Stimulated Raman scattering of an ultrashort XUV radiation pulse by a hydrogen atom

被引:7
|
作者
Dondera, Mihai [1 ,2 ]
Florescu, Viorica [1 ,2 ]
Bachau, Henri [3 ]
机构
[1] Univ Bucharest, Dept Phys, MG-11, Bucharest 077125, Romania
[2] Univ Bucharest, Ctr Adv Quantum Phys, MG-11, Bucharest 077125, Romania
[3] Univ Bordeaux, CEA, CNRS, Ctr Lasers Intenses & Applicat, F-33405 Talence, France
关键词
FREE-ELECTRON LASER; TRANSITIONS; OPERATION;
D O I
10.1103/PhysRevA.95.023417
中图分类号
O43 [光学];
学科分类号
070207 ; 0803 ;
摘要
We consider the hydrogen atom H(1s) exposed to an ultrashort laser pulse with a central frequency ?0 ranging from several hundreds of eV to 1.5 keV (approximate to 55 a.u.) and a peak intensity of 3.51x10(16)W/cm(2). We study the excitation of the atom by stimulated Raman scattering, a process involving pairs of frequencies (omega(1),omega(2)). These frequencies are non-negligible components of the pulse Fourier transform and they satisfy the condition E-g+h omega(1)=Eb+h omega(2), E-g and E-b equivalent to E-n being the ground-state and the excited-state energy, respectively. The numerical results obtained by integrating the time-dependent Schrodinger equation (TDSE) are compared with calculations in lowest order perturbation theory (LOPT). In LOPT we consider, in the second order of PT, the contribution of the term A center dot P in the dipole approximation and, in first order of PT, the expression of A(2) taken for first-order retardation effects. (A denotes the vector potential of the field and P is the momentum operator.) We focus on the Raman excitation of bound states with principal quantum numbers n up to n=13. The evaluation in perturbation theory of the A center dot P contribution to 1s-ns and 1s-nd transition probabilities uses analytic expressions of the corresponding KramersHeisenberg matrix elements. At fixed pulse duration tau=6 pi a.u. (approximate to 0.48 fs), we find that the retardation effects play an important role at high frequencies: they progressively diminish as the frequency decreases until the contribution of A center dot P dominates over the A(2) contribution for omega(0) values of a few a.u. We also study the dependence of the Raman process on the pulse duration for several values of omega(0). In the case omega(0)=13a.u.(approximate to 354eV) where dipole and nondipole contributions are of the same order of magnitude, we present the Raman excitation probability as a function of the pulse duration for excited ns, np, and nd states.
引用
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页数:8
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