Hanna Thomas M, Tiesinga Eite, Mitchell William F, Julienne Paul S
Joint Quantum Institute, National Institute of Standards and Technology, and University of Maryland, 100 Bureau Drive, Stop 8423, Gaithersburg, Maryland 20899-8423, USA.
Applied and Computational Mathematics Division, National Institute of Standards and Technology, 100 Bureau Drive, Stop 8910, Gaithersburg, Maryland 20899-8910, USA.
Phys Rev A. 2012 Feb;85(2). doi: 10.1103/PhysRevA.85.022703.
We study the resonant control of two nonreactive polar molecules in an optical lattice site, focusing on the example of RbCs. Collisional control can be achieved by tuning bound states of the intermolecular dipolar potential by varying the applied electric field or trap frequency. We consider a wide range of electric fields and trapping geometries, showing that a three-dimensional optical lattice allows significantly wider avoided crossings than free space or quasi-two dimensional geometries. Furthermore, we find that dipolar confinement-induced resonances can be created with reasonable trapping frequencies and electric fields, and have widths that will enable useful control in forthcoming experiments.
我们研究了光晶格位点中两个非反应性极性分子的共振控制,重点以铷铯为例。通过改变外加电场或阱频率来调节分子间偶极势的束缚态,从而实现碰撞控制。我们考虑了广泛的电场和俘获几何结构,结果表明,与自由空间或准二维几何结构相比,三维光晶格允许更宽的避免交叉。此外,我们发现,利用合理的俘获频率和电场可以产生偶极囚禁诱导的共振,其宽度将有助于在未来的实验中进行有效控制。