Cold atoms in Optical lattice, vibrational states, coherent control via interference between one- and two-phonon excitation, and a little bit about decoherence,

Slides:



Advertisements
Similar presentations
Chapter 31 Light Quanta.
Advertisements

Interference and Diffraction
Measuring the Speed of Light Jack Young Rich Breazeale Ryan Phelan.
KAPITZA-DIRAC EFFECT Eric Weaver Phys 4P62. General Outline  Theorized in 1933 by Kapitza and Dirac  Reflection of electrons from standing light waves.
Dynamics of a BEC colliding with a time-dependent dipole barrier (+ Special Bonus Features) Institut D’Optique, Palaiseau, France October 8, 2007 Chris.
Samansa Maneshi, Jalani Kanem, Chao Zhuang, Matthew Partlow Aephraim Steinberg Department of Physics, Center for Quantum Information and Quantum Control,
Laser cooling of molecules. 2 Why laser cooling (usually) fails for molecules Laser cooling relies on repeated absorption – spontaneous-emission events.
Lecture 3 Kinetics of electronically excited states
Anderson localization in BECs
Ghost Imaging Sean Crosby Supervisor: Associate Professor Ann Roberts Optics Annual Talks 8 March 2005.
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:
Light Emission. Today’s Topics Excitation Emission Spectra Incandescence –Absorption Spectra.
Danielle Boddy Durham University – Atomic & Molecular Physics group Red MOT is on its way to save the day!
Narrow transitions induced by broad band pulses  |g> |f> Loss of spectral resolution.
Low Temperature Photon Echo Measurements of Organic Dyes in Thin Polymer Films Richard Metzler ‘06, Eliza Blair ‘07, and Carl Grossman, Department of Physics.
Laser-induced vibrational motion through impulsive ionization Grad students: Li Fang, Brad Moser Funding : NSF-AMO October 19, 2007 University of New Mexico.
Strong-field physics revealed through time-domain spectroscopy Grad student: Li Fang Funding : NSF-AMO May 30, 2009 XI Cross Border Workshop on Laser Science.
Strong-field physics revealed through time-domain spectroscopy Grad student: Li Fang Funding : NSF-AMO May 20, 2009 DAMOP Charlottesville, VA George N.
Light Emission. Today’s Topics Excitation Emission Spectra Incandescence –Absorption Spectra.
1 P1X: Optics, Waves and Lasers Lectures, Lasers and their Applications i) to understand what is meant by coherent and incoherent light sources;
Optical Lattices 1 Greiner Lab Winter School 2010 Florian Huber 02/01/2010.
Dissipation and Coherence: Halogens in Rare Gas Solids Signatures of Dissipation in Pump-Probe Spectra Dissipation of Energy in Excited Halogens Dispersion.
Experiments with ultracold RbCs molecules Peter Molony Cs Rb.
Wave Packet Echo in Optical Lattice and Decoherence Time Chao Zhuang U(t) Aug. 15, 2006 CQISC2006 University of Toronto.
Elastic collisions. Spin exchange. Magnetization is conserved. Inelastic collisions. Magnetization is free. Magnetic properties of a dipolar BEC loaded.
Waves Superposition and Standing Waves The Electromagnetic Spectrum Pulse-Echo Techniques Refraction Polarisation Diffraction.
Electronic Spectroscopy of Palladium Dimer (Pd 2 ) 68th OSU International Symposium on Molecular Spectroscopy Yue Qian, Y. W. Ng and A. S-C. Cheung Department.
Have left: B. Pasquiou (PhD), G. Bismut (PhD), M. Efremov, Q. Beaufils, J. C. Keller, T. Zanon, R. Barbé, A. Pouderous, R. Chicireanu Collaborators: Anne.
Quantum information with photons and atoms: from tomography to error correction C. W. Ellenor, M. Mohseni, S.H. Myrskog, J.K. Fox, J. S. Lundeen, K. J.
Quantum interference phenomenon Quantum interference phenomenon in the cold atomic cascade system $$ : National Science Council and National Space Program.
Jalani F. Kanem 1, Samansa Maneshi 1, Matthew Partlow 1, Michael Spanner 2 and Aephraim Steinberg 1 Center for Quantum Information & Quantum Control, Institute.
Chapter 3 Lattice vibration and crystal thermal properties Shuxi Dai Department of Physics Unit 4 : Experimental measurements of Phonons.
Dynamics of Low Density Rydberg Gases Experimental Apparatus E. Brekke, J. O. Day, T. G. Walker University of Wisconsin – Madison Support from NSF and.
Duke University, Physics Department and the Fitzpatrick Institute for Photonics · Durham, NC Collective Nonlinear Optical Effects in an Ultracold Thermal.
Spatial distributions in a cold strontium Rydberg gas Graham Lochead.
1.1 What’s electromagnetic radiation
A. Nass, M. Chapman, D. Graham, W. Haeberli,
Dynamics of a BEC colliding with a time-dependent dipole barrier OSA Frontiers in Photonics 2006 starring Chris Ellenor as Mirco Siercke Aephraim Steinberg’s.
Jerzy Zachorowski M. Smoluchowski Institute of Physics, Jagiellonian University Nonlinear Spectroscopy of Cold Atoms, Preparations for the BEC Experiments.
Spatial distributions in a cold strontium Rydberg gas Graham Lochead.
modes Atomic Vibrations in Crystals = Phonons Hooke’s law: Vibration frequency   f = force constant, M = mass Test for phonon effects by using isotopes.
Collisional loss rate measurement of Cesium atoms in MOT Speaker : Wang guiping Date : December 25.
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, ∣
Chao Zhuang, Samansa Maneshi, XiaoXian Liu, Ardavan Darabi, Chris Paul, Luciano Cruz, and Aephraim Steinberg Department of Physics, Center for Quantum.
Date of download: 9/19/2016 Copyright © 2016 SPIE. All rights reserved. Phase-dependent probe amplitude in the continuous wave regime. The blue line is.
Raman Effect The Scattering of electromagnetic radiation by matter with a change of frequency.
Observation of Quantum Beating in Rubidium at 2. 1 THz and 18
A Versatile SLM Enabled Atomtronic Device for Quantum Simulation in 2D
Free Electron Sources of CoherentRadiation: FREE ELECTRON LASERS
Interaction between Photons and Electrons
Making cold molecules from cold atoms
Cavity Ring-Down Spectroscopy
Multiturn extraction for PS2
Origin of The Electromagnetic (EM) Waves
Sound Or Can You Hear Me Now? Standards:
Bi-plasma interactions on femtosecond time-scales
Model-Independent Measurement of Excited State Fraction in a MOT
Trivia Question In class we talked about using interference to measure the thickness of thin films. In general, optical instruments which use the interference.
Atomic BEC in microtraps: Squeezing & visibility in interferometry
First Results from the K-State MOTRIMS Experiment
PHSC 1013: Physical Science Waves
STATE VARIABLE Speed of a wave v.
Anomalous broadening of driven Rydberg atoms
Volume 101, Issue 4, Pages (August 2011)
University of California, Berkeley
Norm Moulton LPS 15 October, 1999
Quantitative Analysis of the Viscoelastic Properties of Thin Regions of Fibroblasts Using Atomic Force Microscopy  R.E. Mahaffy, S. Park, E. Gerde, J.
Entangling Atoms with Optical Frequency Combs
Electronically Resonant Coherent Multidimensional Vibrational Spectroscopy John C. Wright, Department of Chemistry, University of Wisconsin- Madison Coherent.
JLEIC Weekly R&D Meeting
Presentation transcript:

Cold atoms in Optical lattice, vibrational states, coherent control via interference between one- and two-phonon excitation, and a little bit about decoherence, Chao Zhuang Quantum Optics Day 2009 Department of Physics University of Toronto Aephraim Steinberg Luciano Cruz Samansa Maneshi Nick Chisholm Ardavan Darabi XiaoXian Liu Chris Paul

Outline Experiment Setup Things I will talk about Interference between one- and two-phonon excitation Coherent control using one- and two-phonon Possible way of probing decoherence Things I will talk a little about Echo experiment Pump-probe experiment

Experiment Setup

1D vertical lattice 1D optical lattice: interference of two laser beams g

Cold atoms in optical lattice g Dilute gas No interaction between atoms Fluorescence image Optical Lattice: Lattice spacing : a ~ 0.93μm ER ~ 32nK, U0 =(18-20)ER = (580-640)nK =103 atoms/plain Photon scattering rate ~ 60ms to 100ms MOT: Cold 85Rb atoms T ~ 10μK =1010atoms/cm3

Prepare and measure the states Initial Lattice After adiabatic decrease Thermal state Well Depth t(ms) t1 t1+40

Prepare and measure the states Initial Lattice After adiabatic decrease t1+40 2 bound states t1 7 ms 1 bound state Well Depth t(ms) Isolated ground state

Prepare and measure the states Initial Lattice After adiabatic decrease t1+40 2 bound states t1 7 ms 1 bound state Well Depth t(ms) Isolated ground state

Operations of lattice Use AOM to control the relative phase between the two lattice beams equivalent to displace the lattice in the real space Use AOM to control the intensity of the lattice beam equivalent to change the lattice depth

PM and AM Phase modulation (PM) Amplitude modulation (AM) Relative phase Amplitude modulation (AM) Intensity of laser beam

Things I will talk about

Interference! No Interference No interference Constructive Destructive

One- v.s. two- phonon excitation Interference between the transition probability of the one-phonon excitation and two-phonon excitation aPM aAM

Typical Experiment Data! AM 20% 8cyc TAM = 100ms PM 6o 4cyc TPM = 200ms

How to change the PM loss Experiment Data Simulation aPM aPM

Search with different PM loss Experiment Data Simulation

Coherent control, one v.s. two Branching Ratio

Only relative phase is varied Experiment Data Simulation Red lines indicate different Branching Ratio

Decoherence probe?

Things I will talk a little about

Decoherence Coherence Possible source of decoherence The ability to interfere A stable relative phase Possible source of decoherence Atoms see different lattice depths Atoms move in transverse plain Tunneling from one well to another Photon scattering

Echo experiment Atoms see different lattice depths, but each atom sees only one lattice depth relative phase between ground and excited states Decoherence: dephasing Reverse the ground state and excited state at time T, rephase at 2T, by probing at different 2T, decoherence due to other sources can be observed Each runner has a different constant running speed

Higher-order echo Each runner with a constant acceleration Atoms are moving, which means the lattice depth each atom sees is changing N-th order echo can fix (N-1)-th time depend frequency drift 2nd order echo: T-reverse-2T-reverse-T-revive 3rd order echo: T-reverse-(1+√2)T-reverse - (1+√2)T-reverse-T-revive

Pump-probe experiment 2D contour plot

Generic way to predict echo decay 2ms Delay 5ms Delay 0 1 2 N t ...

Thank you! One more comment: Interference is EVERYWHERE and USEFUL!