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7 May 2008: Condensation of Classical Nonlinear Waves in a Two-Component System. Hayder Salman and Natalia G. BerloffDepartment of Applied Mathematics and Theoretical Physics, University of Cambridge, Cambridge, CB3 0WA, UK. Abstract. We study the formation of

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23 Aug 2023: This. isa. spec. ific. indiv. idual’s. copy. of. the. note. s.P. lease. do. not. copy. and/or. redis. trib. ute. Mathematical Tripos: Part III PM. Contents. 0 Perturbation Methods (16 Lectures) i. 0.1 Introduction. i. 1 Algebraic Equations 1. 1.1

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3 Dec 2022: of (at least) visible light, meaning ka 1. For this reason, we can.

19 Nov 2014: 1 / 2 @preserve Copyright (c) 20112014 Humu <humu2009@gmail.com> 3 This file is part of jsc3d project, which is freely distributable under the 4 terms of the MIT license. 5 6 Permission is hereby granted, free of charge, to any person obtaining a

19 Jul 2019: 2=. mM. hm M. p(m M)2 4mM cos2(ka). i. The resulting dispersion relation is sketched in Figure 57 in the first Brillouin zone. ... This is because it is. valid only at long wavelengths, ka 1.

26 Jul 2013: ¤ and compute a matrix F with components fij = cij =( i ¤j ).The minimal-energy stabilizing feedback controller is then given by u = KÀ , whereK = B ¤ F ¡1.

25 Jun 2004: for occupationnumbers n k defined by a ka k8. &' n kd kk8. ... Tothis end we first filter out the high-frequency harmonics byperforming the transformation a ka kmax$12k.