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5 Feb 2015: 30.94268 12.20211 165.4088 14.02198 102.1661 22.39954 130.5360 24.54925 54.39669 27.35860 55.83458 18.97185 260.9365 28.02304 194.9137 ... 5112 155.7039 259.5173 223.7271 266.5150 248.4850 266.6068 122.2994 271.7742 286.1407 280.3929 241.9675 282.2188 162

5 Feb 2015: 277.1 558.79 317.32 36.05 325.27 668.09 344.24 134.28 340.67 316.73 355.22 397.9 361.75 491.87 386.29

16 Aug 2015: G. R. Gupta, D. Tripathi & H. E. Mason. P1.24. CHIANTI version 8.

4 Aug 2015: pattern-ing the particle surface with active and passive sites (e.g. Janusparticles),23,24,28 (ii) spontaneous symmetry-breaking resultingfrom the advection of the field responsible for the phoreticresponse by ... K. Sia and G. M. Whitesides,

24 Mar 2015: Received 1 December 2014; published 24 March 2015). We describe the first analytically tractable example of an instability of a nonorientable minimal surfaceunder parametric variation of its boundary. ... 24] M. do Carmo and C. K. Peng, Stable complete

31 Dec 2015: 2p 1)" 2p1. L. x. 2+. 2q1Ly. 2# ez, (24). while the sensitivity on the vertical walls Hvert(y) at x = 0 and x = Lx can be obtained by symmetry.The ... Rev. Lett. 99, 048102 (2007).24 R. Golestanian, T. B. Liverpool, and A.

31 Dec 2015: 24]), forexample, at an air-water interface such as the surface of abubble [25,26]. ... Rev. 73, 68 (1948). [24] W. L. Nyborg, Acoustic streaming near a boundary,J.

4 Aug 2015: Cambridge CB3 0HE, United Kingdom(Received 16 February 2015; revised manuscript received 24 April 2015; published 15 July 2015). ... 24] M. Padgett and R. Di Leonardo, Holographic opticaltweezers and their relevance to lab on chip devices, LabChip 11,

31 Mar 2015: Similarly, when viscouseffects are dominant, thinning and pinching occur in a viscous(V) regime (24) where viscous and capillary forces balance, andhmin and ReðtÞ vary with τ as. ... of satellites is associated with inviscid fluids (20, 23, 24,

5 Aug 2015: When the nutrient is essential for life, suchas oxygen for obligate aerobes, f (c) may vanish below somec [24,25]. ... μ̄ = 1λ. λ0. dx y(c)cb. (24). 022701-5. FRANÇOIS J. PEAUDECERF AND RAYMOND E.

9 Nov 2015: We have (P 1)K = 24 equa-tions for K(K 1)/2 = 28 unknowns. ... Dj,k = 0 for |k j| 6. There remain 25 unknowns for the 24 equations.

4 Aug 2015: Integral theorems for small-amplitude motion showedthat the superposition of multiple waves could also lead to anenhancement transition for a range of Deborah numbers [24]. ... Liu, and T. R. Powers, Phys. Rev. Lett. 111,068101 (2013). [24] E.

1 Oct 2015: joe. age height. 24.0 1.7. 30 / 191. Naming indexes of a vector. > ... x. [1] 20.00000 24.14214 27.32051 30.00000 32.36068. 62 / 191.

13 Jan 2015: Hence1. ǫ0Q =. S=V. E dS. (24). The right-hand side is the flux of E out of V. ... The statement (24) is Gauss’s Law. It is ofpractical use.Ex. Consider a point charge q at rest at O, and let V be the sphere of radius r centred

9 Nov 2015: shape. y(x) =µg. 2Tx(x L). (7.24). that obeys y(0) = y(L) = 0. –

22 Apr 2015: h r1/5(a2A)1/5, (20). where the prefactor r1/5 z 0.96 corresponds to the only real zeroof a third order polynomial, 16 384r3 24 192r2 10 611r ... DQ0/e ðqe q0Þ deA: (24). Finally, as the swimmer escapes from the colloid surface(step iii) we have the

17 Dec 2015: 2. ) f(x′). ], (2.24). preserving all quartic Hamiltonians.We note that (2.22) has second order accuracy.

4 Oct 2015: This new vibrational modes are called surface phononsdue to their localisation at the surface [24–26]. ... m & N µ(A1W1) s log(N), (24). in order to guaranty successful recovery with high probability, where µ(B) = max1i,jN |Bi,j|2.

4 Oct 2015: This new vibrational modes are called surface phononsdue to their localisation at the surface [24–26]. ... m & N µ(A1W1) s log(N), (24). in order to guaranty successful recovery with high probability, where µ(B) = max1i,jN |Bi,j|2.

10 Jul 2015: Model-based [5], TurboAMP [24], Bayesian CS [14] etc.), simply by using structured sampling and. ... arXiv:1406.4178, 2014. [24] S. Som and P. Schniter. Compressive imaging using approximate message passing and a markov-tree prior.

3 Jun 2015: 200. 0. 200. 100. 0. colonyaxis. uÒtur. uq. t = 0 ms 6 ms 12 ms 18 ms 24 ms. ... Fi gi vi þXj=i. G(xj, xi) Fj. 24. 35, (3:1). where G(xj, xi) is the Green’s function that couples the differ-ent spheres in the presence

21 Jan 2015: Email address for correspondence: ssp23@cam.ac.uk. first published online 24 March 2014). ... upper fluid to speeds above those induced by the background-pressure-driven flow (3.24) alone.

30 Nov 2015: φ|Rn{0} = 0 , tφ|Rn{0} = 0 and lim|x|. φ = 0 , (10.24).

26 Oct 2015: and hence that the volume element is. dV = dx dy dz = r2 sin θ dr dθ dφ (3.24).

18 Nov 2015: f, f) =1. 2π(f̃, f̃) (8.24). so that the L2-norm of a Fourier transform agrees with the L2-norm the original function,.

8 Nov 2015: RTkz RTz‖2 ‖R(Tkz) R(Tz)‖2 p(Tk z,T z)2. 8δ̂(Tk z,T z)2. 24(1 |z|2)2δ̂(Tk,T)2. ... ζ(z)2 ζ̃2k(z)| C. 24(1 |z|2)δ̂(Tk,T). (5.4). If z σ(T) then at least one of ‖R(Tz)‖ and ‖R(Tz)‖ is equal

28 Sep 2015: 24. Cop. yrig. ht. 201. 5 U. nive. rsity. of C.

15 Jul 2015: P1.24 Giulio Del Zanna. Title - CHIANTI version 8 Authors: Del Zanna, G., Dere, K., Young, P., Landi, E., Mason, H.E.

10 Jul 2015: On the absence of the RIP in real-world applications ofcompressed sensing and the RIP in levels. Alexander BastounisCCA, Centre for Mathematical Sciences. University of CambridgeWilberforce Rd, Cambridge CB3 0WA. United Kingdom. Anders C. HansenDAMTP

8 Nov 2015: RTkz RTz‖2 ‖R(Tkz) R(Tz)‖2 p(Tk z,T z)2. 8δ̂(Tk z,T z)2. 24(1 |z|2)2δ̂(Tk,T)2. ... ζ(z)2 ζ̃2k(z)| C. 24(1 |z|2)δ̂(Tk,T). (5.4). If z σ(T) then at least one of ‖R(Tz)‖ and ‖R(Tz)‖ is equal

30 Nov 2015: 2.3 Self-adjoint differential operators 22. 2.4 Eigenfunctions and weight functions 24. ... 1)k1. ikeikθ (1.24). do in fact converge on the sawtooth function everywhere except at the discontinuity.

18 May 2015: P.H.Haynes Part II Dynamical Systems Michaelmas Term 2014 24. Theorem 6 (Lyapunov’s Second Theorem [L2]).

4 May 2015: Charney [24], Aleksandr Mikhailovich Obukhov [25],. and Ernst Kleinschmidt [26]. 1.4 Cyclone and jet structure. ... dent pioneering work of Charney [24] and Obukhov [25] and are described.

3 Apr 2015: Numerical stability in the presence of variable. coefficients. Ernst Hairer. Section de mathématiquesUniversité de Genève. Email: Ernst.Hairer@unige.ch. Arieh Iserles. Department of Applied Mathematics and Theoretical PhysicsCentre for

27 Apr 2015: e2iω. ω2(2k1). ). 24. Setting h2N1,k(ω) to zero, we obtain an asymptotic expression for the kth ‘onionpeel’.

16 May 2015: on May 16, 2015http://rsfs.royalsocietypublishing.org/Downloaded from. rsfs.royalsocietypublishing.org. ResearchCite this article: Goldstein RE, van de MeentJ-W. 2015 A physical perspective on. cytoplasmic streaming. Interface Focus 5:20150030. http:

23 Sep 2015: elifesciences.org. RESEARCH ARTICLE. Cortical microtubule nucleation canorganise the cytoskeleton of Drosophilaoocytes to define the anteroposterior axisPhilipp Khuc Trong1,2, Hélène Doerflinger3, Jörn Dunkel1,4, Daniel St Johnston3,Raymond E

5 May 2015: On the discretisation of the semiclassical Schrödinger. equation with time-dependent potential. Arieh Iserles, Karolina Kropielnicka† & Pranav Singh‡. April 30, 2015. AMS Mathematics Subject Classification: Primary 65M70, Secondary 35Q41,65L05,

25 Sep 2015: FL47CH15-Goldstein ARI 1 December 2014 20:34. Green Algae as ModelOrganisms for BiologicalFluid DynamicsRaymond E. GoldsteinDepartment of Applied Mathematics and Theoretical Physics, Centre for MathematicalSciences, University of Cambridge,