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28 May 2014: 1, 20, 25]). We shall assume that n = 5 and P λ has exactly one Casimir function C λ for each λ. ... Central European J. Math 10 (2012), 1872–. 1888.[20] F. MAGRI. A simple model of the integrable Hamiltonian equation.

25 Jul 2014: ψ1 0 w3 0. (3.20). and the determinant is a sum of two non-negative numbers. ... Therefore all 3 by 3 minors of the4 by 20 matrix (R, DR) have to vanish.

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.

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: 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.