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23 Sep 2015: along the anterior (kA = 1000 μm, hA0 = 0:8) and strongly along the posterior-lateral cortex (kP = 150 μm, hP0 = 0, see ‘Materials and methods’ MT nucleation. ... the inset of panel C (yellow circles). In all panels, parameter values for anterior

17 Jul 2024: KA Bacik, S Lovett, C-CP Caulfield, NM Vriend. – Physical review letters.

17 Jul 2024: MR Bate, SH Lubow, GI Ogilvie, KA Miller. (2003). (doi: 10.48550/arxiv.astro-ph/0301154).

7 Apr 2021: structure. E = C cos(ka). Then the velocity in a constant electric field oscillates as. ... v(k) =Ca. sin(ka) = Ca. sineEa. t. The Bloch frequency is! =

17 Jul 2024: XC Vidal, M D'Onofrio, PJ Fox, R Torre, KA Ulmer, A Aboubrahim, A Albert, J Alimena, BC Allanach, C Alpigiani, M Altakach, S Amoroso, JK Anders, JY Araz, A Arbey,

16 Jul 2019: eLife 7:e40018. DOI: https://doi.org/10.7554/eLife.40018,PMID: 30033910. Guasto JS, Johnson KA, Gollub JP. ... 2009. The Chlamydomonas Sourcebook. 2nd edition. London: Academic Press.Hinchliff CE, Smith SA, Allman JF, Burleigh JG, Chaudhary R, Coghill LM,

14 Aug 2013: Let K = Ka/xa, a = 0,. , 3 be a vector field generating a one-parameter group oftransformations of M with orbits Γ.

6 Jul 2011: 38. Guasto JS, Johnson KA, Gollub JP (2010) Oscillatory flows induced by microorganismsswimming in two dimensions.

31 Dec 2018: and, for small ka, the sin function is approximately linear. This means that we get.

14 Jul 2014: flow field around swimming microorganisms. Phys Rev Lett 105(16):168101.23. Guasto JS, Johnson KA, Gollub JP (2010) Oscillatory flows induced by microorganisms.

19 Oct 2013: iσζ̂ kA sinh kh = 0. and from the second (pressure) (). gζ̂ iσA cosh kh = 0. Regarding these as a system of two linear algebraic equations for the two unknown constants ζ̂

17 Apr 2007: It therefore followsfrom (22) that Xa, Xa, Ya Y a are gradients and that Ka = Ya Y a is a Killing vector.

19 Oct 2013: J<6{4)01# "9#mI =9? : : "9#r=:; DJzG=x? 0- I?6,z#1 Kj BKj'Kä :6#(8º Jz0 G= 8G? ... 6'? ] BKj0G=>=# Kj Km'Kä :#I =º? :;81#G5#6: º#=>c0- "GG "(8º J= G= 0G=º# Km Kj'EKà :#c X8Ñ?

1 Feb 2008: Aé13<K3è-1 ->EN31ZEF>"3517ð"65:C3EF<@>kA<@ê|:CEF>. S 0 ù ûèé-;Vü35è1zî@1VDN<ì4EN3õþ<Cç3è1î"<@6317òEG;><@3K35è19;éê

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

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 _!

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.

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