By S H Lin
This overview goals to supply an creation to the entire major components of multiphoton experiences up to now. The volume's focus is nearly solely with multiphoton techniques in atoms.
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Extra info for Advances in multi-photon processes and spectroscopy
4, 109 (1979). 34 49. J. A. Armstrong and P. Esherick, in JEPL, op. , p. A. Armstrong, P. J. Wynne, Phys. Rev. A 15_, 180 (1977). 50. W. A. F. Worden, in JEPL, op. , p. 267. 51. F. E. Bjorkholm, Phys. Rev. Lett. 34, 1 (1975). 52. J. Morellec, D. Normand and G. Petite, Phys. Rev. A 1±> 3 0 0 ( 1 9 7 6 h G. Petite, J. Morellec, and D. Normand, J. de Physique, 40, 115 (1979); and the doctoral thesis of G. Petite (University of Paris-South, 1978). 53. H. Eberly, Phys. Rev. Lett. 42, 1049 (1979). 54.
Petite (University of Paris-South, 1978). 53. H. Eberly, Phys. Rev. Lett. 42, 1049 (1979). 54. Y. Gontier and M. Trahin, Phys. Rev. A 1£, 264 (1979). 55. E. Moody and M. Lambropoulos, Phys. Rev. A A5_, 1497 (1977). 56. P. Lambropoulos, Phys. Rev. A 9 , 1992 (1974). This is a notable early development of the resolvent operator perturbative approach to lightinduced shifts and widths of the intermediate resonance in two-photon ionization. Intermediate laser intensity levels (incomplete saturation) and finite laser bandwidth are shown to be within the scope of this approach.
Lett. 39, 269 (1977); and A. M. K. Holmes, and C. Jung, Phys. Rev. A 19, 2371 (1979). 39 Figure Captions Fig. 1 (a) Energy levels and frequencies of the radiation field taking part in a two-photon transition, and (b) same diagram for very closely related Raman effect. Fig. 1 Fig. 2 Experimental setup (a) The flashlamp pulse. (b) The laser pulse. (c) The flashlamp pulse with a dip due to two photon absorption. The position of the dip coincides with the position of the laser pulse. Fig. 1 Fig. , Ref.