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22 Jul 2014: 05/12/2012 Cambridge sub-region 2030 visioning - energy p.11. 0 5,000 10,000 15,000 20,000.

28 Nov 2014: 2 4 6 0 20 40 60 80. 2. 1. Number of coefficients. ... 0.888. 0.887. 0.8872 4 6 0 20 40 60 80. 101.

23 Jun 2014: 10. 20. x. curv. atur. e. 3 2 1 0 1 2 32. ... Lauga, Phys. Rev. Lett. 106, 058103(2011). [20] S. E. Spagnolie and E.

3 Dec 2014: These results are consistent with the asymptotic study of Vélez-Cordero &. The bearable gooeyness of swimming 3. xy. 20 mm. Tracerparticles. (a) (b) (c) (d).

8 Mar 2014: At this stage we note that other higher dimensional concepts, such as curvelets and shearlets, can providebetter approximations rates for cartoon-like-images; a specific class of functions ([10], [20]).

22 Jul 2014: Efficacy. 61. 18. 20. Analysis based on Peterborough’s 518 output areas.

22 Jul 2014: RSA Cambridge GroupMeeting at ideaSpace: 10 February 2011. What will be the developments in technology in the next 20 years that will most change our lives? •

22 Jul 2014: We have an increasing population yet we grow only 60% of our own food (and discard 20%).

21 Oct 2014: New York, NY 10017, USA. -2.0 0.0 2.0 4.0 6.0 8.0 10.0 12.0 14.0 16.0 18.0 20.0 22.0

14 Jun 2014: a) (b). 0.1. 0.2. 0.3. 0 20 40 60 80 100. ... B (1999). 0. 20. 40. 60. 800 10 20 30 40 50 50.

31 May 2014: 8, 37],(ii) polar sampling scheme used in computed tomography [20], (iii) spiral and (iv) interleaving spiralused in MRI [16].

23 Jul 2014: x. y. 25 20 15 10 5 0 5 10 15 20 2525. ... 20. 15. 10. 5. 0. 5. 10. 15. 20. 25Spurious wave reflected by Dirichlet boundary.

14 Jun 2014: new info sub-directory. Chapter 1: Introduction to ESS 13. Changes/New Features in 5.1.20:. •

22 Jul 2014: 0. 50,000. 100,000. 150,000. 200,000. 250,000. 300,000. 350,000. 400,000. 2011 2015 2021 2025 2031. POPULATION. JOBS. DWELLINGS PROBABLE. GOVT 2008. DWELLINGS POSSIBLE. Cambridge 2030. City Region Combined Growth 2011-2031. Actual increases from

19 Nov 2014: Documentation generated by JsDoc Toolkit 2.1.0 on Thu Nov 20 2014 00:20:57 GMT0800 (CST).

28 Nov 2014: 164.4. Two-pit occupancy. 184.5. Arbitrary multiple-pit occupancy. 20. 5. Discussion 216. ... 11. 0. 5. 10. 15. 20. 25. 30. 35. 0 50 100 150 200.

13 Feb 2014: International Journal of Bifurcation and Chaos, Vol. 20, No. 5, pp.

2 Dec 2014: Averaging multiple experiments, we find σ 2.94 1.72 s1 or σ1 20.4 beats. ... Cell Sci. 123, 519(2010). [20] H. Edelsbrunner, D. G. Kirkpatrick, and R.

26 Nov 2014: u(x) =1. |Br|. Br (x). u(y) dy. (3.20). For the first bit observe that non-negativity ofu implies that. ... B(w,R)u. B(z,r)u and then apply. (3.20) to get:. |BR|u(w) =. B(w,R).

21 Oct 2014: Oceans, 20 127-153. Explains and utilises particle tracking. More up to date than Dalziel (1992).

22 Jul 2014: 10%. 20%. 30%. 40%. 50%. 60%. 70%. 80%. 90%. 100%. 1959 1971 1976 1981 1986 1996 2006 2016 2021. % ... Relative Importance of Components. 0%. 10%. 20%. 30%. 40%. 50%. 60%.

13 Feb 2014: For the terms 0ω. m=0. )2(. '"'''. 1,01,00,02. 0,0. 0,20,00,0. =. pppp. ppp. βδβγ. α (11). m= 1. )2('2"'2"3'''.

11 Jun 2014: points. J Diff Geom 26(2):285–314.20. Huisken G (1984) Flow by mean curvature of convex surfaces into spheres. ... J Diff Geom. 20(1):237–266.21. Cryer SA, Steen PH (1992) Collapse of the soap-film bridge: Quasistatic description.

14 Jun 2014: 104 S J Eglen et al. up to 150µm from their clonal column of origin [20–22]. ... Retinal mosaic formation 109. 10. 20. 30. 40. 50. 60. 0 100 200 300 400 500.

20 Jul 2014: Downloaded to IP:31.221.87.87 On: Sun, 20 Jul 2014 12:35:40. 071902-2 D. ... Downloaded to IP:31.221.87.87 On: Sun, 20 Jul 2014 12:35:40. 071902-3 D.

29 Aug 2014: 10 = 1 eiπ/4λ iλ2. 9, (86). 20 =13. (iλ2. eiπ/4λ 1+ 3. ), ... 3, (103). β = ρ/ρp and 10 and 20 are given by Eqs.

14 Jun 2014: July 23, 2008 — as of December 20, 2008. 1. Nota Bene: S is the language, R is one dialect!

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.

29 Aug 2014: With eqs. (A.4), and (A.20)–(A.23), we perform thenumerical integration in eq. ... B.20). 3 Note that the constant c is referred to as a in Stimson’soriginal article [39].

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.

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.

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.

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

12 May 2014: σ/N vs t/N2 (Rouse). Short times finite. 0.1. 1. 0 5 10 15 20.

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-.

22 Dec 2014: a = 0, b = π, (t [0,π],q(t) = 20 cos(2t)), α1 6= 0, β1 6= 0, α2 = β2 = 0,. ... 2. 20 Alberto Gil C. P. Ramos, Arieh Iserles. B.2 Estimating π(Bλ ,1(ck,t).

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.

14 Jun 2014: 7622 • J. Neurosci., August 20, 2003 • 23(20):7621–7629 Sernagor et al. • ... 7626 • J. Neurosci., August 20, 2003 • 23(20):7621–7629 Sernagor et al. •

22 Apr 2014: 20. Similarly to the two-dimensional case and forsimilar geometrical reasons, the surface energy stays constantin the dewetting range (α between 0 and π/2 θE ). 2. Hydrophilic case. In the ... FIG. 20. (Color online) Total surface energy E as a

14 Jul 2014: Φ iscomputed for drops with diameters between 4 20 μm and25 125 μm for dense (area fraction 25%) and semidilutesuspensions (area fraction 10%).Fig. ... Phys Rev Lett 110(22):228102. 20. Aranson IS (2013) The aquatic dance of bacteria.

23 Jul 2014: 20 / 26. Solving linear systems. TheoremLet Binv(l 2(N)) denote the set of bounded invertible operators anddefine the domain = Binv(l 2(N)) l 2(N).

19 Nov 2014: Parameters:. {Number} precision. the decimal preciison. Documentation generated by JsDoc Toolkit 2.1.0 on Thu Nov 20 2014 00:20:57 GMT0800 (CST).

14 Jun 2014: 7 Exp. 8 Exp. 9 Mean rank Pooled rank. AChR. 1 20 1051 176 4 50 16 10 4496 66 654 2AChR. ... 3, 8, 9, 20, and 24). For theother five, however, in situ hybridization revealed a punctatepattern of expression associated with individual muscle fibers(Fig.

21 Jan 2014: ρ(Dλ,0(ck,ck1)). 2. )20. = O (1). [1 00 1. ]O (1). ... 0 O (1) (2hmax). O (1) (2hmax)1 0. ]. 22. where we have called upon assumptions (1.19)–(1.20) and (A.15).