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12 Jan 2014: the higher resolution obtained and the lower magnetic gradientsrequired to scan along such trajectories [24, 28, 31]. ... Note that our analog modelis the same as that used with great success in recent work of Guerquin-Kern, Haberlin, Pruessmann& Unser

21 Oct 2014: Windows 3.1x 10 3.6 EXAMPLE: Windows 95/98 20 3.7 INSTALLATIONS WITH MORE THAN 12MBYTES OF RAM 24 3.8 Running under Windows 25.

31 May 2014: Weighted Fourier frames, which we also refer to as weighted frames of exponentials, werestudied by Gröchenig [25], and later also by Gabardo [24].

10 Jan 2014: 3.2.2 The freely-jointed chain 24. 3.3 Fluctuating continuous objects 24. 3.3.1 Energy Calculations in Fourier Space 26. ... k =kBT. Nb2. 24 Fluctuations and Fluctuation-Induced Forces. This result is especially interesting because the restoring

8 Mar 2014: Linear Stable Sampling Rate: Optimality of 2D WaveletReconstructions from Fourier Measurements. Ben Adcock, Anders C. Hansen, Gitta Kutyniok, and Jackie Ma. March 1, 2014. AbstractIn this paper we analyze two-dimensional wavelet reconstructions from

27 Aug 2014: DAMTP 2014/NA02. On fast trust region methods for quadratic models. with linear constraints. M.J.D. Powell. Abstract: Quadratic models Qk(x), x Rn, of the objective function F(x),xRn, are used by many successful iterative algorithms for minimization,

28 Nov 2014: 24], but we note that these were all held constant in eachnanofluidic device used in our experiments.

9 May 2014: Cop. yrig. ht. 201. 4 U. nive. rsity. of C. ambr. idge. Not. to b. e qu. oted. or. repr. oduc. ed w. ithou. t per. mis. sion. Partial Differential Equations. David Stuartdmas2@cam.ac.uk. Books. In addition to the sets of lecture notes written by

14 Jun 2014: 22. 2.8.3 Activity blockade experiments. 23. 2.8.4 Retinotopic map formation. 24.

14 Jun 2014: Thanks to Kevin Rodgers for contributing code.). Changes/New Features in 5.1.24:. •

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 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.

9 Dec 2014: Generated using V3.2 of the official AMS LATEX template–journal page layout FOR AUTHOR USE ONLY, NOT FOR SUBMISSION! Jupiter’s unearthly jets: a new turbulent model exhibiting. statistical steadiness without large-scale dissipation. Stephen I.

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

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

22 Jan 2014: Received 8 April 2013; revised 24 September 2013; accepted 7 October 2013;first published online 25 November 2013).

21 Oct 2014: πFn(θ φ) dφ = f(θ) , (1.24). – 8 –. using property ii) of the Fejér kernel.

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.

28 Nov 2014: Pg ρ0. r<. wb dV (24). and thus we obtain the scaling relation. ... ρ0a4. )a3 = D. 24. μa7, (53). where we have substituted κ/N 2 = 4/ν.

13 Jul 2014: Arakawa’s method is used for evaluation of thePoisson bracket.24 The time stepping algorithm is the third.