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Open Charm Measurements from STAR

Xin Dong University of Science & Technology of China Lawrence Berkeley National Laboratory. Open Charm Measurements from STAR. Many Thanks to Dr. Gerd Kunde!. H. Huang, H. Ritter, L. Ruan, K. Schweda, P. Sorensen, A. Tai, N. Xu, Z. Xu, H. Zhang L. Grandchamp, J. Raufeisen, R. Vogt.

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Open Charm Measurements from STAR

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  1. Xin Dong University of Science & Technology of China Lawrence Berkeley National Laboratory Open Charm Measurements from STAR Many Thanks to Dr. Gerd Kunde! H. Huang, H. Ritter, L. Ruan, K. Schweda, P. Sorensen, A. Tai, N. Xu, Z. Xu, H. Zhang L. Grandchamp, J. Raufeisen, R. Vogt

  2. Outline • Introduction & Motivation • Direct charm reconstruction • Indirect electron measurements • Discussions • Conclusions & outlook

  3. D mesons Large Q value needed (>≈3GeV) pQCD should work better! , Y’, c π0 measurements are consistent with NLO pQCD calculation! Charm should be better!! PHENIX, PRL 91, 241803(2003) STAR, PRL 92, 171801(2004) Heavy flavor in pQCD

  4. (p)QCD Test Total cross section measurement --- not depend on the fragmentation models  A powerful test of QCD calculations ! Charm spectrum measurement --- fragmentation test for theory predictions.

  5. J/y, D W f X L, K* p, K D, p d Charm quark mostly produced from the initial fusion of partons (mostly gluons) Q2 sensitive to Initial Nuclear Effects Z. Lin & M. Gyulassy, PRL 77 (1996) 1222 Z. Lin & M. Gyulassy, PRC 51 (1995) 2177 dN/dMdy ratio (Sh/no Sh) bT saturates time Heavy flavors – a unique probe to QGP

  6. Y. Dokshitzer &D. Kharzeev PLB 519(2001)199 M. Djordevic & M. Gyulassy QM04, nucl-th/0404006 J. Adams et. al, PRL 91(2003)072304 Heavy quark energy loss ● Heavy Quark has less dE/dx due to suppression of small angle gluon radiation

  7. Statistical model: Large ccbar yield in one heavy ion collision  recombination production J/ψ  possible J/ψ enhancement Statistical model A. Andronic et. al. PLB 571,36(2003) J/ψ production: suppression/enhancement? • J/ψ suppression scenario in QGP ! --- Debye screening Total charm yield from pQCD calculations!

  8. Coalescence approach V. Greco, C.M. Ko, R. Rapp, PLB 595(2004)202 Charm quark flow Charm quark flows -> Strong indication of thermalization of light quarks

  9. Single electrons  Open charm v2 At pT > 2.5 GeV/c: 1) D-meson spectrum is ‘hard’, yields of pion will be small, measure D-decayed electron to infer the open charm v2 2) D-meson flow  indication of light flavor thermal equilibrium. X. Dong et. al, PLB597, 328(2004).

  10. Low-energy fixed target – direct D measurement Fermilab E769, PRL 77, 2388 (1996) ISR 52-63GeV – inconsistency, S.P.K. Tavernier Rep. Prog. Phys. 50, 1439 (1987) UA2: 630 GeV p+pbar (two electron data points), O. Botner et al. PLB 236 (1990) 488 Previous Experiments CDF directy D measurement -- high pT CDF, PRL 91, 241804 (2003)

  11. Measurements in heavy ion collisions PHENIX Au+Au@130GeV Phys. Rev. Lett. 88, 192303 (2002) • Nbin scaling for open charm spectrum • Total cross section consistent with NLO pQCD calculation

  12. STAR detector Barrel EM Cal (BEMC) Silicon Vertex Tracker (SVT)Silicon Strip Detector (SSD) FTPCEndcap EM CalFPD TOFp, TOFr Year 2001+ Magnet Coils Central Trigger Barrel (CTB) ZCal Time Projection Chamber (TPC) Year 2000

  13. ( Br. 3.83%) D0 direct reconstruction STAR PRL, in print Event mixing technique First Direct Open Charm Reconstruction at RHIC

  14. D mesons measured at STAR STAR Preliminary

  15. Open charm spectrum STAR Preliminary • D*/D0 ratio is consistent with other experiments and models • Power-law describes the spectrum well up to ~11GeV/c

  16. Indirect measurement D→e+X STAR PRL, in print Hadron identification: STAR Collaboration, nucl-ex/0309012 electrons Electron identification: TOFr |1/ß-1| < 0.03 TPC dE/dx electrons!!!

  17. 1. With TOF and dEdx, electrons can be identified well from ~0.3GeV/c up to ~3GeV/c! 2. Select electrons (e-) using dE/dx only (2-4GeV) Inclusive electrons Hadron contamination was corrected for ~ 5-30% pT 2-4 GeV/c STAR Preliminary

  18. γ conversion π0, η Dalitz decays Kaon decays ρωΦ vector meson decays heavy quark semi-leptonic decay others Single Electrons Spectra background signal γ conversion and π0Dalitz decays are the dominant sources at low pt region. TPC Measurements of electron background • Background Topology: • TOFr tagged e+/e- • Large TPC acceptance • High efficiency of reconstructing • electron pair For the γconversion and π0 Dalitz decay, background spectra are obtained from data using kinematical selection of the pairs in TPC

  19. Background subtraction Invariant Mass Square STAR Preliminary • Data: background spectrakinematical selection of the  conversion and 0 Dalitz decay pairs in TPC • MC: conversion and 0 Dalitz decay reconstruction efficiency~60% • c) MC: relative contributions of • different sources: • determined from PYTHIA/HIJING + detector simulations Signal Rejected  conversion and 0 Dalitz decay reconstruction efficiency : ~60% at pT>1.0 GeV/c STAR Preliminary

  20. Background contribution STAR PRL, in print An increasing excess found at higher pT region, pT > 1.0 GeV/c, → expected to be contribution of semileptonic decay from heavy flavor hadrons

  21. Combining fit Combined fit for D0 and electrons STAR PRL, in print PYTHIA: MSEL = 1, CTEQ5M1 1) Good agreement between D0 and electrons spectra 2) d+Au and p+p do not show significant nuclear effect

  22. p+p and d+Au electron spectra show approximately binary scaling 1<pT<4GeV/c Charm yields Assumption for the combining fit: 1. D0 spectrum follows the power law function 2. only normalization scale between different D meson pT spectrum 3. All the background subtracted electrons are from D decay

  23. Color Dipole: Phys. Rev. D67 (2003) 054008 HSD:Phys. Rev. C67 (2003) 054905 R.Vogt, A. Tai, private communications Charm production at mid-rapidity STAR Preliminary

  24. Mid-rapidity → Full rapidity 4.7 ± 0.7 Charm total cross-section STAR PRL, in print • NLO pQCD calculations under predict the total charm production cross section at RHIC • Scales (muR or muF) may be energy dependent

  25. J/ψ production PHENIX J/psi in AuAu, PRC 69 (2004) 014901 1) Statistical model prediction implies possible J/psi enhancement 2) But with STAR ccbar cross section (from d+Au) , a much larger enhancement (~3-10) for J/psi production in central Au+Au collisions. This upper limit invalidates the expectation from large open charm cross section!

  26. Consistency check STAR Preliminary STAR Preliminary Directly reconstructed D mesons Electrons from D decay D and electron spectra are consistent!

  27. STAR Preliminary B decay dominated region Open charm spectrum is harder ! D0, D*, D A. Tai, A. Suaide, QM04 STAR Preliminary Phenix: PRL. 88, 92303(2002) D. Kharzeev, hep-ph/0310358

  28. MRST HO Peterson’s function ε=0.06 c quark =4,3,2,1 (GeV)^2 Charm quark hadronization at RHIC bare c-quark spectrum, normalized to measured dn/dy After broadening and fragmentation R. Vogt, hep-ph/0203151 STAR Preliminary A. Tai QM04 1) Higher order processes needed 2) Charm hadronization through fragmentation + recombination?

  29. Non-photonic electron v2 Systematic errors are important! STAR: 0-80%(F.Laue SQM04)PHENIX: Minimum bias statistical error only HSD: E. Bratkovskaya et al., hep-ph/0409071 X. Dong, S. Esumi, et al., Phys. Lett. B597, 328(2004). corrected for e± from  decay M. Kaneta et al, J.Phys. G30, S1217(04)

  30. Conclusions Both direct open charm reconstruction and indirect charm semi-leptonic decay electrons are measured at STAR in d+Au collisions. They provide consistent results. Total charm cross section from this measurement is higher than NLO pQCD calculations. Preliminary D meson spectrum appears to imply a unusual hard fragmentation function for charm quarks. Study open charm v2 and J/ yields to address thermalization issues at RHIC. The run-IV data will just do that.

  31. Upgrade at STAR STAR MRPC - TOF STAR Heavy Flavor Tracker Full open charm measurements Full resonance measurements with both hadron and lepton decays

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