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10 Apr 2011: V R! 26aa0. 5. R6. 24! Expressing this result in terms of the electric polarizabilvia. ... Thus the van deWaals potential assumes the form. V R! 24.

10 Apr 2011: Bt/JI= M , (24) t/JI Bt/J t/J(Mn). and a further differentiation then gives. ... 4. Clearly, a steepest-descent approximation should be valid for that part of the distribution near the region of the mini-mum at n 'Z 24.

5 Aug 2011: N2 ratio of the atmosphere [24]. ... Science 309, 1714–1717. (doi:10.1126/science.1115193). 24 Manning, A. C. & Keeling, R.

6 Oct 2011: 1 7 X 102 1.60 2. 2 5 2.92 3.24 3.59 9. ... 6 2 X 1 0 -1 1.10 1.24 1. 3 7 X 1 0 1 3.

2 Nov 2011: Generalized sampling and infinite-dimensionalcompressed sensing. Ben AdcockDepartment of Mathematics. Simon Fraser UniversityBurnaby, BC V5A 1S6. Canada. Anders C. HansenDAMTP, Centre for Mathematical Sciences. University of CambridgeWilberforce Rd,

3 Dec 2011: Generalized Sampling: Extension to Frames and Inverse andIll-Posed Problems. Ben Adcock Anders C. Hansen † Evelyn Herrholz ‡ Gerd Teschke‡. Abstract. Generalized sampling is new framework for sampling and reconstruction in

10 Apr 2011: a. Dd!1/2. h F pln 0.56/h!G1/2. 3.24! B. Energy of a straight-lamina model. ... detail elsewhere in the context of clorelated models,22–24,26,27,30we do not repeat them here.

10 Apr 2011: 2 Ok5k1. 0ka!0# kk4. e2k4t (24). Evaluating the first few integrals, we find forh# k, h# k1. ... A 5zL4. tk1. 24 (54). whereas the rodlike treatment implies (from Eq.

13 Apr 2011: DAMTP 2010/NA04. Beyond symmetric Broyden for updating quadratic. models in minimization without derivatives. M.J.D. Powell. Abstract: Some highly successful algorithms for unconstrained minimizationwithout derivatives construct changes to the

10 Apr 2011: PHYSICS OF FLUIDS 17, 083101 2005. Stalactite growth as a free-boundary problemMartin B. ShortDepartment of Physics, University of Arizona, Tucson, Arizona 85721. James C. BaygentsDepartment of Chemical and Environmental Engineering and Program in

10 Apr 2011: Tanalysis involves the merging of two previously independideas from dynamical systems theory: The couplingslaved small spatial scales to low-mode dynamics as inreduction of dissipative PDEs to inertial manifolds,24 and ... 24! Again, for B. 1, this

13 Aug 2011: 24. We need to identify the above two frequencies on the left-hand side.

10 Apr 2011: J. Fluid Mech. (2010), vol. 647, pp. 287–308. c Cambridge University Press 2010doi:10.1017/S0022112009993910. 287. On the mechanisms of icicle evolution. JEROME A. NEUFELD†, RAYMOND E. GOLDSTEINAND M. GRAE WORSTER. Institute of Theoretical

10 Apr 2011: Therefore, we expect the MSC to describe fronpropagation at smalla if it applies at all [24]. ... 23] H. Lamb, Hydrodynamics(Cambridge University Press,Cambridge, England, 1993), 6th ed. [24] Preliminary numerical studies by D.

1 Sep 2011: 2.24) is attained by ω(k)n. It seems to be so if k >. m1m22 (when it looks that. ‖ω(k)n ‖ = ω(k)n (1)). Theorem 2.12 (Shadrin ... 24 Twelve Proofs of the Markov Inequality. The proof we are going now to present is, in fact, not that of Bernstein

22 Nov 2011: The problem is not new, and therehave been many different approaches developed for its solution (see, for example, [2, 11, 12, 17, 18, 22,23, 24, 25, 52] and references therein).

20 Jun 2011: 1B), where η is the viscosity, and the distance betweenthe forces (24, 25). ... sions. Chem Phys 375:557–567.24. Batchelor GK (1970) The stress system in a suspension of force-free particles.

10 Apr 2011: arises from a thermal average over the noncritical 24 orientational degrees of freedom.

10 Apr 2011: 1993, 97. 9532. (24) de Koker, R.: McConnell, H. M. J.

10 Apr 2011: SI=II-KI() • (24) With these results we can study some of the aspects. ... 24). Clearly, the orientational entropy is just the difference. In Fig.