Abstract
A search has been made for supersymmetry in a final state containing two photons and missing transverse momentum using the ATLAS detector at the Large Hadron Collider. The search makes use of \(3.2{~\mathrm{fb}^{-1}}\) of proton-proton collision data collected at a centre-of-mass energy of 13 TeV in 2015. Using a combination of data-driven and Monte-Carlo-based approaches, the Standard Model background is estimated to be \(0.27^{+0.22}_{-0.10}\) events. No events are observed in the signal region; considering the expected background and its uncertainty, this observation implies a model-independent 95 % CL upper limit of 0.93 fb (3.0 events) on the visible cross section due to physics beyond the Standard Model. In the context of a generalized model of gauge-mediated supersymmetry breaking with a bino-like next-to-lightest supersymmetric particle, this leads to a lower limit of 1650 GeV on the mass of a degenerate octet of gluino states, independent of the mass of the lighter bino-like neutralino.
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1 Introduction
This paper presents a search for signatures of supersymmetry in events containing two energetic isolated photons and large missing transverse momentum (with magnitude denoted \(E_{\text {T}}^{\text {miss}}\)) in \(3.2{~\mathrm{fb}^{-1}}\) of proton–proton (pp) collision data at \(\sqrt{s}=13\) TeV recorded with the ATLAS detector at the Large Hadron Collider (LHC) in 2015. The results are interpreted in the context of general gauge mediation (GGM) [1, 2] models that include the production of supersymmetric partners of Standard Model (SM) particles that possess color charge. In all models of GGM, the lightest supersymmetric particle (LSP) is the gravitino \(\tilde{G}\) (the partner of the hypothetical quantum of the gravitational field), with a mass significantly less than 1 GeV. In the GGM model considered here, the decay of the supersymmetric states produced in pp collisions would proceed through the next-to-lightest supersymmetric particle (NLSP), which would then decay to the \(\tilde{G}\) LSP and one or more SM particles, with a high probability of decay into \(\gamma \) + \(\tilde{G}\). All accessible supersymmetric states with the exception of the \(\tilde{G}\) are assumed to be short-lived, leading to prompt production of SM particles that would be observed in the ATLAS detector. These results extend those of prior studies with 8 TeV collision data from Run 1 by the ATLAS [3] and CMS [4] experiments.
Supersymmetry (SUSY) [5–10] introduces a symmetry between fermions and bosons, resulting in a SUSY particle (sparticle) with identical quantum numbers, with the exception of a difference of half a unit of spin relative to its corresponding SM partner. If SUSY were an exact symmetry of nature, each sparticle would have a mass equal to that of its SM partner. Since no sparticles have yet been observed, SUSY would have to be a broken symmetry. Assuming R-parity conservation [11], sparticles are produced in pairs. These would then decay through cascades involving other sparticles until the stable, undetectable LSP is produced, leading to a final state with significant \(E_{\text {T}}^{\text {miss}}\).
Experimental signatures of gauge-mediated supersymmetry-breaking models [12–14] are largely determined by the nature of the NLSP. For GGM, the NLSP is often formed from an admixture of any of the SUSY partners of the electroweak gauge and Higgs boson states. In this study the NLSP, assumed to be electrically neutral and purely bino-like (the SUSY partner of the SM U(1) gauge boson), is the lightest gaugino state \(\tilde{\chi }^{0}_{1}\). In this case, the final decay in each of the two cascades in a GGM event would be predominantly \(\tilde{\chi }^{0}_{1}\rightarrow \gamma +\tilde{G}\), leading to final states with \(\gamma \gamma +E_{\text {T}}^{\text {miss}}\).
In addition to the bino-like \(\tilde{\chi }^{0}_{1}\) NLSP, a degenerate octet of gluinos (the SUSY partner of the SM gluon) is taken to be potentially accessible with 13 TeV pp collisions. Both the gluino and \(\tilde{\chi }^{0}_{1}\) masses are considered to be free parameters, with the \(\tilde{\chi }^{0}_{1}\) mass constrained to be less than that of the gluino. All other SUSY masses are set to values that preclude their production in 13 TeV pp collisions. This results in a SUSY production process that proceeds through the creation of pairs of gluino states, each of which subsequently decays via a virtual squark (the 12 squark flavour/chirality eigenstates are taken to be fully degenerate) to a quark–antiquark pair plus the NLSP neutralino. Additional SM objects (jets, leptons, photons) may be produced in these cascades. The \(\tilde{\chi }^{0}_{1}\) branching fraction to \(\gamma \) + \(\tilde{G}\) is 100 % for \(m_{\tilde{\chi }^{0}_{1}} \rightarrow 0\) and approaches \(\cos ^2 \theta _W\) for \(m_{\tilde{\chi }^{0}_{1}} \gg m_Z\), with the remainder of the \(\tilde{\chi }^{0}_{1}\) sample decaying to Z + \(\tilde{G}\). For all \(\tilde{\chi }^{0}_{1}\) masses, then, the branching fraction is dominated by the photonic decay, leading to the diphoton-plus-\(E_{\text {T}}^{\text {miss}}\)signature. For this model with a bino-like NLSP, a typical production and decay channel for strong (gluino) production is exhibited in Fig. 1. Finally, it should be noted that the phenomenology relevant to this search has a negligible dependence on the ratio \(\tan \beta \) of the two SUSY Higgs-doublet vacuum expectation values; for this analysis \(\tan \beta \) is set to 1.5.
2 Samples of simulated processes
For the GGM models under study, the SUSY mass spectra and branching fractions are calculated using SUSPECT 2.41 [15] and SDECAY 1.3b [16], respectively, inside the package SUSY-HIT 1.3 [17]. The Monte Carlo (MC) SUSY signal samples are produced using Herwig++ 2.7.1 [18] with CTEQ6L1 parton distribution functions (PDFs) [19]. Signal cross sections are calculated to next-to-leading order (NLO) in the strong coupling constant, including, for the case of strong production, the resummation of soft gluon emission at next-to-leading-logarithmic accuracy (NLO+NLL) [20–24]. The nominal cross section and its uncertainty are taken from an envelope of cross-section predictions using different PDF sets and factorization and renormalization scales [25]. At fixed centre-of-mass energy, SUSY production cross sections decrease rapidly with increasing SUSY particle mass. At \(\sqrt{s} = 13\) TeV, the gluino-pair production cross section is approximately 25 fb for a gluino mass of 1.4 TeV and falls to below 1 fb for a gluino mass of 2.0 TeV.
While most of the backgrounds to the GGM models under examination are estimated through the use of control samples selected from data, as described below, the extrapolation from control regions (CRs) to the signal region (SR) depends on simulated samples, as do the optimization studies. Diphoton, photon+jet, \(W\gamma \), \(Z\gamma \), \(W\gamma \gamma \) and \(Z\gamma \gamma \) SM processes are generated using the SHERPA 2.1.1 simulation package [26], making use of the CT10 PDFs [27]. The matrix elements are calculated with up to three parton emissions at leading order (four in the case of photon+jet samples) and merged with the SHERPA parton shower [28] using the ME+PS@LO prescription [29]. The \(t\bar{t}\gamma \) process is generated using MadGraph5_aMC@NLO [30] with the CTEQ6L1 PDFs [19], in conjunction with PYTHIA 8.186 [31] with the NNPDF2.3LO PDF set [32, 33] and the A14 set [34] of tuned parameters.
All simulated samples are processed with a full ATLAS detector simulation [35] based on GEANT4 [36]. The effect of additional pp interactions per bunch crossing (“pile-up”) as a function of the instantaneous luminosity is taken into account by overlaying simulated minimum-bias events according to the observed distribution of the number of pile-up interactions in data, with an average of 13 interactions per event.
3 ATLAS detector
The ATLAS experiment records pp collision data with a multipurpose detector [37] that has a forward-backward symmetric cylindrical geometry and nearly 4\(\pi \) solid angle coverage. Closest to the beam line are solid-state tracking devices comprising layers of silicon-based pixel and strip detectors covering \(\left| \eta \right| <2.5\) and straw-tube detectors covering \(\left| \eta \right| <2.0\), located inside a thin superconducting solenoid that provides a 2T magnetic field. Outside of this “inner detector”, fine-grained lead/liquid-argon electromagnetic (EM) calorimeters provide coverage over \(\left| \eta \right| < 3.2\) for the measurement of the energy and direction of electrons and photons. A presampler, covering \(\left| \eta \right| < 1.8\), is used to correct for energy lost upstream of the EM calorimeter. A steel/scintillator-tile hadronic calorimeter covers the region \(|\eta | < 1.7\), while a copper/liquid-argon medium is used for hadronic calorimeters in the end cap region \(1.5< |\eta | < 3.2\). In the forward region \(3.2< |\eta | < 4.9\) liquid-argon calorimeters with copper and tungsten absorbers measure the electromagnetic and hadronic energy. A muon spectrometer consisting of three superconducting toroidal magnet systems, each comprising eight toroidal coils, tracking chambers, and detectors for triggering, surrounds the calorimeter system. The muon system reconstructs penetrating tracks over a range \(|\eta | < 2.7\) and provides input to the trigger system over a range \(|\eta | < 2.4\). A two-level trigger system [38] is used to select events. The first-level trigger is implemented in hardware and uses a subset of the detector information to reduce the accepted rate to less than 100 kHz. This is followed by a software-based ’high-level’ trigger (HLT) that reduces the recorded event rate to approximately 1 kHz.
4 Event reconstruction
Primary vertices are formed from sets of two or more tracks, each with transverse momentum \(p_\mathrm{T}^{\mathrm {track}}>\) 400 MeV, that are mutually consistent with having originated at the same three-dimensional point within the luminous region of the colliding proton beams. When more than one such primary vertex is found, the vertex with the largest sum of the squared transverse momenta of the associated tracks is chosen.
Electron candidates are reconstructed from EM calorimeter energy clusters consistent in transverse shape and longitudinal development with having arisen from the impact of an electromagnetic particle (electron or photon) upon the face of the calorimeter. For the object to be considered an electron, it is required to match a track identified by a reconstruction algorithm optimized for recognizing charged particles with a high probability of bremsstrahlung [39]. The energy of the electron candidate is determined from the EM cluster, while its direction is determined from the associated reconstructed track. Electron candidates are required to have \(p_{\text {T}}> 25~\text{GeV}\) and \(|\eta | < 2.37\), and to be outside the transition region \(1.37< \left| \eta \right| < 1.52\) between the central and forward portions of the EM calorimeter. Finally, the electron track is required to be consistent with originating from the primary vertex in both the \(r-z\) and \(r-\phi \) planes. Further details of the reconstruction of electrons can be found in Refs. [40] and [41].
Electromagnetic clusters are classified as photon candidates provided that they either have no matched track or have one or more matched tracks consistent with having arisen from a photon conversion. Based on the characteristics of the longitudinal and transverse shower development in the EM calorimeter, photons are classified as “loose” or “tight”, with the tight requirements leading to a more pure but less efficienct selection of photons relative to that of the loose requirements [42]. Photon candidates are required to have \(p_{\text {T}}> 25~\text{GeV}\), to be within \(\left| \eta \right| < 2.37\), and to be outside the transition region \(1.37< \left| \eta \right| < 1.52\). Additionally, an isolation requirement is imposed: after correcting for contributions from pile-up and the deposition ascribed to the photon itself, the energy within a cone of \(\Delta R = 0.4\) around the cluster barycentre is required to be less than \(2.45~\text{GeV} + 0.022 \times p_{\mathrm {T}}^{\gamma }\), where \(p_{\mathrm {T}}^{\gamma }\) is the transverse momentum of the cluster. In the case that an EM calorimeter deposition identified as a photon overlaps the cluster of an identified electron within a cone of \(\Delta R = 0.4\), the photon candidate is discarded and the electron candidate is retained. Further details of the reconstruction of photons can be found in Ref. [42].
Muon candidates make use of reconstructed tracks from the inner detector as well as information from the muon system [43]. Muons are required to be either “combined”, for which the muon is reconstructed independently in both the muon spectrometer and the inner detector and then combined, or “segment-tagged”, for which the muon spectrometer is used to tag tracks as muons, without requiring a fully reconstructed candidate in the muon spectrometer. Muons are required to have \(p_{\text {T}}> 25~\text{GeV}\) and \(|\eta |<2.7\), with the muon track required to be consistent with originating from the primary vertex in both the \(r-z\) and \(r-\phi \) planes.
Jets are reconstructed from three-dimensional energy clusters [44] in the electromagnetic and hadronic calorimeters using the anti-\(k_t\) algorithm [45] with a radius parameter R = 0.4. Each cluster is calibrated to the electromagnetic scale prior to jet reconstruction. The reconstructed jets are then calibrated to particle level by the application of a jet energy scale derived from simulation and in situ corrections based on 8 TeV data [46, 47]. In addition, the expected average energy contribution from pile-up clusters is subtracted using a factor dependent on the jet area [46]. Track-based selection requirements are applied to reject jets with \(p_{\text {T}}{} < 60\) GeV and \(|\eta | < 2.4\) that originate from pile-up interactions [48]. Once calibrated, jets are required to have \(p_{\text {T}}>\) 40 GeV and \(|\eta | < 2.8\).
To resolve the ambiguity that arises when a photon is also reconstructed as a jet, if a jet and a photon are reconstructed within an angular distance \(\Delta R = 0.4\) of one another, the photon is retained and the jet is discarded. If a jet and an electron are reconstructed within an angular distance \(\Delta R = 0.2\) of one another, the electron is retained and the jet is discarded; if \(0.2< \Delta R < 0.4\) then the jet is retained and the electron is discarded. Finally, in order to suppress the reconstruction of muons arising from showers induced by jets, if a jet and a muon are found with \(\Delta R < 0.4\) the jet is retained and the muon is discarded.
The missing transverse momentum \(\varvec{p}_{\mathrm {T}}^\mathrm{miss}\) is defined as the negative vector sum of the \(p_{\text {T}}\) of all reconstructed physics objects in the event, with an extra term added to account for soft energy in the event that is not associated with any of the objects. This “\(E_{\text {T}}^{\text {miss}}\) soft term” is calculated from inner-detector tracks with \(p_{\text {T}}\)above 400 MeV matched to the primary vertex to make it less dependent upon pile-up contamination [49, 50]. The scalar observable \(E_{\text {T}}^{\text {miss}}\) is defined to be the magnitude of the resulting \(\varvec{p}_{\mathrm {T}}^\mathrm{miss}\) vector.
Several additional observables are defined to help in the discrimination of SM backgrounds from potential GGM signals. The total visible transverse energy, \(H_{\text {T}}\), is calculated as the scalar sum of the transverse momenta of the reconstructed photons and any additional leptons and jets in the event. The “effective mass”, \(m_{\mathrm {eff}}\), is defined as the scalar sum of \(H_{\text {T}}\) and \(E_{\text {T}}^{\text {miss}}\). The minimum jet–\(\varvec{p}_{\mathrm {T}}^\mathrm{miss}\) separation, \(\Delta \phi _{\mathrm {min}}(\mathrm {jet},\varvec{p}_{\mathrm {T}}^\mathrm{miss}{})\), is defined as the minimum azimuthal angle between the missing transverse momentum vector and the two leading (highest-\(p_{\text {T}}\)) jets with \(p_{\text {T}}> 75\) GeV in the event, if they are present. If no such jets exist, no requirement is placed on this observable.
5 Event selection
The data sample is selected by a HLT trigger requiring the presence of two loose photons, each with \(p_{\text {T}}\) greater than 50 GeV. Offline, two tight photons with \(p_{\text {T}}> 75~\text{GeV}\) are required. In order to ensure that \(E_{\text {T}}^{\text {miss}}\) is measured well, events are removed from the data sample if they contain jets likely to be produced by beam backgrounds, cosmic rays or detector noise [51].
To exploit the significant undetectable transverse momentum carried away by the gravitinos, a requirement on \(E_{\text {T}}^{\text {miss}}\) is imposed on the diphoton event sample. To take advantage of the high production energy scale associated with signal events near the expected reach of the analysis, an additional requirement on \(m_{\mathrm {eff}}\) is applied. To further ensure the accurate reconstruction of \(E_{\text {T}}^{\text {miss}}\) and to suppress backgrounds associated with the mismeasurement of hadronic jets, a requirement of \(\Delta \phi _{\mathrm {min}}(\mathrm {jet},\varvec{p}_{\mathrm {T}}^\mathrm{miss}{})> 0.5\) is imposed. Figure 2 shows the \(E_{\text {T}}^{\text {miss}}\) and \(m_{\mathrm {eff}}\) distributions of the diphoton sample after the application of requirements of \(p_{\mathrm {T}}^{\gamma }> 75\) GeV on each selected photon and of \(\Delta \phi _{\mathrm {min}}(\mathrm {jet},\varvec{p}_{\mathrm {T}}^\mathrm{miss}{})> 0.5\), but with no requirements yet imposed on \(E_{\text {T}}^{\text {miss}}\) and \(m_{\mathrm {eff}}\). Also shown are the expected contributions from SM processes, estimated using the combination of Monte Carlo and data-driven estimates discussed in Sect. 6.
As discussed in Sect. 1, the GGM signal space is parameterized by the masses of the gluino (\(m_{\tilde{g}}\)) and bino-like NLSP (\(m_{\tilde{\chi }^{0}_{1}}\)). The sensitivity of this analysis was optimized for two signal scenarios near the expected reach in \(m_{\tilde{g}}\): high and low neutralino-mass benchmark points were chosen with \((m_{\tilde{g}},m_{\tilde{\chi }^{0}_{1}}) = (1500,1300)\) GeV and \((m_{\tilde{g}},m_{\tilde{\chi }^{0}_{1}}) = (1500,100)\) GeV, respectively.
Based on background estimates derived from the MC samples described in Sect. 2, the selection requirements were optimized as a function of \(E_{\text {T}}^{\text {miss}}\), \(m_{\mathrm {eff}}\) and \(p_{\mathrm {T}}^{\gamma }\) by maximizing the expected discovery sensitivity of the analysis, for each of the two signal benchmark points. The selected values of the minimum requirements on all three optimization parameters were found to be very similar for the low and high neutralino-mass benchmark points, leading to the definition of a single signal region (SR). The selection requirements for this SR are shown in Table 1.
6 Background estimation
Processes that contribute to the Standard Model background of diphoton final states can be divided into three primary components. The largest contribution to the inclusive diphoton spectrum is the “QCD background”, which can be further divided into a contribution from two real photons produced in association with jets, and a “jet-faking-photon” contribution arising from \(\gamma \)+jet and multijet events for which one or both reconstructed photons are faked by a jet, typically by producing a \(\pi ^{0}\rightarrow \gamma \gamma \) decay that is misidentified as a prompt photon. An “electron-faking-photon background” arises predominantly from W, Z, and \(\; t\bar{t}\) events, possibly accompanied by additional jets and/or photons, for which an electron is misidentified as a photon. Electron-to-photon misidentification is due primarily to instances for which an electron radiates a high-momentum photon as it traverses the material of the ATLAS inner detector. Last, an “irreducible background” arises from \(W\gamma \gamma \) and \(Z\gamma \gamma \) events. These backgrounds are estimated with a combination of data-driven and simulation-based methods described as follows.
The component of the QCD background arising from real diphoton events (\(\gamma \gamma \)) is estimated directly from diphoton MC events, rescaled as function of \(E_{\text {T}}^{\text {miss}}\)and the number of selected jets to match the respective distributions for the inclusive diphoton sample in the range \(E_{\text {T}}^{\text {miss}}<\) 100 GeV. While this background dominates the inclusive diphoton sample, it is very steeply falling in \(E_{\text {T}}^{\text {miss}}\), making it small relative to backgrounds with real \(E_{\text {T}}^{\text {miss}}\) for \(E_{\text {T}}^{\text {miss}}\gtrsim \) 100 GeV, independent of the reweighting.
The component of the QCD background arising from jets faking photons and the background arising from electrons faking photons are both estimated with a data-driven “fake-factor” method, for which events in data samples enriched in the background of interest are weighted by factors parameterizing the misidentification rate.
To estimate the jet-faking-photon fake-factor, the jet-faking-photon background is enriched by using an inverted isolation requirement, selecting events only if they contain one or more non-isolated photons. The relative probability of an energy cluster being reconstructed as an isolated, rather than non-isolated, photon is known as the photon-isolation fake factor, and is measured in an orthogonal “non-tight” sample of photons. The selection of this sample requires that all the tight photon identification requirements be satisfied, with the exception that at least one of the requirements on the calorimeter variables defined only with the first (strip) layer of the electromagnetic calorimeter fails. This leads to a sample enriched in identified (non-tight) photons that are actually \(\pi ^0\)s within jets. The correlation between the isolation variable and the photon identification requirements was found to be small and to have no significant impact on the estimation of the jet-faking-photon fake-factor. The fake factors depend upon \(p_{\text {T}}\) and \(\eta \), and vary between 10 and 30 %. The jet-faking photon background is then estimated by weighting events with non-isolated photons by the applicable photon-isolation fake factor.
The electron-faking-photon background is estimated with a similar fake-factor method. For this case, the electron-faking-photon background is enriched by selecting events with a reconstructed electron instead of a second photon. Fake factors for electrons being misidentified as photons are then measured by comparing the ratio of reconstructed \(e\gamma \) to ee events arising from Z bosons decaying to electron–positron pairs, selected within the mass range of 75–105 GeV. The electron-faking-photon background is then estimated by weighting selected \(e\gamma \) events by their corresponding fake factors, which are typically a few percent.
The irreducible background from \(W\gamma \gamma \) events is estimated with MC simulation; however, because it is a potentially dominant background contribution, the overall normalization is derived in a \(\ell \gamma \gamma \) control region (\(W\gamma \gamma \) CR) as follows. Events in the \(W\gamma \gamma \) CR are required to have two tight, isolated photons with \(p_{\text {T}}> 50\) GeV, and exactly one selected lepton (electron or muon) with \(p_{\text {T}}> 25\) GeV. As with the SR, events are required to have \(\Delta \phi _{\mathrm {min}}(\mathrm {jet},\varvec{p}_{\mathrm {T}}^\mathrm{miss}{})> 0.5\), so that the direction of the missing transverse momentum vector is not aligned with that of any high-\(p_{\text {T}}\) jet. To ensure that the control sample has no overlap with the signal region, events are discarded if \(E_{\text {T}}^{\text {miss}}> 175\) GeV. While these requirements target \(W\gamma \gamma \) production, they also are expected to select appreciable backgrounds from \(t\bar{t}\gamma \), \(Z\gamma \) and \(Z\gamma \gamma \) events, and thus additional requirements are applied. To suppress \(t\bar{t}\gamma \) contributions to the \(W\gamma \gamma \) CR, events are discarded if they contain more than two selected jets. To suppress \(Z\gamma \) contributions, events are discarded if there is an e–\(\gamma \) pair in the events with \(83< m_{e\gamma } < 97\) GeV. Finally, to suppress \(Z\gamma \gamma \) contributions, events with \(E_{\text {T}}^{\text {miss}}<50\) GeV are discarded. The event selection requirements for the \(W\gamma \gamma \) CR are summarized in Table 1. A total of seven events are observed in this \(W\gamma \gamma \) control region, of which 1.6 are expected to arise from sources other than \(W\gamma \gamma \) production. The MC expectation for the \(W\gamma \gamma \) process is 1.9 events, leading to a \(W\gamma \gamma \) scale factor of \(2.9 \pm 1.4\), assuming that no GGM signal events contaminate the \(W\gamma \gamma \) CR. This scale factor is consistent with that of the corresponding \(\sqrt{s} =\) 8 TeV analysis [3], and is reconciled by a large and uncertain NLO correction to the \(W\gamma \gamma \) production cross section that depends strongly upon the momentum of the \(W\gamma \gamma \) system [52]. When setting limits on specific signal models, a simultaneous fit to the control region and the signal region is performed, allowing both the signal and \(W\gamma \gamma \) contributions to float to their best-fit values.
Last, the irreducible background from \(Z(\rightarrow \nu \nu )\gamma \gamma \) events, the only background without a data-derived normalization, is estimated with simulation and found to be 0.02 events. A \({\pm }100~\%\) uncertainty is conservatively applied to account for modelling uncertainties [53].
A summary of the background contributions to the signal region is presented in Table 2. The QCD background can be traced to a few hundredths of an event at high \(E_{\text {T}}^{\text {miss}}\)and high \(m_{\mathrm {eff}}\), but no events are observed for either the diphoton Monte Carlo or the jet-faking-photon control sample when the full signal region requirements are applied. Relaxing the \(m_{\mathrm {eff}}\) requirement, and using a conservative extrapolation of the expected QCD background as a function of \(m_{\mathrm {eff}}\), the combined QCD background is estimated to be \(0.05^{+0.20}_{-0.05}\) events. The estimate of the electron-faking-photon background is established by the presence of two \(e\gamma \) events in the background model passing the SR requirements, yielding a background estimate of \(0.03 \pm 0.02\) events after application of the fake-factor weights. Summing all background contributions, a total of \(0.27^{+0.22}_{-0.10}\) SM events are expected in the SR, with the largest contribution, \(0.17 \pm 0.08\) events, expected to arise from \(W\gamma \gamma \) production. The background modelling was found to agree well in several validation regions, including the inclusive high-\(p_{\text {T}}\) diphoton sample, as well as event selections with relaxed \(m_{\mathrm {eff}}\) and \(E_{\text {T}}^{\text {miss}}\) requirements relative to those of the SR.
7 Signal efficiencies and uncertainties
GGM signal acceptances and efficiencies are estimated using MC simulation for each simulated point in the gluino–bino parameter space, and vary significantly across this space due to variations in the photon \(p_{\text {T}}\), \(E_{\text {T}}^{\text {miss}}\), and \(m_{\mathrm {eff}}\) spectra. For example, for a gluino mass of 1600 GeV, the acceptance-times-efficiency product varies between 14 and 28 %, reaching a minimum as the NLSP mass approaches the Z boson mass, below which the photonic branching fraction of the NLSP rises to unity. Table 3 summarizes the contributions to the systematic uncertainty of the signal acceptance-times-efficiency, which are discussed below.
Making use of a bootstrap method [54], the efficiency of the diphoton trigger is determined to be greater than 99 %, with an uncertainty of less than 1 %. The uncertainty in the integrated luminosity is \({\pm }2.1~\%\). It is derived, following a methodology similar to that detailed in Ref. [55], from a calibration of the luminosity scale using x–y beam-separation scans performed in August 2015.
The reconstruction and identification efficiency for tight, isolated photons is estimated with complementary data-driven methods [42]. Photons selected kinematically as originating from radiative decays of a Z boson (\(Z \rightarrow \ell ^+ \ell ^- \gamma \) events) are used to study the photon reconstruction efficiency as a function of \(p_{\text {T}}\) and \(\eta \). Independent measurements making use of a tag-and-probe approach with \(Z \rightarrow ee\) events, with one of the electrons used to probe the calorimeter response to electromagnetic depositions, also provide information about the photon reconstruction efficiency. For photons with \(p_{\text {T}}> 75\) GeV, the identification efficiency varies between 93 and 99 %, depending on the values of the photon \(p_{\text {T}}\) and \(|\eta |\) and whether the photon converted in the inner detector. The uncertainty also depends upon these factors, and is generally no more than a few percent.
Uncertainties in the photon and jet energy scales lead to uncertainties in the signal acceptance-times-efficiency that vary across the GGM parameter space, and contribute the dominant source of acceptance-times-efficiency uncertainty in certain regions of the parameter space. The photon energy scale is determined using samples of \(Z \rightarrow ee\) and \(J/\psi \rightarrow ee\) events [56]. The jet-energy scale uncertainty is constrained from an assessment of the effect of uncertainties in the modelling of jet properties and by varying the response to differing jet flavour composition in MC simulations, as well as from in situ measurements with 8 TeV dijet data [46, 47].
Uncertainties in the values of whole-event observables, such as \(E_{\text {T}}^{\text {miss}}\) and \(m_{\mathrm {eff}}\), arise from uncertainties in the energy of the underlying objects from which they are constructed. Uncertainties in the \(E_{\text {T}}^{\text {miss}}\) soft term due to uncertainties in hadronic fragmentation, detector material modeling and energy scale were found to introduce an uncertainty of less than 0.1 % in the signal acceptance-times-efficiency. The uncertainty due to pile-up is estimated by varying the mean of the distribution of the number of interactions per bunch crossing overlaid in the simulation by \({\pm }11~\%\).
Including the contribution from the statistical limitations of the MC samples used to model the GGM parameter space, the quadrature sum of the individual systematic uncertainties in the signal reconstruction efficiency is, on average, about 4 %. Adding the uncertainty in the integrated luminosity gives a total systematic uncertainty of about 5 %.
8 Results
An accounting of the numbers of events observed in the SR after the successive application of the selection requirements is shown in Table 4 along with the size of the expected SM background. After the full selection is applied, no events are observed in the SR, to be compared to an expectation of \(0.27^{+ 0.22}_{-0.10}\) SM events.
Based on the observation of zero events in the SR and the magnitude of the estimated SM background expectation and uncertainty, an upper limit is set on the number of events from any scenario of physics beyond the SM, using the profile likelihood and \(CL_s\) prescriptions [57]. The various sources of experimental uncertainty, including those in the background expectation, are treated as Gaussian-distributed nuisance parameters in the likelihood definition. Assuming that no events due to physical processes beyond those of the SM populate the \(\ell \gamma \gamma \) CR used to estimate the \(W(\rightarrow \ell \nu )+\gamma \gamma \) background, the observed 95 % confidence-level (CL) upper limit on the number of non-SM events in the SR is found to be 3.0. Taking into account the integrated luminosity of \(3.2{~\mathrm{fb}^{-1}}\), this number-of-event limit translates into a 95 % CL upper limit on the visible cross section for new physics, defined by the product of cross section, branching fraction, acceptance and efficiency, of 0.93 fb.
By considering, in addition, the value and uncertainty of the acceptance-times-efficiency of the selection requirements associated with the SR, as well as the NLO (+NLL) GGM cross Sect. [20–24], which varies steeply with gluino mass, 95 % CL lower limits may be set on the mass of the gluino as a function of the mass of the lighter bino-like neutralino, in the context of the GGM scenario described in Sect. 1. The resulting observed limit on the gluino mass is exhibited, as a function of neutralino mass, in Fig. 3. For the purpose of establishing these model-dependent limits, the \(W(\rightarrow \ell \nu )+\gamma \gamma \)background estimate and the limit on the possible number of events from new physics are extracted from a simultaneous fit to the SR and \(W(\rightarrow \ell \nu )+\gamma \gamma \)control region, although for a gluino mass in the range of the observed limit the signal contamination in the \(W(\rightarrow \ell \nu )+\gamma \gamma \)control sample is less than 0.03 events for any value of the neutralino mass. Also shown for this figure is the expected limit, including its statistical and background uncertainty range, as well as observed limits for a SUSY model cross section \({\pm }1\) standard deviation of theoretical uncertainty from its central value. Because the background expectation is close to zero and no events are observed in data, the expected and observed limits nearly overlap. The observed lower limit on the gluino mass is observed to be roughly independent of neutralino mass, reaching a minimum value of approximately 1650 GeV at a neutralino mass of 250 GeV. Within the context of this model, gluino masses as low as 400 GeV have been excluded in a prior analysis making use of 7 TeV ATLAS data [58].
9 Conclusion
A search has been made for a diphoton + \(E_{\text {T}}^{\text {miss}}\) final state using the ATLAS detector at the Large Hadron Collider in \(3.2{~\mathrm{fb}^{-1}}\) of proton–proton collision data taken at a centre-of-mass energy of 13 TeV in 2015. At least two photon candidates with \(p_{\text {T}}> 75~\text{GeV}\) are required, as well as minimum values of 175 and 1500 GeV of the missing transverse momentum and effective mass of the event, respectively. The resulting signal region targets events with pair-produced high-mass gluinos each decaying to either a high-mass or low-mass bino-like neutralino. Using a combination of data-driven and direct Monte Carlo approaches, the SM background is estimated to be \(0.27^{+0.22}_{-0.10}\) events, with most of the expected background arising from the production of a W boson in association with two energetic photons. No events are observed in the signal region; considering the expected background and its uncertainty, this observation implies model-independent 95 % CL upper limits of 3.0 events (0.93 fb) on the number of events (visible cross section) due to physics beyond the Standard Model. In the context of a generalized model of gauge-mediated supersymmetry breaking with a bino-like NLSP, this leads to a lower limit of 1650 GeV on the mass of a degenerate octet of gluino states, independent of the mass of the lighter bino-like neutralino. This extends the corresponding limit of 1340 GeV derived from a similar analysis of 8 TeV data by the ATLAS Collaboration.
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Acknowledgments
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; BMWFW 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 and DNSRC, Denmark; IN2P3-CNRS, CEA-DSM/IRFU, France; GNSF, Georgia; BMBF, HGF, and MPG, Germany; GSRT, Greece; RGC, Hong Kong SAR, China; ISF, I-CORE and Benoziyo Center, Israel; INFN, Italy; MEXT and JSPS, Japan; CNRST, Morocco; FOM and NWO, The Netherlands; RCN, Norway; MNiSW and NCN, Poland; FCT, Portugal; MNE/IFA, Romania; MES of Russia and NRC KI, Russian Federation; JINR; MESTD, Serbia; MSSR, Slovakia; ARRS and MIZŠ, Slovenia; DST/NRF, South Africa; MINECO, Spain; SRC and Wallenberg Foundation, Sweden; SERI, SNSF and Cantons of Bern and Geneva, Switzerland; MOST, Taiwan; TAEK, Turkey; STFC, United Kingdom; DOE and NSF, United States of America. In addition, individual groups and members have received support from BCKDF, the Canada Council, CANARIE, CRC, Compute Canada, FQRNT, and the Ontario Innovation Trust, Canada; EPLANET, ERC, FP7, Horizon 2020 and Marie Skłodowska-Curie Actions, European Union; Investissements d’Avenir Labex and Idex, ANR, Région Auvergne and Fondation Partager le Savoir, France; DFG and AvH Foundation, Germany; Herakleitos, Thales and Aristeia programmes co-financed by EU-ESF and the Greek NSRF; BSF, GIF and Minerva, Israel; BRF, Norway; Generalitat de Catalunya, Generalitat Valenciana, Spain; the Royal Society and Leverhulme Trust, UK. The crucial computing support from all WLCG partners is acknowledged gratefully, in particular from CERN, 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), the Tier-2 facilities worldwide and large non-WLCG resource providers. Major contributors of computing resources are listed in Ref. [59].
Author information
Authors and Affiliations
Department of Physics, University of Adelaide, Adelaide, Australia
A. Antonov, W. Blum, H. M. Braun, V. Chernyatin, H. Hakobyan, P. Ioannou, P. Jackson, A. A. Komar, L. Lee, A. Loginov, B. Osculati, A. Petridis, D. M. Seliverstov, R. D. St. Denis, T. Todorov, I. Vichou & M. J. White
Physics Department, SUNY Albany, Albany, NY, USA
J. Bouffard, J. Ernst, A. Fischer, S. Guindon & V. Jain
Department of Physics, University of Alberta, Edmonton, AB, Canada
P. Czodrowski, J. Dassoulas, N. Dehghanian, D. M. Gingrich, S. Jabbar, A. Karamaoun, R. W. Moore & J. L. Pinfold
Department of Physics, Ankara University, Ankara, Turkey
O. Cakir, A. K. Ciftci & H. Duran Yildiz
Istanbul Aydin University, Istanbul, Turkey
S. Kuday
Division of Physics, TOBB University of Economics and Technology, Ankara, Turkey
S. Sultansoy
LAPP, CNRS/IN2P3 and Université Savoie Mont Blanc, Annecy-le-Vieux, France
Z. Barnovska-Blenessy, N. Berger, M. Delmastro, L. Di Ciaccio, S. Elles, K. Grevtsov, T. Guillemin, T. Hryn’ova, S. Jézéquel, I. Koletsou, R. Lafaye, J. Levêque, P. Mastrandrea, E. Sauvan, B. H. Smart, T. Todorov, I. Wingerter-Seez & E. Yatsenko
High Energy Physics Division, Argonne National Laboratory, Argonne, IL, USA
R. E. Blair, S. Chekanov, T. LeCompte, J. Love, D. Malon, J. Metcalfe, D. H. Nguyen, A. Paramonov, L. E. Price, J. Proudfoot, S. Ryu, R. W. Stanek, P. van Gemmeren, R. Wang, J. S. Webster, R. Yoshida & J. Zhang
Department of Physics, University of Arizona, Tucson, AZ, USA
E. Cheu, K. A. Johns, S. Jones, W. Lampl, X. Lei, R. Leone, P. Loch, R. Nayyar, F. O’grady, J. P. Rutherfoord, M. A. Shupe, E. W. Varnes & V. Veeraraghavan
Department of Physics, The University of Texas at Arlington, Arlington, TX, USA
A. Brandt, D. Bullock, S. Darmora, K. De, A. Farbin, L. Feremenga, J. Griffiths, H. K. Hadavand, L. Heelan, H. Y. Kim, N. Ozturk, J. Schovancova, A. R. Stradling, G. Usai, A. Vartapetian, A. White & J. Yu
Physics Department, University of Athens, Athens, Greece
S. Angelidakis, S. Chouridou, D. Fassouliotis, N. Giokaris, P. Ioannou, C. Kourkoumelis & N. Tsirintanis
Physics Department, National Technical University of Athens, Zografou, Greece
T. Alexopoulos, N. Benekos, M. Dris, E. N. Gazis, K. Karakostas, N. Karastathis, E. Karentzos, S. Leontsinis, S. Maltezos, E. St. Panagiotopoulou, Th. D. Papadopoulou, G. Tsipolitis & S. Vlachos
Department of Physics, The University of Texas at Austin, Austin, TX, USA
T. Andeen, Y. Ilchenko, R. Narayan & P. U. E. Onyisi
Institute of Physics, Azerbaijan Academy of Sciences, Baku, Azerbaijan
O. Abdinov & F. Khalil-zada
Institut de Física d’Altes Energies (IFAE), The Barcelona Institute of Science and Technology, Barcelona, Spain
N. Anjos, M. Bosman, M. P. Casado, M. Casolino, E. Cavallaro, M. Cavalli-Sforza, T. Farooque, S. Fernandez Perez, C. Fischer, S. Fracchia, D. Gerbaudo, G. Gonzalez Parra, S. Grinstein, A. Juste Rozas, I. Korolkov, J. C. Lange, I. Lopez Paz, M. Martinez, L. M. Mir, A. Pacheco Pages, C. Padilla Aranda, I. Riu, C. Rizzi, A. Rodriguez Perez, V. Sorin, S. Terzo, M. F. Tripiana, S. Tsiskaridze & L. Valery
Institute of Physics, University of Belgrade, Belgrade, Serbia
T. Agatonovic-Jovin, D. Bogavac, P. Bokan, A. Dimitrievska, J. Krstic, M. Marjanovic, Dj. Sijacki, Lj. Simic, N. Vranjes, M. Vranjes Milosavljevic & L. Živković
Department for Physics and Technology, University of Bergen, Bergen, Norway
T. Buanes, O. Dale, G. Eigen, A. Kastanas, W. Liebig, A. Lipniacka, S. Maeland, B. Martin dit Latour, L. Smestad, B. Stugu, Z. Yang & J. Zalieckas
Physics Division, Lawrence Berkeley National Laboratory and University of California, Berkeley, CA, USA
B. T. Amadio, B. Axen, R. M. Barnett, J. Beringer, J. Brosamer, P. Calafiura, F. Cerutti, A. Ciocio, R. N. Clarke, M. Cooke, E. M. Duffield, K. Einsweiler, S. Farrell, A. Gabrielli, M. Garcia-Sciveres, M. Gilchriese, C. Haber, T. Heim, B. Heinemann, I. Hinchliffe, R. R. Hinman, T. R. Holmes, L. Jeanty, W. Lavrijsen, C. Leggett, Z. Marshall, C. C. Ohm, S. Pagan Griso, K. Potamianos, A. Pranko, M. Shapiro, A. Sood, M. J. Tibbetts, M. Trottier-McDonald, V. Tsulaia, S. Viel, H. Wang, W-M. Yao & D. R. Yu
Department of Physics, Humboldt University, Berlin, Germany
D. Biedermann, J. Dietrich, F. M. Giorgi, S. Grancagnolo, G. H. Herbert, I. Hristova, O. M. Kind, H. Kolanoski, H. Lacker, T. Lohse, S. Mergelmeyer, A. Nikiforov, L. Rehnisch, P. Rieck, H. Schulz, D. Sperlich, S. Stamm & M. zur Nedden
Albert Einstein Center for Fundamental Physics and Laboratory for High Energy Physics, University of Bern, Bern, Switzerland
H. P. Beck, A. Cervelli, A. Ereditato, S. Haug, F. Meloni, A. Miucci, G. A. Mullier, M. Rimoldi, M. E. Stramaglia & M. S. Weber
School of Physics and Astronomy, University of Birmingham, Birmingham, UK
P. P. Allport, N. Andari, L. Aperio Bella, M. J. Baca, J. Bracinik, J. H Broughton, D. Casadei, D. G. Charlton, A. C. Daniells, A. G. Foster, L. Gonella, C. M. Hawkes, S. J. Head, S. J. Hillier, M. Levy, R. D. Mudd, J. A. Murillo Quijada, P. R. Newman, K. Nikolopoulos, R. E. Owen, M. Slater, J. P. Thomas, P. D. Thompson, P. M. Watkins, A. T. Watson, M. F. Watson & J. A. Wilson
Department of Physics, Bogazici University, Istanbul, Turkey
M. Arik, S. Istin & V. E. Ozcan
Department of Physics Engineering, Gaziantep University, Gaziantep, Turkey
A. Beddall & A. Bingul
Faculty of Engineering and Natural Sciences, Istanbul Bilgi University, Istanbul, Turkey
S. A. Cetin
Faculty of Engineering and Natural Sciences, Bahcesehir University, Istanbul, Turkey
A. J. Beddall
Centro de Investigaciones, Universidad Antonio Narino, Bogotá, Colombia
M. Losada, D. Moreno, G. Navarro & C. Sandoval
INFN Sezione di Bologna, Bologna, Italy
G. L. Alberghi, L. Bellagamba, S. Biondi, D. Boscherini, A. Bruni, G. Bruni, M. Bruschi, C. Ciocca, G. D’amen, S. De Castro, F. Fabbri, L. Fabbri, M. Franchini, A. Gabrielli, B. Giacobbe, F. M. Giorgi, P. Grafström, F. Lasagni Manghi, I. Massa, L. Massa, A. Mengarelli, M. Negrini, M. Piccinini, A. Polini, L. Rinaldi, M. Romano, C. Sbarra, A. Sbrizzi, N. Semprini-Cesari, A. Sidoti, M. Sioli, R. Spighi, S. A. Tupputi, G. Ucchielli, S. Valentinetti, M. Villa, C. Vittori & A. Zoccoli
Dipartimento di Fisica e Astronomia, Università di Bologna, Bologna, Italy
G. L. Alberghi, S. Biondi, C. Ciocca, G. D’amen, S. De Castro, F. Fabbri, L. Fabbri, M. Franchini, A. Gabrielli, P. Grafström, F. Lasagni Manghi, I. Massa, L. Massa, A. Mengarelli, M. Piccinini, M. Romano, A. Sbrizzi, N. Semprini-Cesari, A. Sidoti, M. Sioli, S. A. Tupputi, G. Ucchielli, S. Valentinetti, M. Villa, C. Vittori & A. Zoccoli
Physikalisches Institut, University of Bonn, Bonn, Germany
O. Arslan, P. Bechtle, F. U. Bernlochner, I. Brock, N. Bruscino, J. Caudron, I. A. Cioara, M. Cristinziani, W. Davey, K. Desch, J. Dingfelder, G. Gaycken, Ch. Geich-Gimbel, M. Ghneimat, C. Grefe, S. Hageböck, M. C. Hansen, D. Hohn, F. Huegging, J. Janssen, V. V. Kostyukhin, J. Kroseberg, H. Krüger, K. Lantzsch, T. Lenz, A. M. Leyko, J. Liebal, R. Moles-Valls, T. Obermann, D. Pohl, O. Ricken, B. Sarrazin, S. Schaepe, E. Schopf, M. J. Schultens, T. Schwindt, P. Seema, J. A. Stillings, E. von Toerne, P. Wagner, T. Wang, N. Wermes, L. A. M. Wiik-Fuchs, B. T. Winter, K. H. Yau Wong, S. P. Y. Yuen & R. Zhang
Department of Physics, Boston University, Boston, MA, USA
S. P. Ahlen, K. M. Black, J. M. Butler, L. Dell’Asta, M. Kruskal, B. A. Long, J. T. Shank, Z. Yan & S. Youssef
Department of Physics, Brandeis University, Waltham, MA, USA
C. Amelung, G. Amundsen, G. Barone, J. R. Bensinger, L. Bianchini, C. Blocker, S. Dhaliwal, M. Goblirsch-Kolb, H. Herde, K. M. Loew, G. Sciolla, A. Venturini & K. Zengel
Universidade Federal do Rio De Janeiro COPPE/EE/IF, Rio de Janeiro, Brazil
Y. Amaral Coutinho, L. P. Caloba, C. Maidantchik, F. Marroquim, A. A. Nepomuceno & J. M. Seixas
Electrical Circuits Department, Federal University of Juiz de Fora (UFJF), Juiz de Fora, Brazil
A. S. Cerqueira, L. Manhaes de Andrade Filho & B. S. Peralva
Federal University of Sao Joao del Rei (UFSJ), Sao Joao del Rei, Brazil
M. A. B. do Vale
Instituto de Fisica, Universidade de Sao Paulo, São Paulo, Brazil
M. Donadelli, J. L. La Rosa Navarro & M. A. L. Leite
Physics Department, Brookhaven National Laboratory, Upton, NY, USA
D. L. Adams, K. Assamagan, M. Begel, W. Buttinger, H. Chen, V. Chernyatin, R. Debbe, J. Elmsheuser, M. Ernst, B. Gibbard, H. A. Gordon, G. Iakovidis, A. Klimentov, V. Kouskoura, A. Kravchenko, F. Lanni, C. A. Lee, H. Liu, D. Lynn, H. Ma, T. Maeno, E. Mountricha, P. Nevski, P. Nilsson, D. Oliveira Damazio, F. Paige, S. Panitkin, D. V. Perepelitsa, M. -A. Pleier, V. Polychronakos, S. Protopopescu, M. Purohit, V. Radeka, S. Rajagopalan, G. Redlinger, S. Snyder, P. Steinberg, S. A. Stucci, H. Takai, A. Tricoli, A. Undrus, T. Wenaus, L. Xu & S. Ye
National Institute of Physics and Nuclear Engineering, Bucharest, Romania
C. Alexa, I. Caprini, M. Caprini, A. Chitan, M. Ciubancan, S. Constantinescu, P. Dita, S. Dita, M. Dobre, A. Jinaru, V. S. Martoiu, J. Maurer, A. Olariu, D. Pantea, M. Rotaru, G. Stoicea, A. Tudorache & V. Tudorache
Physics Department, National Institute for Research and Development of Isotopic and Molecular Technologies, Cluj Napoca, Romania
G. A. Popeneciu
West University in Timisoara, Timisoara, Romania
P. M. Gravila
Departamento de Física, Universidad de Buenos Aires, Buenos Aires, Argentina
J. D. Bossio Sola, G. Marceca, G. Otero y Garzon, R. Piegaia & S. Sacerdoti
Cavendish Laboratory, University of Cambridge, Cambridge, UK
M. Arratia, N. Barlow, J. R. Batley, F. M. Brochu, BH Brunt, J. R. Carter, J. D. Chapman, G. Cottin, T. P. S. Gillam, J. C. Hill, S. Kaneti, C. G. Lester, C. Malone, T. Mueller, M. A. Parker, C. J. Potter, D. Robinson, J. H. N. Rosten, M. Thomson, C. P. Ward & I. Yusuff
Department of Physics, Carleton University, Ottawa, ON, Canada
A. Bellerive, G. Cree, D. Di Valentino, D. Gillberg, T. Koffas, J. Lacey, W. A. Leight, I. Nomidis, F. G. Oakham, G. Pásztor, A. Ruiz-Martinez, M. G. Vincter & S. A. Weber
CERN, Geneva, Switzerland
M. Aleksa, B. Alvarez Gonzalez, S. Amoroso, G. Anders, F. Anghinolfi, O. Arnaez, G. Avolio, M. A. Baak, M. Backhaus, L. Barak, M-S Barisits, T. A. Beermann, O. Beltramello, M. Bianco, J. A. Bogaerts, J. Bortfeldt, A. Boveia, J. Boyd, H. Burckhart, S. Camarda, S. Campana, M. D. M. Capeans Garrido, T. Carli, G. D. Carrillo-Montoya, A. Catinaccio, A. Cattai, M. Cerv, A. S. Chisholm, D. Chromek-Burckhart, G. Conti, A. Cortes-Gonzalez, A. Dell’Acqua, P. O. Deviveiros, A. Di Girolamo, B. Di Girolamo, R. Di Nardo, F. Dittus, D. Dobos, A. Dudarev, M. Dührssen, T. Eifert, N. Ellis, M. Elsing, J. Faltova, P. Farthouat, P. Fassnacht, E. J. Feng, D. Francis, S. M. Fressard-Batraneanu, D. Froidevaux, S. Gadatsch, L. Goossens, B. Gorini, H. M. Gray, C. Gumpert, R. J. Hawkings, L. Helary, C. Helsens, A. M. Henriques Correia, L. Hervas, A. Hoecker, M. Huhtinen, P. Iengo, S. Jakobsen, T. Klioutchnikova, A. Krasznahorkay, C. Lapoire, M. Lassnig, G. Lehmann Miotto, B. Lenzi, P. Lichard, S. Malyukov, A. Manousos, L. Mapelli, A. Marzin, J. Montejo Berlingen, S. Morgenstern, G. Mornacchi, A. M. Nairz, M. Nessi, M. Nordberg, H. Oide, S. Palestini, T. Pauly, H. Pernegger, B. A. Petersen, K. Pommès, A. Poppleton, G. Poulard, J. Poveda, M. E. Pozo Astigarraga, M. Rammensee, M. Raymond, C. Rembser, E. Ritsch, S. Roe, N. Ruthmann, A. Salzburger, D. Schaefer, S. Schlenker, K. Schmieden, F. Sforza, C. A. Solans Sanchez, G. Spigo, S. Stärz, H. J. Stelzer, F. A. Teischinger, H. Ten Kate, G. Unal, M. C. van Woerden, W. Vandelli, R. Voss, R. Vuillermet, P. S. Wells, T. Wengler, S. Wenig, P. Werner, H. G. Wilkens, J. Wotschack, C. J. S. Young & L. Zwalinski
Enrico Fermi Institute, University of Chicago, Chicago, IL, USA
J. Alison, K. J. Anderson, P. Bryant, R. Camacho Toro, Y. Cheng, J. R. Dandoy, G. Facini, R. W. Gardner, A. Kapliy, Y. K. Kim, K. Krizka, H. L. Li, F. S. Merritt, D. W. Miller, M. J. Oreglia, J. E. Pilcher, J. Saxon, M. J. Shochet, G. H. Stark, M. Swiatlowski, I. Vukotic & M. Wu
Departamento de Física, Pontificia Universidad Católica de Chile, Santiago, Chile
S. Blunier, M. A. Diaz & J. P. Ochoa-Ricoux
Departamento de Física, Universidad Técnica Federico Santa María, Valparaiso, Chile
W. K. Brooks, E. Carquin, S. Kuleshov, J. A. López, R. Pezoa, F. Prokoshin, J. E. Salazar Loyola, S. Tapia Araya, G. A. Vasquez & R. White
Institute of High Energy Physics, Chinese Academy of Sciences, Beijing, China
Y. Bai, J. Barreiro Guimarães da Costa, H. J Cheng, Y. Fang, S. Jin, Q. Li, Z. Liang, J. Llorente Merino, X. Lou, J. D. Mansour, Q. Ouyang, C. Peng, H. Ren, L. Y. Shan, X. Sun, D. Xu, H. Zhu & X. Zhuang
Department of Modern Physics, University of Science and Technology of China, Hefei, Anhui, China
J. Gao, C. Geng, Y. Guo, L. Han, Q. Hu, Y. Jiang, B. Li, C. Li, J. B. Liu, M. Liu, Y. L. Liu, Y. Liu, H. Peng, H. Y. Song, W. Wang, G. Zhang, R. Zhang, Z. Zhao & Y. Zhu
Department of Physics, Nanjing University, Nanjing, Jiangsu, China
S. Chen, C. Wang & H. Zhang
School of Physics, Shandong University, Jinan, Shandong, China
Y. Du, C. Feng, L. L. Ma, Y. Ma, B. Osculati, C. Wang, X. Zhang, Y. Zhao & C. G. Zhu
Shanghai Key Laboratory for Particle Physics and Cosmology, Department of Physics and Astronomy, Shanghai Jiao Tong University (also affiliated with PKU-CHEP), Shanghai, China
M. Cano Bret, J. Guo, S. Hu, L. Li & H. Yang
Physics Department, Tsinghua University, Beijing, 100084, China
X. Chen & N. Zhou
Laboratoire de Physique Corpusculaire, Clermont Université and Université Blaise Pascal and CNRS/IN2P3, Clermont-Ferrand, France
D. Boumediene, E. Busato, D. Calvet, S. Calvet, A. R. Chomont, J. Donini, Ph. Gris, R. Madar, D. Pallin, S. M. Romano Saez, C. Santoni, D. Simon & F. Vazeille
Nevis Laboratory, Columbia University, Irvington, NY, USA
S. P. Alkire, A. Angerami, G. Brooijmans, R. M. Carbone, M. R. Clark, B. Cole, E. W. Hughes, K. Iordanidou, M. H. Klein, S. Mohapatra, I. Ochoa, J. A. Parsons, M. N. K. Smith, R. W. Smith, E. N. Thompson, P. M. Tuts, T. Wang & L. Zhou
Niels Bohr Institute, University of Copenhagen, Kobenhavn, Denmark
A. Alonso, G. J. Besjes, M. Dam, G. Galster, J. B. Hansen, J. D. Hansen, P. H. Hansen, A. E. Loevschall-Jensen, J. Monk, S. S. Mortensen, L. E. Pedersen, T. C. Petersen, A. Pingel, C. Wiglesworth & S. Xella
INFN Gruppo Collegato di Cosenza, Laboratori Nazionali di Frascati, Frascati, Italy
V. M. Cairo, G. Callea, M. Capua, G. Crosetti, M. Del Gaudio, L. La Rotonda, A. Mastroberardino, S. Palazzo, A. Policicchio, D. Salvatore, V. Scarfone, M. Schioppa, G. Susinno & E. Tassi
Dipartimento di Fisica, Università della Calabria, Rende, Italy
V. M. Cairo, G. Callea, M. Capua, G. Crosetti, M. Del Gaudio, L. La Rotonda, A. Mastroberardino, S. Palazzo, A. Policicchio, D. Salvatore, V. Scarfone, M. Schioppa, G. Susinno & E. Tassi
Faculty of Physics and Applied Computer Science, AGH University of Science and Technology, Kraków, Poland
L. Adamczyk, T. Bold, W. Dabrowski, G. P. Gach, I. Grabowska-Bold, D. Kisielewska, S. Koperny, T. Z. Kowalski, B. Mindur, M. Przybycien & A. Zemla
Marian Smoluchowski Institute of Physics, Jagiellonian University, Kraków, Poland
M. Palka & E. Richter-Was
Institute of Nuclear Physics, Polish Academy of Sciences, Kraków, Poland
E. Banas, P. A. Bruckman de Renstrom, K. Burka, J. J. Chwastowski, D. Derendarz, J. Godlewski, E. Gornicki, Z. Hajduk, A. Kaczmarska, J. Knapik, K. Korcyl, A. B. Kowalewska, Pa. Malecki, A. Olszewski, J. Olszowska, E. Stanecka, R. Staszewski, M. Trzebinski, A. Trzupek, M. W. Wolter, B. K. Wosiek, K. W. Wozniak & B. Zabinski
Physics Department, Southern Methodist University, Dallas, TX, USA
T. Cao, A. Firan, R. Gupta, J. W. Hetherly, S. Kama, R. Kehoe, S. J. Sekula, R. Stroynowski, T. Varol, H. Wang, J. Ye, X. Zhao & L. Zhou
Physics Department, University of Texas at Dallas, Richardson, TX, USA
J. M. Izen, M. Leyton, B. Meirose, H. Namasivayam & K. Reeves
DESY, Hamburg and Zeuthen, Hamburg, Germany
N. Asbah, J. K. Behr, C. Bertsche, M. Bessner, I. Bloch, D. Britzger, C. Deterre, S. Díez Cornell, B. Dutta, M. Dyndal, C. Eckardt, J. Ferrando, M. Filipuzzi, N. Flaschel, A. Gascon Bravo, K. Gasnikova, A. Glazov, I. M. Gregor, M. Haleem, P. G. Hamnett, K. H. Hiller, J. Howarth, Y. Huang, J. Katzy, J. S. Keller, N. Kondrashova, T. Kuhl, E. M. Lobodzinska, K. Lohwasser, A. Madsen, M. Medinnis, K. Mönig, R. F. Naranjo Garcia, T. Naumann, A. A. O’Rourke, R. Peschke, K. Peters, H. Pirumov, A. Poley, J. E. M. Robinson, R. Schaefer, S. Schmitt, D. South, M. Stanescu-Bellu, M. M. Stanitzki, N. A. Styles, K. Tackmann, A. Trofymov, J. Wang & N. Zakharchuk
Lehrstuh für Experimentelle Physik IV, Technische Universität Dortmund, Dortmund, Germany
I. Burmeister, D. Cinca, K. Dette, J. Erdmann, H. Esch, C. Gössling, M. Homann, R. Klingenberg & K. Kroeninger
Institut für Kern- und Teilchenphysik, Technische Universität Dresden, Dresden, Germany
P. Anger, D. Duschinger, F. Friedrich, J. P. Grohs, C. Gutschow, L. Hauswald, M. Kobel, W. F. Mader, O. Novgorodova, F. Siegert, F. Socher, A. Straessner, A. Vest & S. Wahrmund
Department of Physics, Duke University, Durham, NC, USA
A. T. H. Arce, D. P. Benjamin, D. M. Bjergaard, A. Bocci, B. C. Cerio, A. T. Goshaw, E. Kajomovitz, A. Kotwal, M. C. Kruse, L. Li, S. Li, M. Liu, S. H. Oh & C. Zhou
SUPA-School of Physics and Astronomy, University of Edinburgh, Edinburgh, UK
T. M. Bristow, P. J. Clark, F. A. Dias, N. C. Edwards, Y. Gao, F. M. Garay Walls, P. C. F. Glaysher, R. D. Harrington, C. Leonidopoulos, V. J. Martin, L. Mijović, C. Mills, S. A. Olivares Pino, A. Washbrook & B. M. Wynne
INFN Laboratori Nazionali di Frascati, Frascati, Italy
M. Antonelli, M. Beretta, H. Bilokon, V. Chiarella, M. Curatolo, B. Esposito, C. Gatti, P. Laurelli, G. Maccarrone, G. Mancini, A. Sansoni, M. Testa & E. Vilucchi
Fakultät für Mathematik und Physik, Albert-Ludwigs-Universität, Freiburg, Germany
H. Arnold, C. Betancourt, M. Boehler, R. Bruneliere, F. Buehrer, C. D. Burgard, D. Büscher, F. Cardillo, E. Coniavitis, V. Consorti, N. P. Dang, V. Dao, A. Di Simone, J. Glatzer, G. Gonella, G. Herten, M. Hirose, K. Jakobs, T. Javůrek, P. Jenni, F. Kiss, K. Köneke, A. K. Kopp, S. Kuehn, U. Landgraf, C. Luedtke, M. Nagel, M. Pagáčová, U. Parzefall, M. Ronzani, K. Rosbach, F. Rühr, Z. Rurikova, D. Sammel, C. Schillo, U. Schnoor, M. Schumacher, P. Sommer, J. E. Sundermann, D. Ta, K. K. Temming, P. Tornambe, V. Tsiskaridze, C. Weiser, M. Werner, L. Zhang & S. Zimmermann
Section de Physique, Université de Genève, Geneva, Switzerland
L. S. Ancu, J. Bilbao De Mendizabal, N. Calace, A. Chatterjee, A. Clark, A. Coccaro, C. M. Delitzsch, D. della Volpe, D. Ferrere, T. Golling, S. Gonzalez-Sevilla, J. Gramling, F. Guescini, G. Iacobucci, A. Katre, T. J. Khoo, M. C. Lanfermann, A. E. Lionti, L. March, P. Mermod, O. Nackenhorst, L. Paolozzi, B. Ristić, S. Schramm, A. Sfyrla & X. Wu
INFN Sezione di Genova, Genoa, Italy
D. Barberis, G. Darbo, A. Favareto, A. Ferretto Parodi, G. Gagliardi, A. Gaudiello, C. Gemme, E. Guido, S. Miglioranzi, P. Morettini, F. Parodi, S. Passaggio, L. P. Rossi, M. Sannino & C. Schiavi
Dipartimento di Fisica, Università di Genova, Genoa, Italy
D. Barberis, A. Favareto, A. Ferretto Parodi, G. Gagliardi, A. Gaudiello, E. Guido, S. Miglioranzi, F. Parodi, M. Sannino & C. Schiavi
E. Andronikashvili Institute of Physics, Iv. Javakhishvili Tbilisi State University, Tbilisi, Georgia
E. G. Tskhadadze
High Energy Physics Institute, Tbilisi State University, Tbilisi, Georgia
T. Djobava, A. Durglishvili, J. Khubua & M. Mosidze
II Physikalisches Institut, Justus-Liebig-Universität Giessen, Giessen, Germany
M. Düren, C. Heinz, K. Kreutzfeldt & H. Stenzel
SUPA-School of Physics and Astronomy, University of Glasgow, Glasgow, UK
A. A. Alshehri, R. L. Bates, A. Blue, S. K. Boutle, W. D. Breaden Madden, D. Britton, A. G. Buckley, P. Bussey, C. M. Buttar, A. Buzatu, S. J. Crawley, S. D’Auria, A. T. Doyle, U. Gul, A. Knue, P. Mullen, V. O’Shea, M. Owen, C. S. Pollard, G. Qin, D. Quilty, T. Ravenscroft, A. Robson, R. D. St. Denis, G. A. Stewart & A. S. Thompson
II Physikalisches Institut, Georg-August-Universität, Göttingen, Germany
J. Agricola, M. Bindi, T. Bisanz, U. Blumenschein, G. Brandt, A. De Maria, E. Drechsler, L. Graber, J. Grosse-Knetter, M. Janus, M. J. Kareem, G. Kawamura, S. Lai, B. Lemmer, E. Magradze, M. Mantoani, G. Mchedlidze, M. Moreno Llácer, H. Musheghyan, A. Quadt, J. Rieger, N. -A. Rosien, G. F. Rzehorz, E. Shabalina, P. Stolte, J. Veatch, J. Weingarten & Z. Zinonos
Laboratoire de Physique Subatomique et de Cosmologie, Université Grenoble-Alpes, CNRS/IN2P3, Grenoble, France
S. Albrand, S. Berlendis, A. Bethani, C. Camincher, J. Collot, S. Crépé-Renaudin, P. A. Delsart, C. Gabaldon, M. H. Genest, P. O. J. Gradin, J-Y. Hostachy, F. Ledroit-Guillon, A. Lleres, A. Lucotte, F. Malek, E. Petit, J. Stark, B. Trocmé & M. Wu
Laboratory for Particle Physics and Cosmology, Harvard University, Cambridge, MA, USA
S. K. Chan, B. L. Clark, M. Franklin, P. Giromini, J. Huth, V. Ippolito, T. Lazovich, D. Lopez Mateos, M. Morii, C. S. Rogan, H. P. Skottowe, S. Sun, E. Tolley, B. Tong, A. N. Tuna, A. L. Yen & S. Zambito
Kirchhoff-Institut für Physik, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
V. Andrei, C. Antel, A. E. Baas, O. Brandt, J. I. Djuvsland, M. Dunford, M. P. Geisler, P. Hanke, J. Jongmanns, E. -E. Kluge, V. S. Lang, K. Meier, H. Meyer Zu Theenhausen, D. I. Narrias Villar, M. Sahinsoy, V. Scharf, H. -C. Schultz-Coulon, R. Stamen, P. Starovoitov, S. Suchek & M. Wessels
Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
C. F. Anders, D. E. Ferreira de Lima, M. Giulini, M. Kolb, M. Lisovyi, S. Schaetzel, A. Schoening & D. Sosa
ZITI Institut für technische Informatik, Ruprecht-Karls-Universität Heidelberg, Mannheim, Germany
M. Kretz & A. Kugel
Faculty of Applied Information Science, Hiroshima Institute of Technology, Hiroshima, Japan
Y. Nagasaka
Department of Physics, The Chinese University of Hong Kong, Shatin, NT, Hong Kong
V. Bortolotto, Y. L. Chan, L. R. Flores Castillo, H. Lu, A. Salvucci & K. M. Tsui
Department of Physics, The University of Hong Kong, Hong Kong, China
V. Bortolotto, N. Orlando & Y. Tu
Department of Physics, The Hong Kong University of Science and Technology, Clear Water Bay, Kowloon, Hong Kong, China
V. Bortolotto & K. Prokofiev
Department of Physics, Indiana University, Bloomington, IN, USA
K. Choi, H. Evans, P. Gagnon, R. Kopeliansky, S. Lammers, N. Lorenzo Martinez, F. Luehring, H. Ogren, J. Penwell, B. Weinert & D. Zieminska
Institut für Astro- und Teilchenphysik, Leopold-Franzens-Universität, Innsbruck, Austria
J. Guenther, W. Iwanski, R. Jansky, E. Kneringer, W. Lukas & A. Milic
University of Iowa, Iowa City, IA, USA
J. Abdallah, S. Argyropoulos, J. Benitez, U. Mallik & R. Zaidan
Department of Physics and Astronomy, Iowa State University, Ames, IA, USA
C. Chen, J. Cochran, F. De Lorenzi, H. Jiang, N. Krumnack, D. Pluth, S. Prell, M. D. Werner & J. Yu
Joint Institute for Nuclear Research, JINR Dubna, Dubna, Russia
F. Ahmadov, I. N. Aleksandrov, V. A. Bednyakov, I. R. Boyko, I. A. Budagov, G. A. Chelkov, A. Cheplakov, M. V. Chizhov, D. V. Dedovich, M. Demichev, A. Gongadze, M. I. Gostkin, N. Huseynov, N. Javadov, S. N. Karpov, Z. M. Karpova, E. Khramov, U. Kruchonak, V. Kukhtin, E. Ladygin, V. Lyubushkin, I. A. Minashvili, M. Mineev, V. D. Peshekhonov, E. Plotnikova, I. N. Potrap, V. Pozdnyakov, N. A. Rusakovich, R. Sadykov, A. Sapronov, M. Shiyakova, A. Soloshenko, S. Turchikhin, V. B. Vinogradov, I. Yeletskikh, A. Zhemchugov & N. I. Zimine
KEK, High Energy Accelerator Research Organization, Tsukuba, Japan
K. Amako, M. Aoki, Y. Arai, K. Hanagaki, T. Honda, Y. Ikegami, M. Ikeno, H. Iwasaki, J. Kanzaki, T. Kondo, T. Kono, Y. Makida, R. Nagai, K. Nagano, K. Nakamura, M. Nozaki, S. Odaka, T. Okuyama, O. Sasaki, S. Suzuki, Y. Takubo, S. Tanaka, S. Terada, K. Tokushuku, S. Tsuno, Y. Unno, A. Yamamoto & Y. Yasu
Graduate School of Science, Kobe University, Kobe, Japan
Y. Chen, M. Hasegawa, S. Kido, H. Kurashige, J. Maeda, A. Ochi, S. Shimizu, R. Tanioka, Y. Yamazaki & L. Yuan
Faculty of Science, Kyoto University, Kyoto, Japan
T. Kunigo, R. Monden, T. Sumida & T. Tashiro
Kyoto University of Education, Kyoto, Japan
R. Takashima
Department of Physics, Kyushu University, Fukuoka, Japan
K. Kawagoe, S. Oda, H. Otono, S. Shirabe & J. Tojo
Instituto de Física La Plata, Universidad Nacional de La Plata and CONICET, La Plata, Argentina
M. J. Alconada Verzini, F. Alonso, F. A. Arduh, M. T. Dova, J. Hoya, F. Monticelli & H. Wahlberg
Physics Department, Lancaster University, Lancaster, UK
A. E. Barton, M. D. Beattie, I. A. Bertram, G. Borissov, E. V. Bouhova-Thacker, W. J. Dearnaley, H. Fox, K. Grimm, R. C. W. Henderson, G. Hughes, R. W. L. Jones, V. Kartvelishvili, R. E. Long, P. A. Love, D. Muenstermann, A. J. Parker, M. B. Skinner, M. Smizanska, J. Walder & A. M. Wharton
INFN Sezione di Lecce, Lecce, Italy
M. Aliev, K. Bachas, G. Chiodini, E. Gorini, L. Longo, M. Primavera, M. Reale, S. Spagnolo & A. Ventura
Dipartimento di Matematica e Fisica, Università del Salento, Lecce, Italy
M. Aliev, K. Bachas, E. Gorini, L. Longo, M. Reale, S. Spagnolo & A. Ventura
Oliver Lodge Laboratory, University of Liverpool, Liverpool, UK
A. A. Affolder, J. K. Anders, S. Burdin, M. D’Onofrio, P. Dervan, C. B. Gwilliam, H. S. Hayward, T. J. Jones, B. T. King, M. Klein, U. Klein, J. Kretzschmar, P. Laycock, A. Lehan, S. J. Maxfield, A. Mehta, N. P. Readioff & J. H. Vossebeld
Department of Physics, Jožef Stefan Institute and University of Ljubljana, Ljubljana, Slovenia
V. Cindro, A. Filipčič, A. Gorišek, L. Kanjir, B. P. Kerševan, G. Kramberger, B. Maček, I. Mandić, M. Mikuž, M. Muškinja, T. Sfiligoj & G. Sokhrannyi
School of Physics and Astronomy, Queen Mary University of London, London, UK
L. J. Armitage, A. J. Bevan, M. Bona, J. M. Hays, R. Hickling, M. P. J. Landon, D. Lewis, S. L. Lloyd, J. D. Morris, T. Nooney, E. Piccaro, E. Rizvi & R. L. Sandbach
Department of Physics, Royal Holloway University of London, Surrey, UK
T. Berry, V. Boisvert, T. Brooks, I. A. Connelly, G. Cowan, M. Faucci Giannelli, S. Gadomski, S. George, S. M. Gibson, J. J. Kempster, C. R. Kilby, J. G. Panduro Vazquez, Fr. Pastore, G. Savage, B. C. Sowden, F. Spanò, P. Teixeira-Dias & J. Thomas-Wilsker
Department of Physics and Astronomy, University College London, London, UK
A. S. Bell, J. M. Butterworth, M. Campanelli, V. Christodoulou, B. D. Cooper, P. Davison, R. J. Falla, D. Freeborn, K. Gregersen, Z. J. Grout, N. G. Gutierrez Ortiz, G. G. Hesketh, S. Jiggins, N. Konstantinidis, A. Korn, H. Kucuk, K. J. C. Leney, A. C. Martyniuk, L. I. McClymont, J. A. Mcfayden, E. Nurse, S. Richter, T. Scanlon, P. Sherwood, B. Simmons, D. R. Wardrope & B. M. Waugh
Louisiana Tech University, Ruston, LA, USA
Z. D. Greenwood, G. C. Grossi, D. K. Jana & L. Sawyer
Laboratoire de Physique Nucléaire et de Hautes Energies, UPMC and Université Paris-Diderot and CNRS/IN2P3, Paris, France
T. Beau, M. Bomben, G. Calderini, F. Crescioli, S. De Cecco, A. Demilly, F. Derue, P. Francavilla, M. W. Krasny, D. Lacour, B. Laforge, S. Laplace, O. Le Dortz, G. Lefebvre, A. Lopez Solis, P. M. Luzi, B. Malaescu, G. Marchiori, I. Nikolic-Audit, J. Ocariz, C. E. Pandini, S. Pires, M. Ridel, L. Roos, S. Trincaz-Duvoid, D. Varouchas & Y. C. Yap
Fysiska institutionen, Lunds universitet, Lund, Sweden
T. P. A. Åkesson, S. S. Bocchetta, L. Bryngemark, C. Doglioni, V. Hedberg, G. Jarlskog, E. Lytken, J. U. Mjörnmark, O. Smirnova & O. Viazlo
Departamento de Fisica Teorica C-15, Universidad Autonoma de Madrid, Madrid, Spain
F. Barreiro, S. Calvente Lopez, A. Cueto, J. Del Peso, C. Glasman & J. Terron
Institut für Physik, Universität Mainz, Mainz, Germany
S. Artz, M. Becker, C. Bertella, W. Blum, V. Büscher, J. Cúth, A. Chr. Dudder, O. C. Endner, E. Ertel, F. Fiedler, E. Fullana Torregrosa, M. Geisen, S. Groh, T. Heck, K. B. Jakobi, A. Kaluza, M. Karnevskiy, K. Kleinknecht, L. Köpke, T. H. Lin, L. Masetti, J. Mattmann, C. Meyer, S. Moritz, V. Pleskot, S. Rave, A. Reiss, H. G. Sander, J. Schaeffer, U. Schäfer, C. Schmitt, S. Schmitz, M. Schott, N. Schuh, A. Schulte, E. Simioni, M. Simon, S. Tapprogge, P. Urrejola, S. Webb, E. Yildirim, C. Zimmermann & M. Zinser
School of Physics and Astronomy, University of Manchester, Manchester, UK
S. L. Barnes, R. Bielski, B. E. Cox, C. Da Via, N. S. Dann, G. T. Forcolin, A. Forti, J. M. Iturbe Ponce, X. Li, F. K. Loebinger, S. P. Marsden, J. Masik, F. J. Munoz Sanchez, T. J. Neep, A. Oh, R. Ospanov, J. R. Pater, R. F. Y. Peters, A. D. Pilkington, A. W. J. Pin, D. Price, Y. Qin, M. Queitsch-Maitland, J. A. Raine, H. Schweiger, S. M. Shaw, L. Tomlinson, S. Watts, F. Wilk, M. J. Woudstra & T. R. Wyatt
CPPM, Aix-Marseille Université and CNRS/IN2P3, Marseille, France
G. Aad, M. Alstaty, M. Barbero, A. Calandri, T. P. Calvet, Y. Coadou, C. Diaconu, F. Djama, V. Ellajosyula, L. Feligioni, A. Hadef, G. D. Hallewell, F. Hubaut, S. J. Kahn, E. B. F. G. Knoops, E. Le Guirriec, J. Liu, K. Liu, D. Madaffari, E. Monnier, S. Muanza, E. Nagy, P. Pralavorio, Y. Rodina, A. Rozanov, M. Talby, T. Theveneaux-Pelzer, R. E. Ticse Torres, S. Tisserant, J. Toth, F. Touchard, L. Vacavant & C. Wang
Department of Physics, University of Massachusetts, Amherst, MA, USA
M. Bellomo, N. R. Bernard, B. Brau, C. Dallapiccola, E. J. W. Moyse, P. Pais, N. E. Pettersson, A. Picazio & S. Willocq
Department of Physics, McGill University, Montreal, QC, Canada
C. Belanger-Champagne, A. J. Chuinard, F. Corriveau, R. A. Keyes, B. Lefebvre, R. Mantifel, S. Prince, S. H. Robertson, A. Robichaud-Veronneau, M. C. Stockton, M. Stoebe, B. Vachon, T. Vazquez Schroeder, K. Wang & A. Warburton
School of Physics, University of Melbourne, Melbourne, VIC, Australia
E. L. Barberio, A. J. Brennan, E. Dawe, S. Goldfarb, D. Jennens, T. Kubota, B. Le, E. F. McDonald, M. Milesi, F. Nuti, P. Rados, F. Scutti, L. A. Spiller, K. G. Tan, G. N. Taylor, P. T. E. Taylor, F. C. Ungaro, P. Urquijo, M. Volpi & D. Zanzi
Department of Physics, The University of Michigan, Ann Arbor, MI, USA
D. Amidei, M. A. Chelstowska, H. C. Cheng, T. Dai, E. B. Diehl, R. C. Edgar, H. Feng, C. Ferretti, P. Fleischmann, L. Guan, D. Levin, H. Liu, N. Lu, D. E. Marley, S. P. Mc Kee, A. McCarn, H. A. Neal, J. Qian, T. A. Schwarz, J. Searcy, K. Sekhon, Y. Wu, J. M. Yu, D. Zhang, B. Zhou & J. Zhu
Department of Physics and Astronomy, Michigan State University, East Lansing, MI, USA
G. Arabidze, R. Brock, A. Chegwidden, H. De la Torre, W. C. Fisher, G. Halladjian, R. Hauser, D. Hayden, J. Huston, B. Martin, M. C. Mondragon, P. Plucinski, B. G. Pope, B. D. Schoenrock, R. Schwienhorst & C. Willis
INFN Sezione di Milano, Milan, Italy
G. Alimonti, A. Andreazza, A. Camplani, L. Carminati, D. Cavalli, M. Citterio, G. Costa, M. Fanti, D. Giugni, T. Lari, M. Lazzaroni, L. Mandelli, S. Manzoni, S. M. Mazza, C. Meroni, S. Monzani, L. Perini, F. Ragusa, M. G. Ratti, S. Resconi, S. Shojaii, A. Stabile, G. F. Tartarelli, C. Troncon, R. Turra, M. Villaplana Perez & A. G. Zecchinelli
Dipartimento di Fisica, Università di Milano, Milan, Italy
A. Andreazza, A. Camplani, L. Carminati, M. Fanti, M. Lazzaroni, S. Manzoni, S. M. Mazza, S. Monzani, L. Perini, F. Ragusa, M. G. Ratti, S. Shojaii, R. Turra, M. Villaplana Perez & A. G. Zecchinelli
B.I. Stepanov Institute of Physics, National Academy of Sciences of Belarus, Minsk, Republic of Belarus
S. Harkusha, Y. Kulchitsky, Y. A. Kurochkin & P. V. Tsiareshka
National Scientific and Educational Centre for Particle and High Energy Physics, Minsk, Republic of Belarus
A. Hrynevich
Group of Particle Physics, University of Montreal, Montreal, QC, Canada
J-F. Arguin, G. Azuelos, T. R. V. Billoud, F. Dallaire, O. A. Ducu, L. G. Gagnon, L. Gauthier, C. Leroy, K. Mochizuki, T. Nguyen Manh, R. Rezvani & D. Shoaleh Saadi
P.N. Lebedev Physical Institute of the Russian, Academy of Sciences, Moscow, Russia
A. V. Akimov, I. L. Gavrilenko, A. A. Komar, R. Mashinistov, P. Yu. Nechaeva, A. Shmeleva, A. A. Snesarev, V. V. Sulin, V. O. Tikhomirov & K. Zhukov
Institute for Theoretical and Experimental Physics (ITEP), Moscow, Russia
A. Artamonov, P. A. Gorbounov, V. Khovanskiy, P. B. Shatalov & I. I. Tsukerman
National Research Nuclear University MEPhI, Moscow, Russia
A. Antonov, K. Belotskiy, N. L. Belyaev, O. Bulekov, V. A. Kantserov, D. Krasnopevtsev, A. Romaniouk, E. Shulga, S. Yu. Smirnov, Y. Smirnov, E. Yu. Soldatov, S. Timoshenko & K. Vorobev
D.V. Skobeltsyn Institute of Nuclear Physics, M.V. Lomonosov Moscow State University, Moscow, Russia
L. K. Gladilin, V. A. Kramarenko, A. Maevskiy, S. Yu. Sivoklokov & L. N. Smirnova
Fakultät für Physik, Ludwig-Maximilians-Universität München, Munich, Germany
S. Adomeit, M. Bender, O. Biebel, C. Bock, P. Calfayan, B. K. B. Chow, G. Duckeck, N. M. Hartmann, J. J. Heinrich, R. Hertenberger, F. Hoenig, F. Legger, J. Lorenz, P. J. Lösel, T. Maier, A. Mann, S. Mehlhase, C. Meineck, J. Mitrevski, R. S. P. Mueller, F. Rauscher, A. Ruschke, B. M. Schachtner, D. Schaile, C. Unverdorben, C. Valderanis, R. Walker & J. Wittkowski
Max-Planck-Institut für Physik (Werner-Heisenberg-Institut), Munich, Germany
T. Barillari, S. Bethke, G. Compostella, G. Cortiana, K. M. Ecker, M. J. Flowerdew, C. Giuliani, T. Ince, A. E. Kiryunin, S. Kluth, N. M. Koehler, O. Kortner, S. Kortner, H. Kroha, A. La Rosa, A. Macchiolo, A. A. Maier, T. G. McCarthy, S. Menke, F. Mueller, R. Nisius, S. Nowak, H. Oberlack, R. Richter, D. Salihagic, N. Savic, P. Schacht, K. R. Schmidt-Sommerfeld, F. Spettel, S. Stonjek, H. von der Schmitt & A. Wildauer
Nagasaki Institute of Applied Science, Nagasaki, Japan
T. Fusayasu & M. Shimojima
Graduate School of Science and Kobayashi-Maskawa Institute, Nagoya University, Nagoya, Japan
Y. Horii, K Kentaro, Y. Nakahama, K. Onogi, M. Tomoto, J. Wakabayashi & K. Yamauchi
INFN Sezione di Napoli, Naples, Italy
A. Aloisio, M. G. Alviggi, V. Canale, G. Carlino, F. Cirotto, F. Conventi, R. de Asmundis, M. Della Pietra, A. Doria, V. Izzo, L. Merola, S. Perrella, E. Rossi, A. Sanchez & G. Sekhniaidze
Dipartimento di Fisica, Università di Napoli, Naples, Italy
A. Aloisio, M. G. Alviggi, V. Canale, F. Cirotto, L. Merola, S. Perrella, E. Rossi & A. Sanchez
Department of Physics and Astronomy, University of New Mexico, Albuquerque, NM, USA
I. Gorelov, M. R. Hoeferkamp, N. C. Mc Fadden, S. C. Seidel, A. C. Taylor & K. Toms
Institute for Mathematics, Astrophysics and Particle Physics, Radboud University Nijmegen/Nikhef, Nijmegen, The Netherlands
S. Caron, L. Colasurdo, V. Croft, N. De Groot, F. Filthaut, C. Galea, A. C. König, S. Nektarijevic, J. F. P. Schouwenberg & A. Strubig
Nikhef National Institute for Subatomic Physics and University of Amsterdam, Amsterdam, The Netherlands
R. Aben, I. Angelozzi, M. Bedognetti, L. J. Beemster, S. Bentvelsen, D. Berge, G. J. Bobbink, K. Bos, L. Brenner, L. S. Bruni, P. Butti, R. Castelijn, A. Castelli, A. P. Colijn, P. de Jong, I. Deigaard, D. Duda, P. Ferrari, F. Hartjes, N. P. Hessey, O. Igonkina, P. Kluit, E. Koffeman, J. Mahlstedt, J. Meyer, K. P. Oussoren, G. Sabato, D. Salek, M. Slawinska, N. Valencic, W. Van Den Wollenberg, P. C. Van Der Deijl, H. van der Graaf, I. van Vulpen, P. Vankov, W. Verkerke, J. C. Vermeulen, M. Vreeswijk, H. Weits, S. Williams & T. M. H. Wolf
Department of Physics, Northern Illinois University, DeKalb, IL, USA
J. Adelman, E. Brost, B. Burghgrave, D. Chakraborty, P. Klimek & P. Saha
Budker Institute of Nuclear Physics, SB RAS, Novosibirsk, Russia
A. V. Anisenkov, E. M. Baldin, V. S. Bobrovnikov, A. G. Bogdanchikov, A. R. Buzykaev, V. F. Kazanin, A. G. Kharlamov, T. Kharlamova, A. A. Korol, A. L. Maslennikov, D. A. Maximov, S. V. Peleganchuk, O. L. Rezanova, A. M. Soukharev, A. A. Talyshev & Yu. A. Tikhonov
Department of Physics, New York University, New York, NY, USA
C. Becot, C. Bernius, K. Cranmer, A. Haas, L. Heinrich, B. Kaplan, K. Karthik, R. Konoplich, A. I. Mincer, P. Nemethy & R. M. Neves
Ohio State University, Columbus, OH, USA
J. B. Beacham, S. Che, K. K. Gan, R. Ishmukhametov, H. Kagan, R. D. Kass, K. A. Looper, S. Shrestha & B. B. Tannenwald
Faculty of Science, Okayama University, Okayama, Japan
I. Nakano
Homer L. Dodge Department of Physics and Astronomy, University of Oklahoma, Norman, OK, USA
B. Abbott, M. Alhroob, D. Bertsche, A. De Benedetti, P. Gutierrez, A. Hasib, S. Norberg, B. Pearson, O. Rifki, H. Severini, D. R. Shope, P. Skubic & M. Strauss
Department of Physics, Oklahoma State University, Stillwater, OK, USA
J. Cantero, J. Haley, D. O. Jamin, A. Khanov, F. Rizatdinova & D. Sidorov
Palacký University, RCPTM, Olomouc, Czech Republic
L. Chytka, P. Hamal, M. Hrabovsky, J. Kvita & L. Nozka
Center for High Energy Physics, University of Oregon, Eugene, OR, USA
R. Abreu, B. W. Allen, J. E. Brau, A. Dattagupta, W. H. Hopkins, S. Majewski, C. T. Potter, P. Radloff, N. B. Sinev, I. M. Snyder, D. M. Strom, E. Torrence, C. Wanotayaroj, K. Whalen & F. Winklmeier
LAL, Univ. Paris-Sud, CNRS/IN2P3, Université Paris-Saclay, Orsay, France
B. Abeloos, M. K. Ayoub, A. Bassalat, S. Binet, C. Bourdarios, J. B. De Vivie De Regie, D. Delgove, L. Duflot, M. Escalier, L. Fayard, D. Fournier, E. L. Gkougkousis, C. R. Goudet, J. -F. Grivaz, F. Hariri, S. Henrot-Versille, J. Hrivnac, L. Iconomidou-Fayard, M. Kado, A. Lounis, C. Maiani, N. Makovec, N. Morange, C. Nellist, P. Petroff, L. Poggioli, P. Puzo, D. Rousseau, G. Rybkin, A. C. Schaffer, L. Serin, S. Simion, R. Tanaka, D. Zerwas & Z. Zhang
Graduate School of Science, Osaka University, Osaka, Japan
N. Ishijima, M. Nomachi, Y. Sugaya, J. J. Teoh & Y. Yamaguchi
Department of Physics, University of Oslo, Oslo, Norway
M. K. Bugge, D. Cameron, J. R. Catmore, S. Feigl, L. Franconi, V. Garonne, B. K. Gjelsten, E. Gramstad, V. Morisbak, J. K. Nilsen, F. Ould-Saada, K. Pajchel, M. Pedersen, S. Raddum, A. L. Read, O. Røhne, H. Sandaker, C. Serfon, S. Stapnes & A. Strandlie
Department of Physics, Oxford University, Oxford, UK
G. Artoni, M. Backes, A. J. Barr, K. Becker, L. Beresford, D. Bortoletto, J. T. P. Burr, A. M. Cooper-Sarkar, M. Crispin Ortuzar, W. J. Fawcett, J. A. Frost, E. J. Gallas, F. Giuli, S. Gupta, C. Gwenlan, C. P. Hays, J. Henderson, T. B. Huffman, C. Issever, C. W. Kalderon, K. Nagai, R. B. Nickerson, N. Norjoharuddeen, M. Petrov, M. A. Pickering, V. Radescu, J. C-L. Tseng, G. H. A. Viehhauser, L. Vigani, A. R. Weidberg & J. Zhong
INFN Sezione di Pavia, Pavia, Italy
P. Dondero, E. M. Farina, R. Ferrari, M. Fraternali, G. Gaudio, G. Introzzi, A. Kourkoumeli-Charalampidi, A. Lanza, M. Livan, A. Negri, G. Polesello, D. M. Rebuzzi, A. Rimoldi & V. Vercesi
Dipartimento di Fisica, Università di Pavia, Pavia, Italy
P. Dondero, E. M. Farina, M. Fraternali, G. Introzzi, A. Kourkoumeli-Charalampidi, M. Livan, A. Negri, D. M. Rebuzzi & A. Rimoldi
Department of Physics, University of Pennsylvania, Philadelphia, PA, USA
W. K. Balunas, K. Brendlinger, W. K. Di Clemente, R. R. M. Fletcher, B. Haney, S. Heim, E. Hines, B. Jackson, J. Kroll, E. Lipeles, J. Machado Miguens, C. Meyer, K. P. Mistry, J. Reichert, L. Schaefer, E. Thomson, R. Vanguri, H. H. Williams & K. Yoshihara
National Research Centre “Kurchatov Institute” B.P. Konstantinov Petersburg Nuclear Physics Institute, St. Petersburg, Russia
A. Basalaev, A. Ezhilov, O. L. Fedin, V. Gratchev, M. Levchenko, V. P. Maleev, I. Naryshkin, Y. F. Ryabov, V. A. Schegelsky, D. M. Seliverstov & V. Solovyev
INFN Sezione di Pisa, Pisa, Italy
A. Annovi, F. Bertolucci, N. V. Biesuz, V. Cavasinni, G. Chiarelli, T. Del Prete, M. Dell’Orso, S. Donati, P. Giannetti, S. Leone, C. Roda, F. Scuri, C. L. Sotiropoulou, M. Spalla & G. Volpi
Dipartimento di Fisica E. Fermi, Università di Pisa, Pisa, Italy
A. Annovi, F. Bertolucci, N. V. Biesuz, V. Cavasinni, G. Chiarelli, T. Del Prete, M. Dell’Orso, S. Donati, P. Giannetti, S. Leone, C. Roda, F. Scuri, C. L. Sotiropoulou, M. Spalla & G. Volpi
Department of Physics and Astronomy, University of Pittsburgh, Pittsburgh, PA, USA
R. M. Bianchi, J. Boudreau, C. Escobar, C. Farina, T. M. Hong, J. Mueller, K. Sapp & J. Su
Laboratório de Instrumentação e Física Experimental de Partículas-LIP, Lisbon, Portugal
J. A. Aguilar-Saavedra, S. P. Amor Dos Santos, A. Amorim, J. P. Araque, J. Carvalho, N. F. Castro, P. Conde Muiño, M. J. Da Cunha Sargedas De Sousa, M. C. N. Fiolhais, B. Galhardo, A. Gomes, R. Gonçalo, P. M. Jorge, A. Maio, J. Maneira, L. F. Oleiro Seabra, A. Onofre, R. Pedro, H. Santos, J. G. Saraiva, J. Silva, A. Tavares Delgado, F. Veloso & H. Wolters
Faculdade de Ciências, Universidade de Lisboa, Lisbon, Portugal
A. Amorim, P. Conde Muiño, M. J. Da Cunha Sargedas De Sousa, A. Gomes, P. M. Jorge, J. Machado Miguens, A. Maio, J. Maneira, R. Pedro & A. Tavares Delgado
Department of Physics, University of Coimbra, Coimbra, Portugal
S. P. Amor Dos Santos, J. Carvalho, M. C. N. Fiolhais, B. Galhardo, F. Veloso & H. Wolters
Centro de Física Nuclear da Universidade de Lisboa, Lisbon, Portugal
A. Gomes, A. Maio, J. G. Saraiva & J. Silva
Departamento de Fisica, Universidade do Minho, Braga, Portugal
A. Onofre
Departamento de Fisica Teorica y del Cosmos and CAFPE, Universidad de Granada, Granada, Spain
B. S. Acharya, J. A. Aguilar-Saavedra & M. Pinamonti
Institute of Physics, Academy of Sciences of the Czech Republic, Prague, Czech Republic
J. Chudoba, M. Havranek, J. Hejbal, T. Jakoubek, O. Kepka, A. Kupco, V. Kus, M. Lokajicek, R. Lysak, M. Marcisovsky, M. Mikestikova, S. Nemecek, O. Penc, P. Sicho, P. Staroba, M. Svatos, M. Tasevsky & V. Vrba
Czech Technical University in Prague, Prague, Czech Republic
B. Ali, K. Augsten, D. Caforio, P. Gallus, Z. Hubacek, M. Myska, S. Pospisil, F. Seifert, V. Simak, T. Slavicek, K. Smolek, M. Solar, A. Sopczak, V. Sopko, M. Suk, D. Turecek, V. Vacek, M. Vlasak, P. Vokac, Z. Vykydal & M. Zeman
Faculty of Mathematics and Physics, Charles University in Prague, Prague, Czech Republic
P. Berta, I. Carli, T. Davidek, J. Dolejsi, Z. Dolezal, P. Kodys, T. Kosek, R. Leitner, M. Mlynarikova, P. Reznicek, D. Scheirich, R. Slovak, M. Spousta, T. Sykora, P. Tas, S. Todorova-Nova, S. Valkar & V. Vorobel
State Research Center Institute for High Energy Physics (Protvino), NRC KI, Protvino, Russia
A. Borisov, E. Cheremushkina, S. P. Denisov, R. M. Fakhrutdinov, A. B. Fenyuk, D. Golubkov, A. Kamenshchikov, A. N. Karyukhin, A. S. Kozhin, A. A. Minaenko, A. G. Myagkov, V. Nikolaenko, A. Ryzhov, A. A. Solodkov, O. V. Solovyanov, E. A. Starchenko, A. Vaniachine, A. M. Zaitsev & O. Zenin
Particle Physics Department, Rutherford Appleton Laboratory, Didcot, UK
T. Adye, J. T. Baines, B. M. Barnett, S. Burke, A. Dewhurst, J. Dopke, D. Emeliyanov, B. J. Gallop, C. N. P. Gee, S. J. Haywood, J. Kirk, S. Martin-Haugh, S. J. McMahon, R. P. Middleton, W. J. Murray, P. W. Phillips, D. P. C. Sankey, C. Sawyer, M. Tyndel, F. J. Wickens, M. Wielers & S. D. Worm
INFN Sezione di Roma, Rome, Italy
F. Anulli, P. Bagiacchi, P. Bagnaia, M. Bauce, C. Bini, G. Ciapetti, M. Corradi, D. De Pedis, A. De Salvo, C. Di Donato, S. Falciano, S. Gentile, S. Giagu, G. Gustavino, M. Kuna, F. Lacava, C. Luci, L. Luminari, A. Messina, A. Nisati, E. Pasqualucci, E. Petrolo, L. Pontecorvo, M. Rescigno, S. Rosati, F. Safai Tehrani, M. Vanadia, R. Vari, S. Veneziano, M. Verducci & L. Zanello
Dipartimento di Fisica, Sapienza Università di Roma, Rome, Italy
P. Bagiacchi, P. Bagnaia, M. Bauce, C. Bini, G. Ciapetti, M. Corradi, C. Di Donato, S. Gentile, S. Giagu, G. Gustavino, M. Kuna, F. Lacava, C. Luci, A. Messina, M. Vanadia, M. Verducci & L. Zanello
INFN Sezione di Roma Tor Vergata, Rome, Italy
G. Aielli, P. Camarri, R. Cardarelli, L. Cerrito, A. Di Ciaccio, R. Iuppa, B. Liberti, A. Salamon & R. Santonico
Dipartimento di Fisica, Università di Roma Tor Vergata, Rome, Italy
G. Aielli, P. Camarri, L. Cerrito, A. Di Ciaccio, R. Iuppa, A. Salamon & R. Santonico
INFN Sezione di Roma Tre, Rome, Italy
A. Baroncelli, M. Biglietti, F. Ceradini, B. Di Micco, A. Farilla, E. Graziani, M. Iodice, D. Orestano, F. Petrucci, D. Puddu, G. Salamanna, M. Sessa, C. Stanescu & C. Taccini
Dipartimento di Matematica e Fisica, Università Roma Tre, Rome, Italy
F. Ceradini, B. Di Micco, D. Orestano, F. Petrucci, D. Puddu, G. Salamanna, M. Sessa & C. Taccini
Faculté des Sciences Ain Chock, Réseau Universitaire de Physique des Hautes Energies-Université Hassan II, Casablanca, Morocco
D. Benchekroun, A. Chafaq & A. Hoummada
Faculté des Sciences Semlalia, Université Cadi Ayyad, LPHEA-Marrakech, Marrakech, Morocco
M. El Kacimi & D. Goujdami
Faculté des Sciences, Université Mohamed Premier and LPTPM, Oujda, Morocco
M. Aaboud, J. E. Derkaoui & M. Ouchrif
Faculté des Sciences, Université Mohammed V, Rabat, Morocco
R. Cherkaoui El Moursli, M. Ezzi, F. Fassi, N. Haddad, Z. Idrissi & Y. Tayalati
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
H. Bachacou, F. Balli, F. Bauer, N. Besson, J. -B. Blanchard, M. Boonekamp, L. Chevalier, M. Dano Hoffmann, F. Deliot, D. Denysiuk, A. I. Etienvre, A. Formica, P. F. Giraud, J. Goncalves Pinto Firmino Da Costa, C. Guyot, R. Hanna, S. Hassani, F. Jeanneau, O. Kivernyk, W. Kozanecki, R. Kukla, E. Lançon, J. F. Laporte, E. P. Le Quilleuc, A. A. J. Lesage, B. Mansoulie, J-P. Meyer, R. Nicolaidou, A. Ouraou, L. Pacheco Rodriguez, M. M. Perego, A. Peyaud, M. Saimpert, L. Schoeffel, Ph. Schune, Ph. Schwemling & J. Schwindling
Santa Cruz Institute for Particle Physics, University of California Santa Cruz, Santa Cruz, CA, USA
O. S. AbouZeid, M. Battaglia, C. Debenedetti, A. A. Grillo, M. Hance, A. Kuhl, A. T. Law, A. M. Litke, W. S. Lockman, J. Nielsen, R. Reece, P. Rose, H. F-W. Sadrozinski, S. Schier, B. A. Schumm & A. Seiden
Department of Physics, University of Washington, Seattle, WA, USA
C. Alpigiani, D. Blackburn, A. G. Goussiou, S. -C. Hsu, W. J. Johnson, H. J. Lubatti, M. Marx, S. Meehan, N. Rompotis, R. Rosten, J. Rothberg, H. L. Russell, P. H. Sales De Bruin, E. Torró Pastor, G. Watts & N. L. Whallon
Department of Physics and Astronomy, University of Sheffield, Sheffield, UK
C. Anastopoulos, D. Costanzo, T. Cuhadar Donszelmann, I. Dawson, G. T. Fletcher, G. N. Hamity, M. C. Hodgkinson, P. Hodgson, P. Johansson, J. A. Klinger, E. V. Korolkova, D. Kyriazopoulos, B. Lopez Paredes, C. M. Macdonald, P. S. Miyagawa, K. A. Parker, D. R. Tovey, T. Vickey & O. E. Vickey Boeriu
Department of Physics, Shinshu University, Nagano, Japan
Y. Hasegawa & T. Takeshita
Fachbereich Physik, Universität Siegen, Siegen, Germany
N. B. Atlay, P. Buchholz, A. Campoverde, H. Czirr, I. Fleck, S. Ghasemi, I. Ibragimov, Y. Li, W. Walkowiak & M. Ziolkowski
Department of Physics, Simon Fraser University, Burnaby, BC, Canada
Q. Buat, A. J. Horton, D. Mori, D. C. O’Neil, K. Pachal, B. Stelzer, D. Temple, H. Torres, J. Van Nieuwkoop & M. C. Vetterli
SLAC National Accelerator Laboratory, Stanford, CA, USA
A. J. Armbruster, T. Barklow, R. Bartoldus, H. S. Bawa, J. E. Black, Y. S. Gao, N. Garelli, P. Grenier, N. Ilic, M. Kagan, M. Kocian, T. Koi, C. Malone, J. Moss, R. Mount, B. P. Nachman, G. Piacquadio, F. Rubbo, A. Salnikov, A. Schwartzman, D. Su, L. Tompkins, M. Wittgen, C. Young & Q. Zeng
Faculty of Mathematics, Physics and Informatics, Comenius University, Bratislava, Slovak Republic
R. Astalos, P. Bartos, T. Blazek, T. Dado, M. Melo, L. Plazak, J. Smiesko, I. Sykora, S. Tokár & T. Ženiš
Department of Subnuclear Physics, Institute of Experimental Physics of the Slovak Academy of Sciences, Kosice, Slovak Republic
D. Bruncko, E. Kladiva, P. Strizenec & J. Urban
Department of Physics, University of Cape Town, Cape Town, South Africa
E. Castaneda-Miranda, A. Hamilton & S. Yacoob
Department of Physics, University of Johannesburg, Johannesburg, South Africa
S. H. Connell & N. Govender
School of Physics, University of the Witwatersrand, Johannesburg, South Africa
C. Hsu, H. Jivan, D. Kar, B. R. Mellado Garcia & X. Ruan
Department of Physics, Stockholm University, Stockholm, Sweden
Y. Abulaiti, H. Akerstedt, B. Åsman, K. Bendtz, G. Bertoli, O. Bessidskaia Bylund, C. Bohm, C. Clement, W. A. Cribbs, K. Gellerstedt, S. Hellman, K. Jon-And, O. Lundberg, D. A. Milstead, T. Moa, S. Molander, P. Pani, R. Poettgen, V. Rossetti, N. W. Shaikh, A. Shcherbakova, S. B. Silverstein, J. Sjölin, S. Strandberg, M. Ughetto, E. Valdes Santurio & V. Wallangen
The Oskar Klein Centre, Stockholm, Sweden
Y. Abulaiti, H. Akerstedt, B. Åsman, K. Bendtz, G. Bertoli, O. Bessidskaia Bylund, C. Clement, W. A. Cribbs, K. Gellerstedt, S. Hellman, K. Jon-And, O. Lundberg, D. A. Milstead, T. Moa, S. Molander, P. Pani, R. Poettgen, V. Rossetti, N. W. Shaikh, A. Shcherbakova, J. Sjölin, S. Strandberg, M. Ughetto, E. Valdes Santurio & V. Wallangen
Physics Department, Royal Institute of Technology, Stockholm, Sweden
B. Lund-Jensen, P. E. Sidebo & J. Strandberg
Departments of Physics and Astronomy and Chemistry, Stony Brook University, Stony Brook, NY, USA
T. Balestri, C. P. Bee, K. Chen, J. Hobbs, P. Huo, J. Jia, H. Li, B. E. Lindquist, R. L. McCarthy, A. Montalbano, L. Morvaj, S. K. Radhakrishnan, M. Rijssenbeek, R. D. Schamberger, D. Tsybychev, A. Zaman & M. Zhou
Department of Physics and Astronomy, University of Sussex, Brighton, UK
N. L. Abraham, B. M. M. Allbrooke, L. Asquith, A. Cerri, C. A. Chavez Barajas, U. De Sanctis, A. De Santo, G. Lerner, F. Miano, F. Salvatore, I. Santoyo Castillo, C. Y. Shehu, K. Suruliz, M. R. Sutton, I. Vivarelli & O. J. Winston
School of Physics, University of Sydney, Sydney, Australia
C. W. Black, K. D. Finelli, G. -Y. Jeng, A. Limosani, A. K. Morley, A. F. Saavedra, M. Scarcella, K. E. Varvell, J. Wang & B. Yabsley
Institute of Physics, Academia Sinica, Taipei, Taiwan
S. Hou, P. J. Hsu, S. C. Lee, S. C. Lin, B. Liu, D. Liu, F. Lo Sterzo, R. Mazini, L. Shi, D. A. Soh, P. K. Teng, S. M. Wang & Y. Yang
Department of Physics, Technion: Israel Institute of Technology, Haifa, Israel
H. Abreu, E. Gozani, Y. Rozen, S. Tarem & N. van Eldik
Raymond and Beverly Sackler School of Physics and Astronomy, Tel Aviv University, Tel Aviv, Israel
H. Abramowicz, G. Alexander, A. Ashkenazi, G. Bella, O. Benary, Y. Benhammou, M. Davies, J. Duarte-Campderros, E. Etzion, A. Gershon, O. Gueta, Y. Oren, A. Soffer & N. Taiblum
Department of Physics, Aristotle University of Thessaloniki, Thessaloníki, Greece
C. Gentsos, S. Gkaitatzis, I. Gkialas, D. Iliadis, N. Kimura, K. Kordas, A. Leisos, K. Papageorgiou, C. Petridou & D. Sampsonidis
International Center for Elementary Particle Physics and Department of Physics, The University of Tokyo, Tokyo, Japan
S. Adachi, S. Asai, S. Chen, Y. Enari, K. Hanawa, M. Ishino, N. Kanaya, Y. Kataoka, C. Kato, T. Kawamoto, T. Kishimoto, A. Kobayashi, T. Kobayashi, Y. Komori, C. Kozakai, T. Mashimo, T. Masubuchi, Y. Minami, Y. Minegishi, T. Mori, M. Morinaga, T. Nakamura, Y. Ninomiya, T. Nobe, Y. Okumura, T. Saito, H. Sakamoto, J. Tanaka, K. Terashi, I. Ueda, S. Yamamoto & T. Yamanaka
Graduate School of Science and Technology, Tokyo Metropolitan University, Tokyo, Japan
U. Bratzler & C. Fukunaga
Department of Physics, Tokyo Institute of Technology, Tokyo, Japan
D. Hayakawa, M. Ishitsuka, O. Jinnouchi, D. Kobayashi, M. Kuze, K. Motohashi, M. Tanaka, K. Todome & D. Yamaguchi
Department of Physics, University of Toronto, Toronto, ON, Canada
S. J. Batista, C. C. Chau, K. J. R. Cormier, D. A. DeMarco, R. Di Sipio, M. Diamond, H. Keoshkerian, P. Krieger, A. Liblong, G. Mc Goldrick, R. S. Orr, V. R. Pascuzzi, R. Polifka, M. S. Rudolph, P. Savard, P. Sinervo, J. Taenzer, R. J. Teuscher, W. Trischuk, L. M. Veloce & N. Venturi
TRIUMF, Vancouver, BC, Canada
A. Canepa, S. V. Chekulaev, N. Hod, J. Jovicevic, E. Perez Codina, B. Schneider, O. Stelzer-Chilton, R. Tafirout & I. M. Trigger
Department of Physics and Astronomy, York University, Toronto, ON, Canada
J. Manjarres Ramos, G. Palacino & W. Taylor
Faculty of Pure and Applied Sciences, and Center for Integrated Research in Fundamental Science and Engineering, University of Tsukuba, Tsukuba, Japan
M. Hagihara, K. Hara, F. Ito, K. Kasahara, S. H. Kim, K. Kiuchi, K. Nagata, H. Okawa, K. Sato & F. Ukegawa
Department of Physics and Astronomy, Tufts University, Medford, MA, USA
P. H. Beauchemin, E. Meoni, K. Sliwa, H. Son & J. Wetter
Department of Physics and Astronomy, University of California Irvine, Irvine, CA, USA
D. W. Casper, T. Colombo, A. Corso-Radu, M. Frate, D. Guest, A. J. Lankford, A. S. Mete, A. Nelson, K. Ntekas, D. A. Scannicchio, M. Schernau, C. O. Shimmin, A. Taffard, G. Unel & D. Whiteson
INFN Gruppo Collegato di Udine, Sezione di Trieste, Udine, Italy
A. S. Boldyrev, S. Cheatham, M. Cobal, M. P. Giordani, W. B. Quayle, L. Serkin, K. Shaw, R. Soualah & L. Truong
ICTP, Trieste, Italy
W. B. Quayle, L. Serkin & K. Shaw
Dipartimento di Chimica Fisica e Ambiente, Università di Udine, Udine, Italy
A. S. Boldyrev, S. Cheatham, M. Cobal, M. P. Giordani, R. Soualah & L. Truong
Department of Physics and Astronomy, University of Uppsala, Uppsala, Sweden
E. Bergeaas Kuutmann, R. Brenner, T. Ekelof, M. Ellert, A. Ferrari, H. J. Maddocks, H. Ohman & C. Rangel-Smith
Department of Physics, University of Illinois, Urbana, IL, USA
M. Atkinson, R. Caminal Armadans, V. Cavaliere, P. Chang, S. Errede, B. H. Hooberman, M. Khader, K. Lie, T. M. Liss, L. Liu, J. D. Long, V. I. Martinez Outschoorn, M. S. Neubauer, M. Rybar, R. Shang, A. M. Sickles, I. Vichou & J. C. Zeng
Instituto de Fisica Corpuscular (IFIC) and Departamento de Fisica Atomica, Molecular y Nuclear and Departamento de Ingeniería Electrónica and Instituto de Microelectrónica de Barcelona (IMB-CNM), University of Valencia and CSIC, Valencia, Spain
D. Álvarez Piqueras, L. Barranco Navarro, S. Cabrera Urbán, V. Castillo Gimenez, L. Cerda Alberich, M. J. Costa, P. Fernandez Martinez, A. Ferrer, L. Fiorini, J. Fuster, C. García, J. E. García Navarro, S. González de la Hoz, Y. Hernández Jiménez, E. Higón-Rodriguez, J. Jimenez Pena, M. King, C. Lacasta, V. R. Lacuesta, J. Mamuzic, S. Marti-Garcia, D. Melini, V. A. Mitsou, S. Pedraza Lopez, D. Rodriguez Rodriguez, E. Romero Adam, E. Ros, J. Salt, J. Sánchez, V. Sanchez Martinez, U. Soldevila, A. Valero, J. A. Valls Ferrer & M. Vos
Department of Physics, University of British Columbia, Vancouver, BC, Canada
M. Danninger, W. Fedorko, C. Gay, Z. Gecse, M. Gignac, S. Henkelmann & A. Lister
Department of Physics and Astronomy, University of Victoria, Victoria, BC, Canada
J. Albert, C. David, A. A. Elliot, M. Fincke-Keeler, K. Hamano, E. Hill, R. Keeler, R. Kowalewski, E. S. Kuwertz, T. Kwan, M. LeBlanc, M. Lefebvre, R. A. McPherson, J. Pearce, R. Seuster, R. Sobie, M. Trovatelli & M. Venturi
Department of Physics, University of Warwick, Coventry, UK
M. Beckingham, J. S. Ennis, S. M. Farrington, P. F. Harrison, C. Jeske, G. Jones, T. A. Martin, W. J. Murray, E. Pianori & M. Spangenberg
Waseda University, Tokyo, Japan
T. Iizawa, T. Kaji, T. Mitani, Y. Sakurai & K. Yorita
Department of Particle Physics, The Weizmann Institute of Science, Rehovot, Israel
P. Balek, S. Bressler, Z. H. Citron, E. Duchovni, M. Dumancic, E. Gross, M. K. Köhler, D. Lellouch, L. J. Levinson, G. Mikenberg, A. Milov, M. Pitt, I. Ravinovich, I. Roth, J. Schaarschmidt, V. Smakhtin & D. Turgeman
Department of Physics, University of Wisconsin, Madison, WI, USA
Sw. Banerjee, W. Guan, A. S. Hard, Y. Heng, H. Ji, X. Ju, L. S. Kaplan, L. Kashif, A. Kruse, Y. Ming, F. Wang, W. Wiedenmann, S. L. Wu, H. Yang, F. Zhang & G. Zobernig
Fakultät für Physik und Astronomie, Julius-Maximilians-Universität, Würzburg, Germany
V. Herget, F. Kuger, A. Redelbach, M. Schreyer, O. Sidiropoulou, G. Siragusa, R. Ströhmer, T. Trefzger, S. W. Weber & A. Zibell
Fakultät für Mathematik und Naturwissenschaften, Fachgruppe Physik, Bergische Universität Wuppertal, Wuppertal, Germany
A. A. E. Bannoura, D. Boerner, H. M. Braun, T. Cornelissen, F. Ellinghaus, G. Ernis, J. Fischer, T. Flick, O. Gabizon, G. Gilles, K. Hamacher, T. Harenberg, D. Hirschbuehl, S. Kersten, J. T. Kuechler, P. Mättig, M. Neumann, S. Pataraia, C. J. Riegel, M. Sandhoff, F. Tepel, M. Vogel, W. Wagner & C. Zeitnitz
Department of Physics, Yale University, New Haven, CT, USA
O. K. Baker, E. Benhar Noccioli, J. Cummings, S. Demers, E. Ideal, T. Lagouri, A. G. Leister, A. Loginov, M. Paganini, D. Paredes Hernandez, L. A. Thomsen, P. Tipton, J. G. Vasquez & X. Wang
Yerevan Physics Institute, Yerevan, Armenia
H. Hakobyan & G. Vardanyan
Centre de Calcul de l’Institut National de Physique Nucléaire et de Physique des Particules (IN2P3), Villeurbanne, France
G. Rahal
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Open Access This article is distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution, and reproduction in any medium, provided you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made.
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Aaboud, M., Aad, G., Abbott, B. et al. Search for supersymmetry in a final state containing two photons and missing transverse momentum in \(\varvec{\sqrt{s}}\) = 13 TeV \(\varvec{pp}\) collisions at the LHC using the ATLAS detector. Eur. Phys. J. C 76, 517 (2016). https://doi.org/10.1140/epjc/s10052-016-4344-x
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DOI: https://doi.org/10.1140/epjc/s10052-016-4344-x
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