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31 Jul 2009: www.sciencemag.org SCIENCE VOL 325 24 JULY 2009 489. REPORTS. on. July. ... 24 JULY 2009 VOL 325 SCIENCE www.sciencemag.org490. REPORTS. on. July. 24,.

27 Jul 2009: 4.25)We now consider the reduction of the system (4.23),(4.24). Theorem 1.1 arises as acorollary of Proposition 4.2. ... to a coupled system whichincludes the Z3 two dimensional Toda chain [24] as a special case.

17 Sep 2009: It has been developed over the last30 years by the Oxford school of Penrose and Atiyah with the crucial early input from Ward[24, 25] and Hitchin [10, 11] and further ... Sächs. Akad. Wiss. Leipzig, Maths. Nat. Kl 69 262–77[24] Ward R S 1977 On

15 Oct 2009: Theorem 8 ([24]) If the nonlinearity satisfies the conditions given in 1.3.2 then (POS) is true. ... 24). The stabilityis in the same sense as in the previous theorem, see [17] for full details.

13 Jul 2009: Lipscombe, R. Kennings and M.M. Denn, J. Non-Newtonian Fluid Mech., 24 (1987) 85 [l]). ... References. 1 G.G. Lipscomb, R. Keunings and M.M. Denn, J. Non-Newtonian Fluid Mech., 24 (1987) 85-96.

30 Aug 2009: 2007) 24–26% 40%(Ridgwell and Hargreaves 2007) 34%(Montenegro et al. 2007) 52%. ... Ambio 24(6):376–378Torn MS, Harte J (2006) Missing feedbacks, asymmetric uncertainties, and the underestimation of future.

24 Feb 2009: µe = 0.47 for centre of massIC 2009, runout – p.24/59.

26 Apr 2009: 24) D. Bruss, N.Datta, A. Ekert, L.C. Kwek and C. Macchiavello, Multipartite entangle-.

10 Jul 2009: The displacements xn as a function of position along theline, n, at different times t = 13.5, 24.5, 35.2, and 45.7. ... The different symbols are different times: , t = 13.5; , t = 24.5; , t = 35.2; ,t = 45.7.

23 Jul 2009: The differential equation can be integrated directly taking Po = 24 to produce an implicit expression for the shape. ... z = 0s-1 F 24( 1 - F2). which when substituted in the volume constraint yields.