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Readership: This publication is best suited for the lively scientists and graduates in strong-field group and likewise for different scientists who paintings with the ultrafast lasers in biology and chemistry.
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Extra resources for Advances of Atoms and Molecules in Strong Laser Fields
B) The initial transverse momentum distribution with respect to the tunneling phase of tunneled electrons with consideration of Coulomb potential in the Newtonian equation and without solving the phase equation (CTMC model). (c) The initial transverse momentum distribution with respect to the tunneling phase of tunneled electrons without consideration of Coulomb potential in both the Newtonian and phase equation in QTMC model. (d) The initial transverse momentum distribution with respect to the tunneling phase with consideration of Coulomb effect in both Newtonian and phase equation with QTMC model.
Long, The Raman Effect. A Unified Treatment of the Theory of Raman Scattering by Molecules. (John Wiley Sons, Chichester, 2002). 4. D. Lee and A. C. Albrecht, In eds. J. H. Clark, R and R. E. Hester, Advances in Infrared and Raman Spectroscopy, vol. 12, pp. 179–213, Wiley Heyden, London (1985). 5. S. Mukamel, Principles of Nonlinear Optical Spectroscopy, Oxford University Press, New York (1995). 6. M. F. Kling, S. Zherebtsov, I. Znakovskaya, T. Uphues, G. Sanone, E. Benedetti, F. Ferrari, M. Nisoli, F.
23]. 8F0/ω 0 30 60 tunneling phase (degree) 90 (b) Fig. 5. (a) The final photoelectron momentum pz with respect to the tunneling phase and the scattering angle at the instant of recollision. The final momentum scales with F0/w. Three regions are dissected by the black lines. Region I shows the high-energy photoelectrons with pz < −F0 /ω, Region II shows the photoelectrons with −F0 /ω < pz < 0, and Region III with 0 < pz < F0 /ω, respectively. (b) The photoelectron momentum pz with respect to the tunneling phase with the different transverse momenta px .