 Archan

Nonlinear Effects in Optical Fiber. Dr. Mohammad Faisal Assistant Professor Dept. of EEE, BUET

Nonlinear Effects in Optical Fiber Dr. Mohammad Faisal Assistant Professor Dept. of EEE, BUET Fiber Nonlinearities The response of any dielectric material to the light becomes nonlinear for intense electromagnetic

arxiv: v1 [cond-mat.supr-con] 17 Jul 2015

Frequency-tunable Superconducting Resonators via Nonlinear Kinetic Inductance M. R. Vissers 1, J. Hubmayr 1, M. Sandberg 1, S. Chaudhuri 2, C. Bockstiegel 3, and J. Gao 1 arxiv:1507.05126v1 [cond-mat.supr-con]

Metastable states in an RF driven Josephson oscillator

Metastable states in an RF driven Josephson oscillator R. VIJAYARAGHAVAN Daniel Prober Robert Schoelkopf Steve Girvin Department of Applied Physics Yale University 3-16-2006 APS March Meeting I. Siddiqi

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,

arxiv: v1 [physics.ins-det] 13 Nov 2017

Noname manuscript No. (will be inserted by the editor) Electron-phonon coupling in Ti/TiN MKIDs multilayer microresonator M. Faverzani 1,2 P.K. Day 3 E. Ferri 2 A. Giachero 1,2 B. Margesin 4,5 R. Mezzena

Remote entanglement of transmon qubits

Remote entanglement of transmon qubits 3 Michael Hatridge Department of Applied Physics, Yale University Katrina Sliwa Anirudh Narla Shyam Shankar Zaki Leghtas Mazyar Mirrahimi Evan Zalys-Geller Chen Wang

Expressions for f r (T ) and Q i (T ) from Mattis-Bardeen theory

8 Appendix A Expressions for f r (T ) and Q i (T ) from Mattis-Bardeen theory The Mattis-Bardeen theory of the anomalous skin effect in superconductors [0] may be used to derive the behavior of the resonance

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

Distributing Quantum Information with Microwave Resonators in Circuit QED

Distributing Quantum Information with Microwave Resonators in Circuit QED M. Baur, A. Fedorov, L. Steffen (Quantum Computation) J. Fink, A. F. van Loo (Collective Interactions) T. Thiele, S. Hogan (Hybrid

Parametric Interaction in Josephson Junction Circuits and Transmission Lines

Parametric Interaction in Josephson Junction Circuits and Transmission Lines by Hamid Reza Mohebbi A thesis presented to the University of Waterloo in fulfillment of the thesis requirement for the degree

Fiber Gratings p. 1 Basic Concepts p. 1 Bragg Diffraction p. 2 Photosensitivity p. 3 Fabrication Techniques p. 4 Single-Beam Internal Technique p.

Preface p. xiii Fiber Gratings p. 1 Basic Concepts p. 1 Bragg Diffraction p. 2 Photosensitivity p. 3 Fabrication Techniques p. 4 Single-Beam Internal Technique p. 4 Dual-Beam Holographic Technique p. 5

Non-equilibrium superconductivity in microwave resonators

Non-equilibrium superconductivity in microwave resonators Cooper Pairs 2Δ hν Pieter de Visser Quasipar/cles SRON: Stephen Yates, Jochem Baselmans, Pascale Diener, Andrey Baryshev Delft: Teun Klapwijk,

Lecture 14 Date:

Lecture 14 Date: 18.09.2014 L Type Matching Network Examples Nodal Quality Factor T- and Pi- Matching Networks Microstrip Matching Networks Series- and Shunt-stub Matching L Type Matching Network (contd.)

MoBiKID Kinetic Inductance Detectors for up-coming B-mode satellite experiments

MoBiKID Kinetic Inductance Detectors for up-coming B-mode satellite experiments TIPP 17 - BEIJING INFN, Sezione di Roma Dawn of the universe: where are we? Looking into the CMB for a proof of the Inflation...

Electronics. Basics & Applications. group talk Daniel Biesinger

Electronics Basics & Applications group talk 23.7.2010 by Daniel Biesinger 1 2 Contents Contents Basics Simple applications Equivalent circuit Impedance & Reactance More advanced applications - RC circuits

Cavity Quantum Electrodynamics (QED): Coupling a Harmonic Oscillator to a Qubit

Cavity Quantum Electrodynamics (QED): Coupling a Harmonic Oscillator to a Qubit Cavity QED with Superconducting Circuits coherent quantum mechanics with individual photons and qubits...... basic approach:

Φ / Resonant frequency (GHz) exp. theory Supplementary Figure 2: Resonant frequency ω PO

1 a 1 mm b d SQUID JJ c 30 µm 30 µm 10 µm Supplementary Figure 1: Images of the parametric phase-locked oscillator. a, Optical image of the device. The λ/4-type coplanar waveguide resonator is made of

THz Electron Gun Development. Emilio Nanni 3/30/2016

THz Electron Gun Development Emilio Nanni 3/30/2016 Outline Motivation Experimental Demonstration of THz Acceleration THz Generation Accelerating Structure and Results Moving Forward Parametric THz Amplifiers

Electromagnetic Oscillations and Alternating Current. 1. Electromagnetic oscillations and LC circuit 2. Alternating Current 3.

Electromagnetic Oscillations and Alternating Current 1. Electromagnetic oscillations and LC circuit 2. Alternating Current 3. RLC circuit in AC 1 RL and RC circuits RL RC Charging Discharging I = emf R

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

Progress In Electromagnetics Research M, Vol. 20, 73 80, 2011

Progress In Electromagnetics Research M, Vol. 20, 73 80, 2011 COPLANAR METAMATERIAL MICRO-RESONATOR S. Nemer 1, 2, *, B. Sauviac 1, B. Bayard 1, J. J. Rousseau 1, C. Nader 2, J. Bechara 2, and A. Khoury

Impedance. Reactance. Capacitors

Impedance Ohm's law describes the relationship between current and voltage in circuits that are in equilibrium- that is, when the current and voltage are not changing. When we have a situation where the

Nonlinear effects in optical fibers - v1. Miguel A. Muriel UPM-ETSIT-MUIT-CFOP

Nonlinear effects in optical fibers - v1 Miguel A. Muriel UPM-ETSIT-MUIT-CFOP Miguel A. Muriel-015/10-1 Nonlinear effects in optical fibers 1) Introduction ) Causes 3) Parameters 4) Fundamental processes

Sophomore Physics Laboratory (PH005/105)

CALIFORNIA INSTITUTE OF TECHNOLOGY PHYSICS MATHEMATICS AND ASTRONOMY DIVISION Sophomore Physics Laboratory (PH5/15) Analog Electronics Active Filters Copyright c Virgínio de Oliveira Sannibale, 23 (Revision

ELECTROMAGNETIC OSCILLATIONS AND ALTERNATING CURRENT

Chapter 31: ELECTROMAGNETIC OSCILLATIONS AND ALTERNATING CURRENT 1 A charged capacitor and an inductor are connected in series At time t = 0 the current is zero, but the capacitor is charged If T is the

Introduction to Circuit QED

Introduction to Circuit QED Michael Goerz ARL Quantum Seminar November 10, 2015 Michael Goerz Intro to cqed 1 / 20 Jaynes-Cummings model g κ γ [from Schuster. Phd Thesis. Yale (2007)] Jaynes-Cumming Hamiltonian

Chapter 31: RLC Circuits. PHY2049: Chapter 31 1

hapter 31: RL ircuits PHY049: hapter 31 1 L Oscillations onservation of energy Topics Damped oscillations in RL circuits Energy loss A current RMS quantities Forced oscillations Resistance, reactance,

EE221 Circuits II. Chapter 14 Frequency Response

EE22 Circuits II Chapter 4 Frequency Response Frequency Response Chapter 4 4. Introduction 4.2 Transfer Function 4.3 Bode Plots 4.4 Series Resonance 4.5 Parallel Resonance 4.6 Passive Filters 4.7 Active

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

EE221 Circuits II. Chapter 14 Frequency Response

EE22 Circuits II Chapter 4 Frequency Response Frequency Response Chapter 4 4. Introduction 4.2 Transfer Function 4.3 Bode Plots 4.4 Series Resonance 4.5 Parallel Resonance 4.6 Passive Filters 4.7 Active

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

Microwave Oscillators Design

Microwave Oscillators Design Oscillators Classification Feedback Oscillators β Α Oscillation Condition: Gloop = A β(jω 0 ) = 1 Gloop(jω 0 ) = 1, Gloop(jω 0 )=2nπ Negative resistance oscillators Most used

MUSCAT and Toltec. Dublin KIDs workshop. Dublin 7 th September 2017

MUSCAT and Toltec Dublin KIDs workshop Dublin 7 th September 2017 Scope of talk Overview of the MUSCAT project and the team Instrument overview System design considerations Detector design consideration

A capacitor is a device that stores electric charge (memory devices). A capacitor is a device that stores energy E = Q2 2C = CV 2

Capacitance: Lecture 2: Resistors and Capacitors Capacitance (C) is defined as the ratio of charge (Q) to voltage (V) on an object: C = Q/V = Coulombs/Volt = Farad Capacitance of an object depends on geometry

Sinusoidal Steady-State Analysis

Chapter 4 Sinusoidal Steady-State Analysis In this unit, we consider circuits in which the sources are sinusoidal in nature. The review section of this unit covers most of section 9.1 9.9 of the text.

Supplementary Methods A. Sample fabrication

Supplementary Methods A. Sample fabrication Supplementary Figure 1(a) shows the SEM photograph of a typical sample, with three suspended graphene resonators in an array. The cross-section schematic is

Doing Atomic Physics with Electrical Circuits: Strong Coupling Cavity QED

Doing Atomic Physics with Electrical Circuits: Strong Coupling Cavity QED Ren-Shou Huang, Alexandre Blais, Andreas Wallraff, David Schuster, Sameer Kumar, Luigi Frunzio, Hannes Majer, Steven Girvin, Robert

Towards a quantum interface between light and microwave circuits

Towards a quantum interface between light and microwave circuits ambient light ultracold microwaves Quantum information network built from nodes linked by propagating modes quantum network nodes process

PHYSICS. Chapter 30 Lecture FOR SCIENTISTS AND ENGINEERS A STRATEGIC APPROACH 4/E RANDALL D. KNIGHT

PHYSICS FOR SCIENTISTS AND ENGINEERS A STRATEGIC APPROACH 4/E Chapter 30 Lecture RANDALL D. KNIGHT Chapter 30 Electromagnetic Induction IN THIS CHAPTER, you will learn what electromagnetic induction is

INTRODUCTION TO SUPERCONDUCTING QUBITS AND QUANTUM EXPERIENCE: A 5-QUBIT QUANTUM PROCESSOR IN THE CLOUD

INTRODUCTION TO SUPERCONDUCTING QUBITS AND QUANTUM EXPERIENCE: A 5-QUBIT QUANTUM PROCESSOR IN THE CLOUD Hanhee Paik IBM Quantum Computing Group IBM T. J. Watson Research Center, Yorktown Heights, NY USA

Alternating Currents. The power is transmitted from a power house on high voltage ac because (a) Electric current travels faster at higher volts (b) It is more economical due to less power wastage (c)

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

Quantum Optics with Electrical Circuits: Circuit QED

Quantum Optics with Electrical Circuits: Circuit QED Eperiment Rob Schoelkopf Michel Devoret Andreas Wallraff David Schuster Hannes Majer Luigi Frunzio Andrew Houck Blake Johnson Emily Chan Jared Schwede

Nonlinear Fiber Optics and its Applications in Optical Signal Processing

1/44 Nonlinear Fiber Optics and its Applications in Optical Signal Processing Govind P. Agrawal Institute of Optics University of Rochester Rochester, NY 14627 c 2007 G. P. Agrawal Outline Introduction

Resonant Matching Networks

Chapter 1 Resonant Matching Networks 1.1 Introduction Frequently power from a linear source has to be transferred into a load. If the load impedance may be adjusted, the maximum power theorem states that

Nonlinear effects and pulse propagation in PCFs

Nonlinear effects and pulse propagation in PCFs --Examples of nonlinear effects in small glass core photonic crystal fibers --Physics of nonlinear effects in fibers --Theoretical framework --Solitons and

Measured Transmitted Intensity. Intensity 1. Hair

in Radiation pressure optical cavities Measured Transmitted Intensity Intensity 1 1 t t Hair Experimental setup Observes oscillations Physical intuition Model Relation to: Other nonlinearities, quantum

Terahertz sensing and imaging based on carbon nanotubes:

Terahertz sensing and imaging based on carbon nanotubes: Frequency-selective detection and near-field imaging Yukio Kawano RIKEN, JST PRESTO ykawano@riken.jp http://www.riken.jp/lab-www/adv_device/kawano/index.html

LCR Series Circuits. AC Theory. Introduction to LCR Series Circuits. Module. What you'll learn in Module 9. Module 9 Introduction

Module 9 AC Theory LCR Series Circuits Introduction to LCR Series Circuits What you'll learn in Module 9. Module 9 Introduction Introduction to LCR Series Circuits. Section 9.1 LCR Series Circuits. Amazing

Delayed Feedback and GHz-Scale Chaos on the Driven Diode-Terminated Transmission Line

Delayed Feedback and GHz-Scale Chaos on the Driven Diode-Terminated Transmission Line Steven M. Anlage, Vassili Demergis, Renato Moraes, Edward Ott, Thomas Antonsen Thanks to Alexander Glasser, Marshal

Homework Assignment 11

Homework Assignment Question State and then explain in 2 3 sentences, the advantage of switched capacitor filters compared to continuous-time active filters. (3 points) Continuous time filters use resistors

MEP 382: Design of Applied Measurement Systems Lecture 3: DC & AC Circuit Analysis

Faculty of Engineering MEP 38: Design of Applied Measurement Systems Lecture 3: DC & AC Circuit Analysis Outline oltage and Current Ohm s Law Kirchoff s laws esistors Series and Parallel oltage Dividers

Berkeley. Matching Networks. Prof. Ali M. Niknejad. U.C. Berkeley Copyright c 2016 by Ali M. Niknejad

Berkeley Matching Networks Prof. Ali M. Niknejad U.C. Berkeley Copyright c 2016 by Ali M. Niknejad February 9, 2016 1 / 33 Impedance Matching R S i i i o Z in + v i Matching Network + v o Z out RF design

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,

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

PHY 103 Impedance. Segev BenZvi Department of Physics and Astronomy University of Rochester

PHY 103 Impedance Segev BenZvi Department of Physics and Astronomy University of Rochester Reading Reading for this week: Hopkin, Chapter 1 Heller, Chapter 1 2 Waves in an Air Column Recall the standing

The SQUID-tunable resonator as a microwave parametric oscillator

The SQUID-tunable resonator as a microwave parametric oscillator Tim Duty Yarema Reshitnyk Charles Meaney Gerard Milburn University of Queensland Brisbane, Australia Chris Wilson Martin Sandberg Per Delsing

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

Outline of College Physics OpenStax Book

Outline of College Physics OpenStax Book Taken from the online version of the book Dec. 27, 2017 18. Electric Charge and Electric Field 18.1. Static Electricity and Charge: Conservation of Charge Define

AC Circuits. The Capacitor

The Capacitor Two conductors in close proximity (and electrically isolated from one another) form a capacitor. An electric field is produced by charge differences between the conductors. The capacitance

OPERATIONAL AMPLIFIER APPLICATIONS

OPERATIONAL AMPLIFIER APPLICATIONS 2.1 The Ideal Op Amp (Chapter 2.1) Amplifier Applications 2.2 The Inverting Configuration (Chapter 2.2) 2.3 The Non-inverting Configuration (Chapter 2.3) 2.4 Difference

PHY 103 Impedance. Segev BenZvi Department of Physics and Astronomy University of Rochester

PHY 103 Impedance Segev BenZvi Department of Physics and Astronomy University of Rochester Midterm Exam Proposed date: in class, Thursday October 20 Will be largely conceptual with some basic arithmetic

Highly Nonlinear Fibers and Their Applications

1/32 Highly Nonlinear Fibers and Their Applications Govind P. Agrawal Institute of Optics University of Rochester Rochester, NY 14627 c 2007 G. P. Agrawal Introduction Many nonlinear effects inside optical

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

KH600. 1GHz, Differential Input/Output Amplifier. Features. Description. Applications. Typical Application

KH 1GHz, Differential Input/Output Amplifier www.cadeka.com Features DC - 1GHz bandwidth Fixed 1dB (V/V) gain 1Ω (differential) inputs and outputs -7/-dBc nd/3rd HD at MHz ma output current 9V pp into

RLC Circuit (3) We can then write the differential equation for charge on the capacitor. The solution of this differential equation is

RLC Circuit (3) We can then write the differential equation for charge on the capacitor The solution of this differential equation is (damped harmonic oscillation!), where 25 RLC Circuit (4) If we charge

Low-loss superconducting resonant circuits using vacuum-gap-based microwave components

Low-loss superconducting resonant circuits using vacuum-gap-based microwave components Katarina Cicak 1, Dale Li 1, Joshua A. Strong 1,2, Michael S. Allman 1,2, Fabio Altomare 1, Adam J. Sirois 1,2, Jed

Amplification, entanglement and storage of microwave radiation using superconducting circuits

Amplification, entanglement and storage of microwave radiation using superconducting circuits Jean-Damien Pillet Philip Kim s group at Columbia University, New York, USA Work done in Quantum Electronics

Hybrid Quantum Circuit with a Superconducting Qubit coupled to a Spin Ensemble

Hybrid Quantum Circuit with a Superconducting Qubit coupled to a Spin Ensemble, Cécile GREZES, Andreas DEWES, Denis VION, Daniel ESTEVE, & Patrice BERTET Quantronics Group, SPEC, CEA- Saclay Collaborating

Lecture 9 Time Domain vs. Frequency Domain

. Topics covered Lecture 9 Time Domain vs. Frequency Domain (a) AC power in the time domain (b) AC power in the frequency domain (c) Reactive power (d) Maximum power transfer in AC circuits (e) Frequency

MODULE-4 RESONANCE CIRCUITS

Introduction: MODULE-4 RESONANCE CIRCUITS Resonance is a condition in an RLC circuit in which the capacitive and inductive Reactance s are equal in magnitude, there by resulting in purely resistive impedance.

Quantum-noise reduction techniques in a gravitational-wave detector

Quantum-noise reduction techniques in a gravitational-wave detector AQIS11 satellite session@kias Aug. 2011 Tokyo Inst of Technology Kentaro Somiya Contents Gravitational-wave detector Quantum non-demolition

Dielectric wave guides, resonance, and cavities

Dielectric wave guides, resonance, and cavities 1 Dielectric wave guides Instead of a cavity constructed of conducting walls, a guide can be constructed of dielectric material. In analogy to a conducting

Interaction between surface acoustic waves and a transmon qubit

Interaction between surface acoustic waves and a transmon qubit Ø Introduction Ø Artificial atoms Ø Surface acoustic waves Ø Interaction with a qubit on GaAs Ø Nonlinear phonon reflection Ø Listening to

Physics 4B Chapter 31: Electromagnetic Oscillations and Alternating Current

Physics 4B Chapter 31: Electromagnetic Oscillations and Alternating Current People of mediocre ability sometimes achieve outstanding success because they don't know when to quit. Most men succeed because

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

Self-Phase Modulation in Optical Fiber Communications: Good or Bad?

1/100 Self-Phase Modulation in Optical Fiber Communications: Good or Bad? Govind P. Agrawal Institute of Optics University of Rochester Rochester, NY 14627 c 2007 G. P. Agrawal Outline Historical Introduction

Probing Wigner Crystals in the 2DEG using Microwaves

Probing Wigner Crystals in the 2DEG using Microwaves G. Steele CMX Journal Club Talk 9 September 2003 Based on work from the groups of: L. W. Engel (NHMFL), D. C. Tsui (Princeton), and collaborators. CMX

The Dark Matter Radio. Kent Irwin for the DM Radio Collaboration. DM Radio Pathfinder

The Dark Matter Radio Kent Irwin for the DM Radio Collaboration DM Radio Pathfinder Outline Field-like dark matter: axions and hidden photons Fundamental limits on the detection of axions and hidden photons

Raman Amplification for Telecom Optical Networks. Dominique Bayart Alcatel Lucent Bell Labs France, Research Center of Villarceaux

Raman Amplification for Telecom Optical Networks Dominique Bayart Alcatel Lucent Bell Labs France, Research Center of Villarceaux Training day www.brighter.eu project Cork, June 20th 2008 Outline of the

Prof. Anyes Taffard. Physics 120/220. Voltage Divider Capacitor RC circuits

Prof. Anyes Taffard Physics 120/220 Voltage Divider Capacitor RC circuits Voltage Divider The figure is called a voltage divider. It s one of the most useful and important circuit elements we will encounter.

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

The Quantum Limit and Beyond in Gravitational Wave Detectors

The Quantum Limit and Beyond in Gravitational Wave Detectors Gravitational wave detectors Quantum nature of light Quantum states of mirrors Nergis Mavalvala GW2010, UMinn, October 2010 Outline Quantum

Laser Spectroscopy of HeH + 施宙聰 2011 AMO TALK 2011/9/26

Laser Spectroscopy of HeH + 施宙聰 2011 AMO TALK 2011/9/26 Outline Introduction Previous experimental results Saturation spectroscopy Conclusions and future works Diatomic Molecules Total energy=electronic

Nonlinear ultrafast fiber optic devices based on Carbon Nanotubes

Nonlinear ultrafast fiber optic devices based on Carbon Nanotubes Guillermo E. Villanueva, Claudio J. Oton Michael B. Jakubinek, Benoit Simard,, Jaques Albert, Pere Pérez-Millán Outline Introduction CNT-coated

Chapter 31 Electromagnetic Oscillations and Alternating Current LC Oscillations, Qualitatively

Chapter 3 Electromagnetic Oscillations and Alternating Current LC Oscillations, Qualitatively In the LC circuit the charge, current, and potential difference vary sinusoidally (with period T and angular

Ultrafast nonlinear optical processing in photonics integrated circuits: Slow light enhanced

Ultrafast nonlinear optical processing in photonics integrated circuits: Slow light enhanced Benjamin Eggleton ARC Laureate Fellow Director, CUDOS - Australian Centre of Excellence Centre for Ultrahigh-bandwidth

Day 3: Ultracold atoms from a qubit perspective

Cindy Regal Condensed Matter Summer School, 2018 Day 1: Quantum optomechanics Day 2: Quantum transduction Day 3: Ultracold atoms from a qubit perspective Day 1: Quantum optomechanics Day 2: Quantum transduction

arxiv: v2 [cond-mat.mes-hall] 19 Oct 2010

High-Fidelity Readout in Circuit Quantum Electrodynamics Using the Jaynes-Cummings Nonlinearity arxiv:4.4323v2 [cond-mat.mes-hall] 9 Oct 2 M. D. Reed, L. DiCarlo, B. R. Johnson, L. Sun, D. I. Schuster,

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

Inductors. Hydraulic analogy Duality with capacitor Charging and discharging. Lecture 12: Inductors

Lecture 12: nductors nductors Hydraulic analogy Duality with capacitor Charging and discharging Robert R. McLeod, University of Colorado http://hilaroad.com/camp/projects/magnet.html 99 Lecture 12: nductors

) Rotate L by 120 clockwise to obtain in!! anywhere between load and generator: rotation by 2d in clockwise direction. d=distance from the load to the

3.1 Smith Chart Construction: Start with polar representation of. L ; in on lossless lines related by simple phase change ) Idea: polar plot going from L to in involves simple rotation. in jj 1 ) circle

EMC Considerations for DC Power Design

EMC Considerations for DC Power Design Tzong-Lin Wu, Ph.D. Department of Electrical Engineering National Sun Yat-sen University Power Bus Noise below 5MHz 1 Power Bus Noise below 5MHz (Solution) Add Bulk

PY3107 Experimental Physics II

PY3107 Experimental Physics II ock-in Amplifiers MP aughan and F Peters Related Experiments ock-in ab ignal processing and phase sensitive detection using a lock-in amplifier The problem The signal to