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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.

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.

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.

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,

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.

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

30 Sep 2011: CR strain CC124 [12] was grown axenically in tris-acetate-phosphate medium [11] in a growth chamber(Binder, Germany) set to 24 C and a cycle of 16 h lightat 100 ... Nikaido, J. Cell Sci. 109, 57 (1996). [24] M. A. Silverman and M.

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

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

14 Feb 2011: 0.0997679 0.0314839 0 23 0 199.5 15.5 0.155559 -0.167651 0 24 0 207.5 15.5 -0.00544606 -0.227898 0 25 0 215.5 ... 1 199.5 23.5 0.610019 0.125893 0 24 1 207.5 23.5 0.668408 0.386805 0 25 1 215.5 23.5 0.565238 0.810526

10 Apr 2011: This argument is similar in spiritto that posed by Levinthal and Crane [24] in the con-text of DNA transcription. ... Hohenberg, Physica (Amster-dam) 56D, 303 (1992). [24] C. Levinthal and H.

10 Apr 2011: The last term in Eq. 1 describesthe coupling to strain rate tensor E Exy = xvy yvx 21,24.Our further analysis shows that while this term has somequantitative effect, e.g., ... F. Edwards, The Theory of Polymer DynamicsClarendon Press, Oxford, 1988. 24 N.

10 Apr 2011: The electrostatic contribution was first determined by Odijk [24] and independently by Skolnick and Fixman [25] in the Debye- Hiickel approximation. ... 23). (24). H.N.W. Lekkerkerker I Curvature elasticity o f charged monolayers 325.