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6 Mar 2015: Standard Model. News. I collected e-mail addresses of those interested in examples classes on Monday 26 Jan.

10 Feb 2015: This equation is rewritten in terms of new variables. which are everywhere regular.

5 Feb 2015: I have extracted the bitmap of the combined field (part a of Fig 6), and removed the dendrites from around each cell into a new image.

27 Mar 2015: Stephan Stieberger  (Munich) New relations between gauge and gravity amplitudes in field and string theory.

16 Aug 2015: Intensity Conserving Spline Interpolation (ICSI): A New Tool for Spectroscopic Analysis.

1 Dec 2015: δz(z 1)(w z)2. ). Here α,β,γ,δ are constants. The solutions to these equations define new functions, called the Painlevétranscendents.

27 Mar 2015: NEW: Graduate Student registration fee is £125 (including the banquet). Accommodation.

23 Feb 2015: Cambridge is an important centre for this research, and is providing new opportunities to involve people with different expertise, and so by 2065 the condition may be less of a problem. ... More generally, there is a need to develop new employment models

10 Nov 2015: ψn(x,t) = cn(t)eχnx as x. As before, consider the new functions ψ′n = tψn Aψn.

6 Sep 2015: Atmos. Sci., Thomson, S.I and McIntyre, M.E. 2015: Jupiter's unearthly jets: a new turbulent model exhibiting statistical steadiness without large-scale dissipation.

12 Mar 2015: Find a gauge transformation such that the new vector potential is “transversely.

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

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

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

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,

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.

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 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.

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 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.

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

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.

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: 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

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

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.

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

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,.

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.

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].

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.

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

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.

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

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),

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,.

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.

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