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LArg 5% dead FEBs problem
https://www.hep.phy.cam.ac.uk/~lester/ATLAS/index.html10 Dec 2009: Furthermore, we found what may be a new diagnostic plot for MET which allows us to make an eta-phi map of the energy scale contributing to MET for the leading -
PandoraPFA
https://www.hep.phy.cam.ac.uk/~thomson/pandoraPFA/24 Nov 2009: A new implementation is under development. In the meantime, either use the stable tagged version or the development version below:. -
pp2004_beyond.dvi
https://www.hep.phy.cam.ac.uk/~thomson/lectures/partIIparticles/pp2004_beyond.pdf28 Nov 2009: By making precise measurements we are sensitive toparticles which are not being produced directly - thusplacing constraints on possible new particles/physicsbeyond the Standard Model. ... New acceleratorbased experiments coming online soon (e.g. -
pp2004_rqm.dvi
https://www.hep.phy.cam.ac.uk/~thomson/lectures/partIIparticles/pp2004_rqm.pdf28 Nov 2009: Since are matrices, need 2 componentwave-functions - WEYL SPINORS. The wave-function is forced to have a new degree offreedom - the spin of the fermion. -
ParticleExchange
https://www.hep.phy.cam.ac.uk/~thomson/lectures/partIIIparticles/Handout3_2009.pdf28 Nov 2009: If we are then presented with a new Feynman diagram we don’t want to go through the full calculation again. -
Particle Flow Calorimetry and ILC Detector Design
https://www.hep.phy.cam.ac.uk/~thomson/talks/PFA_Plenary_Thomson.pdf30 Sep 2009: PFA can achieve <4 % jet energy resolution for new particle decays• Gives few % mass resolution for new particle decays • Sufficient to separate W/Z for gauge bosons produced in association. ... Properly designed code Increased flexibility – needed -
WeakLeptons
https://www.hep.phy.cam.ac.uk/~thomson/lectures/partIIIparticles/Handout10_2009.pdf28 Nov 2009: term to allow for parity violation. New structure function. •For anti-neutrino scattering new structure function enters with opposite sign. -
ElectronProton
https://www.hep.phy.cam.ac.uk/~thomson/lectures/partIIIparticles/Handout5_2009.pdf28 Nov 2009: the new term:. Prof. M.A. Thomson Michaelmas 2009 165. •The above differential cross-section depends on a single parameter. -
pp2004_qcd.dvi
https://www.hep.phy.cam.ac.uk/~thomson/lectures/partIIparticles/pp2004_qcd.pdf28 Nov 2009: crease linearly with separa-tion. When. new pairs can becreated. -3. -2. -
Prof. M.A. Thomson Michaelmas 2009 451 Particle PhysicsMichaelmas…
https://www.hep.phy.cam.ac.uk/~thomson/lectures/partIIIparticles/Handout13_2009.pdf28 Nov 2009: 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 thatof electromagnetism : U(1)Y. -
Prof. M.A. Thomson Michaelmas 2009 175 Particle PhysicsMichaelmas…
https://www.hep.phy.cam.ac.uk/~thomson/lectures/partIIIparticles/Handout6_2009.pdf28 Nov 2009: For inelastic scattering introduce four new kinematic variables:. Define:Bjorken x (Lorentz Invariant). ... Relationships between Kinematic Variables. Prof. M.A. Thomson Michaelmas 2009 179. •Can rewrite the new kinematic variables in terms of the -
https://www.hep.phy.cam.ac.uk/~thomson/pandoraPFA/PandoraPFAProcessor.…
https://www.hep.phy.cam.ac.uk/~thomson/pandoraPFA/PandoraPFAProcessor.cc24 Nov 2009: coded numbers removed) // : handle new DHCAL // v03-00-01 : Count tail catcher hits separately in cluster energy by // subdetector counts // : Tidy up hit energy correction code and make more flexible // ... 00-00 : New fully ILD compatible version // : -
Publications List (Prof Mark Andrew Thomson) Publication List In ...
https://www.hep.phy.cam.ac.uk/~thomson/publications/publis.pdf14 Nov 2009: 79] “Decay-mode independent searches for new scalar bosons with the OPAL detector atLEP”,OPAL Collaboration, G. ... OPAL Collaboration, G. Abbiendi et al.,Phys. Lett. B476 (2000) 256-272. [143] “Search for New Physics in Rare B Decays”,OPAL -
https://www.hep.phy.cam.ac.uk/~thomson/pandoraPFA/ProtoCluster.cc
https://www.hep.phy.cam.ac.uk/~thomson/pandoraPFA/ProtoCluster.cc24 Nov 2009: float approach = genericDistanceToTrackSeed(_hitsByPseudoLayer[searchLayer][ihit],distance); if(approach1.)check = true; } } // New style tracking if(_trackingWeight==2){ if(searchLayer=2)check=true; for(int il = searchLayer-3; ilsearchLayer;il++){ -
Quarks
https://www.hep.phy.cam.ac.uk/~thomson/lectures/partIIIparticles/Handout7_2009.pdf28 Nov 2009: Now add an additional up or down quark. From each of the above 4 statesget two new isospin states with. -
Prof. M.A. Thomson Michaelmas 2009 243 Particle PhysicsMichaelmas…
https://www.hep.phy.cam.ac.uk/~thomson/lectures/partIIIparticles/Handout8_2009.pdf28 Nov 2009: Gluon Self-Interactions Two new vertices (no QED analogues). triple-gluonvertex quartic-gluonvertex. In addition to quark-quark scattering, therefore can have gluon-gluon scattering. -
Dirac
https://www.hep.phy.cam.ac.uk/~thomson/lectures/partIIIparticles/Handout2_2009.pdf28 Nov 2009: Introduce a new concept “HELICITY”. Helicity plays an important role in much that follows. ... Introduce a new 4x4 operator:. where are the Pauli spin matrices: i.e. -
pp2004_intro.dvi
https://www.hep.phy.cam.ac.uk/~thomson/lectures/partIIparticles/pp2004_intro.pdf28 Nov 2009: E-M s. WEAK s. Accelerator physics - particle scattering:Direct production of new massive particles in. -
ElectroWeak
https://www.hep.phy.cam.ac.uk/~thomson/lectures/partIIIparticles/Handout14_2009.pdf28 Nov 2009: ONLY 3 GENERATIONS (unless a new 4th generation neutrino has very large mass). -
NeutrinoOscillations
https://www.hep.phy.cam.ac.uk/~thomson/lectures/partIIIparticles/Handout11_2009.pdf28 Nov 2009: taking data: K2K, MINOS, CNGS, Project X• Opening up a new era in precision neutrino physics.
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