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  2. The s2D Method: Simultaneous Sequence-Based Prediction of the…

    www-vendruscolo.ch.cam.ac.uk/sormanni2015jmb-s2d.pdf
    16 Feb 2015: Article. Pietro Sorman. 0022-2836/ 2014 Elsevi. The s2D Method: Simultaneous Sequence-Based Prediction of the StatisticalPopulations of Ordered and DisorderedRegions in Proteins. ni1, Carlo Camilloni1, Pier. o Fariselli 2 and Michele Vendruscolo1. 1
  3. The Causes and Consequences of Changes in Virulence following…

    www.jiggins.gen.cam.ac.uk/pdfs/Longdon2015.pdf
    18 Mar 2015: RESEARCH ARTICLE. The Causes and Consequences of Changes inVirulence following Pathogen Host ShiftsBen Longdon1, Jarrod D. Hadfield2, Jonathan P. Day1, Sophia C. L. Smith1, JohnE. McGonigle1, Rodrigo Cogni1,3, Chuan Cao1, Francis M. Jiggins1. 1
  4. SM.dvi

    www.damtp.cam.ac.uk/user/ho/SM.pdf
    8 Nov 2015: Part III Lecture Notes onThe Standard Model. by H. Osborn. 0. Part I. PCT - Conventions and Results. 1 Dirac Equation and γ-Matrices. The γ-matrices are defined by. {γµ,γν} = 2gµνI , (1.1). where. gµν =. . . . . . 1 0 0 00 1
  5. Resolution Limit for Atomic Decompositions [5mm]

    www-sigproc.eng.cam.ac.uk/foswiki/pub/SPARS2015/Program/talk26_GongguoTang_ResolutionLimit_SPARS.pdf
    2 Sep 2015: Spherical harmonics. Rank-1 tensors: a(u,v,w) = uv wTranslation-invariant signals: a(τ) = [h(tj τ)]nj=1Radar signals: a(τ,ν) = [ψ(tj τ)ei2πνtj ]nj=1Single-pole ... Define ω(t) = 2 if t /{a,b} and 1 otherwise. Adecomposition y =. j cja(tj) with
  6. proc_acacse2.dvi

    geometry.mrao.cam.ac.uk/wp-content/uploads/2015/02/00jl_mexico.pdf
    19 Feb 2015: fw{ w s _| Tj yw yw Q" fw{ w "w sg|wzv|! ' ... w ]Q Tj"fw{ w "w aUTV 7 O y zzB|G U v| $qc , { |w 5Q" w , z yw|{ È»ÉÈÉjÈb"É wO s ¿!_w y w|w w
  7. OP-MOLB150120 2111..2129

    www.jiggins.gen.cam.ac.uk/pdfs/Palmer2015.pdf
    10 Nov 2015: Article. Comparative Genomics Reveals the Origins and Diversity ofArthropod Immune SystemsWilliam J. Palmer,1 and Francis M. Jiggins11Department of Genetics, University of Cambridge, Cambridge, United Kingdom. Corresponding author: E-mail:
  8. On the Solvability Complexity Index, the n-Pseudospectrumand…

    www.damtp.cam.ac.uk/research/afha/anders/JAMS_Final_Preprint2.pdf
    8 Nov 2015: On the Solvability Complexity Index, the n-Pseudospectrumand Approximations of Spectra of Operators. ANDERS C. HANSENApplied and Computational Mathematics, California Institute of Technology,. hansen@acm.caltech.edu. Abstract. We show that it is
  9. On the Solvability Complexity Index, the n-Pseudospectrumand…

    www.damtp.cam.ac.uk/research/afha/people/anders/JAMS_Final_Preprint2.pdf
    8 Nov 2015: On the Solvability Complexity Index, the n-Pseudospectrumand Approximations of Spectra of Operators. ANDERS C. HANSENApplied and Computational Mathematics, California Institute of Technology,. hansen@acm.caltech.edu. Abstract. We show that it is
  10. On the discretisation of the semiclassical Schrödinger equation with …

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2015_02.pdf
    5 May 2015: We define Fk. j1 Tj as the set of all trees of power k in h which appear.
  11. on June 3, 2015http://rsif.royalsocietypublishing.org/Downloaded from …

    www.damtp.cam.ac.uk/user/gold/pdfs/metachronal_jrsi.pdf
    3 Jun 2015: on June 3, 2015http://rsif.royalsocietypublishing.org/Downloaded from. rsif.royalsocietypublishing.org. ResearchCite this article: Brumley DR, Polin M, PedleyTJ, Goldstein RE. 2015 Metachronal waves in. the flagellar beating of Volvox and their.
  12. On Extended State-Space Constructions for Monte Carlo Methods

    www-sigproc.eng.cam.ac.uk/foswiki/pub/Main/AF574/phd_thesis_axel_finke.pdf
    16 Jul 2015: Axel Finke. On Extended State-SpaceConstructions for. Monte Carlo Methods. Thesis submitted for the degree ofDoctor of Philosophy. Department of StatisticsUniversity of Warwick. July 2015. Typeset in LATEX using Linux Libertine & KOMA-Script. to my
  13. New technique to synthesise nanostructured nanowires | University of…

    https://www.cam.ac.uk/research/news/new-technique-to-synthesise-nanostructured-nanowires
    Thumbnail for New technique to synthesise nanostructured nanowires | University of Cambridge 16 Jul 2015: To unravel the complexities of this process, the research team used two customised electron microscopes, one at IBM’s TJ Watson Research Center and a second at Brookhaven National Laboratory.
  14. Multi-layer Sparse Matrix Factorization

    www-sigproc.eng.cam.ac.uk/foswiki/pub/SPARS2015/Program/talk04_presLE_MAGOAROU.pdf
    2 Sep 2015: Multi-layer Sparse Matrix Factorization. Luc Le Magoarou Rémi Gribonval. InriaCentre Inria Rennes - Bretagne Atlantique. France. SPARS 2015. Outline. IntroductionMotivationFast transforms as sparse factorizationsObjectiveMulti-layer sparse benefits
  15. MAXIMUM ENTROPY PROPERTY OF DISCRETE-TIME STABLE SPLINE KERNEL Tohid…

    www-sigproc.eng.cam.ac.uk/foswiki/pub/Main/TA417Publications/ArdeshiriC2015.pdf
    9 Apr 2015: Furthermore, let 0 tj < ti,. Var[g(ti) g(tj)] = E.  ir=j1. ... h(tr)tr tr1. 2. =. ir=j1. λ(tr tr1) = λ(ti tj). (15).
  16. Maximum entropy properties of discrete-time first-order stable spline …

    www-sigproc.eng.cam.ac.uk/foswiki/pub/Main/TA417Publications/ChenACCLP2014.pdf
    13 Apr 2015: Pi,j = K(ti, tj; α), i,j = 1, ,n, ti, tj T (7). ... eβ(tn1tn). eβtn1 eβtn , i = j = n,. 0, |i j| > 1 1eβ min{ti,tj}eβ max{ti,tj}. ,
  17. Mathematics of Operational Research Example Sheet 2 R. Weber ...

    www.statslab.cam.ac.uk/~rrw1/mor/examples2.pdf
    2 Dec 2015: maximizesi,tj. { i. si j. tj : αiβj si tj 0, i, j}.
  18. LINEAR ALGEBRA SIMON WADSLEY Contents 1. Vector spaces 21.1. ...

    https://www.dpmms.cam.ac.uk/~sjw47/LinearAlgebra.pdf
    20 May 2015: with λi F and ti Tr. Since {e1,. ,er1} is linearly independent there must besome 1 6 j 6 k such that λj 6= 0 and tj 6 {e1,. ... er}. Let T ′r1 = T ′r {tj} and. Tr1 = (TT ′r1) {e1,.
  19. LINEAR ALGEBRA SIMON WADSLEY Contents 1. Vector spaces 21.1. ...

    https://www.dpmms.cam.ac.uk/~sjw47/LinearAlgebraM15.pdf
    2 Dec 2015: er1} is linearly independent there must besome 1 6 j 6 k such that λj 6= 0 and tj 6 {e1,. ... er}. Let T ′r1 = T ′r {tj} and. Tr1 = (TT ′r1) {e1,.
  20. Introduction to Cost-Effectiveness Analysis

    https://cscs3.medschl.cam.ac.uk/wp-content/uploads/GAM_slides1.pdf
    2 Mar 2015: Solution• For fixed αj. , the solution to minimizing the penalized least squares in the AM is whereˆ Hyβ = 1 ( )T Tj. ... AM). (GAM). 1 ( )T Tj jj. F X X S X X HXα = = 1 ( )T Tj j.
  21. Intersection and mixing times for reversible chains Yuval Peres∗ ...

    www.statslab.cam.ac.uk/~ps422/intersection-mixing.pdf
    7 Jan 2015: i=0. tj=0 1(Xi = Yj). count the number of intersections up to time t. ... Qt =ti=0. tj=0. pij(x,x). Using the spectral theorem together with transitivity, we obtain.

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