Photoassociation Spectroscopy of Ultracold Molecules Liantuan XIAO State Key Laboratory of Quantum Optics and Quantum Optics Devices, Institute of Laser.

Slides:



Advertisements
Similar presentations
Raman Spectroscopy A) Introduction IR Raman
Advertisements

Zero-Phonon Line: transition without creation or destruction of phonons Phonon Wing: at T = 0 K, creation of one or more phonons 7. Optical Spectroscopy.
LCLS Atomic Physics with Intense X-rays at LCLS Philip H. Bucksbaum, University of Michigan, Ann Arbor, MI Roger Falcone, University of California, Berkeley,
Ultracold Alkali Metal Atoms and Dimers: A Quantum Paradise Paul S. Julienne Atomic Physics Division, NIST Joint Quantum Institute, NIST/U. Md 62 nd International.
D.L. KOKKIN, N.J. REILLY, J.A. JOESTER, M. NAKAJIMA, K. NAUTA, S.H. KABLE and T.W. SCHMIDT Direct Observation of the c State of C 2 School of Chemistry,
Generation of short pulses
Making cold molecules from cold atoms
Rydberg physics with cold strontium James Millen Durham University – Atomic & Molecular Physics group.
Narrow transitions induced by broad band pulses  |g> |f> Loss of spectral resolution.
Ultraslow Dissociation of H 2 + Via Intense Laser Pulses Presented by: Brad Moser And George Gibson DAMOP 2010.
1 National Cheng Kung University, Tainan, Taiwan First Experimental Observation of the Doubly-Excited 2 1  g State of Na 2 Chin-Chun Tsai, Hui-Wen Wu,
Laser Induced Fluorescence Structural information about the ground and excited states of molecules. Excitation experiments  Excited state information.
Time out—states and transitions Spectroscopy—transitions between energy states of a molecule excited by absorption or emission of a photon h =  E = E.
1 Cold molecules Mike Tarbutt LMI Lecture, 05/11/12.
TOF Mass Spectrometer &
Anh T. Le and Timothy C. Steimle* The molecular frame electric dipole moment and hyperfine interaction in hafnium fluoride, HfF. Department of Chemistry.
Precise Measurement of Vibrational Transition Frequency of Optically Trapped molecules NICT Masatoshi Kajita TMU G. Gopakumar, M. Abe, M. Hada We propose.
Evidence of Radiational Transitions in the Triplet Manifold of Large Molecules Haifeng Xu, Philip Johnson Stony Brook University Trevor Sears Brookhaven.
Determination of fundamental constants using laser cooled molecular ions.
Kinetic Investigation of Collision Induced Excitation Transfer in Kr*(4p 5 5p 1 ) + Kr and Kr*(4p 5 5p 1 ) + He Mixtures Md. Humayun Kabir and Michael.
Towards a finite ensemble of ultracold fermions Timo Ottenstein Max-Planck-Institute for Nuclear Physics Heidelberg 19th International IUPAP Conference.
Photoassociation Spectroscopy of Ytterbium Atoms with Dipole-allowed and Intercombination Transitions K. Enomoto, M. Kitagawa, K. Kasa, S. Tojo, T. Fukuhara,
Experiments with ultracold RbCs molecules Peter Molony Cs Rb.
States and transitions
High-resolution threshold photoionization and photoelectron spectroscopy of propene and 2-butyne Julie M. Michaud, Konstantina Vasilatou and Frédéric Merkt.
Progress towards laser cooling strontium atoms on the intercombination transition Danielle Boddy Durham University – Atomic & Molecular Physics group.
Progress Towards Formation and Spectroscopy of Ultracold Ground-state Rb 2 Molecules in an Optical Trap H.K. Pechkis, M. Bellos, J. RayMajumder, R. Carollo,
Lineshape and Sensitivity of Spectroscopic Signals of N 2 + in a Positive Column Collected Using NICE-OHVMS Michael Porambo, Andrew Mills, Brian Siller,
Electronic Spectroscopy of Palladium Dimer (Pd 2 ) 68th OSU International Symposium on Molecular Spectroscopy Yue Qian, Y. W. Ng and A. S-C. Cheung Department.
Analysis of strongly perturbed 1 1  – 2 3  + – b 3  states of the KRb molecule J. T. Kim 1, Y. Lee 2, and B. Kim 3 1 Department of Photonic Engineering,
Ionization Energy Measurements and Spectroscopy of HfO and HfO+
Stefan Truppe MM-Wave Spectroscopy and Determination of the Radiative branching ratios of 11 BH for Laser Cooling Experiments.
Trap loss of spin-polarized 4 He* & He* Feshbach resonances Joe Borbely ( ) Rob van Rooij, Steven Knoop, Wim Vassen.
Molecular Deceleration Georgios Vasilakis. Outline  Why cold molecules are important  Cooling techniques  Molecular deceleration  Principle  Theory.
Precision Measurement of CO 2 Hotband Transition at 4.3  m Using a Hot Cell PEI-LING LUO, JYUN-YU TIAN, HSHAN-CHEN CHEN, Institute of Photonics Technologies,
W I S S E N T E C H N I K L E I D E N S C H A F T  Januar 13 Name und OE, Eingabe über > Kopf- und Fußzeile.
Molecular Triplet States: Excitation, Detection, and Dynamics Wilton L. Virgo Kyle L. Bittinger Robert W. Field Collisional Excitation Transfer in the.
Dynamics of Low Density Rydberg Gases Experimental Apparatus E. Brekke, J. O. Day, T. G. Walker University of Wisconsin – Madison Support from NSF and.
L. PruvostLab. A. Cotton, Orsay, F Molecular spectroscopy Molecular spectroscopy 2008 Weakly bound molecules. Analysis by the Lu-Fano method coupled.
Spatial distributions in a cold strontium Rydberg gas Graham Lochead.
of Xenon Collision Dimers in the VUV Energy Region
Collisional Orientation Transfer Facilitated Polarization Spectroscopy Jianmei Bai, E. H. Ahmed, B. Beser, Yafei Guan, and A. M. Lyyra Temple University.
PFI-ZEKE Spectroscopy of Aluminum-Imidazole and -Pyrimidine Complexes JUNG SUP LEE, XU WANG, SERGIY KRASNOKUTSKI, and DONG-SHENG YANG University of Kentucky.
Triplet-Singlet Mixing in Si­ 3 : the 1 A A 2 Transition Ruohan Zhang and Timothy C. Steimle International Symposium on Molecular Spectroscopy 68.
高精度分光を目指した CaH + の 生成とトラップ 富山大学・理 森脇喜紀. Spectroscopy of 40 CaH + the pure vibrational transition (v=0, J=0, F=1/2, M=±1/2) → (v=1, J=0, F=1/2, M=±1/2)
An analytical potential for the for the a 3  + state of KLi, (derived from observations of the upper vibrational levels only) Houssam Salami, Amanda Ross,
Spatial distributions in a cold strontium Rydberg gas Graham Lochead.
Spectroscopic analysis of the A and 3 1  + states of 39 K 85 Rb J. T. Kim 1, Y. Lee 2, and B. Kim 3 1 Department of Photonic Engineering, Chosun University.
Laser Spectroscopy of the C 1 Σ + – X 1 Σ + Transition of ScI ZHENWU LIAO, MEI YANG, MAN-CHOR CHAN Department of Chemistry, The Chinese University of Hong.
An Experimental Approach to the Prediction of Complete Millimeter and Submillimeter Spectra at Astrophysical Temperatures Ivan Medvedev and Frank C. De.
Production of vibrationally hot H 2 (v=10–14) from H 2 S photolysis Mingli Niu.
Collisional loss rate measurement of Cesium atoms in MOT Speaker : Wang guiping Date : December 25.
Toward Two-Color Sub-Doppler Saturation Recovery Kinetics in CN (X, v = 0, J) Presented By: Hong Xu 06/22/2015 Chemistry Department Brookhaven National.
Initial Development of High Precision, High Resolution Ion Beam Spectrometer in the Near- Infrared Michael Porambo, Brian Siller, Andrew Mills, Manori.
Multi-step and Multi-photon Excitation Studies of Group-IIB Elements
Resonance-enhanced Photoassociative Formation of Ground-state Rb 2 and Spectroscopy of Mixed-Character Excited States H.K. Pechkis, D. Wang, Y. Huang,
ISMS 2017 at CHAMPAIGN-URBANA, ILLINOIS
Spin Polarization Spectroscopy of
QUANTUM TRANSITIONS WITHIN THE FUNCTIONAL INTEGRATION REAL FUNCTIONAL
The Cs2 a3Su+, 33Sg+, and 33Pg states
Doppler-free two-photon absorption spectroscopy of vibronic excited states of naphthalene assisted by an optical frequency comb UNIV. of Electro-Communications.
Making cold molecules from cold atoms
Experimental Mapping of the Absolute Value of the Transition Dipole Moment Function μe(R) of the Na2 A1Σu+ - X1Σg+ Transition E. Ahmed1, B. Beser1, P.
Atomic Absorption Spectroscopy
from W. Demtröder “Molecular Physics”
Raman Spectroscopy A) Introduction IR Raman
Qubit-induced high-order nonlinear interaction of the polar molecules
from W. Demtröder “Molecular Physics”
Norm Moulton LPS 15 October, 1999
Electronic spectroscopy of DCF
Presentation transcript:

Photoassociation Spectroscopy of Ultracold Molecules Liantuan XIAO State Key Laboratory of Quantum Optics and Quantum Optics Devices, Institute of Laser Spectroscopy, Shanxi University, P.R.China NSFC-ISF Joint Workshop on BEC and Ultracold Phenomena 25, Sep Atom/Molecule Photon

Collaborators PIs: Prof. Liantuan Xiao Prof. Suotang Jia Experiment: Dr. Yanting Zhao Dr. Jie Ma Dr. Jizhou Wu Dr. Zhonghua Ji Yichi Zhang (PhD) Yuqing Li (PhD) Jinpeng Yuan (PhD) Theory: Dr. Gang Chen, Dr. Yongang Yang

Outline Background---Ultracold molecules formation Experimental detection technique ---Trap Loss Detection (TLD) ---Ionization Detection (ID) Experimental results---High sensitive spectroscopy Conclusion Photoassociation Spectroscopy of Ultracold Molecules Background---Ultracold molecules formation Experimental detection technique ---Trap Loss Detection (TLD) ---Ionization Detection (ID) Experimental results---High sensitive spectroscopy Conclusion Photoassociation Spectroscopy of Ultracold Molecules

1. Fundamental research * High resolution molecular spectroscopy * Weak interaction in molecules 2. Superchemistry * Elastic and inelastic cold collisions * Cold chemistry. 3. Solid state physics generated by an ultracold dilute ensemble * Observation of BEC with molecules * Investigation of dipole-dipole interactions of polar molecules. 4. Quantum computation Why cold molecules? [1] John M. Doyle, Bretisiav Friedrich. Nature. (1999) Vol. 401, 749. [2] K. M. Jones, E. Tiesinga, P. D. Lett, P. S. Julienne. Rev. Mod. Phys. (2006) Vol. 78, 483.

1) Buffer gas cooling 2) Stark cooling 3) V- ​​ selected cooling 1) Feshbach resonance How to form ultracold molecules : Direct Indirect 2) Photoassociation

Outline Background---Ultracold molecules formation Experimental detection technique ---Trap Loss Detection (TLD) ---Ionization Detection (ID) Experimental results---High sensitive spectroscopy Conclusion Photoassociation Spectroscopy of Ultracold Molecules

Photoassociation Resonant photon absorption by two cold atoms (T~10uK) (1) Deexcitation (2') (2) free Atoms Cold molecules (1) (2) (2’) Photoassociation (PA) of cold atoms: PA process for a pair of cold Cs atoms. Cs 2 and RbCs

* The trap-loss spectrum, reveals virotational progressions for all attractive potentials which can be reached by PA. The decay into either a pair of hot atoms, or a stable molecule, induces a decrease of the atom trap fluorescence. * The ion spectrum, shows the ions yield obtained by photoionisation of the stable ultracold molecules created either in the ground state or in the lowest triplet state. The electronically excited molecules formed by PA have a too short lifetime to give a significant contribution to the photoionisation signal. Cold Molecules detection: * PA spectroscopy of ultracold atoms provides information on the molecular excited state levels which is essential for determination of the molecular parameters, and therefore for potential curves.

Outline Background---Ultracold molecules formation Experimental detection technique ---Trap Loss Detection (TLD) ---Ionization Detection (ID) Experimental results---High sensitive spectroscopy Conclusion Photoassociation Spectroscopy of Ultracold Cesium Molecules

(a) Experimental setup. (b) Detection scheme of the three dimensional fluorescence modulation spectroscopy of ultracold molecules. Improve the trap loss spectrum sensitivity ---Three-dimensional fluorescence modulation spectroscopy We have compared the spectral signal by using direct trap loss detection with three dimensional fluorescence modulation spectroscopy. Under the same conditions, signal to noise ratio (SNR) of three dimensional modulation spectroscopy had increased by more than 20 times than the direct trap loss spectroscopy ! PS: The detail of three-dimensional fluorescence modulation spectroscopy is in the paper ( Phys. Chem. Chem. Phys. 13 (2011) )

Three dimensions velocity selective spectroscopy Fluorescence emit rate : Δ l : probe laser detune Probe laser frequency modulated means to detect partial atoms being selected. Fluorescence intensity modulated Modulated fluorescence Demodulated spectrum A: modulation amplitude f : modulation frequency

By using the three-dimensional modulation spectroscopy the signal-to-noise ratio of the spectra is improved and ultimately the PA spectra obtained by detecting trap loss are extended to a red detuning of ~70 cm -1 below the dissociation limit. J. Mol. Spectrosc., 255, 106 (2009). 1 、 Vibrational spectroscopy of excited states of ultracold Cs 2 Setup

The low-lying vibrational spectroscopy of Cs 2 0 g - pure long-range state have been observed with rotational structures, which are well resolved up to J=0~8. The rotational constants are obtained by fitting experimental data to a nonrigid rotation model. Opt. Express, 18, (2010) 2 、 Rovibrational spectroscopy of excited states of ultracold Cs 2 Dependence of the level intervals on the rotational quantum number J Dependence of the rotational constant B on the vibrational numberυ

According to the calculated Franck-Condon factor, as a function of the vibrational level for PA transition of the Cs 2 0 g - (6P 3/2 ) outer well, the intensity of the trap loss spectra of the lowest level are very small. The v = 2 and 3 vibrational levels of the pure long- range state 0g- (6P3/2) of cesium molecule are detected directly with high rotational resolution. Phys. Chem. Chem. Phys., 13, (2011) 3 、 PA spectrum of the lowest v excited state of ultracold Cs 2 ---v=2,3 Theoretical Franck-Condon factor of Cs 2 0 g - (6P 3/2 ) PA spectra of the vibrational state (v=3) PA spectra of the lowest vibrational state (v=2)

3 、 PA spectrum of the lowest v excited state of ultracold Cs 2 ---v=0,1

4 、 Determination of laser-induced frequency shifts of ultracold Cs 2 (a) Laser-induced frequency shift of the PA resonance as a function of PA laser intensity for different rotational progressions (J=2,3,4) of v=17 of the 0 g − long-range state and (b) different molecular vibrational bound states. Optics Letters, 36, 2038 (2011). We experimentally present a technique for sensitively determining the laser-induced frequency shifts of the ultracold cesium molecular vibrational and rotational levels. The scheme relies on an optical frequency shifter, leading to two laser beams with a precise and adjustable frequency interval.

5 、 Direct measurement of laser-induced frequency shift rate of ultracold Cs 2 We carried on a quantitative determination of the laser- induced frequency shift rate of the ultracold Cs 2 formed via PA by means of the trap loss measurement of the losses of trapped atoms in a standard magneto-optical trap. The experiment was directly performed by varying the photoassociation laser intensity without any additional frequency monitor technologies. Appl. Phys. Lett., 101, (2012) The inset sketch shows the LIFS rate achieved in the same experimental conditions.

Comparison between homonuclear and heteronuclear molecules PA probability is lower for heteronuclear molecules. The ionization detection is a good method for heteronuclear molecules RbCs molecular potential energy curves and ionization detection process

6 、 Photoassociation spectrum of ultracold RbCs molecules by ionization detection RbCs + molecular ion with and without PA laser RbCs photoassociation spectrum in v=10, (4)0 -, correlated to (2) 3 Π Rotational constant is cm -1 and the distortion constant is cm -1.

7 、 The electric dipole moment measurement of RbCs molecules J=0 , J≠0 The measured electric dipole moment the observed RbCs molecules in v=10, (4)0 -, correlated to (2) 3 Πstate is 4.7±0.6Debye by dc Stark effect. Phys. Rev. A, 85, (2012)

8 、 The photoassociation lineshape analysis of ultracold RbCs molecules Intensity and FWHM fitting by wigner formula Spectroscopy intensity vs ionization laser energy The intensity vs PA laser intensity The FWHM vs PA laser intensity Two-photon photoionization rate : J. Phys. Soc. Jap (2013) Using the ionization detection, we observe the saturation of PA process and the suppression of ionization process.

Outline Background---Ultracold molecules formation Experimental detection technique ---Trap Loss Detection (TLD) ---Ionization Detection (ID) Experimental results---High sensitive spectroscopy Conclusion Photoassociation Spectroscopy of Ultracold Molecules

Conclusion  Two detection technology in photoassociative molecules ◆ Improved Trap loss detection in homonuclear molecules ◆ Ionization detection in heteronuclear molecules  Based on the high sensitive detection methods ◆ PA spectroscopy of excited states of ultracold Cs 2 and RbCs ◆ Precision measurement of LIFS rate for Cs 2 ◆ The electric dipole moment measurement of RbCs ◆ The photoassociation lineshape analysis of ultracold RbCs

Thanks for your attention ! Welcome to Institute of Laser University