By et al S. H. Lin (Editor)
Between others, chemistry, physics, biology, and fabric sciences have visible a quick development in either experimental and theoretical reports of multi-photon procedures and spectroscopy of atoms, ions and molecules. This ebook is a vital addition to a complicated sequence that comprises evaluation papers readable not just by way of energetic researchers in those components, but additionally by means of people who find themselves meaning to input the sphere. Written by means of specialists within the sector, the experiences are self-contained to permit readers to know the major thoughts with no a lot practise. This quantity might be priceless to energetic researchers in addition to to scientists in biology, chemistry, fabric sciences, and physics.
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Extra info for Advances In Multi-photon Processes And Spectroscopy
Lett. 93, 183202 (2004). X. M. Tong, Z. X. Zhao, C. D. Lin, Phys. Rev. A 68, 043412 (2003). X. M. Tong, Z. X. Zhao, C. D. Lin, Phys. Rev. Lett. 91, 233203 (2003). G. L. Yudin, M. Y. Ivanov, Phys. Rev. A 64, 035401 (2001). I. html. X. M. Tong, C. D. Lin, Phys. Rev. A 70, 023406 (2004). K. Sandig, H. Figger, T. W. Hansch, Phys. Rev. Lett. 85, 4876 (2000). A. S. , Phys. Rev. A 71, 031403 (2005). ch01 March 2, 1994 9:41 WSPC/SPI-B348: Advances of Multi-Photon Processes and Spectroscopy (AMPS Vol 17) This page intentionally left blank ch02 March 2, 1994 9:41 WSPC/SPI-B348: Advances of Multi-Photon Processes and Spectroscopy (AMPS Vol 17) 2 GENERALIZATION AND APPLICATION TO MOLECULAR SYSTEMS OF KELDYSH’S ATOMIC PHOTOIONIZATION THEORY K.
The time-dependent Schrödinger equation for the electron in the velocity gauge is expressed as i ∂ ψA (r, t) = ∂t 1 −i ∇r − eA(t) 2m 2 + V(r ) ψA (r, t), (4) where m is the mass of the electron, V(r ) the Coulomb potential between the ionizing electron and the remaining atom, which is usually given by V(r ) = −Ze2 /r, (5) and A(t) the vector potential written as A(t) = −(F/ω) sin ωt. (6) If we neglect V(r ), Eq. (4) can be solved easily and ψA (r, t) is given by ψA (r, t) = exp i p·r− 1 2m t dt p − eA(t ) 2 , (7) 0 where p is some ﬁxed momentum of the electron.
A 104, 5660 (2000). 17. H. Niikura, F. Legare, R. Hasbani, A. D. , Nature 417, 917 (2002). 18. H. Niikura, F. Legare, R. Hasbani, M. Y. , Nature 421, 826 (2003). ch01 3rd Reading December 23, 2005 13:10 WSPC/SPI-B348: Advances of Multi-Photon Processes and Spectroscopy (AMPS Vol 17) Probing Orbital Symmetries and Ionization Dynamics 19. 20. 21. 22. 23. 24. 25. 26. 27. 28. 29. 30. 31. 32. 33. 27 T. Zuo, A. D. Bandrauk, Phys. Rev. A 52, R2511 (1995). K. Codling, L. J. Frasinski, P. A. Hatherly, J.