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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.

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

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

19 Feb 2015: The relative vectors between the camerasare given by tij = tj ti.

27 Feb 2015: Nj=1 ‖γ(tj) γ(tj1)‖ where the sup is taken over all. finite partitions 0 = t0 < t1 <. < tN = 1. (i) Give an example for which (γ) =. If γ is continuously

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.

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

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,

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 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).

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}. ,

5 May 2015: We define Fk. j1 Tj as the set of all trees of power k in h which appear.

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,.

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'& #

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.

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.

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

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

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

9 Sep 2015: elife.elifesciences.org. MacKinnon et al. eLife 2014;3:e01483. DOI: 10.7554/eLife.01483 1 of 23. An allosteric Sec61 inhibitor traps nascent transmembrane helices at the lateral gateAndrew L MacKinnon1†, Ville O Paavilainen1†, Ajay Sharma2,