heavy flavor production in p+p collisions in phenx experiment at rhic
DESCRIPTION
Heavy Flavor Production in p+p Collisions in PHENX Experiment at RHIC. W. Xie (RBRC) for PHENIX Collaboration. l. Motivation for Heavy Flavor measurements at RHIC. K +. e - / -. e - / -. e + / +. J/ y. An very important probe for study pQCD. K -. e + / +. l. D 0. - PowerPoint PPT PresentationTRANSCRIPT
Heavy Flavor Production in p+p Collisions in PHENX Experiment at RHIC
W. Xie (RBRC) for PHENIX Collaboration
Motivation for Heavy Flavor measurements at RHIC
• An very important probe for study pQCD.
0D
D0
J/
K+
l
l
K-
e-/-
e+/+
e-/-
e+/+
• A very important Probe for studying properties of Hot Partonic Matter and Cold Muclear Matter
(See Xiaorong Wang’s talk in Heavy-ion section)
Pioneering High Energy Nuclear Interaction eXperiment (460 participant from 57 institutions of 12 countries)
• Maximal Set of Observables– Photons, Electrons, Muons, ID-hadrons
• Highly Selective Triggering– High Rate Capability.– Rare Processes.
How PHENIX Measure Heavy Flavor• high resolution tracking and
momentum measurement from Drift chamber.
Good electron identification from Ring Imaging Cherenkov detector (RICH) and Electromagnetic Calorimeter (EMCal).
High rate capability: powerful level-1 electron trigger
E/p
Hadronic background
J/Psi->ee
Good momentum resolution and muon identification from ID and Trk.
High rate capability: powerful level-1 dimuon trigger
How PHENIX Measure Heavy Flavor
J/Psi->uu
J/Psi->uu
Measure Open Heavy Flavor via electrons at midrapidity
Subtraction of “photonic” sources.• conversion of photons from hadron decays in material
• Dalitz decays of light mesons ()
Converter method• Comparison of e+/- spectra with and without converter
allows separation of photonic and non-photonic sources of single electrons.
measurement via -e coincidences • Yield of -e in vicinity of mass with mixed event
subtraction
cocktail
-e invariant mass
γe+
e-ConverterAu
Au
All 3 methods cross check each other and give consistent results
TrackerIdentifier Absorber
Collision vertex range
Collision
Muon HadronAbsorberSymbols
Detector
1
1 : Hadrons, interacting and absorbed (98%),
2
2 : Charged /K's, “decaying into ” before absorber (≤1%),
3
3 : Hadrons, penetrating and interacting (“stopped”)
4
4 : Hadrons, “punch-through”, 5 : Prompt , ”desired signal”
5
zcoll zcollzcoll
Measure Open Heavy Flavor via muon at forward rapidity
Prompt electron cross section at midrapidity
PRELIMINARYPRELIMINARY
PRELIMINARY
Prompt Muon cross section at forward rapidity
J/Psi Cross Section Measurement
The total cross section in p-p collisions is:
2.61+/-0.20(fit)+/-0.26(abs) µb
J/Psi pT distribution
Fitting function:
A*[1+(pT/B)2]-6
<pT2>= 4.31±0.85
At midrapidity
<pT2>= 2.51±0.21
at forward rapidity
Run3 (Y=0)
Run3 (Y=0)
<pT2>= 4.31±0.85
CSM
COM
CSM
COM
J/Psi pT distribution
Upsilon Measurement PHENIX accumulated ~3pb-1 p-p collision during 2005 run.
1st Upsilons at RHIC !
Phenix muon arm
Future Measurement
S. Lebedev
• We see Chi_c in run5 with 3pb-1
• We are expecting to accumulate a factor of 3 more luminosity in the current ongoing run6.
•RHICII:
•Detector Upgrade