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  2. Cavendish - Teaching - Part II Experimental and Theoretical Physics

    https://www.hep.phy.cam.ac.uk/~thomson/particles/synopsis.html
    23 Jan 2002: The weak neutral current. The Z. 0 resonance. Precision tests of the Standard Model at the Large Electron Positron collider (LEP).
  3. Particle Flow Calorimetry and ILC Detector Design

    https://www.hep.phy.cam.ac.uk/~thomson/talks/Thomson.pdf
    11 Sep 2008: Test Change ParametersB and R Model= SiD-like small LDC LDCPrime GLDB-field B = 2.5 T 3.0 T 3.5 T 4.0 T 4.5 T.
  4. Risk Assessment Hamamatsu PLP-10-040C risk assessment 1 Background…

    https://www.hep.phy.cam.ac.uk/intranet/laser_safety/Room880LaserRiskAssessment.pdf
    30 Mar 2020: The beam exits the fibre where it is used to illuminate the device under test either directly or by diffuse reflection.
  5. Bookmarks for Christopher Lester

    https://www.hep.phy.cam.ac.uk/~lester/dtm662/bookmarks.html
    17 Apr 2000: Bookmarks for Christopher Lester. g" ADD_DATE="955814526" LAST_VISIT="955814685" LAST_MODIFIED="955814506">Search Category -. Newspapers. Reference. X11. SRT. ATLAS Offline Computing - Deliverable ATL-SW-SRT-Documentation-V1. Information for Junior
  6. 2 GENERAL Classic Slimline FF - Installation & Servicing ...

    https://www.hep.phy.cam.ac.uk/~lester/pv/157020.pdf
    13 Jul 2012: The value is used in the UK Government's Standard Assessment Procedure (SAP) for energy rating of dwellings.The test data from which it has been calculated have been certified by ... A test cock. A double check valve of an approved type. •
  7. DAQ Online Software Migration

    https://www.hep.phy.cam.ac.uk/~lester/dtm662/December-OmniMigration-1.ppt
    14 Dec 2004: But:. Awaiting stress test with more than 3-4 modules when Barrel Sector becomes available in early January 2005. ... Few people seem desperate to test our code! Testing cont …. Cambridge:. On three modules, 4.xx can do all that 3.01 can.
  8. Particle Flow Calorimetry and ILC Detector Design

    https://www.hep.phy.cam.ac.uk/~thomson/talks/CERN2008.pdf
    26 Sep 2008: Technologically feasible (although not cheap)Ongoing test beam studies (CALICE collaboration). Comments:. ... CERN, 26/9/2008 Mark Thomson 28. Current performance. Benchmark performance using and events (clean, no neutrinos)Test at for different energies
  9. 7. QCD - Particle and Nuclear Physics

    https://www.hep.phy.cam.ac.uk/~chpotter/particleandnuclearphysics/Lecture_07_QCD.pdf
    9 Apr 2023: QCD potential, confinement. Hadronisation, jets. Running of αsExperimental tests of QCD. ... Tests of QCD. Evidence for colourExistence of gluons, test of their spin and self-interactionsMeasurement of αs and observation that it runs.
  10. Update on MINOS and Overview of Caltech’s Role

    https://www.hep.phy.cam.ac.uk/~thomson/meetings/offaxis/talks/Michael.ppt
    12 Jan 2004: Tests of intrinsic noise levels combined with electronics. Broaden use experience with our systems. ... Test by construction of a small surface array (recall that the beam duty factor is 10-5).
  11. QCDlect4.dvi

    https://www.hep.phy.cam.ac.uk/theory/webber/QCDlect4.pdf
    4 Dec 2008: ξ p. ZEUSH1. DIS:BESTASSOMARK IITPCCELLOAMYALEPHDELPHIL3OPAL. ee:. MLLA QCD fitwithout coherence. Energy-dependence of the peak position ξp tests suppression of hadron production at small.
  12. Neutralino Dark Matter Sabine Kraml, CERN

    https://www.hep.phy.cam.ac.uk/~lester/physics/OtherTalks/skraml_whepp.ppt
    7 Jan 2006: WMAP: 0.094 < Wh2 < 0.129 @ 2s. WHEPP-9 Bhubaneswar. Collider tests of WIMPs. ... Very hard to test at colliders. Astrophysics constraints? WHEPP-9 Bhubaneswar. Solution 3:.
  13. Future Initiatives

    https://www.hep.phy.cam.ac.uk/~thomson/meetings/offaxis/talks/Wojcicki_costs.ppt
    12 Jan 2004: Next year will be focused on R&D and cosmic ray test. ... FNAL. NSF. R&D: Year 1. Test beam prototype. Cosmic ray test.
  14. Black Holes at Colliders CERN 23/02/09 Phenomenology of Black ...

    https://www.hep.phy.cam.ac.uk/theory/webber/BH_LHC2FC.pdf
    8 Oct 2009: many models. We apply this technique to a test case with four extra dimensions and, using. ... temperature. We have applied this technique to our test case with four extra dimensions. –
  15. IOP HEPP 2009 LHC Phenomenology Phenomenology for LHC: A ...

    https://www.hep.phy.cam.ac.uk/theory/webber/BWIoPHEPP09.pdf
    8 Oct 2009: 7. 10-5. 10-4. 10-3. 10-2. 10-1. 1. Fraction of hard events failing IR safety test. ... The fraction of hard events failing the safety test is shown in fig.
  16. H1 H2 H3 H4 H5 H6 H7 H8 H9 ...

    https://www.hep.phy.cam.ac.uk/~lester/teaching/partIIIparticles/handouts2023/H3.pdf
    20 Oct 2023: H14: Precision Tests of the Standard Model. References.
  17. The Tesla Detector

    https://www.hep.phy.cam.ac.uk/~thomson/talks/Paris2005.pdf
    13 Jan 2005: Want to test gHffmfO(%) measurements of thebranching ratios H bb,cc,gg. Important for many physics analysese.g.
  18. Investigating non-standard sources of parity violation at the LHC ...

    https://www.hep.phy.cam.ac.uk/~lester/teaching/PartIIIProjects/2021-RadhaMastandrea.pdf
    4 Feb 2024: sector. We then test the parity variables on two mSME-motivated collider simulations, but do. ... which to test them. For the remainder of this report, we will focus on quark-sector physics.
  19. pp2004_ew.dvi

    https://www.hep.phy.cam.ac.uk/~thomson/particles/lectures/pp2004_ew.pdf
    28 Feb 2004: Dr M.A. Thomson Lent 2004. 9. Experimental Tests of the Standard Model. ... From 1989-2000 experimental measurements at CERNprovided precise tests of the Standard Model.
  20. Microsoft PowerPoint - Amsterdam2003Final

    https://www.hep.phy.cam.ac.uk/~thomson/talks/Amsterdam2003.pdf
    13 Jun 2003: TDR approach. do. Quark-Flavour Identification. Want to test gHffmfO(%) measurements of thebranching ratios Hbb,cc,gg.
  21. Theoretical Background for “Higgs Simulator” Namu Kroupa December 16, …

    https://www.hep.phy.cam.ac.uk/~lester/higgs-simulator/Theoretical_Background.pdf
    16 Dec 2021: φ0 is the massless (“test”) field interacting with the Higgs field, φ2, as in Section (2.4). ... 6. The test field, φ0, thus acquires mass by interaction with the Higgs field.

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