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16 Jul 2012: 24 P. Bader, A. Iserles, K. Kropielnicka & P. Singh. of accuracy exhibited in Figs 4.3–4 is clearly in excess of O(ε7/2. ),

10 May 2012: 24. 2.2 Inverse scattering transform for KdV. 252.2.1 Direct scattering. 272.2.2 Properties of the scattering data. ... dx. 24. Figure 2.1: Sine–Gordon Kink. Kink. x. Note that the Sine–Gordon equations didn’t enter the discussion at this stage.

5 Sep 2012: 7.1. A new scheme of Dirichlet series for particular systems of the form(24). ... Byletting z = P 1y, the system (24) is equivalent to a transformed dynamical system.

3 Oct 2012: Chem. Phys. 81, 6320 1984. 24 E. Allahyarov, H. Lowen, and S.

2 Sep 2012: and, by equation (24) and the integral (21),. dO _f12. d z (0)= (27). ... terms in equation (23) and the oxygen consumption term in equation (24) are zero.

27 Aug 2012: For example, it is nowpossible to measure the force required to hold a swimmingspermatozoon [24–26], alga [27] or bacterium [28] in an opticaltrap.

8 Mar 2012: 23. 4.1.3 The optical theorem. 24. 4.1.4 Solving for the asymptotic scattered wave. ... 4 QUANTUM SCATTERING IN 3D 24. where δl is a function of k.

15 Oct 2012: Aspects of fermions in magnetic AdS geometries. have been previously discussed in [20, 21, 22, 23, 24].

2 Sep 2012: 2 3 ) pDV-D'@iF28@ = 0, (2.24). D(D = 0, x = - 1 , o. ( ... To see how these expansions proceed, we first note that (2.24) may be integrated, using (2.25), to dbtain 0 so CDdS(76Z2)/ -1 V d Z = 0.

2 Sep 2012: NUTRIENT UPTAKE BY A SELF-PROPELLED STEADYSQUIRMER. by VANESA MAGAR†. (Department of Applied Mathematics and Theoretical Physics, University of Cambridge,Silver Street, Cambridge CB3 9EW). TOMONOBU GOTO. (Department of Mechanical Engineering,