Emergent $s$-wave interactions in orbitally active quasi-two-dimensional Fermi gases

Colin J. Dale, Kevin G. S. Xie, Kiera Pond Grehan, Shizhong Zhang, Jeff Maki, Joseph H. Thywissen
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Abstract

We investigate the scattering properties and bound states of a quasi-two-dimensional (q2D) spin-polarized Fermi gas near a $p$-wave Feshbach resonance. Strong confinement promotes the out-of-plane spatial wave functions to a discrete, gapped orbital degree of freedom. Exchange-antisymmetric orbital pair wave functions are predicted to give rise to low-energy q2D interactions with $s$-wave symmetry. Using radiofrequency (rf) spectroscopy, we observe the signature power-law scaling and the dimensional-crossover feature anticipated for the emergent $s$-wave channel. Additionally, we demonstrate that two types of low-energy dimers, with either $s$-wave and $p$-wave symmetry, could be formed via rf spin-flip association from an orbital mixture. These findings illustrate how gapped orbital degrees of freedom can provide additional control over scattering symmetries in strongly confined ultracold gases.
轨道上活跃的准二维费米气体中出现的s$波相互作用
我们研究了水系二维(q2D)自旋极化费米气体在 $p$ 波费什巴赫共振附近的散射特性和束缚态。强约束将平面外空间波函数提升到离散、间隙的轨道自由度。据预测,交换不对称轨道对波函数会产生具有 s$ 波对称性的低能 q2D 相互作用。利用射频(rf)光谱,我们观察到了幂律缩放和维度交叉的特征,这是我们对新出现的s$波通道的预期。此外,我们还证明了两种类型的低能二聚体,其对称性分别为s$波和p$波,可通过射频自旋翻转关联从轨道混合物中形成。这些发现证明了间隙轨道自由度如何在强约束超冷气体中提供对散射对称性的额外控制。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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