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https://www.hep.phy.cam.ac.uk/lhcb/docs/LHCb_technical_proposal.pdf29 Oct 2008: #"%$#&'"%() '. , -. 0/21354567198;:=<?>A@CBD@CE8F:. G H 8;>JIK/ LM8FN5>A@C4 OP@C:7:767N/2>MQR/S8;TVUXW Y[ZBD/]>A67 /]4_Uab@C><?>J/]1c67E6d@C4 e /28;ET5>J/] /24fUEg@K. Oh< ij6@k:8lUJ6@k4 8F45N mn8;>J/ op/]1c8qWrE. "tsvuwtyxS&w z{! uy|&}) ' ' ). s s. -
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https://www.hep.phy.cam.ac.uk/theory/webber/ukforum_webber.pdf4 Dec 2008: w2D 8 ;:6 24 C6A7 ;nF4E <844746 9D ;6E74474E8 2E6 2: ;1@G:7 m. -
Simulation of Old and New PhysicsBryan Webber, University of ...
https://www.hep.phy.cam.ac.uk/theory/webber/ParisNov06.pdf4 Dec 2008: mll/(mll)max = sin(θ/2). where. 24. Helicity dependenceProcess 1 (SUSY). Process 1 (UED, transverse Z: PT/PL = 2x). -
QCDlect4.dvi
https://www.hep.phy.cam.ac.uk/theory/webber/QCDlect4.pdf4 Dec 2008: 104. DATA. • 〈Qjet〉 = 6.4 GeV 〈Qjet〉 = 13.4 GeV 〈Qjet〉 = 24.0 GeV. ... Qjet〉 = 6.4 GeV 〈Qjet〉 = 13.4 GeV 〈Qjet〉 = 24.0 GeV222 〈Qjet〉 = 48.5 GeV. -
QCDlect3.dvi
https://www.hep.phy.cam.ac.uk/theory/webber/QCDlect3.pdf4 Dec 2008: 1 4t0/t t0/t. 24. Quark Sudakov form factor is then. q(t) exp". -
QCDlect2.dvi
https://www.hep.phy.cam.ac.uk/theory/webber/QCDlect2.pdf4 Dec 2008: q. Q2q ,. KQCD = 1 αS(µ. 2). πX. n2Cn. „. s. µ2. «. αS(µ2). π! n. 5. In MS scheme with scale µ =. s,. C2(1) =365. 24 11ζ(3) [11 ... Hence branching in plane of gluon polarization preferred. 24. Consider next g qq̄ branching: Vertex factor is. -
QCDlect1.dvi
https://www.hep.phy.cam.ac.uk/theory/webber/QCDlect1.pdf4 Dec 2008: excellent agreement. 24. History of Asymptotic Freedom. 1954 Yang & Mills study vector field theory with non-Abelian gauge invariance. ... 2N,. dabcdA dabcdA. NA=. N 2(N 2 36). 24,. dabcdF dabcdA. -
QCD Simulation for LHC and Herwig++ Bryan Webber University ...
https://www.hep.phy.cam.ac.uk/theory/webber/kek04.pdf4 Dec 2008: 2. 24. 3. Bryan Webber, QCD Simulation for LHC and Herwig++, KEK, 6 April 2004 15. ... DecayerAMEGIC Hw64Decayer. AMEGICInterface. AMEGIC++. Interfaced. Bryan Webber, QCD Simulation for LHC and Herwig++, KEK, 6 April 2004 24. -
Particle Flow Calorimetry and ILC Detector Design
https://www.hep.phy.cam.ac.uk/~thomson/talks/Thomson.pdf11 Sep 2008: EJETσE/E = α/Ejj|cosθ|<0.7. σE/Ej. 45 GeV 24.9 % 3.7 %. 100 GeV 30.7 % 3.1 %. 180 GeV 43.0 % 3.2 %. 250 GeV 52.2 % ... ILD Workshop, 11/9/2008 Mark Thomson 24. Conclusions. Over to you…. Particle Flow and ILD Detector Optimisation Studies. -
Particle Flow Calorimetry and ILC Detector Design
https://www.hep.phy.cam.ac.uk/~thomson/talks/DESY2008.pdf7 Jul 2008: gaps between Tungsten increase effective RMoliere)• Lateral segmentation: 1cm2 matched to RMoliere• Longitudinal segmentation: 30 layers (24 X0, 0.9λhad)• Typical resolution: σE/E = 0.15/E(GeV). ... From fully reconstructed LDC tracks identify:.
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