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  2. www.damtp.cam.ac.uk/user/mem/oldftp/JUPITER-UNEARTHLY-TALK/0-readme-ju…

    www.damtp.cam.ac.uk/user/mem/oldftp/JUPITER-UNEARTHLY-TALK/0-readme-jupiter-unearthly-oxf150902.txt
    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.
  3. Lopsided coatings of a visco-elastic fluid on a vertical fibre

    www.damtp.cam.ac.uk/user/hinch/talks/APSBoston2015.pdf
    18 Nov 2015: I Second normal stress difference = tension in vortex lines new instability.
  4. B10c.dvi

    www.damtp.cam.ac.uk/user/tong/em/B10c.pdf
    12 Mar 2015: Find a gauge transformation such that the new vector potential is “transversely.
  5. Analysis of time-resolved emission from bright hot pixels of ...

    www.damtp.cam.ac.uk/user/astro/cl7/talks/CT3_4.pdf
    23 Jul 2015: We compare 10,000 realizations w/ 1 observation. New issue: simultaneous comparison 94A335A.
  6. Standard Model Mathematical Tripos, Part IIIDr M B Wingate ...

    www.damtp.cam.ac.uk/user/wingate/Notes/StdM/sheet4.pdf
    6 Mar 2015: If L3,4 is added to the QED Lagrangian for muons andelectrons, show that one can define new fields µ′ and e′ to yield a Lagrangian whichis diagonal in flavour.
  7. Emergent Properties of Magnetic Energy Release in Plasmas

    www.damtp.cam.ac.uk/user/astro/cl7/talks/CT1_5.pdf
    21 Jul 2015: 𝐹. 𝐉 𝑑𝐥. A. New relaxation hypothesis. The magnetic field relaxes to the lowest energy state consistent with rearrangement of field line helicity.
  8. delzanna_mason_2015ar_cores

    www.damtp.cam.ac.uk/user/astro/cl7/talks/CT1_3.pdf
    22 Jul 2015: Fe XVIII and AIA 94 A. New Fe XIV identification (Del Zanna 2012): strong contribution to AIA 94 A It is possible to estimate the Fe XVIII contribution (Del Zanna 2013).
  9. MASTERHow-to-find-us-v2

    www.damtp.cam.ac.uk/user/astro/cl7/How-to-find-us-v2.pdf
    10 Jun 2015: The Backs. River Cam. CASTLEHILL. NEW. NHAM. ROA. D. Gonville & CaiusSports Ground.
  10. Cop yrig ht © 201 5 U nive rsity ...

    www.damtp.cam.ac.uk/user/examples/3R2d.pdf
    2 Dec 2015: d) Recently, a new version of Higgs inflation has been proposed.
  11. Hi-C observations of an active region corona, and investigation of…

    www.damtp.cam.ac.uk/user/astro/cl7/talks/CT1_6.pdf
    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.
  12. 1. TENSOR RENORMALIZATION GROUP. . . . . . ...

    www.damtp.cam.ac.uk/user/wingate/Part3Essay/Wingate_Ess_15_16.pdf
    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
  13. Standard Model Mathematical Tripos, Part IIIDr M B Wingate ...

    www.damtp.cam.ac.uk/user/wingate/Notes/StdM/sheet1.pdf
    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.
  14. Physics 8, 39 (2015) ViewpointHow to Turn an Embryo ...

    www.damtp.cam.ac.uk/user/gold/pdfs/Physics.8.39.pdf
    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,
  15. D18S.dvi

    www.damtp.cam.ac.uk/user/examples/D18S.pdf
    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,
  16. Slide 1

    www.damtp.cam.ac.uk/user/astro/cl7/talks/P3_9.pdf
    16 Aug 2015: INTENSITY CONSERVING SPLINE INTERPOLATION (ICSI): A NEW TOOL FOR SPECTROSCOPIC ANALYSIS.
  17. DysonFreemanArticle

    www.damtp.cam.ac.uk/user/tong/em/dyson.pdf
    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
  18. Mechanics Lecture Notes 1 Lecture 2: Equilibrium of a ...

    www.damtp.cam.ac.uk/user/po242/pdfs/Mech2015/L2.pdf
    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.
  19. A reciprocal theorem for boundary-driven channel flows

    www.damtp.cam.ac.uk/user/lauga/papers/111.pdf
    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.
  20. A note on compressed sensing of structured sparse wavelet ...

    www.damtp.cam.ac.uk/research/afha/anders/DiscreteFourierHaarNote5.pdf
    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.
  21. Instabilities of a thin coating on a vertical fibre; Newtonian,…

    www.damtp.cam.ac.uk/user/hinch/talks/Leeds2015.pdf
    10 Oct 2015: I Second normal stress difference = tension in vortex lines new instability.
  22. Do Dissolving Objects Converge to a Universal Shape?Elias Nakouzi,†…

    www.damtp.cam.ac.uk/user/gold/pdfs/dissolution.pdf
    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
  23. 31 Dec 2015: Pearson Education Inc., New York,2013), p. 712. PROPULSION OF BUBBLE-BASED ACOUSTIC … PHYS.
  24. Instabilities of a thin coating on a vertical fibre; Newtonian,…

    www.damtp.cam.ac.uk/user/hinch/talks/ICL2015.pdf
    4 Nov 2015: I Second normal stress difference = tension in vortex lines new instability.
  25. Geometric pumping in autophoretic channels

    www.damtp.cam.ac.uk/user/lauga/papers/107.pdf
    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.
  26. A note on compressed sensing of structured sparse wavelet ...

    www.damtp.cam.ac.uk/research/afha/people/anders/DiscreteFourierHaarNote5.pdf
    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.
  27. Plethora of transitions during breakup ofliquid filamentsJosé Rafael…

    www.damtp.cam.ac.uk/user/hinch/publications/PNAS-2015.pdf
    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.
  28. Instability of a Möbius Strip Minimal Surface and a ...

    www.damtp.cam.ac.uk/user/gold/pdfs/meeks_mobius.pdf
    24 Mar 2015: 3] C. Isenberg, The Science of Soap Films and Soap Bubbles(Dover, New York, 1992).
  29. 4 Aug 2015: Garland Science, New York, 2014). [2] J. Kärger, T. Binder, C.
  30. PHYSICAL REVIEW E 92, 022701 (2015) Feeding ducks, bacterial ...

    www.damtp.cam.ac.uk/user/gold/pdfs/ducks.pdf
    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.
  31. Stable nonuniform sampling with weighted Fourierframes and recovery…

    www.damtp.cam.ac.uk/research/afha/anders/SAMPTA_Milana.pdf
    30 May 2015: Conf., Belfer Grad. School Sci., Yeshiva Univ., New York,1962–1964), 1966, pp.
  32. On random and deterministic compressed sensingand the Restricted…

    www.damtp.cam.ac.uk/research/afha/anders/RandomAndDeterministicCS.pdf
    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
  33. cgibbs.dvi

    www.damtp.cam.ac.uk/user/tong/statphys/jaynes.pdf
    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.
  34. Stable nonuniform sampling with weighted Fourierframes and recovery…

    www.damtp.cam.ac.uk/research/afha/people/anders/SAMPTA_Milana.pdf
    30 May 2015: Conf., Belfer Grad. School Sci., Yeshiva Univ., New York,1962–1964), 1966, pp.
  35. On random and deterministic compressed sensingand the Restricted…

    www.damtp.cam.ac.uk/research/afha/people/anders/RandomAndDeterministicCS.pdf
    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
  36. PHYSICAL REVIEW E 92, 023004 (2015) Phase-separation models for ...

    www.damtp.cam.ac.uk/user/lauga/papers/109.pdf
    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,.
  37. Why geometric numerical integration? A. Iserles & G.R.W. Quispel…

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2015_05.pdf
    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
  38. Banded, stable, skew-symmetricdifferentiation matrices of high order…

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2015_03.pdf
    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.
  39. On fundamentals of models and sampling in compressed sensing ...

    www.damtp.cam.ac.uk/research/afha/people/alexb/papers/CSModels.pdf
    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.
  40. 10 Green’s functions for PDEs In this final chapter ...

    www.damtp.cam.ac.uk/user/dbs26/1BMethods/GreensPDE.pdf
    30 Nov 2015: as our new form of Green’s second identity involving Gn, where now we take the boundary.
  41. Continuous Compressed Sensing of Inelastic and Quasielastic Helium…

    www.damtp.cam.ac.uk/research/afha/anders/CS4HAS_Arxiv_2.pdf
    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].
  42. Numerical stability in the presence of variable coefficients Ernst ...

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2013_10.pdf
    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
  43. On the absence of the RIP in real-world applications ...

    www.damtp.cam.ac.uk/research/afha/people/alexb/papers/ripl.pdf
    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.
  44. Continuous Compressed Sensing of Inelastic and Quasielastic Helium…

    www.damtp.cam.ac.uk/research/afha/people/anders/CS4HAS_Arxiv_2.pdf
    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].
  45. Scientific Programming with R Stephen EglenLaurent Gatto September 6, …

    www.damtp.cam.ac.uk/user/sje30/teaching/r/2015/spr-4up.pdf
    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.
  46. CORONAL LOOP VII, Workshop

    www.damtp.cam.ac.uk/user/astro/cl7/cl7_abstract_book.pdf
    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.
  47. D26e.dvi

    www.damtp.cam.ac.uk/user/examples/D26e.pdf
    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
  48. On the discretisation of the semiclassical Schrödinger equation with …

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2015_02.pdf
    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,.
  49. J. Fluid Mech. (2014), vol. 745, pp. 592–620. c© ...

    www.damtp.cam.ac.uk/user/jneufeld/pubfiles/Pegler-2014.pdf
    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
  50. on June 3, 2015http://rsif.royalsocietypublishing.org/Downloaded from …

    www.damtp.cam.ac.uk/user/gold/pdfs/metachronal_jrsi.pdf
    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),
  51. J. Fluid Mech. (2014), vol. 757, pp. 330–353. c© ...

    www.damtp.cam.ac.uk/user/jneufeld/pubfiles/Pegler-2014-1.pdf
    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

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