By et al S. H. Lin (Editor)
Between others, chemistry, physics, biology, and fabric sciences have noticeable a swift development in either experimental and theoretical reviews of multi-photon tactics and spectroscopy of atoms, ions and molecules. This publication is a crucial addition to a sophisticated sequence that comprises evaluate papers readable not just via lively researchers in those components, but in addition via those people who are desiring to input the sphere. Written via specialists within the zone, the reports are self-contained to permit readers to understand the major innovations with out a lot instruction. This quantity could be precious to lively researchers in addition to to scientists in biology, chemistry, fabric sciences, and physics.
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Extra resources for Advances In Multi-photon Processes And Spectroscopy
14. M. W. Schmidt, K. K. Baldridge, J. A. Boatz, S. T. , J. Comput. Chem. 14, 1347 (1993). 15. S. Portmann, H. P. Lüthi, CHIMIA 54, 766 (2000). 16. A. H. Zewail, J. Phys. Chem. 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.
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.
A remarkable advantage of our method is that the singular point of the integrand and the zero point of j (u) do not necessarily have to coincide in Eq. 21,22 The quantity L(p ) can be written as √ i 4 ωI0 πa L(p ) = j(us ) , exp (64) 2 ω eF cos θpF 1 − us where cos θpF is deﬁned by F· p+ eF us ω =F p+ eF us cos θpF . ω (65) Notice that at this point, our expression for L(p ) [Eq. (64)] is larger than that of Keldysh [Eq. (58)] by a factor of two, which arises from the contour ch02 March 2, 1994 9:41 WSPC/SPI-B348: Advances of Multi-Photon Processes and Spectroscopy (AMPS Vol 17) 46 K.