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  2. I decided to write a program that would test ...

    https://www.hep.phy.cam.ac.uk/~lester/teaching/Computing2021/www.inference.phy.cam.ac.uk/teaching/comput/C++/i5.html
    22 Oct 2013: I decided to write a program that would test the user's ability at italian cooking Being new to computing this was great fun and learning how to use the "if"
  3. Mark Thomson University of Cambridge TDAQ Strategy for Phase ...

    https://www.hep.phy.cam.ac.uk/~thomson/talks/AUW_Stanford_Thomson.pdf
    4 Jan 2013: MuCTPi. New SW. CaloRODs. PhaseIITrig13Oct2011. L1Track. L1. MDT Trigger New for Phase I. ... New for Phase II. L0 L1L1A. MDT. DPS. L0A. LArTBB. FEx.
  4. Some ideas submitted for session 1 in Michaelmas 2013 ...

    https://www.hep.phy.cam.ac.uk/~lester/teaching/Computing2021/www.inference.phy.cam.ac.uk/teaching/comput/C++/ideas-Mich-2013.html
    22 Oct 2013: user their new favourite number A program to divide a product by a sum, or the reciprocal.
  5. Neutrino Oscillations and the MINOS experiment

    https://www.hep.phy.cam.ac.uk/~thomson/MPP/partIIIparticles/Handout_13_2011.ppt
    10 Sep 2013: The new diagram. interferes negatively with the above two diagrams fixing the unitarity problem. ... The new boson is associated with a new gauge symmetry similar to that.
  6. Part III Particle Physics: Interaction by Particle Exchange

    https://www.hep.phy.cam.ac.uk/~thomson/MPP/partIIIparticles/Handout_3_2011.ppt
    10 Sep 2013: If we are then presented with a new Feynman diagram. we don’t want to go through the full calculation again.
  7. LAr Event Reconstruction with the PANDORA Software Development Kit ...

    https://www.hep.phy.cam.ac.uk/~thomson/talks/LArReco_2012_11_28.pdf
    4 Jan 2013: Flexibility – moving from ILC to LAr reconstruction, involved almost no code changes (just new algortithms). ... 16. Remnant Consolidation Either use the remnant clusters to build new particles, or merge them into the existing particles.
  8. Mark Thomson University of Cambridge Level-0 / Level-1 Trigger ...

    https://www.hep.phy.cam.ac.uk/~thomson/talks/AUW_CERN_2012_Thomson.pdf
    4 Jan 2013:  Phase-2 will represent 90 % of all ATLAS data  We hope for new physics…  At this stage trigger needs flexibility  Strong desire to trigger on leptons at
  9. Neutrino Oscillations and the MINOS experiment

    https://www.hep.phy.cam.ac.uk/~thomson/MPP/partIIIparticles/Handout_10_2011.ppt
    10 Sep 2013: term to allow for parity violation. New structure function. For anti-neutrino scattering new structure function enters with opposite sign.
  10. Neutrino Oscillations and the MINOS experiment

    https://www.hep.phy.cam.ac.uk/~thomson/MPP/partIIIparticles/Handout_5_2011.ppt
    10 Sep 2013: spin-spin interaction. the new term:. The above differential cross-section depends on a single parameter.
  11. Neutrino Oscillations and the MINOS experiment

    https://www.hep.phy.cam.ac.uk/~thomson/MPP/partIIIparticles/Handout_6_2011.ppt
    10 Sep 2013: used in place of MX. For inelastic scattering introduce four new kinematic variables:. ... variables. are not independent. Can rewrite the new kinematic variables in terms of the squared.

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