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31 Aug 2017: Lett. B 772, 265 (2017). 32. “Study of J/ Production in Jets”R. ... Measurement of CP asymmetries in the decays B0 K0µµ and B+ Kµµ”R.

24 Nov 2009: checks // : Clone shared photon track hits // : new photon recovery structure // : removed some obsolete and unhelpful code // 20/6/2007 : Add PerfectPFA // CVS1.6 : get B-field from global // : allow possibility of

13 Nov 2008: From table 1, we see that N = 2 for allbranchings in the processes with {b, q}, {b, b̄} and {b, b} initial states, and for branchingsfrom leg and leg in the ... q) (p̄1p̄2, p̄1k̄1)(b, b̄; t, W, b̄) (p̄1p̄2, p̄2k̄1)(b̄, b; t, W, b̄) (p̄1p̄2,

18 Jun 2012: THEORETICAL PHYSICS 1. B R Webber and W J Stirling. Michaelmas Term 2009. ... Another useful formula from vector analysis says:. (a b) = (a )b (b )a [a curl b] [b curl a].

28 Jun 2006: Hadronic Jets,. B-jets (sometimes). Electrons, Positrons, Muons, Anti-Muons. Tau leptons (sometimes). ... b. b. soft gluon radiation? So main EASY signatures are:. Lots of missing energy.

31 Jul 2021:  (26)and so we can quote the result of [3] in corollary 4.6, with the mapping pq a, Σ (abcd),a b, b c, c d. ... 3 (a,b,c) G(a,b,ca,b,c. )=. a a a b a cb a b b b cc a c b c c.

21 Oct 2014: b->neg = 1; mpadd(r, a, b); if(r! = b) b->neg = 0; return; } if(!a->neg && b->neg){ b->neg = 0; mpadd(r, a, b); if(r! = ... b) b->neg = 1; return; } if(a->neg && b->neg){ a->neg = b->neg = 0; mpsub(r, b, a); if(r! =

21 Sep 2007: full: MARLIN, SGV-input. Identical input events. c. c (b-bkgr). b. b. ... ee-  ZHH:. 4 b-jets in final state requiring. excellent tagging performance;.

19 Oct 2005: 0.1. 0 1. a) b). c) d). e) f). Theta_max. B B Dd+ -. s-s. - π π π π π. Acc. epta. nce. Figure The geometric acceptance as a ... BsBs mixing. The general formalismof B B mixinghas beendescribed many times and is reviewed in Ref Allowing for B!

19 Feb 2024: of magnitude.[ B+ (b̄u) and B0(b̄d) have masses of about 5280 MeV. ... b) Calculate the minimum energy of the ν which would permit e production.