QM Low Mass Leptons Poster

Future Possibilities for Measuring Low Mass Lepton Pairs in: 

Future Possibilities for Measuring Low Mass Lepton Pairs in Quark Matter 2002, Nantes

Why measure low mass lepton pairs?: 

Why measure low mass lepton pairs? In heavy ion collisions, low mass lepton pairs provide a clean signal for studying thermal radiation from the hadron gas in-medium effects on low mass vector mesons open charm cross section at RHIC appears to be large!

Slide3: 

Thermal radiation from HG —  annihilation: +-  *  e+e- Cross section dominated by pole at the  mass of the  em form factor: Dropping -meson mass R. Rapp, J. Wambach et al -meson broadening G.E. Brown et al OR In-medium effects —

Slide4: 

Invariant mass distribution of electron pairs at RHIC R. Rapp Electron pairs from theory . . . Simulated electron pair spectrum and combinatorial background in PHENIX K. Ozawa

How to lower the background?: 

How to lower the background? Fast, compact Time Projection Chamber, encircled by “Hadron Blind” photocathode layer sensitive to light from Cerenkov radiation “Hadron Blind Detector”: choose radiator gas such that only electrons produce Cerenkov radiation Joint R&D effort with STAR Proposed New Detector: Combined TPC/HBD

Slide6: 

Run with low inner magnetic field—optimize measurement of low momentum tracks Electron ID for signal electrons (vector mesons, low mass pairs) from outer PHENIX detectors Electron ID for low momentum electrons (p < 200 MeV/c) from Cerenkov blob on HBD, dE/dx in TPC Reconstruct invariant mass of opposite sign pairs identified as electrons (ee > 90%, prej > 200:1 for particles outside PHENIX acceptance) Strategy for identification and rejection of background electrons Reject pairs which reconstruct to an invariant mass < ~130 GeV/c2

A new inner field coil creates the low-field inner tracking region needed: 

A new inner field coil creates the low-field inner tracking region needed Inner Coil creates a zero-field integral (∫Bdl = 0) region inside the Central Magnet TPC/HBD Proposal: Added bonuses to PHENIX! 2p tracking greater particle ID capabilities inner coil can also enhance outer field: improved momentum resolution for high pt tracks Not a field-free region

R & D: 

R & D Use single gas as TPC drift gas HBD radiator gas operating gas for readout detector must be fast, VUV transparent, work well in readout detector: CH4, CF4,… Gas requirements Currently studying: Drift velocity, diffusion, dE/dx Gas scintillation and timing Different gas mixtures VUV Spectrometer B. Azmoun Quantum efficiency of CsI Absorbance of CF4 Transparency of CF4 down to wavelengths of ~120 nm allows more photoelectrons to be produced on the CsI—region of highest Q.E.

Slide9: 

Micropattern readout detector: Gas Electron Multiplier (GEM) or possibly mMegas Use for both TPC and HBD readout Currently studying: Gain of GEM for stable operation Aging properties of GEM Response to electrons and hadrons (Npe per electron and per MIP) Detector Readout 35 TPC pad rows Pad size: dr ~ 1 cm df ~ 2 mm One octant of TPC Axial drift in TPC: readout on two endplanes

Slide10: 

Gas Electron Multiplier 10x10 cm2 GEM from CERN GEM detector studies currently underway What is a GEM and how does it work? Cu-coated kapton Etched grid of ~40-micron holes Potential difference applied across the holes, creating a strong electric field inside each hole Electrons avalanche through the holes

Slide11: 

HBD readout 100 MeV electron producing a Cerenkov blob on the HBD image plane Large area photocathode: CsI CsI photocathode deposited directly onto GEM surface A. Breskin

Simulation Studies: 

Simulation Studies CF4: ~30 photoelectrons per e- track Occupancy of HBD Assuming 4% of a radiation length from proposed silicon vertex detector upgrade (see poster #89, H. van Hecke) Occupancy of TPC Innermost pad row (r = 20 cm) Central Au-Au at 200 GeV

Slide13: 

How well can we reduce the electron background from Dalitz decays and conversions? K. Ozawa and C.A. Central events (dNch/dy = 650) Both electrons from vector mesons in PHENIX central arm acceptance (pT> 200 MeV/c, |h| < 0.33, 2*|f| < 90o) p >10 MeV/c for all electrons Rejection factor for p’s: 1/200 (1/200)2 for p<4 GeV/c in PHENIX central 100% electron efficiency Perfect momentum resolution

Slide14: 

K. Ozawa Dalitz rejection and Survival Probability of Vector Mesons Survival probability of r,w,f is ~85% for Dalitz rejection ratio of 90%.

Conclusions: 

Conclusions The measurement of low mass lepton pairs requires excellent rejection of Dalitz pairs and conversions to reduce the combinatorial background. A novel new detector is proposed consisting of a TPC and HBD which can greatly reduce the Dalitz and conversion backgrounds. The large charm cross section in heavy ion collisions is another significant source of background which cannot be eliminated by Dalitz rejection. This signal will have to be measured as well in order to fully understand the low mass pair continuum.