首页> 外文OA文献 >Dynamic hyperpolarizability and two-photon detachment in the presence of a strong static electric field: Application to H\u3csup\u3e-\u3c/sup\u3e
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Dynamic hyperpolarizability and two-photon detachment in the presence of a strong static electric field: Application to H\u3csup\u3e-\u3c/sup\u3e

机译:在强静电场存在下的动态超极化和双光子分离:应用于H \ u3csup \ u3e- \ u3c / sup \ u3e

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摘要

Our recent analysis [J. Phys. B 33, R141 (2000)] of the problem of H- in both laser and strong static electric fields, which treated effects that are linear in the laser intensity l (e.g., the dynamic polarizability and the single-photon detachment cross section), is extended here to treat effects of higher order (∼l2) in the laser intensity (e.g., the dynamic hyperpolarizability, the two-photon detachment cross section, the linear in l corrections to the single-photon detachment rate, etc). We introduce the concept of the dynamic hyperpolarizability of an atom in the presence of a strong electric field based on the complex quasienergy approach with properly normalized, quasistationary quasienergy wave functions. Our analysis of the general structure of the dynamic hyperpolarizability tensor of an atom in a nondegenerate (S-) state is performed for arbitrary field geometries and laser polarizations. The connection of the hyperpolarizability γ(F;ω) to the complex quasienergy and to atomic ionization rates is established. Analytic results (in terms of Airy functions) are obtained for five irreducible components of a hyperpolarizability tensor (that are independent of the laser polarization and the field geometry) for the case of a weakly bound electron in a three-dimensional, zero-range potential. These results are used for the analysis of the frequency, field geometry, and laser polarization dependence of the two-photon detachment rate as well as of the linear in laser intensity corrections to the single-photon detachment rate. It is shown that the oscillatory behavior of the frequency dependence of both the real and the imaginary parts of γ(F;ω) exists for both the coplanar and orthogonal field geometries, and that this behavior is qualitatively different for frequencies below and above the single-photon detachment threshold. The threshold behavior of the two-photon detachment rate is analyzed in detail and the static electric-field-induced modification of Wigner’s threshold law for a short-range potential is discussed.
机译:我们最近的分析[J.物理[B 33,R141(2000)]处理激光和强静电场中的H-问题,该问题处理了激光强度l中线性的效应(例如,动态极化率和单光子分离截面),本文扩展到治疗激光强度更高阶(〜l2)的效应(例如,动态超极化率,双光子分离截面,单光子分离速率的线性校正)等。基于具有适当归一化的准平稳拟能波函数的复杂拟能方法,我们介绍了在强电场存在下原子的动态超极化性的概念。对于任意场几何形状和激光偏振,我们对处于非简并(S-)状态的原子的动态超极化率张量的一般结构进行了分析。建立了超极化率γ(F;ω)与复拟能以及原子电离率的关系。对于在三维零位范围电势中弱束缚电子的情况,获得了超极化率张量的五个不可归约分量(与激光极化和场几何形状无关)的分析结果(按照艾里函数) 。这些结果用于分析双光子分离速率的频率,场几何形状和激光偏振依赖性,以及对单光子分离速率的激光强度校正的线性关系。结果表明,对于共面和正交场几何,都存在γ(F;ω)的实部和虚部两者的频率相关性的振荡行为,并且该行为对于单个频率以下和以上的频率在质量上是不同的-光子脱离阈值。详细分析了两个光子脱离速率的阈值行为,并讨论了静电场对威格纳阈值定律的短程电势修正。

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