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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. -
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”. -
Is Top Asymmetry Just SM Physics? Bryan Webber, ETH, ...
https://www.hep.phy.cam.ac.uk/theory/webber/TopAsyZurich.pdf24 Jan 2013: K = B/B = 1 O(αS). arbitrary NNLO. POWHEG matchingdσMC = B (ΦB) dΦB. ... j. j. e-! 2b2jleptonMET. pT > 20 GeV/c , |η| < 2 (|η|b < 1). -
Estimating uncertainties in histograms filled from MarkovChains…
https://www.hep.phy.cam.ac.uk/~lester/2018_MCMC_Uncertainties_01.pdf29 Aug 2019: δrbπb: (. t(b))r= δrbπb. (58). Note that, for any B B matrix A:. ... t(b))b. (by (69)) (77). = πb 2((P P2 P3 PN. )t(b))b. -
Event Generation for LHC CERN Theory Seminar 30/03/11 Monte ...
https://www.hep.phy.cam.ac.uk/theory/webber/MCEGforLHC.pdf30 Mar 2011: K = B/B = 1 O(αS). arbitrary NNLO. POWHEG matching. Event Generation for LHC CERN Theory Seminar 30/03/11. ... Cut now needed on ‘underlying Born’ pt of Z0• Good agreement with CDF (not so good with D0)• First jet is now NLO, second is LO (times -
H1 H2 H3 H4 H5 H6 H7 H8 H9 ...
https://www.hep.phy.cam.ac.uk/~lester/teaching/partIIIparticles/handouts2023/H8-without-appendices.pdf6 Dec 2023: r $ b; r $ g; b! g. SU(3)-colour symmetry is exact. ... 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. -
Particle Physics Dr Lester Handout 14 : Precision Tests ...
https://www.hep.phy.cam.ac.uk/~lester/teaching/partIIIparticles/handouts2023/H14_Frankenstein.pdf23 Nov 2023: b bb. q qb. b. b. « Each jet will contain one b-hadron which will decay weakly« Because is small hadrons containing. ... fb. be–. e+. Z. Z f. fb. b. e. « The only way to distinguish. -
Black Holes at Colliders CERN 23/02/09 Phenomenology of Black ...
https://www.hep.phy.cam.ac.uk/theory/webber/BH_LHC2FC.pdf8 Oct 2009: Black Holes at Colliders CERN 23/02/09. BH formation factor (1). b. ... Classical Limit. 20. pJ. bx. y. ). θ. ζ. p = ω(sin θ, 0, cos θ)b = b(cos θ sin ζ, cos ζ, sin θ sin ζ). -
Microsoft PowerPoint - TASI13-e-masses
https://www.hep.phy.cam.ac.uk/~lester/TASI13-e-masses.pdf28 Jun 2011: b. b. soft gluon radiation? Supersymmetry as Lingua Franca. Some possibilities:. • ... Exercises Ma b. ( )yyxxbaba baba eemmM Δ++= )cosh(2222 η(1) Prove that. -
2. Kinematics, Decays and Reactions - Particle and Nuclear Physics
https://www.hep.phy.cam.ac.uk/~chpotter/particleandnuclearphysics/Lecture_02_KinematicsDecaysReactions.pdf30 Jan 2024: AµBµ = A.B = A0B0 A.B. or pµpµ = pµgµvp. v =µ=0,3. ... σ[60Ni(α,n)63Zn] σ[63Cu(p,n)63Zn]. n.b. common notation for nuclearreactions:aA bB A(a,b)B. Energy of p selected to give samec.m. -
Not examinable Not examinable H1 H2 H3 H4 H5 ...
https://www.hep.phy.cam.ac.uk/~lester/teaching/partIIIparticles/handouts2023/H2-appendices.pdf4 Nov 2023: i if Ai Bi = 11 otherwise. 9>=. >;(by (49)). = s(A, B)d1Y. ... X. X2A. (AX )1 Y (AX ). =X. X2AA. (X )1 Y (X ). =X. X2A. (X )1 Y (X ) (since A A {A B, B 2 A} = A). = -
SMparam.key
https://www.hep.phy.cam.ac.uk/theory/webber/SMparam.pdf2 Jun 2014: tot. BR(X). BR(X)=. b. tot. = 0.56. b. b. (known to 4th order). ... b. ,b. b contributes less, so top mass effect is significant (-2%). -
Preface In this course, we cover some more advanced ...
https://www.hep.phy.cam.ac.uk/theory/webber/tp2_06.pdf18 Jun 2012: a〉 |b〉 = |b〉 |a〉 (commutative law). • (|a〉 |b〉) |c〉 = |a〉 (|b〉) |c〉) (associative law). • ... a|b〉 = 〈b|a〉 (1.11). From the above, we can deduce that. ( -
https://www.hep.phy.cam.ac.uk/theory/webber/camjet/camjet.uu
https://www.hep.phy.cam.ac.uk/theory/webber/camjet/camjet.uu21 Oct 2008: Z8V9?6A,B/Q MPW30QO.GG@O=;:IS'_OB4S[SV9J?]WM_!J/._Y[AC8"VZ']Z]KH__. ... S[WU-R9SMJS41F.7.-B/#OWTIGF0RLK@RQS2NS.%5,$U,AL1$ M-"ZXJ"NES$8N1JBXM2TP2#U#!GH.Y$M1DR5U:8)OJ[KP?,'TEAFI%! -
Neutrino Oscillations and the MINOS experiment
https://www.hep.phy.cam.ac.uk/~thomson/lectures/iss/iss2007_intro.pdf30 Jul 2007: B. B throws a heavy balltowards A. B exerts forceon ball – ball exerts an equal and opposite force on B (N3) and B recoils (N2). ... A. B. A. B. B emits ball and A absorbs it. -
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. -
https://www.hep.phy.cam.ac.uk/~lester/dtm662/mt2/Releases/oxbridgekine…
https://www.hep.phy.cam.ac.uk/~lester/dtm662/mt2/Releases/oxbridgekinetics-0.6/configure19 Jul 2012: conf$$.file echo conf$$.file if ln -s conf$$.file conf$$ 2/dev/null; then # We could just check for DJGPP; but this test a) works b) is more generic # and -
2015 NEXT LECTURES Effective Field Theory Ben Gripaios Cavendish ...
https://www.hep.phy.cam.ac.uk/~gripaios/eft_lecture_notes.pdf4 Jan 2016: Either U(1)B or U(1)L symmetry, together with Lorentz invariance, preventsthe proton from decaying. ... is called an equivalence relation if (i) a a,. (ii) a b = b a, and (iii) a b and b c = a c. -
PowerPoint Presentation
https://www.hep.phy.cam.ac.uk/~lester/dtm662/TenMinutes-1a.ppt29 Jun 2006: Hadronic Jets,. B-jets (sometimes). Electrons, Positrons, Muons, Anti-Muons. Tau leptons (sometimes). ... b. b. soft gluon radiation? So main EASY signatures are:. Lots of missing energy. -
7. QCD - Particle and Nuclear Physics
https://www.hep.phy.cam.ac.uk/~chpotter/particleandnuclearphysics/Lecture_07_QCD.pdf9 Apr 2023: gluons do not have equal parts r, b, g, so carry colour (e.g. ... g. q. q. q. q. αs. αs. r. rb. b. b r̄ r b̄. -
8. Quark Model of Hadrons - Particle and Nuclear Physics
https://www.hep.phy.cam.ac.uk/~chpotter/particleandnuclearphysics/Lecture_08_QuarkModel.pdf26 Feb 2024: Examples:. Mesons(JP = 0. ): B(bū); B0(b̄d); B0s (b̄s); B. c (bc̄). ... m(s) = 510 MeV. )(m(t) = 175 GeV. m(b) = 4.5 GeV. -
Particle and Nuclear Physics Handout #3 Nuclear Physics Lent/Easter…
https://www.hep.phy.cam.ac.uk/~chpotter/particleandnuclearphysics/PNP_Handout3.pdf19 Feb 2024: m(A,Z) = Zmp (A Z)mn B. B = aV A aSA2/3 acZ. ... Prof. Tina Potter 13. Basic Nuclear Properties 20. Nuclear Size Mirror Nuclei115 B. -
11. The Top Quark and the Higgs Mechanism - Particle and Nuclear…
https://www.hep.phy.cam.ac.uk/~chpotter/particleandnuclearphysics/Lecture_11_TopHiggs.pdf11 Nov 2022: t. t̄. q̄. q. b̄. W. W. b. Final state W W bb̄. ... y = 125.09 GeV, |Hm. µ. τ b. W. Zt. SM Higgs boson. -
Neutrino Oscillations and the MINOS experiment
https://www.hep.phy.cam.ac.uk/~thomson/lectures/iss/iss2007_qcd_quarks.pdf30 Jul 2007: In ee- q q the photon carries no colour so onlyr r or b b or g g final states are allowed, e.g. ... 3rd Bottom b -1/3 4.5 GeV/c2. Down d. 3rd. 0.3 GeV/c2. -
NATURAL SCIENCES TRIPOS: Part III Experimental and Theoretical…
https://www.hep.phy.cam.ac.uk/~lester/teaching/partIIIparticles/exams/Major_Topic_Particle_Physics-2013.pdf20 Sep 2013: Their action on Bogus states is defined to be:. H|a,b,c〉=. b(b 1) a(a 1)|a 1,b,c〉V|a,b,c〉=. ... b(b 1) c(c 1)|a,b,c 1〉. You may assume that all Bogus multiplets are connected (i.e. -
Prof. M.A. Thomson Michaelmas 2009 243 Particle PhysicsMichaelmas…
https://www.hep.phy.cam.ac.uk/~thomson/lectures/partIIIparticles/Handout8_2009.pdf28 Nov 2009: e.g. : only one possible exchanged gluon. b b. b b. ... b b. Configurations where quarks swap colours. gr. g r. Appendix II: Colour Potentials. -
Particle Flow Calorimetry and ILC Detector Design
https://www.hep.phy.cam.ac.uk/~thomson/talks/CLIC09_Plenary_Detector_Thomson.pdf13 Oct 2009: Conclusions: Detector should be fairly large. Very high B-field is less important. ... particle flow calorimetry looks promisingArgument for very high B-field not that compelling. -
ElectroWeak
https://www.hep.phy.cam.ac.uk/~thomson/partIIIparticles/handouts/Handout_14_2011.pdf22 Nov 2011: b b b. q q b. b. b! Each jet will contain one b-hadron which will decay weakly! ... e–. e+! f. f b. b. e. Prof. M.A. Thomson Michaelmas 2011 522. -
16. Fission and Fusion - Particle and Nuclear Physics
https://www.hep.phy.cam.ac.uk/~chpotter/particleandnuclearphysics/Lecture_16_FissionFusion.pdf10 Feb 2024: SEMF B(A, Z) = aV A aSA2/3 acZ. 2. A1/3 aA. ... Z2. A1/3(1 ϵ. 2. 5). Change in Binding Energy: B = B(ϵ)B(0) = aCA2/3(Z2. -
Varipoint qxd
https://www.hep.phy.cam.ac.uk/~lester/pv/SOCEX_Instructions.pdf20 Feb 2017: 3. Join the top and bottom marks vertically(A-A) and the left and right marks horizontally(B-B). ... Cleaning and maintenanceN.B. Maintenance work must only be carried out by a competent person familiar withinstantaneous water heaters. -
H1 H2 H3 H4 H5 H6 H7 H8 H9 ...
https://www.hep.phy.cam.ac.uk/~lester/teaching/partIIIparticles/handouts2023/H2-without-appendices.pdf4 Nov 2023: 34) () [(E m)A = ( p)B]. ()h(E m)( p)A = ( p)2B. ... pEm B. B. 8B. or, equivalently, we could say u+ = u 2 span{u1, u2} and u = v 2 span{v1, v2} where:. -
Methods for non-iterative muon sagitta bias calculations Christopher…
https://www.hep.phy.cam.ac.uk/~lester/muon_sagitta_bias_5432.pdf21 Sep 2021: 3.6 Working towards those goal(s). To assist in the calculation of the variances needed by the above goal statements,we will create B dimensional vectors and B B dimensional ... Less obviously the filling time does not. 12. grow with B or (B B) since -
FRS_pubs_2017.dvi
https://www.hep.phy.cam.ac.uk/~gibson/pubs.pdf31 Aug 2017: Lett. B 772, 265 (2017). 32. “Study of J/ Production in Jets”R. ... Measurement of CP asymmetries in the decays B0 K0µµ and B+ Kµµ”R.
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