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14 Jun 2014: T. Schmidt and M. Buzzard, J. Neurobiol., 1993, 24, 384–399.30 L. ... B. Feller, Neuron, 1999, 24,. 673–685.62 E. Marder and J. M.

23 Jul 2014: Final Example [Feinberg/Zee 1999]. Period 24 Periods 1,. , 24. Simon Chandler-Wilde Spectral Inclusion Sets for Spectra and Pseudospectra. ... Final Example [Feinberg/Zee 1999]. Size 24. Simon Chandler-Wilde Spectral Inclusion Sets for Spectra and

6 Oct 2014: ǫABǫF ′Q′C̃A′B′E′Q′ ǫAB(ǫA′E′ǫ. F ′. B′ ǫF ′. A′ ǫB′E′)R. 24+ ǫA′B′ǫ. ... 24. a,b holomorphic functions on C. For these to agree we require.

30 Aug 2014: t(t v). ], (1.24). where t and n are, respectively, the local tangent and normal vectors along the filament. ... 1.24), up to the unknown translational and rotational velocities,(U,), which will be determined by imposing the overall force-free and

29 Aug 2014: parameter, %. We thuswrite. u(0) = u0 % u% O (%2), (24). p(0) = p0 % p% O (%2), (25). ... û% = 0. (31)The fist boundary condition satisfied by the corrective flow û% is found by Taylor expanding theboundary condition (21) to the first order in %.

9 Sep 2014: For example, it is nowpossible to measure the force required to hold a swimmingspermatozoon [24–26], alga [27] or bacterium [28] in an opticaltrap.

21 Oct 2014: Image Processing for Fluid Dynamics.  Stuart Dalziel. DL Research Partners 1993 – 2001. Version 2.3  DL Research Partners; September 2001 1. Contents Contents.1. 1 Concept.1. 2 DigImage: Particle Tracking.3 2.1 IMAGE CAPTURE. 3 2.2 PARTICLE

19 Jun 2014: 512. 512. Err 6.01%Err 6.01%. 1024. 10. 24. Err 3.60%Err 3.60%. ... 24), yet it is unclear how areal-world setup can be implemented where signals are sparse in atransform domain.

6 Nov 2014: In three dimensions the general solution of (2.24)-(2.25) depends on four arbi-. ... 3.16). 24. Note that R acts on δf without ambiguity (alternatively, the ambiguity in bound-.

6 Oct 2014: components, the possible holonomy groups of these irreducible non–symmetric. Riemannian manifolds have been classified by Berger [24]. ... τ := ξA′(dξA. ′ ξB. ′ΓA. ′B′. ). (2.24). Using τ, we can lift the vector fields ξA′AA′ to F