Advances in Chemical Physics, Vol. 83 by I. Prigogine, Stuart A. Rice

By I. Prigogine, Stuart A. Rice

Every one quantity during this sequence is dedicated to assisting the reader to procure basic information regarding numerous issues in chemical physics. This quantity comprises dialogue of high-temperature superconductors, time-resolved optical exams of digital geometric section improvement and masses extra.

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Boya, and B. Kendrick, Phys. Rev. A 43, 1206 (1991). 7. N. F. Scherer, A. J. Ruggiero, M. Du, and G. R. Fleming, J . Chem. Phys. 93, 856 ( 1990). 8. (a) N. F. Scherer, R. J . Carlson, A. Matro, M. Du, A. J. Ruggiero, V. Romero-Rochin, J. A. Cina, G. R. Fleming, and S. A. Rice, J . Chem. Phys. 95, 1487 (1991); (b) N. F. Scherer, A. Matro, R. J. Carlson, M. Du. L. D. Ziegler, J. A. Cina, and G. R. Fleming, J . Chem. Phys. 196, 4180 (1992). 9. ( a ) H . Metiu and V. Engel, J . O p t . SOC. Am. B7, 1709 (1990); (b) V.

Phys. 57, 59 (1984). I . B. Bersuker and V. Z. Polinger, in Advances in Quantum Chemistry, vol. -0. ) (Academic Press, New York, 1982), p. 85. (a) E. J. Heller, J . Chem. Phys. 68, 2066 (1978); (b) Acc. Chem. , 14. 368 (1981). 7) for the dipole matrix elements differs by a factor of f from that used in refs. 25, 30 and 43. (a) R. Heather and H. Metiu, Chern. Phys. Lett. 118, 558 (1985); (b) J . Chem. Phys. 84, 3250 (1986). R. D. Coalson and M. Karplus, J . Chem. Phys. 93, 3919 (1990). R. G. Littlejohn, Phys.

Energy is exchanged between light and matter in a manner that survives cycle-averaging. On the other hand, in passive processes, the interactions are not always in quadrature form. Furthermore, coherence in the material response and the phase (or momentum) matching condition for the radiation fields are essential. In pure passive processes, those without any resonance, the energy exchanged between light and matter does not survive cycle-averaging and matter serves only catalytically to alter the nature of the radiation.

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