<figure><img src="image_1.png" /></figure>

# Observation of an Excited $B_c^\pm$ Meson State with the ATLAS Detector

G. Aad, S. Abdel Khalek, A. Bassalat, C. Becot, S. Binet, C. Bourdarios, D.

Charfeddine, J.B. de Vivie de Regie, L. Duflot, M. Escalier, et al.

► To cite this version:

G. Aad, S. Abdel Khalek, A. Bassalat, C. Becot, S. Binet, et al., Observation of an Excited $B_c^\pm$ Meson State with the ATLAS Detector. Physical Review Letters, 2014, 113, pp.212004. 10.1103/Phys-RevLett.113.212004. in2p3-01022718

HAL Id: in2p3-01022718

https://hal.in2p3.fr/in2p3-01022718

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# Observation of an Excited $B_c^\pm$ Meson State with the ATLAS Detector

The ATLAS Collaboration

## Abstract

A search for excited states of the $B_c^\pm$ meson is performed using 4.9 fb$^{-1}$ of 7 TeV and 19.2 fb$^{-1}$ of 8 TeV $pp$ collision data collected by the ATLAS experiment at the LHC. A new state is observed through its hadronic transition to the ground state, with the latter detected in the decay $B_c^\pm \to J/\psi\pi^\pm$. The state appears in the $m(B_c^\pm\pi^+\pi^-) - m(B_c^\pm)$ mass difference distribution with a significance of 5.2 standard deviations. The mass of the observed state is 6842 $\pm$ 4 $\pm$ 5 MeV, where the first error is statistical and the second is systematic. The mass and decay of this state are consistent with expectations for the second S-wave state of the $B_c^\pm$ meson, $B_c^\pm(2S)$.
# Observation of an Excited $B_c^\pm$ Meson State with the ATLAS Detector

ATLAS Collaboration

A search for excited states of the $B_c^\pm$ meson is performed using 4.9 fb$^{-1}$ of 7 TeV and 19.2 fb$^{-1}$ of 8 TeV pp collision data collected by the ATLAS experiment at the LHC. A new state is observed through its hadronic transition to the ground state, with the latter detected in the decay $B_c^\pm \to J/\psi\pi^\pm$. The state appears in the $m(B_c^\pm\pi^+\pi^-) - m(B_c^\pm)$ mass difference distribution with a significance of 5.2 standard deviations. The mass of the observed state is 6842 $\pm$ 4 $\pm$ 5 MeV, where the first error is statistical and the second is systematic. The mass and decay of this state are consistent with expectations for the second S-wave state of the $B_c^\pm$ meson, $B_c^\pm(2S)$.

PACS numbers: 14.40.Nd

The $B_c^\pm$ meson was first observed by the CDF experiment in the semileptonic decay mode [1], and its hadronic decay mode was observed later by both CDF [2] and D0 [3] experiments. The $B_c^\pm$ meson has also been observed by the LHCb experiment in various decay modes [4]. Excited states of the $B_c^\pm$ meson have not previously been observed. The spectrum and properties of the $B_c^\pm$ family are predicted by non-relativistic potential models, perturbative QCD, and lattice calculations [5]. Measurements of the ground and excited states through fully reconstructed channels will provide tests of the predictions of these models and ultimately the opportunity to extract information on the strong interaction potential.

The second S-wave state, $B_c^\pm(2S)$, is predicted to have a mass in the range 6835–6917 MeV [5]. The next S-wave state, $B_c^\pm(3S)$, is predicted to have a mass above the threshold for decay into a BD meson pair. Both the $1S$ and $2S$ states have pseudoscalar ($0^-$) and vector ($1^-$) spin states that are predicted to differ in mass by about 20–50 MeV. Transitions between the spin states occur through soft photon radiation that escapes identification in ATLAS; the spin states cannot be separated by this analysis.

This Letter presents the observation of a new state whose mass is consistent with predictions for the $B_c^\pm(2S)$, the second S-wave state of the $B_c^\pm$ meson. The $B_c^\pm(2S)$ state is reconstructed in the decay to the $B_c^\pm$ meson and two oppositely charged pions, with the $B_c^\pm$ reconstructed through its decay to $J/\psi\pi^\pm$, $J/\psi \to \mu^+\mu^-$.

The ATLAS collaboration at the Large Hadron Collider (LHC) uses a general-purpose particle detector [6], consisting of several subsystems including the inner detector (ID), the electromagnetic and hadronic calorimeters, and the muon spectrometer (MS). Muon reconstruction at ATLAS makes use of both the ID and the MS.

Muons pass through the calorimeters and reach the MS if their momentum is above approximately 3 GeV. The inner detector features a three-component tracking system, consisting of two silicon-based detectors, the pixel detector and the microstrip semiconductor tracker (SCT), and the transition radiation tracker (TRT). ID tracks are reconstructed if their transverse momentum,

$p_T$ [7], is greater than 400 MeV and the magnitude of their pseudorapidity, $|\eta|$, is less than 2.5. Muon candidates are formed from a stand-alone MS track that is matched to an ID track [8]. In this analysis the MS is only used to identify muons, while their momentum is measured using the ID information only.

The trigger system [9] comprises three levels: the hardware-based Level-1 trigger and the High-Level Triggers (HLT), consisting of the Level-2 trigger and the Event Filter (EF). The Level-1 trigger uses resistive plate chambers (RPC) and thin gap chambers (TGC) to trigger muons in the pseudorapidity ranges of $|\eta| < 1.05$ and $1.05 < |\eta| < 2.5$, respectively. One or more regions of interest identified by the Level-1 muon trigger seed the HLT muon online reconstruction algorithms, where the responses from both the ID and the MS are combined. For this analysis the HLT selection for the $J/\psi$ requires two muons, respectively $\mu_1$ and $\mu_2$, originating at a common vertex, with the invariant mass of the muon pair lying between 2.5 GeV and 4.3 GeV. The individual muon $p_T$ thresholds are $p_T(\mu_1) > 6$ GeV and $p_T(\mu_2) > 4$ GeV.

This study uses pp collision data collected in the years 2011 ($\sqrt{s} = 7$ TeV) and 2012 ($\sqrt{s} = 8$ TeV) by the ATLAS experiment. The datasets used correspond to an integrated luminosity of 4.9 fb$^{-1}$ and 19.2 fb$^{-1}$, respectively. The luminosity estimate has an uncertainty of 1.8% in 2011 [11] and 2.8% in 2012.

To improve the resolution, peaks are sought in the distribution of the variable $Q = m(B_c^\pm\pi\pi) - m(B_c^\pm)$ – $2m(\pi^\pm)$, where $m(B_c^\pm)$ is the offline reconstructed invariant mass of the $B_c^\pm$ candidate, $m(B_c^\pm\pi\pi)$ is the invariant mass of the $B_c^\pm$ candidate combined with two charged pion candidates, and $m(\pi^\pm)$ is the charged pion mass [10]. The $B_c^\pm$ candidates are reconstructed through the decay $B_c^\pm \to J/\psi(\mu^+\mu^-)\pi^\pm$. Since hadronic decays of excited B meson states have no observable displacement from the pp interaction point, these candidates are then combined with two charged pion candidates both originating at the corresponding pp interaction point. The mass difference ($Q$) distribution is formed and analyzed in the range 0 – 700 MeV.

The $B_c^\pm$ selection criteria for the events are optimized
separately for 7 TeV and 8 TeV data using the corresponding Monte Carlo (MC) samples, produced in the ATLAS simulation framework [12, 13]. Differences between the 7 TeV and 8 TeV selection criteria are due to the higher $\sqrt{s}$ and the number of simultaneous pp interactions per bunch crossing hereafter called pile-up. The increase in the $B_c^+$ production cross section between the 7 TeV and 8 TeV MC samples is approximately 3%.

The PYTHIA 6 and 8 MC generators [14, 15], tuned for the LHC conditions [16], are used along with a dedicated PYTHIA extension for $B_c^+$ meson production, based on calculations from Ref. [17]. The following MC samples are used to optimize the event selection criteria (charge conjugates implied): $B_c^+$ decay modes $J/\psi\pi^+$, $J/\psi K^+$, $J/\psi\rho^+$ ($\rho^+ \to \pi^0\pi^+$), $J/\psi\mu^+\nu$, $J/\psi\pi^0\pi^+$, $J/\psi\pi^+\pi^-\pi^+$, as well as $J/\psi X$ produced inclusively or from $b\bar{b}$. The MC simulated events are treated in exactly the same way as the collision data, and the same analysis selections are always applied. The exclusive ($B_c^+$) channels are generated with PYTHIA 6, and inclusive ($J/\psi X$) channels are generated with PYTHIA 8.

This analysis involves several steps. First the $J/\psi$ candidates are formed as described below. Then a pion track candidate from the same vertex is added to form a $B_c^+$ meson candidate. Finally, the $B_c^+(2S)$ candidates are formed by adding two pion candidates originating at the primary vertex (PV; the selection of the primary vertex is defined below).

The $J/\psi$ candidates are reconstructed from pairs of oppositely charged muons. These pairs are fitted to a common vertex with the procedure described in Ref. [18]. The following requirements are applied to each $J/\psi$ candidate:

* The $p_T$ of the higher-$p_T$ muon candidate to be above 6 GeV, and the $p_T$ of the lower-$p_T$ muon candidate to be above 4 GeV; these are approximately the $p_T$ values for which the trigger is fully efficient.

* The $J/\psi$ vertex fit chi-square per degree of freedom $\chi^2/NDOF < 15$ (this selection keeps more than 99.9% of the candidates, and is included only to remove spurious dimuon combinations).

* The invariant mass resolution of the $J/\psi$ depends on the direction of the muons, with more forward candidates showing poorer resolutions. The sample is split into three categories and selection requirements are optimized for each of them: (1) both muons have $|\eta| < 1.05$, (2) one muon has $|\eta| < 1.05$ and the other one has $1.05 < |\eta| < 2.5$, (3) both muons have $1.05 < |\eta| < 2.5$. The invariant mass $m(\mu^+\mu^-)$ is calculated from the track parameters adjusted by the common-vertex fit to be in a three standard deviation $\pm 3\sigma$ mass window around the world average mass $m(J/\psi)$ [10], where the $J/\psi$ re-

constructed width $\sigma$ varies in the range 40–90 MeV depending on muon reconstruction precision in different regions of pseudorapidity and on the data-taking period.

Selection requirements for the $B_c^\pm$ were chosen by maximizing $S/\sqrt{S+B}$, using MC events. Here $S$ is the number of signal events and $B$ refers to the number of background MC events scaled according to the production cross section. The production cross sections are taken from the MC generators' predictions. The optimization has been carried out separately for the two different datasets.

The pion candidate from the $B_c^\pm$ is required to have $p_T > 4$ GeV. Hit requirements in the pixel detector and SCT are imposed on all tracks to ensure a reliable impact parameter reconstruction.

$B_c^\pm$ candidates are reconstructed by fitting two muon tracks from the $J/\psi$ candidate together with a pion candidate track to a common vertex. The invariant mass of the two muons is constrained to the world average of $m(J/\psi)$. The yields per unit of integrated luminosity, and the central values of the dimuon invariant mass distributions are verified to be consistent within each dataset.

A significant part of the combinatorial background consists of real $J/\psi$ candidates combined with candidate pions that are not associated with a $B_c^\pm \to J/\psi\pi^\pm$ decay. This background is reduced by imposing a lower cut on $d_0/\sigma(d_0)$; $d_0$ here represents the projection of the pion track impact parameter relative to the primary vertex onto the transverse plane, and $\sigma(d_0)$ is the track-by-track uncertainty on $d_0$. Pion candidates are required to have $d_0/\sigma(d_0) > 5$ for 7 TeV data and $> 4.5$ for 8 TeV data. In 7 TeV data the PV is defined as the collision vertex with the highest summed scalar $p_T^2$ of its constituent tracks. In 8 TeV data – the data collected with higher pile-up – the PV is identified as the vertex closest in three dimensions to the reconstructed decay vertex of the $B_c^\pm$ candidate. All reconstructed $B_c^\pm$ candidates are also required to satisfy the following selection criteria:

* the $J/\psi\pi$ vertex fit $\chi^2/NDOF < 2$ for 7 TeV and $< 1.5$ for 8 TeV data;

* the $p_T$ of the $B_c^\pm$ candidate to be above 15 GeV for 7 TeV and above 18 GeV for 8 TeV data.

Figure 1 shows the invariant mass distributions for the $B_c^\pm$ candidates for 7 TeV data and 8 TeV data in the mass range 5620–6820 MeV. Both distributions are fitted separately using an extended unbinned maximum likelihood fit, with a Gaussian function modeling the signal and an exponential modeling the background shape. The various exclusive $B_c^\pm$ decay modes mentioned above are shown to have negligible contribution to the background shape. The results of the fits are summarized in Table
I. The fitted mass values are consistent with the world average for the $B_c^{\pm}$ mass [10]. The signal yield per fb$^{-1}$ of the $B_c^{\pm}$ is lower in 8 TeV data due to the harder $p_T$ requirements. The stability of the $B_c^{\pm}$ yield was checked through its normalization to $B^{\pm} \to J/\psi K^{\pm}$ decays that were reconstructed with similar requirements.

<figure><img src="image_3.png" /><figcaption>FIG. 1: Invariant mass distributions of the reconstructed $B_c^{\pm} \to J/\psi \pi^{\pm}$ candidates in 7 TeV data (top) and in 8 TeV data (bottom). The data are represented by the points with error bars (statistical only). The solid line is the projection of the results of the unbinned maximum likelihood fit to all candidates in the mass range 5620-6820 MeV. The dashed line is the projection of the background component of the same fit.</figcaption></figure>

<table><caption>TABLE I: The results of the unbinned maximum likelihood fits of the invariant mass distribution of the $B_c^{\pm}$ candidates. Systematic uncertainties are not included.</caption><thead><tr><td>Data</td><td>Signal events</td><td>Peak mean [MeV]</td><td>Peak width [MeV]</td></tr></thead><tbody><tr><td>7 TeV</td><td>100±23</td><td>6282±8</td><td>49±12</td></tr><tr><td>8 TeV</td><td>227±25</td><td>6277±6</td><td>50±8</td></tr></tbody></table>

The reconstruction of the excited state candidates uses the $B_c^{\pm}$ ground state candidates within $\pm 3\sigma$ of the fitted

mass value of the corresponding dataset. These candidates are combined as described below with two pion candidate tracks associated with the corresponding primary vertex. The $p_T$ threshold of the pion candidates is 400 MeV. No additional selection requirement is applied to the $B_c^{\pm}(2S)$ pion candidates. The three tracks from the secondary vertex and the two tracks from the primary vertex are refitted simultaneously with the following constraints given by the decay topology: the refitted triplet of the $B_c^{\pm}$ tracks and the pair of PV pion tracks must intersect in two separate $B_c^{\pm}$ and $B_c^{\pm}(2S)$ vertices. The invariant mass of the refitted muon tracks is constrained to the $J/\psi$ world average mass, and the combined momentum of the refitted $B_c^{\pm}$ tracks must point to the $B_c^{\pm}(2S)$ vertex. When multiple $B_c^{\pm}(2S)$ candidates are found in the same event, the one with the best $\chi^2$ value returned by the fitter is kept as an excited state candidate. Wrong-charge combinations ($B_c^{\pm}\pi^+\pi^+$ and $B_c^{\pm}\pi^-\pi^-$) are kept separately for comparison with the combinatorial background shape in the right-charge combinations (oppositely charged pion pairs).

Figure 2 shows the mass difference distribution $m(B_c^{\pm}\pi\pi) - m(B_c^{\pm}) - 2m(\pi)$ for the right-charge combinations $B_c^{\pm}\pi^+\pi^-$ as well as the wrong-charge combinations.

A structure is observed in the mass difference distribution. In order to characterize it, an unbinned maximum likelihood fit to the right-charge combinations is performed. The fit includes a third-order polynomial to model the background and a Gaussian function for the structure. The background shape resulting from the fit is verified to be consistent with the wrong-charge combinations (which are not used to constrain the model in the right-charge fit) by fitting the same shape to them, with the normalization as the only free parameter. Alternative models for the signal and the background parameterizations are studied as sources of systematic uncertainty. A Breit-Wigner contribution was tested in convolution with the Gaussian function and was found to be negligible, implying that the natural width of the structure is small relative to the detector resolution. The resulting fit parameters (with statistical uncertainties only), as well as the distributions of the wrong-charge ($B_c^{\pm}\pi^+\pi^+$, $B_c^{\pm}\pi^-\pi^-$) combinations are shown in figure 2. The wrong-charge combinations are normalized to the same yield as the right-charge background.

The relative $B_c^{\pm}(2S)/B_c^{\pm}$ yield ratio is verified to be statistically consistent between the 7 TeV and 8 TeV data.

The fit finds the peak at a mass difference ($Q$) value of $288.2 \pm 5.1$ MeV in the 7 TeV data and $288.4 \pm 4.8$ MeV in the 8 TeV data. The fit yields $22 \pm 6$ signal events in the 7 TeV data and $35 \pm 13$ events in the 8 TeV data. The Gaussian width of the structure is found to be $18.2 \pm 3.8$ MeV in the 7 TeV data and $17.6 \pm 4.0$ MeV in the 8 TeV data. All uncertainties mentioned in this
<figure><img src="image_4.png" /><figcaption>FIG. 2: The $Q = m(B_c^\pm\pi\pi) - m(B_c^\pm) - 2m(\pi^\pm)$ distribution for the right-charge combinations (points with error bars) and for the same (wrong) pion charge combinations (shaded histogram) in 7 TeV data (top) and in 8 TeV data (bottom). The wrong-charge combinations are normalized to the same yield as the right-charge background. The solid line is the projection of the results of the unbinned maximum likelihood fit to all candidates in the range 0–700 MeV. The dashed line is the projection of the background component of the same fit.</figcaption></figure>

paragraph do not include systematic uncertainties.

There are two dominant sources of systematic uncertainty on the position of the peak. One comes from the uncertainty on the mass of the $B_c^\pm$ ground state candidate and is largely canceled in the mass difference distribution. The other involves systematic uncertainties in the fit of the mass difference distribution itself. The uncertainty on the mass of the $B_c^\pm(2S)$ candidate is dominated by the fitting procedure and estimated below to be about 3.6 MeV. The contribution from the uncertainty on the pion momentum scale to the $B_c^\pm$ mass is 1.2 MeV. The residual uncertainty from the $B_c^\pm$ candidate mass in the mass difference distribution, $\delta m_{B_c^\pm(2S)} = \delta m_{B_c^\pm} \times (m_{B_c^\pm}/m_{B_c^\pm(2S)})$, where the $\delta m_{B_c^\pm}$ is the world average uncertainty on the $B_c^\pm$ mass [10], is about 1.7 MeV. The systematic uncertainty on

the mass difference introduced by the fitting procedure is estimated by:

* varying the background model. An exponential threshold function ($f(Q) \sim Q^a e^{-bQ}$, where a and b are free parameters) and second- and fourth-order polynomials were considered as alternatives, resulting in a 3.4 MeV systematic uncertainty;

* varying the fit mass range from 0–700 MeV to 0–1500 MeV, results in a 1.2 MeV contribution to the systematic uncertainty;

* using different models for the signal. A single Breit–Wigner function, a Breit–Wigner function convolved with a Gaussian function, and a double Gaussian function were considered. This results in a negligible systematic uncertainty, compared to the above two;

In each case the largest difference between any of the variations mentioned and the default fit model is used as the systematic uncertainty. The values are calculated as the weighted mean of the 7 and 8 TeV mass values.

An additional systematic uncertainty of 2 MeV is obtained from the study of the mass bias in the selection of the candidate with the best $\chi^2$ of the vertex fit.

The various sources of systematic uncertainty are treated as uncorrelated. The total averaged systematic uncertainty propagated to the mass value of the new structure is approximately 4.1 MeV.

The significance of the new structure is evaluated with pseudo-experiments. A large number of background-only mass difference distributions are generated. Parameters of the generation are taken from the fit with their uncertainties to account for systematic effects. The background shape is scaled to the observed number of events. The mean mass value of the signal contribution is left free to vary within the theoretically motivated range (6835–6917 MeV) to evaluate the “look-elsewhere effect” [19]. The significance is calculated as the fraction of the pseudo-experiments in which the difference of the logarithms of fit likelihoods $\Delta\ln L$ with and without signal is larger than in the data. In terms of standard deviations the significance of the observation is $3.7\sigma$ in the 7 TeV data and $4.5\sigma$ in the 8 TeV data. For the combined 7 TeV and 8 TeV dataset the total significance of the observation is found to be $5.2\sigma$. The local significance of the observation, obtained by fixing the mean value of the signal component, is $5.4\sigma$.

In conclusion, the distribution of the mass difference $Q = m(B_c^\pm\pi^+\pi^-) - m(B_c^\pm) - 2m(\pi^\pm)$ for events with the $B_c^\pm$ meson reconstructed in its decay to $J/\psi\pi^\pm$ has been investigated in pp collisions at the LHC using the ATLAS detector. The analysis is based on an integrated luminosity of 4.9 (19.2) fb$^{-1}$ of pp collisions at a center-of-mass energy of 7 (8) TeV. A new state is observed
at $Q = 288.3 \pm 3.5 \pm 4.1$ MeV (calculated as the error weighted mean of the 7 TeV and 8 TeV mass values) corresponding to a mass of $6842 \pm 4 \pm 5$ MeV, where the first error is statistical and the second is systematic. The significance of the observation is $5.2\sigma$ with the “look elsewhere effect” taken into account, and the local significance is $5.4\sigma$. Within the uncertainties, the mass of the resonance corresponding to the observed structure is consistent with the predicted mass of the $B_c^{\pm}(2S)$ state.

We thank CERN for the very successful operation of the LHC, as well as the support staff from our institutions, without whom ATLAS could not be operated efficiently.

We acknowledge the support of ANPCyT, Argentina; YerPhI, Armenia; ARC, Australia; BMWF and FWF, Austria; ANAS, Azerbaijan; SSTC, Belarus; CNPq and FAPESP, Brazil; NSERC, NRC and CFI, Canada; CERN; CONICYT, Chile; CAS, MOST and NSFC, China; COLCIENCIAS, Colombia; MSMT CR, MPO CR and VSC CR, Czech Republic; DNRF, DNSRC and Lundbeck Foundation, Denmark; EPLANET, ERC and NSRF, European Union; IN2P3-CNRS, CEA-DSM/IRFU, France; GNSF, Georgia; BMBF, DFG, HGF, MPG and AvH Foundation, Germany; GSRT and NSRF, Greece; ISF, MINERVA, GIF, I-CORE and Benoziyo Center, Israel; INFN, Italy; MEXT and JSPS, Japan; CNRST, Morocco; FOM and NWO, Netherlands; BRF and RCN, Norway; MNiSW and NCN, Poland; GRICES and FCT, Portugal; MNE/IFA, Romania; MES of Russia and ROSATOM, Russian Federation; JINR; MSTD, Serbia; MSSR, Slovakia; ARRS and MIZŠ, Slovenia; DST/NRF, South Africa; MINECO, Spain; SRC and Wallenberg Foundation, Sweden; SER, SNSF and Cantons of Bern and Geneva, Switzerland; NSC, Taiwan; TAEK, Turkey; STFC, the Royal Society and Leverhulme Trust, United Kingdom; DOE and NSF, United States of America.

The crucial computing support from all WLCG partners is acknowledged gratefully, in particular from CERN and the ATLAS Tier-1 facilities at TRIUMF (Canada), NDGF (Denmark, Norway, Sweden), CC-IN2P3 (France), KIT/GridKA (Germany), INFN-CNAF (Italy), NL-T1 (Netherlands), PIC (Spain), ASGC (Taiwan), RAL (UK) and BNL (USA) and in the Tier-2 facilities worldwide.

[1] CDF Collaboration, F. Abe et al., Phys. Rev. Lett. 81, 2432 (1998);

[2] CDF Collaboration, A. Abulencia et al., Phys. Rev. Lett. 96, 082002 (2006); CDF Collaboration, T. Aaltonen et al., Phys. Rev. Lett. 100, 182002 (2008).

[3] D0 Collaboration, V. M. Abazov et al., Phys. Rev. Lett. 101, 012001 (2008).

[4] LHCb Collaboration, Phys. Rev. Lett. 108, 251802 (2012); LHCb Collaboration, Phys. Rev. D 87, 071103 (2013); LHCb Collaboration, Phys. Rev. D 87, 112012 (2013); LHCb Collaboration, J. High Energy Phys. 1309, (2013) 075; LHCb Collaboration, J. High Energy Phys. 1311, (2013) 094; LHCb Collaboration, Phys. Rev. Lett. 111, 181801 (2013).

[5] S. Narison, Phys. Lett. B 210, 238 (1988); W. Kwong and J. L. Rosner, Phys. Rev. D 44, 212 (1991); Y.-Q. Chen and Y.-P. Kuang, Phys. Rev. D 46, 1165 (1992); P. Jain and H. Munczek, Phys. Rev. D 48, 5403 (1993); L. Fulcher, Z. Chen and K. C. Yeong, Phys. Rev. D 47, 4122 (1993); E. Eichten and C. Quigg, Phys. Rev. D 49, 5845 (1994); V. V. Kiselev, A. K. Likhoded and A. V. Tkabladze, Phys. Rev. D 51, 3613 (1995); L. Motyka and K. Zalewski, Eur. Phys. J. C 4, 107 (1998); M. Baldicchi and G. M. Prosperi, Phys. Rev. D 62, 114024 (2000); N. Brambilla, A. Pineda, J. Soto and A. Vairo, Phys. Rev. D 63, 014023 (2001); A. Pineda and A. Vairo, Phys. Rev. D 63, 054007 (2001); D. Ebert, R. N. Faustov and V. O. Galkin, Phys. Rev. D 67, 014027 (2003); S. Godfrey, Phys. Rev. D 70, 054017 (2004); A. A. Penin, A. Pineda, V. A. Smirnov and M. Steinhauser, Phys. Lett. B 593, 124 (2004); S. Ikhdair and R. Sever, Int. J. Mod. Phys. A 20, 4035 (2005); I. F. Allison et al. (HPQCD, Fermilab Lattice, and UKQCD Collaborations), Phys. Rev. Lett. 94, 172001 (2005); D. Ebert, R. N. Faustov, V. O. Galkin, Eur. Phys. J. C 71, 1825 (2011); R. J. Dowdall, C. T. H. Davies, T. C. Hammant and R. R. Horgan, Phys. Rev. D 86, 094510 (2012).

[6] ATLAS Collaboration, JINST 3, S08003 (2008).

[7] ATLAS uses a right-handed coordinate system with its origin at the nominal interaction point (IP) in the center of the detector and the *z*-axis along the beam line. The *x*-axis points from the IP to the center of the LHC ring, and the *y*-axis points upward. Polar coordinates (r, φ) are used in the transverse (x, y) plane, φ being the azimuthal angle around the beam pipe. The pseudorapidity is defined in terms of the polar angle θ as $η = -\ln \tan(θ/2)$.

[8] ATLAS Collaboration, CERN-PH-EP-2013-154, (2014), arXiv:1404.4562.

[9] ATLAS Collaboration, Eur. Phys. J. C 72, 1849 (2012).

[10] J. Beringer et al. (Particle Data Group), Phys. Rev. D86, 010001 (2012).

[11] ATLAS Collaboration, Eur. Phys. J. C 73, 2518 (2013).

[12] ATLAS Collaboration, Eur. Phys. J. C 70, 823 (2010).

[13] S. Agostinelli et al., Nucl. Instrum. Meth. A 506, 250 (2003).

[14] T. Sjöstrand, S. Mrenna, and P. Z. Skands, J. High Energy Phys. 0605, 026 (2006).

[15] T. Sjöstrand, S. Mrenna, and P. Z. Skands, Comput. Phys. Commun. 178, 852 (2008).

[16] ATLAS Collaboration, ATLAS Note ATL-PHYS-PUB-2011-009, (2011), http://cds.cern.ch/record/1363300; ATLAS Collaboration, ATLAS Note ATL-PHYS-PUB-2011-014, (2011), https://cds.cern.ch/record/1400677; ATLAS Collaboration, ATLAS Note ATL-PHYS-PUB-2012-003, (2012), https://cds.cern.ch/record/1474107.

[17] A. V. Berezhnoy, V. V. Kiselev, and A. K. Likhoded, Z. Phys. A 356, 79 (1996); A. V. Berezhnoy, A. K. Likhoded and O. P. Yushchenko, Phys. Atom. Nucl. 59, 709 (1996); A. V. Berezhnoy, V. V. Kiselev, A. K. Likhoded and A. I. Onishchenko,
Phys. Atom. Nucl. **60**, 1729 (1997); A. V. Berezh-
noy, Phys. Atom. Nucl. **68**, 1866 (2005).

[18] ATLAS Collaboration, ATLAS Note
ATL-PHYS-2003-031, (2003),

http://inspirehep.net/record/1195847.

[19] E. Gross and O. Vitells, Eur. Phys. J. C **70**, 525 (2010),
arXiv:1005.1891.
The ATLAS Collaboration

G. Aad⁸⁴, B. Abbott¹¹², J. Abdallah¹⁵², S. Abdel Khalek¹¹⁶, O. Abdinov¹¹, R. Aben¹⁰⁶, B. Abi¹¹³, M. Abolins⁸⁹,
O.S. AbouZeid¹⁵⁹, H. Abramowicz¹⁵⁴, H. Abreu¹⁵³, R. Abreu³⁰, Y. Abulaiti¹⁴⁷a,¹⁴⁷b, B.S. Acharya¹⁶⁵a,¹⁶⁵b, a,
L. Adamczyk³⁸a, D.L. Adams²⁵, J. Adelman¹⁷⁷, S. Adomeit⁹⁹, T. Adye¹³⁰, T. Agatonovic-Jovin¹³a,
J.A. Aguilar-Saavedra¹²⁵a,¹²⁵f, M. Agustoni¹⁷, S.P. Ahlen²², F. Ahmadov⁶⁴, b, G. Aielli¹³⁴a,¹³⁴b,
H. Akerstedt¹⁴⁷a,¹⁴⁷b, T.P.A. Åkesson⁸⁰, G. Akimoto¹⁵⁶, A.V. Akimov⁹⁵, G.L. Alberghi²⁰a,²⁰b, J. Albert¹⁷⁰,
S. Albrand⁵⁵, M.J. Alconada Verzini⁷⁰, M. Aleksa³⁰, I.N. Aleksandrov⁶⁴, C. Alexa²⁶a, G. Alexander¹⁵⁴,
G. Alexandre⁴⁹, T. Alexopoulos¹⁰, M. Alhroob¹⁶⁵a,¹⁶⁵c, G. Alimonti⁹⁰a, L. Alio⁸⁴, J. Alison³¹, B.M.M. Allbrooke¹⁸,
L.J. Allison⁷¹, P.P. Allport⁷³, J. Almond⁸³, A. Aloisio¹⁰³a,¹⁰³b, A. Alonso³⁶, F. Alonso⁷⁰, C. Alpigiani⁷⁵,
A. Altheimer³⁵, B. Alvarez Gonzalez⁸⁹, M.G. Alviggios¹⁰³a,¹⁰³b, K. Amako⁶⁵, Y. Amaral Coutinho²⁴a, C. Amelung²³,
D. Amidei⁸⁸, S.P. Amor Dos Santos¹²⁵a,¹²⁵c, A. Amorim¹²⁵a,¹²⁵b, S. Amoroso⁴⁸, N. Amram¹⁵⁴, G. Amundsen²³,
C. Anastopoulos¹⁴⁰, L.S. Ancu⁴⁹, N. Andari³⁰, T. Andeen³⁵, C.F. Anders⁵⁸b, G. Anders³⁰, K.J. Anderson³¹,
A. Andreazza⁹⁰a,⁹⁰b, V. Andrei⁵⁸a, X.S. Anduaga⁷⁰, S. Angelidakis⁹, I. Angelozzi¹⁰⁶, P. Anger⁴⁴, A. Angerami³⁵,
F. Anghinolfi³⁰, A.V. Anisenkov¹⁰⁸, N. Anjos¹²⁵a, A. Annovi⁴⁷, A. Antonaki⁹, M. Antonelli⁴⁷, A. Antonov⁹⁷,
J. Antos¹⁴⁵b, F. Anulli¹³³a, M. Aoki⁶⁵, L. Aperio Bella¹⁸, R. Apolle¹¹⁹, c, G. Arabidze⁸⁹, I. Aracena¹⁴⁴, Y. Arai⁶⁵,
J.P. Araque¹²⁵a, A.T.H. Arce⁴⁵, J-F. Arguin⁹⁴, S. Argyropoulos⁴², M. Arik¹⁹a, A.J. Armbruster³⁰, O. Arnaez³⁰,
V. Arnal⁸¹, H. Arnold⁴⁸, M. Arratia²⁸, O. Arslan²¹, A. Artamonov⁹⁶, G. Artoni²³, S. Asai¹⁵⁶, N. Asbah⁴²,
A. Ashkenazi¹⁵⁴, B. Åsman¹⁴⁷a,¹⁴⁷b, L. Asquith⁶, K. Assamagan²⁵, R. Astalos¹⁴⁵a, M. Atkinson¹⁶⁶, N.B. Atlay¹⁴²,
B. Auerbach⁶, K. Augsten¹²⁷, M. Aurousseau¹⁴⁶b, G. Avolio³⁰, G. Azuelos⁹⁴, d, Y. Azuma¹⁵⁶, M.A. Baak³⁰,
A. Baas⁵⁸a, C. Bacci¹³⁵a,¹³⁵b, H. Bachacou¹³⁷, K. Bachas¹⁵⁵, M. Backes³⁰, M. Backhaus³⁰, J. Backus Mayes¹⁴⁴,
E. Badescu²⁶a, P. Bagiacchi¹³³a,¹³³b, P. Bagnaia¹³³a,¹³³b, Y. Bai³³a, T. Bain³⁵, J.T. Baines¹³⁰, O.K. Baker¹⁷⁷,
P. Balek¹²⁸, F. Balli¹³⁷, E. Banas³⁹, Sw. Banerjee¹⁷⁴, A.A.E. Bannoura¹⁷⁶, V. Bansal¹⁷⁰, H.S. Bansil¹⁸, L. Barak¹⁷³,
S.P. Baranov⁹⁵, E.L. Barberio⁸⁷, D. Barberis⁵⁰a,⁵⁰b, M. Barbero⁸⁴, T. Barillari¹⁰⁰, M. Barisonzi¹⁷⁶, T. Barklow¹⁴⁴,
N. Barlow²⁸, B.M. Barnett¹³⁰, R.M. Barnett¹⁵, Z. Barnovska⁵, A. Baroncelli¹³⁵a, G. Barone⁴⁹, A.J. Barr¹¹⁹,
F. Barreiro⁸¹, J. Barreiro Guimarães da Costa⁷³, R. Bartoldus¹⁴⁴, A.E. Barton⁷¹, P. Bartos¹⁴⁵a, V. Bartsch¹⁵⁰,
A. Bassalat¹¹⁶, A. Basye¹⁶⁶, R.L. Bates⁵³, L. Batkova¹⁴⁵a, J.R. Batley²⁸, M. Battaglia¹³⁸, M. Battistin³⁰,
F. Bauer¹³⁷, H.S. Bawa¹⁴⁴, e, T. Beau⁷⁹, P.H. Beauchemin¹⁶², R. Beccherle¹²³a,¹²³b, P. Bechtle²¹, H.P. Beck¹⁷,
K. Becker¹⁷⁶, S. Becker⁹⁹, M. Beckingham¹⁷¹, C. Becot¹¹⁶, A.J. Beddall¹⁹c, A. Beddall¹⁹c, S. Bedikian¹⁷⁷,
V.A. Bednyakov⁶⁴, C.P. Bee¹⁴⁹, L.J. Beemster¹⁰⁶, T.A. Beermann¹⁷⁶, M. Begel²⁵, K. Behr¹¹⁹,
C. Belanger-Champagne⁸⁶, P.J. Bell⁴⁹, W.H. Bell⁴⁹, G. Bella¹⁵⁴, L. Bellagamba²⁰a, A. Bellerive²⁹, M. Bellomo⁸⁵,
K. Belotskiy⁹⁷, O. Beltramello³⁰, O. Benary¹⁵⁴, D. Benchekroun¹³⁶a, K. Bendtz¹⁴⁷a,¹⁴⁷b, N. Benekos¹⁶⁶,
Y. Benhammou¹⁵⁴, E. Benhar Noccioli⁴⁹, J.A. Benitez Garcia¹⁶⁰b, D.P. Benjamin⁴⁵, J.R. Bensinger²³,
K. Benslama¹³¹, S. Bentvelsen¹⁰⁶, D. Berge¹⁰⁶, E. Bergeaas Kuutmann¹⁶, N. Berger⁵, F. Berghaus¹⁷⁰, J. Beringer¹⁵,
C. Bernard²², P. Bernat⁷⁷, C. Bernius⁷⁸, F.U. Bernlochner¹⁷⁰, T. Berry⁷⁶, P. Berta¹²⁸, C. Bertella⁸⁴,
G. Bertoli¹⁴⁷a,¹⁴⁷b, F. Bertolucci¹²³a,¹²³b, D. Bertsche¹¹², M.I. Besana⁹⁰a, G.J. Besjes¹⁰⁵, O. Bessidskaia¹⁴⁷a,¹⁴⁷b,
M. Bessner⁴², N. Besson¹³⁷, C. Betancourt⁴⁸, S. Bethke¹⁰⁰, W. Bhimji⁴⁶, R.M. Bianchi¹²⁴, L. Bianchini²³,
M. Bianco³⁰, O. Biebel⁹⁹, S.P. Bieniek⁷⁷, K. Bierwagen⁵⁴, J. Biesiada¹⁵, M. Biglietti¹³⁵a, J. Bilbao De Mendizabal⁴⁹,
H. Bilokon⁴⁷, M. Bindi⁵⁴, S. Binet¹¹⁶, A. Bingul¹⁹c, C. Bini¹³³a,¹³³b, C.W. Black¹⁵¹, J.E. Black¹⁴⁴, K.M. Black²²,
D. Blackburn¹³⁹, R.E. Blair⁶, J.-B. Blanchard¹³⁷, T. Blazek¹⁴⁵a, I. Bloch⁴², C. Blocker²³, W. Blum⁸², *,
U. Blumenschein⁵⁴, G.J. Bobbink¹⁰⁶, V.S. Bobrovnikov¹⁰⁸, S.S. Bocchetta⁸⁰, A. Bocci⁴⁵, C. Bock⁹⁹, C.R. Boddy¹¹⁹,
M. Boehler⁴⁸, T.T. Boek¹⁷⁶, J.A. Bogaerts³⁰, A.G. Bogdanchikov¹⁰⁸, A. Bogouch⁹¹, *, C. Bohm¹⁴⁷a, J. Bohm¹²⁶,
V. Boisvert⁷⁶, T. Bold³⁸a, V. Boldea²⁶a, A.S. Boldyrev⁹⁸, M. Bomben⁷⁹, M. Bona⁷⁵, M. Boonekamp¹³⁷,
A. Borisov¹²⁹, G. Borissov⁷¹, M. Borri⁸³, S. Borroni⁴², J. Bortfeldt⁹⁹, V. Bortolotto¹³⁵a,¹³⁵b, K. Bos¹⁰⁶,
D. Boscherini²⁰a, M. Bosman¹², H. Boterenbrood¹⁰⁶, J. Boudreau¹²⁴, J. Bouffard², E.V. Bouhova-Thacker⁷¹,
D. Boumediene³⁴, C. Bourdarios¹¹⁶, N. Bousson¹¹³, S. Boutouil¹³⁶d, A. Boveia³¹, J. Boyd³⁰, I.R. Boyko⁶⁴,
J. Bracinik¹⁸, A. Brandt⁸, G. Brandt¹⁵, O. Brandt⁵⁸a, U. Bratzler¹⁵⁷, B. Brau⁸⁵, J.E. Brau¹¹⁵, H.M. Braun¹⁷⁶, *,
S.F. Brazzale¹⁶⁵a,¹⁶⁵c, B. Brelier¹⁵⁹, K. Brendlinger¹²¹, A.J. Brennan⁸⁷, R. Brenner¹⁶⁷, S. Bressler¹⁷³,
K. Bristow¹⁴⁶c, T.M. Bristow⁴⁶, D. Britton⁵³, F.M. Brochu²⁸, I. Brock²¹, R. Brock⁸⁹, C. Bromberg⁸⁹, J. Bronner¹⁰⁰,
G. Brooijmans¹⁵³, T. Brooks⁷⁶, W.K. Brooks³²b, J. Brosamer¹⁵, E. Brost¹¹⁵, J. Brown⁵⁵,
P.A. Bruckman de Renstrom³⁹, D. Bruncko¹⁴⁵b, R. Bruneliere⁴⁸, S. Brunet⁶⁰, A. Bruni²⁰a, G. Bruni²⁰a,
M. Bruschi²⁰a, L. Bryngemark⁸⁰, T. Buanes¹⁴, Q. Buat¹⁴³, F. Bucci⁴⁹, P. Buchholz¹⁴², R.M. Buckingham¹¹⁹,
A.G. Buckley⁵³, S.I. Buda²⁶a, I.A. Budagov⁶⁴, F. Buehrer⁴⁸, L. Bugge¹¹⁸, M.K. Bugge¹¹⁸, O. Bulekov⁹⁷,
A.C. Bundock⁷³, H. Burckhart³⁰, S. Burdin⁷³, B. Burghgrave¹⁰⁷, S. Burke¹³⁰, I. Burmeister⁴³, E. Busato³⁴,
D. Büscher⁴⁸, V. Büscher⁸², P. Bussey⁵³, C.P. Buszello¹⁶⁷, B. Butler⁵⁷, J.M. Butler²², A.I. Butt³, C.M. Buttar⁵³,
J.M. Butterworth⁷⁷, P. Butti¹⁰⁶, W. Buttinger²⁸, A. Buzatu⁵³, M. Byszewski¹⁰, S. Cabrera Urbán¹⁶⁸,
D. Caforio²⁰a,²⁰b, O. Cakir⁴a, P. Calafiura¹⁵, A. Calandri¹³⁷, G. Calderini⁷⁹, P. Calfayan⁹⁹, R. Calkins¹⁰⁷,
L.P. Caloba²⁴a, D. Calvet³⁴, S. Calvet³⁴, R. Camacho Toro⁴⁹, S. Camarda⁴², D. Cameron¹¹⁸, L.M. Caminada¹⁵,
R. Caminal Armadans¹², S. Campana³⁰, M. Campanelli⁷⁷, A. Campoverde¹⁴⁹, V. Canale¹⁰³a,¹⁰³b, A. Canepa¹⁶⁰a,
M. Cano Bret⁷⁵, J. Cantero⁸¹, R. Cantrill⁷⁶, T. Cao⁴⁰, M.D.M. Capeans Garrido³⁰, I. Caprini²⁶a, M. Caprini²⁶a,
M. Capua³⁷a,³⁷b, R. Caputo⁸², R. Cardarelli¹³⁴a, T. Carli³⁰, G. Carlino¹⁰³a, L. Carminati⁹⁰a,⁹⁰b, S. Caron¹⁰⁵,
E. Carquin³²a, G.D. Carrillo-Montoya¹⁴⁶c, J.R. Carter²⁸, J. Carvalho¹²⁵a,¹²⁵c, D. Casadei⁷⁷, M.P. Casado¹²,
M. Casolino¹², E. Castaneda-Miranda¹⁴⁶b, A. Castelli¹⁰⁶, V. Castillo Gimenez¹⁶⁸, N.F. Castro¹²⁵a, P. Catastini⁵⁷,
A. Catinaccio³⁰, J.R. Catmore¹¹⁸, A. Cattai³⁰, G. Cattani¹³⁴a,¹³⁴b, S. Caughron⁸⁹, V. Cavaliere¹⁶⁶, D. Cavalli⁹⁰a,
M. Cavalli-Sforza¹², V. Cavasinni¹²³a,¹²³b, F. Ceradini¹³⁵a,¹³⁵b, B. Cerio⁴⁵, K. Cerny¹²⁸, A.S. Cerqueira²⁴b,
A. Cerri¹⁵⁰, L. Cerrito⁷⁵, F. Cerutti¹⁵, M. Cerv³⁰, A. Cervelli¹⁷, S.A. Cetin¹⁹b, A. Chafaq¹³⁶a, D. Chakraborty¹⁰⁷,
I. Chalupkova¹²⁸, P. Chang¹⁶⁶, B. Chapleau⁸⁶, J.D. Chapman²⁸, D. Charfeddine¹¹⁶, D.G. Charlton¹⁸, C.C. Chau¹⁵⁹,
C.A. Chavez Barajas¹⁵⁰, S. Cheatham⁸⁶, A. Chegwidden⁸⁹, S. Chekanov⁶, S.V. Chekulaev¹⁶⁰a, G.A. Chelkov⁶⁴f,
M.A. Chelstowska⁸⁸, C. Chen⁶³, H. Chen²⁵, K. Chen¹⁴⁹, L. Chen³³d,g, S. Chen³³c, X. Chen¹⁴⁶c, Y. Chen³⁵,
H.C. Cheng⁸⁸, Y. Cheng³¹, A. Cheplakov⁶⁴, R. Cherkaoui El Moursli¹³⁶e, V. Chernyatin²⁵*, E. Cheu⁷,
L. Chevalier¹³⁷, V. Chiarella⁴⁷, G. Chiefari¹⁰³a,¹⁰³b, J.T. Childers⁶, A. Chilingarov⁷¹, G. Chiodini⁷²a,
A.S. Chisholm¹⁸, R.T. Chislett⁷⁷, A. Chitan²⁶a, M.V. Chizhov⁶⁴, S. Chouridou⁹, B.K.B. Chow⁹⁹,
D. Chromek-Burckhart³⁰, M.L. Chu¹⁵², J. Chudoba¹²⁶, J.J. Chwastowski³⁹, L. Chytka¹¹⁴, G. Ciapetti¹³³a,¹³³b,
A.K. Ciftci⁴a, R. Ciftci⁴a, D. Cinca⁵³, V. Cindro⁷⁴, A. Ciocio¹⁵, P. Cirkovic¹³b, Z.H. Citron¹⁷³, M. Citterio⁹⁰a,
M. Ciubancan²⁶a, A. Clark⁴⁹, P.J. Clark⁴⁶, R.N. Clarke¹⁵, W. Cleland¹²⁴, J.C. Clemens⁸⁴, C. Clement¹⁴⁷a,¹⁴⁷b,
Y. Coadou⁸⁴, M. Cobal¹⁶⁵a,¹⁶⁵c, A. Coccaro¹³⁹, J. Cochran⁶³, L. Coffey²³, J.G. Cogan¹⁴⁴, J. Coggeshall¹⁶⁶,
B. Cole³⁵, S. Cole¹⁰⁷, A.P. Colijn¹⁰⁶, J. Collot⁵⁵, T. Colombo⁵⁸c, G. Colon⁸⁵, G. Compostella¹⁰⁰,
P. Conde Muiño¹²⁵a,¹²⁵b, E. Coniavitis⁴⁸, M.C. Conidi¹², S.H. Connell¹⁴⁶b, I.A. Connelly⁷⁶, S.M. Consonni⁹⁰a,⁹⁰b,
V. Consorti⁴⁸, S. Constantinescu²⁶a, C. Conta¹²⁰a,¹²⁰b, G. Conti⁵⁷, F. Conventi¹⁰³a,h, M. Cooke¹⁵, B.D. Cooper⁷⁷,
A.M. Cooper-Sarkar¹¹⁹, N.J. Cooper-Smith⁷⁶, K. Copic¹⁵, T. Cornelissen¹⁷⁶, M. Corradi²⁰a, F. Corriveau⁸⁶i,
A. Corso-Radu¹⁶⁴, A. Cortes-Gonzalez¹², G. Cortiana¹⁰⁰, G. Costa⁹⁰a, M.J. Costa¹⁶⁸, D. Costanzo¹⁴⁰, D. Côté⁸,
G. Cottin²⁸, G. Cowan⁷⁶, B.E. Cox⁸³, K. Cranmer¹⁰⁹, G. Cree²⁹, S. Crépé-Renaudin⁵⁵, F. Crescioli⁷⁹,
W.A. Cribbs¹⁴⁷a,¹⁴⁷b, M. Crispin Ortuzar¹¹⁹, M. Cristinziani²¹, V. Croft¹⁰⁵, G. Crosetti³⁷a,³⁷b, C.-M. Cuciuc²⁶a,
T. Cuhadar Donszelmann¹⁴⁰, J. Cummings¹⁷⁷, M. Curatolo⁴⁷, C. Cuthbert¹⁵¹, H. Czirr¹⁴², P. Czodrowski³,
Z. Czyczula¹⁷⁷, S. D'Auria⁵³, M. D'Onofrio⁷³, M.J. Da Cunha Sargedas De Sousa¹²⁵a,¹²⁵b, C. Da Via⁸³,
W. Dabrowski³⁸a, A. Dafinca¹¹⁹, T. Dai⁸⁸, O. Dale¹⁴, F. Dallaire⁹⁴, C. Dallapiccola⁵⁸, M. Dam³⁶, A.C. Daniells¹⁸,
M. Dano Hoffmann¹³⁷, V. Dao¹⁰⁵, G. Darbo⁵⁰a, S. Darmora⁸, J.A. Dassoulas⁴², A. Dattagupta⁶⁰, W. Davey²¹,
C. David¹⁷⁰, T. Davidek¹²⁸, E. Davies¹¹⁹c, M. Davies¹⁵⁴, O. Davignon⁷⁹, A.R. Davison⁷⁷, P. Davison⁷⁷,
Y. Davygora⁵⁸a, E. Dawe¹⁴³, I. Dawson¹⁴⁰, R.K. Daya-Ishmukhametova⁸⁵, K. De⁸, R. de Asmundis¹⁰³a,
S. De Castro²⁰a,²⁰b, S. De Cecco⁷⁹, N. De Groot¹⁰⁵, P. de Jong¹⁰⁶, H. De la Torre⁸¹, F. De Lorenzi⁶³,
L. De Nooij¹⁰⁶, D. De Pedis¹³³a, A. De Salvo¹³³a, U. De Sanctis¹⁶⁵a,¹⁶⁵b, A. De Santo¹⁵⁰, J.B. De Vivie De Regie¹¹⁶,
W.J. Dearnaley⁷¹, R. Debbel²⁵, C. Debenedetti¹³⁸, B. Dechenaux⁵⁵, D.V. Dedovich⁶⁴, I. Deigaard¹⁰⁶, J. Del Peso⁸¹,
T. Del Prete¹²³a,¹²³b, F. Deliot¹³⁷, C.M. Delitzsch⁴⁹, M. Deliyergiyev⁷⁴, A. Dell'Acqua³⁰, L. Dell'Asta²²,
M. Dell'Orso¹²³a,¹²³b, M. Della Pietra¹⁰³a,h, D. della Volpe⁴⁹, M. Delmastro⁵, P.A. Delsart⁵⁵, C. Deluca¹⁰⁶,
S. Demers¹⁷⁷, M. Demichev⁶⁴, A. Demilly⁷⁹, S.P. Denisov¹²⁹, D. Derendarz³⁹, J.E. Derkaoui¹³⁶d, F. Derue⁷⁹,
P. Dervan⁷³, K. Desch²¹, C. Deterre⁴², P.O. Deviveiros¹⁰⁶, A. Dewhurst¹³⁰, S. Dhaliwal¹⁰⁶, A. Di Ciaccio¹³⁴a,¹³⁴b,
L. Di Ciaccio⁵, A. Di Domenico¹³³a,¹³³b, C. Di Donato¹⁰³a,¹⁰³b, A. Di Girolamo³⁰, B. Di Girolamo³⁰,
A. Di Mattia¹⁵³, B. Di Micco¹³⁵a,¹³⁵b, R. Di Nardo⁴⁷, A. Di Simone⁴⁸, R. Di Sipio²⁰a,²⁰b, D. Di Valentino²⁹,
F.A. Dias⁴⁶, M.A. Diaz³²a, E.B. Diehl⁸⁸, J. Dietrich⁴², T.A. Dietzsch⁵⁸a, S. Diglio⁸⁴, A. Dimitrievska¹³a,
J. Dingfelder²¹, C. Dionisi¹³³a,¹³³b, P. Dita²⁶a, S. Dita²⁶a, F. Dittus³⁰, F. Djama⁸⁴, T. Djobava⁵¹b,
M.A.B. do Vale²⁴c, A. Do Valle Wemans¹²⁵a,¹²⁵g, T.K.O. Doan⁵, D. Dobos³⁰, C. Doglioni⁴⁹, T. Doherty⁵³,
T. Dohmae¹⁵⁶, J. Dolejsi¹²⁸, Z. Dolezal¹²⁸, B.A. Dolgoshein⁹⁷*, M. Donadelli²⁴d, S. Donati¹²³a,¹²³b,
P. Dondero¹²⁰a,¹²⁰b, J. Donini³⁴, J. Dopke¹³⁰, A. Doria¹⁰³a, M.T. Dova⁷⁰, A.T. Doyle⁵³, M. Dris¹⁰, J. Dubbert⁸⁸,
S. Dube¹⁵, E. Dubreuil³⁴, E. Duchovni¹⁷³, G. Duckeck⁹⁹, O.A. Ducu²⁶a, D. Duda¹⁷⁶, A. Dudarev³⁰, F. Dudziak⁶³,
L. Duflot¹¹⁶, L. Duguid⁷⁶, M. Dührssen³⁰, M. Dunford⁵⁸a, H. Duran Yildiz⁴a, M. Düren⁵², A. Durglishvili⁵¹b,
M. Dwuznik³⁸a, M. Dyndal³⁸a, J. Ebke⁹⁹, W. Edson², N.C. Edwards⁴⁶, W. Ehrenfeld²¹, T. Eifert¹⁴⁴, G. Eigen¹⁴,
K. Einsweiler¹⁵, T. Ekelof¹⁶⁷, M. El Kacimi¹³⁶c, M. Ellert¹⁶⁷, S. Elles⁵, F. Ellinghaus⁸², N. Ellis³⁰, J. Elmsheuser⁹⁹,
M. Elsing³⁰, D. Emeliyanov¹³⁰, Y. Enari¹⁵⁶, O.C. Endner⁸², M. Endo¹¹⁷, R. Engelmann¹⁴⁹, J. Erdmann¹⁷⁷,
A. Ereditato¹⁷, D. Eriksson¹⁴⁷a, G. Ernis¹⁷⁶, J. Ernst², M. Ernst²⁵, J. Ernwein¹³⁷, D. Errede¹⁶⁶, S. Errede¹⁶⁶,
E. Ertel⁸², M. Escalier¹¹⁶, H. Esch⁴³, C. Escobar¹²⁴, B. Esposito⁴⁷, A.I. Etienvre¹³⁷, E. Etzion¹⁵⁴, H. Evans⁶⁰,
A. Ezhilov¹²², L. Fabbri²⁰a,²⁰b, G. Facini³¹, R.M. Fakhrutdinov¹²⁹, S. Falciano¹³³a, R.J. Falla⁷⁷, J. Faltova¹²⁸,
Y. Fang³³a, M. Fanti⁹⁰a,⁹⁰b, A. Farbin⁸, A. Farilla¹³⁵a, T. Farooque¹², S. Farrell¹⁶⁴, S.M. Farrington¹⁷¹,
P. Farthouat³⁰, F. Fassi¹³⁶ᵉ, P. Fassnacht³⁰, D. Fassouliotis⁹, A. Favareto⁵⁰a,⁵⁰b, L. Fayard¹¹⁶, P. Federic¹⁴⁵a,
O.L. Fedin¹²², j, W. Fedorko¹⁶⁹, M. Fehling-Kaschek⁴⁸, S. Feigl³⁰, L. Feligioni⁸⁴, C. Feng³³d, E.J. Feng⁶, H. Feng⁸⁸,
A.B. Fenyuk¹²⁹, S. Fernandez Perez³⁰, S. Ferrag⁵³, J. Ferrando⁵³, A. Ferrari¹⁶⁷, P. Ferrari¹⁰⁶, R. Ferrari¹²⁰a,
D.E. Ferreira de Lima⁵³, A. Ferrer¹⁶⁸, D. Ferrere⁴⁹, C. Ferretti⁸⁸, A. Ferretto Parodi⁵⁰a,⁵⁰b, M. Fiascaris³¹,
F. Fiedler⁸², A. Filipčič⁷⁴, M. Filipuzzi⁴², F. Filthaut¹⁰⁵, M. Fincke-Keeler¹⁷⁰, K.D. Finelli¹⁵¹,
M.C.N. Fiolhais¹²⁵a,¹²⁵c, L. Fiorini¹⁶⁸, A. Firan⁴⁰, A. Fischer², J. Fischer¹⁷⁶, W.C. Fisher⁸⁹, E.A. Fitzgerald²³,
M. Flechl¹⁴⁸, I. Fleck¹⁴², P. Fleischmann⁸⁸, S. Fleischmann¹⁷⁶, G.T. Fletcher¹⁴⁰, G. Fletcher⁷⁵, T. Flick¹⁷⁶,
A. Floderus⁸⁰, L.R. Flores Castillo¹⁷⁴, k, A.C. Florez Bustos¹⁶⁰b, M.J. Flowerdew¹⁰⁰, A. Formica¹³⁷, A. Forti⁸³,
D. Fortin¹⁶⁰a, D. Fournier¹¹⁶, H. Fox⁷¹, S. Fracchia¹², P. Francavilla⁷⁹, M. Franchini²⁰a,²⁰b, S. Franchino³⁰,
D. Francis³⁰, M. Franklin⁵⁷, S. Franz⁶¹, M. Fraternali¹²⁰a,¹²⁰b, S.T. French²⁸, C. Friedrich⁴², F. Friedrich⁴⁴,
D. Froidevaux³⁰, J.A. Frost²⁸, C. Fukunaga¹⁵⁷, E. Fullana Torregrosa⁸², B.G. Fulsom¹⁴⁴, J. Fuster¹⁶⁸,
C. Gabaldon⁵⁵, O. Gabizon¹⁷³, A. Gabrielli²⁰a,²⁰b, A. Gabrielli¹³³a,¹³³b, S. Gadatsch¹⁰⁶, S. Gadomski⁴⁹,
G. Gagliardi⁵⁰a,⁵⁰b, P. Gagnon⁶⁰, C. Galea¹⁰⁵, B. Galhardo¹²⁵a,¹²⁵c, E.J. Gallas¹¹⁹, V. Gallo¹⁷, B.J. Gallop¹³⁰,
P. Gallus¹²⁷, G. Galster³⁶, K.K. Gan¹¹⁰, R.P. Gandrajula⁶², J. Gao³³b, g, Y.S. Gao¹⁴⁴, e, F.M. Garay Walls⁴⁶,
F. Garberson¹⁷⁷, C. García¹⁶⁸, J.E. García Navarro¹⁶⁸, M. Garcia-Sciveres¹⁵, R.W. Gardner³¹, N. Garelli¹⁴⁴,
V. Garonne³⁰, C. Gatti⁴⁷, G. Gaudio¹²⁰a, B. Gaur¹⁴², L. Gauthier⁹⁴, P. Gauzzi¹³³a,¹³³b, I.L. Gavrilenko⁹⁵,
C. Gay¹⁶⁹, G. Gaycken²¹, E.N. Gazis¹⁰, P. Ge³³d, Z. Gecse¹⁶⁹, C.N.P. Gee¹³⁰, D.A.A. Geerts¹⁰⁶,
Ch. Geich-Gimbel²¹, K. Gellerstedt¹⁴⁷a,¹⁴⁷b, C. Gemme⁵⁰a, A. Gemmell⁵³, M.H. Genest⁵⁵, S. Gentile¹³³a,¹³³b,
M. George⁵⁴, S. George⁷⁶, D. Gerbaudo¹⁶⁴, A. Gershon¹⁵⁴, H. Ghazlane¹³⁶b, N. Ghodbane³⁴, B. Giacobbe²⁰a,
S. Giagu¹³³a,¹³³b, V. Giangiobbe¹², P. Giannetti¹²³a,¹²³b, F. Gianotti³⁰, B. Gibbard²⁵, S.M. Gibson⁷⁶,
M. Gilchriese¹⁵, T.P.S. Gillam²⁸, D. Gillberg³⁰, G. Gilles³⁴, D.M. Gingrich³, d, N. Giokaris⁹, M.P. Giordani¹⁶⁵a,¹⁶⁵c,
R. Giordano¹⁰³a,¹⁰³b, F.M. Giorgi²⁰a, F.M. Giorgi¹⁶, P.F. Giraud¹³⁷, D. Giugni⁹⁰a, C. Giuliani⁴⁸, M. Giulini⁵⁸b,
B.K. Gjelsten¹¹⁸, S. Gkaitatzis¹⁵⁵, I. Gkialas¹⁵⁵, l, L.K. Gladilin⁹⁸, C. Glasman⁸¹, J. Glatzer³⁰, P.C.F. Glaysher⁴⁶,
A. Glazov⁴², G.L. Glonti⁶⁴, M. Goblirsch-Kolb¹⁰⁰, J.R. Goddard⁷⁵, J. Godfrey¹⁴³, J. Godlewski³⁰, C. Goeringer⁸²,
S. Goldfarb⁸⁸, T. Golling¹⁷⁷, D. Golubkov¹²⁹, A. Gomes¹²⁵a,¹²⁵b,¹²⁵d, L.S. Gomez Fajardo⁴², R. Gonçalo¹²⁵a,
J. Goncalves Pinto Firmino Da Costa¹³⁷, L. Gonella²¹, S. González de la Hoz¹⁶⁸, G. Gonzalez Parra¹²,
S. Gonzalez-Sevilla⁴⁹, L. Goossens³⁰, P.A. Gorbounov⁹⁶, H.A. Gordon²⁵, I. Gorelov¹⁰⁴, B. Gorini³⁰, E. Gorini⁷²a,⁷²b,
A. Gorišek⁷⁴, E. Gornicki³⁹, A.T. Goshaw⁶, C. Gössling⁴³, M.I. Gostkin⁶⁴, M. Gouighri¹³⁶a, D. Goujdami¹³⁶c,
M.P. Goulette⁴⁹, A.G. Goussiou¹³⁹, C. Goy⁵, S. Gozpinar²³, H.M.X. Grabas¹³⁷, L. Graber⁵⁴, I. Grabowska-Bold³⁸a,
P. Grafström²⁰a,²⁰b, K-J. Grahn⁴², J. Gramling⁴⁹, E. Gramstad¹¹⁸, S. Grancagnolo¹⁶, V. Grassi¹⁴⁹, V. Gratchev¹²²,
H.M. Gray³⁰, E. Graziani¹³⁵a, O.G. Grebenyuk¹²², Z.D. Greenwood⁷⁸, m, K. Gregersen⁷⁷, I.M. Gregor⁴²,
P. Grenier¹⁴⁴, J. Griffiths⁸, A.A. Grillo¹³⁸, K. Grimm⁷¹, S. Grinstein¹², n, Ph. Gris³⁴, Y.V. Grishkevich⁹⁸,
J.-F. Grivaz¹¹⁶, J.P. Grohs⁴⁴, A. Grohsjean⁴², E. Gross¹⁷³, J. Grosse-Knetter⁵⁴, G.C. Grossi¹³⁴a,¹³⁴b,
J. Groth-Jensen¹⁷³, Z.J. Grout¹⁵⁰, L. Guan³³b, F. Guescini⁴⁹, D. Guest¹⁷⁷, O. Gueta¹⁵⁴, C. Guichency³⁴,
E. Guido⁵⁰a,⁵⁰b, T. Guillemin¹¹⁶, S. Guindon², U. Gul⁵³, C. Gumpert⁴⁴, J. Gunther¹²⁷, J. Guo³⁵, S. Gupta¹¹⁹,
P. Gutierrez¹¹², N.G. Gutierrez Ortiz⁵³, C. Gutschow⁷⁷, N. Guttman¹⁵⁴, C. Guyot¹³⁷, C. Gwenlan¹¹⁹,
C.B. Gwilliam⁷³, A. Haas¹⁰⁹, C. Haber¹⁵, H.K. Hadavand⁸, N. Haddad¹³⁶e, P. Haefner²¹, S. Hageböck²¹,
Z. Hajduk³⁹, H. Hakobyan¹⁷⁸, M. Haleem⁴², D. Hall¹¹⁹, G. Halladjian⁸⁹, K. Hamacher¹⁷⁶, P. Hamal¹¹⁴,
K. Hamano¹⁷⁰, M. Hamer⁵⁴, A. Hamilton¹⁴⁶a, S. Hamilton¹⁶², P.G. Hamnett⁴², L. Han³³b, K. Hanagaki¹¹⁷,
K. Hanawa¹⁵⁶, M. Hance¹⁵, P. Hanke⁵⁸a, R. Hanna¹³⁷, J.B. Hansen³⁶, J.D. Hansen³⁶, P.H. Hansen³⁶, K. Hara¹⁶¹,
A.S. Hard¹⁷⁴, T. Harenberg¹⁷⁶, F. Hariri¹¹⁶, S. Harkusha⁹¹, D. Harper⁸⁸, R.D. Harrington⁴⁶, O.M. Harris¹³⁹,
P.F. Harrison¹⁷¹, F. Hartjes¹⁰⁶, S. Hasegawa¹⁰², Y. Hasegawa¹⁴¹, A. Hasib¹¹², S. Hassani¹³⁷, S. Haug¹⁷,
M. Hauschild³⁰, R. Hauser⁸⁹, M. Havranek¹²⁶, C.M. Hawkes¹⁸, R.J. Hawkings³⁰, A.D. Hawkins⁸⁰, T. Hayashi¹⁶¹,
D. Hayden⁸⁹, C.P. Hays¹¹⁹, H.S. Hayward⁷³, S.J. Haywood¹³⁰, S.J. Head¹⁸, T. Heck⁸², V. Hedberg⁸⁰, L. Heelan⁸,
S. Heim¹²¹, T. Heim¹⁷⁶, B. Heinemann¹⁵, L. Heinrich¹⁰⁹, J. Hejbal¹²⁶, L. Helary²², C. Heller⁹⁹, M. Heller³⁰,
S. Hellman¹⁴⁷a,¹⁴⁷b, D. Hellmich²¹, C. Helsens³⁰, J. Henderson¹¹⁹, R.C.W. Henderson⁷¹, Y. Heng¹⁷⁴, C. Hengler⁴²,
A. Henrichs¹⁷⁷, A.M. Henriques Correia³⁰, S. Henrot-Versille¹¹⁶, C. Hensel⁵⁴, G.H. Herbert¹⁶,
Y. Hernández Jiménez¹⁶⁸, R. Herrberg-Schubert¹⁶, G. Herten⁴⁸, R. Hertenberger⁹⁹, L. Hervas³⁰, G.G. Hesketh⁷⁷,
N.P. Hessey¹⁰⁶, R. Hickling⁷⁵, E. Higón-Rodriguez¹⁶⁸, E. Hill¹⁷⁰, J.C. Hill²⁸, K.H. Hiller⁴², S. Hillert²¹,
S.J. Hillier¹⁸, I. Hinchliffe¹⁵, E. Hines¹²¹, M. Hirose¹⁵⁸, D. Hirschbuehl¹⁷⁶, J. Hobbs¹⁴⁹, N. Hod¹⁰⁶,
M.C. Hodgkinson¹⁴⁰, P. Hodgson¹⁴⁰, A. Hoecker³⁰, M.R. Hoeferkamp¹⁰⁴, J. Hoffman⁴⁰, D. Hoffmann⁸⁴,
J.I. Hofmann⁵⁸a, M. Hohlfeld⁸², T.R. Holmes¹⁵, T.M. Hong¹²¹, L. Hooft van Huysduynen¹⁰⁹, J.-Y. Hostachy⁵⁵,
S. Hou¹⁵², A. Hoummada¹³⁶a, J. Howard¹¹⁹, J. Howarth⁴², M. Hrabovsky¹¹⁴, I. Hristova¹⁶, J. Hrivnac¹¹⁶,
T. Hryn'ova⁵, C. Hsu¹⁴⁶c, P.J. Hsu⁸², S.-C. Hsu¹³⁹, D. Hu³⁵, X. Hu²⁵, Y. Huang⁴², Z. Hubacek³⁰, F. Hubaut⁸⁴,
F. Huegging²¹, T.B. Huffman¹¹⁹, E.W. Hughes³⁵, G. Hughes⁷¹, M. Huhtinen³⁰, T.A. Hülsing⁸², M. Hurwitz¹⁵,
N. Huseynov⁶⁴, b, J. Huston⁸⁹, J. Huth⁵⁷, G. Iacobucci⁴⁹, G. Iakovidis¹⁰, I. Ibragimov¹⁴², L. Iconovidou-Fayard¹¹⁶,
E. Ideal¹⁷⁷, P. Iengo¹⁰³a, O. Igonkina¹⁰⁶, T. Iizawa¹⁷², Y. Ikegami⁶⁵, K. Ikematsu¹⁴², M. Ikeno⁶⁵, Y. Ilchenko³¹,º,
D. Iliadis¹⁵⁵, N. Ilic¹⁵⁹, Y. Inamaru⁶⁶, T. Ince¹⁰⁰, P. Ioannou⁹, M. Iodice¹³⁵a, K. Iordanidou⁹, V. Ippolito⁵⁷,
A. Irles Quiles¹⁶⁸, C. Isaksson¹⁶⁷, M. Ishino⁶⁷, M. Ishitsuka¹⁵⁸, R. Ishmukhametov¹¹⁰, C. Issever¹¹⁹, S. Istin¹⁹a,
J.M. Iturbe Ponce³⁸, R. Iuppa¹³⁴a,¹³⁴b, J. Ivarsson⁸⁰, W. Iwanski³⁹, H. Iwasaki⁶⁵, J.M. Izen⁴¹, V. Izzo¹⁰³a,
B. Jackson¹²¹, M. Jackson⁷³, P. Jackson¹, M.R. Jackel³⁰, V. Jain², K. Jakobs⁴⁸, S. Jakobsen³⁰, T. Jakoubek¹²⁶,
J. Jakubek¹²⁷, D.O. Jamin¹⁵², D.K. Jana⁷⁸, E. Jansen⁷⁷, H. Jansen³⁰, J. Janssen²¹, M. Janus¹⁷¹, G. Jarlskog⁸⁰,
N. Javadov⁶⁴,ᵇ, T. Javûrek⁴⁸, L. Jeanty¹⁵, J. Jejelava⁵¹a,ₚ, G.-Y. Jeng¹⁵¹, D. Jennens⁸⁷, P. Jenni⁴⁸,q, J. Jentzsch⁴³,
C. Jeske¹⁷¹, S. Jézéquel⁵, H. Ji¹⁷⁴, W. Ji⁸², J. Jia¹⁴⁹, Y. Jiang³³b, M. Jimenez Belenguer⁴², S. Jin³³a, A. Jinaru²⁶a,
O. Jinnouchi¹⁵⁸, M.D. Joergensen³⁶, K.E. Johansson¹⁴⁷a,¹⁴⁷b, P. Johansson¹⁴⁰, K.A. Johns⁷, K. Jon-And¹⁴⁷a,¹⁴⁷b,
G. Jones¹⁷¹, R.W.L. Jones⁷¹, T.J. Jones⁷³, J. Jongmanns⁵⁸a, P.M. Jorge¹²⁵a,¹²⁵b, K.D. Joshi⁸³, J. Jovicevic¹⁴⁸,
X. Ju¹⁷⁴, C.A. Jung⁴³, R.M. Jungst³⁰, P. Jussel⁶¹, A. Juste Rozas¹²,ⁿ, M. Kaci¹⁶⁸, A. Kaczmarska³⁹, M. Kado¹¹⁶,
H. Kagan¹¹⁰, M. Kagan¹⁴⁴, E. Kajomovitz⁴⁵, C.W. Kalderon¹¹⁹, S. Kama⁴⁰, A. Kamenshchikov¹²⁹, N. Kanaya¹⁵⁶,
M. Kaneda³⁰, S. Kaneti²⁸, V.A. Kantserov⁹⁷, J. Kanzaki⁶⁵, B. Kaplan¹⁰⁹, A. Kapliy³¹, D. Kar⁵³, K. Karakostas¹⁰,
N. Karastathis¹⁰, M. Karnevskiy⁸², S.N. Karpov⁶⁴, Z.M. Karpova⁶⁴, K. Karthik¹⁰⁹, V. Kartvelishvili⁷¹,
A.N. Karyukhin¹²⁹, L. Kashif¹⁷⁴, G. Kasieczka⁵⁸b, R.D. Kass¹¹⁰, A. Kastanas¹⁴, Y. Kataoka¹⁵⁶, A. Katre⁴⁹,
J. Katzy⁴², V. Kaushik⁷, K. Kawagoe⁶⁹, T. Kawamoto¹⁵⁶, G. Kawamura⁵⁴, S. Kazama¹⁵⁶, V.F. Kazanin¹⁰⁸,
M.Y. Kazarinov⁶⁴, R. Keeler¹⁷⁰, R. Kehoe⁴⁰, M. Keil⁵⁴, J.S. Keller⁴², J.J. Kempster⁷⁶, H. Keoshkerian⁵,
O. Kepka¹²⁶, B.P. Kerševan⁷⁴, S. Kersten¹⁷⁶, K. Kessoku¹⁵⁶, J. Keung¹⁵⁹, F. Khalil-zada¹¹, H. Khandanyan¹⁴⁷a,¹⁴⁷b,
A. Khanov¹¹³, A. Khodinov⁹⁷, A. Khomich⁵⁸a, T.J. Khoo²⁸, G. Khoriauli²¹, A. Khoroshilov¹⁷⁶, V. Khovanskiy⁹⁶,
E. Khramov⁶⁴, J. Khubua⁵¹b, H.Y. Kim⁸, H. Kim¹⁴⁷a,¹⁴⁷b, S.H. Kim¹⁶¹, N. Kimura¹⁷², O. Kind¹⁶, B.T. King⁷³,
M. King¹⁶⁸, R.S.B. King¹¹⁹, S.B. King¹⁶⁹, J. Kirk¹³⁰, A.E. Kiryunin¹⁰⁰, T. Kishimoto⁶⁶, D. Kisielewska³⁸a,
F. Kiss⁴⁸, T. Kittelmann¹²⁴, K. Kiuchi¹⁶¹, E. Kladiva¹⁴⁵b, M. Klein⁷³, U. Klein⁷³, K. Kleinknecht⁸²,
P. Klimek¹⁴⁷a,¹⁴⁷b, A. Klimentov²⁵, R. Klingenberg⁴³, J.A. Klinger⁸³, T. Klioutchnikova³⁰, P.F. Klok¹⁰⁵,
E.-E. Kluge⁵⁸a, P. Kluit¹⁰⁶, S. Kluth¹⁰⁰, E. Kneringer⁶¹, E.B.F.G. Knoops⁸⁴, A. Knue⁵³, D. Kobayashi¹⁵⁸,
T. Kobayashi¹⁵⁶, M. Kobel⁴⁴, M. Kocian¹⁴⁴, P. Kodys¹²⁸, P. Koevesarki²¹, T. Koffas²⁹, E. Koffeman¹⁰⁶,
L.A. Kogan¹¹⁹, S. Kohlmann¹⁷⁶, Z. Kohout¹²⁷, T. Kohriki⁶⁵, T. Koi¹⁴⁴, H. Kolanoski¹⁶, I. Koletsou⁵, J. Koll⁸⁹,
A.A. Komar⁹⁵,*, Y. Komori¹⁵⁶, T. Kondo⁶⁵, N. Kondrashova⁴², K. Köneke⁴⁸, A.C. König¹⁰⁵, S. König⁸²,
T. Kono⁶⁵, r, R. Konoplich¹⁰⁹, s, N. Konstantinidis⁷⁷, R. Kopeliansky¹⁵³, S. Koperny³⁸a, L. Köpke⁸², A.K. Kopp⁴⁸,
K. Korcyl³⁹, K. Kordas¹⁵⁵, A. Korn⁷⁷, A.A. Korol¹⁰⁸, t, I. Korolkov¹², E.V. Korolkova¹⁴⁰, V.A. Korotkov¹²⁹,
O. Kortner¹⁰⁰, S. Kortner¹⁰⁰, V.V. Kostyukhin²¹, V.M. Kotov⁶⁴, A. Kotwal⁴⁵, C. Kourkoumelis⁹, V. Kouskoura¹⁵⁵,
A. Koutsman¹⁶⁰a, R. Kowalewski¹⁷⁰, T.Z. Kowalski³⁸a, W. Kozanecki¹³⁷, A.S. Kozhin¹²⁹, V. Kral¹²⁷,
V.A. Kramarenko⁹⁸, G. Kramberger⁷⁴, D. Krasnopevtsev⁹⁷, M.W. Krasny⁷⁹, A. Krasznahorkay³⁰, J.K. Kraus²¹,
A. Kravchenko²⁵, S. Kreiss¹⁰⁹, M. Kretz⁵⁸c, J. Kretzschmar⁷³, K. Kreutzfeldt⁵², P. Krieger¹⁵⁹, K. Kroeninger⁵⁴,
H. Kroha¹⁰⁰, J. Kroll¹²¹, J. Kroseberg²¹, J. Krstic¹³a, U. Kruchonak⁶⁴, H. Krüger²¹, T. Kruker¹⁷, N. Krumnack⁶³,
Z.V. Krumshteyn⁶⁴, A. Kruse¹⁷⁴, M.C. Kruse⁴⁵, M. Kruskal²², T. Kubota⁸⁷, S. Kuday⁴a, S. Kuehn⁴⁸, A. Kugel⁵⁸c,
A. Kuhl¹³⁸, T. Kuhl¹²⁷, V. Kukhtin⁶⁴, Y. Kulchitsky⁹¹, S. Kuleshov³²b, M. Kuna¹³³a,¹³³b, J. Kunkle¹²¹,
A. Kupco¹²⁶, H. Kurashige⁶⁶, Y.A. Kurochkin⁹¹, R. Kurumida⁶⁶, V. Kus¹²⁶, E.S. Kuwertz¹⁴⁸, M. Kuze¹⁵⁸,
J. Kvita¹¹⁴, A. La Rosa⁴⁹, L. La Rotonda³⁷a,³⁷b, C. Lacasta¹⁶⁸, F. Lacava¹³³a,¹³³b, J. Lacey²⁹, H. Lacker¹⁶,
D. Lacour⁷⁹, V.R. Lacuesta¹⁶⁸, E. Ladygin⁶⁴, R. Lafaye⁵, B. Laforge⁷⁹, T. Lagouri¹⁷⁷, S. Lai⁴⁸, H. Laier⁵⁸a,
L. Lambourne⁷⁷, S. Lammers⁶⁰, C.L. Lampen⁷, W. Lampl⁷, E. Lançon¹³⁷, U. Landgraf⁴⁸, M.P.J. Landon⁷⁵,
V.S. Lang⁵⁸a, A.J. Lankford¹⁶⁴, F. Lanni²⁵, K. Lantzsch³⁰, S. Laplace⁷⁹, C. Lapoire²¹, J.F. Laporte¹³⁷, T. Lari⁹⁰a,
M. Lassnig³⁰, P. Laurelli⁴⁷, W. Lavrijsen¹⁵, A.T. Law¹³⁸, P. Laycock⁷³, B.T. Le⁵⁵, O. Le Dortz⁷⁹, E. Le Guirriec⁸⁴,
E. Le Menedeu¹², T. LeCompte⁶, F. Ledroit-Guillon⁵⁵, C.A. Lee¹⁵², H. Lee¹⁰⁶, J.S.H. Lee¹¹⁷, S.C. Lee¹⁵², L. Lee¹⁷⁷,
G. Lefebvre⁷⁹, M. Lefebvre¹⁷⁰, F. Legger⁹⁹, C. Leggett¹⁵, A. Lehan⁷³, M. Lehmacher²¹, G. Lehmann Miotto³⁰,
X. Lei⁷, W.A. Leight²⁹, A. Leisos¹⁵⁵, A.G. Leister¹⁷⁷, M.A.L. Leite²⁴d, R. Leitner¹²⁸, D. Lellouch¹⁷³, B. Lemmer⁵⁴,
K.J.C. Leney⁷⁷, T. Lenz¹⁰⁶, G. Lenzen¹⁷⁶, B. Lenzi³⁰, R. Leone⁷, S. Leone¹²³a,¹²³b, K. Leonhardt⁴⁴,
C. Leonidopoulos⁴⁶, S. Leontinis¹⁰, C. Leroy⁹⁴, C.G. Lester²⁸, C.M. Lester¹²¹, M. Levchenko¹²², J. Levêque⁵,
D. Levin⁸⁸, L.J. Levinson¹⁷³, M. Levy¹⁸, A. Lewis¹¹⁹, G.H. Lewis¹⁰⁹, A.M. Leyko²¹, M. Leyton⁴¹, B. Li³³b,ₐ,
B. Li⁸⁴, H. Li¹⁴⁹, H.L. Li³¹, L. Li⁴⁵, L. Li³³e, S. Li⁴⁵, Y. Li³³c,ₚ, Z. Liang¹³⁸, H. Liao³⁴, B. Liberti¹³⁴a, P. Lichard³⁰,
K. Lie¹⁶⁶, J. Liebal²¹, W. Liebig¹⁴, C. Limbach²¹, A. Limosani⁸⁷, S.C. Lin¹⁵²,ₚ, T.H. Lin⁸², F. Linde¹⁰⁶,
B.E. Lindquist¹⁴⁹, J.T. Linnemann⁸⁹, E. Lipeles¹²¹, A. Lipniacka¹⁴, M. Lisovyi⁴², T.M. Liss¹⁶⁶, D. Lissauer²⁵,
A. Lister¹⁶⁹, A.M. Litke¹³⁸, B. Liu¹⁵², D. Liu¹⁵², J.B. Liu³³b, K. Liu³³b,ₐ, L. Liu⁸⁸, M. Liu⁴⁵, M. Liu³³b, Y. Liu³³b,
M. Livan¹²⁰a,¹²⁰b, S.S.A. Livermore¹¹⁹, A. Lleres⁵⁵, J. Llorente Merino⁸¹, S.L. Lloyd⁷⁵, F. Lo Sterzo¹⁵²,
E. Lobodzinska⁴², P. Loch⁷, W.S. Lockman¹³⁸, T. Loddenkoetter²¹, F.K. Loebinger⁸³, A.E. Loevschall-Jensen³⁶,
A. Loginov¹⁷⁷, C.W. Loh¹⁶⁹, T. Lohse¹⁶, K. Lohwasser⁴², M. Lokajicek¹²⁶, V.P. Lombardo⁵, B.A. Long²²,
J.D. Long⁸⁸, R.E. Long⁷¹, L. Lopes¹²⁵a, D. Lopez Mateos⁵⁷, B. Lopez Paredes¹⁴⁰, I. Lopez Paz¹², J. Lorenz⁹⁹,
N. Lorenzo Martinez⁶⁰, M. Losada¹⁶³, P. Loscutoff¹⁵, X. Lou⁴¹, A. Lounis¹¹⁶, J. Love⁶, P.A. Love⁷¹, A.J. Lowe¹⁴⁴, e, F. Lu³³a, H.J. Lubatti¹³⁹, C. Luci¹³³a, ¹³³b, A. Lucotte⁵⁵, F. Luehring⁶⁰, W. Lukas⁶¹, L. Luminari¹³³a, O. Lundberg¹⁴⁷a, ¹⁴⁷b, B. Lund-Jensen¹⁴⁸, M. Lungwitz⁸², D. Lynn²⁵, R. Lysak¹²⁶, E. Lytken⁸⁰, H. Ma²⁵, L.L. Ma³³d, G. Maccarrone⁴⁷, A. Macchiolo¹⁰⁰, J. Machado Miguens¹²⁵a, ¹²⁵b, D. Macina³⁰, D. Madaffari⁸⁴, R. Madar⁴⁸, H.J. Maddocks⁷¹, W.F. Mader⁴⁴, A. Madsen¹⁶⁷, M. Maeno⁸, T. Maeno²⁵, E. Magradze⁵⁴, K. Mahboubi⁴⁸, J. Mahlstedt¹⁰⁶, S. Mahmoud⁷³, C. Maiani¹³⁷, C. Maidantchik²⁴a, A.A. Maier¹⁰⁰, A. Maio¹²⁵a, ¹²⁵b, ¹²⁵d, S. Majewski¹¹⁵, Y. Makida⁶⁵, N. Makovec¹¹⁶, P. Mal¹³⁷, y, B. Malaescu⁷⁹, Pa. Malecki³⁹, V.P. Maleev¹²², F. Malek⁵⁵, U. Mallik⁶², D. Malon⁶, C. Malone¹⁴⁴, S. Maltezos¹⁰, V.M. Malyshev¹⁰⁸, S. Malyukov³⁰, J. Mamuzic¹³b, B. Mandelli³⁰, L. Mandelli⁹⁰a, I. Mandić⁷⁴, R. Mandrysch⁶², J. Maneira¹²⁵a, ¹²⁵b, A. Manfredini¹⁰⁰, L. Manhaes de Andrade Filho²⁴b, J.A. Manjarres Ramos¹⁶⁰b, A. Mann⁹⁹, P.M. Manning¹³⁸, A. Manousakis-Katsikakis⁹, B. Mansoulie¹³⁷, R. Mantifel⁸⁶, L. Mapelli³⁰, L. March¹⁶⁸, J.F. Marchand²⁹, G. Marchiori⁷⁹, M. Marcisovsky¹²⁶, C.P. Marino¹⁷⁰, M. Marjanovic¹³a, C.N. Marques¹²⁵a, F. Marroquim²⁴a, S.P. Marsden⁸³, Z. Marshall¹⁵, L.F. Marti¹⁷, S. Marti-Garcia¹⁶⁸, B. Martin³⁰, B. Martin⁸⁹, T.A. Martin¹⁷¹, V.J. Martin⁴⁶, B. Martin dit Latour¹⁴, H. Martinez¹³⁷, M. Martinez¹², n, S. Martin-Haugh¹³⁰, A.C. Martyniuk⁷⁷, M. Marx¹³⁹, F. Marzano¹³³a, A. Marzin³⁰, L. Masetti⁸², T. Mashimo¹⁵⁶, R. Mashinistov⁹⁵, J. Masik⁸³, A.L. Maslennikov¹⁰⁸, I. Massa²⁰a, ²⁰b, N. Massol⁵, P. Mastrandrea¹⁴⁹, A. Mastroberardino³⁷a, ³⁷b, T. Masubuchi¹⁵⁶, P. Mättig¹⁷⁶, J. Mattmann⁸², J. Maurer²⁶a, S.J. Maxfield⁷³, D.A. Maximov¹⁰⁸, t, R. Mazini¹⁵², L. Mazzaferro¹³⁴a, ¹³⁴b, G. Mc Goldrick¹⁵⁹, S.P. Mc Kee⁸⁸, A. McCarn⁸⁸, R.L. McCarthy¹⁴⁹, T.G. McCarthy²⁹, N.A. McCubbin¹³⁰, K.W. McFarlane⁵⁶, *, J.A. Mcfayden⁷⁷, G. Mchedlidze⁵⁴, S.J. McMahon¹³⁰, R.A. McPherson¹⁷⁰, i, A. Meade⁸⁵, J. Mechnich¹⁰⁶, M. Medinnis⁴², S. Meehan³¹, S. Mehlhase⁹⁹, A. Mehta⁷³, K. Meier⁵⁸a, C. Meineck⁹⁹, B. Meirose⁸⁰, C. Melachrinos³¹, B.R. Mellado Garcia¹⁴⁶c, F. Meloni¹⁷, A. Mengarelli²⁰a, ²⁰b, S. Menke¹⁰⁰, E. Meoni¹⁶², K.M. Mercurio⁵⁷, S. Mergelmeyer²¹, N. Meric¹³⁷, P. Mermod⁴⁹, L. Merola¹⁰³a, ¹⁰³b, C. Meroni⁹⁰a, F.S. Merritt³¹, H. Merritt¹¹⁰, A. Messina³⁰, z, J. Metcalfe²⁵, A.S. Mete¹⁶⁴, C. Meyer⁸², C. Meyer³¹, J-P. Meyer¹³⁷, J. Meyer³⁰, R.P. Middleton¹³⁰, S. Migas⁷³, L. Mijović²¹, G. Mikenberg¹⁷³, M. Mikestikova¹²⁶, M. Mikuz⁷⁴, A. Milic³⁰, D.W. Miller³¹, C. Mills⁴⁶, A. Milov¹⁷³, D.A. Milstead¹⁴⁷a, ¹⁴⁷b, D. Milstein¹⁷³, A.A. Minaenko¹²⁹, I.A. Minashvili⁶⁴, A.I. Mincer¹⁰⁹, B. Mindur³⁸a, M. Mineev⁶⁴, Y. Ming¹⁷⁴, L.M. Mir¹², G. Mirabelli¹³³a, T. Mitani¹⁷², J. Mitrevski⁹⁹, V.A. Mitsou¹⁶⁸, S. Mitsui⁶⁵, A. Miucci⁴⁹, P.S. Miyagawa¹⁴⁰, J.U. Mjörnmark⁸⁰, T. Moa¹⁴⁷a, ¹⁴⁷b, K. Mochizuki⁸⁴, S. Mohapatra³⁵, W. Mohr⁴⁸, S. Molander¹⁴⁷a, ¹⁴⁷b, R. Moles-Valls¹⁶⁸, K. Mönig⁴², C. Monini⁵⁵, J. Monk³⁶, E. Monnier⁸⁴, J. Montejo Berlingen¹², F. Monticelli⁷⁰, S. Monzani¹³³a, ¹³³b, R.W. Moore³, A. Moraes⁵³, N. Morange⁶², D. Moreno⁸², M. Moreno Llácer⁵⁴, P. Morettini⁵⁰a, M. Morgenstern⁴⁴, M. Morii⁵⁷, S. Moritz⁸², A.K. Morley¹⁴⁸, G. Mornacchi³⁰, J.D. Morris⁷⁵, L. Morvaj¹⁰², H.G. Moser¹⁰⁰, M. Mosidze⁵¹b, J. Moss¹¹⁰, K. Motohashi¹⁵⁸, R. Mount¹⁴⁴, E. Mountricha²⁵, S.V. Mouraviev⁹⁵, *, E.J.W. Moyse⁸⁵, S. Muanza⁸⁴, R.D. Mudd¹⁸, F. Mueller⁵⁸a, J. Mueller¹²⁴, K. Mueller²¹, T. Mueller²⁸, T. Mueller⁸², D. Muenstermann⁴⁹, Y. Munwes¹⁵⁴, J.A. Murillo Quijada¹⁸, W.J. Murray¹⁷¹, ¹³⁰, H. Musheghyan⁵⁴, E. Musto¹⁵³, A.G. Myagkov¹²⁹, aa, M. Myska¹²⁷, O. Nackenhorst⁵⁴, J. Nadal⁵⁴, K. Nagai⁶¹, R. Nagai¹⁵⁸, Y. Nagai⁸⁴, K. Nagano⁶⁵, A. Nagarkar¹¹⁰, Y. Nagasaka⁵⁹, M. Nagel¹⁰⁰, A.M. Nairz³⁰, Y. Nakahama³⁰, K. Nakamura⁶⁵, T. Nakamura¹⁵⁶, I. Nakano¹¹¹, H. Namasivayam⁴¹, G. Nanava²¹, R. Narayan⁵⁸b, T. Nattermann²¹, T. Naumann⁴², G. Navarro¹⁶³, R. Nayyar⁷, H.A. Neal⁸⁸, P.Yu. Nechaeva⁹⁵, T.J. Neep⁸³, P.D. Nef¹⁴⁴, A. Negri¹²⁰a, ¹²⁰b, G. Negri³⁰, M. Negrini²⁰a, S. Nektarijevic⁴⁹, A. Nelson¹⁶⁴, T.K. Nelson¹⁴⁴, S. Nemecek¹²⁶, P. Nemethy¹⁰⁹, A.A. Nepomuceno²⁴a, M. Nessi³⁰, ab, M.S. Neubauer¹⁶⁶, M. Neumann¹⁷⁶, R.M. Neves¹⁰⁹, P. Nevski²⁵, P.R. Newman¹⁸, D.H. Nguyen⁶, R.B. Nickerson¹¹⁹, R. Nicolaidou¹³⁷, B. Nicquevert³⁰, J. Nielsen¹³⁸, N. Nikiforou³⁵, A. Nikiforov¹⁶, V. Nikolaenko¹²⁹, aa, I. Nikolic-Audit⁷⁹, K. Nikolics⁴⁹, K. Nikolopoulos¹⁸, P. Nilsson⁸, Y. Ninomiya¹⁵⁶, A. Nisati¹³³a, R. Nisius¹⁰⁰, T. Nobe¹⁵⁸, L. Nodulman⁶, M. Nomachi¹¹⁷, I. Nomidis¹⁵⁵, S. Norberg¹¹², M. Nordberg³⁰, O. Novgorodova⁴⁴, S. Nowak¹⁰⁰, M. Nozaki⁶⁵, L. Nozka¹¹⁴, K. Ntekas¹⁰, G. Nunes Hanninger⁸⁷, T. Nunnemann⁹⁹, E. Nurse⁷⁷, F. Nuti⁸⁷, B.J. O’Brien⁴⁶, F. O’grady⁷, D.C. O’Neil¹⁴³, V. O’Shea⁵³, F.G. Oakham²⁹, d, H. Oberlack¹⁰⁰, T. Obermann²¹, J. Ocariz⁷⁹, A. Ochi⁶⁶, M.I. Ochoa⁷⁷, S. Oda⁶⁹, S. Odaka⁶⁵, H. Ogren⁶⁰, A. Oh⁸³, S.H. Oh⁴⁵, C.C. Ohm³⁰, H. Ohman¹⁶⁷, T. Ohshima¹⁰², W. Okamura¹¹⁷, H. Okawa²⁵, Y. Okumura³¹, T. Okuyama¹⁵⁶, A. Olariu²⁶a, A.G. Olchevski⁶⁴, S.A. Olivares Pino⁴⁶, D. Oliveira Damazio²⁵, E. Oliver Garcia¹⁶⁸, A. Olszewski³⁹, J. Olszowska³⁹, A. Onofre¹²⁵a, ¹²⁵e, P.U.E. Onyisi³¹, o, C.J. Oram¹⁶⁰a, M.J. Oreglia³¹, Y. Oren¹⁵⁴, D. Orestano¹³⁵a, ¹³⁵b, N. Orlando⁷²a, ⁷²b, C. Oropeza Barrera⁵³, R.S. Orr¹⁵⁹, B. Osculati⁵⁰a, ⁵⁰b, R. Ospanov¹²¹, G. Otero y Garzon²⁷, H. Otono⁶⁹, M. Ouchrif¹³⁶d, E.A. Ouellette¹⁷⁰, F. Ould-Saada¹¹⁸, A. Ouraou¹³⁷, K.P. Oussoren¹⁰⁶, Q. Ouyang³³a, A. Ovcharova¹⁵, M. Owen⁸³, V.E. Ozcan¹⁹a, N. Ozturk⁸, K. Pachal¹¹⁹, A. Pacheco Pages¹², C. Padilla Aranda¹², M. Pagáčová⁴⁸, S. Pagan Griso¹⁵, E. Paganis¹⁴⁰, C. Pahl¹⁰⁰, F. Paige²⁵, P. Pais⁸⁵, K. Pajchel¹¹⁸, G. Palacino¹⁶⁰b, S. Palestini³⁰, M. Palka³⁸b, D. Pallin³⁴, A. Palma¹²⁵a, ¹²⁵b, J.D. Palmer¹⁸, Y.B. Pan¹⁷⁴, E. Panagiotopoulou¹⁰, J.G. Panduro Vazquez⁷⁶, P. Pani¹⁰⁶, N. Panikashvili⁸⁸, S. Panitkin²⁵, D. Pantea²⁶a, L. Paolozzi¹³⁴a, ¹³⁴b, Th.D. Papadopoulou¹⁰, K. Papageorgiou¹⁵⁵, l,
A. Paramonov⁶, D. Paredes Hernandez³⁴, M.A. Parker²⁸, F. Parodi⁵⁰a,⁵⁰b, J.A. Parsons³⁵, U. Parzefall⁴⁸,
E. Pasqualucci¹³³a, S. Passaggio⁵⁰a, A. Passeri¹³⁵a, F. Pastore¹³⁵a,¹³⁵b,*, Fr. Pastore⁷⁶, G. Pásztor²⁹, S. Pataraia¹⁷⁶,
N.D. Patel¹⁵¹, J.R. Pater⁸³, S. Patricelli¹⁰³a,¹⁰³b, T. Pauly³⁰, J. Pearce¹⁷⁰, M. Pedersen¹¹⁸, S. Pedraza Lopez¹⁶⁸,
R. Pedro¹²⁵a,¹²⁵b, S.V. Peleganchuk¹⁰⁸, D. Pelikan¹⁶⁷, H. Peng³³b, B. Penning³¹, J. Penwell⁶⁰, D.V. Perepelitsa²⁵,
E. Perez Codina¹⁶⁰a, M.T. Pérez García-Estaná¹⁶⁸, V. Perez Reale³⁵, L. Perini⁹⁰a,⁹⁰b, H. Pernegger³⁰, R. Perrino⁷²a,
R. Peschke⁴², V.D. Peshekhonov⁶⁴, K. Peters³⁰, R.F.Y. Peters⁸³, B.A. Petersen³⁰, T.C. Petersen³⁶, E. Petit⁴²,
A. Petridis¹⁴⁷a,¹⁴⁷b, C. Petridou¹⁵⁵, E. Petrolo¹³³a, F. Petrucci¹³⁵a,¹³⁵b, N.E. Pettersson¹⁵⁸, R. Pezoa³²b,
P.W. Phillips¹³⁰, G. Piacquadio¹⁴⁴, E. Pianori¹⁷¹, A. Picazio⁴⁹, E. Piccaro⁷⁵, M. Piccinini²⁰²a,²⁰b, R. Piegaia²⁷,
D.T. Pignotti¹¹⁰, J.E. Pilcher³¹, A.D. Pilkington⁷⁷, J. Pina¹²⁵a,¹²⁵b,¹²⁵d, M. Pinamonti¹⁶⁵a,¹⁶⁵c,ac, A. Pinder¹¹⁹,
J.L. Pinfold³, A. Pingel³⁶, B. Pinto¹²⁵a, S. Pires⁷⁹, M. Pitt¹⁷³, C. Pizio⁹⁰a,⁹⁰b, L. Plazak¹⁴⁵a, M.-A. Pleier²⁵,
V. Pleskot¹²⁸, E. Plotnikova⁶⁴, P. Plucinski¹⁴⁷a,¹⁴⁷b, S. Poddar⁵⁸a, F. Podlyski³⁴, R. Poettgen⁸², L. Poggioli¹¹⁶,
D. Pohl²¹, M. Pohl⁴⁹, G. Polesello¹²⁰a, A. Policicchio³⁷a,³⁷b, R. Polifka¹⁵⁹, A. Polini²⁰a, C.S. Pollard⁴⁵,
V. Polychronakos²⁵, K. Pommès³⁰, L. Pontecorvo¹³³a, B.G. Pope⁸⁹, G.A. Popeneciu²⁶b, D.S. Popovic¹³a,
A. Poppleton³⁰, X. Portell Bueso¹², S. Pospisil¹²⁷, K. Potamianos¹⁵, I.N. Potrap⁶⁴, C.J. Potter¹⁵⁰, C.T. Potter¹¹⁵,
G. Poulard³⁰, J. Poveda⁶⁰, V. Pozdnyakov⁶⁴, P. Pralavorio⁸⁴, A. Pranko¹⁵, S. Prasad³⁰, R. Pravahan⁸, S. Prell⁶³,
D. Price⁸³, J. Price⁷³, L.E. Price⁶, D. Prieur¹²⁴, M. Primavera⁷²a, M. Proissl¹⁴⁶, K. Prokofiev⁴⁷, F. Prokoshin³²b,
E. Protopapadaki¹³⁷, S. Protopopescu²⁵, J. Proudfoot⁶, M. Przybycien³⁸a, H. Przysiezniak⁵, E. Ptacek¹¹⁵,
D. Puddu¹³⁵a,¹³⁵b, E. Pueschel⁸⁵, D. Puldon¹⁴⁹, M. Purohit²⁵,ad, P. Puzo¹¹⁶, J. Qian⁸⁸, G. Qin⁵³, Y. Qin⁸³,
A. Quadt⁵⁴, D.R. Quarrie¹⁵, W.B. Quayle¹⁶⁵a,¹⁶⁵b, M. Queitsch-Maitland⁸³, D. Quilty⁵³, A. Qureshi¹⁶⁰b,
V. Radeka²⁵, V. Radescu⁴², S.K. Radhakrishnan¹⁴⁹, P. Radloff¹¹⁵, P. Rados⁸⁷, F. Ragusa⁹⁰a,⁹⁰b, G. Rahal¹⁷⁹,
S. Rajagopalan²⁵, M. Rammensee³⁰, A.S. Randle-Conde⁴⁰, C. Rangel-Smith¹⁶⁷, K. Rao¹⁶⁴, F. Rauscher⁹⁹,
T.C. Rave⁴⁸, T. Ravenscroft⁵³, M. Raymond³⁰, A.L. Read¹¹⁸, N.P. Readioff⁷³, D.M. Rebuzzi¹²⁰a,¹²⁰b,
A. Redelbach¹⁷⁵, G. Redlinger²⁵, R. Reece¹³⁸, K. Reeves⁴¹, L. Rehnisch¹⁶, H. Reisin²⁷, M. Relich¹⁶⁴, C. Rembser³⁰,
H. Ren³³a, Z.L. Ren¹⁵², A. Renaud¹¹⁶, M. Rescigno¹³³a, S. Resconi⁹⁰a, O.L. Rezanova¹⁰⁸,t, P. Reznicek¹²⁸,
R. Rezvani⁹⁴, R. Richter¹⁰⁰, M. Ridel⁷⁹, P. Rieck¹⁶, J. Rieger⁵⁴, M. Rijssenbeek¹⁴⁹, A. Rimoldi¹²⁰a,¹²⁰b,
L. Rinaldi²⁰a, E. Ritsch⁶¹, I. Riu¹², F. Rizatdinova¹¹³, E. Rizvi⁷⁵, S.H. Robertson⁸⁶,i, A. Robichaud-Veronneau⁸⁶,
D. Robinson²⁸, J.E.M. Robinson⁸³, A. Robson⁵³, C. Roda¹²³a,¹²³b, L. Rodrigues³⁰, S. Roe³⁰, O. Røhne¹¹⁸,
S. Rolli¹⁶², A. Romaniouk⁹⁷, M. Romano²⁰a,²⁰b, E. Romero Adam¹⁶⁸, N. Rompotis¹³⁹, L. Roos⁷⁹, E. Ros¹⁶⁸,
S. Rosati¹³³a, K. Rosbach⁴⁹, M. Rose⁷⁶, P.L. Rosendahl¹⁴, O. Rosenthal¹⁴², V. Rossetti¹⁴⁷a,¹⁴⁷b, E. Rossi¹⁰³a,¹⁰³b,
L.P. Rossi⁵⁰a, R. Rosten¹³⁹, M. Rotaru²⁶a, I. Roth¹⁷³, J. Rothberg¹³⁹, D. Rousseau¹¹⁶, C.R. Royon¹³⁷,
A. Rozanov⁸⁴, Y. Rozen¹⁵³, X. Ruan¹⁴⁶c, F. Rubbo¹², I. Rubinskiy⁴², V.I. Rud⁹⁸, C. Rudolph⁴⁴, M.S. Rudolph¹⁵⁹,
F. Rühr⁴⁸, A. Ruiz-Martinez³⁰, Z. Rurikova⁴⁸, N.A. Rusakovitch⁶⁴, A. Ruschke⁹⁹, J.P. Rutherfoord⁷,
N. Ruthmann⁴⁸, Y.F. Ryabov¹²², M. Rybar¹²⁸, G. Rybkin¹¹⁶, N.C. Ryder¹¹⁹, A.F. Saavedra¹⁵¹, S. Sacerdoti²⁷,
A. Saddique³, I. Sadeh¹⁵⁴, H.F.-W. Sadrozinski¹³⁸, R. Sadykov⁶⁴, F. Safai Tehrani¹³³a, H. Sakamoto¹⁵⁶,
Y. Sakurai¹⁷², G. Salamanna¹³⁵a,¹³⁵b, A. Salamon¹³⁴a, M. Saleem¹¹², D. Salek¹⁰⁶, P.H. Sales De Bruin¹³⁹,
D. Salihagic¹⁰⁰, A. Salnikov¹⁴⁴, J. Salt¹⁶⁸, B.M. Salvachua Ferrando⁶, D. Salvatore³⁷a,³⁷b, F. Salvatore¹⁵⁰,
A. Salvucci¹⁰⁵, A. Salzburger³⁰, D. Sampsonidis¹⁵⁵, A. Sanchez¹⁰³a,¹⁰³b, J. Sánchez¹⁶⁸, V. Sanchez Martinez¹⁶⁸,
H. Sandaker¹⁴, R.L. Sandbach⁷⁵, H.G. Sander⁸², M.P. Sanders⁹⁹, M. Sandhoff¹⁷⁶, T. Sandoval²⁸, C. Sandoval¹⁶³,
R. Sandstroem¹⁰⁰, D.P.C. Sankey¹³⁰, A. Sansoni⁴⁷, C. Santoni³⁴, R. Santonico¹³⁴a,¹³⁴b, H. Santos¹²⁵a,
I. Santoyo Castillo¹⁵⁰, K. Sapp¹²⁴, A. Sapronov⁶⁴, J.G. Saraiva¹²⁵a,¹²⁵d, B. Sarrazin²¹, G. Sartisohn¹⁷⁶, O. Sasaki⁶⁵,
Y. Sasaki¹⁵⁶, G. Sauvage⁵,*, E. Sauvan⁵, P. Savard¹⁵⁹,d, D.O. Savu³⁰, C. Sawyer¹¹⁹, L. Sawyer⁷⁸,m, D.H. Saxon⁵³,
J. Saxon¹²¹, C. Sbarra²⁰a, A. Sbrizzi³, T. Scanlon⁷⁷, D.A. Scannicchio¹⁶⁴, M. Scarcella¹⁵¹, V. Scarfone³⁷a,³⁷b,
J. Schaarschmidt¹⁷³, P. Schacht¹⁰⁰, D. Schaefer¹²¹, R. Schaefer⁴², S. Schaepe²¹, S. Schaetzel⁵⁸b, U. Schäfer⁸²,
A.C. Schaffer¹¹⁶, D. Schaile⁹⁹, R.D. Schamberger¹⁴⁹, V. Scharf⁵⁸a, V.A. Schegelsky¹²², D. Scheirich¹²⁸,
M. Schernau¹⁶⁴, M.I. Scherzer³⁵, C. Schiavi⁵⁰a,⁵⁰b, J. Schieck⁹⁹, C. Schillo⁴⁸, M. Schioppa³⁷a,³⁷b, S. Schlenker³⁰,
E. Schmidt⁴⁸, K. Schmieden³⁰, C. Schmitt⁸², S. Schmitt⁵⁸b, B. Schneider¹⁷, Y.J. Schnellbach⁷³, U. Schnoor⁴⁴,
L. Schoeffel¹³⁷, A. Schoening⁵⁸b, B.D. Schoenrock⁸⁹, A.L.S. Schorlemmer⁵⁴, M. Schott⁸², D. Schouten¹⁶⁰a,
J. Schovancova²⁵, S. Schramm¹⁵⁹, M. Schreyer¹⁷⁵, C. Schroeder⁸², N. Schuh⁸², M.J. Schultens²¹,
H.-C. Schultz-Coulon⁵⁸a, H. Schulz¹⁶, M. Schumacher⁴⁸, B.A. Schumm¹³⁸, Ph. Schune¹³⁷, C. Schwanenberger⁸³,
A. Schwartzman¹⁴⁴, Ph. Schwegler¹⁰⁰, Ph. Schwemling¹³⁷, R. Schwienhorst⁸⁹, J. Schwindling¹³⁷, T. Schwindt²¹,
M. Schwoerer⁵, F.G. Sciacca¹⁷, E. Scifo¹¹⁶, G. Sciolla²³, W.G. Scott¹³⁰, F. Scuri¹²³a,¹²³b, F. Scutti²¹, J. Searcy⁸⁸,
G. Sedov⁴², E. Sedykh¹²², S.C. Seidel¹⁰⁴, A. Seiden¹³⁸, F. Seifert¹²⁷, J.M. Seixas²⁴a, G. Sekhniaidze¹⁰³a,
S.J. Sekula⁴⁰, K.E. Selbach⁴⁶, D.M. Seliverstov¹²²,*, G. Sellers⁷³, N. Semprini-Cesari²⁰a,²⁰b, C. Serfon³⁰, L. Serin¹¹⁶,
L. Serkin⁵⁴, T. Serre⁸⁴, R. Seuster¹⁶⁰a, H. Severini¹¹², T. Sfíligoj⁷⁴, F. Sforza¹⁰⁰, A. Sfyrla³⁰, E. Shabalina⁵⁴,
M. Shamim¹¹⁵, L.Y. Shan³³a, R. Shang¹⁶⁶, J.T. Shank²², M. Shapiro¹⁵, P.B. Shatalov⁹⁶, K. Shaw¹⁶⁵a,¹⁶⁵b,
C.Y. Shehu¹⁵⁰, P. Sherwood⁷⁷, L. Shi¹⁵²,ae, S. Shimizu⁶⁶, C.O. Shimmin¹⁶⁴, M. Shimojima¹⁰¹, M. Shiyakova⁶⁴,
A. Shmeleva⁹⁵, M.J. Shochet³¹, D. Short¹¹⁹, S. Shrestha⁶³, E. Shulga⁹⁷, M.A. Shupe⁷, S. Shushkevich⁴², P. Sicho¹²⁶, O. Sidiropoulou¹⁵⁵, D. Sidorov¹¹³, A. Sidoti¹³³a, F. Siegert⁴⁴, Dj. Sijacki¹³a, J. Silva¹²⁵a,¹²⁵d, Y. Silver¹⁵⁴, D. Silverstein¹⁴⁴, S.B. Silverstein¹⁴⁷a, V. Simak¹²⁷, O. Simard⁵, Lj. Simic¹³a, S. Simion¹¹⁶, E. Simioni⁸², B. Simmons⁷⁷, R. Simoniello⁹⁰a,⁹⁰b, M. Simonyan³⁶, P. Sinervo¹⁵⁹, N.B. Sinev¹¹⁵, V. Sipica¹⁴², G. Siragusa¹⁷⁵, A. Sircar⁷⁸, A.N. Sisakyan⁶⁴,*, S.Yu. Sivoklokov⁹⁸, J. Sjölin¹⁴⁷a,¹⁴⁷b, T.B. Sjursen¹⁴, H.P. Skottowe⁵⁷, K.Yu. Skovpen¹⁰⁸, P. Skubic¹¹², M. Slater¹⁸, T. Slavicek¹²⁷, K. Sliwa¹⁶², V. Smakhtin¹⁷³, B.H. Smart⁴⁶, L. Smestad¹⁴, S.Yu. Smirnov⁹⁷, Y. Smirnov⁹⁷, L.N. Smirnova⁹⁸,af, O. Smirnova⁸⁰, K.M. Smith⁵³, M. Smizanska⁷¹, K. Smolek¹²⁷, A.A. Snesarev⁹⁵, G. Snidero⁷⁵, S. Snyder²⁵, R. Sobie¹⁷⁰, i, F. Socher⁴⁴, A. Soffer¹⁵⁴, D.A. Soh¹⁵²,ae, C.A. Solans³⁰, M. Solar¹²⁷, J. Solc¹²⁷, E.Yu. Soldatov⁹⁷, U. Soldevila¹⁶⁸, E. Solfaroli Camillocci¹³³a,¹³³b, A.A. Solodkov¹²⁹, A. Soloshenko⁶⁴, O.V. Solovyevon¹²⁹, V. Solovyev¹²², P. Sommer⁴⁸, H.Y. Song³³b, N. Soni¹, A. Sood¹⁵, A. Sopczak¹²⁷, B. Sopko¹²⁷, V. Sopko¹²⁷, V. Sorin¹², M. Sosebee⁸, R. Soualah¹⁶⁵a,¹⁶⁵c, P. Soueid⁹⁴, A.M. Soukharev¹⁰⁸, D. South⁴², S. Spagnolo⁷²a,⁷²b, F. Spanò⁷⁶, W.R. Spearman⁵⁷, F. Spettel¹⁰⁰, R. Spighi²⁰a, G. Spigo³⁰, L.A. Spiller⁸⁷, M. Spousta¹²⁸, T. Spreitzer¹⁵⁹, B. Spurlock⁸, R.D. St. Denis⁵³,*, S. Staerz⁴⁴, J. Stahlman¹²¹, R. Stamen⁵⁸a, E. Stanecka³⁹, R.W. Stanek⁶, C. Stanescu¹³⁵a, M. Stanescu-Bellu⁴², M.M. Stanitzki⁴², S. Stapnes¹¹⁸, E.A. Starchenko¹²⁹, J. Stark⁵⁵, P. Staroba¹²⁶, P. Starovoitov⁴², R. Staszewski³⁹, P. Stavina¹⁴⁵a,*, P. Steinberg²⁵, B. Stelzer¹⁴³, H.J. Stelzer³⁰, O. Stelzer-Chilton¹⁶⁰a, H. Stenzel⁵², S. Stern¹⁰⁰, G.A. Stewart⁵³, J.A. Stillings²¹, M.C. Stockton⁸⁶, M. Stoebe⁸⁶, G. Stoicea²⁶a, P. Stolte⁵⁴, S. Stonjek¹⁰⁰, A.R. Stradling⁸, A. Straessner⁴⁴, M.E. Stramaglia¹⁷, J. Strandberg¹⁴⁸, S. Strandberg¹⁴⁷a,¹⁴⁷b, A. Strandlie¹¹⁸, E. Strauss¹⁴⁴, M. Strauss¹¹², P. Strizenec¹⁴⁵b, R. Ströhmer¹⁷⁵, D.M. Strom¹¹⁵, R. Stroynowski⁴⁰, S.A. Stucci¹⁷, B. Stugu¹⁴, N.A. Styles⁴², D. Su¹⁴⁴, J. Su¹²⁴, HS. Subramania³, R. Subramaniam⁷⁸, A. Succurro¹², Y. Sugaya¹¹⁷, C. Suhr¹⁰⁷, M. Suk¹²⁷, V.V. Sulin⁹⁵, S. Sultansoy⁴c, T. Sumida⁶⁷, X. Sun³³a, J.E. Sundermann⁴⁸, K. Suruliz¹⁴⁰, G. Susinno³⁷a,³⁷b, M.R. Sutton¹⁵⁰, Y. Suzuki⁶⁵, M. Svatos¹²⁶, S. Swedish¹⁶⁹, M. Swiatlowski¹⁴⁴, I. Sykora¹⁴⁵a, T. Sykora¹²⁸, D. Ta⁸⁹, C. Taccini¹³⁵a,¹³⁵b, K. Tackmann⁴², J. Taenzer¹⁵⁹, A. Taffard¹⁶⁴, R. Tafirout¹⁶⁰a, N. Taiblum¹⁵⁴, Y. Takahashi¹⁰², H. Takai²⁵, R. Takashima⁶⁸, H. Takeda⁶⁶, T. Takeshita¹⁴¹, Y. Takubo⁶⁵, M. Talby⁸⁴, A.A. Talyshev¹⁰⁸, t, J.Y.C. Tam¹⁷⁵, K.G. Tan⁸⁷, J. Tanaka¹⁵⁶, R. Tanaka¹¹⁶, S. Tanaka¹³², S. Tanaka⁶⁵, A.J. Tanasijczuk¹⁴³, B.B. Tannenwald¹¹⁰, N. Tannoury²¹, S. Tapprogge⁸², S. Tarem¹⁵³, F. Tarrade²⁹, G.F. Tartarelli⁹⁰a, P. Tas¹²⁸, M. Tasevsky¹²⁶, T. Tashiro⁶⁷, E. Tassi³⁷a,³⁷b, A. Tavares Delgado¹²⁵a,¹²⁵b, Y. Tayalati¹³⁶d, F.E. Taylor⁹³, G.N. Taylor⁸⁷, W. Taylor¹⁶⁰b, F.A. Teischinger³⁰, M. Teixeira Dias Castanheira⁷⁵, P. Teixeira-Dias⁷⁶, K.K. Temming⁴⁸, H. Ten Kate³⁰, P.K. Teng¹⁵², J.J. Teoh¹¹⁷, S. Terada⁶⁵, K. Terashi¹⁵⁶, J. Terron⁸¹, S. Terzo¹⁰⁰, M. Testa⁴⁷, R.J. Teuscher¹⁵⁹, i, J. Therhaag²¹, T. Theveneaux-Pelzer³⁴, J.P. Thomas¹⁸, J. Thomas-Wilsker⁷⁶, E.N. Thompson³⁵, P.D. Thompson¹⁸, P.D. Thompson¹⁵⁹, A.S. Thompson⁵³, L.A. Thomsen³⁶, E. Thomson¹²¹, M. Thomson²⁸, W.M. Thong⁸⁷, R.P. Thun⁸⁸,*, F. Tian³⁵, M.J. Tibbetts¹⁵, V.O. Tikhomirov⁹⁵,ag, Yu.A. Tikhonov¹⁰⁸, t, S. Timoshenko⁹⁷, E. Tiouchichine⁸⁴, P. Tipton¹⁷⁷, S. Tisserant⁸⁴, T. Todorov⁵, S. Todorova-Nova¹²⁸, B. Toggerson⁷, J. Tojo⁶⁹, S. Tokár¹⁴⁵a, K. Tokushuku⁶⁵, K. Tollefson⁸⁹, L. Tomlinson⁸³, M. Tomoto¹⁰², L. Tompkins³¹, K. Toms¹⁰⁴, N.D. Topilin⁶⁴, E. Torrence¹¹⁵, H. Torres¹⁴³, E. Torró Pastor¹⁶⁸, J. Toth⁸⁴,ah, F. Touchard⁸⁴, D.R. Tovey¹⁴⁰, H.L. Tran¹¹⁶, T. Trefzger¹⁷⁵, L. Tremblet³⁰, A. Tricoli³⁰, I.M. Trigger¹⁶⁰a, S. Trincaz-Duvoid⁷⁹, M.F. Tripiana¹², N. Triplett²⁵, W. Trischuk¹⁵⁹, B. Trocmé⁵⁵, C. Troncon⁹⁰a, M. Trottier-McDonald¹⁴³, M. Trovatelli¹³⁵a,¹³⁵b, P. True⁸⁹, M. Trzebinski³⁹, A. Trzupek³⁹, C. Tsarouchas³⁰, J.C.-L. Tseng¹¹⁹, P.V. Tsiareshka⁹¹, D. Tsionou¹³⁷, G. Tsipolitis¹⁰, N. Tsirintanis⁹, S. Tsiskaridze¹², V. Tsiskaridze⁴⁸, E.G. Tskhadadze⁵¹a, I.I. Tsukerman⁹⁶, V. Tsulaia¹⁵, S. Tsuno⁶⁵, D. Tsybychev¹⁴⁹, A. Tudorache²⁶a, V. Tudorache²⁶a, A.N. Tuna¹²¹, S.A. Tupputi²⁰a,²⁰b, S. Turchikhin⁹⁸,af, D. Turecek¹²⁷, I. Turk Cakir⁴d, R. Turra⁹⁰a,⁹⁰b, P.M. Tuts³⁵, A. Tykhonov⁴⁹, M. Tylmad¹⁴⁷a,¹⁴⁷b, M. Tyndel¹³⁰, K. Uchida²¹, I. Ueda¹⁵⁶, R. Ueno²⁹, M. Ughetto⁸⁴, M. Ugland¹⁴, M. Uhlenbrock²¹, F. Ukegawa¹⁶¹, G. Unal³⁰, A. Undrus²⁵, G. Unel¹⁶⁴, F.C. Ungaro⁴⁸, Y. Unno⁶⁵, C. Unverdorben⁹⁹, D. Urbaniec³⁵, P. Urquijo⁸⁷, G. Usai⁸, A. Usanova⁶¹, L. Vacavant⁸⁴, V. Vacek¹²⁷, B. Vachon⁸⁶, N. Valencic¹⁰⁶, S. Valentinetti²⁰a,²⁰b, A. Valero¹⁶⁸, L. Valery³⁴, S. Valkar¹²⁸, E. Valladolid Gallego¹⁶⁸, S. Vallecorsa⁴⁹, J.A. Valls Ferrer¹⁶⁸, W. Van Den Wollenberg¹⁰⁶, P.C. Van Der Deijl¹⁰⁶, R. van der Geer¹⁰⁶, H. van der Graaf¹⁰⁶, R. Van Der Leeuw¹⁰⁶, D. van der Ster³⁰, N. van Eldik³⁰, P. van Gemmeren⁶, J. Van Nieuwkoop¹⁴³, I. van Vulpen¹⁰⁶, M.C. van Woerden³⁰, M. Vanadia¹³³a,¹³³b, W. Vandelli³⁰, R. Vanguri¹²¹, A. Vaniachine⁶, P. Vankov⁴², F. Vannucci⁷⁹, G. Vardanyan¹⁷⁸, R. Vari¹³³a, E.W. Varnes⁷, T. Varol⁸⁵, D. Varouchas⁷⁹, A. Vartapetian⁸, K.E. Varvell¹⁵¹, F. Vazeille³⁴, T. Vazquez Schroeder⁵⁴, J. Veatch⁷, F. Veloso¹²⁵a,¹²⁵c, S. Veneziano¹³³a, A. Ventura⁷²a,⁷²b, D. Ventura⁸⁵, M. Venturi¹⁷⁰, N. Venturi¹⁵⁹, A. Venturini²³, V. Vercesi¹²⁰a, M. Verducci¹³³a,¹³³b, W. Verkerke¹⁰⁶, J.C. Vermeulen¹⁰⁶, A. Vest⁴⁴, M.C. Vetterli¹⁴³, d, O. Viazlo⁸⁰, I. Vichou¹⁶⁶, T. Vickey¹⁴⁶c,ai, O.E. Vickey Boeriu¹⁴⁶c, G.H.A. Viehhauser¹¹⁹, S. Viel¹⁶⁹, R. Vigne³⁰, M. Villa²⁰a,²⁰b, M. Villaplana Perez⁹⁰a,⁹⁰b, E. Vilucchi⁴⁷, M.G. Vincter²⁹, V.B. Vinogradov⁶⁴, J. Virzi¹⁵, I. Vivarelli¹⁵⁰, F. Vives Vaque³, S. Vlachos¹⁰, D. Vladoiu⁹⁹, M. Vlasak¹²⁷, A. Vogel²¹, M. Vogel³²a, P. Vokac¹²⁷, G. Volpi¹²³a,¹²³b, M. Volpi⁸⁷, H. von der Schmitt¹⁰⁰,
H. von Radziewski⁴⁸, E. von Toerne²¹, V. Vorobel¹²⁸, K. Vorobev⁹⁷, M. Vos¹⁶⁸, R. Voss³⁰, J.H. Vossebeld⁷³, N. Vranjes¹³⁷, M. Vranjes Milosavljevic¹⁰⁶, V. Vrba¹²⁶, M. Vreeswijk¹⁰⁶, T. Vu Anh⁴⁸, R. Vuillermet³⁰, I. Vukotic³¹, Z. Vykydal¹²⁷, P. Wagner²¹, W. Wagner¹⁷⁶, H. Wahlberg⁷⁰, S. Wahrmund⁴⁴, J. Wakabayashi¹⁰², J. Walder⁷¹, R. Walker⁹⁹, W. Walkowiak¹⁴², R. Wall¹⁷⁷, P. Waller⁷³, B. Walsh¹⁷⁷, C. Wang¹⁵²,aj, C. Wang⁴⁵, F. Wang¹⁷⁴, H. Wang¹⁵, H. Wang⁴⁰, J. Wang⁴², J. Wang³³a, K. Wang⁸⁶, R. Wang¹⁰⁴, S.M. Wang¹⁵², T. Wang²¹, X. Wang¹⁷⁷, C. Wanotayaroj¹¹⁵, A. Warburton⁸⁶, C.P. Ward²⁸, D.R. Wardrope⁷⁷, M. Warsinsky⁴⁸, A. Washbrook⁴⁶, C. Wasicki⁴², P.M. Watkins¹⁸, A.T. Watson¹⁸, I.J. Watson¹⁵¹, M.F. Watson¹⁸, G. Watts¹³⁹, S. Watts⁸³, B.M. Waugh⁷⁷, S. Webb⁸³, M.S. Weber¹⁷, S.W. Weber¹⁷⁵, J.S. Webster³¹, A.R. Weidberg¹¹⁹, P. Weigell¹⁰⁰, B. Weinert⁶⁰, J. Weingarten⁵⁴, C. Weiser⁴⁸, H. Weits¹⁰⁶, P.S. Wells³⁰, T. Wenaus²⁵, D. Wendland¹⁶, Z. Weng¹⁵²,ae, T. Wengler³⁰, S. Wenig³⁰, N.ermes²¹, M. Werner⁴⁸, P. Werner³⁰, M. Wessels⁵⁸a, J. Wetter¹⁶², K. Whalen²⁹, A. White⁸, M.J. White¹, R. White³²b, S. White¹²³a,¹²³b, D. Whiteson¹⁶⁴, D. Wicke¹⁷⁶, F.J. Wickens¹³⁰, W. Wiedenmann¹⁷⁴, M. Wielers¹³⁰, P. Wienemann²¹, C. Wiglesworth³⁶, L.A.M. Wiik-Fuchs²¹, P.A. Wijeratne⁷⁷, A. Wildauer¹⁰⁰, M.A. Wildt⁴²,ak, H.G. Wilkens³⁰, J.Z. Will⁹⁹, H.H. Williams¹²¹, S. Williams²⁸, C. Willis⁸⁹, S. Willocq⁸⁵, A. Wilson⁸⁸, J.A. Wilson¹⁸, I. Wingerter-Seez⁵, F. Winklmeier¹¹⁵, B.T. Winter²¹, M. Wittgen¹⁴⁴, T. Wittig⁴³, J. Wittkowski⁹⁹, S.J. Wollstadt⁸², M.W. Wolter³⁹, H. Wolters¹²⁵a,¹²⁵c, B.K. Wosiek³⁹, J. Wotschack³⁰, M.J. Woudstra⁸³, K.W. Wozniak³⁹, M. Wright⁵³, M. Wu⁵⁵, S.L. Wu¹⁷⁴, X. Wu⁴⁹, Y. Wu⁸⁸, E. Wulf³⁵, T.R. Wyatt⁸³, B.M. Wynne⁴⁶, S. Xella³⁶, M. Xiao¹³⁷, D. Xu³³a, L. Xu³³b,al, B. Yabsley¹⁵¹, S. Yacoob¹⁴⁶b,am, M. Yamada⁶⁵, H. Yamaguchi¹⁵⁶, Y. Yamaguchi¹¹⁷, A. Yamamoto⁶⁵, K. Yamamoto⁶³, S. Yamamoto¹⁵⁶, T. Yamamura¹⁵⁶, T. Yamanaka¹⁵⁶, K. Yamauchi¹⁰², Y. Yamazaki⁶⁶, Z. Yan²², H. Yang³³e, H. Yang¹⁷⁴, U.K. Yang⁸³, Y. Yang¹¹⁰, S. Yanush⁹², L. Yao³³a, W-M. Yao¹⁵, Y. Yasu⁶⁵, E. Yatsenko⁴², K.H. Yau Wong²¹, J. Ye⁴⁰, S. Ye²⁵, A.L. Yen⁵⁷, E. Yildirim⁴², M. Yilmaz⁴b, R. Yoosoofmiya¹²⁴, K. Yorita¹⁷², R. Yoshida⁶, K. Yoshihara¹⁵⁶, C. Young¹⁴⁴, C.J.S. Young³⁰, S. Youssef²², D.R. Yu¹⁵, J. Yu⁸, J.M. Yu⁸⁸, J. Yu¹¹³, L. Yuan⁶⁶, A. Yurkewicz¹⁰⁷, I. Yusuff²⁸,an, B. Zabinski³⁹, R. Zaidan⁶², A.M. Zaitsev¹²⁹,aa, A. Zaman¹⁴⁹, S. Zambito²³, L. Zanello¹³³a,¹³³b, D. Zanzi¹⁰⁰, C. Zeitnitz¹⁷⁶, M. Zeman¹²⁷, A. Zemla³⁸a, K. Zengel²³, O. Zenin¹²⁹, T. Ženiš¹⁴⁵a, D. Zerwas¹¹⁶, G. Zevi della Porta⁵⁷, D. Zhang⁸⁸, F. Zhang¹⁷⁴, H. Zhang⁸⁹, J. Zhang⁶, L. Zhang¹⁵², X. Zhang³³d, Z. Zhang¹¹⁶, Z. Zhao³³b, A. Zhemchugov⁶⁴, J. Zhong¹¹⁹, B. Zhou⁸⁸, L. Zhou³⁵, N. Zhou¹⁶⁴, C.G. Zhu³³d, H. Zhu³³a, J. Zhu⁸⁸, Y. Zhu³³b, X. Zhuang³³a, K. Zhukov⁹⁵, A. Zibell¹⁷⁵, D. Zieminska⁶⁰, N.I. Zimine⁶⁴, C. Zimmermann⁸², R. Zimmermann²¹, S. Zimmermann²¹, S. Zimmermann⁴⁸, Z. Zinonos⁵⁴, M. Ziolkowski¹⁴², G. Zobernig¹⁷⁴, A. Zoccoli²⁰a,²⁰b, M. zur Nedden¹⁶, G. Zurzolo¹⁰³a,¹⁰³b, V. Zutshi¹⁰⁷, L. Zwalinski³⁰.

¹ Department of Physics, University of Adelaide, Adelaide, Australia

² Physics Department, SUNY Albany, Albany NY, United States of America

³ Department of Physics, University of Alberta, Edmonton AB, Canada

⁴ (a) Department of Physics, Ankara University, Ankara; (b) Department of Physics, Gazi University, Ankara; (c) Division of Physics, TOBB University of Economics and Technology, Ankara; (d) Turkish Atomic Energy Authority, Ankara, Turkey

⁵ LAPP, CNRS/IN2P3 and Université de Savoie, Annecy-le-Vieux, France

⁶ High Energy Physics Division, Argonne National Laboratory, Argonne IL, United States of America

⁷ Department of Physics, University of Arizona, Tucson AZ, United States of America

⁸ Department of Physics, The University of Texas at Arlington, Arlington TX, United States of America

⁹ Physics Department, University of Athens, Athens, Greece

¹⁰ Physics Department, National Technical University of Athens, Zografou, Greece

¹¹ Institute of Physics, Azerbaijan Academy of Sciences, Baku, Azerbaijan

¹² Institut de Física d'Altes Energies and Departament de Física de la Universitat Autònoma de Barcelona, Barcelona, Spain

¹³ (a) Institute of Physics, University of Belgrade, Belgrade; (b) Vinca Institute of Nuclear Sciences, University of Belgrade, Belgrade, Serbia

¹⁴ Department for Physics and Technology, University of Bergen, Bergen, Norway

¹⁵ Physics Division, Lawrence Berkeley National Laboratory and University of California, Berkeley CA, United States of America

¹⁶ Department of Physics, Humboldt University, Berlin, Germany

¹⁷ Albert Einstein Center for Fundamental Physics and Laboratory for High Energy Physics, University of Bern, Bern, Switzerland

¹⁸ School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom

¹⁹ (a) Department of Physics, Bogazici University, Istanbul; (b) Department of Physics, Dogus University, Istanbul; (c) Department of Physics Engineering, Gaziantep University, Gaziantep, Turkey
20 (a) INFN Sezione di Bologna; (b) Dipartimento di Fisica e Astronomia, Università di Bologna, Bologna, Italy

21 Physikalisches Institut, University of Bonn, Bonn, Germany

22 Department of Physics, Boston University, Boston MA, United States of America

23 Department of Physics, Brandeis University, Waltham MA, United States of America

24 (a) Universidade Federal do Rio De Janeiro COPPE/EE/IF, Rio de Janeiro; (b) Federal University of Juiz de Fora (UFJF), Juiz de Fora; (c) Federal University of Sao Joao del Rei (UFSJ), Sao Joao del Rei; (d) Instituto de Fisica, Universidade de Sao Paulo, Sao Paulo, Brazil

25 Physics Department, Brookhaven National Laboratory, Upton NY, United States of America

26 (a) National Institute of Physics and Nuclear Engineering, Bucharest; (b) National Institute for Research and Development of Isotopic and Molecular Technologies, Physics Department, Cluj Napoca; (c) University Politehnica Bucharest, Bucharest; (d) West University in Timisoara, Timisoara, Romania

27 Departamento de Física, Universidad de Buenos Aires, Buenos Aires, Argentina

28 Cavendish Laboratory, University of Cambridge, Cambridge, United Kingdom

29 Department of Physics, Carleton University, Ottawa ON, Canada

30 CERN, Geneva, Switzerland

31 Enrico Fermi Institute, University of Chicago, Chicago IL, United States of America

32 (a) Departamento de Física, Pontificia Universidad Católica de Chile, Santiago; (b) Departamento de Física, Universidad Técnica Federico Santa María, Valparaíso, Chile

33 (a) Institute of High Energy Physics, Chinese Academy of Sciences, Beijing; (b) Department of Modern Physics, University of Science and Technology of China, Anhui; (c) Department of Physics, Nanjing University, Jiangsu; (d) School of Physics, Shandong University, Shandong; (e) Physics Department, Shanghai Jiao Tong University, Shanghai, China

34 Laboratoire de Physique Corpusculaire, Clermont Université and Université Blaise Pascal and CNRS/IN2P3, Clermont-Ferrand, France

35 Nevis Laboratory, Columbia University, Irvington NY, United States of America

36 Niels Bohr Institute, University of Copenhagen, Kobenhavn, Denmark

37 (a) INFN Gruppo Collegato di Cosenza, Laboratori Nazionali di Frascati; (b) Dipartimento di Fisica, Università della Calabria, Rende, Italy

38 (a) AGH University of Science and Technology, Faculty of Physics and Applied Computer Science, Krakow; (b) Marian Smoluchowski Institute of Physics, Jagiellonian University, Krakow, Poland

39 The Henryk Niewodniczanski Institute of Nuclear Physics, Polish Academy of Sciences, Krakow, Poland

40 Physics Department, Southern Methodist University, Dallas TX, United States of America

41 Physics Department, University of Texas at Dallas, Richardson TX, United States of America

42 DESY, Hamburg and Zeuthen, Germany

43 Institut für Experimentelle Physik IV, Technische Universität Dortmund, Dortmund, Germany

44 Institut für Kern- und Teilchenphysik, Technische Universität Dresden, Dresden, Germany

45 Department of Physics, Duke University, Durham NC, United States of America

46 SUPA - School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom

47 INFN Laboratori Nazionali di Frascati, Frascati, Italy

48 Fakultät für Mathematik und Physik, Albert-Ludwigs-Universität, Freiburg, Germany

49 Section de Physique, Université de Genève, Geneva, Switzerland

50 (a) INFN Sezione di Genova; (b) Dipartimento di Fisica Università di Genova, Genova, Italy

51 (a) E. Andronikashvili Institute of Physics, Iv. Javakhishvili Tbilisi State University, Tbilisi; (b) High Energy Physics Institute, Tbilisi State University, Tbilisi, Georgia

52 II Physikalisches Institut, Justus-Liebig-Universität Giessen, Giessen, Germany

53 SUPA - School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom

54 II Physikalisches Institut, Georg-August-Universität, Göttingen, Germany

55 Laboratoire de Physique Subatomique et de Cosmologie, Université Grenoble-Alpes, CNRS/IN2P3, Grenoble, France

56 Department of Physics, Hampton University, Hampton VA, United States of America

57 Laboratory for Particle Physics and Cosmology, Harvard University, Cambridge MA, United States of America

58 (a) Kirchhoff-Institut für Physik, Ruprecht-Karls-Universität Heidelberg, Heidelberg; (b) Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg; (c) ZITI Institut für technische Informatik, Ruprecht-Karls-Universität Heidelberg, Mannheim, Germany

59 Faculty of Applied Information Science, Hiroshima Institute of Technology, Hiroshima, Japan

60 Department of Physics, Indiana University, Bloomington IN, United States of America
61 Institut für Astro- und Teilchenphysik, Leopold-Franzens-Universität, Innsbruck, Austria

62 University of Iowa, Iowa City IA, United States of America

63 Department of Physics and Astronomy, Iowa State University, Ames IA, United States of America

64 Joint Institute for Nuclear Research, JINR Dubna, Dubna, Russia

65 KEK, High Energy Accelerator Research Organization, Tsukuba, Japan

66 Graduate School of Science, Kobe University, Kobe, Japan

67 Faculty of Science, Kyoto University, Kyoto, Japan

68 Kyoto University of Education, Kyoto, Japan

69 Department of Physics, Kyushu University, Fukuoka, Japan

70 Instituto de Física La Plata, Universidad Nacional de La Plata and CONICET, La Plata, Argentina

71 Physics Department, Lancaster University, Lancaster, United Kingdom

72 (a) INFN Sezione di Lecce; (b) Dipartimento di Matematica e Fisica, Università del Salento, Lecce, Italy

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

74 Department of Physics, Jožef Stefan Institute and University of Ljubljana, Ljubljana, Slovenia

75 School of Physics and Astronomy, Queen Mary University of London, London, United Kingdom

76 Department of Physics, Royal Holloway University of London, Surrey, United Kingdom

77 Department of Physics and Astronomy, University College London, London, United Kingdom

78 Louisiana Tech University, Ruston LA, United States of America

79 Laboratoire de Physique Nucléaire et de Hautes Energies, UPMC and Université Paris-Diderot and CNRS/IN2P3, Paris, France

80 Fysiska institutionen, Lunds universitet, Lund, Sweden

81 Departamento de Fisica Teorica C-15, Universidad Autonoma de Madrid, Madrid, Spain

82 Institut für Physik, Universität Mainz, Mainz, Germany

83 School of Physics and Astronomy, University of Manchester, Manchester, United Kingdom

84 CPPM, Aix-Marseille Université and CNRS/IN2P3, Marseille, France

85 Department of Physics, University of Massachusetts, Amherst MA, United States of America

86 Department of Physics, McGill University, Montreal QC, Canada

87 School of Physics, University of Melbourne, Victoria, Australia

88 Department of Physics, The University of Michigan, Ann Arbor MI, United States of America

89 Department of Physics and Astronomy, Michigan State University, East Lansing MI, United States of America

90 (a) INFN Sezione di Milano; (b) Dipartimento di Fisica, Università di Milano, Milano, Italy

91 B.I. Stepanov Institute of Physics, National Academy of Sciences of Belarus, Minsk, Republic of Belarus

92 National Scientific and Educational Centre for Particle and High Energy Physics, Minsk, Republic of Belarus

93 Department of Physics, Massachusetts Institute of Technology, Cambridge MA, United States of America

94 Group of Particle Physics, University of Montreal, Montreal QC, Canada

95 P.N. Lebedev Institute of Physics, Academy of Sciences, Moscow, Russia

96 Institute for Theoretical and Experimental Physics (ITEP), Moscow, Russia

97 Moscow Engineering and Physics Institute (MEPhI), Moscow, Russia

98 D.V.Skobeltsyn Institute of Nuclear Physics, M.V.Lomonosov Moscow State University, Moscow, Russia

99 Fakultät für Physik, Ludwig-Maximilians-Universität München, München, Germany

100 Max-Planck-Institut für Physik (Werner-Heisenberg-Institut), München, Germany

101 Nagasaki Institute of Applied Science, Nagasaki, Japan

102 Graduate School of Science and Kobayashi-Maskawa Institute, Nagoya University, Nagoya, Japan

103 (a) INFN Sezione di Napoli; (b) Dipartimento di Fisica, Università di Napoli, Napoli, Italy

104 Department of Physics and Astronomy, University of New Mexico, Albuquerque NM, United States of America

105 Institute for Mathematics, Astrophysics and Particle Physics, Radboud University Nijmegen/Nikhef, Nijmegen, Netherlands

106 Nikhef National Institute for Subatomic Physics and University of Amsterdam, Amsterdam, Netherlands

107 Department of Physics, Northern Illinois University, DeKalb IL, United States of America

108 Budker Institute of Nuclear Physics, SB RAS, Novosibirsk, Russia

109 Department of Physics, New York University, New York NY, United States of America

110 Ohio State University, Columbus OH, United States of America

111 Faculty of Science, Okayama University, Okayama, Japan

112 Homer L. Dodge Department of Physics and Astronomy, University of Oklahoma, Norman OK, United States of America

113 Department of Physics, Oklahoma State University, Stillwater OK, United States of America
114 Palacký University, RCPTM, Olomouc, Czech Republic

115 Center for High Energy Physics, University of Oregon, Eugene OR, United States of America

116 LAL, Université Paris-Sud and CNRS/IN2P3, Orsay, France

117 Graduate School of Science, Osaka University, Osaka, Japan

118 Department of Physics, University of Oslo, Oslo, Norway

119 Department of Physics, Oxford University, Oxford, United Kingdom

120 (a) INFN Sezione di Pavia; (b) Dipartimento di Fisica, Università di Pavia, Pavia, Italy

121 Department of Physics, University of Pennsylvania, Philadelphia PA, United States of America

122 Petersburg Nuclear Physics Institute, Gatchina, Russia

123 (a) INFN Sezione di Pisa; (b) Dipartimento di Fisica E. Fermi, Università di Pisa, Pisa, Italy

124 Department of Physics and Astronomy, University of Pittsburgh, Pittsburgh PA, United States of America

125 (a) Laboratorio de Instrumentacao e Fisica Experimental de Particulas - LIP, Lisboa; (b) Faculdade de Ciências, Universidade de Lisboa, Lisboa; (c) Department of Physics, University of Coimbra, Coimbra; (d) Centro de Física Nuclear da Universidade de Lisboa, Lisboa; (e) Departamento de Fisica, Universidade do Minho, Braga; (f) Departamento de Fisica Teorica y del Cosmos and CAFPE, Universidad de Granada, Granada (Spain); (g) Dep Fisica and CEFITEC of Faculdade de Ciencias e Tecnologia, Universidade Nova de Lisboa, Caparica, Portugal

126 Institute of Physics, Academy of Sciences of the Czech Republic, Praha, Czech Republic

127 Czech Technical University in Prague, Praha, Czech Republic

128 Faculty of Mathematics and Physics, Charles University in Prague, Praha, Czech Republic

129 State Research Center Institute for High Energy Physics, Protvino, Russia

130 Particle Physics Department, Rutherford Appleton Laboratory, Didcot, United Kingdom

131 Physics Department, University of Regina, Regina SK, Canada

132 Ritsumeikan University, Kusatsu, Shiga, Japan

133 (a) INFN Sezione di Roma; (b) Dipartimento di Fisica, Sapienza Università di Roma, Roma, Italy

134 (a) INFN Sezione di Roma Tor Vergata; (b) Dipartimento di Fisica, Università di Roma Tor Vergata, Roma, Italy

135 (a) INFN Sezione di Roma Tre; (b) Dipartimento di Matematica e Fisica, Università Roma Tre, Roma, Italy

136 (a) Faculté des Sciences Ain Chock, Réseau Universitaire de Physique des Hautes Energies - Université Hassan II, Casablanca; (b) Centre National de l'Energie des Sciences Techniques Nucleaires, Rabat; (c) Faculté des Sciences Semlalia, Université Cadi Ayyad, LPHEA-Marrakech; (d) Faculté des Sciences, Université Mohammed Premier and LPTPM, Oujda; (e) Faculté des sciences, Université Mohammed V-Agdal, Rabat, Morocco

137 DSM/IRFU (Institut de Recherches sur les Lois Fondamentales de l'Univers), CEA Saclay (Commissariat à l'Energie Atomique et aux Energies Alternatives), Gif-sur-Yvette, France

138 Santa Cruz Institute for Particle Physics, University of California Santa Cruz, Santa Cruz CA, United States of America

139 Department of Physics, University of Washington, Seattle WA, United States of America

140 Department of Physics and Astronomy, University of Sheffield, Sheffield, United Kingdom

141 Department of Physics, Shinshu University, Nagano, Japan

142 Fachbereich Physik, Universität Siegen, Siegen, Germany

143 Department of Physics, Simon Fraser University, Burnaby BC, Canada

144 SLAC National Accelerator Laboratory, Stanford CA, United States of America

145 (a) Faculty of Mathematics, Physics & Informatics, Comenius University, Bratislava; (b) Department of Subnuclear Physics, Institute of Experimental Physics of the Slovak Academy of Sciences, Kosice, Slovak Republic

146 (a) Department of Physics, University of Cape Town, Cape Town; (b) Department of Physics, University of Johannesburg, Johannesburg; (c) School of Physics, University of the Witwatersrand, Johannesburg, South Africa

147 (a) Department of Physics, Stockholm University; (b) The Oskar Klein Centre, Stockholm, Sweden

148 Physics Department, Royal Institute of Technology, Stockholm, Sweden

149 Departments of Physics & Astronomy and Chemistry, Stony Brook University, Stony Brook NY, United States of America

150 Department of Physics and Astronomy, University of Sussex, Brighton, United Kingdom

151 School of Physics, University of Sydney, Sydney, Australia

152 Institute of Physics, Academia Sinica, Taipei, Taiwan

153 Department of Physics, Technion: Israel Institute of Technology, Haifa, Israel

154 Raymond and Beverly Sackler School of Physics and Astronomy, Tel Aviv University, Tel Aviv, Israel

155 Department of Physics, Aristotle University of Thessaloniki, Thessaloniki, Greece

156 International Center for Elementary Particle Physics and Department of Physics, The University of Tokyo, Tokyo, Japan
157 Graduate School of Science and Technology, Tokyo Metropolitan University, Tokyo, Japan

158 Department of Physics, Tokyo Institute of Technology, Tokyo, Japan

159 Department of Physics, University of Toronto, Toronto ON, Canada

160 (a) TRIUMF, Vancouver BC; (b) Department of Physics and Astronomy, York University, Toronto ON, Canada

161 Faculty of Pure and Applied Sciences, University of Tsukuba, Tsukuba, Japan

162 Department of Physics and Astronomy, Tufts University, Medford MA, United States of America

163 Centro de Investigaciones, Universidad Antonio Narino, Bogota, Colombia

164 Department of Physics and Astronomy, University of California Irvine, Irvine CA, United States of America

165 (a) INFN Gruppo Collegato di Udine, Sezione di Trieste, Udine; (b) ICTP, Trieste; (c) Dipartimento di Chimica, Fisica e Ambiente, Università di Udine, Udine, Italy

166 Department of Physics, University of Illinois, Urbana IL, United States of America

167 Department of Physics and Astronomy, University of Uppsala, Uppsala, Sweden

168 Instituto de Física Corpuscular (IFIC) and Departamento de Física Atómica, Molecular y Nuclear and Departamento de Ingeniería Electrónica and Instituto de Microelectrónica de Barcelona (IMB-CNM), University of Valencia and CSIC, Valencia, Spain

169 Department of Physics, University of British Columbia, Vancouver BC, Canada

170 Department of Physics and Astronomy, University of Victoria, Victoria BC, Canada

171 Department of Physics, University of Warwick, Coventry, United Kingdom

172 Waseda University, Tokyo, Japan

173 Department of Particle Physics, The Weizmann Institute of Science, Rehovot, Israel

174 Department of Physics, University of Wisconsin, Madison WI, United States of America

175 Fakultät für Physik und Astronomie, Julius-Maximilians-Universität, Würzburg, Germany

176 Fachbereich C Physik, Bergische Universität Wuppertal, Wuppertal, Germany

177 Department of Physics, Yale University, New Haven CT, United States of America

178 Yerevan Physics Institute, Yerevan, Armenia

179 Centre de Calcul de l'Institut National de Physique Nucléaire et de Physique des Particules (IN2P3), Villeurbanne, France

a Also at Department of Physics, King's College London, London, United Kingdom

b Also at Institute of Physics, Azerbaijan Academy of Sciences, Baku, Azerbaijan

c Also at Particle Physics Department, Rutherford Appleton Laboratory, Didcot, United Kingdom

d Also at TRIUMF, Vancouver BC, Canada

e Also at Department of Physics, California State University, Fresno CA, United States of America

f Also at Tomsk State University, Tomsk, Russia

g Also at CPPM, Aix-Marseille Université and CNRS/IN2P3, Marseille, France

h Also at Università di Napoli Parthenope, Napoli, Italy

i Also at Institute of Particle Physics (IPP), Canada

j Also at Department of Physics, St. Petersburg State Polytechnical University, St. Petersburg, Russia

k Also at Chinese University of Hong Kong, China

l Also at Department of Financial and Management Engineering, University of the Aegean, Chios, Greece

m Also at Louisiana Tech University, Ruston LA, United States of America

n Also at Institutucio Catalana de Recerca i Estudis Avancats, ICREA, Barcelona, Spain

o Also at Department of Physics, The University of Texas at Austin, Austin TX, United States of America

p Also at Institute of Theoretical Physics, Ilia State University, Tbilisi, Georgia

q Also at CERN, Geneva, Switzerland

r Also at Ochadai Academic Production, Ochanomizu University, Tokyo, Japan

s Also at Manhattan College, New York NY, United States of America

t Also at Novosibirsk State University, Novosibirsk, Russia

u Also at Institute of Physics, Academia Sinica, Taipei, Taiwan

v Also at LAL, Université Paris-Sud and CNRS/IN2P3, Orsay, France

w Also at Academia Sinica Grid Computing, Institute of Physics, Academia Sinica, Taipei, Taiwan

x Also at Laboratoire de Physique Nucléaire et de Hautes Energies, UPMC and Université Paris-Diderot and CNRS/IN2P3, Paris, France

y Also at School of Physical Sciences, National Institute of Science Education and Research, Bhubaneswar, India

z Also at Dipartimento di Fisica, Sapienza Università di Roma, Roma, Italy

aa Also at Moscow Institute of Physics and Technology State University, Dolgoprudny, Russia

ab Also at Section de Physique, Université de Genève, Geneva, Switzerland
ac Also at International School for Advanced Studies (SISSA), Trieste, Italy

ad Also at Department of Physics and Astronomy, University of South Carolina, Columbia SC, United States of America

ae Also at School of Physics and Engineering, Sun Yat-sen University, Guangzhou, China

af Also at Faculty of Physics, M.V.Lomonosov Moscow State University, Moscow, Russia

ag Also at Moscow Engineering and Physics Institute (MEPhI), Moscow, Russia

ah Also at Institute for Particle and Nuclear Physics, Wigner Research Centre for Physics, Budapest, Hungary

ai Also at Department of Physics, Oxford University, Oxford, United Kingdom

aj Also at Department of Physics, Nanjing University, Jiangsu, China

ak Also at Institut für Experimentalphysik, Universität Hamburg, Hamburg, Germany

al Also at Department of Physics, The University of Michigan, Ann Arbor MI, United States of America

am Also at Discipline of Physics, University of KwaZulu-Natal, Durban, South Africa

an Also at University of Malaya, Department of Physics, Kuala Lumpur, Malaysia

* Deceased