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10 Jun 2015: The Backs. River Cam. CASTLEHILL. NEW. NHAM. ROA. D. Gonville & CaiusSports Ground.

2 Dec 2015: d) Recently, a new version of Higgs inflation has been proposed.

22 Jul 2015:  Lack of coronal emission in umbra-to-umbra loops is new evidence supporting Parker’s idea that convection at loop footpoints drives coronal heating in ARs.

23 Jul 2015: These new  measurements  of  physical  plasma  parameters  may  provide  important  constraints  on  the  modeling  of  the mass and energy balance in coronal loops.

18 Nov 2015: In practice, however, these have not proven tobe very efficient methods of obtaining accurate values for critical exponents.A new method, called the tensor renormalization group [1], builds upon newideas from

26 Jan 2015: Hint: it is easier to keep the. new 2-dimensional “super-spin” space separate from the 4-dimensional spinor spaceof ψ.] A generalized Lorentz-invariant mass term can be written as.

27 Apr 2015: Intheir new work [5], Höhn et al. observed the live in-verting embryos in three dimensions and quantified theirchanging shapes in real time. ... The work of Höhn et al.[5] also brings a new in-gredient—active matter—to the physics of thin shells,

26 Jul 2015: In the following work we present a new investigation into a certain outflow region that has been noted in other works.

5 Oct 2015: Thediscussion above shows that the origin of this unexpected sign is the non-trivial topology ofthe rotation group—in our new terminology, we have a projective representation of SO(3). ... A scattering process involves a particle, or beam of particles,

27 Jan 2015: Helmholtz understood the theory and taught Pupin what he knew. Pupin returned to New York, became a professor at Columbia University, and taught the successive generations of students who subsequently spread

8 Oct 2015: All we do is to add a pair of equal and opposite forces7 as shown in the diagrams,to give two new forces that are no longer parallel.

31 Dec 2015: Kim and S. J. Karrila, Microhydrodynamics (Dover Publications, Inc., New York, 2005).20 L. ... Press, New York, 2007).21 H. A. Stone and A. D. T.

2 Jun 2015: new theory for compressed sensing [1]. ... C. Hansen, C. Poon, and B. Roman. Breaking the coherence barrier: A new theory forcompressed sensing.

10 Oct 2015: I Second normal stress difference = tension in vortex lines new instability.

1 May 2015: The Self-Made Tapestry: Pattern Formation in Nature;Oxford University Press: New York, 2001.(2) Meng, X. ... New J. Phys. 2013, 15, 103012.(15) Camporeale, C.; Ridolfi, L. Hydrodynamic-Driven StabilityAnalysis of Morphological Patterns on Stalactites and

31 Dec 2015: Pearson Education Inc., New York,2013), p. 712. PROPULSION OF BUBBLE-BASED ACOUSTIC … PHYS.

4 Nov 2015: I Second normal stress difference = tension in vortex lines new instability.

4 Aug 2015: B. Liverpool and A. Ajdari, New J. Phys.,2007, 9, 126. 25 J. ... A. Orszag, Advanced Mathematical Methods. for Scientists and Engineers, McGraw-Hill, New York, 1978.39 L.

2 Jun 2015: new theory for compressed sensing [1]. ... C. Hansen, C. Poon, and B. Roman. Breaking the coherence barrier: A new theory forcompressed sensing.

31 Mar 2015: E. 0.5 mm. Fig. 1. Methods used for studying and new phase diagram for capillary thinning and pinch-off. ... Although the new stagnation zonepersists for some time, the filament does not break while in the.

24 Mar 2015: 3] C. Isenberg, The Science of Soap Films and Soap Bubbles(Dover, New York, 1992).

4 Aug 2015: Garland Science, New York, 2014). [2] J. Kärger, T. Binder, C.

30 May 2015: Conf., Belfer Grad. School Sci., Yeshiva Univ., New York,1962–1964), 1966, pp.

5 Aug 2015: Normalizing this new density func-tion, thus making the integral for the total number of bacterialcells appear at the denominator, we finally re-express Eq. ... Springer-Verlag, New York,2003). [21] M. Tindall, P. Maini, S. Porter, and J.

30 May 2015: Applied and Numerical HarmonicAnalysis. Birkhäuser/Springer, New York, 2013. [Online]. Available:http://dx.doi.org/10.1007/978-0-8176-4948-7. [7] R. ... Adcock, A. C. Hansen, C. Poon, and B. Roman, “Breaking thecoherence barrier: A new theory for

28 May 2015: Other aspects of this new"development have been reported elsewhere (Jaynes 1986, 1988, 1989). ... 2. The Problem. We repeat the familiar story, already told hundreds of times; but with a new ending.

30 May 2015: Conf., Belfer Grad. School Sci., Yeshiva Univ., New York,1962–1964), 1966, pp.

30 May 2015: Applied and Numerical HarmonicAnalysis. Birkhäuser/Springer, New York, 2013. [Online]. Available:http://dx.doi.org/10.1007/978-0-8176-4948-7. [7] R. ... Adcock, A. C. Hansen, C. Poon, and B. Roman, “Breaking thecoherence barrier: A new theory for

4 Aug 2015: Fluid. Mech. 9, 339 (1977).[5] D. Bray, Cell Movements (Garland Publishing, New York, NY,. ... 2009).[7] H. C. Berg, E. coli in Motion (Springer-Verlag, New York, NY,.

17 Dec 2015: Since its emergence, GNI has become the new paradigm in numerical solution ofODEs, while making significant inroads into numerical PDEs. ... As often, yesterday’srevolutionaries became the new establishment. This is an excellent moment to pauseand take

9 Nov 2015: McLachlan, and N. Robidoux. Skew-adjoint finite differencemethods on nonuniform grids. New Zealand J. ... Academic Press,New York-London, 1974. mclachlan03sdo [6] R. I. McLachlan. Spatial discretization of partial differential equations withintegrals.

10 Jul 2015: Aiming to spur new research in this direction, we conclude this note with a listof open problems and topics for future research. ... Poon, and B. Roman. Breaking the coherence barrier: A new theory for compressed sensing.arXiv:1302.0561, 2014.

30 Nov 2015: as our new form of Green’s second identity involving Gn, where now we take the boundary.

3 Apr 2015: Needless to say, it is but an initial foray into a large and important areaand our results, while solving some long-standing problems, pose many new questions.These questions and further

4 Oct 2015: the characteristics of the approxima-tion in the new basis rather than the truncated Fourier series. ... This new vibrational modes are called surface phononsdue to their localisation at the surface [24–26].

10 Jul 2015: To solve this problem, the new conceptsof asymptotic sparsity, asymptotic incoherence and multi-level sampling were introduced. ... We now introducethe fourth new concept in the new theory of compressive sensing: the RIP in levels.

4 Oct 2015: the characteristics of the approxima-tion in the new basis rather than the truncated Fourier series. ... This new vibrational modes are called surface phononsdue to their localisation at the surface [24–26].

1 Oct 2015: 1) , or directly by assigning new element (e.g. 2):. > l1 <- list(who="fred"). > ... z ## same as return(x). }. 140 / 191. Example of writing a new function.

15 Jul 2015: We also propose a new method to isolate the relevant signal from the foreground and background emission. ... We present new Hinode/EIS measurements of non-thermal broadening in 15 active region cores.

28 Sep 2015: Cop. yrig. ht. 201. 5 U. nive. rsity. of C. ambr. idge. Not. to b. e qu. oted. or. repr. oduc. ed w. ithou. t per. mis. sion. Dynamical Systems. M. R. E. ProctorDAMTP, University of Cambridge. Michaelmas Term 2011. cM.R.E.Proctor 2010(These notes

5 May 2015: ε(2k1)σ1. )for k 2. In these new splittings terms. of size O(ε(2k)σ1. ... With this new notation. in place, the Magnus expansions Θ̃ε3 and Θ̃ε4 can be presented more concisely,.

21 Jan 2015: 2Faculty of Science, University of Bristol, Bristol BS8 1UH, UK3School of Mathematics and Statistics, University of New South Wales, Sydney,. ... We also reveal the new asymptotic regimesthat emerge when the injected fluid is more viscous than the

3 Jun 2015: Because the drag is not isotro-pic, the trajectory of an isolated sphere will deviate slightlyfrom the prescribed circle (dr=r0 0:5% here) to a new limitcycle (r(t),

21 Jan 2015: 2Faculty of Science, University of Bristol, Bristol BS8 1UH, UK3School of Mathematics and Statistics, University of New South Wales, Sydney, NSW 2052, Australia4BP Institute and Department of Earth Sciences, University of ... The former is a new

8 Nov 2015: Θφµ1,.µn(x)Θ1 = (1)nφµ1,.µn(x)†. (1.118). Note that this result is consistent with forming new fields by taking derivatives,e.g.

16 May 2015: One contribution of 10 to a theme issue. ‘Bioinspiration of new technologies’.

27 Apr 2015: The kissing polynomials and their. Hankel determinants. Alfredo Deaño, Daan Huybrechs and Arieh Iserles. April 28, 2015. Abstract. We study a family of polynomials that are orthogonal with respect to theweight function eiωx in [1, 1], where ω 0.

23 Sep 2015: point of the system. Computation of 3D flow fields for each realisation in the new ensemble (3D mean:.

25 Sep 2015: Our understanding of the swimming dynamics of microorganisms has advanced over the past fewdecades in part through the development of new technologies. ... 2003, Pepper et al. 2010). Thissection considers two problems involving the swimming of organisms

18 May 2015: Part II Dynamical Systems Michaelmas Term 2014. lecturer: Professor Peter Haynes (phh1@cam.ac.uk). May 18, 2015. These lecture notes, plus examples sheets and any other extra material will be madeavailable at