Speaker: Nguyen Huy Bang

Slides:



Advertisements
Similar presentations
Population Transfer Resonance: A new Three-Photon Resonance for Small Scale Atomic Clocks Ido Ben-Aroya, Gadi Eisenstein EE Department, Technion, Haifa,
Advertisements

The Fit and the Pendulum Quantum Mechanics and New Clocks M. Crescimanno Department of Physics and Astronomy Youngstown State University & R. Walsworth,
Ruby Laser Crystal structure of sapphire: -Al2O3 (aluminum oxide). The shaded atoms make up a unit cell of the structure. The aluminum atom inside the.
TeraHertz Kerr effect in GaP crystal
Title : Investigation on Nonlinear Optical Effects of Weak Light in Coherent Atomic Media  Author : Hui-jun Li  Supervisor: Prof Guoxiang Huang  Subject:
Generation of short pulses
Slow light in photonic crystal waveguides Nikolay Primerov.
Cavity decay rate in presence of a Slow-Light medium
1 Optical Fibre Amplifiers. 2 Introduction to Optical Amplifiers Raman Fibre Amplifier Brillouin Fibre Amplifier Doped Fibre Amplifier.
Frequency Bistability in a Diode Laser Using Diffraction Gratings Forrest Smith 1, Weliton Soares 2, Samuel Alves 2, Itamar Vidal 2, Marcos Oria 2 1 State.
Introduction to Nonlinear Optics
1.2 Population inversion Absorption and Emission of radiation
Maria Simanovskaia Raman-excited spin coherences in NV centers in diamond.
PBG CAVITY IN NV-DIAMOND FOR QUANTUM COMPUTING Team: John-Kwong Lee (Grad Student) Dr. Renu Tripathi (Post-Doc) Dr. Gaur Pati (Post-Doc) Supported By:
Narrow transitions induced by broad band pulses  |g> |f> Loss of spectral resolution.
Five parametric resonances in a micromechanical system Turner K. L., Miller S. A., Hartwell P. G., MacDonald N. C., Strogatz S. H., Adams S. G., Nature,
1 Coherent processes in metastable helium at room temperature Thomas Lauprêtre Fabienne Goldfarb Fabien Bretenaker Laboratoire Aimé Cotton, Orsay, France.
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.
George R. Welch Marlan O. Scully Irina Novikova Andrey Matsko M. Suhail Zubairy Eugeniy Mikhailov M. Suhail Zubairy Irina Novikova Andrey Matsko Ellipticity-Dependent.
First year talk Mark Zentile
Pump-Probe Spectroscopy Chelsey Dorow Physics 211a.
Nonlinear Optics: Phenomena, Materials and Devices -Honors senior undergraduate and graduate level course. -Approximately lecture hours + 3 seminars.
4-1 Chap. 7 (Optical Instruments), Chap. 8 (Optical Atomic Spectroscopy) General design of optical instruments Sources of radiation Selection of wavelength.
Ultrafast Experiments Hangwen Guo Solid State II Department of Physics & Astronomy, The University of Tennessee.
Single atom lasing of a dressed flux qubit
Dressed state amplification by a superconducting qubit E. Il‘ichev, Outline Introduction: Qubit-resonator system Parametric amplification Quantum amplifier.
1 Waves, Light & Quanta Tim Freegarde Web Gallery of Art; National Gallery, London.
T ECHNISCHE U NIVERSITÄT KAISERSLAUTERN K. Bergmann Lecture 6 Lecture course - Riga, fall 2013 Coherent light-matter interaction: Optically driven adiabatic.
Light Propagation in Photorefractive Polymers
The Fit and the Pendulum Quantum Mechanics and New Clocks M. Crescimanno Department of Physics and Astronomy Youngstown State University & R. Walsworth,
Interaction of radiation with atoms and ions (I) Absorption- Stimulated emission E1E1 E2E2 W 12 =W 21 Spontaneous emission More definitionsCross section.
Observation of ultrafast nonlinear response due to coherent coupling between light and confined excitons in a ZnO crystalline film Ashida Lab. Subaru Saeki.
Refractive index enhancement with vanishing absorption in an atomic vapor Deniz Yavuz, Nick Proite, Brett Unks, Tyler Green Department of Physics, University.
Quantum Optics II – Cozumel, Dec. 6-9, 2004
Enhancing the Macroscopic Yield of Narrow-Band High-Order Harmonic Generation by Fano Resonances Muhammed Sayrac Phys-689 Texas A&M University 4/30/2015.
Pablo Barberis Blostein y Marc Bienert
Refractive Index Enhancement in Atomic Vapors Deniz Yavuz, Nick Proite, Brett Unks, Tyler Green, Dan Sikes Department of Physics, University of Wisconsin.
Waves, Light & Quanta Tim Freegarde Web Gallery of Art; National Gallery, London.
Transient enhancement of the nonlinear atom-photon coupling via recoil-induced resonances: Joel A. Greenberg and Daniel. J. Gauthier Duke University 5/22/2009.
PONDEROMOTIVE ROTATOR: REQUIREMENTS Zach Korth (Caltech) – GWADW ‘12 – Waikoloa, HI.
Instability of optical speckle patterns in cold atomic gases ? S.E. Skipetrov CNRS/Grenoble (Part of this.
Investigation of the Saturation Mechanism of Recoil-induced Resonances Joel A. Greenberg, Marcos Oria, and Daniel J. Gauthier Duke University 5/28/2008.
Suggestion for Optical Implementation of Hadamard Gate Amir Feizpour Physics Department Sharif University of Technology.
Date of download: 6/30/2016 Copyright © 2016 SPIE. All rights reserved. Trans-cis conformational change of the azo-dyes under light irradiation. (a) Equivalent.
Date of download: 7/14/2016 Copyright © 2016 SPIE. All rights reserved. Energy level diagram of a Λ-type atomic system. For Rb87, ∣ 1→F′=2, ∣ 2→F′=1, ∣
Electromagnetically Induced Transparency with Broadband Laser Pulses D. D. Yavuz Department of Physics, University of Wisconsin, Madison, WI, Introduction.
Per Delsing Chalmers University of Technology Quantum Device Physics Interaction between artificial atoms and microwaves Experiments: IoChun Hoi, Chris.
Tunable excitons in gated graphene systems
Population distribution of vibrational levels in the 21 state of NaLi
Four wave mixing in submicron waveguides
Circuit QED Experiment
QUANTUM TRANSITIONS WITHIN THE FUNCTIONAL INTEGRATION REAL FUNCTIONAL
Resonant magneto-optical effects in atoms
Multiplexed saturation spectroscopy with electro-optic frequency combs
Introduction to Nonlinear Optics
Light Sources for Optical Communications
Photonic Crystal Fibers (PCFs)
Nonradiative Quantum Coherences in Semiconductors Hailin Wang, University of Oregon, DMR While storage of classical information is a well- established.
Coherent Nonlinear Optics
Tunable Slow Light in Cesium Vapor
Stabilizing the Carrier-Envelope Phase of the Kansas Light Source
Slow light in Photonic Crystals
? Enhancement of light-matter interactions in slow-wave metasurfaces ?
Marco Polo, Daniel Felinto and Sandra Vianna Departamento de Física
Phase shifted and cascaded long-period fiber grating written by using focused high-repetition-rate CO2 laser pulses.
University of California, Berkeley
Kenji Kamide* and Tetsuo Ogawa
by A. Sipahigil, R. E. Evans, D. D. Sukachev, M. J. Burek, J
Superconducting cavity electro-optics: A platform for coherent photon conversion between superconducting and photonic circuits by Linran Fan, Chang-Ling.
Dynamics of a superconducting qubit coupled to quantum two-level systems in its environment Robert Johansson (RIKEN, The Institute of Physical and Chemical.
Presentation transcript:

Speaker: Nguyen Huy Bang Optical Bistability in a five-level cascade EIT medium: an analytical approach Speaker: Nguyen Huy Bang Vinh University, 182 Le Duan street, Vinh City, Vietnam Vinh, 20 March/2016

Outline 1. Introduction 2. Five-level cascade EIT system 3. EIT enhanced Kerr nonlinearity 4. Optical Bistability in a five-level cascade EIT medium 5. Conclusions Vinh, 20 March/2016

1. Introduction What is optical bistability (OB)? Why we need analytical ? Nonlinearity n (Kerr type) Optical feedback Two requirements:

1. Introduction Some applications of OB: Amplifier Pulse shaper Logic gate AND

1. Introduction Key for modern OB devices: nonlinearity as large as possible! Two mechanisms to enhance the nonlinearity: Fabricate new Kerr materials: n2  10-10 cm2/W Using atomic resonances: n2  10-5 cm2/W How ? Resonance absorption. Thermal effect. Face two problems:

Quantum interference paths. 1. Introduction Electromagnetically induced transparency (EIT): Quantum interference paths. Absorption spectrum Three-level system [2] H. Wang, D. Goorskey, and M. Xiao, “Enhanced Kerr nonlinearity via atomic coherence in a three-level atomic system”, Phys.Rev.Lett., 87 (2001) 073601

1. Introduction Optical bistability in a three –level atomic systems: Absorption spectrum Disadvantage of the three-level: single window (narrow spectral region)!

2. Five-level cascade EIT system Five-level cascade system Three-level cascade system Requirement: + Closely-spacing levels: (hyperfine states); + Intense coupling laser J. Wang et al, Phys.Lett.A 328(2004) 437

2. Five-level cascade EIT system The mater equation: 25 equations for ρik (i, k = 1..5) Relationship between ρ and χ: Perturbation technique:

2. Five-level cascade EIT system aik (relative transition strengths ) Optik 125(2014) 3666

2. Five-level cascade EIT system Optik 125(2014) 3666-3669

2. Five-level cascade EIT system Optik 125(2014) 3666-3669

2. Five-level cascade EIT system Optik 125(2014) 3666; J. Noncryst. Solid. 355 (2009) 1295

3. EIT enhanced Kerr nonlinearity Third-order perturbation χ(3): Kerr coefficient Effective coupling parameters J. Opt.Soc.Am. B/Vol.31.No.6 (2014) 1330

3. EIT enhanced Kerr nonlinearity n2 With EIT n2 Without EIT D.X.Khoa et al., Physica Scripta 90 (2015) 045502; H. Wang et al., Phys.Rev.Lett. 87(2001)073601

Dinh Xuan Khoa et al, J. Opt.Soc.Am. B/Vol.31.No.6 (2014) 1330 3. EIT enhanced Kerr nonlinearity n2 can be controlled! Dinh Xuan Khoa et al, J. Opt.Soc.Am. B/Vol.31.No.6 (2014) 1330

Dinh Xuan Khoa et al, J. Opt.Soc.Am. B/Vol.31.No.6 (2014) 1330 3. EIT enhanced Kerr nonlinearity Dinh Xuan Khoa et al, J. Opt.Soc.Am. B/Vol.31.No.6 (2014) 1330

J.Opt.Soc.Am. B (2016) – In press 4. Optical bistability (OB) in a five-level EIT medium n2 18 J.Opt.Soc.Am. B (2016) – In press

J.Opt.Soc.Am. B (2016) – In press 4. Optical bistability (OB) in a five-level EIT medium absorption 19 J.Opt.Soc.Am. B (2016) – In press

J.Opt.Soc.Am. B (2016) – In press 4. Optical bistability (OB) in a five-level EIT medium Influence of the coupling intensity: c = 0, p = 6 MHz , C = 1000 20 20 20 J.Opt.Soc.Am. B (2016) – In press

J.Opt.Soc.Am. B (2016) – In press 4. Optical bistability (OB) in a five-level EIT medium Influence of the probe detuning: c = 0, c = 10 MHz 21 J.Opt.Soc.Am. B (2016) – In press

J.Opt.Soc.Am. B (2016) – In press 4. Optical bistability (OB) in a five-level EIT medium Influence of the cooperation parameter: c = 0, c = 6MHz, c = 10 MHz 22 J.Opt.Soc.Am. B (2016) – In press

J.Opt.Soc.Am. B (2016) – In press 4. Optical bistability (OB) in a five-level EIT medium Possible realization in experiments: 85Rb atoms 23 J.Opt.Soc.Am. B (2016) – In press

5. Conclusions An OB model has been proposed: Working at three atomic resonances in the present of EIT Analytical interpretations input-output; High Kerr nonlinearity (10-5 cm2/W): low threshold; OB behaviors can be controlled with the coupling light Future works: Role of absorptive and dispersive on OB; Role of Kerr nonlinearity on OB; Realize experimentally; Influences of Doppler broadening; All-optical switching;

Thank you! Vinh, 20 March/2016