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pp2004_beyond.dvi
https://www.hep.phy.cam.ac.uk/~thomson/particles/lectures/pp2004_beyond.pdf6 Mar 2004: q. qg. b. b. W-. W+. t. t. Final State (top lifetime too short. ... e-. e+. H0. Z0Z0. b. b. f. f. Dr M.A. Thomson Lent 2004. -
The “Interesting system”
https://www.hep.phy.cam.ac.uk/~lester/tasi/TASI4-spin.ppt24 Apr 2012: NEAR”. “FAR”. “NEAR”. “FAR”. hep-ph/0605067. Instead, rely on b-tag. B. B. _. ... Instead, rely on b-tag. B. B. _. MBL+ and MBL- distributions. -
Schematic Prints
https://www.hep.phy.cam.ac.uk/~hommels/interlock/Pictures/Interlock_Schematic_1.0.pdf25 Feb 2013: 6. 7. 7. 8. 8. D D. C C. B B. -
��� ����� ��� � � � �� � ����������� ...
https://www.hep.phy.cam.ac.uk/theory/webber/cdf_2.pdf4 Dec 2008: "#$ %&('"#) ,. -. / 01 2. 3456 789;: <: =>?@ =. A @ B: =: <?C => <D BE<93. >F =@ <EG>? ... L U=SS= BL :UFN J= Ë:F QK. H9; JM y=P;F BA JM;F;; B= B=> BAMN?=MU= KKAP= B; KKÞ U IF :<A Q=M I<? -
Neutrino Oscillations and the MINOS experiment
https://www.hep.phy.cam.ac.uk/~thomson/MPP/partIIIparticles/Handout_14_2011.ppt10 Sep 2013: jets containing b quarks. H0. b. b. b. q. b. b. ... f. b. b. e. Example event:. Displaced vertex from b-decay. Combined LEP Results. -
Not examinable Not examinable H1 H2 H3 H4 H5 ...
https://www.hep.phy.cam.ac.uk/~lester/teaching/partIIIparticles/handouts2023/H8-appendices.pdf6 Dec 2023: e.g. : two possible exchanged gluons. bb. b b. e.g. : only one possible exchanged gluon. ... b b. gr. g r. 346 / 604. Not examinable. Not examinable. -
Particle Physics Part III Major Option 2008
https://www.hep.phy.cam.ac.uk/~thomson/MPP/partIIIparticles/Handout_8_2011.ppt10 Sep 2013: r. b. b. g. r. g. r. e.g. b. r. b. ... b. b. b. b. e.g. : only one possible exchanged gluon. -
pp2004_beyond.dvi
https://www.hep.phy.cam.ac.uk/~thomson/lectures/partIIparticles/pp2004_beyond.pdf28 Nov 2009: q. qg. b. b. W-. W+. t. t. Final State (top lifetime too short. ... e-. e+. H0. Z0Z0. b. b. f. f. Dr M.A. Thomson Lent 2004. -
Bryan Webber: Top Physics Simulations CERN Top Quark Institute ...
https://www.hep.phy.cam.ac.uk/theory/webber/WebberTopInst09.pdf8 Oct 2009: 200 400 600 800 1000 1200 1400. (p. b/b. in). T/d. ... GeV)T. P200 400 600 800 1000 1200 1400. (p. b/b. in). -
Neutrino Oscillations and the MINOS experiment
https://www.hep.phy.cam.ac.uk/~thomson/lectures/iss/iss2007_ew.pdf31 Jul 2007: e-. e+. H0. Z0Z0. b. b. q. q. Higgs couples to mass –so need to produce it from a massive particle decays tothe most massive particles allowed. ... e-. e+. H0. Z0Z0. b. b. q. q. Made on 30-A. -
Particle Flow and ILC Detector Design
https://www.hep.phy.cam.ac.uk/~thomson/talks/HepForumRALFinal.pdf11 May 2006: B = 2T B = 4T B = 6T. σE/E = α(E/GeV)B-FieldAll angles. ... iv) Iterative Reclustering. Current Performance (as of 6/5/06). e.g. B-Field. -
QCDlect1.dvi
https://www.hep.phy.cam.ac.uk/theory/webber/QCDlect1.pdf4 Dec 2008: 5. A, α p B, β δAB". gαβ (1 λ)pαpβ. p2 iε. #. ... in 1/ log(Q2/Λ2):. αS(Q) =1. b ln(Q2/Λ2). ". 1 b′. b. -
The GLD Concept
https://www.hep.phy.cam.ac.uk/~thomson/talks/Daegu2005.pdf11 Jul 2005: No! Things aren’t that simple…. Dense Jet: B=0. neutral. ve- ve. ... puri. ty. c. b. b). c (b bkgr). ECM = 91 GeV. -
Particle Flow Calorimetry and ILC Detector Design
https://www.hep.phy.cam.ac.uk/~thomson/talks/RALFinal.pdf10 Apr 2007: What is optimal detector size/B-field, etc. THIS IS HARD – BUT VERY IMPORTANT! ... Current Performance. Recent Detector Optimisation Studies. e.g. B-Field at 91.2 GeV. -
Particle Flow and ILC Detector Design
https://www.hep.phy.cam.ac.uk/~thomson/talks/ALCPG_Fermilab.pdf7 Dec 2006: Large detector – spatially separate particlesHigh B-field – separate charged/neutralsHigh granularity ECAL/HCAL – resolve particles. ... What is optimal detector size/B-field, etc. THIS IS HARD – BUT VERY IMPORTANT! -
H1 H2 H3 H4 H5 H6 H7 H8 H9 ...
https://www.hep.phy.cam.ac.uk/~lester/teaching/partIIIparticles/handouts2023/H8.pdf6 Dec 2023: r r. b b. Other configurations where quarks don’t change colour •Only matrices with non-zero entries in 11 and 33 position are involved. ... e.g. : two possible exchanged gluons. bb. b b. e.g. : only one possible exchanged gluon. -
Klein-Gordon Equation● The existence of plane waves φ(r, t) ...
https://www.hep.phy.cam.ac.uk/theory/webber/GFT/gft_handout2_06.pdf24 Nov 2005: p p. a. b. ’. b’. q=pb’ bp. Then (in Lorenz gauge) Aµ satisfies. ... p p. a. b. ’. b’. q=pb’ bp. Hence. |Mf i|2 =e2ae. -
ElectroWeak
https://www.hep.phy.cam.ac.uk/~thomson/lectures/partIIIparticles/Handout14_2009.pdf28 Nov 2009: b. b. One signature for a Higgs boson decay is the production of two b quarks. ... b bb. q qb. b. b. Each jet will contain one b-hadron which will decay weakly Because is small hadrons containing. -
Prof. M.A. Thomson Michaelmas 2011 243 Particle PhysicsMichaelmas…
https://www.hep.phy.cam.ac.uk/~thomson/partIIIparticles/handouts/Handout_8_2011.pdf2 Nov 2011: e.g. : only one possible exchanged gluon. b b. b b. ... b b. Configurations where quarks swap colours. gr. g r. Appendix E: Colour Potentials. -
9. The Weak Force - Particle and Nuclear Physics
https://www.hep.phy.cam.ac.uk/~chpotter/particleandnuclearphysics/Lecture_09_Weak.pdf11 Dec 2023: Bc J/ψeν̄e. W. b. Bc c̄. e. ν̄e. c. c̄ J/ψ. ... t̄. b. gW Vtb. between quarks differing by one family are “Cabibbo Suppressed”.
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