Cold molecule studies of OH, NH, and metastable CO
|
|
- Hilary Murphy
- 5 years ago
- Views:
Transcription
1 ACS, April 2008 p. 1/26 Cold molecule studies of OH, NH, and metastable CO Gerrit C. Groenenboom Theoretical Chemistry Institute for Molecules and Materials Radboud University Nijmegen The Netherlands
2 ACS, April 2008 p. 2/26 Collaborators OH, CO: FHI Berlin Joop Gilijamse Steven Hoekstra Samuel Meek Markus Metsälä Bas van de Meerakker Gerard Meijer NH: Harvard Wes Campbell Hsin-I Lu Edem Tsikata John Doyle
3 ACS, April 2008 p. 3/26 Cold molecule techniques 1998 buffergas cooling John Doyle, CaH 1999 Stark deceleration Gerard Meijer, CO 2001 rotating nozzle Dudley Herschbach, O storage ring Gerard Meijer, ND photoassociation Pierre Pillet, Cs 2 (trapped) 2003 filtering Gerard Rempe, NH Feshbach resonances Rudy Grimm, Li 2 (BEC) 2003 billiard ball collisions Dave Chandler, Ar+NO 2004 optical Stark deceleration Peter Barker, C 6 H reactive collision slowing Hans-Joachim Loesch, K+HBr 2007 Zeeman deceleration Nicolas Vanhaeke, H 2007 molecular synchrotron Gerard Meijer, NH 3... cavity laser cooling Yun Ye, OH (theory)... sympathetic cooling Peter Barker
4 ACS, April 2008 p. 4/26 Xe+OH( 2 Π 3/2f ) collision experiment cooled -70 o C LIF zone PMT Xe Stark decelerator skimmer hexapole detection laser (282 nm) pulsed valve photodissociation laser (193 nm) Bas van de Meerakker, Steven Hoekstra, Joop Gilijamse, Gerard Meijer (Berlin, 2006)
5 ACS, April 2008 p. 5/26 OH X( 2 Π) energy levels cm /2 f e /2 f + e /2 f e /2 N J F 2, X 2 Π 1/2 f - e + ε p 0 1 3/2 N J f + e - ε p F 1, X 2 Π 3/2
6 Xe OH( 2 Π) potentials (cm 1 ) Xe OH (A ) Xe OH (A ) θ (degrees) θ (degrees) R (a 0 ) R (a 0 ) Molpro: RCCSD(T), aug-cc-pvqz+bond orbitals, ECP28MDF ACS, April 2008 p. 6/26
7 ACS, April 2008 p. 7/26 Xe+OH energy dependent cross sections 10 3 F 1 (3/2f) 10 2 F 1 (3/2e) σ (Å 2 ) F (5/2e) 1 F (1/2) 2 F (7/2) 1 F (5/2f) 1 F (3/2) E coll (cm 1 )
8 Xe+OH experimental results ACS, April 2008 p. 8/26
9 ACS, April 2008 p. 9/26 Xe+OH, comparison with experiment 100 σ (%) F 1 (3/2e) F 1 (5/2e) F 1 (5/2f) 0 F 2 (1/2e) E coll (cm 1 ) Gilijamse, Hoekstra, van de Meerakker, Groenenboom, Meijer, Science 313, 1617 (2006)
10 ACS, April 2008 p. 10/26 Xe+OH, convolution and Xe beam σ(e coll ) voh 2 Signal n OH n + v2 Xe Xe v OH v Xe (m/s) FWHM (%) 5
11 ACS, April 2008 p. 11/26 Convergence check Xe+OH: F max /2e 3/2f 5/2e 5/2f 1/2e 1/2f F F l = 45 b = l 2µEcoll 8 bohr
12 ACS, April 2008 p. 12/26 Buffergas loading Buffer-gas Cooling and Loading Hot Molecules 1000 K Superconducting Magnet Coils Cold Walls < 1 K Helium Buffer Gas cm -3 Cold Trapped Molecules John Doyle, Wes Campbell, et al., Harvard Accepts full Boltzmann distribution of source External motion, rotation thermalize quickly Vibration, spin thermalize slowly He provides dissipation in conservative trap potential
13 ACS, April 2008 p. 13/26 NH(v = 1) in trap vs time Number of Trapped NH(v"=1) [arb.] v=1 v"=1 A 3 Π 2 X 3 Σ Time [ms] W. C. Campbell, G. C. Groenenboom, H.-I Lu, E. Tsikata, and J. M. Doyle, Phys. Rev. Lett., 100, (2008)
14 ACS, April 2008 p. 14/26 Measured NH(v = 0, 1) trap lifetime Trapped Molecule Lifetime [ms] v = 0 v = Buffer-Gas Density [10 14 cm -3 ] W. C. Campbell, G. C. Groenenboom, H.-I Lu, E. Tsikata, and J. M. Doyle, Phys. Rev. Lett., 100, (2008)
15 ACS, April 2008 p. 15/26 NH X 3 Σ (v = 1) lifetime (ms) τ 1 = f 4αω 3 3c 2 v = 0,N = 1 µ(r) v = 1,N = 0 2 e2 Rosmus, Werner, 1980, PNO-CEPA 28.7 Dodd et al., 1991, MRCI/RKR 19.3 (23.9) CASSCF/MRCI aug-cc-pvtz rotation cc-pv6z active space (6σ, 3π) core-correlation aug-cc-pv6z RHF+RCCSD(T) finite field 37.4 buffergas cooling experiment: 37.0 ± 0.5 ms
16 ACS, April 2008 p. 16/26 NH( 3 Σ ) permanent dipole moment (v = 0) Experiment, Scarl and Dalby (1974) 0.543± ea 0 CASSCF+MRCI aug-cc-pv6z: Paldus and Li (1996): Conclusion: 30% more N on our sun
17 Radiative lifetime of OH X 2 Π 3/2 (v = 1) Van de Meerakker, Vanhaecke, van der Loo, Groenenboom, and Meijer, Phys. Rev. Lett., 95, (2005) ACS, April 2008 p. 17/26
18 ACS, April 2008 p. 18/26 Radiative lifetime of OH X 2 Π 3/2 (v = 1) Molpro: aug-cc-pv6z, 1σ 5σ, 1π 2π CASSCF/MRCI year τ (ms) Decay in trap ±2 Present calculation (57.2) HITRAN D. D. Nelson et al S. R. Langhoff et al S. R. Langhoff et al H.-J. Werner et al M. van der Loo and G. C. Groenenboom, J. Chem. Phys. 126, (2007)+erratum Application to OH Meinel system: Decrease in atomic hydrogen over the summer pole, D. E. Siskind et al., Geophys. Res. Lett. (2008), submitted
19 ACS, April 2008 p. 19/26 CO(a 3 Π 1 ) lifetime model h a (r) 1 cm h A,a (r) µ X,A (r) 0.5 a.u. τ 1 = v X A vx,v a ev A( 1 Π) a( 3 Π) X( 1 Σ + ) A vx,v a = 4αω3 v a,v X 3c 2 e 2 c 2 Ω,1 v A v X µ X,A v A v A h A,a v a E va E va r (a 0 ) Thomas James, JCP 1971
20 ACS, April 2008 p. 20/26 CO(a 3 Π 1 ) lifetime results (ms) Experiment: 2.63 ± 0.03 Thomas James (JCP 1971): % Ab initio + RKR potentials: % Sykora and Vidal (JCP 1999): % Jongma, Berden, Meijer (JCP 1997): 3.67± % 3.4± % J. Gilijamse et al., J. Chem. Phys., 127, (2007)
21 ACS, April 2008 p. 21/26 CO(a 3 Π 1 ) lifetime extended model lower level calculation (MCSCF/aug-cc-pVTZ) extra 1 Π intermediate states result scaled to 3.16 ms for single intermediate state ms 20.0% ms 27.0% ms 2.4% ms 10.3% ms 3.4% Experiment: 2.63 ms
22 ACS, April 2008 p. 22/26 Check of spin-orbit coupling CO (a 3 Π Ω ) v a Ab initio Experiment error (%) R. W. Field et al., J. Mol. Spectrosc. (1972)
23 ACS, April 2008 p. 23/26 CO A 1 Π X 1 Σ + transition dipole moment µ X,A (ea 0 ) present Spielfiedel (1999) Kirby (1989) EOM HF EOM MCSCF r = 2.0 a 0 r = 2.5 a 0 present (ea 0 ) Spielfiedel [1] 91.6% 99.1% Kirby [2] 94.9% 99.6% 0.25 CCSD-EOM(HF) 93.4% 98.0% EOM(MCSCF) 93.6% 99.4% r (a ) 0 [1] A. Spielfiedel et al., Astron. Astrophys. (1999) [2] K. Kirby and D. L. Cooper, J. Chem. Phys. (1989)
24 ACS, April 2008 p. 24/26 CO A 1 Π X 1 Σ + oscillator strength f osc = v A 2 3 (E v A E vx ) µ va,v X 2 Present % Experiment (1993) Other experiments: Spielfiedel (1999) % Kirby (1989) % W. F. Chan et al., Chem. Phys. (1993) Electron energy loss spectrosc. + TRK sum-rule (7-200 ev)
25 CO A 1 Π(v ) dependent lifetimes (ns) Experiment Fit τ (ns) Ab initio v Experiment: R. W. Field et al., J. Chem. Phys. (1983) Using fitted dipole: τ(co a 3 Π 1 ) = 3.66 ms. ACS, April 2008 p. 25/26
26 ACS, April 2008 p. 26/26 Conclusions Xe+OH: towards crossed controlled beams NH(v = 1) lifetime: 30 % more N on our sun OH(v = 1) lifetime benchmark: Meinel system CO(a 3 Π 1 ) lifetime: nonorthogonality essential, measured A 1 Π(v ) lifetimes wrong
Experiments with Stark decelerated and trapped OH radicals
Experiments with Stark decelerated and trapped OH radicals Sebastiaan Y.T. van de Meerakker and Gerard Meijer Fritz-Haber-Institute der Max-Planck-Gesellschaft, Faradayweg 4-6, 14195 Berlin, Germany E-mail:
More informationCold and ultracold collisions involving open-shell diatomic molecules
Lunteren 2005 p. 1/31 Cold and ultracold collisions involving open-shell diatomic molecules Gerrit C. Groenenboom Institute of Theoretical Chemistry University of Nijmegen The Netherlands Lunteren 2005
More informationDeceleration and trapping of heavy diatomic molecules for precision tests of fundamental symmetries. Steven Hoekstra
Deceleration and trapping of heavy diatomic molecules for precision tests of fundamental symmetries Steven Hoekstra Deceleration and trapping of heavy diatomic molecules for precision tests of fundamental
More informationMagnetic Trapping of NH Molecules with 20 s Lifetimes
Magnetic Trapping of NH Molecules with 20 s Lifetimes E Tsikata 1,2, W C Campbell 1,3, M T Hummon 1,2, H-I Lu 1,4 and J M Doyle 1,2 1 Department of Physics, Harvard University, Cambridge, MA, USA 2 Harvard/MIT
More informationWhy ultracold molecules?
Cold & ultracold molecules new frontiers J. Ye, JILA Michigan Quantum Summer School, Ann Arbor, June 18, 2008 Quantum dipolar gas Precision test QED ee- eehco OH H2O H2CO Quantum measurement Chemical reactions
More informationManipulating Rydberg atoms and molecules in the gas phase and near chip surfaces
RQI Winter School Obergurgl, 12 February 2013 Manipulating Rydberg atoms and molecules in the gas phase and near chip surfaces Ch. Seiler, P. Allmendinger, S. D. Hogan, H. Saßmannshausen, J. Deiglmayr
More informationDECELERATION OF MOLECULES
Seminar Ultra Cold Molecules DECELERATION OF MOLECULES Universität Hannover Matthias Pospiech 29th June 2004 Contents Contents: 1 Introduction Why of interest Lasercooling? 2 Deceleration Experiment Pulsed
More informationP R L HYSICAL EVIEW ETTERS. Articles published week ending 22 JUNE Volume 98, Number 25. Published by The American Physical Society
P R L HYSICAL EVIEW ETTERS Articles published week ending Volume 98, Number 25 Member Subscription Copy Library or Other Institutional Use Prohibited Until 2012 Published by The American Physical Society
More informationCold and Slow Molecular Beam
Cold and Slow Molecular Beam Hsin-I Lu, a,b Julia Rasmussen, c,b Matthew J. Wright, c,b Dave Patterson, c,b and John M. Doyle c,b Employing a two-stage cryogenic buffer gas cell, we produce a cold, hydrodynamically
More informationUltracold Molecules and Cold Controlled Chemistry. Roman Krems University of British Columbia
Ultracold Molecules and Cold Controlled Chemistry Roman Krems University of British Columbia Sergey Alyabyshev Zhiying Li Timur Tscherbul ultra-cold cold warm hot 10-8 10-7 10-6 10-5 10-4 10-3 10-2 10-1
More informationProduction and deceleration of a pulsed beam of metastable NH (a 1 ) radicals
Production and deceleration of a pulsed beam of metastable NH (a 1 ) radicals Sebastiaan Y.T. van de Meerakker, Irena Labazan, Steven Hoekstra, Jochen Küpper, and Gerard Meijer Fritz-Haber-Institut der
More informationarxiv:physics/ v1 [physics.atom-ph] 7 Jun 2003
Phase Space Manipulation of Cold Free Radical OH Molecules J. R. Bochinski, Eric R. Hudson, H. J. Lewandowski, and Jun Ye JILA, National Institute of Standards and Technology and University of Colorado
More informationarxiv: v2 [physics.chem-ph] 15 May 2008
arxiv:0802.2902v2 [physics.chem-ph] 15 May 2008 Reflection of OH molecules from magnetic mirrors 1. Introduction Markus Metsälä, Joop J. Gilijamse, Steven Hoekstra, Sebastiaan Y. T. van de Meerakker, and
More informationAtom-molecule molecule collisions in spin-polarized polarized alkalis: potential energy surfaces and quantum dynamics
Atom-molecule molecule collisions in spin-polarized polarized alkalis: potential energy surfaces and quantum dynamics Pavel Soldán, Marko T. Cvitaš and Jeremy M. Hutson University of Durham with Jean-Michel
More informationExperiments with Stark-decelerated and trapped molecules
Experiments with Stark-decelerated and trapped molecules Joop Jelte Gilijamse Experiments with Stark-decelerated and trapped molecules Joop J. Gilijamse Thesis Radboud Universiteit Nijmegen - Illustrated
More informationResonances in Chemical Reactions : Theory and Experiment. Toshiyuki Takayanagi Saitama University Department of Chemistry
Resonances in Chemical Reactions : Theory and Experiment Toshiyuki Takayanagi Saitama University Department of Chemistry What is Chemical Reaction? Collision process between molecules (atoms) containing
More informationDecelerating and Trapping Large Polar Molecules
Abstract Decelerating and Trapping Large Polar Molecules David Patterson, dave@cua.harvard.edu Manipulating the motion of large polyatomic molecules, such as benzonitrile (C 6 H 5 CN), presents significant
More informationThe Search for the Electron Electric Dipole Moment at JILA
The Search for the Electron Electric Dipole Moment at JILA Laura Sinclair Aaron Leanhardt, Huanqian Loh, Russell Stutz, Eric Cornell Theory Support: Edmund Meyer and John Bohn June 11, 2008 Funding: NSF
More informationarxiv: v1 [physics.atom-ph] 14 Nov 2018
Multistage Zeeman deceleration of NH X 3 Σ radicals Vikram Plomp, Zhi Gao, Theo Cremers, and Sebastiaan Y. T. van de Meerakker Radboud University, Institute for molecules and materials, Heijendaalseweg
More informationUltracold molecules - a new frontier for quantum & chemical physics
Ultracold molecules - a new frontier for quantum & chemical physics Debbie Jin Jun Ye JILA, NIST & CU, Boulder University of Virginia April 24, 2015 NIST, NSF, AFOSR, ARO Ultracold atomic matter Precise
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 informationSinglet triplet excitation spectrum of the CO He complex. II. Photodissociation and bound-free CO a 3 ]X 1 transitions
JOURNAL OF CHEMICAL PHYSICS VOLUME 119, NUMBER 1 1 JULY 2003 Singlet triplet excitation spectrum of the CO He complex. II. Photodissociation and bound-free CO a 3 ]X 1 transitions W. B. Zeimen, G. C. Groenenboom,
More informationEffects of electric static and laser fields on cold collisions of polar molecules. Roman Krems University of British Columbia
Effects of electric static and laser fields on cold collisions of polar molecules Roman Krems University of British Columbia UBC group: Zhiying Li Timur Tscherbul Erik Abrahamsson Sergey Alyabishev Chris
More informationBuffer-gas cooling of NH via the beam loaded buffer-gas method
Eur. Phys. J. D 31, 307 311 (2004) DOI: 10.1140/epjd/e2004-00140-1 THE EUROPEAN PHYSICAL JOURNAL D Buffer-gas cooling of NH via the beam loaded buffer-gas method D. Egorov, W.C. Campbell, B. Friedrich
More informationDynamics of \(OH(^{2}\Pi) He\) Collisions in Combined Electric and Magnetic Fields
Dynamics of \(OH(^{2}\Pi) He\) Collisions in Combined Electric and Magnetic Fields The Harvard community has made this article openly available. Please share how this access benefits you. Your story matters
More informationCold Controlled Chemistry. Roman Krems University of British Columbia
Cold Controlled Chemistry Roman Krems University of British Columbia Sergey Alyabyshev Zhiying Li Timur Tscherbul Outline Cold and ultracold molecules - denitions Chemistry at ultracold temperatures External
More informationRydberg spectroscopy of Zeeman-decelerated beams of metastable Helium molecules
Rydberg spectroscopy of Zeeman-decelerated beams of metastable Helium molecules Paul Jansen, Michael Motsch, Daniel Sprecher, Frédéric Merkt Laboratorium für Physikalische Chemie, ETH Zürich Motivation
More informationElectronic Transition Spectra of Thiophenoxy and Phenoxy Radicals in Hollow cathode discharges
Electronic Transition Spectra of Thiophenoxy and Phenoxy Radicals in Hollow cathode discharges Tokyo Univ. Science Mitsunori ARAKI, Hiromichi WAKO, Kei NIWAYAMA and Koichi TSUKIYAMA 2014/06/16 2015/2/20
More informationCold Molecules and Controlled Ultracold Chemistry. Jeremy Hutson, Durham University
Cold Molecules and Controlled Ultracold Chemistry Jeremy Hutson, Durham University QuAMP Swansea, 11 Sept 2013 Experimentally accessible temperatures What is already possible in ultracold chemistry? Take
More informationMultistage optical Stark decelerator for a pulsed supersonic beam with a quasi-cw optical lattice
Multistage optical Stark decelerator for a pulsed supersonic beam with a quasi-cw optical lattice Yaling Yin, 1, 2 Qi Zhou, 1 Lianzhong Deng, 1 Yong Xia, 1 and Jianping Yin 1,* 1 State Key Laboratory of
More informationDirect Cooling of Molecules
Direct Cooling of Molecules An overview of the current state of the field Why Cool (Polar) Molecules? Ultracold Chemistry Electron EDM Long-range Interactions The ACME Collaboration, 10.1126/science.1248213
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 informationCold Polar Molecules and their Applications for Quantum Information H.P. Büchler
Cold Polar Molecules and their Applications for Quantum Information H.P. Büchler Theoretische Physik III, Universität Stuttgart, Germany Outline Introduction to polar molecules - quantum melting transition
More informationCold SO 2 molecules by Stark deceleration
Eur. Phys. J. D 46, 463 469 (2008) DOI: 10.1140/epjd/e2008-00001-y THE EUROPEAN PHYSICAL JOURNAL D Cold SO 2 molecules by Stark deceleration O. Bucicov 1,M.Nowak 1, S. Jung 1,a,G.Meijer 2,E.Tiemann 1,andC.Lisdat
More informationPositronium: Old Dog, New Tricks
Positronium: Old Dog, New Tricks David B. Cassidy Department of Physics and Astronomy, University College London, UK d.cassidy@ucl.ac.uk Ps production further improved using beams (1972) which can interact
More informationProbing P & T-violation Beyond the Standard Model. Aaron E. Leanhardt
An Electron EDM Search in HfF + : Probing P & T-violation Beyond the Standard Model Aaron E. Leanhardt Experiment: Laura Sinclair, Russell Stutz & Eric Cornell Theory: Ed Meyer & John Bohn JILA, NIST,
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 informationRenner-Teller Effect in Tetra-Atomic Molecules
Groupe de Chimie Théorique du MSME Renner-Teller Effect in Tetra-Atomic Molecules Laurent Jutier, G. Dhont, H. Khalil and C. Léonard jutier@univ-mlv.fr (non linear) Outline General Presentation Structure
More informationarxiv: v2 [physics.atom-ph] 18 Mar 2010
Deceleration of neutral molecules in macroscopic traveling traps arxiv:0911.3324v2 [physics.atom-ph] 18 Mar 2010 Andreas Osterwalder, 1, 2, Samuel A. Meek, 1 Georg Hammer, 1 Henrik Haak, 1 and Gerard Meijer
More informationA few issues on molecular condensates
A few issues on molecular condensates Outline Background Atomic dark state and creating ground molecular BEC Superchemistry and coherent atom-trimer conversion Quantum dynamics of a molecular matterwave
More informationEDM Measurements using Polar Molecules
EDM Measurements using Polar Molecules B. E. Sauer Imperial College London J. J. Hudson, M. R. Tarbutt, Paul Condylis, E. A. Hinds Support from: EPSRC, PPARC, the EU Two motivations to measure EDMs EDM
More informationFundamentals 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 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 informationATOMIC AND LASER SPECTROSCOPY
ALAN CORNEY ATOMIC AND LASER SPECTROSCOPY CLARENDON PRESS OXFORD 1977 Contents 1. INTRODUCTION 1.1. Planck's radiation law. 1 1.2. The photoelectric effect 4 1.3. Early atomic spectroscopy 5 1.4. The postulates
More informationThe He CaH 2 interaction. II. Collisions at cold and ultracold temperatures
JOURNAL OF CHEMICAL PHYSICS VOLUME 118, NUMBER 16 22 APRIL 2003 The He CaH 2 interaction. II. Collisions at cold and ultracold temperatures N. Balakrishnan a) Department of Chemistry, University of Nevada
More informationOkinawa School in Physics 2017 Coherent Quantum Dynamics. Cold Rydberg gases
Okinawa School in Physics 2017 Coherent Quantum Dynamics Cold ydberg gases 1. Basics of ydberg atoms 2. ydberg atoms in external fields. ydberg-ydberg interaction Wenhui Li Centre for Quantum Technologies
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 pulsed, low-temperature beam of supersonically cooled free radical OH molecules
Chemical Physics Letters 395 (2004) 53 57 www.elsevier.com/locate/cplett A pulsed, low-temperature beam of supersonically cooled free radical OH molecules H.J. Lewandowski *, Eric R. Hudson, J.R. Bochinski,
More informationTowards a Precise Measurement of Atomic Parity Violation in a Single Ra + Ion
Towards a Precise Measurement of Atomic Parity Violation in a Single + Ion TRIµP Program Trapped dioactive Isotopes: µ-laboratories for fundamental Physics Kernfysisch Versneller Instituut (KVI) University
More informationAstrochemistry in temperature variable ion traps
Astrochemistry in temperature variable ion traps Dieter Gerlich Experimental methods Gas phase reactions Typical results: k(t) Selected examples Reaction of O +, N +, and FeO + with H 2 Spectroscopy Spectra
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 informationAn Accurate Calculation of Potential Energy Curves and Transition Dipole Moment for Low-Lying Electronic States of CO
Commun. Theor. Phys. 59 (2013) 193 198 Vol. 59, No. 2, February 15, 2013 An Accurate Calculation of Potential Energy Curves and Transition Dipole Moment for Low-Lying Electronic States of CO LU Peng-Fei
More informationAtoms and Molecules Interacting with Light Atomic Physics for the Laser Era
Atoms and Molecules Interacting with Light Atomic Physics for the Laser Era Peter van der Straten Universiteit Utrecht, The Netherlands and Harold Metcalf State University of New York, Stony Brook This
More informationPhysics with Cold Molecules Using Buffer Gas Cooling
Physics with Cold Molecules Using Buffer Gas Cooling Precision Measurement, Collisions, and Laser Cooling Nick Hutzler, Doyle Group, Harvard University Buffer gas cooling Use inert gas in cryogenic environment
More informationCO (a 3) quenching at a metal surface: Evidence of an electron transfer mediated mechanism
CO (a 3) quenching at a metal surface: Evidence of an electron transfer mediated mechanism Fabian Grätz, Daniel P. Engelhart, Roman J. V. Wagner, Gerard Meijer, Alec M. Wodtke, and Tim Schäfer Citation:
More informationSlow Molecules Produced by Photodissociation
Slow Molecules Produced by Photodissociation Bum Suk Zhao, So Eun Shin, Sung Tai Park, Xingnan Sun, and Doo Soo Chung * Department of Chemistry, Seoul National University, Seoul 151-747, Korea PACS: 37.10.Vz,
More informationObservation 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 informationPDF hosted at the Radboud Repository of the Radboud University Nijmegen
PDF hosted at the Radboud Repository of the Radboud University Nijmegen The following full text is a publisher's version. For additional information about this publication click this link. http://hdl.handle.net/066/13885
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 informationA Linear AC Trap for Polar Molecules in Their Ground State
J. Phys. Chem. A 2007, 111, 7411-7419 7411 A Linear AC Trap for Polar Molecules in Their Ground State Melanie Schnell,*, Peter Lu1tzow, Jacqueline van Veldhoven,, Hendrick L. Bethlem,, Jochen Ku1pper,
More informationMeasurement of the electron EDM using Cold YbF Molecules:
Measurement of the electron EDM using Cold YbF Molecules: E.A. Hinds Imperial College London Lepton Moments 2006, Cape Cod, June 2006 How the electron gets structure point electron + + + - + polarisable
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 informationFundamental physics with antihydrogen and antiprotons at the AD. Michael Doser CERN
Fundamental physics with antihydrogen and antiprotons at the AD Michael Doser CERN What measurements are we talking about? 1) Precise spectroscopic comparison between H and H tests of fundamental symmetry
More informationCollision between magnetically trapped NH molecules in the N =0,J =1 state
PHYSICAL REVIEW A 74, 03710 006 Collision between magnetically trapped NH molecules in the N =0,J =1 state Masatoshi Kajita National Institute of Information and Communications Technology, 4--1 Nukui-Kitamachi,
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 informationCross Sections: Key for Modeling
Cross Sections: Key for Modeling Vasili Kharchenko Department of Physics, University of Connecticut Harvard-Smithsonian Center for Astrophysics, Cambridge, USA 1. Introduction: a) non-thermal atoms and
More informationPHOTO-DISSOCIATION OF CO 2 GAS BY USING TWO LASERS
Proceedings of the 3rd Annual ISC Research Symposium ISCRS 9 April 14, 9, Rolla, Missouri PHOTO-DISSOCIATION OF CO GAS BY USING TWO LASERS Zhi Liang MAE department/zlch5@mst.edu Dr. Hai-Lung Tsai MAE department/tsai@mst.edu
More informationExcitation of high angular momentum Rydberg states
J. Phys. B: At. Mol. Phys. 19 (1986) L461-L465. Printed in Great Britain LE ITER TO THE EDITOR Excitation of high angular momentum Rydberg states W A Molanderi, C R Stroud Jr and John A Yeazell The Institute
More informationlaser-cooling of molecules through optical pumping
Ro-vibrational laser-cooling of molecules through optical pumping 2012 Taiwan International Workshop on Ultracold Atoms and Molecules May 18-20, 2012, Taiwan pierre.pillet@lac.u-psud.fr TAIWAN 2012 2 TAIWAN
More informationarxiv: v1 [physics.atom-ph] 27 Oct 2013
Properties of the ground 3 F 2 state and the excited 3 P state of atomic thorium in cold collisions with 3 He Yat Shan Au, 1,3 Colin B. Connolly, 1,3 Wolfgang Ketterle, 2,3 and John M. Doyle 1,3 1 Department
More informationNet Polarization of a Molecular Beam by Strong Electrostatic or Radiative Fields
Net Polarization of a Molecular Beam by Strong Electrostatic or Radiative Fields Bretislav Friedrich Fritz-Haber-Institut der Max-Planck-Gesellschaft Faradayweg 4-6, D-495 Berlin, Germany Abstract We present
More informationLarge spin relaxation rates in trapped submerged-shell atoms
Large spin relaxation rates in trapped submerged-shell atoms The MIT Faculty has made this article openly available. Please share how this access benefits you. Your story matters. Citation As Published
More informationPhysics and Chemistry with Diatomic Molecules Near Absolute Zero. Tanya Zelevinsky & ZLab Columbia University, New York
Physics and Chemistry with Diatomic Molecules Near Absolute Zero Tanya Zelevinsky & ZLab Columbia University, New York Pupin Labs @ Columbia E. Fermi I. I. Rabi 10 What is Ultracold? MK kk 7 6 5 4 3 2
More informationOperation of a Stark decelerator with optimum acceptance
PHYSICAL REVIEW A 79, 2341 29 Operation of a Stark decelerator with optimum acceptance Ludwig Scharfenberg,* Henrik Haak, Gerard Meijer, and Sebastiaan Y. T. van de Meerakker Fritz-Haber-Institut der Max-Planck-Gesellschaft,
More informationThe emission spectrum due to molecule formation through radiative association
Journal of Physics: Conference Series OPEN ACCESS The emission spectrum due to molecule formation through radiative association To cite this article: Magnus Gustafsson and Gunnar Nyman 214 J. Phys.: Conf.
More informationCharacterization of methanol as a magnetic field tracer in star-forming regions
SUPPLEMENTARY INFORMATION Letters https://doi.org/10.1038/s41550-017-0341-8 In the format provided by the authors and unedited. Characterization of methanol as a magnetic field tracer in star-forming regions
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 informationIonization of Rydberg atoms in Intense, Single-cycle THz field
Ionization of Rydberg atoms in Intense, Single-cycle THz field 4 th year seminar of Sha Li Advisor: Bob Jones Dept. of Physics, Univ. of Virginia, Charlottesville, VA, 22904 April. 15 th, 2013 Outline
More informationTrap Loss Due to Nonadiabatic Transitions in Electrostatically Trapped Ammonia
University of Colorado, Boulder CU Scholar Undergraduate Honors Theses Honors Program Spring 2013 Trap Loss Due to Nonadiabatic Transitions in Electrostatically Trapped Ammonia Kentaro Hoeger University
More informationCold Controlled Chemistry. Roman Krems University of British Columbia
Cold Controlled Chemistry Roman Krems University of British Columbia Sergey Alyabyshev Timur Tscherbul Zhiying Li Outline Cold and ultracold molecules - denitions Chemistry at ultracold temperatures External
More informationQuantum Memory with Atomic Ensembles. Yong-Fan Chen Physics Department, Cheng Kung University
Quantum Memory with Atomic Ensembles Yong-Fan Chen Physics Department, Cheng Kung University Outline Laser cooling & trapping Electromagnetically Induced Transparency (EIT) Slow light & Stopped light Manipulating
More informationAssessment of range-separated time-dependent density-functional theory for calculating C 6 dispersion coefficients
1/10 Assessment of range-separated time-dependent density-functional theory for calculating C 6 dispersion coefficients Julien Toulouse 1,2, Elisa Rebolini 1, Tim Gould 3, John F. Dobson 3, Prasenjit Seal
More informationExperimental Storage Ring - ESR E max = 420 MeV/u, 10 Tm, electron-, stochastic- and laser cooling. Indian Institute of Technology Ropar
Experimental Storage Ring - ESR E max = 420 MeV/u, 10 Tm, electron-, stochastic- and laser cooling Specification of the ESR Particle detectors Re-injection to SIS Two 5 kv rf-cavities Fast Injection Schottky
More informationD. De Fazio, T. V. Tscherbul 2, S. Cavalli 3, and V. Aquilanti 3
D. De Fazio, T. V. Tscherbul, S. Cavalli 3, and V. Aquilanti 3 1 Istituto di Struttura della Materia C.N.R., 00016 Roma, Italy Department of Chemistry, University of Toronto, M5S 3H6, Canada 3 Dipartimento
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 informationAdvanced Electronic Structure Theory Density functional theory. Dr Fred Manby
Advanced Electronic Structure Theory Density functional theory Dr Fred Manby fred.manby@bris.ac.uk http://www.chm.bris.ac.uk/pt/manby/ 6 Strengths of DFT DFT is one of many theories used by (computational)
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 informationPossibilities for a Bose-Einstein Condensed Positronium Annihilation Gamma Ray Laser
Possibilities for a Bose-Einstein Condensed Positronium Annihilation Gamma Ray Laser Allen Mills, Jr., University of California Riverside in collaboration with David Cassidy and Harry Tom (UCR) Rod Greaves
More informationStatus of the ESR And Future Options
Status of the ESR And Future Options M. Steck for the Storage Ring Division (C. Dimopoulou, A. Dolinskii, S. Litvinov, F. Nolden, P. Petri, U. Popp, I. Schurig) Outline 1) New Old ESR 2) Slow (Resonant)
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 informationStudy on Bose-Einstein Condensation of Positronium
Study on Bose-Einstein Condensation of Positronium K. Shu 1, T. Murayoshi 1, X. Fan 1, A. Ishida 1, T. Yamazaki 1,T. Namba 1,S. Asai 1, K. Yoshioka 2, M. Kuwata-Gonokami 1, N. Oshima 3, B. E. O Rourke
More informationPhoton Interaction. Spectroscopy
Photon Interaction Incident photon interacts with electrons Core and Valence Cross Sections Photon is Adsorbed Elastic Scattered Inelastic Scattered Electron is Emitted Excitated Dexcitated Stöhr, NEXAPS
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 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 information1. Cold Collision Basics
ICAP Summer School, Seoul, S. Korea, July 18, 2016 1. Cold Collision Basics Paul S. Julienne Joint Quantum Institute NIST and The University of Maryland Thanks to many colleagues in theory and experiment
More informationPhysics of and in Ion Traps
Physics of and in Ion Traps Proposed Topics: TRIUMF, Vancouver June 01 Basics of Paul- and Penning-traps (equ. of motion, trap geometries, influence of trap imperfections,) Ion detection and cooling (Buffer
More informationarxiv: v1 [physics.atom-ph] 16 Apr 2019
Submitted to Molecular Physics Vol. 00, No. 00, Month 200x, 1 12 ARTICLE arxiv:1904.07628v1 [physics.atom-ph] 16 Apr 2019 Fluorescence-lifetime-limited trapping of Rydberg helium atoms on a chip V. Zhelyazkova
More informationLifetimes of ultralong range Rydberg molecules in a dense Bose Einstein condensate
Lifetimes of ultralong range Rydberg molecules in a dense Bose Einstein condensate Experiment: Joseph D. Whalen, F. Camargo, R. Ding, T. C. Killian, F. B. Dunning Theory: J. Pérez Ríos, S. Yoshida, J.
More informationVibrationally exciting molecules trapped on a microchip
Molecular Physics An International Journal at the Interface Between Chemistry and Physics ISSN: 26-8976 (Print) 362-328 (Online) Journal homepage: http://www.tandfonline.com/loi/tmph2 Vibrationally exciting
More informationREPORT DOCUMENTATION PAGE
REPORT DOCUMENTATION PAGE Form Approved OMB NO. 0704-0188 Public Reporting Burden for this collection of information is estimated to average 1 hour per response, including the time for reviewing instructions,
More information