# Search for Quantum Black Hole Production in High-Invariant-Mass Lepton+Jet Final States Using pp Collisions at $\sqrt{s} = 8$ TeV and the ATLAS Detector

G. Aad, S. Albrand, J. Brown, Q. Buat, B. Clement, J. Collot, S.

Crépé-Renaudin, B. Dechenaux, T. Delemontex, P.A. Delsart, et al.

► To cite this version:

G. Aad, S. Albrand, J. Brown, Q. Buat, B. Clement, et al., Search for Quantum Black Hole Production in High-Invariant-Mass Lepton+Jet Final States Using pp Collisions at $\sqrt{s} = 8$ TeV and the ATLAS Detector. Physical Review Letters, 2014, 112, pp.091804. 10.1103/PhysRevLett.112.091804. in2p3-00903820

HAL Id: in2p3-00903820

https://hal.in2p3.fr/in2p3-00903820

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# Search for Quantum Black Hole Production in High-Invariant-Mass Lepton+Jet Final States Using $pp$ Collisions at $\sqrt{s} = 8$ TeV and the ATLAS Detector

The ATLAS Collaboration

## Abstract

This Letter presents a search for quantum black-hole production using $20.3 \text{ fb}^{-1}$ of data collected with the ATLAS detector in $pp$ collisions at the LHC at $\sqrt{s} = 8$ TeV. The quantum black holes are assumed to decay into a final state characterized by a lepton (electron or muon) and a jet. In either channel, no event with a lepton-jet invariant mass of 3.5 TeV or more is observed, consistent with the expected background. Limits are set on the product of cross sections and branching fractions for the lepton+jet final states of quantum black holes produced in a search region for invariant masses above 1 TeV. The combined 95% confidence level upper limit on this product for quantum black holes with threshold mass above 3.5 TeV is 0.18 fb. This limit constrains the threshold quantum black-hole mass to be above 5.3 TeV in the model considered.
# Search for Quantum Black Hole Production in High-Invariant-Mass Lepton+Jet Final States Using *pp* Collisions at $\sqrt{s} = 8$ TeV and the ATLAS Detector

The ATLAS Collaboration

This Letter presents a search for quantum black-hole production using $20.3 \text{ fb}^{-1}$ of data collected with the ATLAS detector in $pp$ collisions at the LHC at $\sqrt{s} = 8$ TeV. The quantum black holes are assumed to decay into a final state characterized by a lepton (electron or muon) and a jet. In either channel, no event with a lepton-jet invariant mass of 3.5 TeV or more is observed, consistent with the expected background. Limits are set on the product of cross sections and branching fractions for the lepton+jet final states of quantum black holes produced in a search region for invariant masses above 1 TeV. The combined 95% confidence level upper limit on this product for quantum black holes with threshold mass above 3.5 TeV is 0.18 fb. This limit constrains the threshold quantum black-hole mass to be above 5.3 TeV in the model considered.

PACS numbers: 13.85.Qk, 04.50.Gh, 04.50.Cd

Quantum black holes (QBHs) [1, 2] are predicted in low-scale quantum gravity theories that offer solutions to the mass hierarchy problem of the Standard Model (SM) by lowering the scale of quantum gravity ($M_D$) from the Planck scale ($\sim 10^{16}$ TeV) to a value of about 1 TeV. In models with large extra dimensions such as the Arkani-Hamed-Dimopoulos-Dvali (ADD) model [3-5], only the gravitational field is allowed to penetrate the $n$ extra dimensions, while all SM fields are localized in the usual four-dimensional space-time. QBHs with masses near $M_D$, postulated to conserve total angular momentum, color and electric charge, may decay to two particles [2, 6]. The behavior of QBHs is distinct from semi-classical black holes that decay via Hawking radiation to a large number of objects [7]. Searches for semi-classical black holes typically require three or more objects [8, 9].

The quantum approximations used in the modeling of black hole production are valid when black-hole masses are above a minimal threshold mass, $M_{\text{th}}$, which is taken to be equivalent to the QBH inverse gravitational radius. If the QBHs investigated in this Letter are accessible at the Large Hadron Collider (LHC) [10], they can produce lepton+jet final states [2, 6] motivating this first dedicated search for high-invariant-mass final states with a single electron (e) or a single muon (μ), and at least one jet. Two-particle QBH decays to a final state consisting of a lepton and a quark-jet violate lepton and baryon number conservation, producing a distinctive signal for physics beyond the SM. Previous searches for QBHs relied on signatures such as dijet mass distributions [11, 12], generic multiobject configurations [9] and photon+jet final states [13].

The largest QBH cross section for the final states considered is predicted for the collision of two u-quarks ($\sigma_{uu}$), which produces charge +4/3 objects with equal branching fractions (BFs) of $BF_{uu} = 11\%$ to each lepton+jet final state. The next largest cross sections are for charge +1/3 ($ud$) and -2/3 ($dd$) QBHs with lepton+jet BFs of $BF_{ud} = 5.7\%$ and $BF_{dd} = 6.7\%$ [6]. Processes with initial states having antiquarks and heavier sea-

quarks are suppressed by at least a factor of 100 and can be neglected. The QBH cross section is a steeply declining function of $M_{\text{th}}$, and has $\Sigma\sigma_{qq} \times \text{BF}_{qq} \approx 8.6 \times 10^5 \text{ fb}$, $8.9 \times 10^2 \text{ fb}$ and 0.75 fb for $M_{\text{th}}$ of 1 TeV, 3 TeV and 5 TeV, respectively [14].

The ATLAS detector [15] includes an inner tracker, covering a pseudorapidity [16] range $|\eta| < 2.5$, surrounded by a superconducting solenoid providing a 2 T central field. A liquid-argon (LAr) electromagnetic (EM) sampling calorimeter ($|\eta| < 3.2$), a scintillator-tile hadronic calorimeter ($|\eta| < 1.7$), a LAr hadronic calorimeter ($1.4 < |\eta| < 3.2$), and a LAr forward calorimeter ($3.1 < |\eta| < 4.9$) provide the energy measurements. The muon spectrometer consists of tracking chambers covering $|\eta| < 2.7$, and trigger chambers covering $|\eta| < 2.4$, in a magnetic field produced by a system of air-core toroids. Events considered in this analysis are required to have one high-transverse-momentum (high-$p_T$) lepton ($e/\mu$) that passes requirements of the three-level trigger system [17]. The thresholds applied at the third trigger level are 60 GeV and 36 GeV for electrons and muons, respectively. The analysis is based on the complete 2012 data set of $pp$ collisions taken at a center-of-mass energy of $\sqrt{s} = 8$ TeV by the ATLAS detector at the LHC, corresponding to an integrated luminosity of $20.3 \pm 0.6 \text{ fb}^{-1}$ [18] after data-quality requirements.

The event selection is designed to be efficient for generic lepton+jet final states and is based on leading-order simulated-signal QBH events obtained from the QBH1.04 generator [14], followed by parton showering and hadronization using PYTHIA8.165 [19]. The signal generator uses the MSTW2008LO [20] set of leading-order parton distribution functions (PDFs) with the AU2 underlying-event tune [21]. This Letter assumes the ADD model with $M_{\text{th}} = M_D$, $n=6$, and the QCD factorization scale for the PDFs set to the inverse gravitational radius [14]. Samples with $M_{\text{th}}$ from 1 TeV to 6 TeV, in steps of 0.5 TeV, are generated for both channels.

Events with a high-$p_T$ lepton and one or more jets can also arise from electroweak (EW) processes includ-
ing vector-boson production with additional jets; diboson (WW, WZ, ZZ), top-quark pair ($t\bar{t}$) and single top-quark ($t$ or $\bar{t}$) production; and multijet processes including non-prompt leptons from semileptonic hadron decays and jets misidentified as leptons.

The EW background in the signal region (SR) is estimated using Monte Carlo (MC) samples normalized to data in control regions. All MC simulated samples are produced using the ATLAS detector simulation [22] based on GEANT4 [23]. The simulated events are reconstructed in the same manner as the data. The $t\bar{t}$ and single-top-quark events are simulated with MC@NLO4.06 [24] and AcerMC3.8 [25], respectively; the production of W+jets and Z+jets is simulated using ALPGEN2.14 [26]; and diboson production is simulated with SHERPA1.4.1 [27]. The leading-order CTEQ6L1 PDFs [28] are used for ALPGEN and AcerMC samples while the next-to-leading-order CT10 PDFs [29] are used for the SHERPA and MC@NLO samples. The generators for all samples except dibosons are interfaced to HERWIG6.520 [30, 31] for parton showering and hadronization and to JIMMY4.31 [32] for the underlying-event model. The results of higher-order calculations are used to adjust the relative fractions of the simulated events as in Refs. [33, 34]. Additional inelastic pp interactions, termed pileup, are included in the event simulation so as to match the distribution in the data (on average 21 interactions per bunch crossing).

Electron candidates are identified as localized deposits of energy in the EM calorimeter with $p_{T_e} > 130$ GeV and $|\eta| < 2.47$, excluding the barrel-endcap transition region, $1.37 < |\eta| < 1.52$, and matched to a track reconstructed in the tracking detectors. Background from jets is reduced by requiring that the shower profiles are consistent with those of electrons [35]. Isolated electrons are selected by requiring the transverse energy deposited in a cone of radius $\Delta R = \sqrt{(\Delta\eta)^2 + (\Delta\phi)^2} = 0.3$ centered on the electron cluster, excluding the energy of the electron cluster itself, to be less than $0.0055 \times p_{T_e} + 3.5$ GeV after corrections for energy due to pileup and energy leakage from the electron cluster into the cone. This criterion provides nearly constant selection efficiency for signal events over the entire $p_{T_e}$ range explored and for all the pileup conditions.

Muon candidates are required to be detected in at least three layers of the muon spectrometer and to have $p_{T_\mu} > 130$ GeV and $|\eta| < 2.4$. Possible background from cosmic rays is reduced by requiring the transverse and longitudinal distances of closest approach to the interaction point to be smaller than 0.2 mm and 1.0 mm, respectively. Signal muons are required to be isolated such that $\sum p_T < 0.05 \times p_{T_\mu}$, where $\sum p_T$ is the sum of the $p_T$ of the other tracks in a cone of radius $\Delta R = 0.3$ around the direction of the muon.

Jets are constructed from three-dimensional noise-suppressed clusters of calorimeter cells using the anti-$k_t$

algorithm with a radius parameter of 0.4 [36, 37]. Jet energies are corrected for losses in material in front of the active calorimeter layers, detector inhomogeneities, the non-compensating nature of the calorimeter, and pileup. Jet energies are calibrated using MC simulation and the combination of several in-situ techniques applied to data [38–40]. All jets are required to have $p_{T_j} > 50$ GeV and $|\eta| < 2.5$. In addition, the most energetic jet is required to have $p_{T_j} > 130$ GeV.

The missing transverse momentum (with magnitude $E_T^{\text{miss}}$), used only in the background estimation, is calculated as the negative of the vectorial sum of calibrated clustered energy deposits in the calorimeters, and is corrected for the momenta of any reconstructed muons [41].

In the electron (muon) channel, events are required to have exactly one electron (muon). Multijet background can be reduced, with minimal loss in signal efficiency, by requiring the average value of $\eta$ for the lepton and leading jet to satisfy $|\langle\eta\rangle| < 1.25$ and the difference between the lepton and leading jet $\eta$ to satisfy $|\Delta\eta| < 1.5$. The signal lepton and jet are mostly back-to-back in $\phi$ and are required to satisfy $|\Delta\phi| > \pi/2$.

The invariant mass ($m_{\text{inv}}$) is calculated from the lepton and highest-$p_T$ jet. The SR is defined by a lower bound on $m_{\text{inv}}$, $m_{\text{min}}$, that accounts for experimental resolution. In the electron channel $m_{\text{min}} = 0.9 M_{\text{this}}$ used. In the muon channel, the requirement is loosened at high invariant mass, as muon resolution has a term quadratic in $p_{T_\mu}$, resulting in $m_{\text{min}} = [0.95 - 0.05 M_{\text{th}}/1 \text{TeV}] M_{\text{th}}$. A low-invariant-mass control region (LIMCR) is defined with $m_{\text{inv}}$ between 400 GeV and 900 GeV, which has a negligible contamination from a potential signal ($< 2\%$) for the lowest $M_{\text{th}}$ considered.

The acceptance of the event selection is about 65%, based on generator-level quantities and calculated by imposing selection criteria that apply directly to phase space (lepton/jet $\eta$, lepton/jet $p_T$, $\Delta\eta$, $\Delta\phi$, $\langle\eta\rangle$, and $m_{\text{inv}}$). All other selection criteria, which in general correspond to event and object quality requirements, are used to calculate the experimental efficiency based on the events included in the acceptance. The experimental efficiency falls from 89(59)% to 81(50)% for masses from 1 TeV to 6 TeV in the electron (muon) channel. The experimental efficiency in the muon channel is lower than that in the electron channel because more stringent requirements are applied to ensure the best possible resolution on $m_{\text{inv}}$. The cumulative signal efficiency is the product of the acceptance and experimental efficiency.

In the electron channel, the multijet background is characterized by small values of $E_T^{\text{miss}}$, while EW background events can have large $E_T^{\text{miss}}$ due to the production of high-momentum neutrinos. The discriminating power of $E_T^{\text{miss}}$ is used to determine the normalization of the two backgrounds to the data in the LIMCR. The multijet template is taken from data in which electron candidates pass relaxed identification criteria but fail the normal
identification selection, and the EW template is taken from MC simulation where electron candidates pass the normal selection. The templates are fit to the $E_T^{\text{miss}}$ distribution in the interval [0, 150] GeV in five separate detector-motivated regions of $\eta$, to determine normalization factors for both the multijet and EW backgrounds.

To extrapolate both the multijet and EW background to the SR, functions of the form $p_1 x^{p_2+p_3 \ln(x)}(1-x)^{p_4}$ (with $x = m_{\text{inv}}/\sqrt{s}$ and fit parameters $p_1-p_4$) [42] are used and the contributions are scaled by the corresponding normalization factor derived in the LIMCR. A simple power-law fit, with $p_3$ and $p_4$ fixed to zero, adequately describes both data and simulation. This is used as the baseline, while $p_3$ and $p_4$ are allowed to vary as part of the evaluation of the systematic uncertainty.

In the muon channel, the multijet and EW backgrounds can be discriminated on the basis of the transverse impact parameter ($d_0$) distribution of the muon since multijet background is dominated by jets containing charm and bottom hadrons decaying to muons while EW backgrounds are dominated by prompt muons. The template for the EW background is selected using Z-boson decays to two muons while the template for multijet background is taken from muons that fail the isolation requirement. Both templates are taken from data. The templates are fit to the $d_0$ distribution in the interval [-0.1, +0.1] mm to determine the normalization factors. The fraction of multijet background, $0.046 \pm 0.005$, is neglected when extrapolating the background in SR. The procedure for extrapolating the EW background to the SR is the same as for the electron channel.

The background estimate in the SR, shown in Fig. 1, was not compared to data until the final fit method and parameters were fixed. The hatched area in Fig. 1 shows the total uncertainty in the background estimate, which is dominated by the systematic uncertainties. In extracting the limits, the fits described above are used to extrapolate the background into the high invariant-mass region.

The systematic uncertainties on the background are evaluated as a function of $m_{\text{inv}}$, and are dominated by uncertainties on the fits used to extrapolate the background to the highest $m_{\text{inv}}$, uncertainties on PDFs, and the choice of MC generator. Systematic uncertainties due to the choice of fitting functions are evaluated by fitting the $m_{\text{inv}}$ spectrum with parameters $p_3$ and $p_4$ free and taking the difference between these fits and the fits with $p_3$ and $p_4$ fixed to zero. Additionally, SHERPA samples are used instead of ALPGEN and the fits are repeated. The uncertainty in the PDFs is estimated using a set of 44 PDF eigenvectors for CTEQ6.6 [43]. For each of the 44 sets, the background fits are repeated and the extrapolated backgrounds are estimated. To estimate the uncertainty in the multijet background in the electron channel, an alternative selection of background-enriched data events, based on photons, is used. The systematic uncer-

<figure><img src="image_2.png" /><figcaption>FIG. 1. Distribution of the invariant mass of the lepton and highest-$p_T$ jet in (a) the electron+jet channel and (b) the muon+jet channel, for data (points with error bars) and for SM backgrounds (solid histograms). Overlaid are two examples of QBH signals. The sum of the uncertainties due to the finite MC sample size and from various sources of systematic uncertainty is shown by the hatched area. To extract the upper limit on the lepton+jet cross section, a fit to the invariant-mass distribution is performed, replacing the uncertainties due to MC sample size by the statistical uncertainties on the fit parameters.</figcaption></figure>

tainties from the simulation of the detector response are associated with the jet and electron energy scales and resolutions, the muon momentum scale and resolution, and the trigger requirement. The combined uncertainty in the background prediction ranges from 16% (1 TeV) to 100% (6 TeV) for the electron channel and from 50% (1 TeV) to 170% (6 TeV) for the muon channel. Background systematic uncertainties for $M_{\text{th}} = 5$ TeV are given in Table I.

Uncertainties on the signal efficiency in each of the mass bins are associated with the requirements on $\Delta\eta$, $\Delta\phi$, $\langle\eta\rangle$, $m_{\text{inv}}$, and isolation. In addition, uncertainties on the detector simulation, mentioned above for the background, as well as the uncertainty in luminosity are taken into account. The combined uncertainty in the signal efficiency from these sources ranges from 3.5% at 1 TeV to
<table><caption>TABLE I. Breakdown of relative systematic uncertainties on the SM background for the threshold mass $M_{th} = 5$ TeV. The uncertainties are added in quadrature to obtain the total uncertainty.</caption><thead><tr><th rowspan="2">Source</th><th colspan="2">Electron+jet</th><th colspan="2">Muon+jet</th></tr><tr><th></th><th>%</th><th></th><th>%</th></tr></thead><tbody><tr><td>Lepton reconstruction, scale and resolution</td><td>+2</td><td>-1</td><td>+30</td><td>-7</td></tr><tr><td>Jet reconstruction, scale and resolution</td><td>+31</td><td>-15</td><td>+5</td><td>-5</td></tr><tr><td>Multijet modeling</td><td>+27</td><td>-27</td><td>-</td><td>-</td></tr><tr><td>PDF</td><td>+52</td><td>-33</td><td>+100</td><td>-69</td></tr><tr><td>Fit</td><td>+77</td><td>-77</td><td>+130</td><td>-71</td></tr><tr><td>Total</td><td>+100</td><td>-89</td><td>+170</td><td>-100</td></tr></tbody></table>

<table><caption>TABLE II. Numbers of expected background (Exp.) and observed (Obs.) events, along with the cumulative signal efficiencies (Eff.), with uncertainties including both the statistical and systematic components for various values of $M_{th}$. Numbers of events are integrated above $m_{inv}$ requirement for the given $M_{th}$.</caption><thead><tr><th rowspan="2">M<sub>th</sub></th><th colspan="3">Electron+jet</th><th colspan="3">Muon+jet</th></tr><tr><th>Obs.</th><th>Exp.</th><th>Eff.</th><th>Obs.</th><th>Exp.</th><th>Eff.</th></tr><tr><th>TeV</th><th colspan="3">%</th><th colspan="3">%</th></tr></thead><tbody><tr><td>1.0</td><td>1200</td><td>1210<sup>+230</sup><sub>-220</sub></td><td>57 ± 4</td><td>620</td><td>550 ± 280</td><td>38 ± 4</td></tr><tr><td>1.5</td><td>100</td><td>110 ± 40</td><td>57 ± 4</td><td>49</td><td>65<sup>+45</sup><sub>-40</sub></td><td>36 ± 4</td></tr><tr><td>2.0</td><td>12</td><td>19<sup>+13</sup><sub>-12</sub></td><td>56 ± 4</td><td>8</td><td>14<sup>+16</sup><sub>-14</sub></td><td>36 ± 4</td></tr><tr><td>2.5</td><td>0</td><td>5.3<sup>+4.5</sup><sub>-3.9</sub></td><td>55 ± 4</td><td>3</td><td>5<sup>+6</sup><sub>-5</sub></td><td>34 ± 4</td></tr><tr><td>3.0</td><td>0</td><td>1.8<sup>+1.8</sup><sub>-1.6</sub></td><td>54 ± 4</td><td>1</td><td>2.1<sup>+2.9</sup><sub>-2.1</sub></td><td>34 ± 4</td></tr><tr><td>3.5</td><td>0</td><td>0.76<sup>+0.79</sup><sub>-0.67</sub></td><td>54 ± 4</td><td>0</td><td>1.0<sup>+1.6</sup><sub>-1.0</sub></td><td>33 ± 4</td></tr><tr><td>4.0</td><td>0</td><td>0.35<sup>+0.38</sup><sub>-0.34</sub></td><td>53 ± 4</td><td>0</td><td>0.57<sup>+0.94</sup><sub>-0.57</sub></td><td>33 ± 5</td></tr><tr><td>5.0</td><td>0</td><td>0.09<sup>+0.10</sup><sub>-0.09</sub></td><td>52 ± 4</td><td>0</td><td>0.24<sup>+0.39</sup><sub>-0.24</sub></td><td>32 ± 5</td></tr><tr><td>6.0</td><td>0</td><td>0.03<sup>+0.04</sup><sub>-0.03</sub></td><td>52 ± 4</td><td>0</td><td>0.13<sup>+0.22</sup><sub>-0.13</sub></td><td>32 ± 6</td></tr></tbody></table>

3.9% at 6 TeV for the electron channel and from 3.6% at 1 TeV to 5.6% at 6 TeV for the muon channel. The cumulative efficiency, shown in Table II, is taken from the signal MC simulation for charge +4/3 QBHs. The differences in the efficiency between the charge +4/3 state and the other charged states are much smaller than the uncertainties mentioned above and are neglected. The effect of the 0.65% uncertainty in the LHC beam energy [44] is to change the QBH production cross section. Since the QBH cross section is nearly constant in $M_{th}/\sqrt{s}$ this is effectively an uncertainty in $M_{th}$ and has a negligible effect on the limits.

The observed numbers of events and the expected backgrounds, shown in Table II, are in agreement within the total uncertainty. There is no evidence for any excess. Upper limits on $\Sigma\sigma_{qq} \times \text{BF}_{qq}$ for the production of QBHs above $M_{th}$ are determined in the interval 1–6 TeV assuming lepton universality and using the CLs method [45, 46], which is designed to give conservative limits in cases where the observed background fluctuates below the expected values. The statistical combination of the channels employs a likelihood function constructed as the product of Poisson probability terms describing the total number of events observed in each channel. Systematic uncertainties are incorporated as nuisance parameters into the likelihood through their effect on the mean of the Poisson functions and through convolution with their assumed Gaussian distributions. Correlations between channels are taken into account.

<figure><img src="image_3.png" /><figcaption>FIG. 2. The combined 95% C.L. upper limits on $\Sigma\sigma_{qq} \times \text{BF}_{qq}$ for QBHs decaying to a lepton and jet, as a function of $M_{th}$, assuming $M_{D} = M_{th}$ and $n = 6$ ADD extra dimensions. The limits take into account statistical and systematic uncertainties. Points along the solid black line indicate the mass of the signal where the limit is computed. Also shown are the $\pm 1\sigma$ and $\pm 2\sigma$ bands indicating the underlying distribution of possible limit outcomes under the background-only hypothesis. The predicted cross section for QBHs is shown as the solid curve.</figcaption></figure>

Figure 2 shows the 95% confidence level (C.L.) combined lepton+jet upper limit on the cross section times branching fraction for the production of QBHs as a function of $M_{th}$. Above 3.5 TeV, the limit is 0.18 fb. For the $n = 6$ QBH model assumed in this Letter, the 95% C.L. lower limit on $M_{th}$ is 5.3 TeV. For $n = 2$, and all other model assumptions the same, the 95% C.L. lower limit on $M_{th}$ is 4.7 TeV. Treating the channels separately, the 95% C.L. upper limit on the electron (muon)+jet $\Sigma\sigma_{qq} \times \text{BF}_{qq}$ above 3.5 TeV is 0.27 (0.49) fb, and the $n = 6$ lower limit on $M_{th}$ is 5.2 (5.1) TeV.

In conclusion, a first search for two body lepton+jet final states with large invariant mass has been performed using $20.3 \text{ fb}^{-1}$ of pp collisions recorded at $\sqrt{s} = 8$ TeV with the ATLAS detector at the LHC. In the invariant-mass region above 1 TeV the observed events are consistent with data-driven extrapolated backgrounds from the low-invariant-mass control region. Above 3.5 TeV the excess.
pected background drops below one event and the 95% C.L. upper limit on the electron (muon)+jet $\Sigma\sigma_{qq} \times \text{BF}_{qq}$ is 0.27 (0.49) fb. Assuming lepton universality, the 95% C.L. upper limit on the sum of the product of QBH lepton+jet production cross sections and branching fractions is 0.18 fb.

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, DIP and Benoziyo Center, Israel; INFN, Italy; MEXT and JSPS, Japan; CNRST, Morocco; FOM and NWO, Netherlands; BRF and RCN, Norway; MNiSW, 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] P. Meade and L. Randall, J. High Energy Phys. 05, 003 (2008), arXiv:0708.3017 [hep-ph].

[2] X. Calmet, W. Gong, and S. D. Hsu, Phys. Lett. B 668, 20 (2008), arXiv:0806.4605 [hep-ph].

[3] N. Arkani-Hamed, S. Dimopoulos, and G. R. Dvali, Phys. Lett. B 429, 263 (1998), arXiv:hep-ph/9803315.

[4] I. Antoniadis, N. Arkani-Hamed, S. Dimopoulos, and G. R. Dvali, Phys. Lett. B 436, 257 (1998), arXiv:hep-ph/9804398.

[5] N. Arkani-Hamed, S. Dimopoulos, and G. R. Dvali, Phys. Rev. D 59, 086004 (1999), arXiv:hep-ph/9807344.

[6] D. M. Gingrich, J. Phys. G 37, 105008 (2010), arXiv:0912.0826 [hep-ph].

[7] L. A. Anchordoqui, J. L. Feng, H. Goldberg, and A. D. Shapere, Phys. Rev. D 65, 124027 (2002), arXiv:hep-ph/0112247.

[8] ATLAS Collaboration, Phys. Lett. B 716, 122 (2012), arXiv:1204.4646 [hep-ex].

[9] CMS Collaboration, J. High Energy Phys. 07, 178 (2013), arXiv:1303.5338 [hep-ex].

[10] L. Evans and P. Bryant, JINST 3, S08001 (2008).

[11] ATLAS Collaboration, J. High Energy Phys. 01, 029 (2013), arXiv:1210.1718 [hep-ex].

[12] CMS Collaboration, JHEP 1301, 013 (2013), arXiv:1210.2387 [hep-ex].

[13] ATLAS Collaboration, Phys. Lett. B 728, 562 (2014), arXiv:1309.3230 [hep-ex].

[14] D. M. Gingrich, Comput. Phys. Commun. 181, 1917 (2010), arXiv:0911.5370 [hep-ph].

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

[16] 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 pipe. The x-axis points from the IP to the center of the LHC ring, and the y-axis points upward. The pseudorapidity is defined in terms of the polar angle $\theta$ as $\eta = -\ln\tan(\theta/2)$. Cylindrical coordinates $(r, \phi)$ are used in the transverse plane, $\phi$ being the azimuthal angle around the beam pipe, referred to the x-axis.

[17] ATLAS Collaboration, Eur. Phys. J. C 72, 1849 (2012), arXiv:1110.1530 [hep-ex].

[18] ATLAS Collaboration, Eur. Phys. J. C 73, 2518 (2013), arXiv:1302.4393 [hep-ex].

[19] T. Sjostrand, S. Mrenna, and P. Z. Skands, Comput. Phys. Commun. 178, 852 (2008), arXiv:0710.3820 [hep-ph].

[20] A. Martin, W. Stirling, R. Thorne, and G. Watt, Eur. Phys. J. C 63, 189 (2009), arXiv:0901.0002 [hep-ph].

[21] ATLAS Collaboration, ATL-PHYS-PUB-2012-003 (2012), http://cds.cern.ch/record/1474107/.

[22] ATLAS Collaboration, Eur. Phys. J. C 70, 823 (2010), arXiv:1005.4568 [physics.ins-det].

[23] GEANT4 Collaboration, Nucl. Instrum. Methods Phys. Res., Sect. A 506, 250 (2003).

[24] S. Frixione et al., J. High Energy Phys. 07, 029 (2008), arXiv:0805.3067 [hep-ph].

[25] B. P. Kersevan and E. Richter-Was, Comput. Phys. Commun. 184, 919 (2013), arXiv:hep-ph/0405247.

[26] M. L. Mangano et al., J. High Energy Phys. 07, 001 (2003), arXiv:hep-ph/0206293.

[27] T. Gleisberg et al., J. High Energy Phys. 02, 007 (2009), arXiv:0811.4622 [hep-ph].

[28] J. Pumplin et al., J. High Energy Phys. 07, 012 (2002), arXiv:hep-ph/0201195.

[29] H.-L. Lai et al., Phys. Rev. D 82, 074024 (2010), arXiv:1007.2241 [hep-ph].

[30] G. Corcella et al., J. High Energy Phys. 01, 010 (2001), arXiv:hep-ph/0011363.

[31] ATLAS Collaboration, ATLAS-PUB-2011-008 (2011), https://cds.cern.ch/record/1345343.

[32] J. Butterworth, J. R. Forshaw, and M. Seymour, Z. Phys. C 72, 637 (1996), arXiv:hep-ph/9601371.

[33] R. Hamberg, W. L. van Neerven, and T. Matsuura, Nucl. Phys. B 359, 343 (1991).

[34] Q. Seth et al., Comput. Phys. Commun. 184, 209 (2013), arXiv:1201.5896 [hep-ph].

[35] ATLAS Collaboration, Eur. Phys. J. C 72, 1909 (2012), arXiv:1110.3174 [hep-ex].
[36] M. Cacciari, G. P. Salam, and G. Soyez, J. High Energy Phys. 04, 063 (2008), arXiv:0802.1189 [hep-ph].

[37] M. Cacciari and G. P. Salam, Phys. Lett. B 641, 57 (2006), arXiv:hep-ph/0512210.

[38] ATLAS Collaboration, Eur. Phys. J. C 73, 2304 (2013), arXiv:1112.6426 [hep-ex].

[39] M. Cacciari, G. P. Salam, and G. Soyez, J. High Energy Phys. 04, 005 (2008), arXiv:0802.1188 [hep-ph].

[40] M. Cacciari, G. P. Salam, and S. Sapeta, J. High Energy Phys. 04, 065 (2010), arXiv:0912.4926 [hep-ph].

[41] ATLAS Collaboration, Eur. Phys. J. C 72, 1844 (2012), arXiv:1108.5602 [hep-ex].

[42] R. M. Harris and K. Kousouris, Int. J. Mod. Phys. A 26, 5005 (2011), arXiv:1110.5302 [hep-ex].

[43] P. M. Nadolsky et al., Phys. Rev. D 78, 013004 (2008), arXiv:0802.0007 [hep-ph].

[44] J. Wenninger, CERN-ATS-2013-040 (2013), http://cds.cern.ch/record/1546734.

[45] T. Junk, Nucl. Instrum. Methods Phys. Res., Sect. A 434, 435 (1999), arXiv:hep-ex/9902006.

[46] A. L. Read, J. Phys. G 28, 2693 (2002).
The ATLAS Collaboration

G. Aad⁴⁸, T. Abajyan²¹, B. Abbott¹¹², J. Abdallah¹⁵², S. Abdel Khalek¹¹⁶, O. Abdinov¹¹, R. Aben¹⁰⁶, B. Abi¹¹³, M. Abolins⁸⁹, O.S. AbouZeid¹⁵⁹, H. Abramowicz¹⁵⁴, H. Abreu¹³⁷, Y. Abulaiti¹⁴⁷a,¹⁴⁷b, B.S. Acharya¹⁶⁵a,¹⁶⁵b, a, L. Adamczyk³⁸a, D.L. Adams²⁵, T.N. Addy⁵⁶, J. Adelman¹⁷⁷, S. Adomeit⁹⁹, T. Adye¹³⁰, S. Aefsky²³, T. Agatonovic-Jovin¹³b, J.A. Aguilar-Saavedra¹²⁵b, b, M. Agustoni¹⁷, S.P. Ahlen²², A. Ahmad¹⁴⁹, F. Ahmadov⁶⁴, c, G. Aielli¹³⁴a,¹³⁴b, T.P.A. Åkesson⁸⁰, G. Akimoto¹⁵⁶, A.V. Akimov⁹⁵, M.A. Alam⁷⁶, 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, S.E. Allwood-Spiers⁵³, J. Almond⁸³, A. Aloisio¹⁰³a,¹⁰³b, R. Alon¹⁷³, A. Alonso³⁶, F. Alonso⁷⁰, A. Altheimer³⁵, B. Alvarez Gonzalez⁸⁹, M.G. Alviggi¹⁰³a,¹⁰³b, K. Amako⁶⁵, Y. Amaral Coutinho²⁴a, C. Amelung²³, V.V. Ammosov¹²⁹,*, S.P. Amor Dos Santos¹²⁵a, A. Amorim¹²⁵a, d, S. Amoroso⁴⁸, N. Amram¹⁵⁴, G. Amundsen²³, C. Anastopoulos³⁰, L.S. Ancu¹⁷, N. Andari³⁰, T. Andeen³⁵, C.F. Anders⁵⁸b, G. Anders⁵⁸a, K.J. Anderson³¹, A. Andreazza⁹⁰a,⁹⁰b, V. Andrei⁵⁸a, X.S. Anduaga⁷⁰, S. Angelidakis⁹, 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, e, G. Arabidze⁸⁹, I. Aracena¹⁴⁴, Y. Arai⁶⁵, A.T.H. Arce⁴⁵, J-F. Arguin⁹⁴, S. Argyropoulos⁴², E. Arik¹⁹a,*, M. Arik¹⁹a, A.J. Armbruster⁸⁸, O. Arnaez⁸², V. Arnal⁸¹, O. Arslan²¹, A. Artamonov⁹⁶, G. Artoni²³, S. Asai¹⁵⁶, N. Asbah⁹⁴, S. Ask²⁸, B. Åsman¹⁴⁷a,¹⁴⁷b, L. Asquith⁶, K. Assamagan²⁵, R. Astalos¹⁴⁵a, A. Astbury¹⁷⁰, M. Atkinson¹⁶⁶, N.B. Atlay¹⁴², B. Auerbach⁶, E. Auge¹¹⁶, K. Augsten¹²⁷, M. Aurousseau¹⁴⁶b, G. Avolio³⁰, G. Azuelos⁹⁴, f, Y. Azuma¹⁵⁶, M.A. Baak³⁰, C. Bacci¹³⁵a,¹³⁵b, A.M. Bach¹⁵, H. Bachacou¹³⁷, K. Bachas¹⁵⁵, M. Backes³⁰, M. Backhaus²¹, J. Backus Mayes¹⁴⁴, E. Badescu²⁶a, P. Bagiacchi¹³³a,¹³³b, P. Bagnaia¹³³a,¹³³b, Y. Bai³³a, D.C. Bailey¹⁵⁹, T. Bain³⁵, J.T. Baines¹³⁰, O.K. Baker¹⁷⁷, S. Baker⁷⁷, P. Balek¹²⁸, F. Balli¹³⁷, E. Banas³⁹, Sw. Banerjee¹⁷⁴, D. Banfi³⁰, A. Bangert¹⁵¹, V. Bansal¹⁷⁰, H.S. Bansil¹⁸, L. Barak¹⁷³, S.P. Baranov⁹⁵, T. Barber⁴⁸, E.L. Barberio⁸⁷, D. Barberis⁵⁰a,⁵⁰b, M. Barbero⁸⁴, T. Barillari¹⁰⁰, M. Barisonzi¹⁷⁶, T. Barklow¹⁴⁴, N. Barlow²⁸, B.M. Barnett¹³⁰, R.M. Barnett¹⁵, A. Baroncelli¹³⁵a, G. Barone⁴⁹, A.J. Barr¹¹⁹, F. Barreiro⁸¹, J. Barreiro Guimarães da Costa⁵⁷, R. Bartoldus¹⁴⁴, A.E. Barton⁷¹, P. Bartos¹⁴⁵a, V. Bartsch¹⁵⁰, A. Bassalat¹¹⁶, A. Basye¹⁶⁶, R.L. Bates⁵³, L. Batkova¹⁴⁵a, J.R. Batley²⁸, M. Battistin³⁰, F. Bauer¹³⁷, H.S. Bawa¹⁴⁴, g, T. Beau⁷⁹, P.H. Beauchemin¹⁶², R. Beccherle¹²³a,¹²³b, P. Bechtle²¹, H.P. Beck¹⁷, K. Becker¹⁷⁶, S. Becker⁹⁹, M. Beckingham¹³⁹, 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, A. Belloni⁵⁷, O.L. Beloborodova¹⁰⁸, h, 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, E. Berglund¹⁰⁶, J. Beringer¹⁵, C. Bernard²², P. Bernat⁷⁷, C. Bernius⁷⁸, F.U. Bernlochner¹⁷⁰, T. Berry⁷⁶, P. Berta¹²⁸, C. Bertella⁸⁴, F. Bertolucci¹²³a,¹²³b, M.I. Besana⁹⁰a, G.J. Besjes¹⁰⁵, O. Bessidskaia¹⁴⁷a,¹⁴⁷b, N. Besson¹³⁷, 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. Bindi²⁰a,²⁰b, S. Binet¹¹⁶, A. Bingul¹⁹c, C. Bini¹³³a,¹³³b, B. Bittner¹⁰⁰, 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.R. Boddy¹¹⁹, M. Boehler⁴⁸, J. Boek¹⁷⁶, T.T. Boek¹⁷⁶, J.A. Bogaerts³⁰, A.G. Bogdanchikov¹⁰⁸, A. Bogouch⁹¹,*, C. Bohm¹⁴⁷a, J. Bohm¹²⁶, V. Boisvert⁷⁶, T. Bold³⁸a, V. Boldea²⁶a, A.S. Boldyrev⁹⁸, N.M. Bolnet¹³⁷, 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. Bouchami⁹⁴, J. Boudreau¹²⁴, E.V. Bouhova-Thacker⁷¹, D. Boumediene³⁴, C. Bourdarios¹¹⁶, N. Bousson⁸⁴, S. Boutouil¹³⁶d, A. Boveia³¹, J. Boyd³⁰, I.R. Boyko⁶⁴, I. Bozovic-Jelisavcic¹³b, J. Bracinik¹⁸, P. Branchini¹³⁵a, 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. Brooijmans³⁵, T. Brooks⁷⁶, W.K. Brooks³²b, J. Brosamer¹⁵, E. Brost¹¹⁵, G. Brown⁸³, J. Brown⁵⁵, P.A. Bruckman de Renstrom³⁹, D. Bruncko¹⁴⁵b, R. Bruneliere⁴⁸, S. Brunet⁶⁰, A. Bruni²⁰a, G. Bruni²⁰a, M. Bruschi²⁰a, L. Bryngemark⁸⁰, T. Buanes¹⁴, Q. Buat⁵⁵, F. Bucci⁴⁹, P. Buchholz¹⁴², R.M. Buckingham¹¹⁹, A.G. Buckley⁴⁶, S.I. Buda²⁶a, I.A. Budagov⁶⁴, B. Budick¹⁰⁹, F. Buehrer⁴⁸, L. Bugge¹¹⁸, M.K. Bugge¹¹⁸, O. Bulekov⁹⁷, A.C. Bundock⁷³, M. Bunse⁴³, H. Burckhart³⁰, S. Burdin⁷³, B. Burghgrave¹⁰⁷, S. Burke¹³⁰, I. Burmeister⁴³, E. Busato³⁴, V. Büscher⁸², P. Bussey⁵³, C.P. Buszello¹⁶⁷, B. Butler⁵⁷, J.M. Butler²², A.I. Butt³, C.M. Buttar⁵³,
J.M. Butterworth<sup>77</sup>, W. Buttinger<sup>28</sup>, A. Buzatu<sup>53</sup>, M. Byszewski<sup>10</sup>, S. Cabrera Urbán<sup>168</sup>, D. Caforio<sup>20a,20b</sup>, O. Cakir<sup>4a</sup>, P. Calafiura<sup>15</sup>, G. Calderini<sup>79</sup>, P. Calfayan<sup>99</sup>, R. Calkins<sup>107</sup>, L.P. Caloba<sup>24a</sup>, R. Caloi<sup>133a,133b</sup>, D. Calvet<sup>34</sup>, S. Calvet<sup>34</sup>, R. Camacho Toro<sup>49</sup>, P. Camarri<sup>134a,134b</sup>, D. Cameron<sup>118</sup>, L.M. Caminada<sup>15</sup>, R. Caminal Armadans<sup>12</sup>, S. Campana<sup>30</sup>, M. Campanelli<sup>77</sup>, A. Campoverde<sup>149</sup>, V. Canale<sup>103a,103b</sup>, F. Canelli<sup>31</sup>, A. Canepa<sup>160a</sup>, J. Cantero<sup>81</sup>, R. Cantrill<sup>76</sup>, T. Cao<sup>40</sup>, M.D.M. Capeans Garrido<sup>30</sup>, I. Caprini<sup>26a</sup>, M. Caprini<sup>26a</sup>, M. Capua<sup>37a,37b</sup>, R. Caputo<sup>82</sup>, R. Cardarelli<sup>134a</sup>, T. Carli<sup>30</sup>, G. Carlino<sup>103a</sup>, L. Carminati<sup>90a,90b</sup>, S. Caron<sup>105</sup>, E. Carquin<sup>32a</sup>, G.D. Carrillo-Montoya<sup>146c</sup>, A.A. Carter<sup>75</sup>, J.R. Carter<sup>28</sup>, J. Carvalho<sup>125a,i</sup>, D. Casadei<sup>77</sup>, M.P. Casado<sup>12</sup>, E. Castaneda-Miranda<sup>146b</sup>, A. Castelli<sup>106</sup>, V. Castillo Gimenez<sup>168</sup>, N.F. Castro<sup>125a</sup>, P. Catastini<sup>57</sup>, A. Catinaccio<sup>30</sup>, J.R. Catmore<sup>71</sup>, A. Cattai<sup>30</sup>, G. Cattani<sup>134a,134b</sup>, S. Caughron<sup>89</sup>, V. Cavaliere<sup>166</sup>, D. Cavalli<sup>90a</sup>, M. Cavalli-Sforza<sup>12</sup>, V. Cavasinni<sup>123a,123b</sup>, F. Ceradini<sup>135a,135b</sup>, B. Cerio<sup>45</sup>, K. Cerny<sup>128</sup>, A.S. Cerqueira<sup>24b</sup>, A. Cerri<sup>150</sup>, L. Cerrito<sup>75</sup>, F. Cerutti<sup>15</sup>, M. Cerv<sup>30</sup>, A. Cervelli<sup>17</sup>, S.A. Cetin<sup>19b</sup>, A. Chafaq<sup>136a</sup>, D. Chakraborty<sup>107</sup>, I. Chalupkova<sup>128</sup>, K. Chan<sup>3</sup>, P. Chang<sup>166</sup>, B. Chapleau<sup>86</sup>, J.D. Chapman<sup>28</sup>, D. Charfeddine<sup>116</sup>, D.G. Charlton<sup>18</sup>, V. Chavda<sup>83</sup>, C.A. Chavez Barajas<sup>30</sup>, S. Cheatham<sup>86</sup>, S. Chekanov<sup>6</sup>, S.V. Chekulaev<sup>160a</sup>, G.A. Chelkov<sup>64</sup>, M.A. Chelstowska<sup>88</sup>, C. Chen<sup>63</sup>, H. Chen<sup>25</sup>, K. Chen<sup>149</sup>, L. Chen<sup>33d,j</sup>, S. Chen<sup>33c</sup>, X. Chen<sup>146c</sup>, Y. Chen<sup>35</sup>, H.C. Cheng<sup>88</sup>, Y. Cheng<sup>31</sup>, A. Cheplakov<sup>64</sup>, R. Cherkaoui El Moursli<sup>136e</sup>, V. Chernyatin<sup>25,*</sup>, E. Cheu<sup>7</sup>, L. Chevalier<sup>137</sup>, V. Chiarella<sup>47</sup>, G. Chiefari<sup>103a,103b</sup>, J.T. Childers<sup>30</sup>, A. Chilingarov<sup>71</sup>, G. Chiodini<sup>72a</sup>, A.S. Chisholm<sup>18</sup>, R.T. Chislett<sup>77</sup>, A. Chitan<sup>26a</sup>, M.V. Chizhov<sup>64</sup>, S. Chouridou<sup>9</sup>, B.K.B. Chow<sup>99</sup>, I.A. Christidi<sup>77</sup>, D. Chromek-Burckhart<sup>30</sup>, M.L. Chu<sup>152</sup>, J. Chudoba<sup>126</sup>, G. Ciapetti<sup>133a,133b</sup>, A.K. Ciftci<sup>4a</sup>, R. Ciftci<sup>4a</sup>, D. Cinca<sup>62</sup>, V. Cindro<sup>74</sup>, A. Ciocio<sup>15</sup>, P. Cirkovic<sup>13b</sup>, Z.H. Citron<sup>173</sup>, M. Citterio<sup>90a</sup>, M. Ciubancan<sup>26a</sup>, A. Clark<sup>49</sup>, P.J. Clark<sup>46</sup>, R.N. Clarke<sup>15</sup>, W. Cleland<sup>124</sup>, J.C. Clemens<sup>84</sup>, B. Clement<sup>55</sup>, C. Clement<sup>147a,147b</sup>, Y. Coadou<sup>84</sup>, M. Cobal<sup>165a,165c</sup>, A. Coccaro<sup>139</sup>, J. Cochran<sup>63</sup>, L. Coffey<sup>23</sup>, J.G. Cogan<sup>144</sup>, J. Coggeshall<sup>166</sup>, B. Cole<sup>35</sup>, S. Cole<sup>107</sup>, A.P. Colijn<sup>106</sup>, C. Collins-Tooth<sup>53</sup>, J. Collot<sup>55</sup>, T. Colombo<sup>58c</sup>, G. Colon<sup>85</sup>, G. Compostella<sup>100</sup>, P. Conde Muiño<sup>125a</sup>, E. Coniavitis<sup>167</sup>, M.C. Conidi<sup>12</sup>, I.A. Connelly<sup>76</sup>, S.M. Consonni<sup>90a,90b</sup>, V. Consorti<sup>48</sup>, S. Constantinescu<sup>26a</sup>, C. Conta<sup>120a,120b</sup>, G. Conti<sup>57</sup>, F. Conventi<sup>103a,k</sup>, M. Cooke<sup>15</sup>, B.D. Cooper<sup>77</sup>, A.M. Cooper-Sarkar<sup>119</sup>, N.J. Cooper-Smith<sup>76</sup>, K. Copic<sup>15</sup>, T. Cornelissen<sup>176</sup>, M. Corradi<sup>20a</sup>, F. Corriveau<sup>86,l</sup>, A. Corso-Radu<sup>164</sup>, A. Cortes-Gonzalez<sup>12</sup>, G. Cortiana<sup>100</sup>, G. Costa<sup>90a</sup>, M.J. Costa<sup>168</sup>, R. Costa Batalha Pedro<sup>125a</sup>, D. Costanzo<sup>140</sup>, D. Côté<sup>8</sup>, G. Cottin<sup>32a</sup>, G. Cowan<sup>76</sup>, B.E. Cox<sup>83</sup>, K. Cranmer<sup>109</sup>, G. Cree<sup>29</sup>, S. Crépé-Renaudin<sup>55</sup>, F. Crescioli<sup>79</sup>, M. Crispin Ortuzar<sup>119</sup>, M. Cristinziani<sup>21</sup>, G. Crosetti<sup>37a,37b</sup>, C.-M. Cuciuc<sup>26a</sup>, C. Cuenca Almenar<sup>177</sup>, T. Cuhadar Donszelmann<sup>140</sup>, J. Cummings<sup>177</sup>, M. Curatolo<sup>47</sup>, C. Cuthbert<sup>151</sup>, H. Czirr<sup>142</sup>, P. Czodrowski<sup>3</sup>, Z. Czyczula<sup>177</sup>, S. D'Auria<sup>53</sup>, M. D'Onofrio<sup>73</sup>, A. D'Orazio<sup>133a,133b</sup>, M.J. Da Cunha Sargedas De Sousa<sup>125a</sup>, C. Da Via<sup>83</sup>, W. Dabrowski<sup>38a</sup>, A. Dafinca<sup>119</sup>, T. Dai<sup>88</sup>, F. Dallaire<sup>94</sup>, C. Dallapiccola<sup>85</sup>, M. Dam<sup>36</sup>, A.C. Daniells<sup>18</sup>, M. Dano Hoffmann<sup>36</sup>, V. Dao<sup>105</sup>, G. Darbo<sup>50a</sup>, G.L. Darlea<sup>26c</sup>, S. Darmora<sup>8</sup>, J.A. Dassoulas<sup>42</sup>, W. Davey<sup>21</sup>, C. David<sup>170</sup>, T. Davidek<sup>128</sup>, E. Davies<sup>119,e</sup>, M. Davies<sup>94</sup>, O. Davignon<sup>79</sup>, A.R. Davison<sup>77</sup>, Y. Davygora<sup>58a</sup>, E. Dawe<sup>143</sup>, I. Dawson<sup>140</sup>, R.K. Daya-Ishmukhametova<sup>23</sup>, K. De<sup>8</sup>, R. de Asmundis<sup>103a</sup>, S. De Castro<sup>20a,20b</sup>, S. De Cecco<sup>79</sup>, J. de Graat<sup>99</sup>, N. De Groot<sup>105</sup>, P. de Jong<sup>106</sup>, C. De La Taille<sup>116</sup>, H. De la Torre<sup>81</sup>, F. De Lorenzi<sup>63</sup>, L. De Nooij<sup>106</sup>, D. De Pedis<sup>133a</sup>, A. De Salvo<sup>133a</sup>, U. De Sanctis<sup>165a,165c</sup>, A. De Santo<sup>150</sup>, J.B. De Vivie De Regie<sup>116</sup>, G. De Zorzi<sup>133a,133b</sup>, W.J. Dearnaley<sup>71</sup>, R. Debbe<sup>25</sup>, C. Debenedetti<sup>46</sup>, B. Dechenaux<sup>55</sup>, D.V. Dedovich<sup>64</sup>, J. Degenhardt<sup>121</sup>, I. Deigaard<sup>106</sup>, J. Del Peso<sup>81</sup>, T. Del Prete<sup>123a,123b</sup>, T. Delemontex<sup>55</sup>, F. Deliot<sup>137</sup>, M. Deliyergiyev<sup>74</sup>, A. Dell'Acqua<sup>30</sup>, L. Dell'Asta<sup>22</sup>, M. Della Pietra<sup>103a,k</sup>, D. della Volpe<sup>49</sup>, M. Delmastro<sup>5</sup>, P.A. Delsart<sup>55</sup>, C. Deluca<sup>106</sup>, S. Demers<sup>177</sup>, M. Demichev<sup>64</sup>, A. Demilly<sup>79</sup>, B. Demirkoz<sup>12,m</sup>, S.P. Denisov<sup>129</sup>, D. Derendarz<sup>39</sup>, J.E. Derkaoui<sup>136d</sup>, F. Derue<sup>79</sup>, P. Dervan<sup>73</sup>, K. Desch<sup>21</sup>, P.O. Deviveiros<sup>106</sup>, A. Dewhurst<sup>130</sup>, S. Dhaliwal<sup>106</sup>, A. Di Ciaccio<sup>134a,134b</sup>, L. Di Ciaccio<sup>5</sup>, C. Di Donato<sup>103a,103b</sup>, A. Di Girolamo<sup>30</sup>, B. Di Girolamo<sup>30</sup>, A. Di Mattia<sup>153</sup>, B. Di Micco<sup>135a,135b</sup>, R. Di Nardo<sup>47</sup>, A. Di Simone<sup>48</sup>, R. Di Sipio<sup>20a,20b</sup>, D. Di Valentino<sup>29</sup>, M.A. Diaz<sup>32a</sup>, E.B. Diehl<sup>88</sup>, J. Dietrich<sup>42</sup>, T.A. Dietzsch<sup>58a</sup>, S. Diglio<sup>87</sup>, A. Dimitrievska<sup>13a</sup>, K. Dindar Yagci<sup>40</sup>, J. Dingfelder<sup>21</sup>, C. Dionisi<sup>133a,133b</sup>, P. Dita<sup>26a</sup>, S. Dita<sup>26a</sup>, F. Dittus<sup>30</sup>, F. Djama<sup>84</sup>, T. Djobava<sup>51b</sup>, M.A.B. do Vale<sup>24c</sup>, A. Do Valle Wemans<sup>125a,n</sup>, T.K.O. Doan<sup>5</sup>, D. Dobos<sup>30</sup>, E. Dobson<sup>77</sup>, C. Doglioni<sup>49</sup>, T. Doherty<sup>53</sup>, T. Dohmae<sup>156</sup>, J. Dolejsi<sup>128</sup>, Z. Dolezal<sup>128</sup>, B.A. Dolgoshein<sup>97,*</sup>, M. Donadelli<sup>24d</sup>, S. Donati<sup>123a,123b</sup>, P. Dondero<sup>120a,120b</sup>, J. Donini<sup>34</sup>, J. Dopke<sup>30</sup>, A. Doria<sup>103a</sup>, A. Dos Anjos<sup>174</sup>, A. Dotti<sup>123a,123b</sup>, M.T. Dova<sup>70</sup>, A.T. Doyle<sup>53</sup>, M. Dris<sup>10</sup>, J. Dubbert<sup>88</sup>, S. Dube<sup>15</sup>, E. Dubreuil<sup>34</sup>, E. Duchovni<sup>173</sup>, G. Duckeck<sup>99</sup>, O.A. Ducu<sup>26a</sup>, D. Duda<sup>176</sup>, A. Dudarev<sup>30</sup>, F. Dudziak<sup>63</sup>, L. Duflot<sup>116</sup>, L. Duguid<sup>76</sup>, M. Dührssen<sup>30</sup>, M. Dunford<sup>58a</sup>, H. Duran Yildiz<sup>4a</sup>, M. Düren<sup>52</sup>, M. Dwuznik<sup>38a</sup>, J. Ebke<sup>99</sup>, W. Edson<sup>2</sup>, C.A. Edwards<sup>76</sup>, N.C. Edwards<sup>46</sup>, W. Ehrenfeld<sup>21</sup>, T. Eifert<sup>144</sup>, G. Eigen<sup>14</sup>, K. Einsweiler<sup>15</sup>, T. Ekelof<sup>167</sup>, M. El Kacimi<sup>136c</sup>, M. Ellert<sup>167</sup>, S. Elles<sup>5</sup>, F. Ellinghaus<sup>82</sup>, K. Ellis<sup>75</sup>, N. Ellis<sup>30</sup>, J. Elmsheuser<sup>99</sup>, M. Elsing<sup>30</sup>, D. Emeliyanov<sup>130</sup>, Y. Enari<sup>156</sup>, O.C. Endner<sup>82</sup>, M. Endo<sup>117</sup>, R. Engelmann<sup>149</sup>, J. Erdmann<sup>177</sup>, A. Ereditato<sup>17</sup>, D. Eriksson<sup>147a</sup>, G. Ernis<sup>176</sup>, J. Ernst<sup>2</sup>, M. Ernst<sup>25</sup>, J. Ernwein<sup>137</sup>, D. Errede<sup>166</sup>, S. Errede<sup>166</sup>, E. Ertel<sup>82</sup>, M. Escalier<sup>116</sup>, H. Esch<sup>43</sup>, C. Escobar<sup>124</sup>, X. Espinal Curull<sup>12</sup>, B. Esposito<sup>47</sup>, F. Etienne<sup>84</sup>, A.I. Etienvre<sup>137</sup>, E. Etzion<sup>154</sup>, D. Evangelakou<sup>54</sup>, H. Evans<sup>60</sup>, L. Fabbri<sup>20a,20b</sup>
G. Facini³⁰, R.M. Fakhrutdinov¹²⁹, S. Falciano¹³³a, Y. Fang³³a, M. Fanti⁹⁰a,⁹⁰b, A. Farbin⁸, A. Farilla¹³⁵a, T. Farooque¹², S. Farrell¹⁶⁴, S.M. Farrington¹⁷¹, P. Farthouat³⁰, F. Fassi¹⁶⁸, P. Fassnacht³⁰, D. Fassouliotis⁹, B. Fatholahzadeh¹⁵⁹, A. Favareto⁵⁰a,⁵⁰b, L. Fayard¹¹⁶, P. Federic¹⁴⁵a, O.L. Fedin¹²², W. Fedorko¹⁶⁹, M. Fehling-Kaschek⁴⁸, S. Feigl³⁰, L. Feligioni⁸⁴, C. Feng³³d, E.J. Feng⁶, H. Feng⁸⁸, A.B. Fenyuk¹²⁹, S. Fernandez Perez³⁰, W. Fernando⁶, S. Ferrag⁵³, J. Ferrando⁵³, V. Ferrara⁴², 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. Finelli⁴⁵, M.C.N. Fiolhais¹²⁵a,⁴, L. Fiorini¹⁶⁸, A. Firan⁴⁰, J. Fischer¹⁷⁶, M.J. Fisher¹¹⁰, E.A. Fitzgerald²³, M. Flechl⁴⁸, I. Fleck¹⁴², P. Fleischmann¹⁷⁵, S. Fleischmann¹⁷⁶, G.T. Fletcher¹⁴⁰, G. Fletcher⁷⁵, T. Flick¹⁷⁶, A. Floderus⁸⁰, L.R. Flores Castillo¹⁷⁴, A.C. Florez Bustos¹⁶⁰b, M.J. Flowerdew¹⁰⁰, A. Formica¹³⁷, A. Forti⁸³, D. Fortin¹⁶⁰a, D. Fournier¹¹⁶, H. Fox⁷¹, P. Francavilla¹², M. Franchini²⁰a,²⁰b, S. Franchino³⁰, D. Francis³⁰, M. Franklin⁵⁷, S. Franz⁶¹, M. Fraternali¹²⁰a,¹²⁰b, S. Fratina¹²¹, S.T. French²⁸, C. Friedrich⁴², F. Friedrich⁴⁴, D. Froidevaux³⁰, J.A. Frost²⁸, C. Fukunaga¹⁵⁷, E. Fullana Torregrosa¹²⁸, B.G. Fulsom¹⁴⁴, J. Fuster¹⁶⁸, C. Gabaldon⁵⁵, O. Gabizon¹⁷³, A. Gabrielli²⁰a,²⁰b, A. Gabrielli¹³³a,¹³³b, S. Gadatsch¹⁰⁶, T. Gadfort²⁵, S. Gadomski⁴⁹, G. Gagliardi⁵⁰a,⁵⁰b, P. Gagnon⁶⁰, C. Galea¹⁰⁵, B. Galhardo¹²⁵a, E.J. Gallas¹¹⁹, V. Gallo¹⁷, B.J. Gallop¹³⁰, P. Gallus¹²⁷, G. Galster³⁶, K.K. Gan¹¹⁰, R.P. Gandrajula⁶², J. Gao³³b,⁴, Y.S. Gao¹⁴⁴,⁹, 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. Gaudío¹²⁰a, B. Gaur¹⁴², L. Gauthier⁹⁴, P. Gauzzi¹³³a,¹³³b, I.L. Gavrilenko⁹⁵, C. Gay¹⁶⁹, G. Gaycken²¹, E.N. Gazis¹⁰, P. Ge³³d,⁰, 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. Ghobbane³⁴, 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, A.R. Gillman¹³⁰, D.M. Gingrich³, f, N. Giokaris⁹, M.P. Giordani¹⁶⁵c, R. Giordano¹⁰³a,¹⁰³b, F.M. Giorgi¹⁶, P. Giovannini¹⁰⁰, P.F. Giraud¹³⁷, D. Giugni⁹⁰a, C. Giuliani⁴⁸, M. Giunta⁹⁴, B.K. Gjelsten¹¹⁸, I. Gkialas¹⁵⁵, p, L.K. Gladilin⁹⁸, C. Glasman⁸¹, J. Glatzer²¹, 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, d, L.S. Gomez Fajardo⁴², R. Gonçalo⁷⁶, J. Goncalves Pinto Firmino Da Costa⁴², L. Gonella²¹, S. González de la Hoz¹⁶⁸, G. Gonzalez Parra¹², M.L. Gonzalez Silva²⁷, S. Gonzalez-Sevilla⁴⁹, L. Goossens³⁰, P.A. Gorbounov⁹⁶, H.A. Gordon²⁵, I. Gorelov¹⁰⁴, G. Gorfine¹⁷⁶, 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, F. Grancagnolo⁷²a, S. Grancagnolo¹⁶, V. Grassi¹⁴⁹, V. Gratchev¹²², H.M. Gray³⁰, J.A. Gray¹⁴⁹, E. Graziani¹³⁵a, O.G. Grebenyuk¹²², Z.D. Greenwood⁷⁸, q, K. Gregersen³⁶, I.M. Gregor⁴², P. Grenier¹⁴⁴, J. Griffiths⁸, N. Grigalashvili⁶⁴, A.A. Grillo¹³⁸, K. Grimm⁷¹, S. Grinstein¹², r, 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, K. Grybel¹⁴², L. Guan³³b, F. Guescini⁴⁹, D. Guest¹⁷⁷, O. Gueta¹⁵⁴, C. Guicheney³⁴, 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, P. Haefner²¹, S. Hageboeck²¹, Z. Hajduk³⁹, H. Hakobyan¹⁷⁸, M. Haleem⁴², D. Hall¹¹⁹, G. Halladjian⁸⁹, K. Hamacher¹⁷⁶, P. Hamal¹¹⁴, K. Hamano⁸⁷, M. Hamer⁵⁴, A. Hamilton¹⁴⁶a, s, S. Hamilton¹⁶², L. Han³³b, K. Hanagaki¹¹⁷, K. Hanawa¹⁵⁶, M. Hance¹⁵, P. Hanke⁵⁸a, J.R. Hansen³⁶, J.B. Hansen³⁶, J.D. Hansen³⁶, P.H. Hansen³⁶, P. Hansson¹⁴⁴, K. Hara¹⁶¹, A.S. Hard¹⁷⁴, T. Harenberg¹⁷⁶, S. Harkusha⁹¹, D. Harper⁸⁸, R.D. Harrington⁴⁶, O.M. Harris¹³⁹, P.F. Harrison¹⁷¹, F. Hartjes¹⁰⁶, A. Harvey⁵⁶, S. Hasegawa¹⁰², Y. Hasegawa¹⁴¹, S. Hassani¹³⁷, S. Haug¹⁷, M. Hauschild³⁰, R. Hauser⁸⁹, M. Havranek²¹, 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, S. Heisterkamp³⁶, J. Hejbal¹²⁶, L. Hellyar²², C. Heller⁹⁹, M. Heller³⁰, S. Hellman¹⁴⁷a,¹⁴⁷b, D. Hellmich²¹, C. Helsens³⁰, J. Henderson¹¹⁹, R.C.W. Henderson⁷¹, 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, J.C. Hill²⁸, K.H. Hiller⁴², S. Hillert²¹, S.J. Hillier¹⁸, I. Hinchliffe¹⁵, E. Hines¹²¹, M. Hirose¹¹⁷, 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. Howarth⁸³, M. Hrabovsky¹¹⁴, I. Hristova¹⁶, J. Hrivnac¹¹⁶, T. Hryn'ova⁵, P.J. Hsu⁸², S.-C. Hsu¹³⁹, D. Hu³⁵, X. Hu²⁵, Y. Huang¹⁴⁶c, Z. Hubacek³⁰, F. Hubaut⁸⁴, F. Huegging²¹,
A. Huettmann<sup>42</sup>, T.B. Huffman<sup>119</sup>, E.W. Hughes<sup>35</sup>, G. Hughes<sup>71</sup>, M. Huhtinen<sup>30</sup>, T.A. Hülsing<sup>82</sup>, M. Hurwitz<sup>15</sup>, N. Huseynov<sup>64,c</sup>, J. Huston<sup>89</sup>, J. Huth<sup>57</sup>, G. Iacobucci<sup>49</sup>, G. Iakovidis<sup>10</sup>, I. Ibragimov<sup>142</sup>, L. Iconomidou-Fayard<sup>116</sup>, J. Idarraga<sup>116</sup>, E. Ideal<sup>177</sup>, P. Iengo<sup>103a</sup>, O. Igonkina<sup>106</sup>, T. Iizawa<sup>172</sup>, Y. Ikegami<sup>65</sup>, K. Ikematsu<sup>142</sup>, M. Ikeno<sup>65</sup>, D. Iliadis<sup>155</sup>, N. Ilic<sup>159</sup>, Y. Inamaru<sup>66</sup>, T. Ince<sup>100</sup>, P. Ioannou<sup>9</sup>, M. Iodice<sup>135a</sup>, K. Iordanidou<sup>9</sup>, V. Ippolito<sup>133a,133b</sup>, A. Irles Quiles<sup>168</sup>, C. Isaksson<sup>167</sup>, M. Ishino<sup>67</sup>, M. Ishitsuka<sup>158</sup>, R. Ishmukhametov<sup>110</sup>, C. Issever<sup>119</sup>, S. Istin<sup>19a</sup>, J.M. Iturbe Ponce<sup>83</sup>, A.V. Ivashin<sup>129</sup>, W. Iwanski<sup>39</sup>, H. Iwasaki<sup>65</sup>, J.M. Izen<sup>41</sup>, V. Izzo<sup>103a</sup>, B. Jackson<sup>121</sup>, J.N. Jackson<sup>73</sup>, M. Jackson<sup>73</sup>, P. Jackson<sup>1</sup>, M.R. Jaekel<sup>30</sup>, V. Jain<sup>2</sup>, K. Jakobs<sup>48</sup>, S. Jakobsen<sup>36</sup>, T. Jakoubek<sup>126</sup>, J. Jakubek<sup>127</sup>, D.O. Jamin<sup>152</sup>, D.K. Jana<sup>78</sup>, E. Jansen<sup>77</sup>, H. Jansen<sup>30</sup>, J. Janssen<sup>21</sup>, M. Janus<sup>171</sup>, G. Jarlskog<sup>80</sup>, L. Jeanty<sup>15</sup>, G.-Y. Jeng<sup>151</sup>, I. Jen-La Plante<sup>31</sup>, D. Jennens<sup>87</sup>, P. Jenni<sup>48,t</sup>, J. Jentzsch<sup>43</sup>, C. Jeske<sup>171</sup>, S. Jézéquel<sup>5</sup>, M.K. Jha<sup>20a</sup>, H. Ji<sup>174</sup>, W. Ji<sup>82</sup>, J. Jia<sup>149</sup>, Y. Jiang<sup>33b</sup>, M. Jimenez Belenguer<sup>42</sup>, S. Jin<sup>33a</sup>, A. Jinaru<sup>26a</sup>, O. Jinnouchi<sup>158</sup>, M.D. Joergensen<sup>36</sup>, D. Joffe<sup>40</sup>, K.E. Johansson<sup>147a</sup>, P. Johansson<sup>140</sup>, K.A. Johns<sup>7</sup>, K. Jon-And<sup>147a,147b</sup>, G. Jones<sup>171</sup>, R.W.L. Jones<sup>71</sup>, T.J. Jones<sup>73</sup>, P.M. Jorge<sup>125a</sup>, K.D. Joshi<sup>83</sup>, J. Jovicevic<sup>148</sup>, X. Ju<sup>174</sup>, C.A. Jung<sup>43</sup>, R.M. Jungst<sup>30</sup>, P. Jussel<sup>61</sup>, A. Juste Rozas<sup>12,r</sup>, M. Kaci<sup>168</sup>, A. Kaczmarska<sup>39</sup>, M. Kado<sup>116</sup>, H. Kagan<sup>110</sup>, M. Kagan<sup>144</sup>, E. Kajomovitz<sup>45</sup>, S. Kama<sup>40</sup>, N. Kanaya<sup>156</sup>, M. Kaneda<sup>30</sup>, S. Kaneti<sup>28</sup>, T. Kanno<sup>158</sup>, V.A. Kantserov<sup>97</sup>, J. Kanzaki<sup>65</sup>, B. Kaplan<sup>109</sup>, A. Kapliy<sup>31</sup>, D. Kar<sup>53</sup>, K. Karakostas<sup>10</sup>, N. Karastathis<sup>10</sup>, M. Karnevskiy<sup>82</sup>, S.N. Karpov<sup>64</sup>, K. Karthik<sup>109</sup>, V. Kartvelishvili<sup>71</sup>, A.N. Karyukhin<sup>129</sup>, L. Kashif<sup>174</sup>, G. Kasieczka<sup>58b</sup>, R.D. Kass<sup>110</sup>, A. Kastanas<sup>14</sup>, Y. Kataoka<sup>156</sup>, A. Katre<sup>49</sup>, J. Katzy<sup>42</sup>, V. Kaushik<sup>7</sup>, K. Kawagoe<sup>69</sup>, T. Kawamoto<sup>156</sup>, G. Kawamura<sup>54</sup>, S. Kazama<sup>156</sup>, V.F. Kazanin<sup>108</sup>, M.Y. Kazarinov<sup>64</sup>, R. Keeler<sup>170</sup>, P.T. Keener<sup>121</sup>, R. Kehoe<sup>40</sup>, M. Keil<sup>54</sup>, J.S. Keller<sup>139</sup>, H. Keoshkerian<sup>5</sup>, O. Kepka<sup>126</sup>, B.P. Kerševan<sup>74</sup>, S. Kersten<sup>176</sup>, K. Kessoku<sup>156</sup>, J. Keung<sup>159</sup>, F. Khalil-zada<sup>11</sup>, H. Khandanyan<sup>147a,147b</sup>, A. Khanov<sup>113</sup>, D. Kharchenko<sup>64</sup>, A. Khodinov<sup>97</sup>, A. Khomich<sup>58a</sup>, T.J. Khoo<sup>28</sup>, G. Khoriauli<sup>21</sup>, A. Khoroshilov<sup>176</sup>, V. Khovanskiy<sup>96</sup>, E. Khramov<sup>64</sup>, J. Khubua<sup>51b</sup>, H. Kim<sup>147a,147b</sup>, S.H. Kim<sup>161</sup>, N. Kimura<sup>172</sup>, O. Kind<sup>16</sup>, B.T. King<sup>73</sup>, M. King<sup>168</sup>, R.S.B. King<sup>119</sup>, S.B. King<sup>169</sup>, J. Kirk<sup>130</sup>, A.E. Kiryunin<sup>100</sup>, T. Kishimoto<sup>66</sup>, D. Kisielewska<sup>38a</sup>, T. Kitamura<sup>66</sup>, T. Kittelmann<sup>124</sup>, K. Kiuchi<sup>161</sup>, E. Kladiva<sup>145b</sup>, M. Klein<sup>73</sup>, U. Klein<sup>73</sup>, K. Kleinknecht<sup>82</sup>, P. Klimek<sup>147a,147b</sup>, A. Klimentov<sup>25</sup>, R. Klingenberg<sup>43</sup>, J.A. Klinger<sup>83</sup>, E.B. Klinkby<sup>36</sup>, T. Klioutchnikova<sup>30</sup>, P.F. Klok<sup>105</sup>, E.-E. Kluge<sup>58a</sup>, P. Kluit<sup>106</sup>, S. Kluth<sup>100</sup>, E. Kneringer<sup>61</sup>, E.B.F.G. Knoops<sup>84</sup>, A. Knue<sup>53</sup>, T. Kobayashi<sup>156</sup>, M. Kobel<sup>44</sup>, M. Kocian<sup>144</sup>, P. Kodys<sup>128</sup>, S. Koenig<sup>82</sup>, P. Koevesarki<sup>21</sup>, T. Koffas<sup>29</sup>, E. Koffeman<sup>106</sup>, L.A. Kogan<sup>119</sup>, S. Kohlmann<sup>176</sup>, Z. Kohout<sup>127</sup>, T. Kohriki<sup>65</sup>, T. Koi<sup>144</sup>, H. Kolanoski<sup>16</sup>, I. Koletsou<sup>5</sup>, J. Koll<sup>89</sup>, A.A. Komar<sup>95,*</sup>, Y. Komori<sup>156</sup>, T. Kondo<sup>65</sup>, K. Köneke<sup>48</sup>, A.C. König<sup>105</sup>, T. Kono<sup>65,u</sup>, R. Konoplich<sup>109,v</sup>, N. Konstantinidis<sup>77</sup>, R. Kopeliansky<sup>153</sup>, S. Koperny<sup>38a</sup>, L. Köpke<sup>82</sup>, A.K. Kopp<sup>48</sup>, K. Korcyl<sup>39</sup>, K. Kordas<sup>155</sup>, A. Korn<sup>46</sup>, A.A. Korol<sup>108</sup>, I. Korolkov<sup>12</sup>, E.V. Korolkova<sup>140</sup>, V.A. Korotkov<sup>129</sup>, O. Kortner<sup>100</sup>, S. Kortner<sup>100</sup>, V.V. Kostyukhin<sup>21</sup>, S. Kotov<sup>100</sup>, V.M. Kotov<sup>64</sup>, A. Kotwal<sup>45</sup>, C. Kourkoumelis<sup>9</sup>, V. Kouskoura<sup>155</sup>, A. Koutsman<sup>160a</sup>, R. Kowalewski<sup>170</sup>, T.Z. Kowalski<sup>38a</sup>, W. Kozanecki<sup>137</sup>, A.S. Kozhin<sup>129</sup>, V. Kral<sup>127</sup>, V.A. Kramarenko<sup>98</sup>, G. Kramberger<sup>74</sup>, D. Krasnopevtsev<sup>97</sup>, M.W. Krasny<sup>79</sup>, A. Krasznahorkay<sup>30</sup>, J.K. Kraus<sup>21</sup>, A. Kravchenko<sup>25</sup>, S. Kreiss<sup>109</sup>, J. Kretzschmar<sup>73</sup>, K. Kreutzfeldt<sup>52</sup>, N. Krieger<sup>54</sup>, P. Krieger<sup>159</sup>, K. Kroeninger<sup>54</sup>, H. Kroha<sup>100</sup>, J. Kroll<sup>121</sup>, J. Kroseberg<sup>21</sup>, J. Krstic<sup>13a</sup>, U. Kruchonak<sup>64</sup>, H. Krüger<sup>21</sup>, T. Kruker<sup>17</sup>, N. Krumnack<sup>63</sup>, Z.V. Krumshteyn<sup>64</sup>, A. Kruse<sup>174</sup>, M.C. Kruse<sup>45</sup>, M. Kruskal<sup>22</sup>, T. Kubota<sup>87</sup>, S. Kuday<sup>4a</sup>, S. Kuehn<sup>48</sup>, A. Kugel<sup>58c</sup>, T. Kuhl<sup>42</sup>, V. Kukhtin<sup>64</sup>, Y. Kulchitsky<sup>91</sup>, S. Kuleshov<sup>32b</sup>, M. Kuna<sup>133a,133b</sup>, J. Kunkle<sup>121</sup>, A. Kupco<sup>126</sup>, H. Kurashige<sup>66</sup>, Y.A. Kurochkin<sup>91</sup>, R. Kurumida<sup>66</sup>, V. Kus<sup>126</sup>, E.S. Kuwertz<sup>148</sup>, M. Kuze<sup>158</sup>, J. Kvita<sup>143</sup>, A. La Rosa<sup>49</sup>, L. La Rotonda<sup>37a,37b</sup>, L. Labarga<sup>81</sup>, S. Lablak<sup>136a</sup>, C. Lacasta<sup>168</sup>, F. Lacava<sup>133a,133b</sup>, J. Lacey<sup>29</sup>, H. Lacker<sup>16</sup>, D. Lacour<sup>79</sup>, V.R. Lacuesta<sup>168</sup>, E. Ladygin<sup>64</sup>, R. Lafaye<sup>5</sup>, B. Laforge<sup>79</sup>, T. Lagouri<sup>177</sup>, S. Lai<sup>48</sup>, H. Laier<sup>58a</sup>, E. Laisne<sup>55</sup>, L. Lambourne<sup>77</sup>, C.L. Lampen<sup>7</sup>, W. Lampl<sup>7</sup>, E. Lançon<sup>137</sup>, U. Landgraf<sup>48</sup>, M.P.J. Landon<sup>75</sup>, V.S. Lang<sup>58a</sup>, C. Lange<sup>42</sup>, A.J. Lankford<sup>164</sup>, F. Lanni<sup>25</sup>, K. Lantzsch<sup>30</sup>, A. Lanza<sup>120a</sup>, S. Laplace<sup>79</sup>, C. Lapoire<sup>21</sup>, J.F. Laporte<sup>137</sup>, T. Lari<sup>90a</sup>, A. Larner<sup>119</sup>, M. Lassnig<sup>30</sup>, P. Laurelli<sup>47</sup>, V. Lavorini<sup>37a,37b</sup>, W. Lavrijsen<sup>15</sup>, P. Laycock<sup>73</sup>, B.T. Le<sup>55</sup>, O. Le Dortz<sup>79</sup>, E. Le Guirrie<sup>84</sup>, E. Le Menedeu<sup>12</sup>, T. LeCompte<sup>6</sup>, F. Ledroit-Guillon<sup>55</sup>, C.A. Lee<sup>152</sup>, H. Lee<sup>106</sup>, J.S.H. Lee<sup>117</sup>, S.C. Lee<sup>152</sup>, L. Lee<sup>177</sup>, G. Lefebvre<sup>79</sup>, M. Lefebvre<sup>170</sup>, F. Legger<sup>99</sup>, C. Leggett<sup>15</sup>, A. Lehan<sup>73</sup>, M. Lehmacher<sup>21</sup>, G. Lehmann Miotto<sup>30</sup>, X. Lei<sup>7</sup>, A.G. Leister<sup>177</sup>, M.A.L. Leite<sup>24d</sup>, R. Leitner<sup>128</sup>, D. Lellouch<sup>173</sup>, B. Lemmer<sup>54</sup>, K.J.C. Leney<sup>146c</sup>, T. Lenz<sup>106</sup>, G. Lenzen<sup>176</sup>, B. Lenzi<sup>30</sup>, R. Leone<sup>7</sup>, K. Leonhardt<sup>44</sup>, S. Leontsinis<sup>10</sup>, C. Leroy<sup>94</sup>, C.G. Lester<sup>28</sup>, C.M. Lester<sup>121</sup>, J. Levêque<sup>5</sup>, D. Levin<sup>88</sup>, L.J. Levinson<sup>173</sup>, A. Lewis<sup>119</sup>, G.H. Lewis<sup>109</sup>, A.M. Leyko<sup>21</sup>, M. Leyton<sup>16</sup>, B. Li<sup>33b,w</sup>, B. Li<sup>84</sup>, H. Li<sup>149</sup>, H.L. Li<sup>31</sup>, S. Li<sup>45</sup>, X. Li<sup>88</sup>, Z. Liang<sup>119,x</sup>, H. Liao<sup>34</sup>, B. Liberti<sup>134a</sup>, P. Lichard<sup>30</sup>, K. Lie<sup>166</sup>, J. Liebal<sup>21</sup>, W. Liebig<sup>14</sup>, C. Limbach<sup>21</sup>, A. Limosani<sup>87</sup>, M. Limper<sup>62</sup>, S.C. Lin<sup>152,y</sup>, F. Linde<sup>106</sup>, B.E. Lindquist<sup>149</sup>, J.T. Linnemann<sup>89</sup>, E. Lipeles<sup>121</sup>, A. Lipniacka<sup>14</sup>, M. Lisovyi<sup>42</sup>, T.M. Liss<sup>166</sup>, D. Lissauer<sup>25</sup>, A. Lister<sup>169</sup>, A.M. Litke<sup>138</sup>, B. Liu<sup>152</sup>, D. Liu<sup>152</sup>, J.B. Liu<sup>33b</sup>, K. Liu<sup>33b,z</sup>, L. Liu<sup>88</sup>, M. Liu<sup>45</sup>, M. Liu<sup>33b</sup>, Y. Liu<sup>33b</sup>, M. Livan<sup>120a,120b</sup>, S.S.A. Livermore<sup>119</sup>, A. Lleres<sup>55</sup>, J. Llorente Merino<sup>81</sup>, S.L. Lloyd<sup>75</sup>, F. Lo Sterzo<sup>152</sup>, E. Lobodzinska<sup>42</sup>, P. Loch<sup>7</sup>, W.S. Lockman<sup>138</sup>, T. Loddenkoetter<sup>21</sup>, F.K. Loebinger<sup>83</sup>, A.E. Loevschall-Jensen<sup>36</sup>, A. Loginov<sup>177</sup>, C.W. Loh<sup>169</sup>, T. Lohse<sup>16</sup>, K. Lohwasser<sup>48</sup>, M. Lokajicek<sup>126</sup>,
V.P. Lombardo⁵, J.D. Long⁸⁸, R.E. Long⁷¹, L. Lopes¹²⁵a, D. Lopez Mateos⁵⁷, B. Lopez Paredes¹⁴⁰, J. Lorenz⁹⁹, N. Lorenzo Martinez¹¹⁶, M. Losada¹⁶³, P. Loscutoff¹⁵, M.J. Losty¹⁶⁰a,*, X. Lou⁴¹, A. Lounis¹¹⁶, J. Love⁶, P.A. Love⁷¹, A.J. Lowe¹⁴⁴, g, F. Lu³³a, H.J. Lubatti¹³⁹, C. Luci¹³³a,¹³³b, A. Lucotte⁵⁵, D. Ludwig⁴², I. Ludwig⁴⁸, F. Luehring⁶⁰, W. Lukas⁶¹, L. Luminari¹³³a, J. Lundberg¹⁴⁷a,¹⁴⁷b, O. Lundberg¹⁴⁷a,¹⁴⁷b, B. Lund-Jensen¹⁴⁸, M. Lungwitz⁸², D. Lynn²⁵, R. Lysak¹²⁶, E. Lytken⁸⁰, H. Ma²⁵, L.L. Ma³³d, G. Maccarrone⁴⁷, A. Macchiolo¹⁰⁰, B. Maček⁷⁴, J. Machado Miguens¹²⁵a, D. Macina³⁰, R. Mackeprang³⁶, R. Madar⁴⁸, H.J. Maddocks⁷¹, W.F. Mader⁴⁴, A. Madsen¹⁶⁷, M. Maeno⁸, T. Maeno²⁵, L. Magnoni¹⁶⁴, E. Magradze⁵⁴, K. Mahboubi⁴⁸, J. Mahlstedt¹⁰⁶, S. Mahmoud⁷³, G. Mahout¹⁸, C. Maiani¹³⁷, C. Maidantchik²⁴a, A. Maio¹²⁵a,d, S. Majewski¹¹⁵, Y. Makida⁶⁵, N. Makovec¹¹⁶, P. Mal¹³⁷,aa, 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, A. Manfredini¹⁰⁰, L. Manhaes de Andrade Filho²⁴b, J.A. Manjarres Ramos¹³⁷, A. Mann⁹⁹, P.M. Manning¹³⁸, A. Manousakis-Katsikakis⁹, B. Mansoulie¹³⁷, R. Mantifel⁸⁶, L. Mapelli³⁰, L. March¹⁶⁸, J.F. Marchand²⁹, F. Marchese¹³⁴a,¹³⁴b, G. Marchiori⁷⁹, M. Marcisovsky¹²⁶, C.P. Marino¹⁷⁰, C.N. Marques¹²⁵a, F. Marroquim²⁴a, Z. Marshall¹⁵, L.F. Marti¹⁷, S. Marti-Garcia¹⁶⁸, B. Martin³⁰, B. Martin⁸⁹, J.P. Martin⁹⁴, T.A. Martin¹⁷¹, V.J. Martin⁴⁶, B. Martin dit Latour⁴⁹, H. Martinez¹³⁷, M. Martinez¹²,r, S. Martin-Haugh¹³⁰, A.C. Martyniuk⁷⁷, M. Marx¹³⁹, F. Marzano¹³³a, A. Marzin¹¹², L. Masetti⁸², T. Mashimo¹⁵⁶, R. Mashinistov⁹⁵, J. Masik⁸³, A.L. Maslennikov¹⁰⁸, I. Massa²⁰a,²⁰b, N. Massol⁵, P. Mastrandrea¹⁴⁹, A. Mastroberardino³⁷a,³⁷b, T. Masubuchi¹⁵⁶, H. Matsunaga¹⁵⁶, T. Matsushita⁶⁶, P. Mättig¹⁷⁶, S. Mättig⁴², J. Mattmann⁸², C. Mattravers¹¹⁹,e, J. Maurer⁸⁴, S.J. Maxfield⁷³, D.A. Maximov¹⁰⁸,h, 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. Mcfayden¹⁴⁰, G. Mchedlidze⁵⁴, T. Mclaughlan¹⁸, S.J. McMahon¹³⁰, R.A. McPherson¹⁷⁰,l, A. Meade⁸⁵, J. Mechnich¹⁰⁶, M. Mechtel¹⁷⁶, M. Medinnis⁴², S. Meehan³¹, R. Meera-Lebbai¹¹², S. Mehlhase³⁶, A. Mehta⁷³, K. Meier⁵⁸a, C. Meineck⁹⁹, B. Meirose⁸⁰, C. Melachrinos³¹, B.R. Mellado Garcia¹⁴⁶c, F. Meloni⁹⁰a,⁹⁰b, L. Mendoza Navas¹⁶³, 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,ab, J. Metcalfe²⁵, A.S. Mete¹⁶⁴, C. Meyer⁸², C. Meyer³¹, J-P. Meyer¹³⁷, J. Meyer³⁰, J. Meyer⁵⁴, R.P. Middleton¹³⁰, S. Migas⁷³, L. Mijović¹³⁷, G. Mikenberg¹⁷³, M. Mikestikova¹²⁶, M. Mikuž⁷⁴, D.W. Miller³¹, C. Mills⁵⁷, A. Milov¹⁷³, D.A. Milstead¹⁴⁷a,¹⁴⁷b, D. Milstein¹⁷³, A.A. Minaenko¹²⁹, M. Miñano Moya¹⁶⁸, 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, V. Moeller²⁸, S. Mohapatra³⁵, W. Mohr⁴⁸, S. Molander¹⁴⁷a,¹⁴⁷b, R. Moles-Valls¹⁶⁸, K. Mönig⁴², C. Monini⁵⁵, J. Monk³⁶, E. Monnier⁸⁴, J. Montejo Berlingen¹², F. Monticelli⁷⁰, S. Monzani²⁰a,²⁰b, R.W. Moore³, C. Mora Herrera⁴⁹, A. Moraes⁵³, N. Morange⁶², J. Morel⁵⁴, 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, R. Mount¹⁴⁴, E. Mountricha²⁵, S.V. Mouraviev⁹⁵,*, E.J.W. Moyse⁸⁵, S.G. 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,e, I. Mussche¹⁰⁶, E. Musto¹⁵³, A.G. Myagkov¹²⁹,ac, M. Myska¹²⁶, 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, A. Napier¹⁶², R. Narayan⁵⁸b, M. Nash⁷⁷,e, T. Nattermann²¹, T. Naumann⁴², G. Navarro¹⁶³, R. Nayyar⁷, H.A. Neal⁸⁸, P.Yu. Nechaeva⁹⁵, T.J. Neep⁸³, A. Negri¹²⁰a,¹²⁰b, G. Negri³⁰, M. Negrini²⁰a, S. Nektarijevic⁴⁹, A. Nelson¹⁶⁴, T.K. Nelson¹⁴⁴, S. Nemecek¹²⁶, P. Nemethy¹⁰⁹, A.A. Nepomuceno²⁴a, M. Nessi³⁰,ad, M.S. Neubauer¹⁶⁶, M. Neumann¹⁷⁶, A. Neusiedl⁸², R.M. Neves¹⁰⁹, P. Nevski²⁵, F.M. Newcomer¹²¹, P.R. Newman¹⁸, D.H. Nguyen⁶, V. Nguyen Thi Hong¹³⁷, R.B. Nickerson¹¹⁹, R. Nicolaidou¹³⁷, B. Nicquevert³⁰, J. Nielsen¹³⁸, N. Nikiforou³⁵, A. Nikiforov¹⁶, V. Nikolaenko¹²⁹,ac, 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, J. Novakova¹²⁸, M. Nozaki⁶⁵, L. Nozka¹¹⁴, K. Ntekas¹⁰, A.-E. Nuncio-Quiroz²¹, 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,f, H. Oberlack¹⁰⁰, J. Ocariz⁷⁹, A. Ochi⁶⁶, M.I. Ochoa⁷⁷, S. Oda⁶⁹, S. Odaka⁶⁵, H. Ogren⁶⁰, A. Oh⁸³, S.H. Oh⁴⁵, C.C. Ohm³⁰, 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, D. Olivito¹²¹, A. Olszewski³⁹, J. Olszowska³⁹, A. Onofre¹²⁵a,ae, P.U.E. Onyisi³¹,af, 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, S. Owen¹⁴⁰, V.E. Ozcan¹⁹a, N. Ozturk⁸, K. Pachal¹¹⁹, A. Pacheco Pages¹²,
C. Padilla Aranda¹², S. Pagan Griso¹⁵, E. Paganis¹⁴⁰, C. Pahl¹⁰⁰, F. Paige²⁵, P. Pais⁸⁵, K. Pajchel¹¹⁸,
G. Palacino¹⁶⁰b, S. Palestini³⁰, D. Pallin³⁴, A. Palma¹²⁵a, J.D. Palmer¹⁸, Y.B. Pan¹⁷⁴, E. Panagiotopoulou¹⁰,
J.G. Panduro Vazquez⁷⁶, P. Pani¹⁰⁶, N. Panikashvili⁸⁸, S. Panitkin²⁵, D. Pantea²⁶a, Th.D. Papadopoulou¹⁰,
K. Papageorgiou¹⁵⁵,p, 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. Pásztor⁴⁹,ag, S. Pataraia¹⁷⁶, N.D. Patel¹⁵¹, J.R. Pater⁸³, S. Patricelli¹⁰³a,¹⁰³b, T. Pauly³⁰, J. Pearce¹⁷⁰,
M. Pedersen¹¹⁸, S. Pedraza Lopez¹⁶⁸, S.V. Peleganchuk¹⁰⁸, D. Pelikan¹⁶⁷, H. Peng³³b, B. Penning³¹, J. Penwell⁶⁰,
D.V. Perepelitsa³⁵, E. Perez Codina¹⁶⁰a, M.T. Pérez García-Estañ¹⁶⁸, V. Perez Reale³⁵, L. Perini⁹⁰a,⁹⁰b,
H. Pernegger³⁰, R. Perrino⁷²a, R. Peschke⁴², V.D. Peshekhonov⁶⁴, K. Peters³⁰, R.F.Y. Peters⁵⁴,ah, B.A. Petersen³⁰,
J. Petersen³⁰, T.C. Petersen³⁶, E. Petit⁴², A. Petridis¹⁴⁷a,¹⁴⁷b, C. Petridou¹⁵⁵, E. Petrolo¹³³a, F. Petrucci¹³⁵a,¹³⁵b,
M. Petteni¹⁴³, R. Pezoa³²b, P.W. Phillips¹³⁰, G. Piacquadio¹⁴⁴, E. Pianori¹⁷¹, A. Picazio⁴⁹, E. Piccaro⁷⁵,
M. Piccinini²⁰a,²⁰b, S.M. Piec⁴², R. Piegaia²⁷, D.T. Pignotti¹¹⁰, J.E. Pilcher³¹, A.D. Pilkington⁷⁷, J. Pina¹²⁵a,d,
M. Pinamonti¹⁶⁵a,¹⁶⁵c,ai, A. Pinder¹¹⁹, J.L. Pinfold³, A. Pingel³⁶, B. Pinto¹²⁵a, C. Pizio⁹⁰a,⁹⁰b, 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, D. Pomeroy²³, K. Pommès³⁰, L. Pontecorvo¹³³a, B.G. Pope⁸⁹, G.A. Popeneciu²⁶b,
D.S. Popovic¹³a, A. Poppleton³⁰, X. Portell Bueso¹², G.E. Pospelov¹⁰⁰, S. Pospisil¹²⁷, K. Potamianos¹⁵,
I.N. Potrap⁶⁴, C.J. Potter¹⁵⁰, C.T. Potter¹¹⁵, G. Poulard³⁰, J. Poveda⁶⁰, V. Pozdnyakov⁶⁴, R. Prabhu⁷⁷,
P. Pralavorio⁸⁴, A. Pranko¹⁵, S. Prasad³⁰, R. Pravahan⁸, S. Prell⁶³, D. Price⁸³, J. Price⁷³, L.E. Price⁶, D. Prieur¹²⁴,
M. Primavera⁷²a, M. Proissl⁴⁶, K. Prokofiev¹⁰⁹, F. Prokoshin³²b, E. Protopapadaki¹³⁷, S. Protopopescu²⁵,
J. Proudfoot⁶, X. Prudent⁴⁴, M. Przybycien³⁸a, H. Przysiezniak⁵, S. Psoroulas²¹, E. Ptacek¹¹⁵, E. Pueschel⁸⁵,
D. Puldon¹⁴⁹, M. Purohit²⁵,aj, P. Puzo¹¹⁶, Y. Pylypchenko⁶², J. Qian⁸⁸, A. Quadt⁵⁴, D.R. Quarrie¹⁵,
W.B. Quayle¹⁶⁵a,¹⁶⁵b, D. Quilty⁵³, V. Radeka²⁵, V. Radescu⁴², S.K. Radhakrishnan¹⁴⁹, P. Radloff¹¹⁵,
F. Ragusa⁹⁰a,⁹⁰b, G. Rahal¹⁷⁹, S. Rajagopalan²⁵, M. Rammensee⁴⁸, M. Rammes¹⁴², A.S. Randle-Conde⁴⁰,
C. Rangel-Smith⁷⁹, K. Rao¹⁶⁴, F. Rauscher⁹⁹, T.C. Rave⁴⁸, T. Ravenscroft⁵³, M. Raymond³⁰, A.L. Read¹¹⁸,
D.M. Rebuzzi¹²⁰a,¹²⁰b, A. Redelbach¹⁷⁵, G. Redlinger²⁵, R. Reece¹³⁸, K. Reeves⁴¹, L. Rehnisch¹⁶, A. Reinsch¹¹⁵,
H. Reisin²⁷, M. Relich¹⁶⁴, C. Rembser³⁰, Z.L. Ren¹⁵², A. Renaud¹¹⁶, M. Rescigno¹³³a, S. Resconi⁹⁰a, B. Resende¹³⁷,
P. Reznicek⁹⁹, R. Rezvani⁹⁴, R. Richter¹⁰⁰, M. Ridel⁷⁹, P. Rieck¹⁶, M. Rijssenbeek¹⁴⁹, A. Rimoldi¹²⁰a,¹²⁰b,
L. Rinaldi²⁰a, E. Ritsch⁶¹, I. Riu¹², F. Rizatdinova¹¹³, E. Rizvi⁷⁵, S.H. Robertson⁸⁶,l, A. Robichaud-Veronneau¹¹⁹,
D. Robinson²⁸, J.E.M. Robinson⁸³, A. Robson⁵³, J.G. Rocha de Lima¹⁰⁷, C. Roda¹²³a,¹²³b, D. Roda Dos Santos¹²⁶,
L. Rodrigues³⁰, S. Roe³⁰, O. Røhne¹¹⁸, S. Rolli¹⁶², A. Romaniouk⁹⁷, M. Romano²⁰a,²⁰b, G. Romeo²⁷,
E. Romero Adam¹⁶⁸, N. Rompotis¹³⁹, L. Roos⁷⁹, E. Ros¹⁶⁸, S. Rosati¹³³a, K. Rosbach⁴⁹, A. Rose¹⁵⁰, 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. Rühr⁷, A. Ruiz-Martinez⁶³, Z. Rurikova⁴⁸,
N.A. Rusakovitch⁶⁴, A. Ruschke⁹⁹, J.P. Rutherfoord⁷, N. Ruthmann⁴⁸, P. Ruzicka¹²⁶, 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. Salamanna⁷⁵, 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, H.G. Sander⁸², M.P. Sanders⁹⁹, M. Sandhoff¹⁷⁶,
T. Sandoval²⁸, C. Sandoval¹⁶⁵a,¹⁶⁵b, 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,
E. Sarkisyan-Grinbaum⁸, B. Sarrazin²¹, G. Sartisohn¹⁷⁶, O. Sasaki⁶⁵, Y. Sasaki¹⁵⁶, I. Satsounkevitch⁹¹,
G. Sauvage⁵,*, E. Sauvan⁵, J.B. Sauvan¹¹⁶, P. Savard¹⁵⁹, f, D.O. Savu³⁰, C. Sawyer¹¹⁹, L. Sawyer⁷⁸,q, D.H. Saxon⁵³,
J. Saxon¹²¹, C. Sbarra²⁰a, A. Sbrizzi³, T. Scanlon³⁰, D.A. Scannicchio¹⁶⁴, M. Scarcella¹⁵¹, J. Schaarschmidt¹⁷³,
P. Schacht¹⁰⁰, D. Schaefer¹²¹, A. Schaelicke⁴⁶, 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, C. Schmitt⁹⁹, 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, M. Schram⁸⁶, S. Schramm¹⁵⁹, M. Schreyer¹⁷⁵, C. Schroeder⁸², N. Schroer⁵⁸c, N. Schuh⁸²,
M.J. Schultens²¹, H.-C. Schultz-Coulon⁵⁸a, H. Schulz¹⁶, M. Schumacher⁴⁸, B.A. Schumm¹³⁸, Ph. Schune¹³⁷,
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, M. Seman¹⁴⁵b, N. Semprini-Cesari²⁰a,²⁰b,
C. Serfon³⁰, L. Serin¹¹⁶, L. Serkin⁵⁴, T. Serre⁸⁴, R. Seuster¹⁶⁰a, H. Severini¹¹², F. Sforza¹⁰⁰, A. Sfyrla³⁰,
E. Shabalina⁵⁴, M. Shamim¹¹⁵, L.Y. Shan³³a, J.T. Shank²², Q.T. Shao⁸⁷, M. Shapiro¹⁵, P.B. Shatalov⁹⁶,
K. Shaw¹⁶⁵a,¹⁶⁵c, P. Sherwood⁷⁷, S. Shimizu⁶⁶, C.O. Shimmin¹⁶⁴, M. Shimojima¹⁰¹, T. Shin⁵⁶, M. Shiyakova⁶⁴,
A. Shmeleva⁹⁵, M.J. Shochet³¹, D. Short¹¹⁹, S. Shrestha⁶³, E. Shulga⁹⁷, M.A. Shupe⁷, S. Shushkevich⁴², P. Sicho¹²⁶,
D. Sidorov¹¹³, A. Sidoti¹³³a, F. Siegert⁴⁸, Dj. Sijacki¹³a, O. Silbert¹⁷³, J. Silva¹²⁵a, 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, L.A. Skinnari¹⁵, H.P. Skottowe⁵⁷,
K.Yu. Skovpen¹⁰⁸, P. Skubic¹¹², M. Slater¹⁸, T. Slavicek¹²⁷, K. Sliwa¹⁶², V. Smakhtin¹⁷³, B.H. Smart⁴⁶,
L. Smestad¹¹⁸, S.Yu. Smirnov⁹⁷, Y. Smirnov⁹⁷, L.N. Smirnova⁹⁸,ak, O. Smirnova⁸⁰, K.M. Smith⁵³, M. Smizanska⁷¹,
K. Smolek¹²⁷, A.A. Snesarev⁹⁵, G. Snidero⁷⁵, J. Snow¹¹², S. Snyder²⁵, R. Sobie¹⁷⁰,†, F. Socher⁴⁴, J. Sodomka¹²⁷,
A. Soffer¹⁵⁴, D.A. Soh¹⁵², x, C.A. Solans³⁰, M. Solar¹²⁷, J. Solc¹²⁷, E.Yu. Soldatov⁹⁷, U. Soldevila¹⁶⁸,
E. Solfaroli Camillocci¹³³a,¹³³b, A.A. Solodkov¹²⁹, O.V. Solovyanov¹²⁹, V. Solovyev¹²², N. Soni¹, A. Sood¹⁵,
V. Sopko¹²⁷, B. Sopko¹²⁷, M. Sosebee⁸, R. Soualah¹⁶⁵a,¹⁶⁵c, P. Soueid⁹⁴, A.M. Soukharev¹⁰⁸, D. South⁴²,
S. Spagnolo⁷²a,⁷²b, F. Spanò⁷⁶, W.R. Spearman⁵⁷, R. Spighi²⁰a, G. Spigo³⁰, M. Spousta¹²⁸, T. Spreitzer¹⁵⁹,
B. Spurlock⁸, R.D. St. Denis⁵³, 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,*, G. Steele⁵³, P. Steinbach⁴⁴, P. Steinberg²⁵, I. Stekl¹²⁷,
B. Stelzer¹⁴³, H.J. Stelzer⁸⁹, O. Stelzer-Chilton¹⁶⁰a, H. Stenzel⁵², S. Stern¹⁰⁰, G.A. Stewart³⁰, J.A. Stillings²¹,
M.C. Stockton⁸⁶, M. Stoebe⁸⁶, K. Stoerig⁴⁸, G. Stoicea²⁶a, S. Stonjek¹⁰⁰, A.R. Stradling⁸, A. Straessner⁴⁴,
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, I. Stumer²⁵,*, J. Stupak¹⁴⁹,
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. Sun⁵⁵, 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, 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, h, J.Y.C. Tam¹⁷⁵, M.C. Tamsett⁷⁸, al, K.G. Tan⁸⁷, J. Tanaka¹⁵⁶, R. Tanaka¹¹⁶, S. Tanaka¹³²,
S. Tanaka⁶⁵, A.J. Tanasijczuk¹⁴³, K. Tani⁶⁶, N. Tannoury⁸⁴, S. Tapprogge⁸², S. Tarem¹⁵³, F. Tarrade²⁹,
G.F. Tartarelli⁹⁰a, P. Tas¹²⁸, M. Tasevsky¹²⁶, T. Tashiro⁶⁷, E. Tassi³⁷a,³⁷b, A. Tavares Delgado¹²⁵a, Y. Tayalati¹³⁶d,
C. Taylor⁷⁷, 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, S. Terada⁶⁵, K. Terashi¹⁵⁶, J. Terron⁸¹,
S. Terzo¹⁰⁰, M. Testa⁴⁷, R.J. Teuscher¹⁵⁹, l, J. Therhaag²¹, T. Theveneaux-Pelzer³⁴, S. Thoma⁴⁸, 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, T. Tic¹²⁶,
V.O. Tikhomirov⁹⁵, am, Yu.A. Tikhonov¹⁰⁸, h, S. Timoshenko⁹⁷, E. Tiouchichine⁸⁴, P. Tipton¹⁷⁷, S. Tisserant⁸⁴,
T. Todorov⁵, S. Todorova-Nova¹²⁸, B. Toggerson¹⁶⁴, 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, ag, F. Touchard⁸⁴, D.R. Tovey¹⁴⁰, H.L. Tran¹¹⁶, T. Trefzger¹⁷⁵, L. Tremblet³⁰,
A. Tricoli³⁰, I.M. Trigger¹⁶⁰a, S. Trincaz-Duvoid⁷⁹, M.F. Tripiana⁷⁰, 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. Tsriritanis⁹,
S. Tsiskaridze¹², V. Tsiskaridze⁴⁸, E.G. Tskhadadze⁵¹a, I.I. Tsukerman⁹⁶, V. Tsulaia¹⁵, J.-W. Tsung²¹, S. Tsuno⁶⁵,
D. Tsybychev¹⁴⁹, A. Tua¹⁴⁰, A. Tudorache²⁶a, V. Tudorache²⁶a, A.N. Tuna¹²¹, S.A. Tupputi²⁰a,²⁰b,
S. Turchikhin⁹⁸, ak, D. Turecek¹²⁷, I. Turk Cakir⁴d, R. Turra⁹⁰a,⁹⁰b, P.M. Tuts³⁵, A. Tykhonov⁷⁴,
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, D. Urbaniec³⁵,
P. Urquijo²¹, 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, R. Van Berg¹²¹, 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, A. Vaniachine⁶, P. Vankov⁴², F. Vannucci⁷⁹,
G. Vardanyan¹⁷⁸, R. Vari¹³³a, E.W. Varnes⁷, T. Varol⁸⁵, D. Varouchas¹⁵, A. Vartapetian⁸, K.E. Varvell¹⁵¹,
V.I. Vassilakopoulos⁵⁶, F. Vazeille³⁴, T. Vazquez Schroeder⁵⁴, J. Veatch⁷, F. Veloso¹²⁵a, S. Veneziano¹³³a,
A. Ventura⁷²a,⁷²b, D. Ventura⁸⁵, M. Venturi⁴⁸, N. Venturi¹⁵⁹, A. Venturini²³, V. Vercesi¹²⁰a, M. Verducci¹³⁹,
W. Verkerke¹⁰⁶, J.C. Vermeulen¹⁰⁶, A. Vest⁴⁴, M.C. Vetterli¹⁴³, f, O. Viazlo⁸⁰, I. Vichou¹⁶⁶, T. Vickey¹⁴⁶c, an,
O.E. Vickey Boeriu¹⁴⁶c, G.H.A. Viehhauser¹¹⁹, S. Viel¹⁶⁹, R. Vigne³⁰, M. Villa²⁰a,²⁰b, M. Villaplana Perez¹⁶⁸,
E. Vilucchi⁴⁷, M.G. Vincter²⁹, V.B. Vinogradov⁶⁴, J. Virzi¹⁵, O. Vitells¹⁷³, I. Vivarelli¹⁵⁰, F. Vives Vaque³,
S. Vlachos¹⁰, D. Vladoiu⁹⁹, M. Vlasak¹²⁷, A. Vogel²¹, P. Vokac¹²⁷, G. Volpi⁴⁷, M. Volpi⁸⁷, H. von der Schmitt¹⁰⁰,
H. von Radziewski⁴⁸, E. von Toerne²¹, V. Vorobel¹²⁸, 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,
W. Wagner¹⁷⁶, P. Wagner²¹, S. Wahrmund⁴⁴, J. Wakabayashi¹⁰², J. Walder⁷¹, R. Walker⁹⁹, W. Walkowiak¹⁴²,
R. Wall¹⁷⁷, P. Waller⁷³, B. Walsh¹⁷⁷, C. Wang¹⁵², C. Wang⁴⁵, H. Wang¹⁵, H. Wang⁴⁰, J. Wang¹⁵², J. Wang³³a,
K. Wang⁸⁶, R. Wang¹⁰⁴, S.M. Wang¹⁵², T. Wang²¹, X. Wang¹⁷⁷, A. Warburton⁸⁶, C.P. Ward²⁸, D.R. Wardrobe⁷⁷,
M. Warsinsky⁴⁸, A. Washbrook⁴⁶, C. Wasicki⁴², I. Watanabe⁶⁶, P.M. Watkins¹⁸, A.T. Watson¹⁸, I.J. Watson¹⁵¹,
M.F. Watson¹⁸, G. Watts¹³⁹, S. Watts⁸³, A.T. Waugh¹⁵¹, B.M. Waugh⁷⁷, S. Webb⁸³, M.S. Weber¹⁷, S.W. Weber¹⁷⁵,
J.S. Webster³¹, A.R. Weidberg¹¹⁹, P. Weigell¹⁰⁰, J. Weingarten⁵⁴, C. Weiser⁴⁸, H. Weits¹⁰⁶, P.S. Wells³⁰,
T. Wenaus²⁵, D. Wendland¹⁶, Z. Weng¹⁵², x, T. Wengler³⁰, S. Wenig³⁰, N. Wermes²¹, M. Werner⁴⁸, P. Werner³⁰,
M. Wessels⁵⁸a, J. Wetter¹⁶², K. Whalen²⁹, A. White⁸, M.J. White¹, R. White³²b, S. White¹²³a,¹²³b, D. Whiteson¹⁶⁴,
D. Whittington⁶⁰, D. Wicke¹⁷⁶, F.J. Wickens¹³⁰, W. Wiedenmann¹⁷⁴, M. Wielers⁸⁰, e, P. Wienemann²¹,
C. Wiglesworth³⁶, L.A.M. Wiik-Fuchs²¹, P.A. Wijeratne⁷⁷, A. Wildauer¹⁰⁰, M.A. Wildt⁴², ao, H.G. Wilkens³⁰,
J.Z. Will⁹⁹, H.H. Williams¹²¹, S. Williams²⁸, S. Willocq⁸⁵, J.A. Wilson¹⁸, A. Wilson⁸⁸, I. Wingerter-Seez⁵,
S. Winkelmann⁴⁸, F. Winklmeier¹¹⁵, M. Wittgen¹⁴⁴, T. Wittig⁴³, J. Wittkowski⁹⁹, S.J. Wollstadt⁸², M.W. Wolter³⁹,
H. Wolters¹²⁵a, i, B.K. Wosiek³⁹, J. Wotschack³⁰, M.J. Woudstra⁸³, K.W. Wozniak³⁹, K. Wraight⁵³, M. Wright⁵³,
S.L. Wu¹⁷⁴, X. Wu⁴⁹, Y. Wu⁸⁸, E. Wulf³⁵, T.R. Wyatt⁸³, B.M. Wynne⁴⁶, S. Xella³⁶, M. Xiao¹³⁷, D. Xu³³a,
L. Xu³³b, ap, B. Yabsley¹⁵¹, S. Yacoob¹⁴⁶b, aq, M. Yamada⁶⁵, H. Yamaguchi¹⁵⁶, Y. Yamaguchi¹⁵⁶, 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, 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, B. Zabinski³⁹, R. Zaidan⁶², A.M. Zaitsev¹²⁹, ac, A. Zaman¹⁴⁹, S. Zambito²³,
L. Zanello¹³³a,¹³³b, D. Zanzi¹⁰⁰, A. Zaytsev²⁵, C. Zeitnitz¹⁷⁶, M. Zeman¹²⁷, A. Zemla³⁸a, K. Zengel²³, O. Zenin¹²⁹,
T. Ženiš¹⁴⁵a, D. Zerwas¹¹⁶, G. Zevi della Porta⁵⁷, D. Zhang⁸⁸, 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, A. Zibell⁹⁹, D. Zieminska⁶⁰, N.I. Zimin⁶⁴, C. Zimmermann⁸², R. Zimmermann²¹,
S. Zimmermann²¹, S. Zimmermann⁴⁸, Z. Zinonos⁵⁴, M. Ziolkowski¹⁴², R. Zitoun⁵, L. Živković³⁵, G. Zobernig¹⁷⁴,
A. Zoccoli²⁰a,²⁰b, M. zur Nedden¹⁶, G. Zurzolo¹⁰³a,¹⁰³b, V. Zutshi¹⁰⁷, L. Zwalinski³⁰.

¹ School of Chemistry and 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) Department 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, Copenhagen, Denmark

37 (a) INFN Gruppo Collegato di Cosenza; (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 Joseph Fourier and CNRS/IN2P3 and Institut National Polytechnique de Grenoble, 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 Física Teórica C-15, Universidad Autónoma 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 Scienze Fisiche, 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
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, Portugal; (b) Departamento de Fisica Teorica y del Cosmos and CAFPE, Universidad de Granada, Granada, Spain

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 I; (b) Dipartimento di Fisica, Università La Sapienza, 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 Mohamed 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; (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 Laboratorio de Instrumentacao e Fisica Experimental de Particulas - LIP, Lisboa, Portugal

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

d Also at Faculdade de Ciencias and CFNUL, Universidade de Lisboa, Lisboa, Portugal

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

f Also at TRIUMF, Vancouver BC, Canada

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

h Also at Novosibirsk State University, Novosibirsk, Russia

i Also at Department of Physics, University of Coimbra, Coimbra, Portugal

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

k Also at Università di Napoli Parthenope, Napoli, Italy

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

m Also at Department of Physics, Middle East Technical University, Ankara, Turkey

n Also at Dep Fisica and CEFITEC of Faculdade de Ciencias e Tecnologia, Universidade Nova de Lisboa, Caparica, Portugal

o Also at Department of Physics and Astronomy, Michigan State University, East Lansing MI, United States of America

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

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

r Also at Institucio Catalana de Recerca i Estudis Avancats, ICREA, Barcelona, Spain

s Also at Department of Physics, University of Cape Town, Cape Town, South Africa

t Also at CERN, Geneva, Switzerland

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

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

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

x Also at School of Physics and Engineering, Sun Yat-sen University, Guanzhou, China

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

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

aa Also at School of Physical Sciences, National Institute of Science Education and Research, Bhubaneswar, India
ab Also at Dipartimento di Fisica, Università La Sapienza, Roma, Italy

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

ad Also at Section de Physique, Université de Genève, Geneva, Switzerland

ae Also at Departamento de Fisica, Universidade de Minho, Braga, Portugal

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

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

ah Also at DESY, Hamburg and Zeuthen, Germany

ai Also at International School for Advanced Studies (SISSA), Trieste, Italy

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

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

al Also at Physics Department, Brookhaven National Laboratory, Upton NY, United States of America

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

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

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

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

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

* Deceased