AustralieFrV1, PascalFrancis, Curation, bibRecord, 004780

Population redistribution in optically trapped polar molecules

Identifieur interne : 004780 ( PascalFrancis/Curation ); précédent : 004779; suivant : 004781

Population redistribution in optically trapped polar molecules

Auteurs : J. Deiglmayr [Allemagne] ; M. Repp [Allemagne] ; O. Dulieu [France] ; R. Wester [Australie] ; M. Weidemüller [Allemagne]

Source :

The European physical journal. D, Atomic, molecular and optical physics : (Print) [ 1434-6060 ] ; 2011.

RBID : Pascal:12-0019049

Descripteurs français

Pascal (Inist)
- Piégeage optique, Emission spontanée, Photoassociation, Etude théorique, Calcul ab initio, Courbe potentiel, Etat fondamental, Etat rotationnel, Moment dipolaire électrique, Molécule polaire, Molécule ultrafroide, Rayonnement corps noir, Etude comparative, Collision atome atome, Collision sous rayonnement, 3450R, 3380P, 3115A.

English descriptors

KwdEn :
- Ab initio calculations, Atom-atom collisions, Blackbody radiation, Comparative study, Electric dipole moments, Ground states, Optical trapping, Photoassociation, Polar molecule, Potential energy curve, Radiation assisted collision, Rotational states, Spontaneous emission, Theoretical study, Ultracold molecules.

Abstract

We investigate the rovibrational population redistribution of polar molecules in the electronic ground state induced by spontaneous emission and blackbody radiation. As a model system we use optically trapped LiCs molecules formed by photoassociation in an ultracold two-species gas. The population dynamics of vibrational and rotational states is modeled using an ab initio electric dipole moment function and experimental potential energy curves. Comparison with the evolution of the v" = 3 electronic ground state yields good qualitative agreement. The analysis provides important input to assess applications of ultracold LiCs molecules in quantum simulation and ultracold chemistry.

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A03		`1`		`@0 Eur. phys. j., D At. mol. opt. phys.`
A05				`@2 65`
A06				`@2 1-2`
A08	`01`	`1`	`ENG`	`@1 Population redistribution in optically trapped polar molecules`
A09	`01`	`1`	`ENG`	`@1 Cold Quantum Matter`
A11	`01`	`1`		`@1 DEIGLMAYR (J.)`
A11	`02`	`1`		`@1 REPP (M.)`
A11	`03`	`1`		`@1 DULIEU (O.)`
A11	`04`	`1`		`@1 WESTER (R.)`
A11	`05`	`1`		`@1 WEIDEMÜLLER (M.)`
A12	`01`	`1`		`@1 BIRKL (Gerhard) @9 ed.`
A12	`02`	`1`		`@1 FOOT (Christopher) @9 ed.`
A12	`03`	`1`		`@1 FREEGARDE (Tim) @9 ed.`
A12	`04`	`1`		`@1 GRIMM (Rudolf) @9 ed.`
A12	`05`	`1`		`@1 HUTSON (Jeremy M.) @9 ed.`
A12	`06`	`1`		`@1 WEIDEMÜLLER (Matthias) @9 ed.`
A14	`01`			`@1 Ruprecht-Karls-Universität Heidelberg, Physikalisches Institut, Philosophenweg 12 @2 69120 Heidelberg @3 DEU @Z 1 aut. @Z 2 aut. @Z 5 aut.`
A14	`02`			`@1 Laboratoire Aime Cotton, CNRS, Universite Paris Sud XI, Bât. 505 @2 91405 Orsay @3 FRA @Z 3 aut.`
A14	`03`			`@1 Universität Innsbruck, Institut f. Ionenphysik und Angewandte Physik, Technikerstrasse 25/3 @2 6020 Innsbruck @3 AUS @Z 4 aut.`
A15	`01`			`@1 University of Darmstad @3 DEU @Z 1 aut.`
A15	`02`			`@1 University of Oxford @3 GBR @Z 2 aut.`
A15	`03`			`@1 University of Southampton @3 GBR @Z 3 aut.`
A15	`04`			`@1 University of Innsbruck @3 AUS @Z 4 aut.`
A15	`05`			`@1 University of Durham @3 GBR @Z 5 aut.`
A15	`06`			`@1 University of Heidelberg @3 DEU @Z 6 aut.`
A20				`@1 99-104`
A21				`@1 2011`
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A47	`01`	`1`		`@0 12-0019049`
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A64	`01`	`1`		`@0 The European physical journal. D, Atomic, molecular and optical physics : (Print)`
A66	`01`			`@0 FRA`
C01	`01`		`ENG`	@0 We investigate the rovibrational population redistribution of polar molecules in the electronic ground state induced by spontaneous emission and blackbody radiation. As a model system we use optically trapped LiCs molecules formed by photoassociation in an ultracold two-species gas. The population dynamics of vibrational and rotational states is modeled using an ab initio electric dipole moment function and experimental potential energy curves. Comparison with the evolution of the v" = 3 electronic ground state yields good qualitative agreement. The analysis provides important input to assess applications of ultracold LiCs molecules in quantum simulation and ultracold chemistry.
C02	`01`	`3`		`@0 001B30A15A`
C02	`02`	`3`		`@0 001B30D50R`
C02	`03`	`3`		`@0 001B30C80P`
C03	`01`	`3`	`FRE`	`@0 Piégeage optique @5 03`
C03	`01`	`3`	`ENG`	`@0 Optical trapping @5 03`
C03	`02`	`3`	`FRE`	`@0 Emission spontanée @5 04`
C03	`02`	`3`	`ENG`	`@0 Spontaneous emission @5 04`
C03	`03`	`3`	`FRE`	`@0 Photoassociation @5 05`
C03	`03`	`3`	`ENG`	`@0 Photoassociation @5 05`
C03	`04`	`3`	`FRE`	`@0 Etude théorique @5 21`
C03	`04`	`3`	`ENG`	`@0 Theoretical study @5 21`
C03	`05`	`3`	`FRE`	`@0 Calcul ab initio @5 23`
C03	`05`	`3`	`ENG`	`@0 Ab initio calculations @5 23`
C03	`06`	`X`	`FRE`	`@0 Courbe potentiel @5 24`
C03	`06`	`X`	`ENG`	`@0 Potential energy curve @5 24`
C03	`06`	`X`	`SPA`	`@0 Curva potencial @5 24`
C03	`07`	`3`	`FRE`	`@0 Etat fondamental @5 41`
C03	`07`	`3`	`ENG`	`@0 Ground states @5 41`
C03	`08`	`3`	`FRE`	`@0 Etat rotationnel @5 42`
C03	`08`	`3`	`ENG`	`@0 Rotational states @5 42`
C03	`09`	`3`	`FRE`	`@0 Moment dipolaire électrique @5 43`
C03	`09`	`3`	`ENG`	`@0 Electric dipole moments @5 43`
C03	`10`	`X`	`FRE`	`@0 Molécule polaire @5 57`
C03	`10`	`X`	`ENG`	`@0 Polar molecule @5 57`
C03	`10`	`X`	`SPA`	`@0 Molécula polar @5 57`
C03	`11`	`3`	`FRE`	`@0 Molécule ultrafroide @2 NK @5 58`
C03	`11`	`3`	`ENG`	`@0 Ultracold molecules @2 NK @5 58`
C03	`12`	`3`	`FRE`	`@0 Rayonnement corps noir @5 61`
C03	`12`	`3`	`ENG`	`@0 Blackbody radiation @5 61`
C03	`13`	`X`	`FRE`	`@0 Etude comparative @5 62`
C03	`13`	`X`	`ENG`	`@0 Comparative study @5 62`
C03	`13`	`X`	`SPA`	`@0 Estudio comparativo @5 62`
C03	`14`	`3`	`FRE`	`@0 Collision atome atome @5 63`
C03	`14`	`3`	`ENG`	`@0 Atom-atom collisions @5 63`
C03	`15`	`X`	`FRE`	`@0 Collision sous rayonnement @5 64`
C03	`15`	`X`	`ENG`	`@0 Radiation assisted collision @5 64`
C03	`15`	`X`	`SPA`	`@0 Colisión bajo radiación @5 64`
C03	`16`	`3`	`FRE`	`@0 3450R @4 INC @5 83`
C03	`17`	`3`	`FRE`	`@0 3380P @4 INC @5 84`
C03	`18`	`3`	`FRE`	`@0 3115A @4 INC @5 91`
N21				`@1 002`

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<front><div type="abstract" xml:lang="en">We investigate the rovibrational population redistribution of polar molecules in the electronic ground state induced by spontaneous emission and blackbody radiation. As a model system we use optically trapped LiCs molecules formed by photoassociation in an ultracold two-species gas. The population dynamics of vibrational and rotational states is modeled using an ab initio electric dipole moment function and experimental potential energy curves. Comparison with the evolution of the v" = 3 electronic ground state yields good qualitative agreement. The analysis provides important input to assess applications of ultracold LiCs molecules in quantum simulation and ultracold chemistry.</div>
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<fC01 i1="01" l="ENG"><s0>We investigate the rovibrational population redistribution of polar molecules in the electronic ground state induced by spontaneous emission and blackbody radiation. As a model system we use optically trapped LiCs molecules formed by photoassociation in an ultracold two-species gas. The population dynamics of vibrational and rotational states is modeled using an ab initio electric dipole moment function and experimental potential energy curves. Comparison with the evolution of the v" = 3 electronic ground state yields good qualitative agreement. The analysis provides important input to assess applications of ultracold LiCs molecules in quantum simulation and ultracold chemistry.</s0>
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<fC03 i1="05" i2="3" l="ENG"><s0>Ab initio calculations</s0>
<s5>23</s5>
</fC03>
<fC03 i1="06" i2="X" l="FRE"><s0>Courbe potentiel</s0>
<s5>24</s5>
</fC03>
<fC03 i1="06" i2="X" l="ENG"><s0>Potential energy curve</s0>
<s5>24</s5>
</fC03>
<fC03 i1="06" i2="X" l="SPA"><s0>Curva potencial</s0>
<s5>24</s5>
</fC03>
<fC03 i1="07" i2="3" l="FRE"><s0>Etat fondamental</s0>
<s5>41</s5>
</fC03>
<fC03 i1="07" i2="3" l="ENG"><s0>Ground states</s0>
<s5>41</s5>
</fC03>
<fC03 i1="08" i2="3" l="FRE"><s0>Etat rotationnel</s0>
<s5>42</s5>
</fC03>
<fC03 i1="08" i2="3" l="ENG"><s0>Rotational states</s0>
<s5>42</s5>
</fC03>
<fC03 i1="09" i2="3" l="FRE"><s0>Moment dipolaire électrique</s0>
<s5>43</s5>
</fC03>
<fC03 i1="09" i2="3" l="ENG"><s0>Electric dipole moments</s0>
<s5>43</s5>
</fC03>
<fC03 i1="10" i2="X" l="FRE"><s0>Molécule polaire</s0>
<s5>57</s5>
</fC03>
<fC03 i1="10" i2="X" l="ENG"><s0>Polar molecule</s0>
<s5>57</s5>
</fC03>
<fC03 i1="10" i2="X" l="SPA"><s0>Molécula polar</s0>
<s5>57</s5>
</fC03>
<fC03 i1="11" i2="3" l="FRE"><s0>Molécule ultrafroide</s0>
<s2>NK</s2>
<s5>58</s5>
</fC03>
<fC03 i1="11" i2="3" l="ENG"><s0>Ultracold molecules</s0>
<s2>NK</s2>
<s5>58</s5>
</fC03>
<fC03 i1="12" i2="3" l="FRE"><s0>Rayonnement corps noir</s0>
<s5>61</s5>
</fC03>
<fC03 i1="12" i2="3" l="ENG"><s0>Blackbody radiation</s0>
<s5>61</s5>
</fC03>
<fC03 i1="13" i2="X" l="FRE"><s0>Etude comparative</s0>
<s5>62</s5>
</fC03>
<fC03 i1="13" i2="X" l="ENG"><s0>Comparative study</s0>
<s5>62</s5>
</fC03>
<fC03 i1="13" i2="X" l="SPA"><s0>Estudio comparativo</s0>
<s5>62</s5>
</fC03>
<fC03 i1="14" i2="3" l="FRE"><s0>Collision atome atome</s0>
<s5>63</s5>
</fC03>
<fC03 i1="14" i2="3" l="ENG"><s0>Atom-atom collisions</s0>
<s5>63</s5>
</fC03>
<fC03 i1="15" i2="X" l="FRE"><s0>Collision sous rayonnement</s0>
<s5>64</s5>
</fC03>
<fC03 i1="15" i2="X" l="ENG"><s0>Radiation assisted collision</s0>
<s5>64</s5>
</fC03>
<fC03 i1="15" i2="X" l="SPA"><s0>Colisión bajo radiación</s0>
<s5>64</s5>
</fC03>
<fC03 i1="16" i2="3" l="FRE"><s0>3450R</s0>
<s4>INC</s4>
<s5>83</s5>
</fC03>
<fC03 i1="17" i2="3" l="FRE"><s0>3380P</s0>
<s4>INC</s4>
<s5>84</s5>
</fC03>
<fC03 i1="18" i2="3" l="FRE"><s0>3115A</s0>
<s4>INC</s4>
<s5>91</s5>
</fC03>
<fN21><s1>002</s1>
</fN21>
</pA>
</standard>
</inist>
</record>

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   |texte=   Population redistribution in optically trapped polar molecules
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	Serveur d'exploration sur les relations entre la France et l'Australie
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Population redistribution in optically trapped polar molecules

Population redistribution in optically trapped polar molecules

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