Search

14 Nov 2009: M.A. Thomson. Nucl. Instr. Meth. A382 (1996) 553. Tests of Lepton University from Tau Decays at LEP (.ps).

8 Oct 2009: many models. We apply this technique to a test case with four extra dimensions and, using. ... temperature. We have applied this technique to our test case with four extra dimensions. –

28 Nov 2009: Dr M.A. Thomson Lent 2004. 22. Experimental Tests of QED. QED is an incredibly successful theory. ... Test Charge. At large R test chargesees screened e- charge. -. -. -. -. -. -. -.

8 Oct 2009: 7. 10-5. 10-4. 10-3. 10-2. 10-1. 1. Fraction of hard events failing IR safety test. ... The fraction of hard events failing the safety test is shown in fig.

28 Nov 2009: Dr M.A. Thomson Lent 2004. 9. Experimental Tests of the Standard Model. ... From 1989-2000 experimental measurements at CERNprovided precise tests of the Standard Model.

29 Sep 2009: Highly non-trivial test (of both computations) for shapes and rates! MTWW =. (ET ll /ET )2 (pT ll /pT )2 where ET ll =. p2T ll m. 2ll. and /ET. /p2T m2ll

28 Nov 2009: Bhabha scattering events. Data consistent with SM expectation Provides a direct test of vertex. ... Within the SM of Electroweak unification with the Higgs mechanism:. Precision Tests of the Standard Model.

14 Nov 2009: J. C17 (2000) 19-51. [131] “A Measurement of the τ Mass and the First CPT Test with τ Leptons”,OPAL Collaboration, G. ... 215] “Tests of the Standard Model and Constraints on New Physics from Measurements ofFermion-pair Production at 130-172 GeV

30 Sep 2009: Need a dedicated PFA test beam demonstration? [is this even possible?]. ... 1.141.00. e.g. Study suggests PandoraPFA is rather robust to hadronic modellingIf true, argues against need for dedicated PFA test beam demonstration.

28 Nov 2009: In the Standard Model, ONLY are independent. Their consistency is an incredibly powerful test ofthe Standard Model of Electroweak Interactions!

28 Nov 2009: also test universality of the WEAK interaction in -decays, e.g.

13 Oct 2009: Technologically feasible (although not cheap)Ongoing test beam studies (CALICE collaboration). Comments:.

15 Sep 2009: ξ p. ZEUSH1. DIS:BESTASSOMARK IITPCCELLOAMYALEPHDELPHIL3OPAL. ee:. MLLA QCD fitwithout coherence. Energy-dependence of the peak position ξp tests suppression of hadron production at small.

28 Nov 2009: Prof. M.A. Thomson Michaelmas 2009 271. Test QCD predictions by looking at production of pairs of high energy jets.

29 Sep 2009: Mass & Spin Determination KEK 18/09/2009. Bryan WebberCambridge University. 1. Determining Masses and Spins of New Particles(with missing energy). KEK seminar18 September 2009. Mass & Spin Determination KEK 18/09/2009. Outline. 2. Mass

28 Nov 2009: Consider a test particle near a mas-. sive source of bosons which mediate aforce.

28 Nov 2009: Neutrinos and Neutrino OscillationsHandout 12: The CKM Matrix and CP ViolationHandout 13: Electroweak Unification and the W and Z BosonsHandout 14: Tests of the Standard ModelHandout 15: The Higgs Boson and

16 Apr 2009: TILC09, Tsukuba, 17/04/2009 Mark Thomson 26. Determine BR(H bb), BR(H cc), BR(H gg) from Higgs-strahlung events Test of flavour tagging performanceCut based selections of three

28 Nov 2009: Particles/anti-particles have identical mass, lifetime, magnetic moments,…Best current experimental test:. Believe CPT has to hold:if CP invariance holds time reversal symmetryif CP is violated time reversal symmetry