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Test of QCD in 2-5 GeV with BESII
Z.G. Zhao 6/27/2002, PSI Test of QCD in 2-5 GeV with BESII W.B. Yan, Z.G. Zhao (Representing BES Collaboration) University of Michigan, Ann Arbor, MI, USA IHEP of CAS, Beijing, China Final Results of R-values in 2-5 GeV distribution, thrust and 2nd binomial moment e+e-(K)+X Summary ICHEP2002, Amsterdam Z.G. Zhao Z.G. Zhao
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Definition of R Experimentally R: one of the most
Z.G. Zhao 6/27/2002, PSI Definition of R R: one of the most fundamental quantities in particle physics, counts directly the number of quarks, their flavor and colors Experimentally Nhad: observed hadronic events Nbg: background events L: integrated luminosity had: detection efficiency for Nhad : radiative correction ICHEP2002, Amsterdam Z.G. Zhao Z.G. Zhao
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Motivations of the R Scan
Hunting for new physics from a(g-2)/2 Interpretation of E821 at BNL Reducing the uncertainty of (MZ2) essential for precision tests of the SM Relative contributions to the uncertainties of a and (MZ2) ICHEP2002, Amsterdam Z.G. Zhao
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BES’s R Scan Total 91 energy pts in 2-5 GeV Single and separated beam
collision to study beam associated background Special runs taken at J/, 2.6, 3.0, 3.5 GeV with larger data sample to determine trg L measured by large angle Bhabha LUARLW is developed to improve JETSET for had low energy region, particularly for Ecm< 3 GeV D, D*, Ds, Ds* productions are simulated according to Eichiten Model A generator is built into LUARLW to handle decays of resonances in the radiative return processes e+e- J/ or (2S) ICHEP2002, Amsterdam Z.G. Zhao
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Events Recorded by BESII
Events collected at BESII Data MC ICHEP2002, Amsterdam Z.G. Zhao
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Some Hadronic Event Shapes at Ecm=2.2 GeV (LUARLW)
Variation of Detection Efficiency and ISR in 2-5 GeV Tune the parameters to reproduce 14 distributions of the observed kinematic variables and hadronic event shape. Hatched region: MC Histogram: Data ICHEP2002, Amsterdam Z.G. Zhao
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R Values in 2-5 GeV ICHEP2002, Amsterdam Z.G. Zhao
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R Below 10 GeV Before BES R Scan After BES R Scan ICHEP2002, Amsterdam
Z.G. Zhao
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The SM Fit to mH (95% C.L.) (95% C.L.) With BES data Without BES data
ICHEP2002, Amsterdam Z.G. Zhao
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Evaluation of s and s(MZ) from R(BES)
R(pQCD) and R(BES) Exhibits QCD correction known to O(s3(s)) so far. Precision meas. of R can determine s and thus evaluate s(MZ). Using R at 3.0 and 4.8 GeV, one has: BES: PDG2000: D. Michel pQCD calculation agree amazingly well with BES data J.H. Kuhn, M.Rreinhauser Nucl. Phys. B619(2001)588 ICHEP2002, Amsterdam Z.G. Zhao
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Distribution: =-ln(2p/s)
MLLA/LPHD calculations Limiting spectrum when Q0=eff B=a/b, a=11Nc/3+2nf/3Nc2, b=(11Nc-2nf)/3 CF=(Nc2-1)/2Nc=4/3, Nc: quark flavor = 3 nf: # qark flavor produced IB: modified Bessel Function. = 0+ix, where tanh 0 =2 -1, =1-/ * MLLA/LPHD fit with BES data BES Preliminary ICHEP2002, Amsterdam Z.G. Zhao
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Multiplicity and Second Binomial Moment
Average multiplicity: NLO: BES Preliminary ICHEP2002, Amsterdam Z.G. Zhao
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Thrust and Mean Thrust Thrust: Mean thrust: 1-T Free para.
BES Preliminary A, B constant Free para. ICHEP2002, Amsterdam Z.G. Zhao
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Summary BES measured R in 2-5 GeV with average uncertainties of 6.6% (a factor of 2-3 improvement) significant impact on the SM fit: mHiggs moves up from 61 GeV to 90 GeV, up limit from 170 GeV to 210 GeV R scan data at continuum can be used to test QCD - Preliminary results of , T, and R2 are consistent with e+e-, ep and N data at high energy. - , T consistent with MLLA/LPHD predictions, but R2 differs to NLO calculation CLEOC and BESIII can provide more accurate data at continuum to test QCD at a few percent level. ICHEP2002, Amsterdam Z.G. Zhao
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[e+e-(K) + X] and Fragmentation Function, S/U Ratio
Dqh(x,s) [e+e-(K) + X] are also needed to help determine polarized parton density 0.15 0.20 0.25 0.30 0.35 0.40 0.45 K + p exp. n N exp. eN exp. 20.9 K * / r 20.9 K/ p BESII(3.0) preliminary S/U S/U: input parameters in hadron production generatorneeded for determining h ICHEP2002, Amsterdam Z.G. Zhao
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