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  2. Cambridge Jet Clustering Algorithm

    https://www.hep.phy.cam.ac.uk/theory/webber/camjet/
    12 Nov 2008: Note that for the LaTeX version you will need the class file JHEP.cls, which is the style for the new electronic journal JHEP.
  3. #Originally taken from…

    https://www.hep.phy.cam.ac.uk/~lester/Grid/job-to-data.html
    10 Apr 2008: #Originally taken from https://twiki.cern.ch/twiki/bin/view/Atlas/GangaTutorial427 #New page now at: https://twiki.cern.ch/twiki/bin/view/Atlas/GangaTutorial43 # In cambridge, just alias ganga to ... cam.ac.uk:2119/jobmanager-lcgc # 18 completed
  4. https://www.hep.phy.cam.ac.uk/~lester/Grid/20080225a.txt

    https://www.hep.phy.cam.ac.uk/~lester/Grid/20080225a.txt
    25 Feb 2008: aan_eta);! addBranch("ElectronPt", m_aan_pt);! addBranch("ElecPtRatio", m_aan_elecetres);! /// ROOT histograms ---------------------------------------! m_h_elecpt = new TH1F("elec_pt","pt el",50,0,250.GeV);! sc = ... AANT/Electron/elec_pt",m_h_elecpt); -
  5. SctRodDaq

    https://www.hep.phy.cam.ac.uk/~lester/SctRodDaq_ForPat.ppt
    23 Oct 2008: XML. Config. New XML. Config.
  6. SctRodDaq

    https://www.hep.phy.cam.ac.uk/~lester/SctRodDaq_ForPat.pdf
    23 Oct 2008: Link MaskingCalib Data. XMLConfig. New XMLConfig. SctRodDaq. The ASICs are called “ABCD”s.
  7. The beginning of physics

    https://www.hep.phy.cam.ac.uk/scatter/Resources/PU.ppt
    15 Dec 2008: Or there must be new physics. Supersymmetry is a favourite candidate for new physics (symmetry is good, more is better) but. ... Requires new particles to exist (Who ordered that?, Rabi). Properties must explain why they haven’t been observed already
  8. The CosmiX control panel

    https://www.hep.phy.cam.ac.uk/scatter/Resources/CosmiX/Cosmix.pdf
    14 May 2008: Start: Create new logging file and enable logging. Warning! An existing file of the same name will be overwritten. • ... This will cause problems as it is. incompatible with the new device drivers.
  9. Particle Flow Calorimetry and ILC Detector Design

    https://www.hep.phy.cam.ac.uk/~thomson/talks/Thomson.pdf
    11 Sep 2008: Understanding PFATry to use various “Perfect PFA” algorithms to pin down mainperformance drivers (resolution, confusion, …). Aim : understand main features of studies presented hereDeveloped new version of PandoraPerfectPFA.
  10. https://www.hep.phy.cam.ac.uk/theory/webber/camjet/hepph/JHEP.cls

    https://www.hep.phy.cam.ac.uk/theory/webber/camjet/hepph/JHEP.cls
    21 Oct 2008: special{psfile=logo.eps}hfil}}} %%%%%%%%%%%%%%%%%%%%%%%%%%%% NEW SWITCHES %%%%%%%%%%%%%%%%%%%%%%%%%%%%%% newifif@preprint@preprintfalse % DEFAULT IS PUBLISHED! ... letold@parparagraph % letold@sparsubparagraph % % ------- new forms ------- %
  11. QCDlect4.dvi

    https://www.hep.phy.cam.ac.uk/theory/webber/QCDlect4.pdf
    4 Dec 2008: Final State Relevance Progress? V V jet tt̄H, new physics V V = γγ, W W. ... V V V SUSY trilepton ZZZ. V V bb̄ VBF H V V , tt̄H, new physicsV V 2 jets VBF H V VV 3 jets various new physics signatures.
  12. HOMESITE HELPABOUTSEARCH…

    https://www.hep.phy.cam.ac.uk/theory/webber/asymf.pdf
    4 Dec 2008: In the early 1960’s, many new strongly-interacting particles (hadrons) were discovered, all apparently. ... quite implausible. until amazing experimental data started arriving from the new Stanford Linear.
  13. Particle Flow Calorimetry and ILC Detector Design

    https://www.hep.phy.cam.ac.uk/~thomson/talks/CLIC2008_Thomson.pdf
    15 Oct 2008: sounds easy….PFA performance depends on detailed reconstructionRelatively new, still developing ideasStudies need to be based on a sophisticated detector simulations. ... Requires new effort. CLIC08, CERN, 15/10/2008 Mark Thomson 33. End. CLIC08, CERN,
  14. Particle Flow Calorimetry and ILC Detector Design

    https://www.hep.phy.cam.ac.uk/~thomson/talks/CERN2008.pdf
    26 Sep 2008: New paradigm – nobody really knows how to approach this. So where are we now? ... needs detailed studyWill depend on physics program, e.g. lower energy operation (staged?) / threshold scanswhat matters at higher energies, W/Z separation or new.
  15. Particle Flow Calorimetry and ILC Detector Design

    https://www.hep.phy.cam.ac.uk/~thomson/talks/DESY2008.pdf
    7 Jul 2008: Limited by typical HCAL resolution of > 50%/E(GeV). a new approach to calorimetry. ... New paradigm – nobody really knows how to approach this. So where are we now?
  16. Long Baseline Neutrino Oscillation Experiments

    https://www.hep.phy.cam.ac.uk/~thomson/talks/PIC2008Thomson.pdf
    27 Jun 2008: Tota. l Pro. tons. (E20. ). First results (PRL)Prelim. NC. New PRL.
  17. Simulation of Old and New PhysicsBryan Webber, University of ...

    https://www.hep.phy.cam.ac.uk/theory/webber/ParisNov06.pdf
    4 Dec 2008: MultijetsImportant backgrounds to new physics. Only LO available up to high parton multiplicity(ALPGEN, AMEGIC++, MADGRAPH, HELAC,.). ... We present a new technique for measuring the temperature of black holes that applies to.
  18. Black Holes at the LHC?Bryan Webber, Cambridge Large Extra ...

    https://www.hep.phy.cam.ac.uk/theory/webber/BhamNov06.pdf
    4 Dec 2008: We present a new technique for measuring the temperature of black holes that applies to. ... discussed and a new technique has been introduced. This new technique has been shown.
  19. Particle Flow Calorimetry and ILC Detector Design

    https://www.hep.phy.cam.ac.uk/~thomson/talks/BonnFinal.pdf
    31 Jan 2008: Limited by typical HCAL resolution of > 50%/E(GeV). a new approach to calorimetry. ... New paradigm – nobody really knows how to approach this. So where are we now?
  20. QCD Simulation for LHC and Herwig++ Bryan Webber University ...

    https://www.hep.phy.cam.ac.uk/theory/webber/kek04.pdf
    4 Dec 2008: P. M/B W (ci,q′, dq′,j|i, j). New! Meson/Baryon ratio is parametrized in terms of. ... Underlying event.• Hadronic decays: NEW! τ –decays, spin correlations (P Richardson).• New ideas: NLO, multiscale, SUSY.
  21. QCDlect3.dvi

    https://www.hep.phy.cam.ac.uk/theory/webber/QCDlect3.pdf
    4 Dec 2008: Due to successive. branching, a parton cascade or shower develops. Each outgoing line is source of new.
  22. • Spin correlations in SUSY and UED models • ...

    https://www.hep.phy.cam.ac.uk/theory/webber/SSYvsUEDspins.pdf
    4 Dec 2008: χ̃01, χ̃02,. ). spins differ by one-half. UED: new particles are KK excitationsq q , g g , l l , (γ, Z,. ) ( ... We suppose that the new particle masses have beenmeasured, either by an edge analysis along the lines of refs.
  23. JHEP_005P_0608.dvi

    https://www.hep.phy.cam.ac.uk/theory/webber/MCatNLO/jhep072008029.pdf
    13 Nov 2008: therefore refrain from describing here the necessary steps for the implementation of a new. ... new computation is specifically required for W t production). In this section, we will limit.

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