charge dependent azimuthal correlations in pb–pb collisions at √s nn = 2.76tev

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Charge dependent azimuthal correlations in Pb–Pb collisions at √s NN = 2.76TeV Panos Christakoglou 1,2 , for the ALICE Collaboration 1 NIKHEF 2 Utrecht University 27.05.2011 1 [email protected] - Quark Matter 2011, Annecy-France

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Charge dependent azimuthal correlations in Pb–Pb collisions at √s NN = 2.76TeV. Panos Christakoglou 1,2 , for the ALICE Collaboration 1 NIKHEF 2 Utrecht University. Motivation. Suggestions that heavy-ion collisions may form domains where the parity symmetry is locally violated - PowerPoint PPT Presentation

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Page 1: Charge dependent azimuthal correlations in Pb–Pb  collisions at √s NN  = 2.76TeV

Charge dependent azimuthal correlations in Pb–Pb collisions at √sNN = 2.76TeV

Panos Christakoglou1,2, for the ALICE Collaboration

1NIKHEF2Utrecht University

27.05.2011 [email protected] - Quark Matter 2011, Annecy-France

Page 2: Charge dependent azimuthal correlations in Pb–Pb  collisions at √s NN  = 2.76TeV

Motivation

Suggestions that heavy-ion collisions may form domains where the parity symmetry is locally violated

In non-central collisions, these domains may manifest themselves by a separation of charge, above and below the reaction plane.

The resulting charge separation is a consequence of two factorso the difference in numbers of quarks with positive and negative chiralities due to

a non-zero topological charge of the region,o the interaction of these particles with the extremely strong and short lived

magnetic field produced in such a collision (the Chiral Magnetic Effect). The existence of the CME, is directly related to the Chiral Symmetry

restoration and to weird B field effects

27.05.2011 [email protected] - Quark Matter 2011, Annecy-France 2

• D. Kharzeev, Phys. Lett. B633, 260 (2006). • D. Kharzeev and A. Zhitnitsky, Nucl. Phys. A797, 67 (2007).• D. E. Kharzeev, L. D. McLerran and H. J. Warringa, Nucl. Phys. A803, 227 (2008).• K. Fukushima, D. E. Kharzeev and H. J. Warringa, Phys. Rev. D78, 074033 (2008).

See also Dima’s talk on Monday at this session

Page 3: Charge dependent azimuthal correlations in Pb–Pb  collisions at √s NN  = 2.76TeV

Proposed tools: correlation analysis

Affected by the signal and the correlations both in and out-of-plane.

Sensitive also to detector effects

27.05.2011 [email protected] - Quark Matter 2011, Annecy-France 3

2–particle correlator 3–particle correlator

Measuring both correlators allows us to get an idea about the potential parity signal but also about the background contributionso Correlations in and out of plane

Background: Difference between the correlations projected onto an axis in the reaction plane and the ones projected onto an axis perpendicular to the reaction plane

Page 4: Charge dependent azimuthal correlations in Pb–Pb  collisions at √s NN  = 2.76TeV

Studies in ALICE: Analysis details

Analysis of the Pb-Pb events recorded in November/December 2010 during the first LHC heavy-ion runo Event sample split in two sets having

different magnetic field polarities (results used for the systematic uncertainties)

The trigger consists of the following criteria (at least two out of three):o two pixel chips hit in the outer layer of the

SPD,o signal in VZERO-A detector,o signal in VZERO-C detector.

27.05.2011 [email protected] - Quark Matter 2011, Annecy-France 4

For a description of the experimental setup, check Jurgen Schukraft‘s talk

The centrality is selected using the VZERO magnitude as the default estimatoro Centrality bins: 0-5%, 5-10%, 10-20%,

…,70-80%o Different centrality estimators (TPC tracks,

SPD clusters) investigates Results used for the systematic uncertainty

Due to the small magnitude of the potential signal, we need to have the acceptance corrections under control:o The TPC tracks provide a uniform

acceptance with minimal correctionso Disadvantage: contamination from

secondaries Investigated by varying the cut on the

distance of closest approach (results used for the systematic uncertainty).

For a description of the centrality determination, check Alberica Toia’s talk

Page 5: Charge dependent azimuthal correlations in Pb–Pb  collisions at √s NN  = 2.76TeV

ALICE 2–particle correlations: Centrality dependence

Correlations between opposite charges are positive and large

Correlations of same charged pairs are also positive and have a smaller magnitude

Results between (++) and (--) are consistent

27.05.2011 [email protected] - Quark Matter 2011, Annecy-France 5

(++) and (--) combined into one set of points (“Same charge”).

Similarity to STAR: the magnitude of the opposite charged pairs which is larger than the same charged ones.

Difference with STAR: o Sign of the same charged

correlations o Strength of the correlations

Page 6: Charge dependent azimuthal correlations in Pb–Pb  collisions at √s NN  = 2.76TeV

3-particle correlations

27.05.2011 [email protected] - Quark Matter 2011, Annecy-France 6

Page 7: Charge dependent azimuthal correlations in Pb–Pb  collisions at √s NN  = 2.76TeV

Three-particle correlators: Differential analysis in Δη

27.05.2011 [email protected] - Quark Matter 2011, Annecy-France

Charge separation starts to develop when moving away from the most central bins

Correlations between opposite charges are smaller than those between same charges

Correlation width Δη = |ηα - ηβ|~1

Page 8: Charge dependent azimuthal correlations in Pb–Pb  collisions at √s NN  = 2.76TeV

Three-particle correlators: Differential analysis in ΔpT

27.05.2011 [email protected] - Quark Matter 2011, Annecy-France

Correlations not localized in small values of ΔpT

o Contribution from short range correlations of same/opposite charges limited?

Page 9: Charge dependent azimuthal correlations in Pb–Pb  collisions at √s NN  = 2.76TeV

Three-particle correlators: Differential analysis in sum pT

27.05.2011 [email protected] - Quark Matter 2011, Annecy-France

Correlations of same charges have larger signal with increasing transverse momentum of the pair contrary to the expectation from theory (i.e. signal localized at the low pT region)

D. Kharzeev et al., Nucl. Phys. A803, 227 (2008)

Page 10: Charge dependent azimuthal correlations in Pb–Pb  collisions at √s NN  = 2.76TeV

Centrality dependence: Charge combinations

Clear charge separation observed Results for (++) and (--) consistent (combined in the next plots into one “Same

charge” point) The magnitude of the correlations between the same charged pairs is larger

than the one of the opposite charges (excluding the last bin)

27.05.2011 [email protected] - Quark Matter 2011, Annecy-France 10

Page 11: Charge dependent azimuthal correlations in Pb–Pb  collisions at √s NN  = 2.76TeV

Different methods: event plane estimation

27.05.2011 [email protected] - Quark Matter 2011, Annecy-France 11

TPC

VZERO

ZDC

Investigation with four independent methods

For further details on the ZDC and the VZERO check the talk of Ilya Selyuzhenkov

Page 12: Charge dependent azimuthal correlations in Pb–Pb  collisions at √s NN  = 2.76TeV

Centrality dependence: Comparison of methods

27.05.2011 [email protected] - Quark Matter 2011, Annecy-France 12

Very good agreement between the four methods

Page 13: Charge dependent azimuthal correlations in Pb–Pb  collisions at √s NN  = 2.76TeV

Integrated 3-particle correlator: LHC vs RHIC

27.05.2011 [email protected] - Quark Matter 2011, Annecy-France 13

Stat. error: error barsSyst. error: shaded area

Magnitude of the effect seems to be similar to what is reported by STAR. Most theories predict a much lower effect at LHC energies.

o Signal and background should both scale with the square of the multiplicity

The effect can be similar depending on the t0 of the magnetic field (D. Kharzeev et al., Nucl. Phys. A803, (227) 2008)

STAR Collaboration: Phys. Rev. Lett. 81, 251601 (2009) STAR Collaboration: Phys. Rev. C81, 054908 (2010)

Page 14: Charge dependent azimuthal correlations in Pb–Pb  collisions at √s NN  = 2.76TeV

Comparison of 2– and 3–particle correlators

27.05.2011 [email protected] - Quark Matter 2011, Annecy-France 14

STAR Collaboration: Phys. Rev. C81, 054908 (2010)

STAR’s 2-particle correlations for same charged pairs have the same magnitude as the points coming from the 3-particle correlation analysis.o Larger magnitude of the correlations in than out of plane?

ALICE data demonstrate a larger magnitude of the 2-particle correlations but also a change in signo Differences in the correlations vs reaction plane between energies?o Larger magnitude of the correlations out of than in plane?

Page 15: Charge dependent azimuthal correlations in Pb–Pb  collisions at √s NN  = 2.76TeV

Integrated 3-particle correlator: Comparison with models

27.05.2011 [email protected] - Quark Matter 2011, Annecy-France 15

HIJING points consistent with the (+-) data pointso HIJING w/o flow consistent with each other

HIJING points scaled with the square of the multiplicity, consistent with the idea of having the correlations originating from emerging clusters (jets, resonances)

V.D. Toneev and V. Voronyuk, arXiv:1012.1508v1 [nucl-th]

S. A. Voloshin, Phys. Rev. C 70, 057901 (2004).

The only published prediction for LHC energies (@4.5 TeV)

According to the authors the magnitude should roughly scale with 1/√so Applied in the figure to convert the prediction to √sNN

= 2.76 TeV

Page 16: Charge dependent azimuthal correlations in Pb–Pb  collisions at √s NN  = 2.76TeV

Summary and outlook

The possibility of observing parity odd domains was investigated by using both a 2-particle and a 3-particle P-even correlator.

The results from the 2-particle correlator studies show that the sign of the correlations is the same regardless of the charge combination, contrary to what was observed in STARo Change in the correlation pattern vs reaction plane?

The results of the 3-particle correlator indicate that:o the signal has a hadronic width of one unit in η,o doesn’t have any obvious contribution from short range correlations (i.e.

HBT),o increases with increasing pair pt.

The centrality dependence of the integrated 3-particle correlator illustrates a remarkable agreement in both the magnitude and the behavior with the results reported by STAR in Au-Au collisions at √sNN = 0.2 TeV

The majority of models predict a smaller signal at LHC energies.

27.05.2011 [email protected] - Quark Matter 2011, Annecy-France 16

Theory is challenged by the latest findings; looking forward to the feedback from the theory community!!!

Page 17: Charge dependent azimuthal correlations in Pb–Pb  collisions at √s NN  = 2.76TeV

BACKUP

27.05.2011 [email protected] - Quark Matter 2011, Annecy-France 17

Page 18: Charge dependent azimuthal correlations in Pb–Pb  collisions at √s NN  = 2.76TeV

What we know so far…(STAR)

27.05.2011 [email protected] - Quark Matter 2011, Annecy-France 18

Correlations between opposite charges are positive and large

Correlations of same charged pairs are negative and have a significantly smaller magnitude

STAR Collaboration: Phys. Rev. C81, 054908 (2010)

Differential analysis of the 3-particle correlator indicates that the signal:o increases with increasing pt of the pair,o has a hadronic width of one unit in η,o demonstrates a weak dependence on the pair’s pt difference

Differences in the correlations of same and opposite charged pairs.o The sign follows the one of the 2-particle correlatoro The magnitude of the correlations of same charged pairs is

larger than the one of opposite charged particleso None of the studied models describe the data

STAR Collaboration: Phys. Rev. Lett. 81, 251601 (2009)

Page 19: Charge dependent azimuthal correlations in Pb–Pb  collisions at √s NN  = 2.76TeV

ALICE 2–particle correlations: Differential analysis

Correlations have the same behavior regardless of the charge combination.

Change of sign @ ~2 GeV/c Change of physics @ ~5

GeV/c in ΔpT

27.05.2011 [email protected] - Quark Matter 2011, Annecy-France 19

Correlations localized in η Different charge

combinations have the same correlations in sign but not in magnitude.

Page 20: Charge dependent azimuthal correlations in Pb–Pb  collisions at √s NN  = 2.76TeV

Summary and outlook

The possibility of observing parity odd domains was investigated by using both a 2-particle and a 3-particle P-even correlator.

The results from the 2-particle correlator studies show that:o there is a change in physics at Δpt~5GeV/c, which is already seen by

other analyses (flow, RAA),

o the sign of the correlations is the same regardless of the charge combination, contrary to what was observed in STAR

Change in the correlation pattern vs reaction plane? The results of the 3-particle correlator indicate that:

o the signal has a hadronic width of one unit in η,o doesn’t have any obvious contribution from short range correlations

(i.e. HBT),o increases with increasing pair pt.

The centrality dependence of the integrated 3-particle correlator illustrates a remarkable agreement in both the magnitude and the behavior with the results reported by STAR in Au-Au collisions at √sNN = 0.2 TeV

The majority of models predict a smaller signal at LHC energies.

27.05.2011 [email protected] - Quark Matter 2011, Annecy-France 20

Theory is challenged by the latest findings; looking forward to the feedback from the theory community!!!