α S in e + e - collisions at LEP and JADE
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1 α S in e + e - collisions at LEP and JADE XXIII International Conference on High Energy Physics, Moscow 2006 Jochen Schieck submitted papers: 1. L3, Studies of Hadronic Event Structure in e+e- Annihilation from 30 GeV to 209 GeV with the L3 Detector, Phys. Rept. 399:71 (2004) 2. OPAL, Determination of α S Using Jet Rates at LEP with the OPAL Detector, EPJ C45: 547 (2006) 3. OPAL, Measurement of the Strong Coupling α S from Four-Jet Observables in e + e - Annihilation, accepted by EPJ C 4. JADE, Measurement of the Strong Coupling α S from Four-Jet Observables in e + e - Annihilation using JADE data, accepted by EPJ C 25 July 2006 alpha_s in e+e- collisions (LEP,JADE) - Jochen Schieck - MPI für Physik, Münche 1
2 e + e - Data Sample JADE LEP energy range [GeV] * events per energy point 1k 20k 1k-3k > 100k 0.5k 5k JADE (14-44 GeV) LEP (30-86; GeV) JADE (14-44 GeV): bb-events subtracted LEP I (91 GeV): no background * radiative return events assumes factorization gluon from photon production (Dasgupta, Salam : hep-ph/ ) LEP I.5 (> 130 GeV): radiative return events subtracted LEP II (>160 GeV): W + W - events subtracted 25 July 2006 alpha_s in e+e- collisions (LEP,JADE) - Jochen Schieck - MPI für Physik, Münche 2
3 Measurement of α S using Event Shapes size of α S proportional to the number of radiated gluons gluon radiation pictured by event shapes variables e.g. Thrust: T = max r n i i r r p n i r p i q q 1-T=0 q q g 1/3>1-T>0 1 dσ σ df data well described by MC event shapes observables used by L3: 1-T, C, B T, B W, y 23, M H (and D, mean only) L3 25 July 2006 alpha_s in e+e- collisions (LEP,JADE) - Jochen Schieck - MPI für Physik, Münche 3
4 Hadronization with Power Corrections determine 1 st moment of event shapes 1 dσ mean value F = F df σ df sample full region of phase space L3 ~α S 3 QCD predictions at parton level (NLO) apply hadronization correction Power Corrections: DMW approach, hadronization corrections described GeV with single parameter α 0 confidence level for common α 0 : 1% (stat. only) (DMW: theoretical uncertainty ~20%) α s = ±0.0045± α 0 = 0.478±0.054±0.024 (stat±systematic) 25 July 2006 alpha_s in e+e- collisions (LEP,JADE) - Jochen Schieck - MPI für Physik, Münche 4
5 Hadronizaton using Monte Carlo Models appy fit to event-shape distribution describe hadronization correction with Monte Carlo models resummed calculations (NLO+NLLA) QCD: χ 2 /d.o.f. = 17.9/15 (only part of the distribution fitted) L3 QCD fit Data const.: χ 2 /d.o.f.= 51.7/15 α s = ±0.0012± s=202 GeV (exp±theo) 25 July 2006 alpha_s in e+e- collisions (LEP,JADE) - Jochen Schieck - MPI für Physik, Münche 5
6 Measurement of α S using Jet Rates number of jets reflects strength of the strong coupling α S cluster particles according to jetfinder scheme: Cambridge Durham: y ij = 2 i 2 vis 2min( E E, E 2 j ) (1 combine particles with smallest y ij cosθ ) ij number of jets as a function of y cut number of events with a certain y July 2006 alpha_s in e+e- collisions (LEP,JADE) - Jochen Schieck - MPI für Physik, Münche 6
7 Measurement of α S using Jet Rates average jetrate N 1 ( ycut ) = nσ n( ycut ) σ tot differential 2-jet rate y 23 apply NLO+NLLA QCD calculations R 3 = α S A+ α S2 B+O(α S3 )+NLLA terms n GeV α s = ±0.0006±0.0012±0.0010± (stat±exp±had±theo) uncertainty dominated by theory 25 July 2006 alpha_s in e+e- collisions (LEP,JADE) - Jochen Schieck - MPI für Physik, Münche 7
8 Measurement of α S using Four-Jet Rate leading order prediction four-jet rate ~ α S 2 R 4 =α s 2 B + α s 3 C +NLLA terms reduced scale sensitvity: ΔR4 ( x μ ) α S ln x μ 3 scale variation natural scale x μ =1 close to minimum reduced scale senistivity α s = ±0.0003±0.0015±0.0011±0.0012± (stat±exp±had±theo±bmass) 25 July 2006 alpha_s in e+e- collisions (LEP,JADE) - Jochen Schieck - MPI für Physik, Münche 8
9 Measurement of α S using Four-Jet Rate resurrection of data taken with the JADE detector allows unique access to e + e - data taken at 14 GeV s 44 GeV more than 40k multihadronic events data well described by Monte Carlo models tuned at LEP 1 (OPAL) similar sensitivity to α S like LEP measurements 25 July 2006 alpha_s in e+e- collisions (LEP,JADE) - Jochen Schieck - MPI für Physik, Münche 9
10 Measurement of α S using Four-Jet Rate total. error stat. error α s = ±0.0004±0.0012±0.0024± (stat±exp±had±theo) 25 July 2006 alpha_s in e+e- collisions (LEP,JADE) - Jochen Schieck - MPI für Physik, Münche 10
11 Running of Strong Coupling α S JADE GeV OPAL GeV JADE+OPAL GeV 3.9/5 57% 6.4/12 90% 12.0/18 85% α S = ± constant α S χ 2 /d.o.f. χ 2 probability 7.0/5 22% 12.4/12 42% 149.5/18 9 x % α S = ± combination of α S values using description of LEP QCD WG JADE data alone return no significant proof for running of α S LEP alone consistent with being constant combination of LEP and JADE date confirms running of α S with high significance 25 July 2006 alpha_s in e+e- collisions (LEP,JADE) - Jochen Schieck - MPI für Physik, Münche 11
12 Measurement of α S using Event Shape Observables ~ α S 2 perturbative predictions for D-Parameter and T Minor only available in NLO no resummed calculation available data not well described increased scale sensitvity D-Par: α S = ±0.0014± T Min : α S = ±0.0016± (stat±syst.) 25 July 2006 alpha_s in e+e- collisions (LEP,JADE) - Jochen Schieck - MPI für Physik, Münche 12
13 Conclusion still ongoing QCD analysis at LEP all measurements return values of α S consistent with the current world average α S determined from the four-jet rate leads to smaller scale uncertainty LEP and JADE data combined confirm running of α S with high significance 25 July 2006 alpha_s in e+e- collisions (LEP,JADE) - Jochen Schieck - MPI für Physik, Münche 13
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