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  2. Part II Particle Physics Home Page

    https://www.hep.phy.cam.ac.uk/~thomson/particles/
    14 Sep 2006: Lent Term 2004. For my new (2006-) Part III Major Option Course, follow thisExamples SheetPart II Examples Class.
  3. ATLAS SUSY Working Group: Rome Production

    https://www.hep.phy.cam.ac.uk/~lester/snaps/romeindex.html
    20 Jul 2006: Focus Point model (isasugra 7.71: m0=3550 GeV, m12 = 300 GeV, A0 = 0, tan beta = 10, sgn(mu) = ). DC1 bulk region model with new UE (isasugra 7.64: m0=100
  4. RomeSUSYWiki

    https://www.hep.phy.cam.ac.uk/~lester/snaps/RomeSUSYWiki.html
    20 Jul 2006: Lari. (5=) SU3 DC1 bulk region model with new UE (isasugra 7.64: m0=100 geV, m12 = 300 geV, A0 = -300 geV, tan beta = 6, sgn(mu) = ). 50k. 10K events corresponds
  5. PFA progress and strategy for the LDC concept

    https://www.hep.phy.cam.ac.uk/~thomson/talks/lcsws06PandoraPFA.pdf
    10 Apr 2006: associatedThen try to associate with hits in current layer (M pixel cut)If no association made form new Cluster+ tracks used to seed clusters. ... still a few features (i.e. does something silly)some problems with tracking photon ID is quite basic+ some
  6. gphoto2-fuse-fs

    https://www.hep.phy.cam.ac.uk/~lester/gphoto2-fuse-fs/
    27 Feb 2006: Philip's version looks easier to build than mine, and works with new version of gphoto2 etc which mine doesn't! :).
  7. Two Years Six Years What is WMAP trying to ...

    https://www.hep.phy.cam.ac.uk/~lester/dtm662/test-talk2.pdf
    15 Apr 2006: see four-fold degeneracy. Preliminarymu. mA. 6-D. Break higgs doublet universality.Gain two new parameters, mu and mA.
  8. Christopher Lester – University of Cambridge.Work in association with …

    https://www.hep.phy.cam.ac.uk/~lester/dtm662/test-talk3.pdf
    15 Apr 2006: mA. 6-D. Break higgs doublet universality.Gain two new parameters, mu and mA. ... 2) Understand them.Look for degeneracies.Resolve degeneracies if possible (new expt methods).
  9. Christopher Lester – University of Cambridge. Work in association ...

    https://www.hep.phy.cam.ac.uk/~lester/dtm662/test-talk3.ppt
    15 Apr 2006: 6-D. Break higgs doublet universality. Gain two new parameters, mu and mA. ... 2) Understand them. Look for degeneracies. Resolve degeneracies if possible (new expt methods).
  10. 14 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 ...

    https://www.hep.phy.cam.ac.uk/~lester/dtm662/jobs/page14.pdf
    30 May 2006: The main new contribution of this paper is to ourknowledge of what current constraints on mSUGRAmean for particle physics in a quantitative sense.
  11. PFA progress and strategy for the LDC concept

    https://www.hep.phy.cam.ac.uk/~thomson/talks/Cambridge06Plans.pdf
    6 Apr 2006: How frequent - format? Many people at this meeting Cambridge, some relatively newto the ILC framework, if someone starts working on a new topiccan make a big impact!
  12. PowerPoint Presentation

    https://www.hep.phy.cam.ac.uk/~lester/dtm662/TenMinutes-1a.ppt
    29 Jun 2006: No gauge coupling unification. Standard Model Bad. Standard Model Good. New Physics, e.g. ... 2017. Conclusions. Expect new particles, new physics and other discoveries at the LHC.
  13. Particle Flow and ILC Detector Design

    https://www.hep.phy.cam.ac.uk/~thomson/talks/HepForumRALFinal.pdf
    11 May 2006: Calorimeter ReconstructionHigh granularity calorimeters –very different from previous detectorsAs trad. calorimeters – not great“Tracking calorimeter” – requiresa new approach to ECAL/HCALreconstruction. ... Calorimetry at the ILC = HARDWARE
  14. PFA progress and strategy for the LDC concept

    https://www.hep.phy.cam.ac.uk/~thomson/talks/lcswSoftSimSummary.pdf
    10 Apr 2006: LCWS06 Bangalore 13/3/06 Mark Thomson 6. Another new example :DigiSimSee V.Zutshi’s talk. ... Reconstruction Software. Another new example :DigiSim. IVth Concept Reconstruction. Break even point.
  15. Particle Flow and ILC Detector Design

    https://www.hep.phy.cam.ac.uk/~thomson/talks/RHULFinal.pdf
    10 Apr 2006: Aim to give impression of the issues involved in this new type of“calorimetry”. ... Calorimetry at the ILC = HARDWARE SOFTWARE (new paradigm)Will be difficult to disentangle detector/algorithm….
  16. PFA progress and strategy for the LDC concept

    https://www.hep.phy.cam.ac.uk/~thomson/talks/CambridgePandoraPFA.pdf
    5 Apr 2006: Mark ThomsonUniversity of Cambridge. This Talk:. PhilosophyThe AlgorithmSome New ResultsConfusionConclusionsOutlook. Cambridge 5/4/06 Mark Thomson 2. ... layer (M pixel cut)If no association made form new Cluster+ tracks used to seed clusters.
  17. PowerPoint Presentation

    https://www.hep.phy.cam.ac.uk/~lester/dtm662/Lecture-6i.ppt
    28 Jun 2006: No gauge coupling unification. Standard Model Bad. Standard Model Good. New Physics, e.g. ... 2017. Conclusions. Expect new particles, new physics and other discoveries at the LHC.
  18. Neutralino Dark Matter Sabine Kraml, CERN

    https://www.hep.phy.cam.ac.uk/~lester/physics/OtherTalks/skraml_whepp.ppt
    7 Jan 2006: T-odd little Higgs, branons,. Q-balls, etc., etc. New Physics. WHEPP-9 Bhubaneswar. ... What if CP is violated? [we actually need new sources of CP violation.
  19. Particle Flow and ILC Detector Design

    https://www.hep.phy.cam.ac.uk/~thomson/talks/HSSW.pdf
    8 Sep 2006: HSSW FNAL 8/09/2006 Mark Thomson 14. Calorimeter ReconstructionHigh granularity calorimeters –very different from previous detectors“Tracking calorimeter” – requiresa new approach to ECAL/HCALreconstruction. ... Calorimetry at the ILC = HARDWARE
  20. Particle Flow and ILC Detector Design

    https://www.hep.phy.cam.ac.uk/~thomson/talks/ALCPG_Fermilab.pdf
    7 Dec 2006: Also issues with tracking which will improve with new full trackreconstruction (better track extrapolation will help). ... Calorimetry at the ILC = HARDWARE SOFTWARE (new paradigm)It is difficult to disentangle detector/algorithm….
  21. Full supersymmetry simulation for ATLAS in DC1

    https://www.hep.phy.cam.ac.uk/~lester/physics/CSC/DC1.pdf
    27 Nov 2006: This required setting (nonstandard) VarTag values to distinguish thevariables. Essentially all cuts were removed for hadronic τ’s; cuts using a new τ likelihood function weremade at the analysis stage. ... To suppress the large jet background a new

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