Charmonia production in ALICE

# Charmonia production in ALICE

Christophe Suire for the ALICE Collaboration Institut de Physique Nucléaire d’Orsay, CNRS-IN2P3, Université Paris-Sud, France
###### Abstract

Quarkonia states are expected to provide essential information on the properties of the high-density strongly-interacting system formed in the early stages of high-energy heavy-ion collisions. ALICE is the LHC experiment dedicated to the study of nucleus-nucleus collisions and can study charmonia at forward rapidity () via the decay channel and at mid rapidity () via the decay channel. In both cases charmonia are measured down to zero transverse momentum. The inclusive  production as a function of transverse momentum and rapidity in pp collisions at 2.76 and 7 TeV are presented. For pp collisions at 7 TeV, the inclusive  production as a function of the charged particle multiplicity, the inclusive  polarization at forward rapidity and the  prompt to non-prompt fraction are discussed.

Finally, the analysis of the inclusive  production in the Pb-Pb data collected fall 2011 at a center of mass energy of TeV is presented. Results on the nuclear modification factor are then shown as a function of centrality, transverse momentum and rapidity and compared to model predictions. First results on inclusive  elliptic flow are given.

###### keywords:
Hadron-induced high- and super-high-energy interactions, Relativistic heavy-ion collisions, Quark-Gluon plasma,  production and suppression mechanisms.

## 1 Charmonia in heavy-ion collisions

Charmonia suppression via color-screening of the heavy-quark potential was originally proposed as a probe of the QCD matter formed in relativistic heavy-ion collisions in 1986 Matsui:1986dk ().  production was extensively studied at the Super Proton Synchrotron (SPS) and at the Relativistic Heavy Ion Collider (RHIC). Indeed,  suppression in most central heavy-ion collisions was observed over a large energy range ( 20 to 200 GeV/). The LHC has opened a new energy regime for the study of quarkonium in heavy-ion collisions. In a Pb-Pb collision at TeV, an average of one  particle is expected to be produced in every central Pb-Pb collision, together with about 100 c pairs. Several models BraunMunzinger:2000px (); Thews:2000rj (); Andronic:2007bi (); Zhao:2007hh () have included, already at RHIC energy, a  regeneration component from deconfined charm quarks in the medium which counteracts the J/ suppression in a QGP. At LHC, this regeneration component may become important, even dominant.

The in-medium modification of the  production can be quantified with the nuclear modification factor , defined as the  yield measured in nucleus-nucleus collisions divided by the yield measured in pp collisions and the number of binary nucleon-nucleon collisions occurring in the nucleus-nucleus collision. To interpret the , one must keep in mind the following points. First, prompt  production in hadronic interactions consists of the sum of direct  ( 65%) and excited states such as and ( 35%). Since the and have lower dissociation temperatures than the , a   measurement around 0.65 is compatible within errors with the suppression of excited states only. In addition to these prompt   one should also take into account that a non-prompt component from beauty hadron decays is present at LHC energy. The  includes cold nuclear matter (CNM) effects, dominated by nuclear absorption and (anti-) shadowing. These CNM effects can be responsible for  suppression independently from the creation of a deconfined medium. To quantify CNM effects, proton-nucleus collisions are needed. At SPS energy, the observed  suppression would be compatible with the dissociation of excited states, once the CNM effects are taken into account. At RHIC, a   of 0.25 in most central Au-Au collisions was measured by the PHENIX experiment Adare:2006ns () with a strong centrality dependence. After estimating the correction due to the CNM effects, the suppression of direct  is at least 40% or more. At the LHC,  are abundantly produced and detailed studies of its production are possible in both elementary and heavy-ion collisions, such as azimuthal asymmetry, polarization, dependence on rapidity and on transverse momentum, etc. Such studies may give us some answers about the balance between suppression and recombination mechanisms of .

The asymmetry the azimuthal distribution of  in the plane perpendicular to the beam direction, the so-called elliptic flow or vis indeed a very interesting experimental observable. When heavy-ions collide at finite impact parameter (non-central collisions), the geometrical overlap region and therefore the initial matter distribution is anisotropic and is converted into a momentum anisotropy of the produced particles. The possible onset of  production via recombination mechanisms should be, according to models, accompanied with a non-zero or possibly large v value Liu:2009gx () at low . Indeed, if charm quarks reach some level of thermalization in the medium, they may acquire an elliptic flow that can be further transferred to the  assuming the  is formed via recombination.

In the following section, the ALICE experiment and the data samples will be described. Then,  production results in pp collisions at 2.76 TeV and 7 TeV will be presented. The  production in Pb-Pb collisions at 2.76 will be studied through the  dependence on centrality,  and . Finally,  elliptic flow measurement will be shown.

## 2 Experimental apparatus and data sample

ALICE is a general purpose heavy-ion experiment and is described in Aamodt:2008zz (). It consists of a central part covering the pseudo-rapidity and a muon spectrometer covering . At forward (mid) rapidity,  production is measured in the dimuon (dielectron) decay channel; in both cases the  coverage extends down to zero. Only detectors that are relevant to the analysis will be presented.

At mid rapidity, the   analysis makes use of the high precision tracking and particle identification of the Inner Tracking System (ITS) and the Time Projection Chamber (TPC). The ITS consists of six cylindrical layers of silicon detectors; at a radius 3.9 and 7.6 cm, the first two layers are equipped with silicon pixels (SPD), then two layers of silicon drifts at radius 15 and 23.9 cm and finally, two layers of silicon strips at radius 38 and 43 cm. Its main tasks are the primary and secondary vertex reconstruction; the resolution on the primary vertex ranges from 100 m (pp collisions) to 10 m (central Pb-Pb collisions). The SPD has triggering capabilities and can provide a signal at level 0. The large cylindrical TPC has full azimuthal coverage and extends from z = -2.50 m to z = 2.50 m 111The z axis is defined here as the beam line axis in the counter clockwise direction and its origin is at the center of the ALICE detector.. The TPC radial coverage ranges from r = 85 cm to r = 247 cm. This large drift detector is the main track reconstruction device at central rapidity since it can provide up to 159 space points per track. Particle identification (PID) is achieved via the measurement of the specific energy loss (dE/dx) of particles in the detector gas (Ne/CO/N). The excellent dE/dx resolution of 5% allows to identify electrons by using inclusion cut around the Bethe-Bloch fit for electrons and exclusion cuts for protons and pions. ALICE has further capabilities to improve electron identification and triggering thanks to the Time-Of-Flight (TOF), the Transition Radiation Detector (TRD) and the Electromagnetic Calorimeter (EMCAL) detectors. However, these detectors have not been used in the analysis presented here.

At forward rapidity (  ) the production of quarkonium states is measured in the muon spectrometer 222In the ALICE reference frame, the muon spectrometer covers a negative range and consequently a negative range. We have chosen to present our results with a positive notation.. The spectrometer consists of a ten interaction length thick absorber ( -0.9 m z -5.0 m) filtering the muons in front of five tracking stations (MCH) made of two planes of cathode pad chambers each. The third station is located inside a dipole magnet with a 3 Tm field integral. The MCH chambers are positioned between z=-5.2 and z=-14.4 m. The tracking apparatus is completed by a triggering system (MTR) made of two stations, located at z=-16.1 and z=-17.1 m, each equipped of two planes of resistive plate chambers. The MTR chambers are downstream of a 1.2 m thick iron wall, which absorbs secondary hadrons escaping from the front absorber and low momentum muons coming mainly from and K decays. Throughout its full length, a conical absorber made of tungsten, lead and steel protects the muon spectrometer against secondary particles produced by the interaction of large- primaries in the beam pipe. The forward VZERO detectors, two arrays of 32 scintillator tiles covering the range (VZERO-A) and (VZERO-C), are positioned at z=340 and z=-90 cm. And finally, the zero degree calorimeters (ZDC) placed 116 m down and up-stream ALICE can detect spectator neutrons and protons.

In proton-proton collisions, the minimum bias (MB) trigger uses information of the SPD and VZERO detectors. It is defined as the logical OR of the three following conditions: (i) a signal in two readout chips in the outer layer of the SPD, (ii) a signal in VZERO-A, (iii) a signal in VZERO-C. This MB trigger requires the coincidence of the crossing of two proton bunches at the experiment interaction point (IP). ALICE MB trigger selects about 86% of the proton-proton inelastic cross section. Specific cross sections were measured during van der Meer scan in pp collisions at 7 and 2.76 TeV and allowed to determine the absolute normalization of the inclusive  cross section. The muon minimum bias trigger (-MB) requires, in addition to the MB conditions given above, a signal in the MTR system. The MTR can reconstruct a trigger track, determine its  and select different thresholds (  0.5, 1 and 4 GeV/). The -MB trigger helps to take advantage of the full luminosity delivered by the LHC in the muon spectrometer. The MB trigger used in Pb-Pb collisions collected in 2010 requires the logical AND of the conditions (i),(ii) and (iii) given above. The centrality of the collision is determined from the amplitude of the VZERO signal fitted with a geometrical-Glauber model PhysRevLett.106.032301 (). In 2011, the MB conditions were reduced to the AND of conditions (ii) and (iii) but additional requirements were added to select rare events. In particular, event multiplicity and dimuon triggers were added and ZDC were used for rejecting electromagnetic Pb-Pb interactions and satellite Pb-Pb collisions. Once the centrality selection cut has been applied, triggers are fully efficient with negligible contamination.

## 3 J/ψ production in pp collisions

The  production in pp collisions is extensively studied in ALICE and only a selection of the available results will be presented in this section. Further details on the related analysis can be found in Geuna:hp2012 ().

The inclusive  production was measured in pp collisions at 7 TeV in the dimuon and dielectron channels in the rapidity ranges and down to  = 0. The analysis was made with an integrated luminosity in the dimuon (dielectron) channel. The measured cross section values are and . At forward rapidity differential cross section d/dd measurement from ALICE fully overlaps with LHCb and a good agreement is found. At mid rapidity, the situation is different since ATLAS and CMS cannot measure  with   6 GeV/. Thus combining ALICE and CMS/ATLAS data offers a rather complete inclusive  production measurement over a large rapidity range. These comparisons are available in Aamodt:2011gj ().

The same analysis was carried out with pp collisions at 2.76 TeV collected in March 2011. Since the center of mass energy per nucleon-nucleon collisions is identical to the one of the Pb-Pb collisions, this analysis provides an essential reference data to measure the  nuclear modification factor. The integrated luminosity for the analysis is in the dimuon (dielectron) channel. The integrated cross sections are and . Note that the uncertainties quoted here on the pp measurement are one of the main source of uncertainty of the nuclear modification factor discussed in the next section. The differential cross sections d/dd have been extracted down to  = 0 at both rapidities. These results are compared to a theoretical model, NRQCD calculation that includes Color Singlet and Color Octet terms at NLO, which describes reasonably well the measurement at 2.76 TeV and also the one at 7 TeV Aamodt:2011tmp ().

In the previous results, one could remark that the  cross section has a large uncertainty related to the unknown polarization. ALICE has studied  polarization in pp collisions 7 TeV in the dimuon channel. Measurements of the polar and azimuthal angle distributions of the decay muons allowed us to extract the  polarization for 2   8 GeV/ and 2.5   4. The parameters describing the  polarizations are consistent with zero in the kinematic range under study Abelev:2011md (). This measurement is, at the present date, the only  polarization measurement at the LHC. It is crucial in the near future to extend the polarization measurement down to zero  and to high  in order to provide more stringent tests to theoretical calculations. In addition, since the pp cross section enters the nuclear modification factor calculation, the polarization, if different from zero, may have a strong impact at low transverse momentum. Such a measurement needs a large statistic and strengthens the requirement to collect a large amount of data at the same center of mass energy as the Pb-Pb collisions.

An interesting feature of the  production in pp collisions at 7 TeV arises from its dependence on the charged particle multiplicity. The d/d is calculated from the number of tracks reconstructed in using pairs of hits (tracklets) in the SPD. These measurements were performed at both rapidities in the dimuon and dielectron channels. Expressed in terms of the relative  yield as a function of the relative charged multiplicity , a linear increase is clearly seen at both rapidities. For (), the relative  yield is enhanced by a factor of about 5 at forward rapidity and about 8 at mid rapidity. This trend is not reproduced by PYTHIA 6.4.25 in the Perugia 2011 tune which exhibits an opposite tendency, i.e. a decrease of the  multiplicity with respect to the event multiplicity Abelev:2012rz (). One could infer that the  production is strongly connected with the underlying hadronic activity. Whether this hadronic activity comes from multiple parton interactions remains an open question. Further investigations are needed to better understand this measurement that challenges our understanding of the  production in pp collisions. In particular, the event multiplicity dependence should be completed by the  dependence and extended to the open charm cross section (e.g. D mesons).

All the results presented up to now refer to inclusive  production which sums three distinct contributions: the prompt  produced directly in the pp collisions, the prompt  produced indirectly via the decay of heavier charmonia states and the non-prompt  produced in the decay of beauty hadrons. At central rapidity (), the measurement of the non-prompt  was achieved in pp collisions at 7 TeV for   GeV/. This measurement is only accessible in ALICE since the other experiments cannot detect  at mid rapidity below a  of 6.5 GeV/ where most of the cross section lies. The integrated luminosity for the analysis is . This measurement relies on the discrimination of  produced detached from the primary vertex of the pp collisions thanks to the good spatial resolution of the ITS. By fitting simultaneously the invariant mass spectra and the pseudo-proper decay length of the reconstructed , one can can measure the relative abundances of prompt and non-prompt , and the background. The fraction of  from beauty hadrons () in the measured kinematic range is about 15% with a strong  dependence. Then, is combined with the the inclusive  cross section measured in  Aamodt:2011gj () to extract the prompt  cross section . Comparisons with models lead to a good description of the prompt  dependence with  and of the total beauty cross section Abelev:2012gx ().

## 4 Nuclear modification factor in Pb-Pb collisions at √sNN= 2.76 TeV

Inclusive  production was studied in Pb-Pb collisions at 2.76 TeV at mid and forward rapidity in the dielectron and dimuon decay channels using respectively an integrated luminosity 2.1 and b. A crucial feature of the ALICE detector is to measure, in both channels, the  production down to  = 0 GeV/c. The large data sample analyzed in the dimuon channel allowed us to perform differential analysis of the nuclear modification factor () as function of centrality, , and . In the dielectron channel, only the centrality dependence in 3 centrality classes (0–10%, 10–40% and 40–80%) could be achieved. One should note that the acceptance times efficiency factor in the dielectron (dimuon) channel is quite high () and weakly depends on the collision centrality with a maximum relative loss of 12% (8%) from peripheral to most central collisions. Details on both analysis are given in Wiechula:hp2012 ().

On the left side of Fig. 1, the inclusive   is shown as a function of the number of nucleons participating in the collision PhysRevLett.106.032301 () at mid and forward rapidity. At forward rapidity, a clear suppression is seen for   with almost no centrality dependence. These results show a good agreement with the ones published in PhysRevLett.109.072301 () based on b collected in 2010. At mid rapidity, a similar pattern could be possible but the coarser centrality classes and larger uncertainties prevent to draw any firm conclusion. The centrality integrated   at forward and mid rapidity are and . In both cases, the systematic uncertainty is dominated by the pp reference. On the right side of Fig. 1, the centrality dependence of   at high- is compared between ALICE and CMS Chatrchyan:2012np (). A larger suppression,  , is measured in the most central collisions with a clear centrality dependence. One could see here an indication that the   is  dependent at forward rapidity and possibly at mid rapidity; selecting high-  drives down the .

The  dependence of the   is confirmed and can be better observed in Fig. 2 (left side). The inclusive   is shown as a function of  for the 0%–90% most central Pb-Pb collisions and exhibits a decrease from 0.6 to 0.35 approximately. At high-  a rather direct comparison with CMS results Chatrchyan:2012np () is possible; the only difference is that the CMS measurement covers a more central rapidity range (). A reasonable agreement between the two measurements is found for high-  . For  smaller than 4 GeV/, the difference with PHENIX measurement Adare:2011yf () is striking. The PHENIX result concern the 0%–20% most central Au-Au collisions whereas the ALICE result is for a much wider centrality range (0%–90%). However, the bulk of the  production () occurring in 0%–20% most central collisions, the comparison remains meaningful. In addition, work is ongoing to extract the  versus  in smaller centrality classes.

The   dependence on rapidity has been measured over a wide range thanks to the combination of our measurement in the central barrel and in the muon spectrometer, and is displayed on the right side of Fig. 2. At forward rapidity, the   decreases by from to . The measurement at mid rapidity, because of its large uncertainties, does not allow to draw a clear conclusion but hints towards a rather flat behavior between  = 2.5 and  = 0. On the same figure, an estimate of the   due only to shadowing effects is given for two models. Indeed at LHC energies, modification of the gluon distribution function is dominated by shadowing effects Lourenco:2008sk (). The first model is a Next to Leading Order calculation within the Color Evaporation Model Vogt:2010aa () with the EPS09 nuclear PDF (nPDF). The second model is a Leading Order calculation within the CS Model Ferreiro:2011rw () with the nDSg nPDF. In the first model, the upper and lower limits correspond to the uncertainty of the EPS09 nPDF, and in the second model the band covers the uncertainty in the factorization scale of the for nDSg PDF.

One could not exclude that shadowing effects are responsible for a large part of the  suppression observed in  from  = 0 to   3, this would imply that the expected color screening  suppression observed at lower energy (RHIC) or higher  (CMS) is either small or compensated by recombination mechanisms. In the rapidity range from 3 to 4, our results show that the suppression goes beyond the shadowing-only prediction given by models with our current knowledge of nPDF.

The influence of the contribution of beauty hadron feed-down to the inclusive  yield in our  and  range was estimated. Non-prompt  are indeed different since their suppression or production is insensitive to color screening or recombination phenomena that are expected to occur in the hot and dense medium created in the Pb-Pb collisions. The beauty hadron decay mostly occurs outside the fireball, and a measurement of the non-prompt   is connected to the beauty quark in-medium energy loss. At forward rapidity, the non-prompt  was measured by the LHCb collaboration to be about 10% in pp collisions at TeV Aaij:2011jh () in our  range. Assuming the scaling of beauty production with the number of binary nucleon-nucleon collisions and neglecting the shadowing effects, the prompt   would be, and this is an upper limit, 11% smaller than our inclusive measurement. To estimate the influence of non-prompt  as a function of  and  on our inclusive  measurement, we have extrapolated the LHCb measurement at TeV down TeV using an center of mass energy dependence extracted from CDF and CMS data. Assuming a range of energy loss for the beauty quarks from (b) = 0.2 to (b)= 1, we have found that the  from beauty hadrons have a negligible influence on our measurement.

In Fig. 3, our   measurement is compared with theoretical models that all include a  regeneration component from deconfined charm quarks in the medium.

The Statistical Hadronization Model BraunMunzinger:2000px (); Andronic:2011yq () assumes deconfinement and a thermal equilibration of the bulk of the c pairs. Then, charmonium production occurs only at phase boundary by statistical hadronization of charm quarks. The prediction is given for two values of since no measurements are available at this rapidity for Pb-Pb collisions. The two transport model results Zhao:2011cv (); Liu:2009nb () presented in the same figure differ mostly in the rate equation controlling the  dissociation and regeneration. Both are shown as a band that connects the results obtained with (lower limit) and without (higher limit) shadowing and can be interpreted as the uncertainty of the prediction. The model from Zhao & al. implements a simple shadowing estimate leading to a 30% suppression in most central Pb-Pb collisions. The charm cross-section dd at is mb and the  from beauty hadrons is estimated at 10% and no quenching is assumed. The model from Liu & al. takes the shadowing from EKS98 and uses a smaller charm cross-section dd mb. The  from beauty hadrons is estimated at 10% and b quenching is fixed at (b)= 0.4 for all the  range. In both transport models, the amount of regenerated  in the most central collisions contributes to about 50% of the production yield, the rest being from initial production. We can see on the left side of Fig. 3 that all three models reproduce correctly the centrality dependence of the forward   for  . A similar observation can be made for the mid rapidity results Wiechula:hp2012 (). The  dependence of the forward   is also successfully reproduced by the transport models, as shown on Fig. 3 right side. In addition, both models predict that a large fraction of  from regeneration have a  below 3.5 GeV/.

## 5 Elliptic flow in Pb-Pb collisions √sNN= 2.76 TeV

The elliptic flow of inclusive  has been measured as a function of the transverse momentum of the . For this measurement, the reaction plane has been determined with the VZERO-A detector. The large rapidity gap between the  acceptance and the VZEROA detector minimizes the influence of non-flow effects. One the left side of Fig. 4, an example of the signal extraction is given; one can clearly see the cosine shape of the measured  signal in the 6 bins, where is the difference between the azimuthal angle of the  and the angle of the reaction plane. Further analysis details can be found in Massacrier:hp2012 (). Figure 4 shows, on the right side, the first measurement of  elliptic flow at the LHC. The   is given as a function of  in the 20%–60% centrality range. A non-null   seems to be present at intermediate   and would tend to vanish at low and high . Uncertainties are still too large to draw definitive conclusions, nevertheless we have a non-zero signal for  with  between 2 to 4 GeV/ with 2.2 significance. At lower energy, the  elliptic flow was measured by STAR and appear to be consistent with zero at   10 GeV/ in 20%–60% centrality range, whereas charged hadrons and exhibit a rather strong flow in this same kinematic domain Tang:2011kr (). Model prediction (private communication) for ALICE was provided by the authors of Liu:2009nb () and is shown on Fig. 4. The full line assumes a thermalization of the beauty quarks in the medium, for which there is no evidence so far, and should be considered as an upper limit. The dashed line, a more realistic prediction in which beauty quarks are not thermalized, shows indeed a non-zero  , which matches qualitatively our data. It is important to add that this model reproduces successfully the ALICE  measurement.

## 6 Conclusion

Quarkonia production in ALICE in pp and Pb-Pb collisions at = 2.76 and 7 TeV has been presented. In pp collisions, the ,  and multiplicity dependence of  production,  polarization and non-prompt  have been studied. Results have shown good agreement or complementarity with other LHC results. All these measurements provide stringent constraints to model predictions. In Pb-Pb collisions, the  nuclear modification factor was studied as a function of centrality,  and . The   dependence on the number of participant nucleons is flat and centrality integrated values are large at mid and forward rapidity (). This result is clearly different from the ones seen at lower energies (e.g. RHIC and SPS). The rapidity dependence of the   shows that suppression at large rapidity ( 2.5   4 ) is beyond the one that could be expected from shadowing only predictions. The   is large at low  and then decreases with increasing . The trends observed in the data as a function of centrality and  can be reproduced by models based on deconfinement followed by charm recombination. In these models,  from recombination mostly occur at low  and account for half of the produced  in the most central collisions. Finally, we have presented the  elliptic flow in semi-central Pb-Pb collisions. For the first time, a non-zero   is observed in the intermediate  range. We have now accumulated hints that the  production in Pb-Pb collisions at LHC energy may be governed, for an important part, by charm quarks recombination processes. In order to confirm this observation, the shadowing must be measured and constrained since it remains unknown at LHC energies and this will be addressed by a pPb run scheduled at the beginning of 2013. One should add here that the uncertainties in   results depend directly on the pp reference data; thus it is crucial to collect a large amount of pp collisions at the same collision energy that of Pb-Pb sample, in order to have precise measurements of  and charm differential cross section and  polarization.

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