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Particle Flow and ILC Detector Design
https://www.hep.phy.cam.ac.uk/~thomson/talks/LDC_thomson.pdf8 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. -
Particle Flow and ILC Detector Design
https://www.hep.phy.cam.ac.uk/~thomson/talks/GLD_LDC_thomson.pdf29 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. -
Neutrino Oscillations and the MINOS experiment
https://www.hep.phy.cam.ac.uk/~thomson/lectures/iss/iss2007_ew.pdf31 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. -
Neutrino Oscillations and the MINOS experiment
https://www.hep.phy.cam.ac.uk/~thomson/lectures/iss/iss2007_weak.pdf31 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. -
Particle Flow Calorimetry and ILC Detector Design
https://www.hep.phy.cam.ac.uk/~thomson/talks/EPS2007_Thomson.pdf18 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. -
Monte Carlo Methods 4 Bryan Webber Monte Carlo Methods ...
https://www.hep.phy.cam.ac.uk/theory/webber/MunichPDF/MClecture4.pdf21 Nov 2007: Rev. Lett. 84 (2000) 845. / GeV Z P0 20 40 60 80 100 120 140 160 180 200. -
Particle Flow Calorimetry at the ILCM. A. Thomson Cavendish ...
https://www.hep.phy.cam.ac.uk/~thomson/publications/hsw06.pdf16 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. -
Particle Flow Calorimetry and ILC Detector Design
https://www.hep.phy.cam.ac.uk/~thomson/talks/IoP2007_Thomson_ILC.pdf3 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. -
Particle Flow and ILC Detector Design
https://www.hep.phy.cam.ac.uk/~thomson/talks/Pandora_Paris2007.pdf3 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 -
Monte Carlo Methods 5 Bryan Webber Monte Carlo Methods ...
https://www.hep.phy.cam.ac.uk/theory/webber/MunichPDF/MClecture5.pdf22 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. -
Particle Flow Calorimetry and ILC Detector Design
https://www.hep.phy.cam.ac.uk/~thomson/talks/RALFinal.pdf10 Apr 2007: Look at jet energy resolution for Z uds events at• s = 200 GeV• s = 360 GeV. ... Use Mokka to generate Z uds events @ 200 GeV with differentECAL segmentation: 5x5, 10x10, 20x20 [mm2]. • -
Event Generator Physics 5 Bryan Webber Event Generator Physics ...
https://www.hep.phy.cam.ac.uk/theory/webber/MCnet/MClecture5.pdf19 Apr 2007: Jet Transverse Energy [GeV]0 50 100 150 200 250 300 350. -
Fran k G aede , LD C U K ...
https://www.hep.phy.cam.ac.uk/~thomson/meetings/ild/talks/gaede_ldc_framework.pdf21 Sep 2007: aede. , CH. EP. 200. 7, V. icto. ria, C. anad. ... CH. EP. 200. 7, V. icto. ria, C. anad. a S. -
CALICE-UK and ILD
https://www.hep.phy.cam.ac.uk/~thomson/meetings/ild/talks/watson_ILD_1.ppt21 Sep 2007: 100-200 GeV jets! Caveat : work in progress, things will change. ... 200 GeV. MPV = 3.4 keV. σ = 0.8 keV. Geant4 energy of simulated hits. -
Slide 1
https://www.hep.phy.cam.ac.uk/~thomson/meetings/ild/talks/CMB-GLDC-Cambs07.ppt21 Sep 2007: Silicone adhesive pads. 1mm diameter 200 microns high on 5mm pitch. -
Monte Carlo Methods 6 Bryan Webber Monte Carlo Methods ...
https://www.hep.phy.cam.ac.uk/theory/webber/MunichPDF/MClecture6.pdf11 Nov 2007: 100000. (a). 0. 200. 400. -2000 -1000 0 1000 2000. Constant 373.9. ... G. eV. )H. T. 150. 200. 250. 300. 350. 400. (GeV)PLM700 800 900 1000 1100 1200 1300. -
Neutrino Oscillations and the MINOS experiment
https://www.hep.phy.cam.ac.uk/~thomson/lectures/iss/iss2007_qcd_quarks.pdf30 Jul 2007: 1x10-15 m apart : 200 N (equivalent weight of small child). -
Neutrino Oscillations and the MINOS experiment
https://www.hep.phy.cam.ac.uk/~thomson/lectures/iss/iss2007_intro.pdf30 Jul 2007: 1 Widdecombe = 200 kg,but a little clumsy for particles, me= 3x10-31 kg. -
Event Generator Physics 4 Bryan Webber Event Generator Physics ...
https://www.hep.phy.cam.ac.uk/theory/webber/MCnet/MClecture4.pdf19 Apr 2007: Rev. Lett. 84 (2000) 845. / GeV Z P0 20 40 60 80 100 120 140 160 180 200. ... pW. p1st jet. [ GeV ] Wp0 20 40 60 80 100 120 140 160 180 200. [ -
Particle Flow Calorimetry and ILC Detector Design
https://www.hep.phy.cam.ac.uk/~thomson/meetings/ild/talks/ILDDetectorOptimisation.pdf21 Sep 2007: ILD-UK, Cambridge, 21/9/2007 Mark Thomson 13. ECAL Transverse Granularity• e.g. Z uds events @ 200 GeV with different. -
EUROPEAN ORGANIZATION FOR NUCLEAR RESEARCH OPAL PR 42420th July ...
https://www.hep.phy.cam.ac.uk/~thomson/publications/pr424.pdf25 Jul 2007: EUROPEAN ORGANIZATION FOR NUCLEAR RESEARCH. OPAL PR 42420th July 2007. Measurement of the ee WW. cross section and W decay branchingfractions at LEP. The OPAL Collaboration. Abstract. From a total data sample of 701.1 pb1 recorded with ee
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