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

5 Sep 2007: Anal. Priloz. 21,. 81–82 1987.24 Ovsienko, V. and Rogers, C., “Deforming the Lie algebra of vector fields on S1 inside the Poisson algebra on ṪS1,”.

25 Jan 2007: Geodesic Deviation (23). Eij = j gi. Tidal Tensor (24). Now the gravitational field is conservative, curl g = 0, and so we may introducethe Newtonian Potential by. ... 24. Cop. yrig. ht. 200. 6 U. nive. rsity. of C.

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.

19 Oct 2007: subtraction,r = 1, with 12, 24, 48 and 96 terms respectively. ... 24. Huybrechs, D. & Vandewalle, S. (2006), ‘On the evaluation ofhighly oscillatory integrals byanalytic continuation’,SIAM J.

27 Jul 2007: Digital Object Identifier (DOI) 10.1007/s00220-007-0208-4Commun. Math. Phys. 272, 85–118 (2007) Communications in. MathematicalPhysics. Anti-self-dual Conformal Structures with Null KillingVectors from Projective Structures. Maciej Dunajski, Simon

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.

2 Nov 2007: "# $%& '&(),#-.(/ 0&&1&. 243563798:3<;>=?A@CBD7FEG. HJICKMLONCPRQOLSUT#VXWJYJZ[]_]_Facb dMefWhgi]jDbkbCW1limCend_bk[oefoXpqb d_]rq[DpXb sCtendbk[oO]efZW#mX]_Wpud_[W1vkmXt1bkpCendWwpXb

6 Nov 2007: A =. kT log 2 1β. log[. 1 β2(qJM h)2/2 β4(qJM h)4/24. ]. ... hA1/24. |A2|3/2. A4 is not particularly interesting: the denominator |A2| is the interesting part.

21 Jun 2007: The Mathematical Institute, 24{29 St Giles’, Oxford OX1 3LB, UK(dunajski@maths.ox.ac.uk). Received 4 June 2001; accepted 21 September 2001; published online 28 March 2002.