Les Houches 2009: Metastable Helium Atom Laser
|
|
- Blake Banks
- 6 years ago
- Views:
Transcription
1 Les Houches 2009: Metastable Helium Atom Laser Les Houches, Chamonix, February 2005
2 Australian Research Council Centre of Excellence for Quantum-Atom Optics UQ Brisbane SUT Melbourne ANU Canberra
3 Snowy Mountains, Australia - September 2006
4 Metastable Helium Atom Optics He 2 3 S 1 (He*) is the longest lived (~8000s) atomic metastable state yet measured (SEAN S TALK). Metastable helium: Atom optics with nano-grenades, K.G.H. Baldwin, Contemporary Physics 46, 105 (2005). We first developed a bright He* beam line for cold atom studies Electron - He* collisions Atom lithography Atom guiding in hollow fibres We now have a He* BEC apparatus for ultracold atom and BEC studies Energy singlets 3 1 S o 2 1 S o 3 3 D P S 1 triplets 3 3 P nm trap laser (metastable) 389 nm laser Atom laser studies Atomic physics - He* lifetimes Quantum statistical effects 1 1 S o 19.8 ev electron excitation
5 He* BEC Facility LVIS ~ 2 x He* / s Vel. ~ 30 m / s Trap ~ 5 x 10 8 He* at ~ 1 mk He* atom source Low Velocity Intense Source (LVIS) BEC trap chamber (UHV) Load ~ 2x10 10 He*/s Vel. ~ m/s Trap ~ 3x10 9 He* Laser collimation Laser trap Slowing laser
6 Magnetic Trap 1 cm 1 cm 1 cm Equivalent coil configurations BEC ~ 3x10 6 He* at ~ 1μK Highly stable magnetic field trapping potential ~10-5 gauss BiQUIC magnetic trap coils
7 BEC chamber He* in Magnetic trap BEC 1 cm 1st MOT 2nd MOT Re-entrant window (top view)
8 He* BEC Experiments: 2D spatial profile MCP and phosphor 2-D detector T > T c T < T c T ~ 0.3T c
9 BEC vs. Atom Laser Slowly cool to increase db and occupy the ground state Further cool and force other atoms into ground state via stimulated Bosonic emission de Broglie waves in the lowest mode of the trap ( cavity ) form a single quantum state with the same wavelength and the same phase Only need to output couple to form an atom laser beam
10 RF Outcoupling Atom Laser 25 m f = RF coupling rf1 m f = 0 g MCP Detector
11 Atom Laser Noise Without stabilisation With stabilisation Atom laser output Power spectrum 100 times suppression
12 Atom laser spatial profile - less than ideal Reason: Initial theory by Th. Busch, M. Kohl, T. Esslinger and K. Mølmer, PRA 65, (2002) the chemical potential gradient not only spreads the atom laser beam => but atom trajectories with same final position yield quantum interference
13 Rb c.f. He* atom laser experiments Riou et al. (Orsay) theory and expt. PRL 96, (2006) Our He* experimental results Opt. Exp. 26, (2007)
14 Rb vs. He*: out-coupling surfaces Rb atoms experience a large sag - almost flat outcoupling surface He* atoms experience little sag - spherical shells
15 Fountain Effect
16 Simulated atom laser transverse spatial profiles Strong trap (460 Hz - small sag) output - coupled from near the trap centre Weak trap (50 Hz - large sag) Low frequency (horizontal) interference fringes High frequency (vertical) interference fringes Distance on MCP (a.u.)
17 Atom Laser Profile Dip in shadow of BEC Structure? Twin peaked structure
18 First observation of fringes
19 High output-coupling fringes
20 Profiles for two radial frequencies rf = 10 khz f r = 460 Hz f r = 113 Hz rf = 6 khz rf = 4 khz rf = 1 khz 3.1 mm rf = 3 khz 10 mm rf = 0.5 khz
21 He* Atom Laser: Conclusions Measured spatial profile of a He* atom laser Observed predicted interference fringes for the first time Atom laser beam not ideal - highly multimode transverse spatial profile
22 Q: How do we fix the horrible spatial profile of the He* atom laser? A: By matter wave guiding in an optical dipole potential.
23 Guerin et al. PRL (2006) - Orsay Hybrid trap - a magnetic trap crossed with an optical dipole guiding beam - and RF output coupled into the dipole guide Mode occupancy inferred from the transverse energy spread, with ~14% in lowest order mode
24 Couvert et al. EPL (2008) - ENS Crossed dipole trap which is outcoupled horizontally by an inhomogeneous magnetic field m F = -1 m F = 0 Mode occupancy inferred from the transverse energy spread, with ~50% in lowest order mode
25 ANU optical atom waveguide He* atoms cooled to ~1 μk in a magnetic trap BEC Atoms transferred to an optical dipole trap (1500 x 1075 x 23 Hz) and condensed to BEC Laser intensity reduced from 41 to 17 mw over 100 ms Far-detuned optical dipole potential from a 50 mw, 1550nm laser focused to 30 μm 200 mm Atoms no longer trapped and fall under gravity onto MCP 2D spatial detector (MCP)
26 Waveguide results BEC dropped onto MCP Atom laser profile Nearly single mode guided matter waves
27 Stern-Gerlach separation m F = -1 m F = 0 m F = +1
28 Guided image Expanded view of guided image: 1 pixel = 50 μm
29 Dual Gaussian Fit Close to theoretically predicted width Total profile Lowest order mode > 70% Additional modes
30 Multimode vs. single mode Single mode guiding (same pixel scale) Multimode guiding - note speckle pattern
31 Averaged multimode 1 3 multimode guided images average of Single mode (same scale)
32 Diffracted image Guided atoms diffracted through Quantifoil R2/2 (2 micron holes separated by 2 microns in carbon film) Single mode Multimode
33 3D - Diffracted image (B) (A)
34 Conclusions Optically trapped He* BEC is coupled into a far-detuned dipole potential waveguide Output of waveguide is mostly single mode (> 70%) Multimode excitation produces a speckle pattern Speckle pattern averages to a smooth profile much larger than the single mode guided image Significantly improved beam quality c.f. atom laser beam Potential applications to guided atom interferometry
35 He* BEC experiment Oscar Turazza Robert Dall Lesa Byron Sean Hodgman Andrew Truscott
36 Blue Lake, Snowy Mountains, Australia, 2004 Thank you for your attention!
37 Magnetic Field Nuller Separate feedback circuits Feedback Amplifier Helmholtz Coils Sensors Trap Centre x - axis Magnetic flux gate + pickup coils (16Hz crossover) C.J. Dedman, R.G. Dall, L.J. Byron, and A.G. Truscott, Review of Scientific Instruments 78, (2007)
38 DC magnetic noise Feedback Enabled
39 Atom Laser Coherence (2 frequency outcoupling) Above T c I. Bloch, T. W. Hänsch and T. Esslinger. Nature 403, (13 January 2000) Below T c
Quantum correlations and atomic speckle
Quantum correlations and atomic speckle S. S. Hodgman R. G. Dall A. G. Manning M. T. Johnsson K. G. H. Baldwin A. G. Truscott ARC Centre of Excellence for Quantum-Atom Optics, Research School of Physics
More informationMultipath Interferometer on an AtomChip. Francesco Saverio Cataliotti
Multipath Interferometer on an AtomChip Francesco Saverio Cataliotti Outlook Bose-Einstein condensates on a microchip Atom Interferometry Multipath Interferometry on an AtomChip Results and Conclusions
More information(Noise) correlations in optical lattices
(Noise) correlations in optical lattices Dries van Oosten WA QUANTUM http://www.quantum.physik.uni mainz.de/bec The Teams The Fermions: Christoph Clausen Thorsten Best Ulrich Schneider Sebastian Will Lucia
More informationLecture 3. Bose-Einstein condensation Ultracold molecules
Lecture 3 Bose-Einstein condensation Ultracold molecules 66 Bose-Einstein condensation Bose 1924, Einstein 1925: macroscopic occupation of the lowest energy level db h 2 mk De Broglie wavelength d 1/3
More informationAtom lasers. FOMO summer school 2016 Florian Schreck, University of Amsterdam MIT 1997 NIST Munich Yale 1998
Atom lasers MIT 1997 Yale 1998 NIST 1999 Munich 1999 FOMO summer school 2016 Florian Schreck, University of Amsterdam Overview What? Why? Pulsed atom lasers Experiments with atom lasers Continuous atom
More informationIntroduction to Cold Atoms and Bose-Einstein Condensation. Randy Hulet
Introduction to Cold Atoms and Bose-Einstein Condensation Randy Hulet Outline Introduction to methods and concepts of cold atom physics Interactions Feshbach resonances Quantum Gases Quantum regime nλ
More informationConfining ultracold atoms on a ring in reduced dimensions
Confining ultracold atoms on a ring in reduced dimensions Hélène Perrin Laboratoire de physique des lasers, CNRS-Université Paris Nord Charge and heat dynamics in nano-systems Orsay, October 11, 2011 What
More informationQuantum Mechanica. Peter van der Straten Universiteit Utrecht. Peter van der Straten (Atom Optics) Quantum Mechanica January 15, / 22
Quantum Mechanica Peter van der Straten Universiteit Utrecht Peter van der Straten (Atom Optics) Quantum Mechanica January 15, 2013 1 / 22 Matrix methode Peter van der Straten (Atom Optics) Quantum Mechanica
More informationCold Metastable Neon Atoms Towards Degenerated Ne*- Ensembles
Cold Metastable Neon Atoms Towards Degenerated Ne*- Ensembles Supported by the DFG Schwerpunktprogramm SPP 1116 and the European Research Training Network Cold Quantum Gases Peter Spoden, Martin Zinner,
More informationIntroduction to cold atoms and Bose-Einstein condensation (II)
Introduction to cold atoms and Bose-Einstein condensation (II) Wolfgang Ketterle Massachusetts Institute of Technology MIT-Harvard Center for Ultracold Atoms 7/7/04 Boulder Summer School * 1925 History
More informationA novel 2-D + magneto-optical trap configuration for cold atoms
A novel 2-D + magneto-optical trap configuration for cold atoms M. Semonyo 1, S. Dlamini 1, M. J. Morrissey 1 and F. Petruccione 1,2 1 Quantum Research Group, School of Chemistry & Physics, University
More informationBEC of 6 Li 2 molecules: Exploring the BEC-BCS crossover
Institut für Experimentalphysik Universität Innsbruck Dresden, 12.10. 2004 BEC of 6 Li 2 molecules: Exploring the BEC-BCS crossover Johannes Hecker Denschlag The lithium team Selim Jochim Markus Bartenstein
More informationAtom Quantum Sensors on ground and in space
Atom Quantum Sensors on ground and in space Ernst M. Rasel AG Wolfgang Ertmer Quantum Sensors Division Institut für Quantenoptik Leibniz Universität Hannover IQ - Quantum Sensors Inertial Quantum Probes
More informationBose-Einstein Condensate: A New state of matter
Bose-Einstein Condensate: A New state of matter KISHORE T. KAPALE June 24, 2003 BOSE-EINSTEIN CONDENSATE: A NEW STATE OF MATTER 1 Outline Introductory Concepts Bosons and Fermions Classical and Quantum
More informationUltracold Fermi Gases with unbalanced spin populations
7 Li Bose-Einstein Condensate 6 Li Fermi sea Ultracold Fermi Gases with unbalanced spin populations Nir Navon Fermix 2009 Meeting Trento, Italy 3 June 2009 Outline Introduction Concepts in imbalanced Fermi
More informationMicrofibres for Quantum Optics. Dr Síle Nic Chormaic Quantum Optics Group
Microfibres for Quantum Optics Dr Síle Nic Chormaic Quantum Optics Group Motivation Strong need to engineer atoms and photons for the development of new technologies quantum technologies Future advances
More informationDevelopment of a compact Yb optical lattice clock
Development of a compact Yb optical lattice clock A. A. Görlitz, C. Abou-Jaoudeh, C. Bruni, B. I. Ernsting, A. Nevsky, S. Schiller C. ESA Workshop on Optical Atomic Clocks D. Frascati, 14 th 16 th of October
More informationarxiv: v2 [physics.atom-ph] 9 Oct 2008
Probing a Bose-Einstein condensate with an atom laser arxiv:8.477v2 [physics.atom-ph] 9 Oct 28 D. Döring, N. P. Robins, C. Figl, and J. D. Close Australian Research Council Centre of Excellence for Quantum-Atom
More informationHong Ou Mandel experiment with atoms
BEC on an MCP Hong Ou Mandel experiment with atoms Chris Westbrook Laboratoire Charles Fabry, Palaiseau FRISNO 13, Aussois 18 march 2015 2 particles at a beam splitter 1 particle at each input 4 possibilities:
More informationLecture 2. Trapping of neutral atoms Evaporative cooling. Foot 9.6, , 10.5
Lecture Trapping of neutral atoms Evaporative cooling Foot 9.6, 10.1-10.3, 10.5 34 Why atom traps? Limitation of laser cooling temperature (sub)-doppler (sub)-recoil density light-assisted collisions reabsorption
More informationThe Hanbury Brown Twiss effect for matter waves. Chris Westbrook Laboratoire Charles Fabry, Palaiseau Workshop on HBT interferometry 12 may 2014
The Hanbury Brown Twiss effect for matter waves Chris Westbrook Laboratoire Charles Fabry, Palaiseau Workshop on HBT interferometry 12 may 2014 Outline: Hanbury Brown Twiss effect... 1.... in optics and
More informationTowards compact transportable atom-interferometric inertial sensors
Towards compact transportable atom-interferometric inertial sensors G. Stern (SYRTE/LCFIO) Increasing the interrogation time T is often the limiting parameter for the sensitivity. Different solutions:
More informationHong-Ou-Mandel effect with matter waves
Hong-Ou-Mandel effect with matter waves R. Lopes, A. Imanaliev, A. Aspect, M. Cheneau, DB, C. I. Westbrook Laboratoire Charles Fabry, Institut d Optique, CNRS, Univ Paris-Sud Progresses in quantum information
More informationBose-Einstein condensates & tests of quantum mechanics
Bose-Einstein condensates & tests of quantum mechanics Poul Lindholm Pedersen Ultracold Quantum Gases Group PhD day, 31 10 12 Bose-Einstein condensation T high Classical particles T = 0 Pure condensate
More informationPROGRESS TOWARDS CONSTRUCTION OF A FERMIONIC ATOMIC CLOCK FOR NASA S DEEP SPACE NETWORK
PROGRESS TOWARDS CONSTRUCTION OF A FERMIONIC ATOMIC CLOCK FOR NASA S DEEP SPACE NETWORK Megan K. Ivory Advisor: Dr. Seth A. Aubin College of William and Mary Atomic clocks are the most accurate time and
More informationQuantum Gases. Subhadeep Gupta. UW REU Seminar, 11 July 2011
Quantum Gases Subhadeep Gupta UW REU Seminar, 11 July 2011 Ultracold Atoms, Mixtures, and Molecules Subhadeep Gupta UW REU Seminar, 11 July 2011 Ultracold Atoms High sensitivity (large signal to noise,
More informationQuantum Computing with neutral atoms and artificial ions
Quantum Computing with neutral atoms and artificial ions NIST, Gaithersburg: Carl Williams Paul Julienne T. C. Quantum Optics Group, Innsbruck: Peter Zoller Andrew Daley Uwe Dorner Peter Fedichev Peter
More informationPrecision Interferometry with a Bose-Einstein Condensate. Cass Sackett. Research Talk 17 October 2008
Precision Interferometry with a Bose-Einstein Condensate Cass Sackett Research Talk 17 October 2008 Outline Atom interferometry Bose condensates Our interferometer One application What is atom interferometry?
More informationQuantum superpositions and correlations in coupled atomic-molecular BECs
Quantum superpositions and correlations in coupled atomic-molecular BECs Karén Kheruntsyan and Peter Drummond Department of Physics, University of Queensland, Brisbane, AUSTRALIA Quantum superpositions
More informationPROGRESS TOWARDS CONSTRUCTION OF A FERMION ATOMIC CLOCK FOR NASA S DEEP SPACE NETWORK
PROGRESS TOWARDS CONSTRUCTION OF A FERMION ATOMIC CLOCK FOR NASA S DEEP SPACE NETWORK Megan K. Ivory Advisor: Dr. Seth A. Aubin College of William and Mary Abstract: The most accurate time and frequency
More informationMatter wave interferometry beyond classical limits
Max-Planck-Institut für Quantenoptik Varenna school on Atom Interferometry, 15.07.2013-20.07.2013 The Plan Lecture 1 (Wednesday): Quantum noise in interferometry and Spin Squeezing Lecture 2 (Friday):
More informationCondensation of Excitons in a Trap
Condensation of Excitons in a Trap I (arb. units) Alex High, Jason Leonard, Mikas Remeika, & Leonid Butov University of California at San Diego Micah Hanson & Art Gossard University of California at Santa
More informationProgress on Atom Interferometer (AI) in BUAA
Progress on Atom Interferometer (AI) in BUAA Group of Prof. FANG Jiancheng Beihang University ZHANG Yuchi, Hu Zhaohui, QI Lu, WANG Tongyu, WANG Tao 01.09.2011 7 th UK-China Workshop on Space Science and
More informationNon-equilibrium Dynamics in Ultracold Fermionic and Bosonic Gases
Non-equilibrium Dynamics in Ultracold Fermionic and Bosonic Gases Michael KöhlK ETH Zürich Z (www.quantumoptics.ethz.ch( www.quantumoptics.ethz.ch) Introduction Why should a condensed matter physicist
More informationLaser Cooling of Thulium Atoms
Laser Cooling of Thulium Atoms N. Kolachevsky P.N. Lebedev Physical Institute Moscow Institute of Physics and Technology Russian Quantum Center D. Sukachev E. Kalganova G.Vishnyakova A. Sokolov A. Akimov
More informationIn Situ Imaging of Cold Atomic Gases
In Situ Imaging of Cold Atomic Gases J. D. Crossno Abstract: In general, the complex atomic susceptibility, that dictates both the amplitude and phase modulation imparted by an atom on a probing monochromatic
More informationDept. of Physics, MIT Manipal 1
Chapter 1: Optics 1. In the phenomenon of interference, there is A Annihilation of light energy B Addition of energy C Redistribution energy D Creation of energy 2. Interference fringes are obtained using
More informationYtterbium quantum gases in Florence
Ytterbium quantum gases in Florence Leonardo Fallani University of Florence & LENS Credits Marco Mancini Giacomo Cappellini Guido Pagano Florian Schäfer Jacopo Catani Leonardo Fallani Massimo Inguscio
More informationUltracold atoms and molecules
Advanced Experimental Techniques Ultracold atoms and molecules Steven Knoop s.knoop@vu.nl VU, June 014 1 Ultracold atoms laser cooling evaporative cooling BEC Bose-Einstein condensation atom trap: magnetic
More informationExperiments with an Ultracold Three-Component Fermi Gas
Experiments with an Ultracold Three-Component Fermi Gas The Pennsylvania State University Ken O Hara Jason Williams Eric Hazlett Ronald Stites John Huckans Overview New Physics with Three Component Fermi
More informationA new experimental apparatus for quantum atom optics
A new experimental apparatus for quantum atom optics Andreas Hüper, Jiao Geng, Ilka Kruse, Jan Mahnke, Wolfgang Ertmer and Carsten Klempt Institut für Quantenoptik, Leibniz Universität Hannover Outline
More informationULTRACOLD METASTABLE HELIUM-4 AND HELIUM-3 GASES
ULTRACOLD METASTABLE HELIUM-4 AND HELIUM-3 GASES W. VASSEN, T. JELTES, J.M. MCNAMARA, A.S. TYCHKOV, W. HOGERVORST Laser Centre Vrije Universiteit Amsterdam, The Netherlands K.A.H. VAN LEEUWEN Dept. of
More informationOptical manipulation of atomic motion for a compact gravitational sensor with a Bose-Einstein condensate interferometer
Optical manipulation of atomic motion for a compact gravitational sensor with a Bose-Einstein condensate interferometer A Dissertation Presented to the Faculty of the School of Engineering and Applied
More informationNanoKelvin Quantum Engineering
NanoKelvin Quantum Engineering Few x 10 5 Yb atoms 250mm 400 nk 250 nk < 200 nk Control of atomic c.m. position and momentum. Today: Bose-Fermi double superfluid Precision BEC interferometry Ultracold
More informationProspects for a superradiant laser
Prospects for a superradiant laser M. Holland murray.holland@colorado.edu Dominic Meiser Jun Ye Kioloa Workshop D. Meiser, Jun Ye, D. Carlson, and MH, PRL 102, 163601 (2009). D. Meiser and MH, PRA 81,
More informationSome Topics in Optics
Some Topics in Optics The HeNe LASER The index of refraction and dispersion Interference The Michelson Interferometer Diffraction Wavemeter Fabry-Pérot Etalon and Interferometer The Helium Neon LASER A
More informationRealization of Bose-Einstein Condensation in dilute gases
Realization of Bose-Einstein Condensation in dilute gases Guang Bian May 3, 8 Abstract: This essay describes theoretical aspects of Bose-Einstein Condensation and the first experimental realization of
More informationHigh stability laser source for cold atoms applications
High stability laser source for cold atoms applications Cold atoms research, which historically started as part of the atomic physics field, has grown into a wide, highly interdisciplinary research effort.
More informationQuantum atom optics with Bose-Einstein condensates
Quantum atom optics with Bose-Einstein condensates Piotr Deuar Institute of Physics, Polish Academy of Sciences, Warsaw, Poland With particular thanks to: Chris Westbrook, Denis Boiron, J-C Jaskula, Alain
More informationDifferent ion-qubit choises. - One electron in the valence shell; Alkali like 2 S 1/2 ground state.
Different ion-qubit choises - One electron in the valence shell; Alkali like 2 S 1/2 ground state. Electronic levels Structure n 2 P 3/2 n 2 P n 2 P 1/2 w/o D Be + Mg + Zn + Cd + 313 nm 280 nm 206 nm 226
More informationPrecision atom interferometry in a 10 meter tower
Precision atom interferometry in a 10 meter tower Leibniz Universität Hannover RTG 1729, Lecture 1 Jason Hogan Stanford University January 23, 2014 Cold Atom Inertial Sensors Cold atom sensors: Laser cooling;
More informationSpontaneous topological defects in the formation of a Bose-Einstein condensate
Spontaneous topological defects in the formation of a Bose-Einstein condensate Matthew Davis 1, Ashton Bradley 1,, Geoff Lee 1, Brian Anderson 2 1 ARC Centre of Excellence for Quantum-Atom Optics, University
More informationDirect observation of quantum phonon fluctuations in ultracold 1D Bose gases
Laboratoire Charles Fabry, Palaiseau, France Atom Optics Group (Prof. A. Aspect) Direct observation of quantum phonon fluctuations in ultracold 1D Bose gases Julien Armijo* * Now at Facultad de ciencias,
More informationSpinor dynamics-driven formation of a dual-beam atom laser
Spinor dynamics-driven formation of a dual-beam atom laser N. Lundblad, R.J. Thompson, D.C. Aveline, and L. Maleki Jet Propulsion Laboratory, California Institute of Technology, 4800 Oak Grove Drive, Pasadena,
More informationOptimization of transfer of laser-cooled atom cloud to a quadrupole magnetic trap
PRAMANA c Indian Academy of Sciences Vol. 82, No. 2 journal of February 2014 physics pp. 419 423 Optimization of transfer of laser-cooled atom cloud to a quadrupole magnetic trap SPRAM, S K TIWARI, S R
More informationForca-G: A trapped atom interferometer for the measurement of short range forces
Forca-G: A trapped atom interferometer for the measurement of short range forces Bruno Pelle, Quentin Beaufils, Gunnar Tackmann, Xiaolong Wang, Adèle Hilico and Franck Pereira dos Santos Sophie Pelisson,
More informationLes Puces à Atomes. Jakob Reichel. Laboratoire Kastler Brossel de l E.N.S., Paris
Les Puces à Atomes Jakob Reichel Laboratoire Kastler Brossel de l E.N.S., Paris Atom chips: Cold atoms meet the nanoworld ~ 100 nm BEC (~ 10 5 atoms, ~ 100 nk) microstructured surface bulk material ( ~
More informationA Quantum Gas Microscope for Detecting Single Atoms in a Hubbard regime Optical Lattice
A Quantum Gas Microscope for Detecting Single Atoms in a Hubbard regime Optical Lattice Nature 462, 74 77 (5 November 2009) Team 6 Hyuneil Kim Zhidong Leong Yulia Maximenko Jason Merritt 1 Outline Background
More informationSYRTE - IACI. AtoM Interferometry dual Gravi- GradiOmeter AMIGGO. from capability demonstrations in laboratory to space missions
SYRTE - IACI AtoM Interferometry dual Gravi- GradiOmeter AMIGGO from capability demonstrations in laboratory to space missions A. Trimeche, R. Caldani, M. Langlois, S. Merlet, C. Garrido Alzar and F. Pereira
More informationA study of the BEC-BCS crossover region with Lithium 6
A study of the BEC-BCS crossover region with Lithium 6 T.Bourdel, L. Khaykovich, J. Cubizolles, J. Zhang, F. Chevy, M. Teichmann, L. Tarruell, S. Kokkelmans, Christophe Salomon Theory: D. Petrov, G. Shlyapnikov,
More informationExperimental AMO eets meets M odel Model Building: Part I (Precision Atom Interferometry)
Experimental AMO meets Model Building: Part I (Precision Atom Interferometry) Interference of Rb atoms Chiow, et. al, PRL, 2011 Young s double slit with atoms Young s 2 slit with Helium atoms Interference
More informationFrom laser cooling to BEC First experiments of superfluid hydrodynamics
From laser cooling to BEC First experiments of superfluid hydrodynamics Alice Sinatra Quantum Fluids course - Complement 1 2013-2014 Plan 1 COOLING AND TRAPPING 2 CONDENSATION 3 NON-LINEAR PHYSICS AND
More informationYbRb A Candidate for an Ultracold Paramagnetic Molecule
YbRb A Candidate for an Ultracold Paramagnetic Molecule Axel Görlitz Heinrich-Heine-Universität Düsseldorf Santa Barbara, 26 th February 2013 Outline 1. Introduction: The Yb-Rb system 2. Yb + Rb: Interactions
More informationQuantum Computation with Neutral Atoms Lectures 14-15
Quantum Computation with Neutral Atoms Lectures 14-15 15 Marianna Safronova Department of Physics and Astronomy Back to the real world: What do we need to build a quantum computer? Qubits which retain
More informationCold Magnesium Atoms for an Optical Clock
Cold Magnesium Atoms for an Optical Clock Tanja Mehlstäubler Jan Friebe Volker Michels Karsten Moldenhauer Nils Rehbein Dr. Hardo Stöhr Dr. Ernst-Maria Rasel Prof. Dr. Wolfgang Ertmer Institute of Quantum
More informationDipole traps and optical lattices for quantum simulations
Dipole traps and optical lattices for quantum simulations by Mathis Baumert A thesis submitted to The University of Birmingham for the degree of DOCTOR OF PHILOSOPHY Midlands Ultra-cold Atom Research Centre
More informationMetal Vapour Lasers Use vapoured metal as a gain medium Developed by W. Silfvast (1966) Two types: Ionized Metal vapour (He-Cd) Neutral Metal vapour
Metal Vapour Lasers Use vapoured metal as a gain medium Developed by W. Silfvast (1966) Two types: Ionized Metal vapour (He-Cd) Neutral Metal vapour (Cu) All operate by vaporizing metal in container Helium
More informationAll-optical formation of a Bose-Einstein condensate for applications in scanning electron microscopy
Appl. Phys. B manuscript No. (will be inserted by the editor) All-optical formation of a Bose-Einstein condensate for applications in scanning electron microscopy T. Gericke 1, P. Würtz 1, D. Reitz 1,
More informationSupported by NIST, the Packard Foundation, the NSF, ARO. Penn State
Measuring the electron edm using Cs and Rb atoms in optical lattices (and other experiments) Fang Fang Osama Kassis Xiao Li Dr. Karl Nelson Trevor Wenger Josh Albert Dr. Toshiya Kinoshita DSW Penn State
More informationShau-Yu Lan 藍劭宇. University of California, Berkeley Department of Physics
Atom Interferometry Experiments for Precision Measurement of Fundamental Physics Shau-Yu Lan 藍劭宇 University of California, Berkeley Department of Physics Contents Principle of Light-Pulse Atom Interferometer
More informationFringe spacing and phase of interfering matter waves
Fringe spacing and phase of interfering matter waves O. Vainio, 1,2 C. J. Vale, 1, * M. J. Davis, 1 N. R. Heckenberg, 1 and H. Rubinsztein-Dunlop 1 1 School of Physical Sciences, University of Queensland,
More informationQuantum Electronics Laser Physics PS Theory of the Laser Oscillation
Quantum Electronics Laser Physics PS407 6. Theory of the Laser Oscillation 1 I. Laser oscillator: Overview Laser is an optical oscillator. Resonant optical amplifier whose output is fed back into its input
More informationStudies of the Spin Dynamics of Charge Carriers in Semiconductors and their Interfaces. S. K. Singh, T. V. Shahbazyan, I. E. Perakis and N. H.
Studies of the Spin Dynamics of Charge Carriers in Semiconductors and their Interfaces S. K. Singh, T. V. Shahbazyan, I. E. Perakis and N. H. Tolk Department of Physics and Astronomy Vanderbilt University,
More information12 rad be Ω max 10 / Hz. This result is better by two orders of magnitude than any
1 Abstract Recent developments in spatial atom interferometry have stimulated new fields in atomic physics and quantum optics, opening up new areas in fundamental research. Moreover, there are ideas for
More informationCoherent manipulation of atomic wavefunctions in an optical lattice. V. V. Ivanov & A. Alberti, M. Schioppo, G. Ferrari and G. M.
Coherent manipulation of atomic wavefunctions in an optical lattice V. V. Ivanov & A. Alberti, M. Schioppo, G. Ferrari and G. M. Tino Group Andrea Alberti Marco Schioppo Guglielmo M. Tino me Gabriele Ferarri
More informationOptical Lattice Clock with Spin-1/2 Ytterbium Atoms. Nathan D. Lemke
Optical Lattice Clock with Spin-1/2 Ytterbium Atoms Nathan D. Lemke number of seconds to gain/lose one second Clocks, past & present 10 18 10 15 one second per billion years one second per million years
More informationMODERN OPTICS. P47 Optics: Unit 9
MODERN OPTICS P47 Optics: Unit 9 Course Outline Unit 1: Electromagnetic Waves Unit 2: Interaction with Matter Unit 3: Geometric Optics Unit 4: Superposition of Waves Unit 5: Polarization Unit 6: Interference
More informationRevolution in Physics. What is the second quantum revolution? Think different from Particle-Wave Duality
PHYS 34 Modern Physics Ultracold Atoms and Trappe Ions Today and Mar.3 Contents: a) Revolution in physics nd Quantum revolution b) Quantum simulation, measurement, and information c) Atomic ensemble and
More informationLONG-LIVED QUANTUM MEMORY USING NUCLEAR SPINS
LONG-LIVED QUANTUM MEMORY USING NUCLEAR SPINS Laboratoire Kastler Brossel A. Sinatra, G. Reinaudi, F. Laloë (ENS, Paris) A. Dantan, E. Giacobino, M. Pinard (UPMC, Paris) NUCLEAR SPINS HAVE LONG RELAXATION
More informationCOPYRIGHTED MATERIAL. Index
347 Index a AC fields 81 119 electric 81, 109 116 laser 81, 136 magnetic 112 microwave 107 109 AC field traps see Traps AC Stark effect 82, 84, 90, 96, 97 101, 104 109 Adiabatic approximation 3, 10, 32
More informationA Mixture of Bose and Fermi Superfluids. C. Salomon
A Mixture of Bose and Fermi Superfluids C. Salomon Enrico Fermi School Quantum Matter at Ultralow Temperatures Varenna, July 8, 2014 The ENS Fermi Gas Team F. Chevy, Y. Castin, F. Werner, C.S. Lithium
More informationLecture 4. Feshbach resonances Ultracold molecules
Lecture 4 Feshbach resonances Ultracold molecules 95 Reminder: scattering length V(r) a tan 0( k) lim k0 k r a: scattering length Single-channel scattering a 96 Multi-channel scattering alkali-metal atom:
More informationLecture 3: Helium Readings: Foot Chapter 3
Lecture 3: Helium Readings: Foot Chapter 3 Last Week: the hydrogen atom, eigenstate wave functions, and the gross and fine energy structure for hydrogen-like single-electron atoms E n Z n = hcr Zα / µ
More informationSensitivity limits of atom interferometry gravity gradiometers and strainmeters. Fiodor Sorrentino INFN Genova
Sensitivity limits of atom interferometry gravity gradiometers and strainmeters Fiodor Sorrentino INFN Genova 1 Outline AI sensors, state of the art performance Main noise sources Potential improvements
More information6. Interference of BECs
6. Interference of BECs Josephson effects Weak link: tunnel junction between two traps. Josephson oscillation An initial imbalance between the population of the double well potential leads to periodic
More informationEYLSA laser for atom cooling
1/7 For decades, cold atom system and Bose-Einstein condensates (obtained from ultra-cold atoms) have been two of the most studied topics in fundamental physics. Several Nobel prizes have been awarded
More informationDavid McIntyre. A slow beam of laser cooled rubidium atoms will be used as the matter-wave source. The atom
AD-A282 483 R&T 3124128 MATTER-WAVE INTERFEROMETRY WITH LASER COOLED ATOMS David McIntyre Department of Physics, Oregon State University, Corvallis, OR 97331-6507 Grant No: N00014-91-J-1198 DTIC Annual
More informationInterferometry and precision measurements with Bose-condensed atoms
Interferometry and precision measurements with Bose-condensed atoms Daniel Döring A thesis submitted for the degree of Doctor of Philosophy of The Australian National University. April 2011 Declaration
More informationIon traps. Trapping of charged particles in electromagnetic. Laser cooling, sympathetic cooling, optical clocks
Ion traps Trapping of charged particles in electromagnetic fields Dynamics of trapped ions Applications to nuclear physics and QED The Paul trap Laser cooling, sympathetic cooling, optical clocks Coulomb
More informationModel Answer (Paper code: AR-7112) M. Sc. (Physics) IV Semester Paper I: Laser Physics and Spectroscopy
Model Answer (Paper code: AR-7112) M. Sc. (Physics) IV Semester Paper I: Laser Physics and Spectroscopy Section I Q1. Answer (i) (b) (ii) (d) (iii) (c) (iv) (c) (v) (a) (vi) (b) (vii) (b) (viii) (a) (ix)
More informationUltra-Cold Plasma: Ion Motion
Ultra-Cold Plasma: Ion Motion F. Robicheaux Physics Department, Auburn University Collaborator: James D. Hanson This work supported by the DOE. Discussion w/ experimentalists: Rolston, Roberts, Killian,
More informationBose-Einstein condensation of lithium molecules and studies of a strongly interacting Fermi gas
Bose-Einstein condensation of lithium molecules and studies of a strongly interacting Fermi gas Wolfgang Ketterle Massachusetts Institute of Technology MIT-Harvard Center for Ultracold Atoms 3/4/04 Workshop
More informationLIST OF TOPICS BASIC LASER PHYSICS. Preface xiii Units and Notation xv List of Symbols xvii
ate LIST OF TOPICS Preface xiii Units and Notation xv List of Symbols xvii BASIC LASER PHYSICS Chapter 1 An Introduction to Lasers 1.1 What Is a Laser? 2 1.2 Atomic Energy Levels and Spontaneous Emission
More informationBose-Einstein condensates in optical lattices
Bose-Einstein condensates in optical lattices Creating number squeezed states of atoms Matthew Davis University of Queensland p.1 Overview What is a BEC? What is an optical lattice? What happens to a BEC
More informationarxiv:atom-ph/ v2 24 Mar 1997
An Atom Laser Based on Raman Transitions G.M. Moy, J.J. Hope and C.M. Savage Department of Physics and Theoretical Physics, The Australian National University, Australian Capital Territory 0200, Australia.
More informationCold fermions, Feshbach resonance, and molecular condensates (II)
Cold fermions, Feshbach resonance, and molecular condensates (II) D. Jin JILA, NIST and the University of Colorado I. Cold fermions II. III. Feshbach resonance BCS-BEC crossover (Experiments at JILA) $$
More informationLASER COOLING AND TRAPPING OF ATOMIC STRONTIUM FOR ULTRACOLD ATOMS PHYSICS, HIGH-PRECISION SPECTROSCOPY AND QUANTUM SENSORS
Brief Review Modern Physics Letters B, Vol. 20, No. 21 (2006) 1287 1320 c World Scientific Publishing Company LASER COOLING AND TRAPPING OF ATOMIC STRONTIUM FOR ULTRACOLD ATOMS PHYSICS, HIGH-PRECISION
More informationLasers... the optical cavity
Lasers... the optical cavity history principle, intuitive aspects, characteristics 2 levels systems Ti: Helium Al2O3 - Neon model-locked laser laser VCSEL bragg mirrors cleaved facets 13 ptical and/or
More informationNonlinear Optics and Gap Solitons in Periodic Photonic Structures
Nonlinear Optics and Gap Solitons in Periodic Photonic Structures Yuri Kivshar Nonlinear Physics Centre Research School of Physical Sciences and Engineering Australian National University Perspectives
More information