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  2. HOMESITE HELPABOUTSEARCH…

    https://www.hep.phy.cam.ac.uk/theory/webber/asymf.pdf
    4 Dec 2008: Bryan Webber, Asymptotic Freedom, CPS, 3 Nov 2004 20. History of Asymptotic Freedom. ... 20. 50. 0. 30. 40. 60. 10 12 1614(E/GeV). 1α. log10.
  3. QCD Simulation for LHC and Herwig++ Bryan Webber University ...

    https://www.hep.phy.cam.ac.uk/theory/webber/kek04.pdf
    4 Dec 2008: Bryan Webber, QCD Simulation for LHC and Herwig++, KEK, 6 April 2004 20. ... 19.6. 19.8. 20. 20.2. 20.4. 20.6. 20.8. 21. 21.2. 21.4. 0 2 4 6 8 10 12.
  4. Particle Flow Calorimetry and ILC Detector Design

    https://www.hep.phy.cam.ac.uk/~thomson/talks/ILDOptimisation.pdf
    14 Jan 2008: Solenoid B-field 3.0 4.0 3.50 3.50. VTX Inner Layer (mm) 20 16 18 18. ... merging etc, walk before running…. ILD Meeting, DESY Zeuthen, 14/1/2008 Mark Thomson 20.
  5. Particle Flow Calorimetry and ILC Detector Design

    https://www.hep.phy.cam.ac.uk/~thomson/talks/CERN2008.pdf
    26 Sep 2008: V0s KinksProngs Backscatters. ii) ECAL/HCAL Clustering. CERN, 26/9/2008 Mark Thomson 20. ... 30 GeV π+. 20 GeV n. At some point reach the limit of “pure” particle flowi.e.
  6. QCD Phenomenology at High Energy Bryan Webber QCD Phenomenology ...

    https://www.hep.phy.cam.ac.uk/theory/webber/QCDlect5.pdf
    4 Dec 2008: 20. QCD Phenomenology at High Energy Bryan Webber. V Del Duca, S Frixione, C Oleari & BW, in prep. ... 30[GeV] νT]; E2 20[GeV/c WT M. Jets: |<2.0ηJetClu R=0.4; |hadron level; no UE correction.
  7. Particle Flow Calorimetry and ILC Detector Design

    https://www.hep.phy.cam.ac.uk/~thomson/talks/DESY2008.pdf
    7 Jul 2008: We already have a first version….(many vital contributions from DESY). DESY, 7/7/2008 Mark Thomson 20. ... e.g. if have 30 GeV track pointing to 20 GeV clusterSOMETHING IS WRONG.
  8. QCDlect1.dvi

    https://www.hep.phy.cam.ac.uk/theory/webber/QCDlect1.pdf
    4 Dec 2008: fixes c1. 20. Nowadays, most calculations are performed in modified minimal subtraction (MS). ... 20. 3CATF nf. β2 =2857. 54C. 3A 2C. 2F TF nf.
  9. https://www.hep.phy.cam.ac.uk/theory/webber/camjet/camjet.uu

    https://www.hep.phy.cam.ac.uk/theory/webber/camjet/camjet.uu
    21 Oct 2008: M["M;66&:Z.]H3O"'4EVY'$=B2Q&4FL5XP926$J2_P6=6#[.K#,%5C38 MCK&V8S2;23)01V6,B:G,#M,,8[B$!#M/IAM68H8KPH57&:R:(TU(Q ... I_I3!YH58CR MX#N72LH4_V[L)JS"SYE9[?1'?=)-%,-5%FR(HZD"NY%D93R'0]5TF2 MP=M.OA/SFOYSK&IWBK%E1:A4U5U'EW,MRNH_2U;4TJNU%&A:Q)-#20
  10. Particle Flow Calorimetry and ILC Detector Design

    https://www.hep.phy.cam.ac.uk/~thomson/talks/CLIC2008_Thomson.pdf
    15 Oct 2008: 500 GeV Jet. 500 GeV Jet. CLIC08, CERN, 15/10/2008 Mark Thomson 20.
  11. JHEP_005P_0608.dvi

    https://www.hep.phy.cam.ac.uk/theory/webber/MCatNLO/jhep072008029.pdf
    13 Nov 2008: Given that the computation of ref. [17] adopted the phase-space slicing method [18 – 20]. ... f (H1)a (x̄1f )f(H2)b (x̄2f ) dσ̂. (f1,l)i. MC. dx̄1f dx̄2f , (3.20).

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