Kevin J. Weatherill. Joint Quantum Centre (Durham-Newcastle) Department of Physics Durham University

Similar documents
Joint Quantum Centre Durham/Newcastle. Durham

Cooperative atom-light interaction in a blockaded Rydberg ensemble

Microwave Control of the Interaction Between Two Optical Photons. David Szwer 09/09/ / 40

Cold Polar Molecules and their Applications for Quantum Information H.P. Büchler

Exploring long-range interacting quantum many-body systems with Rydberg atoms

Slow and stored light using Rydberg atoms

Rydberg excited Calcium Ions for quantum interactions

arxiv: v1 [quant-ph] 22 May 2012

Ultracold molecules - a new frontier for quantum & chemical physics

Single Emitter Detection with Fluorescence and Extinction Spectroscopy

Chapter4: Quantum Optical Control

Lifetimes of ultralong range Rydberg molecules in a dense Bose Einstein condensate

Non-equilibrium spin systems - from quantum soft-matter to nuclear magnetic resonance

Michael Fleischhauer. Dept. of Physics & research center OPTIMAS University of Kaiserslautern, Germany. GRK 1729, Hannover,

Rydberg excited Calcium Ions for quantum interactions. Innsbruck Mainz Nottingham

Optical Lattice Clock with Spin-1/2 Ytterbium Atoms. Nathan D. Lemke

Optical Gain and Multi-Quantum Excitation in Optically Pumped Alkali Atom Rare Gas Mixtures

Andy Schwarzkopf Raithel Lab 1/20/2010

Chapter 2: Interacting Rydberg atoms

Microwave control of the interaction between two optical photons

What happens when light falls on a material? Transmission Reflection Absorption Luminescence. Elastic Scattering Inelastic Scattering

Ho:YLF pumped HBr laser

Cooperative Phenomena

High Resolution Laser Spectroscopy of Cesium Vapor Layers with Nanometric Thickness

OPTICAL GAIN AND LASERS

1. Transition dipole moment

Quantum optics of many-body systems

Wolfgang Demtroder. Laser Spectroscopy. Basic Concepts and Instrumentation. Second Enlarged Edition With 644 Figures and 91 Problems.

Chem 442 Review of Spectroscopy

Graphene for THz technology

Application of IR Raman Spectroscopy

requency generation spectroscopy Rahul N

Simple strategy for enhancing terahertz emission from coherent longitudinal optical phonons using undoped GaAs/n-type GaAs epitaxial layer structures

The Center for Ultracold Atoms at MIT and Harvard Theoretical work at CUA. NSF Visiting Committee, April 28-29, 2014

Introduction to Atomic Physics and Quantum Optics

Quantum Computation with Neutral Atoms Lectures 14-15

Chapter 29 Molecular and Solid-State Physics

Nonlinear Electrodynamics and Optics of Graphene

Quantum Many-Body Phenomena in Arrays of Coupled Cavities

Effect of nonlinearity on wave scattering and localization. Yuri S. Kivshar

Advanced Spectroscopy Laboratory

Module 4 : Third order nonlinear optical processes. Lecture 28 : Inelastic Scattering Processes. Objectives

Seminars in Nanosystems - I

The phases of matter familiar for us from everyday life are: solid, liquid, gas and plasma (e.f. flames of fire). There are, however, many other

Search for Quantum Coherence in Nanometer-scale targets

Chemistry Instrumental Analysis Lecture 5. Chem 4631

Molecular spectroscopy

Small Signal Gain in DPAL Systems

Introduction to Modern Quantum Optics

PHYS598 AQG Introduction to the course

Quantum information processing with individual neutral atoms in optical tweezers. Philippe Grangier. Institut d Optique, Palaiseau, France

From cavity optomechanics to the Dicke quantum phase transition

Wavelength λ Velocity v. Electric Field Strength Amplitude A. Time t or Distance x time for 1 λ to pass fixed point. # of λ passing per s ν= 1 p

PC Laboratory Raman Spectroscopy

Harvard University Physics 284 Spring 2018 Strongly correlated systems in atomic and condensed matter physics

Ground state cooling via Sideband cooling. Fabian Flassig TUM June 26th, 2013

Physics and Chemistry with Diatomic Molecules Near Absolute Zero. Tanya Zelevinsky & ZLab Columbia University, New York

Richard Miles and Arthur Dogariu. Mechanical and Aerospace Engineering Princeton University, Princeton, NJ 08540, USA

Introduction to Nonlinear Optics

Lecture 11, May 11, 2017

Introduction to Atomic Physics and Quantum Optics

arxiv:quant-ph/ v1 10 Aug 2005

Quantum Computation with Neutral Atoms

Separation of molecules by chirality using circularly polarized light

Okinawa School in Physics 2017 Coherent Quantum Dynamics. Cold Rydberg gases

Wednesday 3 September Session 3: Metamaterials Theory (16:15 16:45, Huxley LT308)

(Noise) correlations in optical lattices

CONTENTS. 2 CLASSICAL DESCRIPTION 2.1 The resonance phenomenon 2.2 The vector picture for pulse EPR experiments 2.3 Relaxation and the Bloch equations

Comparison between optical bistabilities versus power and frequency in a composite cavity-atom system

CHAPTER 13 Molecular Spectroscopy 2: Electronic Transitions

Laser Physics OXFORD UNIVERSITY PRESS SIMON HOOKER COLIN WEBB. and. Department of Physics, University of Oxford

(Al,In)GaN laser diodes in spectral, spatial, and time domain: near-field measurements and basic simulations

arxiv: v3 [quant-ph] 22 Dec 2012

Cavity QED: Quantum Control with Single Atoms and Single Photons. Scott Parkins 17 April 2008

A Quantum Gas Microscope for Detecting Single Atoms in a Hubbard regime Optical Lattice

Prospects for a superradiant laser

Measuring Spin-Lattice Relaxation Time

Supporting Information

Applications of Terahertz Radiation (T-ray) Yao-Chang Lee, National Synchrotron Research Radiation Center

Multi-cycle THz pulse generation in poled lithium niobate crystals

Survey on Laser Spectroscopic Techniques for Condensed Matter

Distributing Quantum Information with Microwave Resonators in Circuit QED

Cavity QED with quantum dots in microcavities

24/ Rayleigh and Raman scattering. Stokes and anti-stokes lines. Rotational Raman spectroscopy. Polarizability ellipsoid. Selection rules.

Model Answer (Paper code: AR-7112) M. Sc. (Physics) IV Semester Paper I: Laser Physics and Spectroscopy

ANALYSIS OF AN INJECTION-LOCKED BISTABLE SEMICONDUCTOR LASER WITH THE FREQUENCY CHIRPING

Elements of Quantum Optics

Mutual transparency of coherent laser beams through a terahertz-field-driven quantum well

A laser system for the excitation of rubidium Rydberg states using second harmonic generation in a PPLN waveguide crystal

Energy Transfer Upconversion Processes

Precision Interferometry with a Bose-Einstein Condensate. Cass Sackett. Research Talk 17 October 2008

Supplementary Figures

Polariton Condensation

Comments to Atkins: Physical chemistry, 7th edition.

High Accuracy Strontium Ion Optical Clock

Quantum defect and fine-structure measurements of P, D, F and G Rydberg states of atomic caesium

Atoms, Molecules and Solids. From Last Time Superposition of quantum states Philosophy of quantum mechanics Interpretation of the wave function:

Ytterbium quantum gases in Florence

Single-photon cesium Rydberg excitation spectroscopy using nm UV laser and room-temperature vapor cell

Laser stabilization via saturated absorption spectroscopy of iodine for applications in laser cooling and Bose-Einstein condensate creation

Transcription:

Non-equilibrium phase transition in a dilute thermal gas. Joint Quantum Centre (Durham-Newcastle) Department of Physics Durham University

Non-equilibrium phase transition in a dilute thermal gas. Talk Outline 1. Non-linear optics using Rydberg atoms 2. Optical bistability and phase transitions 3. Experiment and results 4. Outlook: Non-local effects and THz detection? 5. Acknowledgements

Rydberg Atoms s p d Rydberg states: large n (>20) Scaling with principal quantum number n Size n 2 Dipole moment n 2 Lifetime n 3 long lived Polarizability n 7 Sensitive to electric fields Van der Waals n 11 Strong atom-atom interactions Dipole moment n -3/2 Weak atom-light interactions of optical transitions

Rydberg Atoms s p d Rydberg states: large n (>20) Scaling with principal quantum number n Size n 2 Dipole moment n 2 Lifetime n 3 long lived Polarizability n 7 Sensitive to electric fields Van der Waals n 11 Strong atom-atom interactions Dipole moment n -3/2 Weak atom-light interactions of optical transitions Range of interaction >> interatomic spacing > excitation wavelength

Rydberg Atoms s p d Rydberg states: large n (>20) Scaling with principal quantum number n Size n 2 Dipole moment n 2 Lifetime n 3 long lived Polarizability n 7 Sensitive to electric fields Van der Waals n 11 Strong atom-atom interactions Dipole moment n -3/2 Weak atom-light interactions of optical transitions Range of interaction >> interatomic spacing > excitation wavelength Strongly interacting systems

Rydberg Non-linear (and Quantum) Optics. Back-action on the light field. 2007 Coherent optical detection of Rydberg atoms (Adams: Durham)

Rydberg Non-linear (and Quantum) Optics. Back-action on the light field. 2007 Coherent optical detection of Rydberg atoms (Adams: Durham) 2008 Giant DC Kerr non-linearities E field sensitivity

Rydberg Non-linear (and Quantum) Optics. Back-action on the light field. 2007 Coherent optical detection of Rydberg atoms (Adams: Durham) 2008 Giant DC Kerr non-linearities E field sensitivity 2010 Cooperative optical non-linearities Atom-atom interactions

Rydberg Non-linear (and Quantum) Optics. Back-action on the light field. 2007 Coherent optical detection of Rydberg atoms (Adams: Durham) 2008 Giant DC Kerr non-linearities E field sensitivity 2010 Cooperative optical non-linearities Atom-atom interactions 2012 Single photon sources (Kuzmich: Georgia-Tech, Lukin + Vuletic, Harvard) 2013 Microwave controlled interactions between optical photons (Adams, Durham) 2013 Single photon switch (Durr + Rempe, Garching) + many others Pfau, Weidemuller, Grangier, Spreeuw etc. Non-linear optics using cold Rydberg Atoms J. D. Pritchard, K. J. Weatherill and C. S. Adams Annual Review of Cold Atoms and Molecules 1, 301 (2013) Arxiv:1205.4890

Intrinsic Optical Bistability First- and second-order phase transitions in the Dicke model: Relation to optical bistability Bowden and Sung, Phys. Rev. A 19, 2393 (1979) feedback Experimental observation using Yb ions in crystal Atoms 31 K Simple Optical Bloch model 27 K 23 K 19 K 15 K 11 K Can we observe intrinsic optical bistability in a dilute Rydberg gas at room temperature? Hehlen et al, Phys. Rev. Lett. 73, 1103 (1994)

Experiment: Three Step Excitation Scheme. Caesium Cheap, convenient and simple to use IR diode lasers High power and wide tunability on final step 21

3-photon spectroscopy. Scanned Locked Locked Probe Cooperative non-equilibrium phase transition in a dilute Rydberg ensemble C. Carr, C. Wade, R. Ritter, C. S. Adams and K. J. Weatherill, Phys Rev. Lett 111, 113901(2013) 22

3-photon spectroscopy. Scanned Locked Locked Probe Cooperative non-equilibrium phase transition in a dilute Rydberg ensemble C. Carr, C. Wade, R. Ritter, C. S. Adams and K. J. Weatherill, Phys Rev. Lett 111, 113901(2013) 23

Fluorescence Spectra. transmission fluorescence Spectrometer and PMT Lasers Cooperative non-equilibrium phase transition in a dilute Rydberg ensemble C. Carr, C. Wade, R. Ritter, C. S. Adams and K. J. Weatherill, Phys Rev. Lett 111, 113901 (2013) 24

Fluorescence Spectra. transmission fluorescence Spectrometer and PMT Lasers Cooperative non-equilibrium phase transition in a dilute Rydberg ensemble C. Carr, C. Wade, R. Ritter, C. S. Adams and K. J. Weatherill, Phys Rev. Lett 111, 113901 (2013) 25

Fluorescence Spectra. transmission fluorescence Spectrometer and PMT Lasers Cooperative non-equilibrium phase transition in a dilute Rydberg ensemble C. Carr, C. Wade, R. Ritter, C. S. Adams and K. J. Weatherill, Phys Rev. Lett 111, 113901 (2013) 26

Fluorescence Spectra. transmission fluorescence Spectrometer and PMT Lasers Cooperative non-equilibrium phase transition in a dilute Rydberg ensemble C. Carr, C. Wade, R. Ritter, C. S. Adams and K. J. Weatherill, Phys Rev. Lett 111, 113901 (2013) 27

Fluorescence Spectra. transmission fluorescence Spectrometer and PMT Lasers Cooperative non-equilibrium phase transition in a dilute Rydberg ensemble C. Carr, C. Wade, R. Ritter, C. S. Adams and K. J. Weatherill, Phys Rev. Lett 111, 113901 (2013) 28

Longitudinal Phase Transition Lasers Cooperative non-equilibrium phase transition in a dilute Rydberg ensemble C. Carr, C. Wade, R. Ritter, C. S. Adams and K. J. Weatherill, Phys Rev. Lett 111, 113901 (2013)

Critical Slowing Down Critical slowing down is key signature of OB and phase transition. G. Grynberg et al, J. Phys. Lett. 44, 449 (1983)

Non-equilibrium phase transition in a dilute thermal gas. Extreme regime with strong driving and strong dissipation Laser driving superradiant dissipation Simple Optical Bloch model dynamic equilibrium Mean-field effect from long-range and thermally averaged atom-atom interactions Quantum soft matter?

Outlook. Interesting new regime with Interesting possibilities. THz Can we detect THz radiation? lasers Non-local switching experiments? Investigate geometric effects on Superradiance? And lots more.. Quantum statistics of photons etc.

Recap. Talk Outline 1. Non-linear optics using Rydberg atoms 2. Optical Bistability and phase transitions 3. Experiment and results 4. Outlook: Non-local effects and THz detection?

Acknowledgements Chris Carr, Ralf Ritter, Chris Wade, Charles Adams. Seedcorn award. EU Marie Curie ITN COHERENCE Network.