2020
DOI: 10.1103/physreva.101.041601
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Observation of state-to-state hyperfine-changing collisions in a Bose-Fermi mixture of Li6 and K41 atoms

Abstract: Hyperfine-changing collisions are of fundamental interest for the studying of ultracold heteronuclear mixtures. Here, we report the state-to-state study of the hyperfine-changing-collision dynamics in a Bose-Fermi mixture of 6 Li and 41 K atoms. The collision products are directly observed and the spin-changing dynamics is measured. Based on a two-body collision model, the experimental results are simultaneously fitted from which the spin-changing rate coefficient of 1.9(2) × 10 −12 cm 3 · s −1 is gained, bein… Show more

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Cited by 4 publications
(4 citation statements)
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“…In the present case, such a two-photon excited channel is irrelevant. Therefore the idea would be to look for hyperfine-changing collisions (hcc) [66][67][68][69][70] leading to trap loss, especially in shallow traps. This phenomena is taken into account in an effective way in our model through the P S parameter.…”
Section: Resultsmentioning
confidence: 99%
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“…In the present case, such a two-photon excited channel is irrelevant. Therefore the idea would be to look for hyperfine-changing collisions (hcc) [66][67][68][69][70] leading to trap loss, especially in shallow traps. This phenomena is taken into account in an effective way in our model through the P S parameter.…”
Section: Resultsmentioning
confidence: 99%
“…This phenomena is taken into account in an effective way in our model through the P S parameter. Such collisions have long been considered as a serious issue to achieve quantum degeneracy, and now as an additional possibility for controlling the appearance of new quantum phases in quantum gases [70]. Therefore, the OS would manifest by a reduction of losses from the trap, when one of the atoms is prepared in an excited level of the ground state hyperfine manifold.…”
Section: Resultsmentioning
confidence: 99%
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“…[51,52] Secondly, the hyperfine-changing collision for the combinations of 87 Rb|1, 1 + 40 K|9/2, 9/2 is a process of energy absorption and is forbidden. [53][54][55] Thirdly, the difference of heteronuclear elastic collision rates (−235a 0 and −430a 0 ) [56] is a reason for the longer lifetime. Finally, the longer lifetime of 87 Rb |1, 1 and fast thermalization of 87 Rb|1, 1 + 40 K|9/2, 9/2 are also a reason for the spin combination of 87 Rb|1, 1 + 40 K|9/2, 9/2 maintaining longer lifetimes.…”
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confidence: 99%