Search

30 Mar 2011: K = B/B = 1 O(αS). arbitrary NNLO. POWHEG matching. Event Generation for LHC CERN Theory Seminar 30/03/11. ... Cut now needed on ‘underlying Born’ pt of Z0• Good agreement with CDF (not so good with D0)• First jet is now NLO, second is LO (times

6 Dec 2023: r $ b; r $ g; b! g. SU(3)-colour symmetry is exact. ... r r. b b. Other configurations where quarks don’t change colour •Only matrices with non-zero entries in 11 and 33 position are involved.

23 Nov 2023: b bb. q qb. b. b. « Each jet will contain one b-hadron which will decay weakly« Because is small hadrons containing. ... fb. be–. e+. Z. Z f. fb. b. e. « The only way to distinguish.

8 Oct 2009: Black Holes at Colliders CERN 23/02/09. BH formation factor (1). b. ... Classical Limit. 20. pJ. bx. y. ). θ. ζ. p = ω(sin θ, 0, cos θ)b = b(cos θ sin ζ, cos ζ, sin θ sin ζ).

28 Jun 2011: b. b. soft gluon radiation? Supersymmetry as Lingua Franca. Some possibilities:. • ... Exercises Ma b. ( )yyxxbaba baba eemmM Δ++= )cosh(2222 η(1) Prove that.

30 Jan 2024: AµBµ = A.B = A0B0 A.B. or pµpµ = pµgµvp. v =µ=0,3. ... σ[60Ni(α,n)63Zn] σ[63Cu(p,n)63Zn]. n.b. common notation for nuclearreactions:aA bB A(a,b)B. Energy of p selected to give samec.m.

4 Nov 2023: i if Ai Bi = 11 otherwise. 9>=. >;(by (49)). = s(A, B)d1Y. ... X. X2A. (AX )1 Y (AX ). =X. X2AA. (X )1 Y (X ). =X. X2A. (X )1 Y (X ) (since A A {A B, B 2 A} = A). =

2 Jun 2014: tot. BR(X). BR(X)=. b. tot. = 0.56. b. b. (known to 4th order). ... b. ,b. b contributes less, so top mass effect is significant (-2%).

18 Jun 2012: a〉 |b〉 = |b〉 |a〉 (commutative law). • (|a〉 |b〉) |c〉 = |a〉 (|b〉) |c〉) (associative law). • ... a|b〉 = 〈b|a〉 (1.11). From the above, we can deduce that. (

21 Oct 2008: Z8V9?6A,B/Q MPW30QO.GG@O=;:IS'_OB4S[SV9J?]WM_!J/._Y[AC8"VZ']Z]KH__. ... S[WU-R9SMJS41F.7.-B/#OWTIGF0RLK@RQS2NS.%5,$U,AL1$ M-"ZXJ"NES$8N1JBXM2TP2#U#!GH.Y$M1DR5U:8)OJ[KP?,'TEAFI%!