hadronic resonance production in pb+pb collisions from the alice experiment
DESCRIPTION
Hadronic resonance production in Pb+Pb collisions from the ALICE experiment. Anders Knospe on behalf of the ALICE Collaboration The University of Texas at Austin 29 May 2012. Introduction f Yield K * 0 Mass and Width Hadron -Resonance Correlations Summary. Outline. - PowerPoint PPT PresentationTRANSCRIPT
Hadronic resonance production in Pb+Pb collisions
from the ALICE experimentAnders Knospe
on behalf of the ALICE CollaborationThe University of Texas at Austin
29 May 2012
2 Outline• Introduction• f Yield• K*0 Mass and Width• Hadron-Resonance Correlations• Summary
3 Introduction• Temperature and Lifetime of Fireball
– Resonance formation through recombination– Rescattering prevents resonance reconstruction– Statistical Model, UrQMD, fit to resonance/non-resonance ratios
• Chiral Symmetry Restoration– Resonances can be produced with jets in QGP– Produced off-shell or interact with medium mass shift– Interactions with medium width broadening (reduced lifetime)
• For T=250 MeV: f lifetime may change by up to factor of 10*
G. Torrieri and J. Rafelski, Phys. Lett. B 509 239 (2001)
Statistical Model
* L. Holt and K. Haglin, J. Phys. G31, S245 (2005)
4 Hadron-Resonance Correlations• To probe QGP: compare resonances that passed
through medium with those that did not– Hadron-resonance correlations
jet, le
ading
hadro
n
Resonance in near side: no medium interaction
Resonance in away side:Low pT (below ~2 GeV/c): dominated by interactions in hadronic mediumHigh pT: dominated by interactionswith early hadronic or partonic medium
Resonance transverse to jet:Thermal production in hadronic medium
Method proposed by:C. Markert, R. Bellwied, I. Vitev, Phys. Lett. B 669 92-97 (2008)
f Yield
6 Event & Track Selection• Pb+Pb collisions at
√sNN=2.76 TeV– 9.5 M events– |vz| < 10 cm
• fK-K+ (B.R.=0.489)• PID with TPC dE/dx:
|nsK|<2
TPC: PID and Tracking
ITS: Tracking
Centrality estimate: from measurement of multiplicity in V0 detector (scintillator arrays on each side of collision vertex)
7 Signal Extraction• Invariant mass
– |ypair|<0.5• Combinatorial Background
– Event Mixing (default)– Like-Sign
• Residual Background Fit: polynomial• Yield: integrate histogram, subtract
residual background• Peak Fit: res. back. + BW peak
– Find yield, mass, widthBACKGROUND SUBTRACTION
Background Fit Region(exact boundaries varied)
f Analysis
8 Uncorrected f Yields• Statistics up to pT~10 GeV/c• Coming for Quark Matter:
– Corrected Spectra– dN/dy– Ratios: f/p, f/K
Uncorrected f Yields
9 Particle Ratios• f/p:
– NA49 (17.5 GeV) and STAR (200 GeV): A+A higher than p+p
– PHENIX 200 GeV Au+Au• f/p = 0.015 ± 0.003• lower than STAR Au+Au• Consistent with STAR and
ALICE p+p– Ratio for p+p appears to saturate
at LHC energies: Is this also true for A+A?
• f/K: A single trend for both p+p and A+A over a wide energy range– Will Pb+Pb agree?– Au+Au 200 GeV:
• PHENIX f/K = 0.0911 ± 0.021• STAR higher than PHENIX
Lower energy: seePRC 71 064902 (2005) andPRC 79 064903 (2009)
?
?
K*0 Mass and Width
11 Signal Extraction• 3.4 M events• K*0p±K+ (BR=0.67)• PID with TPC dE/dx:
|nsp|<2, |nsK|<2• Calculate invariant mass of pK
pairs– rapidity cut: |ypair|<0.5
• Combinatorial Background:– Event Mixing– Like-Sign Pairs
• Fit signal: BW peak + linear background
• Uncorrected spectra:– Statistics up to pT~10 GeV/c– Corrected spectra for QM
2012
Uncorrected K*0
12 K*0 Mass and Width• No centrality dependence• Mass:
– High pT: Pb+Pb consistent with p+p and HIJING– Low pT: Pb+Pb consistent with p+p (deviation from PDG not due to medium)
– Low pT: Pb+Pb not consistent with HIJING• detector effects in simulation under investigation
• Width: consistent with simulation; no width change beyond 10 MeV/c2
K*0 Mass K*0 Width
13
Hadron-Resonance Correlations
14 Hadron-Resonance Correlations
Want to select for resonances produced early in collision and reduce contribution from hadronic phase: look for high-pT resonances in away side
C. Markert, R. Bellwied, I. Vitev, Phys. Lett. B 669 92-97 (2008)
15 Angular Correlations• Angular Correlation of trigger hadron with a f meson
– pT(h)>3 GeV/c– pT(f)>1.5 GeV/c
Pb+Pb
p+p
16 Mass and Width vs. Df
mass/expected value width/expected value
p+pp+p
Pb+Pb Pb+Pb
• f mass and width as a function of angle (Dφ) w.r.t. leading hadron
• pT(h)>3 GeV/c• pT(f)>1.5 GeV/c• Measured values divided
by expected value• No clear difference in
behavior between p+p and Pb+Pb
• In Pb+Pb: no mass shift or width broadening observed in away side
• However: f signal may be dominated by non-jet f for this pT range
12/9/2011
12/9/2011
12/9/2011 12/9/2011
17 Summary• K*0 and f signals observed in Pb+Pb collisions at 2.76 TeV
– Corrected f and K*0 spectra and ratios to non-resonances will be presented at Quark Matter 2012
• K*0 mass: Pb+Pb consistent with p+p and with HIJING at high pT
– any mass shift is not due to a medium effect• K*0 width: Pb+Pb consistent with HIJING• h-f correlations: away side looks like near side
– No mass shift or width broadening in away side– Will things be different for higher pT(f) or higher pT(trigger)?
• We do not observe the signatures of chiral symmetry restoration.