國立交通大學電子物理系 專題演講 Quantum optics in 3-level superconducting artificial atoms: Controlling one-photon and two-photon transparency Abstract We experimentally.

Slides:



Advertisements
Similar presentations
Trapped ultracold atoms: Bosons Bose-Einstein condensation of a dilute bosonic gas Probe of superfluidity: vortices.
Advertisements

Cavity cooling of a single atom James Millen 21/01/09.
Superconducting qubits
Zero-Phonon Line: transition without creation or destruction of phonons Phonon Wing: at T = 0 K, creation of one or more phonons 7. Optical Spectroscopy.
CQED Susceptibility of Superconducting Transmons coupled to a Microstrip Resonator Cavity David Pappas, Martin Sandberg, Jiansong Gao, Michael Vissers.
LASERS A short introduction on how “lasing” is achieved.
Third order nonlinear optics 1. Two Photon pumping 2.. Third harmonic generation 3. Doppler free spectroscopy 4. Lambda structures.
Non-equilibrium dynamics in the Dicke model Izabella Lovas Supervisor: Balázs Dóra Budapest University of Technology and Economics
A) The wavelength and frequency of a light wave
Quantum Computing with Trapped Ion Hyperfine Qubits.
Atomically-Resolved Optical Properties of Single Molecules Arthur Yu Mentor: Wilson Ho IM-SURE 2007.
Cavity QED as a Deterministic Photon Source Gary Howell Feb. 9, 2007.
References Acknowledgements This work is funded by EPSRC 1.R. P. Abel, U. Krohn, P. Siddons, I. G. Hughes & C. S. Adams, Opt Lett (2009). 2.A.
Quantum Computation Using Optical Lattices Ben Zaks Victor Acosta Physics 191 Prof. Whaley UC-Berkeley.

Guillaume TAREL, PhC Course, QD EMISSION 1 Control of spontaneous emission of QD using photonic crystals.
Optically Pumping Nuclear Magnetic Spin M.R.Ross, D.Morris, P.H. Bucksbaum, T. Chupp Physics Department, University of Michigan J. Taylor, N. Gershenfeld.
4-1 Chap. 7 (Optical Instruments), Chap. 8 (Optical Atomic Spectroscopy) General design of optical instruments Sources of radiation Selection of wavelength.
1 Cold molecules Mike Tarbutt LMI Lecture, 05/11/12.
Dressed state amplification by a superconducting qubit E. Il‘ichev, Outline Introduction: Qubit-resonator system Parametric amplification Quantum amplifier.
Фото MANIPULATING THE QUANTUM STATE OF SINGLE ATOMS AND PHOTONS works of Nobel Laureates in physics 2012 A.V.Masalov Lebedev Physics Institute, RAS, Moscow.
Charge Carrier Related Nonlinearities
Arrangement of Electrons
PROPOSAL OF A UNIVERSAL QUANTUM COPYING MACHINE IN CAVITY QED Joanna Gonzalez Miguel Orszag Sergio Dagach Facultad de Física Pontificia Universidad Católica.
Adiabatic approximation
Ch ; Lecture 26 – Quantum description of absorption.
Meet the transmon and his friends
Chapter 7 Atomic Structure & Periodicity. Electromagnetic Radiation O Waves (wavelength, frequency & speed) O  c (page 342: #39) O Hertz O Max Planck.
Atomic transitions and electromagnetic waves
Pablo Barberis Blostein y Marc Bienert
Introduction to materials physics #4
For long wavelength, compared to the size of the atom The term containing A 2 in the dipole approximation does not involve atomic operators, consequently.
Conditional Dynamics of Interacting Quantum Dots Lucio Robledo, Jeroen Elzerman, Gregor Jundt, Mete Atatüre, Alexander Högele, Stefan Fält, Atac Imamoglu.
Quantum Theory/Numbers Week 5/6 Big idea #1. 1) How do we know when an electron has moved from an excited state to the ground state? The electron will.
QM2 Concept Test 13.6 Choose all of the following statements that are correct about electromagnetic radiation and transitions between two energy.
Suggestion for Optical Implementation of Hadamard Gate Amir Feizpour Physics Department Sharif University of Technology.
Microwave Transitions Between Pair States Composed of Two Rb Rydberg Atoms Jeonghun Lee Advisor: Tom F. Gallagher Department of Physics, University of.
Absorption Small-Signal Loss Coefficient. Absorption Light might either be attenuated or amplified as it propagates through the medium. What determines.
Per Delsing Chalmers University of Technology Quantum Device Physics Interaction between artificial atoms and microwaves Experiments: IoChun Hoi, Chris.
Jiří Minář Centre for Quantum Technologies
Coherent excited states in superconductors due to a microwave field
Raman Effect The Scattering of electromagnetic radiation by matter with a change of frequency.
The Photonics Institute The Photonics Institute Student Seminar
Superconducting artificial atoms coupled to 1D open space
Circuit QED Experiment
Pitch and Catch of Non-Classical Microwaves
Quantum Phase Transition of Light: A Renormalization Group Study
專題演講 Spin Accumulation induced Magnetocapacitance in a Ferromagnetic Single Electron Transistor Abstract We show that non-equilibrium spin accumulation.
Remote tuning of an optical resonator
From low temperature physics to nanoscience and thermoelectricity
Today’s Plan Review 2-level system (Schordinger eq, Rabi, Bloch)
Lasers and effects of magnetic field
Optical qubits
Using MAPP to Generate a VHDL Model of the Microring Resonator
Strong coupling of a superradiant spin ensemble B. C. Rose, A. M
Coupled atom-cavity system
Coupling a Single Electron Spin to a Microwave Cavity
Superconducting qubit for quantum thermodynamics experiments
Resolution of Transient States of Nitrile Anions via Photodissociation Action Spectroscopy; Our Progress to Date The 2 traces show resonant Cu atomic.
Cavity QED
武汉物数所理论交叉学术交流系列报告 (第一三四期)
PHY 752 Solid State Physics
Quantum World at Atomic Scale:
Atomic transitions and electromagnetic waves
Quantum Theory.
Linear Optical Quantum Computing
Norm Moulton LPS 15 October, 1999
Consider the experimental evidence you just saw,
Second quantization and Green’s functions
Jaynes-Cummings Hamiltonian
Presentation transcript:

國立交通大學電子物理系 專題演講 Quantum optics in 3-level superconducting artificial atoms: Controlling one-photon and two-photon transparency Abstract We experimentally study interactions between two microwave fields mediated by transmon-type 3-level artificial atom. The transmon has good selection rule, preventing one-photon transition, but allowing two-photon transition from ground state(0) to 2nd excited state(2). By pumping a control tone in resonance to the transition between 1st(1) and 2nd excited state(2), we control the one-photon transparency for 0 to 1 transition and two-photon transparency for 0 to 2 transition. Realization of large Kerr non-linearity using a 4-level system is discussed. Time:10/22(Thu.) 13:20-15:10 Place:基礎科學大樓B1 次軒聽 (SC001) Speaker:郭華丞(Watson, Kuo) , 國立中興大學物理系 Host:陳煜璋 (Yu-Chang, Chang)