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  2. 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.
  3. 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,.
  4. !"#$%&' !"#$%&' !"#$%&'…

    https://www.lib.cam.ac.uk/files/thistgeog_2.pdf
    20 May 2015: RF4&' #!F,',15(00& #$F,''lZ& #RF,')(/5 #WUFn-&;V' #OFn-&);1c,'; #$F'&1)& #RJ5194(m #WJ&1.Q%l2'&) #RJ,';,7+& #TJ,16) #OJ'nC& #WG1'& #IG1'&jS,(' #!K(()-l'& #
  5. 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.
  6. 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}. ,
  7. 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).
  8. 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
  9. 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.
  10. https://www.hep.phy.cam.ac.uk/~lester/dtm662/mt2/Releases/oxbridgekine…

    https://www.hep.phy.cam.ac.uk/~lester/dtm662/mt2/Releases/oxbridgekinetics-0.8/README
    2 Mar 2015: Mt2_332_Calculator that expose the splitting at the MT2 minimum (used by MAOS methods and some top-quark mass reconstruction methods) 0.8 2nd March 2015 - At request of TJ
  11. https://www.hep.phy.cam.ac.uk/~lester/dtm662/mt2/Releases/oxbridgekine…

    https://www.hep.phy.cam.ac.uk/~lester/dtm662/mt2/Releases/oxbridgekinetics-0.8/configure
    2 Mar 2015: #! /bin/sh # Guess values for system-dependent variables and create Makefiles. # Generated by GNU Autoconf 2.63 for OxbridgeKinetics 0.8. # # Report bugs to lester@hep.phy.cam.ac.uk. # # Copyright (C) 1992, 1993, 1994, 1995, 1996, 1998, 1999, 2000,

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