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5 Dec 2007: Conditions in the outer flow, including the boundary conditions, can be chosen in a special way (Warn & Warn 1978, 56; (2.24) below) such that the changes induced in the outer ... 2.24) jl,n being the nth zero of the Bessel function J1.

25 Jan 2007: mis. sion. P.H.Haynes Mathematics IA Algebra and Geometry Michaelmas Term 2002 24.

5 Feb 2007: L. Jaffe, Phys. Today 48N9, 24 (1995). [15] D. B. Renner et al.

16 Feb 2007: uthor for correspondence (m.dunajski@damtp.cam.ac.uk). eived 13 June 2006epted 24 November 2006 945 This journal is q 2007 The Royal Society.

19 Oct 2007: dxδ(x) = 1 (1.24). The Fourier transform of the delta-function provides a useful representation that we.

25 Jan 2007: ithou. t per. mis. sion. where D = 0E; H = 10B: (24)The latter vectors are used to describe non-trivial electrical and magnetic properties ofmedia for which and are callled permittivity ... We might ask: can we obtain an understanding of the elementary

27 Nov 2007: Instead, one uses a space oftempered distributions). 24. Example 6.1.2 H = L2(Rn) (where n = 1, 2, 3 are important cases) is a space of complex-valued functions such ... Ĥ =. 3j=1 P̂. 2j. 2m+ V (X̂j) =. 2. 2m2 V (xj) (6.24).

19 Nov 2007: Logarithmic approach to long-time:. value depends on initial condition. Pipemix - Nottingham 2007 – p.24/25.

17 Apr 2007: IOP PUBLISHING CLASSICAL AND QUANTUM GRAVITY. Class. Quantum Grav. 24 (2007) 1841–1862 doi:10.1088/0264-9381/24/7/010. ... An early example of this technique in gravityis the slow motion of Majumdar–Papepetrou black holes [24].

19 Jun 2007: d4x Tr (δAµ δAµ) = 2Sinst ρ2 (1.24). Note that, unlike the others, this component of the metric depends on the collective. ... theory [22, 23, 24]. We’ll do things the simple way. The brane construction is another place.