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4 Aug 2010: See S. Catani, G. Marchesini and B.R.Webber, Nucl. Phys. B349 (1991) 635. ... Strictly the distribution is exponential in 1-COS(THETA), with mean CLSMR; increasing CLSMR increases the decorrelation.

4 Jan 2016: ii) For a massive boson with momentum p = (p sin θ, 0, p cos θ), a suitable choice ofthe three possible polarisation vectors is:. ... ǫν1 = (0, 0, 1, 0), ǫν2 = (0, cos θ, 0, sin θ), ǫνL =. 1. mZ(pZ, EZ sin θ, 0, EZ cos θ). iii) In the

26 Oct 2012: 2(ceR)2(cµR). 2 2(ceR)2(cµL)2 2(ceL)2(cµR)2 2(ceL)2(cµL)2) cos θ}= A(1 cos2 θ) B cos θ,. ... 1. A(1 cos2 θ) B cos θd(cos θ). = 2πA. [. x x3. 3. ]1. 1. =16. 3πA. =16. 3π. g4Z256π2Γ 2Z. [.

19 Nov 2007: d = d cos θiq dφiq. Angular Ordering. Monte Carlo Methods 2 Bryan Webber. ... Hence. 1 cos θjq = a b cos φiqz = exp(iφiq).

26 Oct 2012: d cos θ=. dy. d cos θdσ. dy 1. 2(1 y)2 = 1. ... Γ(B0d Bd0). 0. eΓt(1 cos mt)dt = 1Γ. x2. 1 x2.

16 Jan 2007: 0. 50. 100. 150. 200. 250. 300. 350. 400. 450. b) udsZ|<0.8θ|cos. ... b) The jet energy resolution, defined as the α inσEE - α E GeV , plotted versus cos θqq for four different values of , s.

4 Dec 2008: Spacelike branching: gluon splitting on incoming line (a). p2b = EaEc(1 cos θ) 0. ... p2b m2q = EaEc(1 va cos θ) 0 ,. Hence Ec 0 soft divergence remains; collinear enhancement becomes a divergence as.

6 Dec 2023: p3 = (E, E sin, 0, E cos). p4 = (E,E sin, 0,E cos). ... ML =gWp2 (0, 0, 0, 1) mW (0,cos,i, sin) =. 1p2gW mW sin.

4 Dec 2008: i. 29. Angular Ordering. To prove angular ordering property, write. 1 cos θjq = a b cos φiq. ... where. a = 1 cos θij cos θiq , b = sin θij sin θiq.

15 Sep 2009: i. 5. Angular Ordering. To prove angular ordering property, write. 1 cos θjq = a b cos φiq. ... where. a = 1 cos θij cos θiq , b = sin θij sin θiq.