Ludwig-Maximilians-Universität, Schellingstraße 4, 80799 München, Germany and Max-Planck-Institut für Quantenoptik, Hans-Kopfermann-Straße 1, 85748 Garching, Germany.
Phys Rev Lett. 2018 Apr 6;120(14):143601. doi: 10.1103/PhysRevLett.120.143601.
We report on the experimental realization of a state-dependent lattice for a two-orbital fermionic quantum gas with strong interorbital spin exchange. In our state-dependent lattice, the ground and metastable excited electronic states of ^{173}Yb take the roles of itinerant and localized magnetic moments, respectively. Repulsive on-site interactions in conjunction with the tunnel mobility lead to spin exchange between mobile and localized particles, modeling the coupling term in the well-known Kondo Hamiltonian. In addition, we find that this exchange process can be tuned resonantly by varying the on-site confinement. We attribute this to a resonant coupling to center-of-mass excited bound states of one interorbital scattering channel.
我们报告了一种实验实现的双轨道费米子量子气体的态相关格子,该气体具有强的轨道间自旋交换。在我们的态相关格子中,^{173}Yb 的基态和亚稳态激发电子态分别充当巡游和局域磁矩的角色。排斥的局域相互作用与隧道迁移率相结合,导致移动和局域粒子之间的自旋交换,模拟了著名的康顿哈密顿量中的耦合项。此外,我们发现通过改变局域限制,这个交换过程可以通过共振来调节。我们将这归因于对一个轨道间散射通道的质心激发束缚态的共振耦合。