Campbell D L, Spielman I B
Joint Quantum Institute, University of Maryland and National Institute of Standards and Technology, College Park, MD 20742, USA.
New J Phys. 2016 Mar;18. doi: 10.1088/1367-2630/18/3/033035. Epub 2016 Apr 1.
We theoretically explore a Rashba spin-orbit coupling scheme which operates entirely in the absolute ground state manifold of an alkali atom, thereby minimizing all inelastic processes. An energy gap between ground eigenstates of the proposed coupling can be continuously opened or closed by modifying laser polarizations. Our technique uses far-detuned 'Raman' laser coupling to create the Rashba potential, which has the benefit of low spontaneous emission rates. At these detunings, the Raman matrix elements that link magnetic sublevel quantum numbers separated by two are also suppressed. These matrix elements are necessary to produce the Rashba Hamiltonian within a single total angular momentum manifold. However, the far-detuned Raman couplings can link the three states familiar to quantum chemistry, which possess the necessary connectivity to realize the Rashba potential. We show that these states are essentially the hyperfine spin eigenstates of Rb dressed by a strong radio-frequency magnetic field.
我们从理论上探索了一种Rashba自旋轨道耦合方案,该方案完全在碱金属原子的绝对基态流形中运行,从而将所有非弹性过程降至最低。通过改变激光偏振,可以连续打开或关闭所提出耦合的基态本征态之间的能隙。我们的技术使用远失谐的“拉曼”激光耦合来创建Rashba势,其优点是自发发射率低。在这些失谐情况下,连接相差两个磁子能级量子数的拉曼矩阵元也会受到抑制。这些矩阵元对于在单个总角动量流形内产生Rashba哈密顿量是必要的。然而,远失谐拉曼耦合可以连接量子化学中熟悉的三个态,它们具有实现Rashba势所需的连通性。我们表明,这些态本质上是由强射频磁场修饰的Rb的超精细自旋本征态。