A new experimental apparatus for quantum atom optics

Size: px
Start display at page:

Download "A new experimental apparatus for quantum atom optics"

Transcription

1 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

2 Outline I. Motivation: Accessible physics II. Experimental techniques III. Our approach 2

3 Sub-shot-noise interferometry Standard Quantum Limit (SQL): θ~ 1 N KRb Heisenberg Limit: θ~ 1 N 3

4 From optical parametric down-conversion to spin dynamics 87 Rb F=1 m F = Optical parametric down-conversion Coherent pump Non-linear crystal Signal and idler beam Spinor Bose-Einstein condensate 87 Rb BEC in m F =0 Spin dynamics Atoms in m F =±1 4

5 Twin-Fock state interferometry [1] Lücke et al. Science 11, Vol. 334 no pp , 2011 [2] Lücke PhD Thesis,

6 Counting uncertainty for twin Fock state interferometry Between 6400 to 7600 atoms [1] Lücke et al. Science 11, Vol. 334 no pp , 2011 [2] Lücke PhD Thesis,

7 Single-Particle Fock State Wigner Function of n-particle Fock state: W x, p = 2 π 1 n L n (4(x 2 + p 2 ))e 2(x2 +p 2 ) [1] Lvovsky et al. Physical Review Letters, Vol 87, No 5, 2001 [2] Introductionary Quantum Optics, C.C. Gerry & P. L. Knight 7

8 Single-Particle Fock State for photons [1] Lvovsky et al., Physical Review Letters, Vol 87, No 5,

9 Few-Particle Fock State for photons 2 3 [1] Cooper et al., Optics Express, Vol 21, No 5,

10 Outline I. Motivation: Accessible physics a. Improved sub-shot-noise interferometry b. Negative Wigner Function of the 1 -Fock state II. Experimental techniques III. Our approach 10

11 MOTs as a tool for counting atoms 11

12 MOTs as a tool for counting atoms Photons per atom: n p = R sc ηt Photon shot noise: N a n p < 1 Interrogation t 100 ms Up to 1200 atoms in single atom detection m F =+1 m F =0 m F =-1 [1] Hume et al. Physical Review Letters, 111, ,

13 Double MOT with a Light Barrier 24µm Pulsed 125kHz 120 ms integration time Up to 470 atoms per site [1] Stroescu et al., PRA 91, ,

14 Outline I. Motivation: Accessible physics a. Improved sub-shot-noise interferometry b. Negative Wigner Function of the 1 -Fock state II. Experimental techniques a. In magneto-optical traps III. Our approach 14

15 Design Goals 1. Create a 87 Rb BEC in a few seconds a. Optical dipole trap b. Micro chip trap 2. Detect multiple modes a. MOT with a light barrier b. Multiple MOTs (with a chip) 3. with single atom counting precision Large NA detection Stray light suppression Resolve light barrier MOT 4. Maximize optical access 5. Reduce magnetic field noise [1] [1] Clément et al., PRA, 79, ,

16 The Experimental Setup ODT 3D-MOT Detection NA 3D MOT coils Quadrupol coils 16

17 Coil Design Gradient of ~300 G/cm for efficient transfer to ODT Two half circles to avoid large eddy currents Optical access of 3D MOT beams with a diameter of d=20 mm 4 Layers, with 2x29 and 2x24 windings About 1.8-2kW at 150 A Water cooling on top and bottom 17

18 Detection Optics Large NA (NA = 0.4, i.e. α = 23.5 deg) Out of Chamber Only commercially available lenses Stray light reduced 18

19 Detection Optics Magnification: ~ 18 Resolution: ~1.2 µm 19

20 Detection: Scattered Light Background incoming MOT light R 1 R2 R 0 R 3 to the detection 20

21 Detection: Scattered Light Background Amount of incident photons in MOT beam: N ph s Multiple reflections inside the chamber: R n ( ) n Surface quality and scattering rate: P sc Out-of-focus supression by pinhole: P pin Numerical aperture: NA N bkg s N bkg (t = 100 ms) 25 σ phsn (t = 100 ms)

22 Next Steps in 2016 Component February March April May June July Coil assembly Finalize design wind, test with water cooling µmetal Shield Depends on coil design Finalize design and order Hopefully arrives Test shielding and stability Glass chamber Frame is ready Hopefully arrives Bake and pump Special 4 way vacuum cross Hopefully arrives Vacom parts MOT laser system Optical dipole trap Light sheet system arrived Order and slight rebuild Build test setup for intensity and position stabilization Design, pick components Detection optics ready to order (fast) arrive Test imaging of lens system 22

23 The Team Wolfgang Ertmer Carsten Klempt Andreas Hüper Jiao Geng Jan Mahnke Ilka Kruse Thank you for your attention! 23

0.5 atoms improve the clock signal of 10,000 atoms

0.5 atoms improve the clock signal of 10,000 atoms 0.5 atoms improve the clock signal of 10,000 atoms I. Kruse 1, J. Peise 1, K. Lange 1, B. Lücke 1, L. Pezzè 2, W. Ertmer 1, L. Santos 3, A. Smerzi 2, C. Klempt 1 1 Institut für Quantenoptik, Leibniz Universität

More information

Multipath Interferometer on an AtomChip. Francesco Saverio Cataliotti

Multipath 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

Atom Quantum Sensors on ground and in space

Atom 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 information

PROGRESS 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 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 information

Bose-Einstein condensates & tests of quantum mechanics

Bose-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 information

Confining ultracold atoms on a ring in reduced dimensions

Confining 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 information

PROGRESS 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 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 information

Towards quantum metrology with N00N states enabled by ensemble-cavity interaction. Massachusetts Institute of Technology

Towards quantum metrology with N00N states enabled by ensemble-cavity interaction. Massachusetts Institute of Technology Towards quantum metrology with N00N states enabled by ensemble-cavity interaction Hao Zhang Monika Schleier-Smith Robert McConnell Jiazhong Hu Vladan Vuletic Massachusetts Institute of Technology MIT-Harvard

More information

Quantum superpositions and correlations in coupled atomic-molecular BECs

Quantum 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 information

Interferometry and precision measurements with Bose-condensed atoms

Interferometry 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 information

Optimization of transfer of laser-cooled atom cloud to a quadrupole magnetic trap

Optimization 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 information

Les 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 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 information

Matter wave interferometry beyond classical limits

Matter 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 information

UNIVERSITY OF SOUTHAMPTON

UNIVERSITY OF SOUTHAMPTON UNIVERSITY OF SOUTHAMPTON PHYS6012W1 SEMESTER 1 EXAMINATION 2012/13 Coherent Light, Coherent Matter Duration: 120 MINS Answer all questions in Section A and only two questions in Section B. Section A carries

More information

Observation of Feshbach resonances in ultracold

Observation of Feshbach resonances in ultracold Observation of Feshbach resonances in ultracold Rb and 133 Cs mixtures at high magnetic field Rubidium Caesium Hung-Wen, Cho Motivation Bialkali molecules in the ground state have a large permanent electric

More information

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

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

More information

Squeezed Light for Gravitational Wave Interferometers

Squeezed Light for Gravitational Wave Interferometers Squeezed Light for Gravitational Wave Interferometers R. Schnabel, S. Chelkowski, H. Vahlbruch, B. Hage, A. Franzen, and K. Danzmann. Institut für Atom- und Molekülphysik, Universität Hannover Max-Planck-Institut

More information

Cold Metastable Neon Atoms Towards Degenerated Ne*- Ensembles

Cold 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 information

Quantum Computing with neutral atoms and artificial ions

Quantum 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 information

Precision 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 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 information

Supported by NIST, the Packard Foundation, the NSF, ARO. Penn State

Supported 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 information

Quantum entanglement and light propagation through Bose-Einstein condensate (BEC) M. Emre Taşgın

Quantum entanglement and light propagation through Bose-Einstein condensate (BEC) M. Emre Taşgın Quantum entanglement and light propagation through Bose-Einstein condensate (BEC) M. Emre Taşgın Advisor: M. Özgür Oktel Co-Advisor: Özgür E. Müstecaplıoğlu Outline Superradiance and BEC Superradiance

More information

Lecture 3. Bose-Einstein condensation Ultracold molecules

Lecture 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 information

Les Houches 2009: Metastable Helium Atom Laser

Les Houches 2009: Metastable Helium Atom Laser Les Houches 2009: Metastable Helium Atom Laser Les Houches, Chamonix, February 2005 Australian Research Council Centre of Excellence for Quantum-Atom Optics UQ Brisbane SUT Melbourne ANU Canberra Snowy

More information

Increasing atomic clock precision with and without entanglement

Increasing atomic clock precision with and without entanglement Lehman College Increasing atomic clock precision with and without entanglement Christopher C. Gerry Department of Physics and Astronomy Lehman College, The City University of New York Bronx, New York 0468-589

More information

COPYRIGHTED MATERIAL. Index

COPYRIGHTED 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 information

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

Exploring long-range interacting quantum many-body systems with Rydberg atoms Exploring long-range interacting quantum many-body systems with Rydberg atoms Christian Groß Max-Planck-Institut für Quantenoptik Hannover, November 2015 Motivation: Quantum simulation Idea: Mimicking

More information

Ytterbium quantum gases in Florence

Ytterbium 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 information

Quantum optics. Marian O. Scully Texas A&M University and Max-Planck-Institut für Quantenoptik. M. Suhail Zubairy Quaid-i-Azam University

Quantum optics. Marian O. Scully Texas A&M University and Max-Planck-Institut für Quantenoptik. M. Suhail Zubairy Quaid-i-Azam University Quantum optics Marian O. Scully Texas A&M University and Max-Planck-Institut für Quantenoptik M. Suhail Zubairy Quaid-i-Azam University 1 CAMBRIDGE UNIVERSITY PRESS Preface xix 1 Quantum theory of radiation

More information

Introduction to entanglement theory & Detection of multipartite entanglement close to symmetric Dicke states

Introduction to entanglement theory & Detection of multipartite entanglement close to symmetric Dicke states Introduction to entanglement theory & Detection of multipartite entanglement close to symmetric Dicke states G. Tóth 1,2,3 Collaboration: Entanglement th.: G. Vitagliano 1, I. Apellaniz 1, I.L. Egusquiza

More information

Quantum Memory in Atomic Ensembles BY GEORG BRAUNBECK

Quantum Memory in Atomic Ensembles BY GEORG BRAUNBECK Quantum Memory in Atomic Ensembles BY GEORG BRAUNBECK Table of contents 1. Motivation 2. Quantum memory 3. Implementations in general 4. Implementation based on EIT in detail QUBIT STORAGE IN ATOMIC ENSEMBLES

More information

Quantum 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, / 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 information

NanoKelvin Quantum Engineering. Subhadeep Gupta UW NSF-INT Phys REU, 28 th July 2014

NanoKelvin Quantum Engineering. Subhadeep Gupta UW NSF-INT Phys REU, 28 th July 2014 NanoKelvin Quantum Engineering Subhadeep Gupta UW NSF-INT Phys REU, 28 th July 2014 NanoKelvin Quantum Engineering with Ultracold Atoms < 200 nk Our group: Precision BEC interferometry. Ultracold Mixtures

More information

Hong-Ou-Mandel effect with matter waves

Hong-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 information

Compensation of gravity gradients and rotations in precision atom interferometry

Compensation of gravity gradients and rotations in precision atom interferometry Compensation of gravity gradients and rotations in precision atom interferometry Albert Roura partly based on Phys. Rev. Lett. 118, 160401 (2017) Vienna, 11 April 2018 Motivation Tests of universality

More information

Lecture 2. Trapping of neutral atoms Evaporative cooling. Foot 9.6, , 10.5

Lecture 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 information

Quantum Gases. Subhadeep Gupta. UW REU Seminar, 11 July 2011

Quantum 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 information

Observation of Bose-Einstein Condensation in a Dilute Atomic Vapor

Observation of Bose-Einstein Condensation in a Dilute Atomic Vapor Observation of Bose-Einstein Condensation in a Dilute Atomic Vapor M. H. Anderson, J. R. Ensher, M. R. Matthews, C. E. Wieman, E. A. Cornell Science 14 Jul 1995; Vol. 269, Issue 5221, pp. 198-201 DOI:

More information

Einstein-Podolsky-Rosen entanglement t of massive mirrors

Einstein-Podolsky-Rosen entanglement t of massive mirrors Einstein-Podolsky-Rosen entanglement t of massive mirrors Roman Schnabel Albert-Einstein-Institut t i tit t (AEI) Institut für Gravitationsphysik Leibniz Universität Hannover Outline Squeezed and two-mode

More information

Ultracold atoms and molecules

Ultracold 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 information

Parametric down-conversion

Parametric down-conversion Parametric down-conversion 1 Introduction You have seen that laser light, for all its intensity and coherence, gave us the same PP(mm) counts distribution as a thermal light source with a high fluctuation

More information

Feedback control of atomic coherent spin states

Feedback control of atomic coherent spin states Feedback control of atomic coherent spin states Andrea Bertoldi Institut d Optique, France RG Colloquium Hannover 13/12/2012 Feedback control h(t) Constant flow is required to keep time P = r H2O g h(t)

More information

In Situ Imaging of Cold Atomic Gases

In 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 information

SYRTE - 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 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 information

Fundamentals of Spectroscopy for Optical Remote Sensing. Course Outline 2009

Fundamentals of Spectroscopy for Optical Remote Sensing. Course Outline 2009 Fundamentals of Spectroscopy for Optical Remote Sensing Course Outline 2009 Part I. Fundamentals of Quantum Mechanics Chapter 1. Concepts of Quantum and Experimental Facts 1.1. Blackbody Radiation and

More information

12 rad be Ω max 10 / Hz. This result is better by two orders of magnitude than any

12 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 information

Path Entanglement. Liat Dovrat. Quantum Optics Seminar

Path Entanglement. Liat Dovrat. Quantum Optics Seminar Path Entanglement Liat Dovrat Quantum Optics Seminar March 2008 Lecture Outline Path entangled states. Generation of path entangled states. Characteristics of the entangled state: Super Resolution Beating

More information

EYLSA laser for atom cooling

EYLSA 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 information

XRD endstation: condensed matter systems

XRD endstation: condensed matter systems XRD endstation: condensed matter systems Justine Schlappa SCS Instrument Beamline Scientist Hamburg, January 24, 2017 2 Outline Motivation Baseline XRD setup R&D setup Two-color operation and split&delay

More information

Frequency Tunable Atomic Magnetometer based on an Atom Interferometer

Frequency Tunable Atomic Magnetometer based on an Atom Interferometer Frequency Tunable Atomic Magnetometer based on an Atom Interferometer D.A. Braje 1, J.P. Davis 2, C.L. Adler 2,3, and F.A. Narducci 2 Blaubeuren Quantum Optics Summer School 29 July 2013 1 MIT Lincoln

More information

All-optical formation of a Bose-Einstein condensate for applications in scanning electron microscopy

All-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 information

Generation of squeezed vacuum with hot and ultra-cold Rb atoms

Generation of squeezed vacuum with hot and ultra-cold Rb atoms Generation of squeezed vacuum with hot and ultra-cold Rb atoms Eugeniy E. Mikhailov, Travis Horrom, Irina Novikova Salim Balik 2, Arturo Lezama 3, Mark Havey 2 The College of William & Mary, USA 2 Old

More information

NanoKelvin Quantum Engineering

NanoKelvin 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 information

Towards compact transportable atom-interferometric inertial sensors

Towards 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 information

Fluids with dipolar coupling

Fluids with dipolar coupling Fluids with dipolar coupling Rosensweig instability M. D. Cowley and R. E. Rosensweig, J. Fluid Mech. 30, 671 (1967) CO.CO.MAT SFB/TRR21 STUTTGART, ULM, TÜBINGEN FerMix 2009 Meeting, Trento A Quantum Ferrofluid

More information

Quantum Logic Spectroscopy and Precision Measurements

Quantum Logic Spectroscopy and Precision Measurements Quantum Logic Spectroscopy and Precision Measurements Piet O. Schmidt PTB Braunschweig and Leibniz Universität Hannover Bad Honnef, 4. November 2009 Overview What is Quantum Metrology? Quantum Logic with

More information

Ultracold Fermi Gases with unbalanced spin populations

Ultracold 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 information

Advanced accelerometer/gradiometer concepts based on atom interferometry

Advanced accelerometer/gradiometer concepts based on atom interferometry Advanced accelerometer/gradiometer concepts based on atom interferometry Malte Schmidt, Alexander Senger, Matthias Hauth, Sebastian Grede, Christian Freier, Achim Peters Humboldt-Universität zu Berlin

More information

(Noise) correlations in optical lattices

(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 information

A 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 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 information

Detection of Single Photon Emission by Hanbury-Brown Twiss Interferometry

Detection of Single Photon Emission by Hanbury-Brown Twiss Interferometry Detection of Single Photon Emission by Hanbury-Brown Twiss Interferometry Greg Howland and Steven Bloch May 11, 009 Abstract We prepare a solution of nano-diamond particles on a glass microscope slide

More information

MESOSCOPIC QUANTUM OPTICS

MESOSCOPIC QUANTUM OPTICS MESOSCOPIC QUANTUM OPTICS by Yoshihisa Yamamoto Ata Imamoglu A Wiley-Interscience Publication JOHN WILEY & SONS, INC. New York Chichester Weinheim Brisbane Toronto Singapore Preface xi 1 Basic Concepts

More information

Supplementary Figure S1 Definition of the wave vector components: Parallel and perpendicular wave vector of the exciton and of the emitted photons.

Supplementary Figure S1 Definition of the wave vector components: Parallel and perpendicular wave vector of the exciton and of the emitted photons. Supplementary Figure S1 Definition of the wave vector components: Parallel and perpendicular wave vector of the exciton and of the emitted photons. Supplementary Figure S2 The calculated temperature dependence

More information

QUANTUM- CLASSICAL ANALOGIES

QUANTUM- CLASSICAL ANALOGIES D. Dragoman M. Dragoman QUANTUM- CLASSICAL ANALOGIES With 78 Figures ^Ü Springer 1 Introduction 1 2 Analogies Between Ballistic Electrons and Electromagnetic Waves 9 2.1 Analog Parameters for Ballistic

More information

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

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 1 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 phases of matter that have been experimentally observed,

More information

Experimental realization of spin-orbit coupling in degenerate Fermi gas. Jing Zhang

Experimental realization of spin-orbit coupling in degenerate Fermi gas. Jing Zhang QC12, Pohang, Korea Experimental realization of spin-orbit coupling in degenerate Fermi gas Jing Zhang State Key Laboratory of Quantum Optics and Quantum Optics Devices, Institute of Opto-Electronics,

More information

Hong Ou Mandel experiment with atoms

Hong 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 information

Realization of Bose-Einstein Condensation in dilute gases

Realization 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 information

Introduction to cold atoms and Bose-Einstein condensation (II)

Introduction 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 information

Quantum enhanced magnetometer and squeezed state of light tunable filter

Quantum enhanced magnetometer and squeezed state of light tunable filter Quantum enhanced magnetometer and squeezed state of light tunable filter Eugeniy E. Mikhailov The College of William & Mary October 5, 22 Eugeniy E. Mikhailov (W&M) Squeezed light October 5, 22 / 42 Transition

More information

Atom lasers. FOMO summer school 2016 Florian Schreck, University of Amsterdam MIT 1997 NIST Munich Yale 1998

Atom 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 information

The amazing story of Laser Cooling and Trapping

The amazing story of Laser Cooling and Trapping The amazing story of Laser Cooling and Trapping following Bill Phillips Nobel Lecture http://www.nobelprize.org/nobel_prizes/physics/ laureates/1997/phillips-lecture.pdf Laser cooling of atomic beams 1

More information

BEC of 6 Li 2 molecules: Exploring the BEC-BCS crossover

BEC 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 information

Status of the MAGIX Spectrometer Design. Julian Müller MAGIX collaboration meeting 2017

Status of the MAGIX Spectrometer Design. Julian Müller MAGIX collaboration meeting 2017 Status of the MAGIX Spectrometer Design Julian Müller MAGIX collaboration meeting 2017 Magneto Optic Design Requirements relative momentum resolution Δp p < 10 4 resolution of the scattering angle Δθ

More information

Conference on Research Frontiers in Ultra-Cold Atoms. 4-8 May Generation of a synthetic vector potential in ultracold neutral Rubidium

Conference on Research Frontiers in Ultra-Cold Atoms. 4-8 May Generation of a synthetic vector potential in ultracold neutral Rubidium 3-8 Conference on Research Frontiers in Ultra-Cold Atoms 4-8 May 9 Generation of a synthetic vector potential in ultracold neutral Rubidium SPIELMAN Ian National Institute of Standards and Technology Laser

More information

CW-Lyman- Source for Laser Cooling of Antihydrogen in a Magnetic Trap

CW-Lyman- Source for Laser Cooling of Antihydrogen in a Magnetic Trap CW-Lyman- Source for Laser Cooling of Antihydrogen in a Magnetic Trap F. Markert, M. Scheid, D. Kolbe, A. Müllers, T. Weber, V. Neises, R. Steinborn and J. Walz Institut für Physik, Johannes Gutenberg-Universität

More information

Laser Cooling and Trapping of Atoms

Laser Cooling and Trapping of Atoms Chapter 2 Laser Cooling and Trapping of Atoms Since its conception in 1975 [71, 72] laser cooling has revolutionized the field of atomic physics research, an achievement that has been recognized by the

More information

Status of the Search for an EDM of 225 Ra

Status of the Search for an EDM of 225 Ra Status of the Search for an EDM of 225 Ra I. Ahmad, K. Bailey, J. Guest, R. J. Holt, Z.-T. Lu, T. O Connor, D. H. Potterveld, N. D. Scielzo Roy Holt Lepton Moments 2006 Cape Cod Outline Why is an EDM interesting?

More information

Ultrafast Wavelength Tuning and Scaling Properties of a Noncollinear Optical Parametric Oscillator (NOPO)

Ultrafast Wavelength Tuning and Scaling Properties of a Noncollinear Optical Parametric Oscillator (NOPO) Ultrafast Wavelength Tuning and Scaling Properties of a Noncollinear Optical Parametric Oscillator (NOPO) Thomas Binhammer 1, Yuliya Khanukaeva 2, Alexander Pape 1, Oliver Prochnow 1, Jan Ahrens 1, Andreas

More information

Development of a compact Yb optical lattice clock

Development 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 information

Do we need quantum light to test quantum memory? M. Lobino, C. Kupchak, E. Figueroa, J. Appel, B. C. Sanders, Alex Lvovsky

Do we need quantum light to test quantum memory? M. Lobino, C. Kupchak, E. Figueroa, J. Appel, B. C. Sanders, Alex Lvovsky Do we need quantum light to test quantum memory? M. Lobino, C. Kupchak, E. Figueroa, J. Appel, B. C. Sanders, Alex Lvovsky Outline EIT and quantum memory for light Quantum processes: an introduction Process

More information

Atom interferometry applications in gravimetry

Atom interferometry applications in gravimetry Prof. Achim Peters, Ph.D. Atom interferometry applications in gravimetry and some thoughts on current sensitivity limitations and concepts for future improvements International Workshop on Gravitational

More information

Gottfried Wilhelm Leibniz Universität Hannover

Gottfried Wilhelm Leibniz Universität Hannover Exploring the Potential of Ultra Cold Gases for Fundamental Tests in Space Wolfgang Ertmer Gottfried Wilhelm Leibniz Universität Hannover Institute for Quantum Optics (IQ) Centre for Quantum Engineering

More information

A facility for Femtosecond Soft X-Ray Imaging on the Nanoscale

A facility for Femtosecond Soft X-Ray Imaging on the Nanoscale A facility for Femtosecond Soft X-Ray Imaging on the Nanoscale Jan Lüning Outline Scientific motivation: Random magnetization processes Technique: Lensless imaging by Fourier Transform holography Feasibility:

More information

Schemes to generate entangled photon pairs via spontaneous parametric down conversion

Schemes to generate entangled photon pairs via spontaneous parametric down conversion Schemes to generate entangled photon pairs via spontaneous parametric down conversion Atsushi Yabushita Department of Electrophysics National Chiao-Tung University? Outline Introduction Optical parametric

More information

Bose-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 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 information

Direct observation of quantum phonon fluctuations in ultracold 1D Bose gases

Direct 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 information

Seoul National University Research Assistant Research topic: Atom optics, Hollow-core optical fiber Advisor: Prof.

Seoul National University Research Assistant Research topic: Atom optics, Hollow-core optical fiber Advisor: Prof. Yong-il Shin Department of Physics and Astronomy Seoul National University, Gwanak-gu, Seoul 151-747, Korea E-mail: yishin@snu.ac.kr (Phone: +82-2-880-4226) Web: http://phya.snu.ac.kr/yishin ResearchID:

More information

Quantum optics and squeezed states of light

Quantum optics and squeezed states of light Quantum optics and squeezed states of light Eugeniy E. Mikhailov The College of William & Mary June 15, 2012 Eugeniy E. Mikhailov (W&M) Quantum optics June 15, 2012 1 / 44 From ray optics to semiclassical

More information

Workshop on Topics in Quantum Turbulence March Experiments on Bose Condensates

Workshop on Topics in Quantum Turbulence March Experiments on Bose Condensates 2023-24 Workshop on Topics in Quantum Turbulence 16-20 March 2009 Experiments on Bose Condensates K. Helmerson National Institute of Standards and Technology Gaithersburg U.S.A. Atomic gas Bose-Einstein

More information

Introduction to Cold Atoms and Bose-Einstein Condensation. Randy Hulet

Introduction 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 information

Single Emitter Detection with Fluorescence and Extinction Spectroscopy

Single Emitter Detection with Fluorescence and Extinction Spectroscopy Single Emitter Detection with Fluorescence and Extinction Spectroscopy Michael Krall Elements of Nanophotonics Associated Seminar Recent Progress in Nanooptics & Photonics May 07, 2009 Outline Single molecule

More information

Experimental realization of spin-orbit coupled degenerate Fermi gas. Jing Zhang

Experimental realization of spin-orbit coupled degenerate Fermi gas. Jing Zhang Hangzhou Workshop on Quantum Matter, 2013 Experimental realization of spin-orbit coupled degenerate Fermi gas Jing Zhang State Key Laboratory of Quantum Optics and Quantum Optics Devices, Institute of

More information

Take that, Bell s Inequality!

Take that, Bell s Inequality! Take that, Bell s Inequality! Scott Barker November 10, 2011 Abstract Bell s inequality was tested using the CHSH method. Entangled photons were produced from two different laser beams by passing light

More information

Vortices and other topological defects in ultracold atomic gases

Vortices and other topological defects in ultracold atomic gases Vortices and other topological defects in ultracold atomic gases Michikazu Kobayashi (Kyoto Univ.) 1. Introduction of topological defects in ultracold atoms 2. Kosterlitz-Thouless transition in spinor

More information

Quantum correlations and atomic speckle

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 information

Revolution in Physics. What is the second quantum revolution? Think different from Particle-Wave Duality

Revolution 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 information

Experiments with an Ultracold Three-Component Fermi Gas

Experiments 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 information

Decoherence in QM physics 491 fall 2009 friday feature M. Gold updated Oct. 1, 2015

Decoherence in QM physics 491 fall 2009 friday feature M. Gold updated Oct. 1, 2015 diffraction experiment Decoherence in QM physics 491 fall 2009 friday feature M. Gold updated Oct. 1, 2015 In reality, it contains the only mystery, the basic peculiarities of all of quantum mechanics.

More information

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

Ground state cooling via Sideband cooling. Fabian Flassig TUM June 26th, 2013 Ground state cooling via Sideband cooling Fabian Flassig TUM June 26th, 2013 Motivation Gain ultimate control over all relevant degrees of freedom Necessary for constant atomic transition frequencies Do

More information