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Mark Thomson's Home Page
https://www.hep.phy.cam.ac.uk/~thomson/publications/pub.html14 Nov 2009: J. Phys. G: Nucl. Part. Phys. 24 (1998) 365. Measurement of the W Boson Mass and W. -
PFA progress and strategy for the LDC concept
https://www.hep.phy.cam.ac.uk/~thomson/talks/CambridgePandoraPFA.pdf5 Apr 2006: PFA performance much more complex than α/E. Cambridge 5/4/06 Mark Thomson 24. -
3. Colliders and Detectors - Particle and Nuclear Physics
https://www.hep.phy.cam.ac.uk/~chpotter/particleandnuclearphysics/Lecture_03_CollidersDetectors.pdf11 Nov 2022: 1.34:. 1.33:. 1.32:. 1.31:. 1.30:. 1.29:. 1.28:. 1.27:. 1.26:. 1.25:. 1.24:. ... 0.27:. 0.26:. 0.25:. 0.24:. 0.23:. 0.22:. 0.21:. 0.20:. 0.19:. 0.18:. 0.17:. -
Event Generator Physics 4 Bryan Webber Event Generator Physics ...
https://www.hep.phy.cam.ac.uk/theory/webber/MCnet/MClecture4.pdf19 Apr 2007: 11 -50.76 31.35 35.3 69.5 4.95 14 W+ 24 195 12 11 19 20 50.36 -31.10 -35.0 104.5 78.64. ... 23 9.40 65.65 13.2 67.8 4.95 26 W- -24 195 24 23 32 33 -9.37 -65.43 -13.1 106.4 82.28. -
Particle Flow Calorimetry and ILC Detector Design
https://www.hep.phy.cam.ac.uk/~thomson/talks/ILDOptimisation.pdf14 Jan 2008: LoI? Production. ILD Meeting, DESY Zeuthen, 14/1/2008 Mark Thomson 24. Where are we now? -
QCDlect3.dvi
https://www.hep.phy.cam.ac.uk/theory/webber/QCDlect3.pdf4 Dec 2008: 1 4t0/t t0/t. 24. Quark Sudakov form factor is then. q(t) exp". -
H1 H2 H3 H4 H5 H6 H7 H8 H9 ...
https://www.hep.phy.cam.ac.uk/~lester/teaching/partIIIparticles/handouts2023/H5.pdf25 Oct 2023: r) 0er/a. with a 0.24 fmCorresponds to a rms charge radiusrrms 0.8 fm.Although suggestive, does not implyproton is composite! -
https://www.hep.phy.cam.ac.uk/~lester/Grid/20080225a.txt
https://www.hep.phy.cam.ac.uk/~lester/Grid/20080225a.txt25 Feb 2008: UserAnalysis/cmt/requirements,v retrieving revision 1.62 diff -c -r1.62 requirements cmt/requirements 24 Apr 2007 20:42:07 -0000 1.62 --- cmt/requirements 25 Feb 2008 -
Neutrino Oscillations and the MINOS experiment
https://www.hep.phy.cam.ac.uk/~thomson/lectures/iss/iss2007_weak.pdf31 Jul 2007: θ. Above. Below. ν. νµ. ν frombelow. 24. Neutrino OscillationsSuppose νµ and ντ are not fundamental particlesAssume they are mixtures of two fundamentalneutrino states, ν1 and ν2 of mass m1 and -
Particle Flow and ILC Detector Design
https://www.hep.phy.cam.ac.uk/~thomson/talks/ALCPG_Fermilab.pdf7 Dec 2006: gaps between Tungsten increase effective RMoliere)• Lateral segmentation: 1cm2 matched to RMoliere• Longitudinal segmentation: 30 layers (24 X0, 0.9λhad)• Typical resolution: σE/E = 0.15/E(GeV). ... ALCPG Seminar, Fermilab 8/12/2006 Mark Thomson
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