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22 Dec 2014: a = 0, b = π, (t [0,π],q(t) = 20 cos(2t)), α1 6= 0, β1 6= 0, α2 = β2 = 0,. ... 2. 20 Alberto Gil C. P. Ramos, Arieh Iserles. B.2 Estimating π(Bλ ,1(ck,t).

30 Jul 2014: Using l = 20 μm, r = 5 μm, and F/8πμ 2 103 μm2/s, we find k > (3 102/α) pNμm. ... The orbits were separated by d = 20 μm and had a radial stiffness with spring con-stant λ.

14 Jun 2014: 7622 • J. Neurosci., August 20, 2003 • 23(20):7621–7629 Sernagor et al. • ... 7626 • J. Neurosci., August 20, 2003 • 23(20):7621–7629 Sernagor et al. •

22 Apr 2014: 20. Similarly to the two-dimensional case and forsimilar geometrical reasons, the surface energy stays constantin the dewetting range (α between 0 and π/2 θE ). 2. Hydrophilic case. In the ... FIG. 20. (Color online) Total surface energy E as a

14 Jul 2014: Φ iscomputed for drops with diameters between 4 20 μm and25 125 μm for dense (area fraction 25%) and semidilutesuspensions (area fraction 10%).Fig. ... Phys Rev Lett 110(22):228102. 20. Aranson IS (2013) The aquatic dance of bacteria.

23 Jul 2014: 20 / 26. Solving linear systems. TheoremLet Binv(l 2(N)) denote the set of bounded invertible operators anddefine the domain = Binv(l 2(N)) l 2(N).

21 Jan 2014: ρ(Dλ,0(ck,ck1)). 2. )20. = O (1). [1 00 1. ]O (1). ... 0 O (1) (2hmax). O (1) (2hmax)1 0. ]. 22. where we have called upon assumptions (1.19)–(1.20) and (A.15).

14 Jun 2014: 7 Exp. 8 Exp. 9 Mean rank Pooled rank. AChR. 1 20 1051 176 4 50 16 10 4496 66 654 2AChR. ... 3, 8, 9, 20, and 24). For theother five, however, in situ hybridization revealed a punctatepattern of expression associated with individual muscle fibers(Fig.

26 Feb 2014: capture of axonemal components in near-physiological states, at molecular-level resolution [20]. ... 20. (iii). (ii). (i). no slips. few slips. many slips. 0 10time (s).

24 Apr 2014: c0(1, ζ)=C0(ζ)c, (3.19)ur0(1, ζ)=0, (3.20). u‖0 =M(ζ)‖C0, (3.21). with M, the mobility coefficient, given by. ... M(ζ)=. 0ρ(. eφ̃0(ρ,ζ) 1). dρ. (3.22). Combining (3.20) and (3.21), we therefore establish that, provided ε2Pe 1, theouter