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

25 Jul 2014: e. it is orthogonal to ahyper-surface) as. Ka b Kc = BCιB′ιC ′ιA′αA B′C ′αAαBαCιA′and ((K d K))a = a bcd Kbc Kd = 0 as abcd involves

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

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.

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

27 Apr 2024: Lent Term, 2015. ElectromagnetismUniversity of Cambridge Mathematical Tripos. David Tong. Department of Applied Mathematics and Theoretical Physics,. Centre for Mathematical Sciences,. Wilberforce Road,. Cambridge, CB3 OBA, UK.

8 Jul 2009: This should be compared withLube et al.’s (2005) results who found for a > 1.15 a similar dependence with a:h/r0 = ka.

30 Nov 2015: From (8.43) we have that. F1[sin ka] = i2(δ(x a) δ(x a)) (10.32).