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By B.T. Arnold

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293. : Phys. Lett. : Phys. Rev. Lett. : Phys. Rev. Lett. : Adv. Atomic Molecular Opt. Phys. , van den Heuvell, Muller, H. : Multiphoton Processes. , Knight, P. L. ). Cambridge University Press, Cambridge (1988) Gallagher, T. : Phys. Rev. Lett. 61, 2304 (1988) Corkum, P. , Burnett, N. : Phys. Rev. Lett. : J. : Appl. Phys. B. : Phys. Rev. Lett. : Europhys. Lett. : J. , Chen, S. : Chin. Phys. : J. Phys. , Eberly, J. : J. Opt. Soc. Am. B 7, 564 (1990) Eberly, J. , Kulander, K. : Sci. : Phys. Rev. Lett.

185 PW/cm2 is the threshold intensity separates the tunneling regime and over-the-barrier regime as schematically plotted in Fig. 8. Reprinted with the permission from Ref [29]. Copyright 2007, American Physical Society where E M ≈ I p1 + I p2 is the most probable energy and ρ(E) is the state density around E. u.. With the above initial conditions, the Newtonian equations are solved using the 4-5th step-adaptive Runge-Kutta algorithm and DI events are identified by energy criterion. e. by rate (t0 )) classical trajectories of electron pair are traced and a few thousands or more of DI events are collected for statistics.

7) In practice, the energy is usually not equally allotted to the returned electron and struck electron after recollision. Numerically, we have made statistics on the distribution probability with respect to the asymmetry parameter κ , where the parameters are chosen close to the threshold. It shows that, the distribution function has a broad peak around zero with a long tail and decreases to zero at κ = 1. According to our calculation, the main profile of the distribution function is general while some detailed structures vary with the field parameters and the atomic structure.

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