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https://www.hep.phy.cam.ac.uk/~lester/Grid/20080225b.txt
https://www.hep.phy.cam.ac.uk/~lester/Grid/20080225b.txt25 Feb 2008: AnalysisSkeleton_topOptions.py 2008-02-25 11:24:24.000000000 0000 --- AnalysisSkeleton_topOptions_cowden.py 2008-02-25 11:23:27.000000000 0000 29,41 CBNT_AthenaAware = AnalysisSkeleton() ############# The properties of -
https://www.hep.phy.cam.ac.uk/~lester/Grid/20080225a.txt
https://www.hep.phy.cam.ac.uk/~lester/Grid/20080225a.txt25 Feb 2008: UserAnalysis/cmt/requirements,v retrieving revision 1.62 diff -c -r1.62 requirements cmt/requirements 24 Apr 2007 20:42:07 -0000 1.62 --- cmt/requirements 25 Feb 2008 -
1 2 3 4 5 6 7 8 9 ...
https://www.hep.phy.cam.ac.uk/history/ua2/MPI-PhE-94-04.pdf26 Nov 2008: 23. 24. 25. 26. 27. 28. 29. 30. 31. 32. 33. -
1 2 3 4 5 6 7 8 9 ...
https://www.hep.phy.cam.ac.uk/intranet/history/ua2/MPI-PhE-94-04.pdf26 Nov 2008: 23. 24. 25. 26. 27. 28. 29. 30. 31. 32. 33. -
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. -
Long Baseline Neutrino Oscillation Experiments
https://www.hep.phy.cam.ac.uk/~thomson/talks/PIC2008Thomson.pdf27 Jun 2008: Physics in Collision, 27/6/2008 Mark Thomson 24. CNGS - OPERACERN to Gran Sasso Neutrino Beam:. -
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:. -
Particle Flow Calorimetry and ILC Detector Design
https://www.hep.phy.cam.ac.uk/~thomson/talks/ILDOptimisation.pdf14 Jan 2008: LoI? Production. ILD Meeting, DESY Zeuthen, 14/1/2008 Mark Thomson 24. Where are we now? -
Particle Flow Calorimetry and ILC Detector Design
https://www.hep.phy.cam.ac.uk/~thomson/talks/CLIC2008_Thomson.pdf15 Oct 2008: A few comments:. CLIC08, CERN, 15/10/2008 Mark Thomson 24. Study Z mass resolution as function of EZwith ILD detector (TPC based, B=3.5 T, 6 λI HCAL). -
Particle Flow Calorimetry and ILC Detector Design
https://www.hep.phy.cam.ac.uk/~thomson/talks/CERN2008.pdf26 Sep 2008: The ONLY(?) way to addressthis is “statistically”. CERN, 26/9/2008 Mark Thomson 24. -
Particle Flow Calorimetry and ILC Detector Design
https://www.hep.phy.cam.ac.uk/~thomson/talks/BonnFinal.pdf31 Jan 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). ... Nightmare from point of view of detector -
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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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