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3 Jul 2024: GR Grimmett, TJ Osborne, PF Scudo. – Journal of Statistical Physics.

3 Jul 2024: AI Malz, R Hlozek, TJ Allam, A Bahmanyar, R Biswas, M Dai, L Galbany, EEO Ishida, SW Jha, DO Jones, R Kessler, M Lochner, AA Mahabal, KS Mandel, JR Martinez-Galarza,

15 Oct 2021: xk), together with achoice of k points τ = (t0,. , tk1) such that tj [xj,xj1] for j = 0,. ... k 1 there exists tj [xj,xj1] such that:. F(xj1) F(xj) = f(tj)xj.

12 Oct 2007: Sinceσ(Tj) = Tj for all σ Gal(Kv/Kv(θj)), these cocycles are equal. ... X = Q gives e2(σQ Q,Tj) = tj(σQ)/tj(Q) = σ(tj(Q))/tj(Q) for.

25 Jan 2024: random variables, independent of N. Show that if g(s,x) is a function and Tj are thejump times of N then. ... E[exp{θNtj=1. g(Tj,Xj)}] = exp{λ t0. (E(eθg(s,X)) 1)ds}. This is called Campbell’s theorem.(b) Cars arrive at the beginning of a long

9 Nov 2023: closed: if tj B with tj tfin then tfin B. Relies on higher orderCk estimates for all the quantities and Arzela-Ascoli theorem to showconvergence. ... the gauge assumptions need to be constructed for the extendedspacetime. closed: if tj B with tj tfin

11 Oct 2006: "!#$%&(')( ,.-0/. 1 3246587:96;8<=5?>A@BDCFEGCIHKJL>A5JMNMPO6>AN;Q5R S6T:5U@3NVW5?XY5?>ZJLO6O 5?7[JYJN7VAZJLVWVAD>]5U57:96;8< 5>A@3T _VA65_aT>A;cbdAb ef GdAb e#gQJL>A5hJMMO6>AN;Q5ji. Gk-05?Vml05U5U7 1 hJ76SQ

28 Jan 2013: Find all relations between Fi and Fj, Ti and Tj for differing values ofi and j.

31 Jan 2023: random variables, independent of N. Show that if g(s,x) is a function and Tj are thejump times of N then. ... E[exp{θNtj=1. g(Tj,Xj)}] = exp{λ t0. (E(eθg(s,X)) 1)ds}. This is called Campbell’s theorem.(b) Cars arrive at the beginning of a long

13 Dec 2017: Find all relations between Fi and Fj, Ti and Tj for differing values ofi and j.