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QCDlect1.dvi
https://www.hep.phy.cam.ac.uk/theory/webber/QCDlect1.pdf4 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. -
QCDlect3.dvi
https://www.hep.phy.cam.ac.uk/theory/webber/QCDlect3.pdf4 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. -
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https://www.hep.phy.cam.ac.uk/lhcb/docs/LHCb_technical_proposal.pdf29 Oct 2008: Sq H $#(w &y"w } 2tH &D4 B-B } 2tH &w%wt&'u. ... xK.ucw (! sv"8=ds-B-B-8&'u#xh+.144 s w64! udw H. -
• Spin correlations in SUSY and UED models • ...
https://www.hep.phy.cam.ac.uk/theory/webber/SSYvsUEDspins.pdf4 Dec 2008: 0.8. 0.9. 1. 0 0.2 0.4 0.6 0.8 1. cos! cos! ... b. in. SUSY. UED. PS. Data. 200 fb-1. S5. Figure 5: The points show the cos θll distribution for the S5 signal sample ("̃+"̃. -
JHEP_005P_0608.dvi
https://www.hep.phy.cam.ac.uk/theory/webber/MCatNLO/jhep072008029.pdf13 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,
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