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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.

7 Oct 2015: TJ Zuehlsdorff, ND Hine, JS Spencer, NM Harrison, DJ Riley and PD Haynes,TCM Group, 19 JJ Thomson Ave, Cambridge, CB3 0HE, UK  Privacy policy  Design by Drs .

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).

2 Dec 2015: maximizesi,tj. { i. si j. tj : αiβj si tj 0, i, j}.

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

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

25 Sep 2015: FL47CH15-Goldstein ARI 1 December 2014 20:34. Green Algae as ModelOrganisms for BiologicalFluid DynamicsRaymond E. GoldsteinDepartment of Applied Mathematics and Theoretical Physics, Centre for MathematicalSciences, University of Cambridge,

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,.

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 Sep 2015: Assume p > q. Let Tj = inf{n > 1 : Xn = j} if this is finite, and Tj = otherwise. ... Let Ti = inf{n > 1 : Xn = i}. For each i 6= j letqij = P(Tj < Ti | X0 = i) and mij = E(Tj | X0 = i).

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

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,.

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 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.

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:

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.

11 Sep 2015: Manufacturing engineering TS. Mechanical engineering TJ. Road and Bridge engineering TE-TG.

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