Measurement of Z0-boson production at large rapidities in Pb–Pb collisions at sNN=5.02TeV

The production of Z 0 bosons at large rapidities in Pb–Pb collisions at √ s NN = 5 . 02 TeV is reported. Z 0 candidates are reconstructed in the dimuon decay channel (Z 0 → μ + μ − ), based on muons selected with pseudo-rapidity − 4 . 0 < η < − 2 . 5 and p T > 20 GeV/ c . The invariant yield and the nuclear modiﬁcation factor, R AA , are presented as a function of rapidity and collision centrality. The value of R AA for the 0–20% central Pb–Pb collisions is 0 . 67 ± 0 . 11 (stat.) ± 0 . 03 (syst.) ± 0 . 06 (corr. syst.), exhibiting a deviation of 2 . 6 σ from unity. The results are well-described by calculations that include nuclear modiﬁcations of the parton distribution functions, while the predictions using vacuum PDFs deviate from data by 2 . 3 σ in the 0–90% centrality class and by 3 σ in the 0–20% central collisions. . This paper presents the ﬁrst measurement of Z 0 -boson production in Pb–Pb collisions at √ s NN = 5 . 02 TeV at large rapidities. Opposite-sign muon pairs from Z 0 -boson decays with 2 . 5 < y < 4 . 0 1 are measured with the ALICE detector. The yield of μ + μ − pairs includes contributions from virtual-photon processes and from their interference effects. This measurement probes the nPDFs of large- x valence quarks ( x 1 (cid:2) 10 − 1 ) and low- x sea quarks ( x 2 (cid:3) 10 − 3 ) at Q 2 ∼ M 2Z . The invariant yields and R AA are reported as a function of rapidity and collision centrality. The results are compared to model calculations including nPDFs. These measurements complement the measurements in p–Pb collisions at √ s NN = 5 . 02 TeV at large rapidities [32,33], providing increased precision and new information on rapidity and centrality dependence. The combination of these results with future W ± measurements in a similar kinematic interval will provide constraints on the ﬂavor dependence of nPDFs, in particular the strange quark contribution [21].


Introduction
Z 0 bosons are weakly interacting probes formed early in the evolution of hadronic collisions (t f ∼ 1/M 0.01 fm/c), with a typical decay time t d ∼ 0.1 fm/c. Their leptonic decays are of particular interest in heavy-ion collisions, since leptons do not interact strongly and their in-medium energy loss by bremsstrahlung is negligible [1]. Z 0 -boson production rates in hadronic collisions are well-understood, and their measurement via leptonic decays therefore serves as a valuable medium-blind reference for hard processes in heavy-ion collisions [2,3]. Z 0 -boson properties have been extensively studied at LEP (CERN), SLC (SLAC), Tevatron (FNAL) and LHC (CERN) in e + e − , pp and pp collisions [4][5][6][7][8][9][10][11][12][13][14][15]. Z 0 -boson production in hadronic collisions is well-described by perturbative Quantum Chromodynamics (pQCD) calculations at next-to-next-to-leading order (NNLO) [16,17], and their comparison with data provides constraints on Parton Distribution Functions (PDFs) [18,19]. In heavy-ion collisions, Z 0 -boson production can be affected by initial-state effects. As a result of the different balance of the number of u and d valence quarks in protons and in lead nuclei (isospin), the yield of Z 0 bosons in Pb-Pb collisions at √ s NN = 5.02 TeV is expected to increase relative to that in pp collisions by 5-8% at large rapidities, and decrease by 3% at central rapidities [20]. Modifications of the PDFs in nuclei (nPDFs) [21][22][23][24][25][26][27] introduce a rapidity-dependent change in yield, with a decrease in yield relative to that in pp collisions of 8-15% at large rapidities, corresponding to the Bjorken-x E-mail address: alice -publications @cern .ch. ranges x 1 10 −1 and x 2 10 −3 , and an increase by 3% at central rapidity, corresponding to x 1,2 ∼ 10 −2 [20,21]. The yield could also depend upon effects such as multiple scattering and mediuminduced bremsstrahlung of the initial partons in large nuclei [28]. The ATLAS, ALICE, CMS and LHCb collaborations have reported measurements of W ± -and Z 0 -boson production in p-Pb collisions at √ s NN = 5.02 TeV [29][30][31][32][33], with complementary rapidity coverage. These measurements are well-described by next-to-leading order (NLO) pQCD calculations [20] and by NNLO calculations using the Fully Exclusive W and Z Production code (FEWZ) [34], utilising both nPDFs [32] and vacuum PDFs. The forward-backward asymmetry of W ± -boson production suggests the presence of nuclear modification of PDFs [31]. This sensitivity to nuclear effects indicates the need to include these data in the future nPDF fits. In Pb-Pb collisions, W ± -and Z 0 -boson measurements at √ s NN = 2.76 TeV have been carried out at central rapidity by the ATLAS and CMS collaborations [35][36][37][38]. Preliminary Z 0 -boson measurements in Pb-Pb collisions at √ s NN = 5.02 TeV at central rapidity have also been reported recently by ATLAS [39]. The W ± -and Z 0 -boson nuclear modification factor, R AA , defined as the ratio of the yields in Pb-Pb collisions and the cross-section in pp collisions normalised by the nuclear overlap function T AA , which represents the effective overlap area of the two interacting nuclei [40], is measured to be consistent with unity within uncertainties, with no centrality dependence [37][38][39].
Measurements at high collision energy and large rapidities are sensitive to low Bjorken-x processes, and are therefore important to further constrain the initial-state effects on electroweak boson production and to establish a reference for medium-sensitive observables. This paper presents the first measurement of Z 0 -boson production in Pb-Pb collisions at √ s NN = 5.02 TeV at large rapidities. Opposite-sign muon pairs from Z 0 -boson decays with 2.5 < y < 4.0 1 are measured with the ALICE detector. The yield of μ + μ − pairs includes contributions from virtual-photon processes and from their interference effects. This measurement probes the nPDFs of large-x valence quarks (x 1 10 −1 ) and low-x sea quarks (x 2 10 −3 ) at Q 2 ∼ M 2 Z . The invariant yields and R AA are reported as a function of rapidity and collision centrality. The results are compared to model calculations including nPDFs. These measurements complement the measurements in p-Pb collisions at √ s NN = 5.02 TeV at large rapidities [32,33], providing increased precision and new information on rapidity and centrality dependence. The combination of these results with future W ± measurements in a similar kinematic interval will provide constraints on the flavor dependence of nPDFs, in particular the strange quark contribution [21]. This letter is organised as follows: the experimental setup and data sample are described in Sect. 2; the analysis procedure is presented in Sect. 3; the results are presented in Sect. 4; and a summary is given in Sect. 5.

Experimental setup and dataset
The ALICE detector is described in detail in Ref. [41]. Z 0 bosons are reconstructed via their muonic decay with the ALICE muon spectrometer, which provides muon trigger, tracking and identification in the pseudo-rapidity range −4.0 < η < −2.5. The muon spectrometer, as seen from the interaction point, consists of a front absorber of 10 interaction lengths (λ int ) thickness, which reduces the contamination of hadrons and muons from the decay of light particles; five tracking stations; an iron absorber with thickness 7.2 λ int ; and two trigger stations. Each tracking station is composed of two planes of multi-wire proportional chambers with cathode-plane readout, while each trigger station consists of two planes of resistive plate chambers. The third tracking station is located inside the gap of a dipole magnet, which provides a 3 T·m magnetic field integral. The muon spectrometer is completed by a beam shield surrounding the beam pipe that protects the apparatus from secondary particles produced in the interaction of large-η primary particles with the pipe itself.
The interaction vertex is reconstructed using the two cylindrical layers of the Silicon Pixel Detector, located at a radial distance of 3.9 and 7.6 cm from the beam axis and covering |η| < 2 and |η| < 1.4, respectively. The V0 detector, consisting of two arrays of scintillator counters covering 2.8 < η < 5.1 and −3.7 < η < −1.8, is used for triggering and evaluation of collision centrality. Finally, the Zero Degree Calorimeter, placed at 112.5 m from the interaction point along the beam line, is used to reject electromagnetic interactions [42].
The dataset used in this analysis consists of Pb-Pb events at √ s NN = 5.02 TeV selected with a dimuon trigger that requires the coincidence of a minimum-bias (MB) trigger and a pair of tracks with opposite sign in the muon spectrometer, each with p T 1 GeV/c. The MB trigger is defined by the coincidence of the signals from both arrays of the V0. The MB trigger is fully efficient for events within the 0-90% centrality interval, which are used in this analysis. The muon trigger efficiency has a plateau of about 98% for muons with p T > 5 GeV/c. The resulting efficiency for pairs of opposite-sign muons, with muon p T > 20 GeV/c and 1 In the ALICE reference frame the muon spectrometer covers a negative η range and, consequently, a negative y range. However, since the Pb-Pb system is symmetric in rapidity, a positive y notation is used to present the results. −4.0 < η < −2.5, is 95%. After all event selection cuts, the dataset corresponds to an integrated luminosity of about 225 μb −1 .

Analysis procedure
The procedure for Z 0 -boson signal extraction in this analysis is the same as that used in the analysis of p-Pb collisions at √ s NN = 5.02 TeV [32]. Tracks are reconstructed in the muon spectrometer using the algorithm described in Ref. [43]. Tracks are selected for analysis if they have pseudorapidity −4.0 < η < −2.5 and polar angle 170 • < θ abs < 178 • , measured at the end of the front absorber. This selection rejects particles that cross the highdensity region of the front absorber and undergo significant multiple scattering. Tracks reconstructed in the tracking stations are identified as muons if they match a track segment in the trigger stations, placed downstream the iron wall. The contamination from background tracks that do not point to the interaction vertex is reduced by utilising the product of the momentum and the distance of closest approach to the interaction vertex. This cut removes 88% of all tracks for events in the 0-90% centrality interval, while retaining all signal candidates with negligible residual background contribution.
Only muons with p T > 20 GeV/c are used in this analysis.
This selection reduces the contribution of muons from the decay of charm, beauty and low-mass resonances (see below). Z 0 -boson candidates are formed by combining pairs of opposite-sign muons. The candidates are further selected by requiring that their rapidity, calculated using the measured invariant mass, is in the interval 2.5 < y < 4.0. Fig. 1 presents the μ + μ − invariant mass distribution in the centrality intervals 0-90% in Fig. 1(a), 0-20% in Fig. 1(b), and 20-90% in Fig. 1 . The isospin of the Pb-nucleus is accounted for by a weighted average of neutron and proton interactions, but no modification of the nucleon PDF was applied to account for nuclear effects. The simulations account for variations in the detector response with time and in-situ alignment effects. A data-driven description of the muon momentum resolution is also implemented (see Ref. [32] for details). The shape of the μ + μ − invariant mass distribution, which is mainly affected by the momentum resolution, is similar in data and MC.
Various background sources contribute to the μ + μ − invariant mass distribution. Contamination from the decay of tt (tt −→ 44,47] and found to be smaller than 0.5% of the signal yield, which is considered as a systematic uncertainty. The contribution of opposite-sign muon pairs from the decay of cc (cc −→ μ + μ − X ) and bb (bb −→ μ + μ − X ) pairs was studied in p-Pb collisions [32] and found to be smaller than that of tt and τ pairs. In Pb-Pb collisions, the presence of high-p T muons from the decay of heavy-flavour pairs is expected to be further reduced due to the in-medium energy loss of heavy quarks. This contribution was therefore neglected. Finally, the combinatorial contribution from the random pairing of muons in the event is evaluated via like-sign muon pairs (μ ± μ ± ). This combinatorial contribution is found to be small (one candidate in the 20-90% centrality interval) and is subtracted from the signal estimate. The number of Z 0 candidates is estimated using the procedure described in Ref.
[32], by counting the entries in the μ + μ − invariant mass interval 60 < M μμ < 120 GeV/c 2 after subtracting the contribution from like-sign pairs for each centrality and rapidity interval. A total of 64 candidates is found in the 0-90% centrality bin, of which 37 are in the 0-20% bin and 27 in the 20-90% bin. As a function of rapidity, 33 candidates are in the interval 2.5 < y < 3.0, and 31 are in the interval 3.0 < y < 4.0. The raw yields are corrected for the detector acceptance and for reconstruction and selection efficiency ( A · ε). The value of A · ε is 75% for events in the 0-90% centrality interval, estimated using the POWHEG [44] simulations described previously. The dependence of the efficiency on the detector occupancy was evaluated by embedding the generated Z 0 signal in real MB Pb-Pb data. The A · ε term is constant as a function of centrality from peripheral to semi-central events and decreases in the most central collisions.
The value of A · ε is 78% in the 20-90% centrality interval and 74% in the 0-20% interval, with centrality-independent systematic uncertainty of 5%, as discussed below.
To evaluate the invariant yields (dN/d y), the raw dimuontriggered mass distribution must be normalised by the factor F i μ-trig/MB , which is the inverse of the probability to observe a dimuon pair in a MB event for the centrality class i. The value of F i μ-trig/MB is calculated in two different ways, by applying the dimuon selection criterion to MB events, and by the relative counting rate of the two triggers [48]. The variation in F i μ-trig/MB determined by these two methods is 0.5% and contributes to the systematic uncertainty.
The nuclear modification factor R AA requires the determination of the collision centrality, which is typically quantified by the average number of nucleons participating in the interaction for a given Table 1 Values of the average nuclear overlap function, T AA , the number of participating nucleons, N part , and the number of binary nucleon-nucleon collisions, N coll , for each centrality interval. The average number of participants as weighted by the average number of collisions, N part N coll , is also reported. Centrality 2.61 ± 0.09 73 ± 1 183 ± 15 141 ± 2 centrality bin, N part . However, the rate of hard processes is known to scale with the average number of nucleon-nucleon collisions N coll . The average centrality for hard processes is therefore presented as the average number of participant nucleons weighted by the number of collisions N part N coll . Table 1 shows the estimates of the average nuclear overlap function T AA , the number of participating nucleons N part and the number of binary nucleon-nucleon collisions N coll , which are obtained via a Glauber model fit of the signal amplitude in the two arrays of the V0 detector [49,50]. The resulting N part N coll is also shown. The classification of the events in given centrality intervals has an associated uncertainty of 1.5-2.3% (centrality dependent), that was estimated by comparing the number of candidates selected by varying the centrality ranges by ±0.5%, to account for the centrality resolution [49,50].
The sources of systematic uncertainties in the yields and R AA are summarised in Table 2. The systematic uncertainty in the track- Table 2 Relative systematic uncertainties in the yields and R AA . The ranges quoted for T AA and the centrality limits, represent the uncertainty variation with centrality. The centrality-dependent correlated uncertainties are marked by the symbol ( ), while the uncertainty sources that are correlated as a function of rapidity are indicated by ( ).

Source
Relative systematic uncertainty Background contamination

<1.0%
Tracking efficiency 3.0% ( ) Trigger efficiency 1.5% ( ) Tracker/trigger matching 1.0% ( ) Alignment 3.5% ( ) ing efficiency is 3%, obtained from the comparison of the efficiency estimated in data and MC by exploiting the redundancy of the tracking chamber information [51]. The systematic uncertainty of the dimuon trigger efficiency is 1.5%, evaluated by propagating the uncertainty of the efficiency of the detection elements, which is estimated from data using the redundancy of the trigger chamber information. In addition, the choice of the χ 2 cut used to match the tracker and trigger tracks introduces 1% uncertainty, obtained from the difference between data and simulation when applying different χ 2 cuts. The uncertainties in the track resolution and alignment are estimated by comparing the A · ε values obtained with two different simulations. In the full simulation, the alignment is measured using the MILLEPEDE [52] package and the residual misalignment is taken into account. In the fast simulation, the tracker response is based on a parameterisation of the measured resolution of the clusters associated with a track [32]. The resulting systematic uncertainty is 3.5%. The total systematic uncertainty in the yield and R AA are determined by summing in quadrature the uncertainty from each source, listed in Table 2. All uncertainties except those due to T AA and the centrality bin boundaries are independent of collision centrality. Correlations in centrality or rapidity of the uncertainties of different sources are indicated in Table 2. The relative systematic uncertainty in the proton-proton reference σ pp , which affects the R AA , corresponds to 4.5% and is estimated by varying the factorization and renormalisation scales and accounting for the uncertainties in the PDFs [20].

Results
The invariant yield of μ + μ − from Z 0 bosons in 2.5 < y < 4.0, divided by T AA , is 6.11 ± 0.76 (stat.) ± 0.38 (syst.) pb for the 0-90% centrality interval. The comparison with theoretical calculations at NLO is shown in Fig. 2. The CT14 [53] prediction utilises free proton and neutron PDFs, with relative weights to account for the isospin of the Pb nucleus. The uncertainty on the model include the uncertainty on the NLO calculations and of the measurements considered in the PDF fit. The measured invariant yield deviates from the lower limit of this prediction by 2.3σ . For the description of nuclear PDFs, two different approaches were considered. The standard approach evaluates the nPDF as the free PDF multiplied by a parameterisation of nuclear modifications. The calculations obtained with the EPS09 [54] and the more recent EPPS16 [22] parameterisations are shown. In the other approach, the nPDFs are obtained by fitting the nuclear data in a similar way as done for free proton data, but using a parameterisation that depends on the atomic mass of the nucleus. The results obtained with the nCTEQ15 nuclear PDFs [21,55] are also presented. The nPDF sets are characterised by their different approximations and by different input data included in the calculations (see Ref. [22] and references therein for details). Only the most recent EPPS16 parameterisation includes LHC jet, W ± and Z 0 data, although the W ± and Z 0 data provide only weak constraints on nPDFs at the current perturbative order of the calculation (NLO) [21,56]. In general, the nPDFs have larger uncertainties compared to the free proton PDFs, since they are less constrained from data. CT14+EPS09 and CT14+EPPS16 estimates combine CT14 and EPS09 or EPPS16 uncertainties, whereas nCTEQ15 does a global study of the proton and nuclear measurement uncertainties included in the fit. EPPS16 allows much more freedom for the flavour dependence of nPDFs than other current analyses, which results in larger uncertainties. All pQCD calculations shown in Fig. 2 that use nPDFs describe the measurement well.
The rapidity dependence of the Z 0 -boson invariant yields divided by T AA is shown in Fig. 3(a). The results are compared to pQCD calculations using the CT14 [53] PDF set both with (green filled box) and without (blue hatched box) the EPPS16 [22] parameterisation of the nPDFs. In both cases, the Pb-isospin effect is modelled by combining the proton and neutron PDFs or nPDFs. EPPS16 decreases the yields but does not have a strong influence on the rapidity dependence of the calculation. The calculations that utilise vacuum PDFs overestimate data in the two rapidity intervals, whereas those that utilise nPDFs are in good agreement with data.
In this analysis, the ratio R AA utilises a theoretically calculated reference cross section for pp collisions [20], which is σ pp = 11.92 ± 0.43 pb. The value of R AA for the 0-90% centrality class is determined to be 0.77 ± 0.10 (stat.) ± 0.06 (syst.), deviating by 2.1σ from unity. The pQCD calculation using CT14 [53] and considering only the isospin effects, finds R CT14 AA = 1.052 ± 0.038. The modification of the PDFs in nuclei results in a net reduction of the yields, and consequently in R AA values lower than unity, with R CT14+EPPS16 AA = 0.845 ± 0.068, in agreement with data. The rapid- compared to theoretical calculations with and without nuclear modification of the PDFs. The filled blue boxes show the calculation using the CT14 PDF, while the green stippled boxes show the calculation using CT14 PDF with EPPS16 nPDF [22,53]. All model calculations incorporate PDFs or nPDFs that account for the isospin of the Pb nucleus. ity dependence of R AA is presented in Fig. 3(b). The values are smaller than unity, with a slight rapidity dependence. The data are well-described by calculations including nPDFs (green filled boxes), while the calculations including only isospin effects (blue hatched boxes) tend to overestimate the measured values. Z 0 -boson production is studied as a function of the collision centrality, expressed in terms of N part N coll as shown in Fig. 4. The value of R AA is compatible with unity in peripheral collisions, with R AA (20-90%) = 0.96 ± 0.19 (stat.) ± 0.04 (syst.) ± 0.06 (corr. syst.), while it is 2.6σ smaller than unity in the central collisions, with R AA (0-20%) = 0.67 ± 0.11 (stat.) ± 0.03 (syst.) ± 0.04 (corr. syst.).
The value for 0-20% central collisions deviates from the predictions using vacuum PDFs (R CT14 AA ) by 3σ . The data are compared to calculations including a centrality-dependent nuclear modification of the PDFs [57], which describe the data within uncertainties.

Conclusion
We have reported the first measurement of Z 0 -boson production at forward rapidities in Pb-Pb collisions at √ s NN = 5.02 TeV. In contrast, the calculations with vacuum PDFs overestimate the centrality-integrated R AA by 2.3σ and R AA in the 0-20% most central collisions by 3σ .

Acknowledgements
The ALICE Collaboration would like to thank H. Paukkunen for providing the pQCD calculations with EPS09 and EPPS16, and F. Lyonnet and A. Kusina for providing the pQCD calculations with nCTEQ15.
The ALICE Collaboration would like to thank all its engineers and technicians for their invaluable contributions to the construction of the experiment and the CERN accelerator teams for the outstanding performance of the LHC complex. The ALICE Collab- References [1]