Transcript Slide 1
Quarkonium progress in STAR Manuel Calderón de la Barca Sánchez UC Davis Heavy Flavor Working Group, STAR; XXII Winter Workshop on Nuclear Dynamics La Jolla, CA 15/March/2006 Outline Motivation STAR capabilities Trigger e+e- Triggered samples so far Run IV Au+Au: Run V p+p: J/y Prospects for Run VI and beyond. 15/March/2006 Manuel Calderón de la Barca 2 Why are we interested in quarkonia? Charmonium suppression: longstanding QGP signature Original idea: screening. lattice calculations confirm screening effects Nucl.Phys.Proc.Suppl.1 29:560-562,2004 15/March/2006 O. Kaczmarek, et al., Nucl.Phys.Proc.Suppl.129:560-562,2004 Manuel Calderón de la Barca 3 Quarkonium at SPS NA50 data: “Anomalous” suppression. NA60 data: Confirmation (with smaller errors) PHENIX at RHIC, see Wei Xie next… Satz, Digal, Fortunato (percolation) Rapp, Grandchamp, Brown (diss. and recomb.) Theory challenge Capella, Ferreiro (comovers) Description of SPS and RHIC data 15/March/2006 Manuel Calderón de la Barca 4 Binding Energy & TD Binding Energy & Sequential Suppression. State y(2s) cc(1p) J/y(1s) Eb (GeV) 0.05 0.23 0.64 TD/TC 0.1-0.2 0.74 1.1 State (3s) cb(2p) (2s) cb(2p) (1s) Eb (GeV) 0.2 0.3 0.54 0.67 1.1 TD/TC 0.75 0.83 1.1 1.13 2.31 Digal, Petreczky, Satz; Phys.Rev.D64:094015,2001 Using lattice free energy as potential. The premise: A full quarkonium spectroscopy can help address the question of deconfinement; ~ direct connection to first principles LQCD. Reality Check: Uncertainties in the calculations (~factor 2), free energy vs. internal energy potential models vs. spectral functions Gluons breaking up J/y, recombination contribution?, 15/March/2006 Manuel Calderón de la Barca 5 Lessons learned the hard way To connect with theory, we need a good systematic programme: p+p, Au+Au, vs. cent. vs. √s Measure not just J/y. Excited states are needed for feeddown. Y states are a key, but Small cross section Mass resolution? 15/March/2006 Manuel Calderón de la Barca 6 What can STAR contribute? STAR was not built for di-leptons, but… Large acceptance at mid-rapidity |h|<1 , 0<f<2p Pair acceptance ~ single acceptance2 Electron ID-capabilities TPC dE/dx EMC E>1-2 GeV (full barrel in 2006) TOF p<2-3 GeV/c (only patch, full barrel in the future) Triggering capabilities on Barrel EMC Suitable for single electrons (proxy for open charm) (see J. Harris’s talk tomorrow afternoon) Suitable for di-electrons? J/y, are rare, triggering where possible J/y in pp in all systems (no signal without a trigger) large dataset if triggering not possible: J/y in Au+Au 15/March/2006 Manuel Calderón de la Barca 7 Electron ID 1.5<p< 5 GeV, |p/E-1|<1 Combine detectors TPC dE/dx in a limited region Barrel EMC for p>1 GeV/c TPC+BEMC P.Djawotho 15/March/2006 Manuel Calderón de la Barca 8 Electron Efficiency and Purity P. Djawotho 15/March/2006 Manuel Calderón de la Barca 9 J/Y “Topology” Trigger: Level-0 Fast, T ≤1ms Divide f into 6 sections Find a tower above a threshold Look in the 3 opposite sections in f If another tower above threshold, issue trigger. 15/March/2006 Manuel Calderón de la Barca 10 J/Y Software Trigger: Level-2 Looking for e+e- pair Approximate electron daughters with tower cluster Use L0 tower cluster, combine with L2 clusters Energy, Position cos(q) Vertex from trigger detectors timing BBC Resolution ~ 6 cm in Au+Au, but 30 cm in p+p. Otherwise assume vtx at (0,0,0). Make tower cluster pairs, neglecting me: m2inv 2E1E2(1-cos(q12)) Issue decision in T<500 ms. 15/March/2006 Manuel Calderón de la Barca 11 Can it be used in Au+Au? High rejection only for peripheral events. Most signal in central events. 98% of the yield is in top 60% central. There is no free lunch… p+p: environment well matched for trigger Au+Au: must rely on a large dataset. 15/March/2006 Manuel Calderón de la Barca 12 Trigger: L0 + L2 Advantage: mass is large Can use a simpler L0 trigger Require one BEMC towerwith ET>3.5 GeV T. Kollegger Use similar L2 algorithm Can trigger in p+p and also in central Au+Au! Rare triggers can go to “express stream” processing. Very quick turnaround time. Disadvantage: production rate is tiny! Expected less than 100 in the full Run IV Au+Au dataset. Reality, got only a few counts due to many compounded effects Smaller acceptance Less running time BEMC miscalibration Some detectors not ready for L2 in Run IV 15/March/2006 Manuel Calderón de la Barca 13 J/y in Au+Au Run IV No triggering is possible, too much background. Search in the Au+Au dataset of Run IV Signal? Hints so far… Analysis using TPC alone STAR Preliminary J. González Dielectron Invariant Mass (GeV/c2) EMC had smaller acceptance p ~ 1.5 GeV/c, borderline for EMC PID 15/March/2006 Manuel Calderón de la Barca 14 Trigger in Au+Au Run IV L0: events with Etower > 3.5 GeV. L2: events with cluster pair masses m>7 GeV/c2. Trigger works! 15/March/2006 Manuel Calderón de la Barca 15 Trigger performance in Au+Au Events sampled per day 4-20 M per day Variations due to need to meet other STAR goals Half-field running Part of heavy-flavor progam: D* -> D+p Additional triggers reducing trigger livetime. 15/March/2006 Manuel Calderón de la Barca 16 Analysis in Au+Au run IV Sampled 34.2 mb-1 More than 200 M minimum bias events scanned with Upsilon trigger. Comparison w/ offline ~50 M minimum bias events. Small dataset processed Only 3 signal counts (with no background counts) were observed. 1st STAR measurement where we are Luminositylimited in a big way. 15/March/2006 Half field running, no BEMC-based triggers. Manuel Calderón de la Barca 17 Analysis in Au+Au Upper limit estimation: +- ++ -- Npairs 8.4<m< 10.7 GeV 2 0 0 Npairs 10.7<m< 13.0 GeV 0 0 1 90% C.L. : signal < 4.91 B*ds/dy C.L. < 7.6 mb T. Kollegger Acceptance increase will help Factor ~ 4. 15/March/2006 Manuel Calderón de la Barca 18 Trigger performance in Run V Energy (MeV) Invariant mass (MeV/c2) Online monitoring of trigger information. Extremely fast turnaround. No need to wait for offline production to find if trigger is behaving as expected. 15/March/2006 Manuel Calderón de la Barca 19 Sample from Run V, p+p Collected 1.7 M triggers Simulation: expected a sample of 6070 J/y’s in this test data set. Data: P. Djawotho Yield small, but consistent with simulations. Ready for Run VI! 15/March/2006 Manuel Calderón de la Barca 20 Data and simulation comparison Width is consistent with our detector resolution. Mass is slightly lower than expected (2s) 15/March/2006 Manuel Calderón de la Barca 21 Future Run VI p+p: Barrell EMC now fully installed |h|<1, full azimuth Increase by factor 4 over Run IV dielectron acceptance. L2 trigger has proved to work Will be heavily used in Run VI (jets, dijets) Longer term upgrades Improve vertex knowledge at L0 ~1 cm resolution using upgrade to pVPD used in TOF Additional PID capabilities by full barrel TOF (2009) TOF also allows a better background rejection. R&D on possible muon trigger in |h|<1, 60% azimuth 15/March/2006 Manuel Calderón de la Barca 22