By Peter Lambropoulos, S. J. Smith (auth.), Professor Peter Lambropoulos Ph.D., Professor Stephen J. Smith Ph.D. (eds.)

The chapters of this quantity signify the invited papers brought on the third foreign convention on Multiphoton tactics (ICOMP III) held in Iraklion, Crete, Greece, September 5-11, 1984. The invited papers at a convention like ICOMP can't almost certainly conceal the total box which has grown to colossal proportions in recent times, overlapping with such diversified parts as atomic and molecular spectroscopy, plasma physics, nonlinear optics, quantum optics, and so on. We think those contributions signify that a part of the examine task which has been attracting the main curiosity some time past 12 months or so, in addition to reports of a few of the extra proven issues. Even inside this scope, and given the confines imposed through the fi­ nite period of a convention, vital and well timed issues are necessarily passed over. yet then, there'll be ICOMP IV. the gathering of articles during this quantity, mixed with vast ref­ erences to comparable paintings given through the authors, may still offer an introduc­ tion to the key difficulties of the sector and its cutting-edge. The chapters were prepared in accordance with thematic proximity, starting with atoms, and carrying on with on with molecules and surfaces. This classi­ fication, although, wouldn't disguise the entire material even in the restricted scope of the convention and of this volume.

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Extra info for Multiphoton Processes: Proceedings of the 3rd International Conference, Iraklion, Crete, Greece September 5–12, 1984

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A physical description of what is gdillg on may be obtained from considerations of second-order perturbation theory. In two-photon excitations, the "time" that a system spends in a real intermediate state is proportional to 1/ Aw, where Aw is the detuning from the state. Now, the readjustment time of a Rydberg wave function due to a change in the potential is given by the inverse of the energy-spacing between adjacent levels; this time is 3xlO-16n 3 • Thus, for far enough detuning from the relevant intermediate states, the transition will appear "sudden" to the Rydberg electron.

The customary procedures based on a single electron model do not produce a sufficient coupling strength, as described earlier [1,2J. The tunneling model, such as that developed by KELDYSH [22], is found to give neither the correct dependence on intensity nor the observed relationship on atomic number. 53 ~m, and 193 nm. The data strongly indicate that a collective response of an entire shell, or a major fraction thereof, is directly involved 34 in the nonlinear coupling. Collective responses of atomic shells, as noted above, have been discussed in relation to the mechanism of single photon photoionization.

Lompre, G. Mainfray, and C. Manus: Phys. Rev. A~, 2503 (1983) 6. H. Egger, T. S. Luk, K. Boyer, D. F. Muller, H. Purnmer, T. Srinivasan, and C. K. Rhodes: Appl. Phys. Lett. 41, 1032 (1982) 7. W. C. Wiley and I. H. McLaren: Rev. Sci. Instr. 26, 1150 (1955) 8. H. Egger, T. S. Luk, W. ~1iiller, H. Purnrner, and C. K. Rhodes: Collision-free multiple ionization of atoms and XUV stimulated in krypton at 193 nm~ AlP Conference Proceedings, Laser Techniques in the Extreme Ultraviolet, Boulder, Colorado, 5-7 March 1984 (to be published); H.

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