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28 Mar 2014: Biomim. 9 (2014) 036007 R M Arco et al. 0 10 20 30 40 500. ... J.71 3430. [20] Kim M J and Breuer K S 2008 Microfluidic pump powered byself-organizing bacteria Small 4 111.

28 Nov 2014: du. dt+ Au = 0 , for u(0) X given. (6.20). ... tA)j/j! This semigroup gives the solution to(6.20)in the formu(t) = S(t)u(0),which is continuously differentiable intoX.

14 Oct 2014: an), obtained byintegrating the characteristic ode:. dxjds. = aj ,dz. ds= b(x, z) = cz d , (1.20).

14 Jun 2014: mean diameter from 30 –150 m, and SD 20 – 60 m, both at 10-mintervals). ... 20% of the clos-est neighbors in random simulations up to 20 m.

14 Jun 2014: Stable, multi-platform. (2.14.0 due. 2010-10-31.). • R-core now 20 people, key academics in field, including John Chambers. ... 20 / 1. Naming indexes of a vector. j o e < c ( 2 4 , 1.

1 Apr 2014: 5. Open Questions 20. 1. Introduction and Summary. Among the many AdS string compactifications, there is one which remains enigmatic. ... N = (0, 2) models [17] and N = (2, 2) Landau-Ginzburg theories [18], Liouville theories[19] and non-Abelian gauge

14 Jun 2014: D! Sigmoidalinteraction function from equation 3 with a 2,f 20 µm, d 40 µm! ... 2! with d12 varying from 0 toeither 18 or 20 mm in 1-µm increments.

23 Jul 2014: Example. 0 20 40 60 80 100. 0.9. 1.1. 1.3. Time. ... 40. 50. Computational setting 1. 0.05 0.10 0.15. 0. 20. 40.

9 Nov 2014: 4L. n=1. n2 (A2n B2n). (5.20). Notice in particular that this total energy is independent of time; just like in simple har-.

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.