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在三能级和四能级双原子系统中利用啁啾激光脉冲通过光致势对绝热通道的分析。

Analysis of adiabatic passage by light-induced potentials with chirped laser pulses in three- and four-level diatomic systems.

作者信息

Heesel E, Garraway B M, Marangos J P

机构信息

Quantum Optics and Laser Science Group, Blackett Laboratory, Imperial College, London SW7 2BW, United Kingdom.

出版信息

J Chem Phys. 2006 Jan 14;124(2):024320. doi: 10.1063/1.2150435.

Abstract

This paper describes an investigation into the process of adiabatic passage by light-induced potentials (APLIP), which was previously suggested as a method for employing two strong picosecond laser pulses to transfer the population between two electronic states. We have extended earlier numerical studies in order to assess the feasibility of an experimental implementation of the APLIP concept. APLIP has been modeled in a three-level model system based on Na2 with chirped pulses, using laser parameters available from a typical chirped pulse amplified Ti:sapphire laser. The model showed that the APLIP process remains essentially unchanged for chirped pulses of equal magnitude and the opposite, or equal and positive sign of chirp as compared to the transform-limited case. We also examined the case of additional electronic states by introduction of a fourth state that lies close to the "target," i.e., final, state. The investigation showed that there are circumstances in which a significant fraction of the population gets transferred to this state which will disrupt the APLIP process. However, by switching to this fourth state as the target state in an experiment, good transfer efficiency is recovered. The results of the extension of the original APLIP modeling to chirped pulses and additional electronic states indicate that an APLIP experimental realization should be feasible in Na2.

摘要

本文描述了对光致势绝热通道(APLIP)过程的一项研究,该过程先前被提议作为一种利用两个强皮秒激光脉冲在两个电子态之间转移粒子数的方法。我们扩展了早期的数值研究,以评估APLIP概念实验实现的可行性。基于Na₂并使用啁啾脉冲,在一个三能级模型系统中对APLIP进行了建模,所使用的激光参数来自典型的啁啾脉冲放大钛宝石激光器。该模型表明,与变换极限情况相比,对于幅度相等且啁啾符号相反或相等且为正的啁啾脉冲,APLIP过程基本保持不变。我们还通过引入一个靠近“目标”(即终态)的第四态来研究额外电子态的情况。研究表明,在某些情况下,相当一部分粒子数会转移到这个态,这将干扰APLIP过程。然而,在实验中通过切换到这个第四态作为目标态,可以恢复良好的转移效率。将原始APLIP建模扩展到啁啾脉冲和额外电子态的结果表明,在Na₂中实现APLIP实验应该是可行的。

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