Measurement of Z → τ + τ − production in proton-proton collisions at √s=8 TeV

JHEP09(2018)159

Received: June 15, 2018 Revised: August 3, 2018 Accepted: September 20, 2018 Published: September 27, 2018

Measurement of Z → τ

τ

production in

proton-proton collisions at

√

s = 8 TeV

The LHCb collaboration

E-mail: chitsanu.khurewathanakul@cern.ch

Abstract: A measurement of Z → τ+τ− production cross-section is presented using

data, corresponding to an integrated luminosity of 2 fb−1, from pp collisions at√s = 8 TeV

collected by the LHCb experiment. The τ+τ− candidates are reconstructed in final states

with the first tau lepton decaying leptonically, and the second decaying either leptonically or to one or three charged hadrons. The production cross-section is measured for Z bosons

with invariant mass between 60 and 120 GeV/c2, which decay to tau leptons with transverse

momenta greater than 20 GeV/c and pseudorapidities between 2.0 and 4.5. The

cross-section is determined to be σpp→Z→τ+_τ− = 95.8 ± 2.1 ± 4.6 ± 0.2 ± 1.1 pb, where the first

uncertainty is statistical, the second is systematic, the third is due to the LHC beam energy uncertainty, and the fourth to the integrated luminosity uncertainty. This result is compatible with NNLO Standard model predictions. The ratio of the cross-sections for

Z → τ+τ− to Z → µ+µ− (Z → e+e−), determined to be 1.01 ± 0.05 (1.02 ± 0.06), is

consistent with the lepton-universality hypothesis in Z decays.

Keywords: Electroweak interaction, Forward physics, Hadron-Hadron scattering (exper-iments), Lepton production, Tau Physics

JHEP09(2018)159

Contents

1 Introduction 1

2 Detector and datasets 2

3 Event selection 2

4 Signal and background estimation 5

5 Cross-section measurement 8

6 Conclusion 9

The LHCb collaboration 14

1 Introduction

The measurement of the production cross-section for a Z boson1 using different decay

modes in proton-proton (pp) collisions, σ_{pp→Z→f ¯f}, is an important verification of Standard

Model (SM) predictions. The ratio of the Z → τ+τ− production cross-sections to other

leptonic decay modes provides a test of lepton universality (LU). The LEP experiments

have performed high accuracy tests of LU at the Z pole, with a precision better than 1% [1].

Consequently, the observation in proton-proton collisions of any apparent deviation from LU in Z decays would be an evidence of new phenomena producing final-state leptons,

like in the theoretical context of mSUGRA [2], constrained NMSSM [3], Randall-Sundrum

models [4,5], or lepton-violating decays of Higgs-like bosons [6–10].

This analysis extends the LHCb results obtained with pp collisions at √s = 7 TeV [11]

to√s = 8 TeV. The cross-section is measured for leptons from the Z decay with transverse

momentum (pT) above 20 GeV/c and a Z invariant mass between 60 and 120 GeV/c2, as for

the previously published Z → µ+µ−and Z → e+e−cross-sections [12,13]. The cross-section

measurements in the pseudorapidity range 2.0 < η < 4.5 covered by the LHCb experiment

are complementary to those with the central detectors ATLAS [14] and CMS [15].

In the present analysis, the reconstruction of the tau-pair candidates is performed in both leptonic and hadronic decay modes of the tau, requiring at least one leptonic mode

for the tau-pair candidate. The reconstruction of high-pT tau leptons in the 3-prong decay

mode is performed for the first time in LHCb.

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2 Detector and datasets

The LHCb detector [16,17] is a single-arm forward spectrometer designed for the study of

particles containing b or c quarks. The detector includes a high-precision tracking system consisting of a silicon-strip vertex detector surrounding the pp interaction region, a large-area silicon-strip detector located upstream of a dipole magnet with a bending power of 4 Tm, and three stations of silicon-strip detectors and straw drift tubes placed downstream of the magnet. The tracking system provides a measurement of momentum of charged particles with a relative uncertainty that varies from 0.5% at low momentum to 1.0% at 200 GeV/c. The minimum distance of a track to a primary vertex (PV), the impact

param-eter (IP), is measured with a resolution of (15 + 29/pT) µm, where pT is the component

of the momentum transverse to the beam, in GeV/c. Photons, electrons and hadrons are identified by a calorimeter system consisting of scintillating-pad (SPD) and preshower de-tectors (PS), an electromagnetic calorimeter (ECAL) and a hadronic calorimeter (HCAL). Muons are identified by a system composed of five stations of alternating layers of iron and multiwire proportional chambers.

The online event selection is performed by a trigger, which consists of a hardware stage, based on information from the calorimeter and muon systems, followed by a software stage, which applies a full event reconstruction. The hardware trigger imposes a global event cut (GEC) requiring the hit multiplicity in the SPD to be less than 600, to prevent events with high occupancy from dominating the processing time in the software trigger.

This analysis uses pp collisions at √s = 8 TeV corresponding to a total integrated

lu-minosity of L = (1976 ± 23) pb−1[18]. Simulated data samples are used to study the event

selection, determine efficiencies, and estimate systematic uncertainties. In the simulation,

pp collisions are generated using Pythia 8 [19,20] with a specific LHCb configuration [21],

and parton density functions taken from CTEQ6L [22]. Decays of hadronic particles are

described by EvtGen [23], in which final-state radiation is generated using Photos [24].

The interaction of the generated particles with the detector, and its response, are

imple-mented using the Geant4 toolkit [25,26] as described in ref. [27].

3 Event selection

The Z boson is reconstructed from τ particles decaying into leptonic (muons or electrons) or hadronic (one or three charged hadrons) final states. Charged tracks are reconstructed by the tracking system and matched with clusters of ECAL/HCAL cells and hits in the muon detector. Muon candidates are identified by matching tracks to hits in the muon stations downstream of the calorimeters. They are required to leave hits in at least three

muon stations, or four muon stations if they have pT > 10 GeV/c. Electron candidates

must fail the muon identification criteria and fall within the acceptance of the PS, ECAL, and HCAL sub-detectors. On average, 30% of a material radiation length is crossed by a particle before the bending magnet, causing a considerable energy loss by bremsstrahlung for electrons and positrons. Hence, the electron or positron candidate momentum is

JHEP09(2018)159

is designed to register particles from heavy-flavour hadron decays, calorimeter cells with transverse energy above about 10 GeV saturate the electronics, and lead to incomplete elec-tron bremsstrahlung recovery. A large energy deposit in the PS, ECAL, but not in HCAL

is required, satisfying EPS > 50 MeV, EECAL/p > 0.1, and EHCAL/p < 0.05, where p is

the reconstructed momentum of the electron candidate, after applying the bremsstrahlung photon recovery. Charged hadrons are required to be within the HCAL acceptance, deposit

an energy of EHCAL/p > 0.05, and must fail the muon identification criteria. The pion

mass is assigned to all charged hadrons.

The analysis is divided into seven “streams”, labelled as τµτµ, τµτe, τµτh1, τµτh3,

τeτe, τeτh1, and τeτh3, where the subscript denotes the final state reconstructed.

Charge-conjugate processes are implied throughout. The streams are chosen such that at least one τ lepton decays leptonically. The tau-pair candidates are selected by triggers requiring muons or electrons with a minimum transverse momentum of 15 GeV/c. The trigger efficiency is between 70% and 85%, depending on the number of leptons in the stream. The final states

presented in this analysis account for 58% of all Z → τ+τ− decays. In the following,

a τ candidate corresponds to a single particle for the τe, τµ, and τh1 decay channels,

or a combination of the three hadrons in the case of τh3. A pair of τ candidates must

be associated to the same PV. In case where multiple PVs are presented in the event,

the associated PV is defined as that with a smallest change in vertex-fit χ2 when it is

reconstructed with and without the τ candidate.

The dominating backgrounds are of QCD origin with one or several jets (call “QCD events” in the following), as well as electroweak processes, mainly W /Z +jets (“Vj”). The following requirements on the transverse momentum of τ decay products are used to reduce

these backgrounds. For all the streams the triggering lepton must have pT > 20 GeV/c. For

the processes τµτµ, τeτe, and τµτe the second lepton pT threshold is 5 GeV/c. The hadron

of the τh1candidates is required to have pT > 10 GeV/c. For the τh3decay channel, each of

the three charged hadrons are selected with pT> 1 GeV/c, and at least one must be above

6 GeV/c. In addition, the τh3candidates must have a total pT in excess of 12 GeV/c, and an

invariant mass in the range 0.7 to 1.5 GeV/c2. This leads to the τh3identification efficiency

of about 30%, comparable with the value of 35% found in the context of the B0→ D∗−τ+ντ

analysis [29]. For all streams, the reconstructed direction of the τ candidate must be in

the fiducial geometrical acceptance 2.0 < η < 4.5.

Additional selection criteria are needed to suppress background processes due to semileptonic c- or b-hadron decays, misidentification of hadrons as leptons, or, especially

in the τh3 stream, combinations of unrelated particles.

Signal candidates tend to have back-to-back tracks in the plane transverse to the

beam axis, and a higher invariant mass than the background. Hence, the tau-pair is

required to have an invariant mass above 20 GeV/c2, or 30 GeV/c2 for the stream containing

τh1,τh3 candidates. Additionally, for the dilepton streams τµτµ, τeτe, the selected mass

range is below 60 GeV/c2, to avoid the on-shell Z → µ+µ− and Z → e+e− regions. The

absolute difference in azimuthal angle of the two τ candidates is required to be greater than 2.7 radians. The above selections are found to be 70 to 80% efficient, depending on the analysis stream.

JHEP09(2018)159

Charged particles in QCD events tend to be associated with jet activity, in contrast

to signal candidates where they are isolated. An isolation variable, ˆIpT, is defined as

the pT of the candidate divided by the transverse component of the vectorial sum of all

track momenta in a cone surrounding the candidate of radius Rηφ = 0.5, defined in the

pseudorapidity-azimuthal angle (η − φ) space. A fully isolated candidate has ˆIpT = 1, while

lower values indicate the presence of jet activity. The selection ˆIpT > 0.9 is applied to all τ

candidates, with an efficiency of more than 64% for the tau-pair signal and rejecting about 98% of QCD events.

The lifetime of the τ lepton is used to separate the signal from prompt background. For the τ decay channels with a single charged particle, it is not possible to reconstruct a secondary vertex and a selection on the particle IP to the associated PV is applied. The efficiency on the signal from these criteria is in the range 71 to 79%.

In the τh3 case, a vertex reconstruction is possible: the maximum distance between

the three tracks in the η − φ space is required to be less than 0.005 · pT where pT is the

transverse momentum of τh3 in GeV/c. The proper decay time is subsequently estimated

from the distance of the reconstructed vertex to the associated PV, and the momentum of the candidate, taken as an approximation of the τ momentum. A minimum of 60 fs is imposed for this variable, efficiently discarding the prompt background whilst keeping

about 77% of the signal. For the τh3 decay, a correction to the mass is also possible by

exploiting the direction of flight, recovering part of the momentum lost due to undetected particles. The corrected mass is defined as

mcorr≡

q

m2_{+ p}2_sin2_{θ + p sin θ , (3.1)}

where m and p are the invariant mass and momentum computed from the three tracks and θ is the angle between the momentum and flight direction of the candidate. The requirement

mcorr < 3 GeV/c2 reduces the QCD background by about 50% and the Vj background

by about 60%, retaining 80% of the signal. Figure 1 shows the mass distributions of τh3

candidates before and after correction for data, compared to the distributions of Z → τ+τ−

decays and of the Vj background from simulation.

In the τeτeand τµτµstreams an additional background component arises from Z → l+l−

decays. This process produces two muons or two electrons with similar pT values, in

contrast to signal which tends to have unbalanced pT due to the missing momentum from

unreconstructed neutrinos and neutral hadrons. The pT asymmetry, ApT, is defined as the

absolute pT difference of the two candidates divided by their sum. For the two leptonic

streams ApT is required to be greater than 0.1. A particular case is the τµτe stream,

where background from Vj processes arises, with one lepton coming from the jet causing a

relatively large pTimbalance with respect to the lepton from the W/Z boson. A suppression

by a factor of two of this source of background, with a loss of 10% of the signal is obtained

imposing a maximal ApT value of 0.6. For τh1 and τh3 the ApT criterion has been found

inefficient for background rejection, hence no such a constraint is imposed to these two decay modes.

JHEP09(2018)159

candidates from the τµτh3 channel. The yields are normalised to the integrated luminosity of

the data. The results from data are represented by the black points. The error bars represent the statistical uncertainty only. The distributions are compared to the signal distributions from simulated Z → τ+_τ− _{(blue) events and the Vj (red) background.}

τµτµ τµτh1 τµτh3 τeτe τeτh1 τeτh3 τµτe Z → l+_l− _{249.7(88) 1.2(5) — 420.8(253) 16.1(22) — 25.3(54)} QCD 50.9(102) 235.8(193) 21.2(53) 42.7(88) 330.8(228) 19.4(51) 160.0(169) Vj 12.7(74) 144.2(430) 5.1(34) 5.8(27) 68.3(197) 10.1(58) 65.3(257) V V 0.2(1) 1.2(2) 0.2(1) 0.2(1) 0.8(1) 0.2(1) 10.0(5) tt 1.0(2) 2.2(2) 0.6(1) 0.2() 0.7(1) 0.1() 5.5(2) Z → bb 0.8(4) 0.3(2) 0.1(1) 0.1(1) 0.3(2) 0.1(1) 0.3(2) Cross-feed 4.5(11) 22.2(25) 13.9(20) 13.0(39) 16.5(24) 7.3(17) 52.5(42) Total bkg. 319.9(127) 407.1(375) 41.1(53) 482.7(242) 433.5(220) 37.2(58) 318.9(236) Observed 696 1373 205 610 861 110 1322 Z → τ+_τ− _{376.1(290) 965.9(521) 163.9(142) 127.3(329) 427.5(358) 72.8(111) 1003.1(418)}

Table 1. Expected backgrounds yields and total number of candidates observed. In the last row the uncertainties are the statistical and systematic contributions combined.

4 Signal and background estimation

After the selections described in the previous section, a maximum of one Z → τ+τ−

candi-date per event is found. The number of signal candicandi-dates is determined from the number of observed candidates in data subtracted by the total number of estimated backgrounds. The

results are summarized in table 1. The invariant-mass distributions for such candidates

are shown in figure 2, for the seven analysis streams.

A data-driven approach is used to estimate the amount of background from QCD and Vj processes. Same-sign (SS) tau-pair candidates are selected with identical criteria as the signal, but requiring the tau candidates to have identical electric charge. From simulation, the SS candidates yield is found to originate mainly from QCD and Vj processes, while

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(a) (b)

(c) (d)

(e) (f )

(g)

Figure 2. Invariant-mass distributions for (a) τµτµ, (b) τeτe, (c) τµτh1, (d) τeτh1, (e)

τµτh3, (f) τeτh3, (g) τµτe candidates with the

excluded mass ranges indicated by the gray areas. The Z → τ+_τ− _{simulation (red) is}

normalised to the observed signal. The Z (blue), QCD (brown), and electroweak (ma-genta) backgrounds are estimated from data. The tt, V V backgrounds and cross-feed (green) are estimated from simulation (see text) and generally not visible.

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the mis-reconstructed Z → τ+τ− process contributes less than 1%: NSS = N_QCDSS + N_VjSS+

N_{Z → τ}SS +_τ−. The last term originates, for instance, from an electron either from a π0 decay

or pair-production, a single hadron from partially-reconstructed τh3, 3-prong from false

combinatorics, or a muon from a misidentified hadron. The amount of QCD and Vj events

in the SS dataset is determined by a fit to the pT(τ1) − pT(τ2) distribution, for each analysis

stream [11]. In the fit, the QCD distribution templates are taken from an SS QCD-enriched

dataset, obtained by the anti-isolation requirement ˆIpT < 0.6; the distributions templates

for the two Vj processes (W +jet, Z+jet) are obtained from simulation and are found to be statistically consistent. Subsequently, the number of QCD and Vj background candidates is

computed as NQCD= rQCD· NQCDSS , and NVj = rVj· NVjSS. The value of rVj is obtained from

simulation, considering both W and Z contributions, and varies from 1.05±0.08 for the τeτe

up to 2.37 ± 0.30 for the τµτh1. The same-sign and opposite-sign QCD-enriched datasets

provide the rQCD values, which are all close to unity, with the exception of 1.30 ± 0.05,

obtained for τµτµ.

The Z → l+l− decays (l = e, µ) are a background for all the streams, except for τµτh3

and τeτh3. The number of Z → l+l−decays contaminating the τµτµstream is determined by

applying all selection criteria except for the requirement on the dimuon mass: this produces a sample with a clear peak at the Z mass, as well as an off-shell contribution at lower mass,

as shown in figure 2a. A template distribution obtained from simulation is normalised to

the data in the 80–100 GeV/c2 mass interval. The fraction of genuine Z → τ+τ−candidates

in the normalisation region is found to be negligible from simulation. The contribution from

Z → µ+µ− decays to the background in the signal region is inferred from the normalised

distribution. A similar procedure is applied to estimate the τeτebackground from Z → e+e−

decays, but with the normalisation performed in the 70–100 GeV/c2 interval to account for

the electron momentum resolution degraded by an incomplete electron bremsstrahlung recovery. For this process, 1% of non-Z background candidates are subtracted from the normalisation region, as estimated from SS dilepton events.

The process Z → µ+µ− can be observed as a fake τµτh1 candidate when one of the

muons is misidentified as a charged hadron. This background is evaluated by applying the

τµτh1 selection but requiring a second identified muon rather than a hadron, and scaling

by the probability for a muon to be misidentified as a hadron. The misidentification

probability, obtained from simulation and cross-checked using a tag-and-probe method

applied to Z → µ+µ− data (requiring an identified muon as a tag, and an

oppositely-charged track as a probe), is of the order of 10−3 for muons with pT < 10 GeV/c, and

10−4–10−5 at larger pT values. The uncertainty on the estimation of this background

is obtained from the lepton misidentification probability uncertainty combined with the statistical uncertainty of the dimuon candidates sample. A similar procedure allows the

estimation of Z → µ+µ−, Z → e+e− backgrounds in τµτe, τeτh1 streams.

Other background processes are due to diboson decays, tt events, and Z decays into b hadrons. Their contributions are relatively small and obtained from simulation.

Some of the selected tau-pair candidates may not originate from the stream under

study. For instance, a τh1 candidate may be selected from a partially reconstructed τh3

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sample. The statistical uncertainty is 1 to 3%, to which a small contribution from the uncertainties on the branching fractions of the contaminating streams is added.

5 Cross-section measurement

The production cross-section of Z boson to tau-pair is measured for each analysis stream using

σpp→Z→τ+_τ− =

Nobs/εobsrec −

P

kNbkg,k/εbkg,krec

L B A ε_sel , (5.1)

where Nobs is the number of observed Z bosons and Nbkg,k is the estimated background

from source k.

The total integrated luminosity is denoted by L, and B is the product of the branching fractions of the tau lepton pair to decay to the given final state, with values and

uncertain-ties taken from the world averages [30]. The acceptance factor, A, is needed to normalise

the results of each analysis stream to the kinematical region 60 < Mτ τ < 120 GeV/c2,

2.0 < ητ < 4.5, and pτ_T > 20 GeV/c, which allows the comparison with the Z → µ+µ−,

Z → e+e− decay measurements in LHCb [12,13]. This factor is the fraction of Z → τ+τ−

events where the generated τ satisfy the chosen kinematical selections, which also fulfill the fiducial acceptance selection. The value of A for each stream is obtained from simulation,

using the POWHEG-BOX [31–34] at next-to-leading order with PDF MSTW08NLO90cl [35], and

Pythia 8.175 [19,20]. The uncertainty on A from the choice of PDF is estimated following

the procedure explained in ref. [36].

The event reconstruction and selection efficiencies, εrec and εsel, as well as their

uncer-tainties, are estimated from simulation and calibrated using a data-driven method (where

applicable) derived from the method described in refs. [11–13]. The term εrecis the product

of the GEC, trigger, tracking and particle identification efficiencies. The smallest value of

εrecis found to be 9% in the τeτh3stream, while the largest value is 65% for τµτµ. The GEC

efficiency is determined from Z → l+l−decays in data collected with a relaxed requirement.

The muon and electron trigger efficiencies are evaluated as a function of η and pT using

a tag-and-probe method applied on Z → l+l− decays. The tracking efficiency for muons

uses a tag-and-probe method from Z → µ+µ− decays in data, whereas for electrons and

charged hadrons simulated samples are used. The particle identification efficiency is also

obtained by a tag-and-probe procedure. In order to cover the signal pTspectrum, different

data samples are selected: Z → µ+µ− and J/ψ → µ+µ− decays for muons, Z → e+e− and

B+ → J/ψ (→ e+_e−_)K+ _{decays for electrons, and D}∗+ _{→ D}0_{(→ K}−_π+_)π+ _{decays for}

charged hadrons.

The efficiency of the selection ranges between 20% for τeτe and 50% for τµτe. The

values are obtained from the simulation. Corrections at the level of 1% are inferred by

the comparison of the selection-variable distributions for Z → µ+µ− decays in data and

simulated samples, which are also added to the systematic uncertainty.

A summary of uncertainties is given in table 2, with the statistical uncertainty from

Nobs obtained assuming Poissonian statistics. The contribution of the LHC beam energy

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τµτµ τµτh1 τµτh3 τeτe τeτh1 τeτh3 τµτe

Tau branching fractions product 0.5 0.3 0.5 0.5 0.3 0.5 0.3

PDF, acceptance, FSR 1.3 1.9 1.5 1.3 1.9 1.5 1.3 Reconstruction 2.1 3.1 5.6 4.5 5.4 7.0 2.7 Selection 5.0 3.5 4.7 5.7 3.5 5.1 3.9 Background estimation† 3.4 3.9 3.2 19.0 5.2 8.0 2.4 Systematic 6.4 6.2 8.0 20.3 8.4 11.8 5.2 Statistical† 6.9 3.8 8.1 17.6 6.6 13.1 3.4 Beam energy 0.2 0.2 0.2 0.2 0.2 0.2 0.2 Luminosity 1.2 1.2 1.2 1.2 1.2 1.2 1.2 Total 9.6 7.5 11.5 27.0 10.8 17.7 6.5

Table 2. Relative uncertainties of the various contributions affecting the cross-section measure-ment, given in percent. The uncertainties are correlated between streams, except in rows denoted with†.

luminosity is measured using van der Meer scans [39] and beam-gas imaging method [40],

giving a combined uncertainty of 1.2% [18].

The cross-section results compared with the previous Z → µ+_µ− _{and Z → e}+_e−

mea-surements inside the same acceptance region at 8 TeV [12, 13], are presented in figure 3,

where the region is defined for Z bosons with an invariant mass between 60 and 120 GeV/c2

decaying to leptons with pT > 20 GeV/c and 2.0 < η < 4.5. The predictions from

theo-retical models are calculated with the Fewz [41, 42] generator at NNLO for the PDF

sets ABM12 [43], CT10 [44], CT14 [45], HERA15 [46], MSTW08 [35], MMHT14 [47], and

NNPDF30 [48]. A best linear unbiased estimator is used to combine the measurements

from all streams taking into account their correlations, giving a χ2 per degree of freedom

of 0.69 (p-value of 0.658). The combined cross-section is

σ_pp→Z→τ+_τ− = 95.8 ± 2.1 ± 4.6 ± 0.2 ± 1.1 pb ,

where the uncertainties are statistical, systematic, due to the LHC beam energy uncer-tainty, and to the integrated luminosity unceruncer-tainty, respectively.

Lepton universality is tested from the cross-section ratios [12,13]

σ_pp→Z→τ8 TeV +_τ− σ8 TeV pp→Z→µ+_µ− = 1.01 ± 0.05 , σ 8 TeV pp→Z→τ+_τ− σ8 TeV pp→Z→e+_e− = 1.02 ± 0.06 ,

where the uncertainties due to the LHC beam energy and to the integrated luminosity are assumed to be fully correlated as the analyses share the same dataset, whilst the statistical and systematic uncertainties are assumed to be uncorrelated.

6 Conclusion

A measurement of Z → τ+τ− production cross-section in pp collisions at √s = 8 TeV

tau-JHEP09(2018)159

Figure 3. Summary of the measurements of Z → l+l− production cross-section inside the LHCb acceptance region from pp collisions at 8 TeV. The error bar represents the total uncertainty. The dotted inner error bar corresponds to the statistical contribution. The coloured band corresponds to the combined measurement of Z → τ+_τ−_{from this analysis. The last 7 rows represent the NNLO}

predictions with different parameterizations of the PDFs.

pair of invariant mass between 60 and 120 GeV/c2, with the tau leptons having a transverse

momentum greater than 20 GeV/c, and pseudorapidity between 2.0 and 4.5.

The reconstruction of tau-pair candidates is performed in both leptonic and hadronic decay modes of the tau lepton, requiring at least one leptonic mode for the tau-pair

com-bination. The backgrounds to Z → τ+τ− are mainly from QCD and W /Z +jets and are

estimated with a data-driven method.

The production cross-section with all uncertainties summed in quadrature yields 95.8(52) pb, in agreement with the SM prediction. The results are consistent with the

Z → e+e− and Z → µ+µ− cross-sections measured at LHCb. They are compatible with

LU at the level of 6%.

Acknowledgments

We express our gratitude to our colleagues in the CERN accelerator departments for the excellent performance of the LHC. We thank the technical and administrative staff at the LHCb institutes. We acknowledge support from CERN and from the national agencies: CAPES, CNPq, FAPERJ and FINEP (Brazil); MOST and NSFC (China); CNRS/IN2P3 (France); BMBF, DFG and MPG (Germany); INFN (Italy); NWO (Netherlands); MNiSW

JHEP09(2018)159

and NCN (Poland); MEN/IFA (Romania); MinES and FASO (Russia); MinECo (Spain); SNSF and SER (Switzerland); NASU (Ukraine); STFC (United Kingdom); NSF (U.S.A.). We acknowledge the computing resources that are provided by CERN, IN2P3 (France), KIT and DESY (Germany), INFN (Italy), SURF (Netherlands), PIC (Spain), GridPP (United Kingdom), RRCKI and Yandex LLC (Russia), CSCS (Switzerland), IFIN-HH (Romania), CBPF (Brazil), PL-GRID (Poland) and OSC (U.S.A.). We are indebted to the communities behind the multiple open-source software packages on which we depend. Individual groups or members have received support from AvH Foundation (Germany), EPLANET, Marie Sk lodowska-Curie Actions and ERC (European Union), ANR, Labex

P2IO and OCEVU, and R´egion Auvergne-Rhˆone-Alpes (France), Key Research Program of

Frontier Sciences of CAS, CAS PIFI, and the Thousand Talents Program (China), RFBR, RSF and Yandex LLC (Russia), GVA, XuntaGal and GENCAT (Spain), Herchel Smith Fund, the Royal Society, the English-Speaking Union and the Leverhulme Trust (United Kingdom).

Open Access. This article is distributed under the terms of the Creative Commons

Attribution License (CC-BY 4.0), which permits any use, distribution and reproduction in

any medium, provided the original author(s) and source are credited.

References

[1] SLD Electroweak Group, Heavy Flavour Group, LEP Electroweak Working Group, OPAL, DELPHI, ALEPH, SLD and L3 collaborations, S. Schael et al., Precision electroweak measurements on the Z resonance,Phys. Rept. 427 (2006) 257

[hep-ex/0509008] [INSPIRE].

[2] F. Heinemann, The Discovery potential of the ˜χ0

2 in mSUGRA in the τ -channel at high tan β

at the LHC, Ph.D. Thesis, ETH, Zurich Switzerland (2003),hep-ex/0406056[INSPIRE].

[3] U. Ellwanger, A. Florent and D. Zerwas, Discovering the constrained NMSSM with tau leptons at the LHC,JHEP 01 (2011) 103[arXiv:1011.0931] [INSPIRE].

[4] G. Perez and L. Randall, Natural Neutrino Masses and Mixings from Warped Geometry, JHEP 01 (2009) 077[arXiv:0805.4652] [INSPIRE].

[5] S. Casagrande, F. Goertz, U. Haisch, M. Neubert and T. Pfoh, Flavor Physics in the Randall-Sundrum Model: I. Theoretical Setup and Electroweak Precision Tests,JHEP 10 (2008) 094[arXiv:0807.4937] [INSPIRE].

[6] R. Harnik, J. Kopp and J. Zupan, Flavor Violating Higgs Decays,JHEP 03 (2013) 026 [arXiv:1209.1397] [INSPIRE].

[7] G. Blankenburg, J. Ellis and G. Isidori, Flavour-Changing Decays of a 125 GeV Higgs-like Particle,Phys. Lett. B 712 (2012) 386[arXiv:1202.5704] [INSPIRE].

[8] J.L. Diaz-Cruz and J.J. Toscano, Lepton flavor violating decays of Higgs bosons beyond the standard model,Phys. Rev. D 62 (2000) 116005[hep-ph/9910233] [INSPIRE].

[9] A. Goudelis, O. Lebedev and J.-h. Park, Higgs-induced lepton flavor violation,Phys. Lett. B 707 (2012) 369[arXiv:1111.1715] [INSPIRE].

JHEP09(2018)159

Higgs boson to µ∓τ± decay in supersymmetry without R parity,Phys. Rev. D 87 (2013) 015025[arXiv:1210.8241] [INSPIRE].

[11] LHCb collaboration, A study of the Z production cross-section in pp collisions at √

s = 7 TeV using tau final states,JHEP 01 (2013) 111[arXiv:1210.6289] [INSPIRE].

[12] LHCb collaboration, Measurement of forward W and Z boson production in pp collisions at √

s = 8 TeV,JHEP 01 (2016) 155[arXiv:1511.08039] [INSPIRE].

[13] LHCb collaboration, Measurement of forward Z → e+_e− _{production at}√_{s = 8 TeV,JHEP}

05 (2015) 109[arXiv:1503.00963] [INSPIRE].

[14] ATLAS collaboration, Simultaneous measurements of the t¯t, W+_W− _{and Z/γ}∗_{→ τ τ}

production cross-sections in pp collisions at √s = 7 TeV with the ATLAS detector,Nucl. Part. Phys. Proc. 273–275 (2016) 2192[INSPIRE].

[15] CMS collaboration, Measurement of the inclusive Z cross section via decays to tau pairs in pp collisions at√s = 7 TeV,JHEP 08 (2011) 117[arXiv:1104.1617] [INSPIRE].

[16] LHCb collaboration, The LHCb Detector at the LHC,2008 JINST 3 S08005[INSPIRE].

[17] LHCb collaboration, LHCb Detector Performance, Int. J. Mod. Phys. A 30 (2015) 1530022 [arXiv:1412.6352] [INSPIRE].

[18] LHCb collaboration, Precision luminosity measurements at LHCb,2014 JINST 9 P12005 [arXiv:1410.0149] [INSPIRE].

[19] T. Sj¨ostrand, S. Mrenna and P.Z. Skands, A Brief Introduction to PYTHIA 8.1,Comput. Phys. Commun. 178 (2008) 852[arXiv:0710.3820] [INSPIRE].

[20] T. Sj¨ostrand, S. Mrenna and P.Z. Skands, PYTHIA 6.4 Physics and Manual, JHEP 05 (2006) 026[hep-ph/0603175] [INSPIRE].

[21] LHCb collaboration, Handling of the generation of primary events in Gauss, the LHCb simulation framework,J. Phys. Conf. Ser. 331 (2011) 032047[INSPIRE].

[22] J. Pumplin, D.R. Stump, J. Huston, H.L. Lai, P.M. Nadolsky and W.K. Tung, New generation of parton distributions with uncertainties from global QCD analysis,JHEP 07 (2002) 012[hep-ph/0201195] [INSPIRE].

[23] D.J. Lange, The EvtGen particle decay simulation package, Nucl. Instrum. Meth. A 462 (2001) 152[INSPIRE].

[24] P. Golonka and Z. Was, PHOTOS Monte Carlo: A Precision tool for QED corrections in Z and W decays,Eur. Phys. J. C 45 (2006) 97[hep-ph/0506026] [INSPIRE].

[25] Geant4 collaboration, J. Allison et al., Geant4 developments and applications, IEEE Trans. Nucl. Sci. 53 (2006) 270[INSPIRE].

[26] GEANT4 collaboration, S. Agostinelli et al., GEANT4: A Simulation toolkit,Nucl. Instrum. Meth. A 506 (2003) 250[INSPIRE].

[27] LHCb collaboration, The LHCb simulation application, Gauss: Design, evolution and experience,J. Phys. Conf. Ser. 331 (2011) 032023 [INSPIRE].

[28] LHCb collaboration, LHCb calorimeters and muon system lepton identification,AIP Conf. Proc. 722 (2004) 123.

[29] LHCb collaboration, Measurement of the ratio of the B0_{→ D}∗−_τ+_ν

τ and B0→ D∗−µ+νµ

branching fractions using three-prong τ -lepton decays,Phys. Rev. Lett. 120 (2018) 171802 [arXiv:1708.08856] [INSPIRE].

JHEP09(2018)159

Chin. Phys. C 40 (2016) 100001[INSPIRE].

[31] S. Alioli, P. Nason, C. Oleari and E. Re, NLO vector-boson production matched with shower in POWHEG,JHEP 07 (2008) 060[arXiv:0805.4802] [INSPIRE].

[32] P. Nason, A New method for combining NLO QCD with shower Monte Carlo algorithms, JHEP 11 (2004) 040[hep-ph/0409146] [INSPIRE].

[33] S. Frixione, P. Nason and C. Oleari, Matching NLO QCD computations with Parton Shower simulations: the POWHEG method,JHEP 11 (2007) 070[arXiv:0709.2092] [INSPIRE].

[34] S. Alioli, P. Nason, C. Oleari and E. Re, A general framework for implementing NLO calculations in shower Monte Carlo programs: the POWHEG BOX,JHEP 06 (2010) 043 [arXiv:1002.2581] [INSPIRE].

[35] A.D. Martin, W.J. Stirling, R.S. Thorne and G. Watt, Parton distributions for the LHC, Eur. Phys. J. C 63 (2009) 189[arXiv:0901.0002] [INSPIRE].

[36] M. Botje et al., The PDF4LHC Working Group Interim Recommendations, arXiv:1101.0538[INSPIRE].

[37] E. Todesco and J. Wenninger, Large Hadron Collider momentum calibration and accuracy, Phys. Rev. Accel. Beams 20 (2017) 081003[INSPIRE].

[38] S. Catani, L. Cieri, G. Ferrera, D. de Florian and M. Grazzini, Vector boson production at hadron colliders: a fully exclusive QCD calculation at NNLO,Phys. Rev. Lett. 103 (2009) 082001[arXiv:0903.2120] [INSPIRE].

[39] S. van der Meer, Calibration of the effective beam height in the ISR,CERN-ISR-PO-68-31 (1968) [INSPIRE].

[40] M. Ferro-Luzzi, Proposal for an absolute luminosity determination in colliding beam experiments using vertex detection of beam-gas interactions,Nucl. Instrum. Meth. A 553 (2005) 388[INSPIRE].

[41] Y. Li and F. Petriello, Combining QCD and electroweak corrections to dilepton production in FEWZ,Phys. Rev. D 86 (2012) 094034[arXiv:1208.5967] [INSPIRE].

[42] R. Gavin, Y. Li, F. Petriello and S. Quackenbush, FEWZ 2.0: A code for hadronic Z production at next-to-next-to-leading order,Comput. Phys. Commun. 182 (2011) 2388 [arXiv:1011.3540] [INSPIRE].

[43] S. Alekhin, J. Blumlein and S. Moch, The ABM parton distributions tuned to LHC data, Phys. Rev. D 89 (2014) 054028[arXiv:1310.3059] [INSPIRE].

[44] H.-L. Lai et al., New parton distributions for collider physics,Phys. Rev. D 82 (2010) 074024 [arXiv:1007.2241] [INSPIRE].

[45] S. Dulat et al., New parton distribution functions from a global analysis of quantum chromodynamics,Phys. Rev. D 93 (2016) 033006[arXiv:1506.07443] [INSPIRE].

[46] ZEUS and H1 collaborations, F.D. Aaron et al., Combined Measurement and QCD Analysis of the Inclusive e±p Scattering Cross Sections at HERA,JHEP 01 (2010) 109

[arXiv:0911.0884] [INSPIRE].

[47] L.A. Harland-Lang, A.D. Martin, P. Motylinski and R.S. Thorne, Parton distributions in the LHC era: MMHT 2014 PDFs,Eur. Phys. J. C 75 (2015) 204[arXiv:1412.3989] [INSPIRE].

[48] NNPDF collaboration, R.D. Ball et al., Parton distributions for the LHC Run II,JHEP 04 (2015) 040[arXiv:1410.8849] [INSPIRE].

JHEP09(2018)159

The LHCb collaboration

R. Aaij27, B. Adeva41, M. Adinolfi48, C.A. Aidala73, Z. Ajaltouni5, S. Akar59, P. Albicocco18, J. Albrecht10_{, F. Alessio}42_{, M. Alexander}53_{, A. Alfonso Albero}40_{, S. Ali}27_{, G. Alkhazov}33_,

P. Alvarez Cartelle55_{, A.A. Alves Jr}59_{, S. Amato}2_{, S. Amerio}23_{, Y. Amhis}7_{, L. An}3_,

L. Anderlini17_{, G. Andreassi}43_{, M. Andreotti}16,g_{, J.E. Andrews}60_{, R.B. Appleby}56_{, F. Archilli}27_,

P. d’Argent12, J. Arnau Romeu6, A. Artamonov39, M. Artuso61, K. Arzymatov37, E. Aslanides6, M. Atzeni44_{, S. Bachmann}12_{, J.J. Back}50_{, S. Baker}55_{, V. Balagura}7,b_{, W. Baldini}16_{, A. Baranov}37_,

R.J. Barlow56_{, S. Barsuk}7_{, W. Barter}56_{, F. Baryshnikov}70_{, V. Batozskaya}31_{, B. Batsukh}61_,

V. Battista43, A. Bay43, J. Beddow53, F. Bedeschi24, I. Bediaga1, A. Beiter61, L.J. Bel27,

N. Beliy63_{, V. Bellee}43_{, N. Belloli}20,i_{, K. Belous}39_{, I. Belyaev}34,42_{, E. Ben-Haim}8_{, G. Bencivenni}18_,

S. Benson27_{, S. Beranek}9_{, A. Berezhnoy}35_{, R. Bernet}44_{, D. Berninghoff}12_{, E. Bertholet}8_,

A. Bertolin23_{, C. Betancourt}44_{, F. Betti}15,42_{, M.O. Bettler}49_{, M. van Beuzekom}27_,

Ia. Bezshyiko44, S. Bhasin48, J. Bhom29, S. Bifani47, P. Billoir8, A. Birnkraut10, A. Bizzeti17,u, M. Bjørn57_{, M.P. Blago}42_{, T. Blake}50_{, F. Blanc}43_{, S. Blusk}61_{, D. Bobulska}53_{, V. Bocci}26_,

O. Boente Garcia41_{, T. Boettcher}58_{, A. Bondar}38,w_{, N. Bondar}33_{, S. Borghi}56,42_{, M. Borisyak}37_,

M. Borsato41,42_{, F. Bossu}7_{, M. Boubdir}9_{, T.J.V. Bowcock}54_{, C. Bozzi}16,42_{, S. Braun}12_,

M. Brodski42, J. Brodzicka29, D. Brundu22, E. Buchanan48, A. Buonaura44, C. Burr56, A. Bursche22_{, J. Buytaert}42_{, W. Byczynski}42_{, S. Cadeddu}22_{, H. Cai}64_{, R. Calabrese}16,g_,

R. Calladine47_{, M. Calvi}20,i_{, M. Calvo Gomez}40,m_{, A. Camboni}40,m_{, P. Campana}18_,

D.H. Campora Perez42, L. Capriotti56, A. Carbone15,e, G. Carboni25, R. Cardinale19,h, A. Cardini22_{, P. Carniti}20,i_{, L. Carson}52_{, K. Carvalho Akiba}2_{, G. Casse}54_{, L. Cassina}20_,

M. Cattaneo42_{, G. Cavallero}19,h_{, R. Cenci}24,p_{, D. Chamont}7_{, M.G. Chapman}48_{, M. Charles}8_,

Ph. Charpentier42_{, G. Chatzikonstantinidis}47_{, M. Chefdeville}4_{, V. Chekalina}37_{, C. Chen}3_,

S. Chen22, S.-G. Chitic42, V. Chobanova41, M. Chrzaszcz42, A. Chubykin33, P. Ciambrone18, X. Cid Vidal41_{, G. Ciezarek}42_{, P.E.L. Clarke}52_{, M. Clemencic}42_{, H.V. Cliff}49_{, J. Closier}42_,

V. Coco42_{, J. Cogan}6_{, E. Cogneras}5_{, L. Cojocariu}32_{, P. Collins}42_{, T. Colombo}42_,

A. Comerma-Montells12, A. Contu22, G. Coombs42, S. Coquereau40, G. Corti42, M. Corvo16,g, C.M. Costa Sobral50, B. Couturier42, G.A. Cowan52, D.C. Craik58, A. Crocombe50,

M. Cruz Torres1_{, R. Currie}52_{, C. D’Ambrosio}42_{, F. Da Cunha Marinho}2_{, C.L. Da Silva}74_,

E. Dall’Occo27_{, J. Dalseno}48_{, A. Danilina}34_{, A. Davis}3_{, O. De Aguiar Francisco}42_{, K. De Bruyn}42_,

S. De Capua56, M. De Cian43, J.M. De Miranda1, L. De Paula2, M. De Serio14,d, P. De Simone18, C.T. Dean53_{, D. Decamp}4_{, L. Del Buono}8_{, B. Delaney}49_{, H.-P. Dembinski}11_{, M. Demmer}10_,

A. Dendek30_{, D. Derkach}37_{, O. Deschamps}5_{, F. Desse}7_{, F. Dettori}54_{, B. Dey}65_{, A. Di Canto}42_,

P. Di Nezza18_{, S. Didenko}70_{, H. Dijkstra}42_{, F. Dordei}42_{, M. Dorigo}42,y_{, A. Dosil Su´arez}41_,

L. Douglas53, A. Dovbnya45, K. Dreimanis54, L. Dufour27, G. Dujany8, P. Durante42, J.M. Durham74_{, D. Dutta}56_{, R. Dzhelyadin}39_{, M. Dziewiecki}12_{, A. Dziurda}29_{, A. Dzyuba}33_,

S. Easo51_{, U. Egede}55_{, V. Egorychev}34_{, S. Eidelman}38,w_{, S. Eisenhardt}52_{, U. Eitschberger}10_,

R. Ekelhof10, L. Eklund53, S. Ely61, A. Ene32, S. Escher9, S. Esen27, T. Evans59, A. Falabella15, N. Farley47, S. Farry54, D. Fazzini20,42,i, L. Federici25, G. Fernandez40, P. Fernandez Declara42, A. Fernandez Prieto41_{, F. Ferrari}15_{, L. Ferreira Lopes}43_{, F. Ferreira Rodrigues}2_{, M. Ferro-Luzzi}42_,

S. Filippov36_{, R.A. Fini}14_{, M. Fiorini}16,g_{, M. Firlej}30_{, C. Fitzpatrick}43_{, T. Fiutowski}30_,

F. Fleuret7,b, M. Fontana22,42, F. Fontanelli19,h, R. Forty42, V. Franco Lima54, M. Frank42, C. Frei42_{, J. Fu}21,q_{, W. Funk}42_{, C. F¨arber}42_{, M. F´eo Pereira Rivello Carvalho}27_{, E. Gabriel}52_,

A. Gallas Torreira41_{, D. Galli}15,e_{, S. Gallorini}23_{, S. Gambetta}52_{, M. Gandelman}2_{, P. Gandini}21_,

Y. Gao3_{, L.M. Garcia Martin}72_{, B. Garcia Plana}41_{, J. Garc´ıa Pardi˜nas}44_{, J. Garra Tico}49_,

L. Garrido40, D. Gascon40, C. Gaspar42, L. Gavardi10, G. Gazzoni5, D. Gerick12, E. Gersabeck56, M. Gersabeck56_{, T. Gershon}50_{, D. Gerstel}6_{, Ph. Ghez}4_{, S. Gian`ı}43_{, V. Gibson}49_{, O.G. Girard}43_,

JHEP09(2018)159

I.V. Gorelov35_{, C. Gotti}20,i_{, E. Govorkova}27_{, J.P. Grabowski}12_{, R. Graciani Diaz}40_,

L.A. Granado Cardoso42, E. Graug´es40, E. Graverini44, G. Graziani17, A. Grecu32, R. Greim27, P. Griffith22, L. Grillo56, L. Gruber42, B.R. Gruberg Cazon57, O. Gr¨unberg67, C. Gu3,

E. Gushchin36_{, Yu. Guz}39,42_{, T. Gys}42_{, C. G¨obel}62_{, T. Hadavizadeh}57_{, C. Hadjivasiliou}5_,

G. Haefeli43_{, C. Haen}42_{, S.C. Haines}49_{, B. Hamilton}60_{, X. Han}12_{, T.H. Hancock}57_,

S. Hansmann-Menzemer12, N. Harnew57, S.T. Harnew48, T. Harrison54, C. Hasse42, M. Hatch42, J. He63_{, M. Hecker}55_{, K. Heinicke}10_{, A. Heister}9_{, K. Hennessy}54_{, L. Henry}72_{, E. van Herwijnen}42_,

M. Heß67_{, A. Hicheur}2_{, D. Hill}57_{, M. Hilton}56_{, P.H. Hopchev}43_{, W. Hu}65_{, W. Huang}63_,

Z.C. Huard59_{, W. Hulsbergen}27_{, T. Humair}55_{, M. Hushchyn}37_{, D. Hutchcroft}54_{, D. Hynds}27_,

P. Ibis10, M. Idzik30, P. Ilten47, K. Ivshin33, R. Jacobsson42, J. Jalocha57, E. Jans27, A. Jawahery60_{, F. Jiang}3_{, M. John}57_{, D. Johnson}42_{, C.R. Jones}49_{, C. Joram}42_{, B. Jost}42_,

N. Jurik57_{, S. Kandybei}45_{, M. Karacson}42_{, J.M. Kariuki}48_{, S. Karodia}53_{, N. Kazeev}37_,

M. Kecke12, F. Keizer49, M. Kelsey61, M. Kenzie49, T. Ketel28, E. Khairullin37, B. Khanji12, C. Khurewathanakul43, K.E. Kim61, T. Kirn9, S. Klaver18, K. Klimaszewski31, T. Klimkovich11, S. Koliiev46_{, M. Kolpin}12_{, R. Kopecna}12_{, P. Koppenburg}27_{, I. Kostiuk}27_{, S. Kotriakhova}33_,

M. Kozeiha5_{, L. Kravchuk}36_{, M. Kreps}50_{, F. Kress}55_{, P. Krokovny}38,w_{, W. Krupa}30_,

W. Krzemien31, W. Kucewicz29,l, M. Kucharczyk29, V. Kudryavtsev38,w, A.K. Kuonen43, T. Kvaratskheliya34,42_{, D. Lacarrere}42_{, G. Lafferty}56_{, A. Lai}22_{, D. Lancierini}44_{, G. Lanfranchi}18_,

C. Langenbruch9_{, T. Latham}50_{, C. Lazzeroni}47_{, R. Le Gac}6_{, A. Leflat}35_{, J. Lefran¸cois}7_,

R. Lef´evre5_{, F. Lemaitre}42_{, O. Leroy}6_{, T. Lesiak}29_{, B. Leverington}12_{, P.-R. Li}63_{, T. Li}3_{, Z. Li}61_,

X. Liang61, T. Likhomanenko69, R. Lindner42, F. Lionetto44, V. Lisovskyi7, X. Liu3, D. Loh50, A. Loi22_{, I. Longstaff}53_{, J.H. Lopes}2_{, G.H. Lovell}49_{, D. Lucchesi}23,o_{, M. Lucio Martinez}41_,

A. Lupato23_{, E. Luppi}16,g_{, O. Lupton}42_{, A. Lusiani}24_{, X. Lyu}63_{, F. Machefert}7_{, F. Maciuc}32_,

V. Macko43, P. Mackowiak10, S. Maddrell-Mander48, O. Maev33,42, K. Maguire56,

D. Maisuzenko33, M.W. Majewski30, S. Malde57, B. Malecki29, A. Malinin69, T. Maltsev38,w, G. Manca22,f_{, G. Mancinelli}6_{, D. Marangotto}21,q_{, J. Maratas}5,v_{, J.F. Marchand}4_{, U. Marconi}15_,

C. Marin Benito40_{, M. Marinangeli}43_{, P. Marino}43_{, J. Marks}12_{, G. Martellotti}26_{, M. Martin}6_,

M. Martinelli42, D. Martinez Santos41, F. Martinez Vidal72, A. Massafferri1, R. Matev42,

A. Mathad50_{, Z. Mathe}42_{, C. Matteuzzi}20_{, A. Mauri}44_{, E. Maurice}7,b_{, B. Maurin}43_{, A. Mazurov}47_,

M. McCann55,42_{, A. McNab}56_{, R. McNulty}13_{, J.V. Mead}54_{, B. Meadows}59_{, C. Meaux}6_,

F. Meier10_{, N. Meinert}67_{, D. Melnychuk}31_{, M. Merk}27_{, A. Merli}21,q_{, E. Michielin}23_,

D.A. Milanes66, E. Millard50, M.-N. Minard4, L. Minzoni16,g, D.S. Mitzel12, A. Mogini8, J. Molina Rodriguez1,z_{, T. Momb¨acher}10_{, I.A. Monroy}66_{, S. Monteil}5_{, M. Morandin}23_,

G. Morello18_{, M.J. Morello}24,t_{, O. Morgunova}69_{, J. Moron}30_{, A.B. Morris}6_{, R. Mountain}61_,

F. Muheim52, M. Mulder27, C.H. Murphy57, D. Murray56, D. M¨uller42, J. M¨uller10, K. M¨uller44, V. M¨uller10, P. Naik48, T. Nakada43, R. Nandakumar51, A. Nandi57, T. Nanut43, I. Nasteva2, M. Needham52_{, N. Neri}21_{, S. Neubert}12_{, N. Neufeld}42_{, M. Neuner}12_{, T.D. Nguyen}43_,

C. Nguyen-Mau43,n_{, S. Nieswand}9_{, R. Niet}10_{, N. Nikitin}35_{, A. Nogay}69_{, D.P. O’Hanlon}15_,

A. Oblakowska-Mucha30, V. Obraztsov39, S. Ogilvy18, R. Oldeman22,f, C.J.G. Onderwater68, A. Ossowska29_{, J.M. Otalora Goicochea}2_{, P. Owen}44_{, A. Oyanguren}72_{, P.R. Pais}43_{, A. Palano}14_,

M. Palutan18,42_{, G. Panshin}71_{, A. Papanestis}51_{, M. Pappagallo}52_{, L.L. Pappalardo}16,g_,

W. Parker60_{, C. Parkes}56_{, G. Passaleva}17,42_{, A. Pastore}14_{, M. Patel}55_{, C. Patrignani}15,e_,

A. Pearce42, A. Pellegrino27, G. Penso26, M. Pepe Altarelli42, S. Perazzini42, D. Pereima34, P. Perret5_{, L. Pescatore}43_{, K. Petridis}48_{, A. Petrolini}19,h_{, A. Petrov}69_{, S. Petrucci}52_,

M. Petruzzo21,q_{, B. Pietrzyk}4_{, G. Pietrzyk}43_{, M. Pikies}29_{, M. Pili}57_{, D. Pinci}26_{, J. Pinzino}42_,

F. Pisani42, A. Piucci12, V. Placinta32, S. Playfer52, J. Plews47, M. Plo Casasus41, F. Polci8, M. Poli Lener18_{, A. Poluektov}50_{, N. Polukhina}70,c_{, I. Polyakov}61_{, E. Polycarpo}2_{, G.J. Pomery}48_,

JHEP09(2018)159

C. Prouve48_{, V. Pugatch}46_{, A. Puig Navarro}44_{, H. Pullen}57_{, G. Punzi}24,p_{, W. Qian}63_{, J. Qin}63_,

R. Quagliani8, B. Quintana5, B. Rachwal30, J.H. Rademacker48, M. Rama24, M. Ramos Pernas41, M.S. Rangel2, F. Ratnikov37,x, G. Raven28, M. Ravonel Salzgeber42, M. Reboud4, F. Redi43, S. Reichert10_{, A.C. dos Reis}1_{, F. Reiss}8_{, C. Remon Alepuz}72_{, Z. Ren}3_{, V. Renaudin}7_,

S. Ricciardi51_{, S. Richards}48_{, K. Rinnert}54_{, P. Robbe}7_{, A. Robert}8_{, A.B. Rodrigues}43_,

E. Rodrigues59, J.A. Rodriguez Lopez66, M. Roehrken42, A. Rogozhnikov37, S. Roiser42,

A. Rollings57_{, V. Romanovskiy}39_{, A. Romero Vidal}41_{, M. Rotondo}18_{, M.S. Rudolph}61_{, T. Ruf}42_,

J. Ruiz Vidal72_{, J.J. Saborido Silva}41_{, N. Sagidova}33_{, B. Saitta}22,f_{, V. Salustino Guimaraes}62_,

C. Sanchez Gras27_{, C. Sanchez Mayordomo}72_{, B. Sanmartin Sedes}41_{, R. Santacesaria}26_,

C. Santamarina Rios41, M. Santimaria18, E. Santovetti25,j, G. Sarpis56, A. Sarti18,k, C. Satriano26,s_{, A. Satta}25_{, M. Saur}63_{, D. Savrina}34,35_{, S. Schael}9_{, M. Schellenberg}10_,

M. Schiller53_{, H. Schindler}42_{, M. Schmelling}11_{, T. Schmelzer}10_{, B. Schmidt}42_{, O. Schneider}43_,

A. Schopper42, H.F. Schreiner59, M. Schubiger43, M.H. Schune7, R. Schwemmer42, B. Sciascia18, A. Sciubba26,k, A. Semennikov34, E.S. Sepulveda8, A. Sergi47,42, N. Serra44, J. Serrano6,

L. Sestini23_{, P. Seyfert}42_{, M. Shapkin}39_{, Y. Shcheglov}33,†_{, T. Shears}54_{, L. Shekhtman}38,w_,

V. Shevchenko69_{, E. Shmanin}70_{, B.G. Siddi}16_{, R. Silva Coutinho}44_{, L. Silva de Oliveira}2_,

G. Simi23,o, S. Simone14,d, N. Skidmore12, T. Skwarnicki61, J.G. Smeaton49, E. Smith9, I.T. Smith52_{, M. Smith}55_{, M. Soares}15_{, l. Soares Lavra}1_{, M.D. Sokoloff}59_{, F.J.P. Soler}53_,

B. Souza De Paula2_{, B. Spaan}10_{, P. Spradlin}53_{, F. Stagni}42_{, M. Stahl}12_{, S. Stahl}42_{, P. Stefko}43_,

S. Stefkova55_{, O. Steinkamp}44_{, S. Stemmle}12_{, O. Stenyakin}39_{, M. Stepanova}33_{, H. Stevens}10_,

S. Stone61, B. Storaci44, S. Stracka24,p, M.E. Stramaglia43, M. Straticiuc32, U. Straumann44, S. Strokov71_{, J. Sun}3_{, L. Sun}64_{, K. Swientek}30_{, V. Syropoulos}28_{, T. Szumlak}30_{, M. Szymanski}63_,

S. T’Jampens4_{, Z. Tang}3_{, A. Tayduganov}6_{, T. Tekampe}10_{, G. Tellarini}16_{, F. Teubert}42_,

E. Thomas42, J. van Tilburg27, M.J. Tilley55, V. Tisserand5, S. Tolk42, L. Tomassetti16,g,

D. Tonelli24, D.Y. Tou8, R. Tourinho Jadallah Aoude1, E. Tournefier4, S. Tourneur43, M. Traill53, M.T. Tran43_{, A. Trisovic}49_{, A. Tsaregorodtsev}6_{, A. Tully}49_{, N. Tuning}27,42_{, A. Ukleja}31_,

A. Usachov7_{, A. Ustyuzhanin}37_{, U. Uwer}12_{, C. Vacca}22,f_{, A. Vagner}71_{, V. Vagnoni}15_{, A. Valassi}42_,

S. Valat42, G. Valenti15, R. Vazquez Gomez42, P. Vazquez Regueiro41, S. Vecchi16, M. van Veghel27_{, J.J. Velthuis}48_{, M. Veltri}17,r_{, G. Veneziano}57_{, A. Venkateswaran}61_,

T.A. Verlage9_{, M. Vernet}5_{, M. Vesterinen}57_{, J.V. Viana Barbosa}42_{, D. Vieira}63_,

M. Vieites Diaz41_{, H. Viemann}67_{, X. Vilasis-Cardona}40,m_{, A. Vitkovskiy}27_{, M. Vitti}49_,

V. Volkov35, A. Vollhardt44, B. Voneki42, A. Vorobyev33, V. Vorobyev38,w, J.A. de Vries27, C. V´azquez Sierra27_{, R. Waldi}67_{, J. Walsh}24_{, J. Wang}61_{, M. Wang}3_{, Y. Wang}65_{, Z. Wang}44_,

D.R. Ward49_{, H.M. Wark}54_{, N.K. Watson}47_{, D. Websdale}55_{, A. Weiden}44_{, C. Weisser}58_,

M. Whitehead9, J. Wicht50, G. Wilkinson57, M. Wilkinson61, I. Williams49, M.R.J. Williams56, M. Williams58, T. Williams47, F.F. Wilson51,42, J. Wimberley60, M. Winn7, J. Wishahi10, W. Wislicki31_{, M. Witek}29_{, G. Wormser}7_{, S.A. Wotton}49_{, K. Wyllie}42_{, D. Xiao}65_{, Y. Xie}65_,

A. Xu3_{, M. Xu}65_{, Q. Xu}63_{, Z. Xu}3_{, Z. Xu}4_{, Z. Yang}3_{, Z. Yang}60_{, Y. Yao}61_{, L.E. Yeomans}54_,

H. Yin65, J. Yu65,ab, X. Yuan61, O. Yushchenko39, K.A. Zarebski47, M. Zavertyaev11,c, D. Zhang65_{, L. Zhang}3_{, W.C. Zhang}3,aa_{, Y. Zhang}7_{, A. Zhelezov}12_{, Y. Zheng}63_{, X. Zhu}3_,

V. Zhukov9,35_{, J.B. Zonneveld}52_{, S. Zucchelli}15

1

Centro Brasileiro de Pesquisas F´ısicas (CBPF), Rio de Janeiro, Brazil

2

Universidade Federal do Rio de Janeiro (UFRJ), Rio de Janeiro, Brazil

3 _{Center for High Energy Physics, Tsinghua University, Beijing, China}

4 _{Univ. Grenoble Alpes, Univ. Savoie Mont Blanc, CNRS, IN2P3-LAPP, Annecy, France} 5 _{Clermont Universit´e, Universit´e Blaise Pascal, CNRS/IN2P3, LPC, Clermont-Ferrand, France} 6 _{Aix Marseille Universit´e, CNRS/IN2P3, CPPM, Marseille, France}

JHEP09(2018)159

8 _{LPNHE, Sorbonne Universit´e, Paris Diderot Sorbonne Paris Cit´e, CNRS/IN2P3, Paris, France} 9

I. Physikalisches Institut, RWTH Aachen University, Aachen, Germany

10

Fakult¨at Physik, Technische Universit¨at Dortmund, Dortmund, Germany

11

Max-Planck-Institut f¨ur Kernphysik (MPIK), Heidelberg, Germany

12

Physikalisches Institut, Ruprecht-Karls-Universit¨at Heidelberg, Heidelberg, Germany

13

School of Physics, University College Dublin, Dublin, Ireland

14

INFN Sezione di Bari, Bari, Italy

15

INFN Sezione di Bologna, Bologna, Italy

16 _{INFN Sezione di Ferrara, Ferrara, Italy} 17 _{INFN Sezione di Firenze, Firenze, Italy}

18 _{INFN Laboratori Nazionali di Frascati, Frascati, Italy} 19 _{INFN Sezione di Genova, Genova, Italy}

20 _{INFN Sezione di Milano-Bicocca, Milano, Italy} 21

INFN Sezione di Milano, Milano, Italy

22

INFN Sezione di Cagliari, Monserrato, Italy

23

INFN Sezione di Padova, Padova, Italy

24

INFN Sezione di Pisa, Pisa, Italy

25

INFN Sezione di Roma Tor Vergata, Roma, Italy

26

INFN Sezione di Roma La Sapienza, Roma, Italy

27

Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands

28 _{Nikhef National Institute for Subatomic Physics and VU University Amsterdam, Amsterdam,}

Netherlands

29 _{Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Krak´ow, Poland} 30 _{AGH — University of Science and Technology, Faculty of Physics and Applied Computer Science,}

Krak´ow, Poland

31

National Center for Nuclear Research (NCBJ), Warsaw, Poland

32

Horia Hulubei National Institute of Physics and Nuclear Engineering, Bucharest-Magurele, Romania

33

Petersburg Nuclear Physics Institute (PNPI), Gatchina, Russia

34

Institute of Theoretical and Experimental Physics (ITEP), Moscow, Russia

35

Institute of Nuclear Physics, Moscow State University (SINP MSU), Moscow, Russia

36

Institute for Nuclear Research of the Russian Academy of Sciences (INR RAS), Moscow, Russia

37 _{Yandex School of Data Analysis, Moscow, Russia}

38 _{Budker Institute of Nuclear Physics (SB RAS), Novosibirsk, Russia} 39 _{Institute for High Energy Physics (IHEP), Protvino, Russia} 40 _{ICCUB, Universitat de Barcelona, Barcelona, Spain}

41 _{Instituto Galego de F´ısica de Altas Enerx´ıas (IGFAE), Universidade de Santiago de Compostela,}

Santiago de Compostela, Spain

42

European Organization for Nuclear Research (CERN), Geneva, Switzerland

43

Institute of Physics, Ecole Polytechnique F´ed´erale de Lausanne (EPFL), Lausanne, Switzerland

44

Physik-Institut, Universit¨at Z¨urich, Z¨urich, Switzerland

45

NSC Kharkiv Institute of Physics and Technology (NSC KIPT), Kharkiv, Ukraine

46

Institute for Nuclear Research of the National Academy of Sciences (KINR), Kyiv, Ukraine

47

University of Birmingham, Birmingham, United Kingdom

48

H.H. Wills Physics Laboratory, University of Bristol, Bristol, United Kingdom

49 _{Cavendish Laboratory, University of Cambridge, Cambridge, United Kingdom} 50 _{Department of Physics, University of Warwick, Coventry, United Kingdom} 51 _{STFC Rutherford Appleton Laboratory, Didcot, United Kingdom}

52 _{School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom} 53

School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom

54

Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom

55

JHEP09(2018)159

57 _{Department of Physics, University of Oxford, Oxford, United Kingdom} 58

Massachusetts Institute of Technology, Cambridge, MA, United States

59

University of Cincinnati, Cincinnati, OH, United States

60

University of Maryland, College Park, MD, United States

61

Syracuse University, Syracuse, NY, United States

62

Pontif´ıcia Universidade Cat´olica do Rio de Janeiro (PUC-Rio), Rio de Janeiro, Brazil, associated to2

63

University of Chinese Academy of Sciences, Beijing, China, associated to 3

64 _{School of Physics and Technology, Wuhan University, Wuhan, China, associated to}3 65 _{Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China,}

associated to3

66 _{Departamento de Fisica, Universidad Nacional de Colombia, Bogota, Colombia, associated to}8 67 _{Institut f¨ur Physik, Universit¨at Rostock, Rostock, Germany, associated to} 12

68

Van Swinderen Institute, University of Groningen, Groningen, Netherlands, associated to27

69

National Research Centre Kurchatov Institute, Moscow, Russia, associated to34

70

National University of Science and Technology “MISIS”, Moscow, Russia, associated to34

71

National Research Tomsk Polytechnic University, Tomsk, Russia, associated to34

72

Instituto de Fisica Corpuscular, Centro Mixto Universidad de Valencia — CSIC, Valencia, Spain, associated to40

73

University of Michigan, Ann Arbor, United States, associated to61

74 _{Los Alamos National Laboratory (LANL), Los Alamos, United States, associated to} 61

a _{Universidade Federal do Triˆangulo Mineiro (UFTM), Uberaba-MG, Brazil} b _{Laboratoire Leprince-Ringuet, Palaiseau, France}

c _{P.N. Lebedev Physical Institute, Russian Academy of Science (LPI RAS), Moscow, Russia} d

Universit`a di Bari, Bari, Italy

e

Universit`a di Bologna, Bologna, Italy

f

Universit`a di Cagliari, Cagliari, Italy

g

Universit`a di Ferrara, Ferrara, Italy

h

Universit`a di Genova, Genova, Italy

i

Universit`a di Milano Bicocca, Milano, Italy

j

Universit`a di Roma Tor Vergata, Roma, Italy

k _{Universit`a di Roma La Sapienza, Roma, Italy}

l _{AGH — University of Science and Technology, Faculty of Computer Science, Electronics and}

Telecommunications, Krak´ow, Poland

m _{LIFAELS, La Salle, Universitat Ramon Llull, Barcelona, Spain} n _{Hanoi University of Science, Hanoi, Vietnam}

o

Universit`a di Padova, Padova, Italy

p

Universit`a di Pisa, Pisa, Italy

q

Universit`a degli Studi di Milano, Milano, Italy

r

Universit`a di Urbino, Urbino, Italy

s

Universit`a della Basilicata, Potenza, Italy

t

Scuola Normale Superiore, Pisa, Italy

u

Universit`a di Modena e Reggio Emilia, Modena, Italy

v

MSU — Iligan Institute of Technology (MSU-IIT), Iligan, Philippines

w _{Novosibirsk State University, Novosibirsk, Russia}

x _{National Research University Higher School of Economics, Moscow, Russia} y _{Sezione INFN di Trieste, Trieste, Italy}

z _{Escuela Agr´ıcola Panamericana, San Antonio de Oriente, Honduras} aa

School of Physics and Information Technology, Shaanxi Normal University (SNNU), Xi’an, China

ab

Physics and Micro Electronic College, Hunan University, Changsha City, China

†