By David Bates (ed.), Benjamin Bederson (ed.)
This sequence, proven in 1965, addresses fresh advancements within the common zone of atomic, molecular, and optical physics. the sphere is in a country of quick development, as new experimental and theoretical suggestions are delivered to undergo on many aged and new difficulties. Such difficulties diversity from experiences of the basic homes of radiation and subject, via stories of hitherto inaccesible states of "ordinary" and unique atoms and molecules, the keep an eye on of atoms and molecules through mild, the behaviour of atoms and molecules in severe radiation fields, the particular constitution of such structures, together with complicated molecules and molecular clusters, and a variety of interplay phenomena between atoms, molecules, and their constituent components and fields. themes coated additionally comprise similar utilized parts, comparable to atmospheric technological know-how, astrophysics, floor physics, and laser physics.
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Extra info for Advances In Atomic, Molecular, and Optical Physics, Vol. 30
For these transitions, the CC010 results show the best agreement with the experiment. On the other hand, the CCOIO results for the 1 ' S + 2'S, z3P transitions are very poor, generally worse than the CC5 calculation. The essential ingredient of the CCOlO is its optical potential. Brunger et al. 28 Shinobu Nakazaki '6 He l'S-Z3S 1 0 20 C 40 60 i 80 200eV 5 100 120 6 140 ANGLE ( d e g ) FIG. 9. Differential cross sections for the three cases of the target wave function in the 5-state R-matrix calculations for the 1 ' S + 2's transition in He at 200 eV.
8 eV; - .. , 1979); -. , 1990). ExperiTrajmar (1973); ment: V, Crooks et al. (1972); 0,Hall et al. 2 eV; + , Cartwright et al. (1989); 0, Brunger et al. (1990). ~ J v, 0"-140°, because almost all the experiments so far have been done in this region, and a detailed comparison can be made in such a widened figure. , the forward scattering at 200 eV for the 1's + 2's transition). Therefore, the following discussion is concentrated on the mutual comparison of the theoretical results and how well those theoretical results can reproduce the experimental data.
30 Shinobu Nakazaki The DWPO method is a variation of the distorted wave method but partially includes the effect of target polarization. In the original version of the DWPO (Scott and McDowell, 1975, 1976), no distortion is considered in the final channel. The DWPO calculation gives a poor DCS, compared with the experiments, for the transition and incident energy considered. The revised DWPO method by Srivastava et al. (1985, 1989) takes into account the distortion both in the initial and final channels.
Advances In Atomic, Molecular, and Optical Physics, Vol. 30 by David Bates (ed.), Benjamin Bederson (ed.)