open heavy flavor results from phenix

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Open Heavy Flavor Results from PHENIX Laura Patel for the PHENIX Collaboration Georgia State University

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Open Heavy Flavor Results from PHENIX. Laura Patel for the PHENIX Collaboration Georgia State University. Outline. Motivation & Background PHENIX Heavy Flavor (HF) Results p+p (charm & bottom cross sections) Heavy Ion (Cu+Cu, Au+Au) d+Au Summary. Motivation. - PowerPoint PPT Presentation

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Page 1: Open Heavy Flavor Results from PHENIX

Open Heavy Flavor Results from PHENIX

Laura Patelfor the PHENIX Collaboration

Georgia State University

Page 2: Open Heavy Flavor Results from PHENIX

Outline

• Motivation & Background

• PHENIX Heavy Flavor (HF) Results

• p+p (charm & bottom cross sections)

• Heavy Ion (Cu+Cu, Au+Au)

• d+Au

• Summary

DIS (4/24/13) 2 L. Patel (GSU)

Page 3: Open Heavy Flavor Results from PHENIX

Motivation

• Heavy quarks can be used to probe medium properties.

• Heavy quarks are produced early in the collision due to their large mass (~4.2 GeV for b and ~1.3 GeV for c).

• Heavy quark production can be used as a test of pQCD theory.

DIS (4/24/13) 3 L. Patel (GSU)

Page 4: Open Heavy Flavor Results from PHENIX

Quantifying Medium Effects

• Nuclear modification factors:

DIS (4/24/13) 4 L. Patel (GSU)

RAA =dNAA /dpT

Ncoll × dN pp /dpT

RCP =

dNAA /dpT

< Ncoll > (central)

dNAA /dpT

< Ncoll > (peripheral)

R < 1 (suppression)

R > 1 (enhancement) R = 1 (no medium effect or balance)

p+p measurements A+A measurements

Ncoll Averaged number of binary collisions

d+A measurements

Baseline probe CNM effects probe HNM+CNM effects

Page 5: Open Heavy Flavor Results from PHENIX

Relativistic Heavy Ion Collider

DIS (4/24/13) 5 L. Patel (GSU)

PHENIX

STAR

Page 6: Open Heavy Flavor Results from PHENIX

Forward rapidity arms:Muons•1.2<|η|<2.2• pμ > 1 GeV/c• Δφ = 2π

PHENIX

DIS (4/24/13) 6 L. Patel (GSU)

Central arms:Hadrons, photons, electrons•|η|<0.35• pe > 0.2 GeV/c• Δφ=π(2 arms x π/2)

Page 7: Open Heavy Flavor Results from PHENIX

Open Heavy Flavor Measurements

• Indirect measurement of charm and bottom through semi-leptonic decay.

• Electrons at mid-rapidity

• Muons at forward/backward rapidity

DIS (4/24/13) 7 L. Patel (GSU)

cc €

D0

D 0

l+

K −

X

X '

K +€

l−€

bb

B

B€

l+

D €

X

X '

D€

l−

Y

l+

Page 8: Open Heavy Flavor Results from PHENIX

Single Leptons in p+p at 200 GeV

• e and baseline measurements in central and forward rapidity

DIS (4/24/13) 8 L. Patel (GSU)

• Consistent with FONLL upper limit

PRL 97, 252002 (2006)

Page 9: Open Heavy Flavor Results from PHENIX

Charm & Bottom Cross Sections

• PHENIX has multiple measurements for charm and bottom production.

• All are in agreement with pQCD values.

DIS (4/24/13) 9 L. Patel (GSU)

Page 10: Open Heavy Flavor Results from PHENIX

Cu+Cu at 200 GeV

• Cu+Cu collisions provide a cross over between d+Au and Au+Au.

• The medium created in central Cu+Cu collisions has a different density than central Au+Au

DIS (4/24/13) 10 L. Patel (GSU)

Ncoll=1

Ncoll~1000

d+AuCu+Cu

Au+Au

Page 11: Open Heavy Flavor Results from PHENIX

Single Leptons in Cu+Cu

• Suppression of muons from HF in most central collisions.

DIS (4/24/13) 11 L. Patel (GSU)

Phys. Rev. C 86, 024909 (2012)

• Larger suppression at forward rapidity.

• Additional CNM effects are expected at forward rapidity.

Page 12: Open Heavy Flavor Results from PHENIX

Single Leptons in Au+Au

• Use single electrons from HF to study the medium.

DIS (4/24/13) 12 L. Patel (GSU)

• Suppression in Au+Au for pT>1.5 GeV.

PRC 84, 044905 (2011)

• No suppression in d+Au

• Suppression in Au+Au must be due to HNM effects.

PRC 84, 044905 (2011)

PRL 109, 242301 (2012)

Page 13: Open Heavy Flavor Results from PHENIX

Disentangling Cold Nuclear Matter Effects

• Difficult to conclude much in heavy ion collisions without a thorough understanding of CNM.

• d+Au collisions provide an environment to probe CNM effects!

• No QGP is expected to form.

DIS (4/24/13) 13 L. Patel (GSU)

Page 14: Open Heavy Flavor Results from PHENIX

Cold Nuclear Matter Effects

DIS (4/24/13) 14 L. Patel (GSU)

• Nuclear PDF is modified: Shadowing, Anti-shadowing, EMC, Saturation

low x high x

• Gluon saturation

• Unlike quarkonia, there are no final state breakup effects!

Page 15: Open Heavy Flavor Results from PHENIX

Single HF Leptons in d+Au

DIS (4/24/13) 15 L. Patel (GSU)

PRL 109, 242301 (2012)

• RdA ~1 in peripheral collisions

• Enhancement in central collisions

• Suppression in the d-going direction• Enhancement in the Au-going direction, similar to central region

Page 16: Open Heavy Flavor Results from PHENIX

Future Work

• A more detailed understanding of heavy quark energy loss requires separation of charm and bottom.

• To accomplish, this PHENIX recently installed two silicon vertex tracker detectors.

DIS (4/24/13) 16 L. Patel (GSU)

VTX ( commissioned in 2011) and FVTX (commissioned 2012)

VTX+FVTX

Page 17: Open Heavy Flavor Results from PHENIX

PHENIX (F)VTX

• VTX installed in Run-11 & FVTX in Run-12.

• Will allow separation of B & D.

• New results coming soon!DIS (4/24/13) 17 L. Patel (GSU)

Page 18: Open Heavy Flavor Results from PHENIX

Summary

• PHENIX has multiple measurements for heavy flavor cross sections in p+p.

• Heavy ion results show suppression beyond that expected from CNM.

• d+Au results show some some rapidity dependent modification in open heavy flavor.

• Quantifying the HNM effects is an ongoing process.

DIS (4/24/13) 18 L. Patel (GSU)

Page 19: Open Heavy Flavor Results from PHENIX

Backup

DIS (4/24/13) 19 L. Patel (GSU)

Page 20: Open Heavy Flavor Results from PHENIX

Single e Signal Extraction

DIS (4/24/13) 20 L. Patel (GSU)

Cocktail method

Dominated by uncertainty on pion spectra

Converter method

Dominated by low stats of conv-in data (1 day)

noninconv

nonoutconv

NNRN

NNN

)1(

Excellent agreement between two independent methods

Page 21: Open Heavy Flavor Results from PHENIX

Single Muon Analysis

• Background

• Decay muons from light vector mesons

• Punch through hadrons

• Hadron cocktail input tuned to match data distributions

• Decay muon z-vertex dependence

• “stopped” hadron spectra

DIS (4/24/13) 21 L. Patel (GSU)

Page 22: Open Heavy Flavor Results from PHENIX

Previous Single Lepton Results in p+p

DIS (4/24/13) 22 L. Patel (GSU)

Page 23: Open Heavy Flavor Results from PHENIX

Dielectron Analysis p+p at 200 GeV

• Use simulation for each component.

• Excellent agreement between data and cocktail.

DIS (4/24/13) 23 L. Patel (GSU)

Phys. Lett. B 670, 313 (2009)

Page 24: Open Heavy Flavor Results from PHENIX

Dielectron Analysis p+p at 200 GeV

• Cocktail subtraction leaves only continuum contributions.

• Simultaneously fit the charm & bottom components. (DY is fixed)

• Use Pythia to extrapolate a total cross section.

• Cross Sections:

DIS (4/24/13) 24 L. Patel (GSU)

σcc = 544 ± 39(stat) ±142(sys) ± 200(model)μb

σbb

= 3.9 ± 2.4(stat)−2+3(sys)μb

Phys. Lett. B 670, 313 (2009)

Page 25: Open Heavy Flavor Results from PHENIX

Like-sign Dimuon Analysis p+p at 500 GeV

• Like-sign technique: contains combinatorial and correlated signal.

• Event mixing technique: contains only combinatorial signal.

DIS (4/24/13) 25 L. Patel (GSU)

N±±corr = N±±

like - N±±mixed

Correlated Like-Sign Signal

• Use like-sign dimuons to calculate total cross section

Page 26: Open Heavy Flavor Results from PHENIX

Like-sign Dimuon Analysis p+p at 500 GeV

• Use simulation to get line shapes.

• Simultaneous fit of two components:

DIS (4/24/13) 26 L. Patel (GSU)

F(m) = p0 exp(−m / p1) + p2 exp(−m / p3)

Hadronic backgroundcontribution

Open Bottomcontribution

Cross Section:

σbb

= 25.2 ± 3.2(stat)−9.5+11.4 (sys)μb

• Extrapolate to total cross section using Pythia.

Page 27: Open Heavy Flavor Results from PHENIX

Heavy Ion Collisions- Mass Spectra

Diverse Physics Signatures

• Low mass: sensitive to chiral symmetry restoration

• Intermediate mass: thermal radiation, modification of open charm & charmonia

• High mass: modification of open bottom & Upsilon

DIS (4/24/13) 27 L. Patel (GSU)