Abdelrahman A, Hannaford P, Alameh K
Electron Science Research Institute, Edith Cowan University, 270 Joondalup Drive, Perth, WA 6027, Australia.
Opt Express. 2009 Dec 21;17(26):24358-70. doi: 10.1364/OE.17.024358.
We propose a new method to create an asymmetric two-dimensional magnetic lattice which exhibits magnetic band gap structure similar to semiconductor devices. The quantum device is assumed to host bound states of collective excitations formed in a magnetically trapped quantum degenerate gas of ultracold atoms such as a Bose-Einstein condensate (BEC) or a degenerate Fermi gas. A theoretical framework is established to describe possible realization of the exciton-Mott to discharging Josephson states oscillations in which the adiabatically controlled oscillations induce ac and dc Josephson atomic currents where this effect can be used to transfer n Josephson qubits across the asymmetric two-dimensional magnetic lattice. We consider second-quantized Hamiltonians to describe the Mott insulator state and the coherence of multiple tunneling between adjacent magnetic lattice sites where we derive the self consistent non-linear Schrödinger equation with a proper field operator to describe the exciton Mott quantum phase transition via the induced Josephson atomic current across the n magnetic bands.
我们提出了一种创建非对称二维磁晶格的新方法,该晶格展现出类似于半导体器件的磁带隙结构。假设量子器件承载在磁阱中超冷原子的磁捕获量子简并气体(如玻色 - 爱因斯坦凝聚体(BEC)或简并费米气体)中形成的集体激发的束缚态。建立了一个理论框架来描述激子 - 莫特到放电约瑟夫森态振荡的可能实现,其中绝热控制的振荡会诱导交流和直流约瑟夫森原子电流,这种效应可用于在非对称二维磁晶格中传输n个约瑟夫森量子比特。我们考虑二次量子化哈密顿量来描述莫特绝缘体状态以及相邻磁晶格位点之间多次隧穿的相干性,在此我们通过适当的场算符推导出自洽非线性薛定谔方程,以描述通过跨越n个磁能带的感应约瑟夫森原子电流实现的激子莫特量子相变。