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30 Apr 2018: 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 ... 1.0 30th April 2018 - At request of TJ Khoo, made LesterNachman method availabl

16 May 2018: 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 ... 1.1 30th April 2018 - At request of TJ Khoo, made LesterNachman method availabl

13 Mar 2018: with,. po =K. k=1. {(T tkπk. ) k1. j=1. (1 T tj πj )}δ(mt=k). ... p({yt}Nt=1|Hs) =. t. j,k. τ tj. pl(yt1k , y. tj|τ. tj , µ.

13 Mar 2018: with,. po =K. k=1. {(T tkπk. ) k1. j=1. (1 T tj πj )}δ(mt=k). ... p({yt}Nt=1|Hs) =. t. j,k. τ tj. pl(yt1k , y. tj|τ. tj , µ.

13 Mar 2018: Now each point is typically parametrized as. x̃j := x̃(xj, tj) :=[x>j tj. ... xj1 xj2 xj3 tj. ]>(20). where xj =[xj1,xj2,xj3. ]>is the vector of unscaled inhomogeneous coordinates of.

13 Dec 2018: dx8,. Tj ,n5 2 Exj 21. ... xjGr1;r28!dx8,. Sj ,n8 5 Exj 21. xjGr2;r18!dx8,. Tj ,n8 5 2 Exj 21.

8 Jan 2018: j=0. fj(a). j!tj. (vii) Observe thatf(t). g(t)=f(n1)(θt). g(n1)(φt)with θt, φt a as t a and use continuity.

20 Feb 2018: 0j),(b,a)),. ,k((b. tj,a. tj),(b,a))]. T,j = 1,. , l.Therefore, in principle, one needs to be able to calculate thekernel function k((b′,a′),(b,a))

13 Mar 2018: Now each point is typically parametrized as. x̃j := x̃(xj, tj) :=[x>j tj. ... xj1 xj2 xj3 tj. ]>(20). where xj =[xj1,xj2,xj3. ]>is the vector of unscaled inhomogeneous coordinates of.

18 Oct 2018: BA Brookes, TJ Davies, AC Fisher, RG Evans, SJ Wilkins, K Yunus and RG Compton.

18 Oct 2018: Rep. 7-43298 (2017). Reid JS, Lagrosas ND, Jonsson HH, Reid EA, Atwood SA, Boyd TJ, Ghate VP, Xian P, Posselt DJ, Simpas JB, Uy SN, Zaiger K, Blake DR, Bucholtz ... Chem. Phys. 16:14057–14078 (2016). Reid JS, Lagrosas ND, Jonsson HH, Reid EA, Sessions

20 Feb 2018: tj). ᵀ log ptj, where ytj and p. tj are out-.

17 Aug 2018: c) = supa=t0<t1<<tk =b. k1j=0. d (c (tj) ,c (tj1)) d (c(a),c(b)).

14 Mar 2018: Notice by the editor 1PriNciPal officers of the UNiversity 2officers iN iNstitUtioNs Placed UNder the sUPervisioN of the GeNeral board 3. Professors 3Readers 15Composition of the Schools 19Faculties and Departments 20. Architecture and History of

13 Mar 2018: This. was determined empirically as a conservative threshold. Tocompare two trajectories Xi and Xj , which respectively ex-tend in time over ti and tj , we consider only the over-lapping range ... of frames {fn : n ti tj}.

30 May 2018: ,. where tj = 1 0.5(sin(j) i cos(j)) for j 4.

13 Mar 2018: w j ZT R j Z ' U jU Tj. From (2), we have w jU Ti U jU Tj Ui = O,i.e.

13 Mar 2018: T4R/v/9 Z3/4 O@Tj]ft5/b[H=kQU] =_ QU=@dkS5/0c+/P1[fSRQU/Pc+/P23]H[a[H==_s]H/P2j;RQU=54-S5v/4 O@TZ59A[mSR1? _ ... c&1@2ºÙ-?A]H/PQb]i=j]mt5/0=kS5]m;RS5]I=_ ]ft5/]mQH1 v {/PQuE1 [b9B2BÛë>@ÜU )c+=kQU/b/?A/dk132@]b1@;R;RQU=51v

20 Feb 2018: tj is the last output token (i.e. a word,. a delexicalised2 slot name or a delexicalised2 slot value),and htj1 is the decoder’s last hidden state.

13 Mar 2018: pinhole camera P̂ [13] is given by P̂ II tj , wheret 0 0 T, for any > 0, symmetry considerations showthat the profile ŝ of S will be bilaterally symmetric with. ... calibration matrix K [13]. Let KR H. Thus, P HII tj and the point Ux in space with