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12 Aug 2016: G?Gh3j|kA:?lH7aPG IP q 2! 6! > ,I, G G)?%c e %3:S&&$J0 )' ,-/./0 %3$H&( )4 5/./0 %dlH&=<>) )@ /B/.2?87%URF&=<>) )@ u/./ &2)5 )! ) ;!V @v _!

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).

8 Jul 2021: RESEARCH ARTICLE. The bank of swimming organisms at the. micron scale (BOSO-Micro). Marcos F. Velho Rodrigues1, Maciej LisickiID2, Eric Lauga1. 1 Department of Applied Mathematics and Theoretical Physics, University of Cambridge, Cambridge, United.

13 Mar 2019: δ(r a). Show that the phase shifts are given by. tan δl = kλa2[jl(ka)]. ... 2. 1 kλa2jl(ka)nl(ka). [Hint: The δ-function leads to two continuity conditions at r = a.

2 Sep 2012: detail, including a fluctuation-rounded stretch-coil transition of actin filaments. DOI: 10.1103/PhysRevLett.108.038103 PACS numbers: 87.16.Ka, 47.63.b, 83.50.Jf, 87.15.H.

19 Oct 2013: ó ö ëLë BnF í öJLFLö-K ëlê D[F é KÁ@ òóí ø ê @pöFWK5î ð ø¥FWJö5ñ ê¥ò ø¥KpF ý ñ êÒëLê û#ø¥K¿ö-Dî ê Dù0JöJK5î[Jö-î ... ïí K5î ê F ê¥ò D ë F é öF@ ò D ú J ó K5îF é KÄ@pö ð ë K ëÁò ùbF é K

13 Dec 2018: These microwave frequencies are typically in the C, S, X, Ka, or Ku bands (frequencies above about 1000 MHz).

1 Jul 2024: R Hložek, AI Malz, KA Ponder, M Dai, G Narayan, EEO Ishida, TA AllamJr, A Bahmanyar, X Bi, R Biswas, K Boone, S Chen, N Du, A Erdem, L Galbany, A

1 Jul 2024: 17+. MC Witthoeft, NR Badnell, G Del Zanna, KA Berrington, JC Pelan. –

31 Jul 2008: On modified asymptotic series involving confluent. hypergeometric functions. Alfredo DeañoDAMTP, Centre for Mathematical Sciences,. University of Cambridge,Wilberforce Road, CB3 0WA, UK. Nico M. TemmeCWI, P.O. Box 94079, 1090 GB Amsterdam, The

3 Feb 2013: Phys Rev Lett 105(16):168101. 17. Guasto JS, Johnson KA, Gollub JP (2010) Oscillatory flows induced by microorganismsswimming in two dimensions.

25 Jan 2007: N M Mt 2ik2[σ3, M ] kA(x, t)M B(x, t)M. (4.3.13).