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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

22 Jul 2015: u1. u2. ui…. …. t1t2. tj…. …Li. apply. gather scatter… …. apply. apply. u1. u2. ui…. …. t1. t2. tj…. …. gather scatter. ... Li. applyu1u2. ui…. …. t1. t2. tj…. …Li. gatherapply. scatter. (a) (b) (c).

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

22 Aug 2015: If the energy of a traffic process Xj atscale Tj=2. jT0 is higher than the energy of a Poisson process that has the same. ... average rate with Xj, then we say that Xj is bursty at scale Tj.

12 Feb 2015: Pj’s local state is WANT) – If (Tj, Pj) < (Ti, Pi) then queue request from Pi – Otherwise, reply with OK, and con@nue wai@ng. • ... Variant scheme (due to Lamport): – To enter, process Pi mul@casts request(Pi, Ti) [same as before] – On

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,.

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,

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).

8 Jan 2015: l1]Tj. Cambridge UniversityEngineering Department. MPhil in Advanced Computer Science 10. Module L101: Machine Learning for Language Processing.

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,.

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.

3 Mar 2015: P1 P2. …. T1 T2 T3. User address. space. T1 T2 T3 Tj.