光学晶格中的磁孤子

Xingdong Zhao
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摘要

在这一章中,我们讨论了在光学晶格内的原子自旋子玻色-爱因斯坦凝聚体(BECs)中产生的磁孤子。每个晶格位置的自旋子BECs表现得像自旋磁体,并且可以通过静态磁偶极子-偶极子相互作用(MDDI)相互作用,因此磁孤子可能存在于蓝失谐光学晶格中。通过在晶格中施加外部激光场或在红失谐光学晶格中加载原子,光致偶极子-偶极子相互作用(LDDI)可以产生新的磁孤子。由MDDI和ODDI诱导的远程耦合在光学晶格中的自旋动力学中起主导作用。与固体材料中的自旋链相比较,分别讨论了自旋链的最近邻近似、次近邻近似和远距离情况。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Magnetic Solitons in Optical Lattice
In this chapter, we discuss the magnetic solitons achieved in atomic spinor Bose-Einstein condensates (BECs) confined within optical lattice. Spinor BECs at each lattice site behave like spin magnets and can interact with each other through the static magnetic dipole-dipole interaction (MDDI), due to which the magnetic soliton may exist in blue-detuned optical lattice. By imposing an external laser field into the lattice or loading atoms in a red-detuned optical lattice, the light-induced dipole-dipole interaction (LDDI) can produce new magnetic solitons. The long-range couplings induced by the MDDI and ODDI play a dominant role in the spin dynamics in an optical lattice. Compared with spin chain in solid material, the nearest-neighbor approximation, next-nearest-neighbor approximation, and long-range case are discussed, respectively.
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