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  2. Particle Flow and ILC Detector Design

    https://www.hep.phy.cam.ac.uk/~thomson/talks/LDC_thomson.pdf
    8 May 2007: s = 91 GeV. s = 360 GeV s = 200 GeV. ... ECAL Transverse Granularity• Use Mokka to generate Z uds events @ 200 GeV with different.
  3. Particle Flow and ILC Detector Design

    https://www.hep.phy.cam.ac.uk/~thomson/talks/GLD_LDC_thomson.pdf
    29 May 2007: rms90. For jet energies < 100 GeVILC goal reached! For jet energies 200 GeVclose to 40 %/E(GeV)! ... Typical 1 TeV ILC jet energies 50-200 GeV. There is no doubt in my mind that PFA can deliver therequired ILC jet energy performance.
  4. Neutrino Oscillations and the MINOS experiment

    https://www.hep.phy.cam.ac.uk/~thomson/lectures/iss/iss2007_ew.pdf
    31 Jul 2007: 6. 0. 5. 10. 15. 20. 25. 150 160 170 180 190 200 210. ... Signal. Combinatorial b/g. Other b/g. 0. 50. 100. 150. 200. 250.
  5. Neutrino Oscillations and the MINOS experiment

    https://www.hep.phy.cam.ac.uk/~thomson/lectures/iss/iss2007_weak.pdf
    31 Jul 2007: 1:1:3(universal force remember colour). 10. How Weak is Weak? EM Force between two electrons:1x10-15 m apart : 200 N (equivalent weight of small child). ... π+. • Horn pulsed with 200 kA • Toroidal Magnetic field B I/r between.
  6. Particle Flow Calorimetry and ILC Detector Design

    https://www.hep.phy.cam.ac.uk/~thomson/talks/EPS2007_Thomson.pdf
    18 Jul 2007: Ejj/GeV α(Ej)100 < 27 %. < 38 %200. Typical di-jet energies at ILC (100-300 GeV) suggests jet energy resolution goal of.
  7. Monte Carlo Methods 4 Bryan Webber Monte Carlo Methods ...

    https://www.hep.phy.cam.ac.uk/theory/webber/MunichPDF/MClecture4.pdf
    21 Nov 2007: Rev. Lett. 84 (2000) 845. / GeV Z P0 20 40 60 80 100 120 140 160 180 200.
  8. Particle Flow Calorimetry at the ILCM. A. Thomson Cavendish ...

    https://www.hep.phy.cam.ac.uk/~thomson/publications/hsw06.pdf
    16 Jan 2007: 0. 50. 100. 150. 200. 250. 300. 350. 400. 450. b) udsZ|<0.8θ|cos. ... For higher energies the performance degrades significantly reaching the equiv-alent of 0 6 E GeV for 200 GeV jets.
  9. Particle Flow Calorimetry and ILC Detector Design

    https://www.hep.phy.cam.ac.uk/~thomson/talks/IoP2007_Thomson_ILC.pdf
    3 Apr 2007: ILC : the machine Basic Machine Design Parameters. Centre-of-mass energy adjustable from 200-500 GeV• upgradeable to 1 TeV (i.e. ... ee- qq 0.1 /Bunch Trainee- γγ X 200 /Bunch Train. 500 hits/BX in Vertex det.5 tracks/BX in TPC.
  10. Particle Flow and ILC Detector Design

    https://www.hep.phy.cam.ac.uk/~thomson/talks/Pandora_Paris2007.pdf
    3 May 2007: rms90. For jet energies < 100 GeVILC goal reached! For jet energies 200 GeVclose to 40 %/E(GeV)! ... Radius more important athigher energies. B-field studies on the way…. ECAL Transverse Granularity• Use Mokka to generate Z uds events @ 200 GeV with
  11. Monte Carlo Methods 5 Bryan Webber Monte Carlo Methods ...

    https://www.hep.phy.cam.ac.uk/theory/webber/MunichPDF/MClecture5.pdf
    22 Nov 2007: 0 0.5. 1. 0 50 100 150 200 250 300 350 400. ... 0 0.5. 1. 0 50 100 150 200 250 300. d!/d.

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