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Experimental Review of Unpolarised Structure Functions

Experimental Review of Unpolarised Structure Functions. SF and parton densities A few historical remarks Recent JLAB and NuTeV results HERA results: F 2 , gluon,  s , jets, F 2 cc , F 2 bb , F L , NC&CC at high Q 2 , xF 3 , pdf First results from HERA II Summary.

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Experimental Review of Unpolarised Structure Functions

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  1. Experimental Review of Unpolarised Structure Functions • SF and parton densities • A few historical remarks • Recent JLAB and NuTeV results • HERA results: • F2, gluon, s, jets, F2cc, F2bb, FL , • NC&CC at high Q2, xF3 , • pdf • First results from HERA II • Summary Vladimir Chekelian (MPI for Physics, Munich) V. Chekelian, Unpolarised SF

  2. Unpolarised SF and Parton Densities DIS DIS cross section and SF in QPM: QCD evolution (NLO, NNLO) DGLAP BFKL, CCFM Factorisation ^ s - perturbative QCD cross section pdf - universal parton distribution functions V. Chekelian, Unpolarised SF

  3. SF: a few Historical Remarks 1969SLAC-MIT observation that the proton SF is independent of Q2 at fixed Bjorken x  Bjorken scaling QPM 1974 - … SLAC, EMC, BCDMS, NMC, CDHS, CHARM, CCFR, … logarithmic Q2 dependence of F2(x,Q2) established in e//N scattering experiments  scaling violations QCD V. Chekelian, Unpolarised SF

  4. 2004 Nobel Prize in Physics for the Discovery of Asymptotic FreedomDavid Gross, David Politzer, Frank Wilczek Selected Publications of Frank Wilczek, with Brief Commentary http://web.mit.edu/physics/facultyandstaff/faculty_documents/wilczek_select_pubs.pdf QCD: Foundational Papers … in the fifth and sixth papers further experimental consequences, regarding the pointwise evolution of structure functions, were derived. The most dramatic of these, that proton viewed at ever higher resolution would appear more and more as field energy (soft glue), was only clearly verified at HERA twenty years later. … V. Chekelian, Unpolarised SF

  5. Rise of F2 to Low x at HERA 1992 the first HERA data: - discovery of the F2 rise at low x driven by gluon ! can not rise forever search for new gluon dynamics (saturation effects, …) after 12 years of HERA: precise data allowing to look for smallest deviations 2004 V. Chekelian, Unpolarised SF

  6. Kinematic Reach in Q2 and x full HERA x range is needed for LHC LHC TeVatron HERA fixed target experiments SLAC,BCDMS,NMC,E665, … V. Chekelian, Unpolarised SF

  7. FT and FLin Resonance Region (JLAB E94-110 ) 1 < W < 2 GeV FT FL Quark-hadron duality works well for both FT and FL above Q2 ~ 1.5 GeV2 V. Chekelian, Unpolarised SF

  8. Recent NuTeV Results F2 xF3 -Fe - extended to high y (low x) - most precise measurements of this kind - half of syst.err. of CCFR Strange Sea Asymmetry vs. the “NuTeV Anomaly”:  see talk of S. Forte V. Chekelian, Unpolarised SF

  9. F2(x,Q2) Measurements at HERA precision data 2-3% 5 decades in x 5 decades in Q2 rich possibilities to determine pdfs, test QCD, transition to p, search for saturation effects, … V. Chekelian, Unpolarised SF

  10. Low x at HERA locally from fit  = 0.08  constant at fixed Q2 (x < 0.01) (Q2) depends linearly on ln(Q2)  agrees with QCD for Q2  2 GeV2  change of behavior at Q2  1 GeV2  soft pomeron limit  = 0.08 (DL) no taming of the rise of F2 towards low x for Q2  0.5 GeV2 V. Chekelian, Unpolarised SF

  11. Scaling Violations at Low x continuous rise towards low x consistent with QCD fit (Q2  3 GeV2) no evidence for new gluon dynamics V. Chekelian, Unpolarised SF

  12. Gluon Density from HERA NLO QCD Fits ZEUS inclusive DIS & jets H1 inclusive DIS Gluonscaling violations pin down the gluon alows to resolve correlation of charm treatment important at Q2 ~ 1 GeV2 the gluon distribution becomes very small  xg is NOT an observable Gluon jets, heavy flavours, FL(x,Q2) directly sensitive to xg V. Chekelian, Unpolarised SF

  13. Strong Coupling from HERA NLO QCD Fits and Jets From scaling violations: Jets - small exper. error ~1% - theory error in NNLO expected to be 3 times smaller V. Chekelian, Unpolarised SF

  14. Charm Structure Function F2cc(x,Q2) charm contribution up to 25-30% consistent with with gluon from scaling violations V. Chekelian, Unpolarised SF

  15. Beauty Structure Function F2bb(x,Q2) • long lifetimes of b,c hadrons • use all tracks with pt>500 MeV • and hits in the H1 silicon tracker • jet gives b-direction b c u,d,s Contribution to total  significance S=  /()  - track impact parameter in r- F2bb - for the first time beauty contribution is ~ 3% consistent with with QCD calculations V. Chekelian, Unpolarised SF

  16. Determination of FL(x,Q2) by H1 direct FL measurements still to be done at HERA  low beam energy running V. Chekelian, Unpolarised SF

  17. NC and CC at High Q2 e±p quarks are pointlike down to proton radius/1000 r < 10-18 m NCCC at Q2 MZ2,MW2 unification of electromagnetic weak interactions Neutral Current Charged Current high Q2 -> high x provide possibility to unfold different quark flavours V. Chekelian, Unpolarised SF

  18. Structure Function xF3 at HERA reduced NC cross section: e- e+ xF3 constrains uv,dv at high x V. Chekelian, Unpolarised SF

  19. Charged Currents - reduced CC cross section The CC e+p cross section - dominated by d quark The CC e-p cross section - dominated by u quark CC e+p (e-p) cross sections are suited for constraining d (u) quark density e-p e+p V. Chekelian, Unpolarised SF

  20. PDFs from HERA Parton distributions unfolded using HERA NC and CC data only Gluon and sea are devided by 20 • - H1 and ZEUS parton distributions are in agreement • Treatment of systematics, parameterisations forms • and other details are subject to conventions - HERA QCD fits agree with the global fits H1 ZEUS V. Chekelian, Unpolarised SF

  21. First Results from HERA II detector and luminosity upgrade - efficient data taking since 2003 - O(1fb-1) till 2007 longitudinally polarised e beam H1 Ee=27.6 GeV Ep=920 GeV s = 319 GeV typically Pe~50% rise-time ~22min ZEUS Spin Rotators for the 3 IR’s e beam naturally transversely polarized (Sokolov-Ternov effect) V. Chekelian, Unpolarised SF

  22. CCusing Longitudinally Polarised e+ Polarisation dependence is firmly established HERA II Pe= 33% HERA I Pe= 0 Linear fit sCC= a+b(1+Pe) HERA II Pe= - 40% consistent with - linear (1+Pe) dependence - intercept of 0 after shutdown fall 2004  e- running extrapolation to Pe=-1 tests the absence of right-handed current V. Chekelian, Unpolarised SF

  23. Summary for more than 30 years SF provide a crucial experimental input to establish QPM, QCD and to determine pdfs still very active area: NuTeV, JLAB, … HERA II ~ O(1fb-1) till 2007, low energy running for FL new level of precision (exp. ~1%, theory NNLO) allows - to investigate applicability domains for different QCD evolutions - to understand high density (low x) QCD - to provide information essential for future LHC collider see HERA-LHC workshop: http://www.desy.de/~heralhc/ large potential for the long term future - HERA III (ed, …), eRHIC, e(ILC)p(HERA,TeVatron) V. Chekelian, Unpolarised SF

  24. Strange Sea Asymmetry Results from NuTeV the “NuTeV Anomaly” a 3.1  discrepancy: NuTeV sin2W=0.22770.0016 LEP EWWGsin2W=0.22270.0037 Test one of the interpretations (from many): - strange/anti-strange sea quark asymmetry dimuon production: s -c  -+X(CCFR, NuTeV) Asymmetry S-= xs-dx = x[s(x)-sbar(x)]dx = - 0.0009 0.0014 To explain “NuTeV Anomaly” would require S- = + 0.0060 V. Chekelian, Unpolarised SF

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