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Measurement of Open Heavy Flavor Production in STAR Experiment at RHIC

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Measurement of Open Heavy Flavor Production in STAR Experiment at RHIC. W. Xie for STAR Collaboration (Purdue University, West Lafayette).  l. Motivation for Studying Heavy Quarks. Heavy quark mass are external parameter to QCD. Sensitive to initial gluon density and gluon distribution. - PowerPoint PPT Presentation
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Measurement of Open Heavy Flavor Production in STAR Experiment at RHIC W. Xie for STAR Collaboration (Purdue University, West Lafayette) 1 DIS2010 Convitto della Calza, Firenze, 19th - 23rd April 2010
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Measurement of Open Heavy Flavor Production in STAR Experiment at RHIC

W. Xie for STAR Collaboration

(Purdue University, West Lafayette)

1DIS2010 Convitto della Calza, Firenze, 19th - 23rd April 2010

Motivation for Studying Heavy Quarks

• Heavy quark mass are external parameter to QCD.

• Sensitive to initial gluon density and gluon distribution.

• Interact with the medium differently from light quarks.

• Suppression or enhancement pattern of heavy quarkonium production reveal critical features of the medium.

• Cold Nuclear effect (CNM):– Different scaling properties in central

and forward rapidity region CGC.– Gluon shadowing, etc

0D

D0

K+

lK-

e-/-

e-/-

e+/+

Heavy quarkonia

Open heavy flavor

2

Non-photonic electron

3

MRPC ToF barrelMRPC ToF barrel

BBC

PMD

FPD

FMS

EMC barrelEMC End Cap

DAQ1000DAQ1000

FGT

Completed

Ongoing

MTD

R&DHFT

TPC

FHC

HLT

The STAR Detector

The Long Standing Issue on RHIC NPE Measurement

4

Results differ by a factor of two inpT spectra Total cross section p+p collisions Au+Au collisions

Investigation is underway

STAR PRL 97(2007)192301PHENIX PRL 98(2007)172301

PRL 94(2005)082301PRL 97(2006)252002

STAR d+Au PRL 94(2005)62301

STAR

STAR Solution

Significantly Increase the S/B of this analysis (2008-present)Cross check NPE measurements with early runs.

STAR preliminary

R(cm)

Beam pipe + SVT + SSD+ Dalitz

Beam pipe + Dalitz

TPC Inner Field cage

Cou

nt

Yield of conversion electrons at different radial location 5

STAR high pT NPE Measurements in 200GeV p+p collisions

Measurement done using TPC+EMC using run08 and run05 data.pT>2.5GeV/c NPE measurement with dramatically different background agree with each very well

• Combined using “Best Linear Unbiased Estimate”. χ2/ndf = 4.81/7 = 0.69 6

Comparison with the Published NPE Results

STAR and PHENIX NPE result in 200GeV p+p collisionsAre consistent within errors at pt > 2.5 GeV/c

STAR High pT NPE results are consistent with FONLL in 200GeV p+p collisions

7

8/18

Disentangle Charm and Bottom Production

• Wider φ distribution for B meson because of the larger mass.

•Combined fit on data to obtain the B meson contribution to non-photonic electron.

DheB

BheBhe rr )1(

)/( BDBB eeer

B

D hep-ph/0602067

9/18

Disentangle Charm and Bottom Production

cc0D0D

eK

K

0D

eK

bb0D

KB B

0*D

• Near side: mostly from B mesons •Away side: charm (~75%), Bottom (~25%)

STAR preliminary

JPG35(2008)104117

JPG35(2008)104117

~30-60% of non-photonic electron come from B meson decay in 200GeV p+p collisions.

10

B Quark contribution is Significant in p+p colliosions

Nuclear Physics A830 (2009)849c

STAR preliminary

Constrain B quark Cross Section

11

Nuclear Physics A830 (2009)849c

STAR preliminary

•Obtain B quark high pT spectrum

•Constrain B quark Production Cross Section at RHIC using Model predictions.

12

Future of Heavy Flavor Measurement at STARMTD (MRPC)

Summary and Perspective

13

STAR NPE results and PHENIX published result are consistent within errors at pt > 2.5 GeV/c in 200GeV p+p Collisions.

STAR hight pT NPE Results are consistent with FONLL.

New measurements of D mesons and low pT NPE using TOF should provide good constraints on total charm cross section

Expecting exciting results in the coming years with upgraded detectors and luminosity.

backup

14

15

Future of Heavy Flavor Measurement at STAR

Courtesy of T. Ullirich

MTD (MRPC)

16

Analysis Method in STAR for High pT NPE

17

)(

)()(photonicN

inclusiveNnpeN

Photonic Reconstruction Efficiency estimated from embedding.Small variation in ε can leads to large difference in NPE

Dominant background:

ee

ee

0

Combining run5 and run8 resultsUsing “Best Linear Unbiased Estimate” NIM A500(2003)391,

•χ2/ndf = 4.8/7 = 0.69 •Run05 and run08 are consistent with each other. 18

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