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arXiv physics/0201017physics.atom-ph
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通过拉曼跃迁的$λ/4$、$λ/8$和更高阶原子光栅

$λ/4$, $λ/8$, and higher order atom gratings via Raman transitions

B. Dubetsky, P. R. Berman

摘要:

提出了一种使用具有波长$λ$的光场产生具有周期$λ/4$和$λ/8$的原子光栅的方法。反向传播光场驱动基态子能级之间的拉曼跃迁。拉曼场可以由波矢量为2k的有效双光子场来描述,其中k是其中一个场的传播矢量。通过将该拉曼场与具有传播矢量-2 k的{ \em another}拉曼场相结合,实际上产生驻波拉曼场\label{91} %,其“强度”随$\cos (4 k\cdot r).$变化。当原子移动通过该驻波场时,产生具有周期$λ/4$的原子光栅,增加了给定基态流形中的总基态布居可以具有$λ/8$周期性的可能性。导出了产生这种光栅所需的条件。此外,它示出,甚至更高阶的光栅具有小于$λ/8$的周期性可以产生使用一个包括三个(双光子)拉曼场的拉曼场几何形状。虽然大多数计算是在拉曼-纳特近似下进行的,但也讨论了使用拉曼场来产生缩减周期的光晶格。

英文摘要:

A method is proposed for producing atom gratings having period $λ/4$ and $λ/8$ using optical fields having wavelength $λ$. Counterpropagating optical fields drive Raman transitions between ground state sublevels. The Raman fields can be described by an effective two photon field having wave vector 2 k, where k is the propagation vector of one of the fields. By combining this Raman field with {\em another} Raman field having propagation vector -2 k, one, in effect, creates a standing wave Raman field \label{91}%which whose ``intensity'' varies as $\cos (4 k\cdot r).$ When atoms move through this standing wave field, atom gratings having period $λ/4$ are produced, with the added possibility that the total ground state population in a given ground state manifold can have $λ/8$ periodicity. The conditions required to produce such gratings are derived. Moreover, it is shown that even higher order gratings having periodicity smaller than $λ/8$ can be produced using a multicolor field geometry involving three (two-photon) Raman fields. Although most calculations are carried out in the Raman-Nath approximation, the use of Raman fields to create reduced period optical lattices is also discussed.

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