heavy flavor production in p+p collisions in phenx experiment at rhic

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Heavy Flavor Production in p+p Collisions in PHENX Experiment at RHIC W. Xie (RBRC) for PHENIX Collaboration

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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 Presentation

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Page 1: Heavy Flavor Production in p+p Collisions in PHENX Experiment at RHIC

Heavy Flavor Production in p+p Collisions in PHENX Experiment at RHIC

W. Xie (RBRC) for PHENIX Collaboration

Page 2: Heavy Flavor Production in p+p Collisions in PHENX Experiment at RHIC

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)

Page 3: Heavy Flavor Production in p+p Collisions in PHENX Experiment at RHIC

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.

Page 4: Heavy Flavor Production in p+p Collisions in PHENX Experiment at RHIC

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

Page 5: Heavy Flavor Production in p+p Collisions in PHENX Experiment at RHIC

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

Page 6: Heavy Flavor Production in p+p Collisions in PHENX Experiment at RHIC

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

Page 7: Heavy Flavor Production in p+p Collisions in PHENX Experiment at RHIC

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

Physics Dept.
This is the simplified scheme of the muon spectrometer. Bulk of the hadrons displayed as 1 are absorbed in the front absorber.Small fraction of them decay into muon before absorption and still are the largest source of muons, which are called decay muons.Some hadrons penetrateall absorber layers and we call them punch-through,which is another source of backgroundto the measurement.Some hadrons penetrate front absorberbutare absorbed in the muon identifier.They are observable, used for the light hadron analysis, and used to estimate the punch-through's.Muons from semi-leptonic decay are produced instantly and we call them prompt muons.Depending on the location of collision, average distance for decay change linearly.So, actual yield of muon will depend on collision point. We use this characteristics to extract decay muons.
Page 8: Heavy Flavor Production in p+p Collisions in PHENX Experiment at RHIC

Prompt electron cross section at midrapidity

Page 9: Heavy Flavor Production in p+p Collisions in PHENX Experiment at RHIC

PRELIMINARYPRELIMINARY

PRELIMINARY

Prompt Muon cross section at forward rapidity

Physics Dept.
This page shows the non-photonic electron and the prompt muon spectra, both of which are dominated by the semileptonic decay of heavy flavor.A notable observation is non-photonic electron and prompt muon spectra are quite similar.
Page 10: Heavy Flavor Production in p+p Collisions in PHENX Experiment at RHIC

J/Psi Cross Section Measurement

The total cross section in p-p collisions is:

2.61+/-0.20(fit)+/-0.26(abs) µb

Page 11: Heavy Flavor Production in p+p Collisions in PHENX Experiment at RHIC

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)

Page 12: Heavy Flavor Production in p+p Collisions in PHENX Experiment at RHIC

Run3 (Y=0)

<pT2>= 4.31±0.85

CSM

COM

CSM

COM

J/Psi pT distribution

Page 13: Heavy Flavor Production in p+p Collisions in PHENX Experiment at RHIC

Upsilon Measurement PHENIX accumulated ~3pb-1 p-p collision during 2005 run.

1st Upsilons at RHIC !

Phenix muon arm

Page 14: Heavy Flavor Production in p+p Collisions in PHENX Experiment at RHIC

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