By R. Knapp, G. Papanicolaou, B. White (auth.), Dr. Alan R. Bishop, Dr. David K. Campbell, Dr. Stephanos Pnevmatikos (eds.)
ill the previous 3 many years there was enonnous growth in picking the es sential function that "nonlinearity" performs in actual structures. Classical nonlinear wave equations can help localized, sturdy "soliton" recommendations, and nonlinearities in quantum platforms can result in self-trapped excitations, comparable to polarons. due to the fact those nonlinear excitations frequently dominate the delivery and reaction homes of the platforms within which they exist, actual modeling in their results is vital to reading quite a lot of actual phenomena. extra, the dramatic de velopments in "deterministic chaos", together with the popularity that even basic nonlinear dynamical structures can produce likely random temporal evolution, have equally proven that an realizing of chaotic dynamics is key to a correct interpretation of the habit of many actual platforms. As a conse quence of those advancements, the research of nonlinear phenomena has emerged as a subject matter in its personal correct. in the course of those similar 3 many years, comparable growth has happened in comprehend ing the results of "disorder". prompted by means of Anderson's pioneering paintings on "dis ordered" quantum stable country fabrics, this attempt has additionally grown right into a box that now contains a number of classical and quantum platforms and treats "disorder" coming up from many assets, together with impurities, random spatial constructions, and stochastic utilized fields. considerably, those advancements have happened fairly independently, with particularly little overlapping research.
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Additional resources for Disorder and Nonlinearity: Proceedings of the Workshop J.R. Oppenheimer Study Center Los Alamos, New Mexico, 4–6 May, 1988
Holstein: Phys. Rev. B35, 7474 (1987). 8. F. Delyon, Y. E. Levy, and B. Souilard: Phys. Rev. Lett. 57,2010 (1986). 9. L. Kahn, N. S. Almeida, and D. L. Mills: Phys. Rev. B37, 8072 (1988). 10. T. C. is, C. R. Emmhizer, and R. H. G. l- Time Prediction in Dynamics, ed. by C. W. , L. E. Reichl and V. G. , 1983). 11. Yi Wan and C. M. Soukoulis: to be published. 37 A New Look at Hopping, Trapping and Anderson Localisation P. Phillips 1, K. H. E. Parris 2 IDepartment of Chemistry, Massachusetts Institute of Technology, Cambridge, MA02139, USA 2Department of Physics, University of Missouri, Rolla, M065401, USA Abstract: We review a new set of transformations that provide a direct route to the diffusion constant in the random hopping and trapping models for transport among a random distribution of localised electronic states.
A.  Papanicolaou, G. C. , Vetterling W. , Papanicolaou, G. (1986), "Multiple Scattering Through Localization Length Scales", Phys. Rev. , Papanicolaou, G. (1986), "Minimum Wave Localization Length in a one Dimensional Randoin Medium", Phys. Rev. B 347 p4757-4761  Spigler, Renato (1986), "Mean Power Reflection from a One-dimensional Nonlinear Random Medium", J. Math. Phys. 277 p1760-1771  Spigler, Renato (1985), "Nonlinear Parametric Oscillations in Certain Stochastic Systems: A Random van der Pol Oscillator", J.
Hem. The inner most orbit in Fig. 0139 (d. Eq. (9) and Fig. 4(b». Such orbits are responsible for the part. 45 in Fig. 4( a). ing to the transmission. ed from the unstable period-4 periodic orbits are evident in Fig. 71. , v) plane and are not shown on the plot. es. In fad, such quasi-periodic orbits exist up to the edges of the gaps 011 the IRol2 vs T2 curve, and it. is such orbits that keep the local chaotic orbits from escaping to infinity. In Fig. ion between the IRol2 vs T2 curve. re indicated in Fig.