2021
DOI: 10.1103/physreva.104.023321
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Three-body spin mixing in spin-1 Bose-Einstein condensates

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Cited by 7 publications
(3 citation statements)
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“…1). In contrast to other studies of few-body physics in a spinor gas [40,41], we work at large magnetic fields (µ B B A hf ) and with a single, well-defined, entrance spin channel (the bb-channel). The model is designed to capture resonant scattering and associated loosely bound states.…”
Section: Model Descriptionmentioning
confidence: 99%
“…1). In contrast to other studies of few-body physics in a spinor gas [40,41], we work at large magnetic fields (µ B B A hf ) and with a single, well-defined, entrance spin channel (the bb-channel). The model is designed to capture resonant scattering and associated loosely bound states.…”
Section: Model Descriptionmentioning
confidence: 99%
“…1). In contrast to other studies of few-body physics in a spinor gas [41,42], we work at large magnetic fields (µ B B A hf ) and with a single, well-defined, entrance spin channel (the bb-channel). The model is designed to capture resonant scattering and associated loosely bound states.…”
Section: Model Descriptionmentioning
confidence: 99%
“…* shinatan@pku.edu.cn For three-body collisions, there are also big differences due to different spatial dimensions or different quantum statistics of the particles. The scattering hypervolume was defined for identical bosons [24], distinguishable particles [25][26][27], and spin-polarized fermions [28] in three dimensions. The scattering hypervolume is a threebody analog of the two-body s-wave or p-wave scattering length.…”
Section: Introductionmentioning
confidence: 99%