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

18 Mar 2008: nullgeodesics. In spinors, if Ka D AoA0 then an ˛-plane distribution is defined by oA0 ,and a ˇ-plane distribution by A, and it follows from the Killing equation that

8 Apr 2008: Plugging. into the equation we find c = kaa0kbka. for kb 6= ka.

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

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

30 Sep 2008: ii) χ(a) = 0 A sin(ka) = 0 ka = nπ where n = 1, 2,. ... Imposing continuity of χ(x) at x = a gives,. A cos(ka) = D exp(κa) (35).

3 Oct 2008: Natural Sciences Tripos, Part IB. Michaelmas Term 2008. Mathematical Methods I. Dr Gordon Ogilvie. Schedule. Vector calculus. Suffix notation. Contractions using δij and ǫijk. Re-minder of vector products, grad, div, curl, 2 and their

17 Nov 2008: The answer is. G = dt2. ka 3 a3 c+. a da2(ka 3 a3 c. ... L = a3. 4L(Z) 3. 8π G(a(ȧ)2 ka), where Z = ψ̇ 2 (4.4).