Hot Quarks 2004 July 23, 2004, Taos, New Mexico Tatsuya Chujo Hadron Production at Intermediate p T at RHIC Tatsuya Chujo Vanderbilt University for the.

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Presentation transcript:

Hot Quarks 2004 July 23, 2004, Taos, New Mexico Tatsuya Chujo Hadron Production at Intermediate p T at RHIC Tatsuya Chujo Vanderbilt University for the PHENIX Collaboration Tatsuya Chujo Vanderbilt University for the PHENIX Collaboration

Tatsuya ChujoHot Quarks 2004 July 23, 2004, Taos, New Mexico 2 Outline 1.Motivation Baryon anomaly intermediate p T (2-5 GeV/c) at RHIC. 2.Experimental data in Au+Au  s NN =200 GeV 1)  meson (N coll scaling property, R cp ) 2)Meson vs. baryon R cp. 3)Jet correlation with PID trigger. 4)Models vs. data (hydro+jet, recombination). 3.Proton and antiproton production in Au+Au  s NN =62.4 GeV 4.Summary and outlook 1.Motivation Baryon anomaly intermediate p T (2-5 GeV/c) at RHIC. 2.Experimental data in Au+Au  s NN =200 GeV 1)  meson (N coll scaling property, R cp ) 2)Meson vs. baryon R cp. 3)Jet correlation with PID trigger. 4)Models vs. data (hydro+jet, recombination). 3.Proton and antiproton production in Au+Au  s NN =62.4 GeV 4.Summary and outlook

Tatsuya ChujoHot Quarks 2004 July 23, 2004, Taos, New Mexico 3 1. Baryon Anomaly at RHIC PHENIX: PRL 91, (2003), PRC 69, (2004) p, pbar : No suppression, N coll scaling at 1.5 GeV GeV  0 : Suppression Factor ~3 enhancement on both p/  and pbar/  ratios in central Au+Au compared to peripheral Au+Au, p+p at Intermediate p T. Peripheral Au+Au at high p T : Consistent with gluon/quark jet fragmentation and IRS data.

Tatsuya ChujoHot Quarks 2004 July 23, 2004, Taos, New Mexico Scaling properties of  (1020)  meson: Similar mass as proton, but meson.  Ideal test particle whether the observed baryon anomaly is a mass effect or not. proton, pbar: PHENIX: PRL 91, (2003), PRC 69, (2004)  : PHENIX final data, will be submitted to PRC. p, pbar: low p T (< 1.5 GeV/c): different shape due to the radial flow, intermediate p T : Ncoll scaling  : does not scale with N coll

Tatsuya ChujoHot Quarks 2004 July 23, 2004, Taos, New Mexico 5 R cp of  meson Followed the  0 data points, not protons! Indicates the absence of suppression of proton at intermediate p T is not a mass effect.

Tatsuya ChujoHot Quarks 2004 July 23, 2004, Taos, New Mexico Compilation on R cp from STAR Presented by M. Lamont (QM04) Two distinct groups in R cp, i.e. meson and baryon, not by particle mass. Separate at p T ~ 2 GeV/c and come together at 5 GeV/c. baryon meson

Tatsuya ChujoHot Quarks 2004 July 23, 2004, Taos, New Mexico Mid-p T protons from fragmentation? Intermediate p T is the transition region from soft to hard process. What is the origin of proton and antiproton production at the intermediate p T ? Note: Recombination model of purely thermal quarks implies the observed baryon excess comes from soft, not from fragmentation (no jet partner hadrons).  Jet correlation with identified particle trigger (p+pbar,  +K) are employed in Au+Au and d+Au. Intermediate p T is the transition region from soft to hard process. What is the origin of proton and antiproton production at the intermediate p T ? Note: Recombination model of purely thermal quarks implies the observed baryon excess comes from soft, not from fragmentation (no jet partner hadrons).  Jet correlation with identified particle trigger (p+pbar,  +K) are employed in Au+Au and d+Au.

Tatsuya ChujoHot Quarks 2004 July 23, 2004, Taos, New Mexico 8 Jet Correlation with PID trigger Trigger (PID) p T = GeV/c Near side Away side Count associated low p T particles with PID mid-p T trigger Near side: Number of jet associated particles from same jet. Away side: Number of fragments from opposing jet. A. Sickles (QM04) *Line: calculated combinatorial BG modulated by the measured v 2.

Tatsuya ChujoHot Quarks 2004 July 23, 2004, Taos, New Mexico 9 Jet correlation: near side No apparent difference on jet partner yield between trigger baryons and mesons, perhaps except most central Au+Au for baryons. Suggested intermediate p T baryon arises from a fragmentation from jet. Trigger (PID) p T = GeV/c Near side Away side d-Au Duke reco model Red (proton) Blue (pion), A. Sickles (QM04)

Tatsuya ChujoHot Quarks 2004 July 23, 2004, Taos, New Mexico 10 Jet correlation: away side Trigger (PID) p T = GeV/c Near side Away side Meson and baryon are comparable and decreasing at most central Au+Au collisions. In agreement with the disappearance/ broadening of back-to-back jet correlation in central Au+Au. A. Sickles (QM04) d-Au

Tatsuya ChujoHot Quarks 2004 July 23, 2004, Taos, New Mexico Hydro+Jet vs. data Hirano, Nara (Hydro+Jet model) PRC 69, (2004). nucl-th/ (+CGC). Excellent agreement in  0 suppression pattern. Trend in Rcp(p) and p/pi ratio are right, but quantitative disagreement with data. Challenging for  and K* due to the mesons with large mass.  Explained by the less interaction cross section? p/  R cp

Tatsuya ChujoHot Quarks 2004 July 23, 2004, Taos, New Mexico 12 Recombination Models vs. data Qualitative agreement with R cp (proton) data. Better description when (thermal - hard) is included, which supports the experimental result on jet correlations. Duke model, PRC 68, (2003) p/  R cp

Tatsuya ChujoHot Quarks 2004 July 23, 2004, Taos, New Mexico p, pbar production  s NN = 62.4 GeV Why 62.4 GeV? 1)Located in the middle between SPS(17GeV) and RHIC top energy (200 GeV) in  s NN (log scale). 2)Many reference data from ISR. 3)Provide a constraint on jet quenching model. 4)Allow to study the excitation function of baryon production/transport, further constrain on various models for hadron production at intermediate p T. Why 62.4 GeV? 1)Located in the middle between SPS(17GeV) and RHIC top energy (200 GeV) in  s NN (log scale). 2)Many reference data from ISR. 3)Provide a constraint on jet quenching model. 4)Allow to study the excitation function of baryon production/transport, further constrain on various models for hadron production at intermediate p T.

Tatsuya ChujoHot Quarks 2004 July 23, 2004, Taos, New Mexico GeV R AA : Charged hadron and   Common reference p+p  charged+X is used, instead of ISR  0 reference.  0 yield is divided by (charged reference)/1.6. Clear difference between charged and  0 at intermediate p T up to 4 GeV/c. Suggests a large proton contribution in this p T region, as seen in 200 GeV data. Common reference p+p  charged+X is used, instead of ISR  0 reference.  0 yield is divided by (charged reference)/1.6. Clear difference between charged and  0 at intermediate p T up to 4 GeV/c. Suggests a large proton contribution in this p T region, as seen in 200 GeV data. 00 charged 0-10%

Tatsuya ChujoHot Quarks 2004 July 23, 2004, Taos, New Mexico 15 h + /  0 and h - /  0 62 GeV Monotonic increase for both ratios at measured p T, starting from 1.6. Difference between negative and positive hadron to  0 ratio. Monotonic increase for both ratios at measured p T, starting from 1.6. Difference between negative and positive hadron to  0 ratio. ISR h+/0h+/0 h-/0h-/0

Tatsuya ChujoHot Quarks 2004 July 23, 2004, Taos, New Mexico 16 p/    pbar/   62 GeV Large proton contribution at intermediate p T 62.4 GeV. Less antiproton in central collisions at 62.4 GeV than 130/200 GeV. Indicating more baryon transport and less p- pbar pair production at 62 GeV than 200 GeV. The 62 GeV p T spectra will tell us more about the excitation function of chemical properties, scaling and radial flow at RHIC (stay tuned!). Large proton contribution at intermediate p T 62.4 GeV. Less antiproton in central collisions at 62.4 GeV than 130/200 GeV. Indicating more baryon transport and less p- pbar pair production at 62 GeV than 200 GeV. The 62 GeV p T spectra will tell us more about the excitation function of chemical properties, scaling and radial flow at RHIC (stay tuned!).

Tatsuya ChujoHot Quarks 2004 July 23, 2004, Taos, New Mexico Summary Experimental data seems to have a better agreement with a recombination model with thermal-hard parton interactions. Important difference between Hydro+Jet and recombination model is the origin of flow, i.e. partonic flow or hadronic flow? Discriminatory measurements are essential to understand the hadron production at intermediate p T. High statistics identified trigger particle correlations. v 2 for  meson. Charm: v 2 and R cp for D meson, J/ . Hadron PID (especially baryons) at higher p T up to 10 GeV/c to study the fragmentation region at RHIC. Experimental data seems to have a better agreement with a recombination model with thermal-hard parton interactions. Important difference between Hydro+Jet and recombination model is the origin of flow, i.e. partonic flow or hadronic flow? Discriminatory measurements are essential to understand the hadron production at intermediate p T. High statistics identified trigger particle correlations. v 2 for  meson. Charm: v 2 and R cp for D meson, J/ . Hadron PID (especially baryons) at higher p T up to 10 GeV/c to study the fragmentation region at RHIC.

Tatsuya ChujoHot Quarks 2004 July 23, 2004, Taos, New Mexico 18 High p T PID Upgrade Aerogel & MRPC-TOF Together with the Aerogel, TOF and RICH, we can extend the PID beyond 5 GeV/c. Coverage: ~ 4 m 2 in west arm. AEROGEL: Full installation for Run5. MRPC-TOF: Prototype installation in Run5 Physics run in Run6.

Tatsuya ChujoHot Quarks 2004 July 23, 2004, Taos, New Mexico 19 MRPC-TOF Prototype Test Prototype KEK (June 1-8, 2004) TOF resolution: 85 ps achieved.

Tatsuya ChujoHot Quarks 2004 July 23, 2004, Taos, New Mexico 20 PHENIX Collaboration

Backup Slides

Tatsuya ChujoHot Quarks 2004 July 23, 2004, Taos, New Mexico 22 Hybrid model: Hydro + Jet 3D Hydro calculation. Required QGP type EOS in order to reproduce p T spectra and elliptic flow. Jet quenching included. Hydro push thermal distribution to higher pT at hadronic stage (mass effect). T=T c, ~0.25c T=100 MeV, ~0.55c Intermediate p T = GeV/c  : hard region p : soft region N SOFT ~N HARD Hirano, Nara (Hydro+Jet model) PRC 69, (2004). nucl-th/ (+CGC).

Tatsuya ChujoHot Quarks 2004 July 23, 2004, Taos, New Mexico 23 Quark Recombination Models Quarks in a densely populated phase space combine to form the final state hadrons. 1.Duke model (Fries, Muller, Nonaka, Bass) Exponential thermal quark distribution, fragmentation for high pT (w/ eloss). Relative normalization (recombination  fragmentation). No gluons in the system. Parameterized collective flow developed in the partonic phase (v T ~0.55c at T=T c ). 2.Oregon model (Hwa and Yang) All hadrons arise from recombination (NO fragmentation). Hard partons are allowed to fragment into a shower of partons. e.g.) thermal-thermal, thermal-shower, shower-shower (for mesons). 3.Texas model (Greco, Ko, Levai) Allow recombination of hard partons with thermal partons by Monte-Carlo. Taking into account decays (e.g.  2  ) which produces low pt pions.

Tatsuya ChujoHot Quarks 2004 July 23, 2004, Taos, New Mexico 24 Recombination Model References Duke Model R.J. Fries, B. Muller, C. Nonaka, S.A. Bass, PRL 90, (2003). R.J. Fries, B. Muller, C. Nonaka, S.A. Bass, PRC 68, (2003). Oregon Model R.C. Hwa, C.B. Yang, PRC 67, (2003). R.C. Hwa, C.B. Yang, nucl-th/ TAMU Model V. Greco, C.M. Ko, P. Levai, PRL 90, (2003). V. Greco, C.M. Ko, RPC 68, (2003). Duke Model R.J. Fries, B. Muller, C. Nonaka, S.A. Bass, PRL 90, (2003). R.J. Fries, B. Muller, C. Nonaka, S.A. Bass, PRC 68, (2003). Oregon Model R.C. Hwa, C.B. Yang, PRC 67, (2003). R.C. Hwa, C.B. Yang, nucl-th/ TAMU Model V. Greco, C.M. Ko, P. Levai, PRL 90, (2003). V. Greco, C.M. Ko, RPC 68, (2003).

Tatsuya ChujoHot Quarks 2004 July 23, 2004, Taos, New Mexico 25 Another Scenarios… pQCD does not reproduce Bbar/B vs. p T. Baryon Junction Mechanism ? (Vitev, Gyulassy PRC 65, , 2002) Different formation time between baryons and mesons ?

Tatsuya ChujoHot Quarks 2004 July 23, 2004, Taos, New Mexico 26  R cp by STAR