Effective light-induced Hamiltonian for atoms with large nuclear spin

D. Burba, H. Dunikowski, M. Robert-de-Saint-Vincent, E. Witkowska, G. Juzeliūnas
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Abstract

Ultracold fermionic atoms, having two valence electrons, exhibit a distinctive internal state structure, wherein the nuclear spin becomes decoupled from the electronic degrees of freedom in the ground electronic state. Consequently, the nuclear spin states are well isolated from the environment, rendering these atomic systems an opportune platform for quantum computation and quantum simulations. Coupling with off-resonance light is an essential tool to selectively and coherently manipulate the nuclear spin states. In this paper, we present a systematic derivation of the effective Hamiltonian for the nuclear spin states of ultracold fermionic atoms due to such an off-resonance light. We obtain compact expressions for the scalar, vector, and tensor light shifts taking into account both linear and quadratic contributions to the hyperfine splitting. The analysis has been carried out using the Green operator approach and solving the corresponding Dyson equation. Finally, we analyze different scenarios of light configurations which lead to the vector- and tensor-light shifts, as well as the pure spin-orbit coupling for the nuclear spin.

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大核自旋原子的有效光诱导哈密顿方程
拥有两个价电子的超冷费米子原子呈现出一种独特的内部状态结构,在这种结构中,核自旋与基态电子自由度脱钩。因此,核自旋态与环境完全隔离,使这些原子系统成为量子计算和量子模拟的理想平台。与非共振光耦合是选择性地、相干地操纵核自旋态的重要工具。在本文中,我们系统地推导了超冷费米子原子核自旋态的有效哈密顿。考虑到超精细分裂的线性和二次贡献,我们得到了标量、矢量和张量光移的紧凑表达式。分析采用格林算子方法,并求解相应的戴森方程。最后,我们分析了导致矢量和张量光变的不同光配置方案,以及核自旋的纯自旋轨道耦合。
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