2005
DOI: 10.1103/physrevlett.94.083004
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Photoassociative Spectroscopy at Long Range in Ultracold Strontium

Abstract: We report photoassociative spectroscopy of 88 Sr2 in a magneto-optical trap operating on the 1 S0 → 3 P1 intercombination line at 689 nm. Photoassociative transitions are driven with a laser red-detuned by 600-2400 MHz from the 1 S0 → 1 P1 atomic resonance at 461 nm. Photoassociation takes place at extremely large internuclear separation, and the photoassociative spectrum is strongly affected by relativistic retardation. A fit of the transition frequencies determines the 1 P1 atomic lifetime (τ = 5.22 ± 0.03 n… Show more

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Cited by 66 publications
(68 citation statements)
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“…The laser cooling, trapping and manipulation of Rb atoms have been wellestablished at the very beginning of the ultracold matter studies [20]. At present the strontium atom is one of the most popular atomic species in ultracold physics [21,22]: for example, the studies of Bose-Einstein condensation of Sr atoms and Bose-Fermi mixtures (of different Sr isotopes) has recently been reported [23][24][25][26][27]. Moreover, the Innsbruck group has developed the STIRAP scheme to produce weakly bound Sr 2 molecules in ground electronic state.…”
Section: Introductionmentioning
confidence: 99%
“…The laser cooling, trapping and manipulation of Rb atoms have been wellestablished at the very beginning of the ultracold matter studies [20]. At present the strontium atom is one of the most popular atomic species in ultracold physics [21,22]: for example, the studies of Bose-Einstein condensation of Sr atoms and Bose-Fermi mixtures (of different Sr isotopes) has recently been reported [23][24][25][26][27]. Moreover, the Innsbruck group has developed the STIRAP scheme to produce weakly bound Sr 2 molecules in ground electronic state.…”
Section: Introductionmentioning
confidence: 99%
“…The creation of samples of 88 Sr or 84 Sr atoms in an optical dipole trap (ODT) starts with laser cooling and trapping phases that have been described in detail previously [22,[27][28][29]. Atoms are trapped in a magneto-optical trap (MOT) operating on the 461-nm 1 S 0 -1 P 1 transition (Fig.…”
Section: Methodsmentioning
confidence: 99%
“…It also reflects the near-ideal scattering properties of this isotope, which has an s-wave elastic scattering length of a = 122.7(3) a 0 [15], where a 0 = 0.53Å. The ground state scattering properties of all Sr isotopes are well-characterized from one- [29,30,31] and twophoton [15] photoassociative spectroscopy, fourier transform molecular spectroscopy [32], and experiments trap- ping various isotopes in optical traps [33,34]. Our apparatus and experimental sequence for laser cooling atoms and loading them into our optical dipole trap were described in [15,35,36], and a timing diagram is shown in Fig.…”
mentioning
confidence: 98%