Abstract
The results of a search for the production of second generation scalar leptoquarks are presented for final states consisting of either two muons and at least two jets or a muon plus missing transverse momentum and at least two jets. A total of 1.03 fb−1 integrated luminosity of proton-proton collision data produced by the Large Hadron Collider at \(\sqrt{s}=7~\mbox{TeV}\) and recorded by the ATLAS detector is used for the search. The event yields in the signal regions are found to be consistent with the Standard Model background expectations. The production of second generation leptoquarks is excluded for a leptoquark mass m LQ<594 (685) GeV at 95 % confidence level, for a branching ratio of 0.5 (1.0) for leptoquark decay to a muon and a quark.
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Searches for scalar leptoquarks in pp collisions at \(\varvec{\sqrt{s}}\) = 8 TeV with the ATLAS detector
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1 Introduction
The remarkable similarities between quarks and leptons in the Standard Model (SM) lead to the supposition that there could be a fundamental relationship between them at a sufficiently high energy scale, manifested by the existence of leptoquarks (LQ) [1–8]. LQs are hypothetical particles which carry both baryon and lepton number and have fractional electrical charge. The present search is performed within the minimal Buchmüller-Rückl-Wyler model [9], where LQs are restricted to couple to quarks and leptons of one generation. In this model, LQs are required to have pure chiral couplings to SM fermions in order to avoid inducing four-fermion interactions that would cause flavour-changing neutral currents and lepton family-number violations. At the Large Hadron Collider (LHC), scalar LQs can be produced either in pairs or singly. Single LQ production involves the unknown λ LQ−ℓ−q coupling, while pair production of scalar LQs occurs mostly via gluon-gluon fusion, dominant for m LQ≲1 TeV, and \(q\overline{q}\)-annihilation, dominant at larger masses. Both pair-production modes involve only the strong coupling constant, and therefore all model dependence is contained in the assumed LQ mass m LQ and the branching ratio β for LQ decay to a charged lepton and a quark.Footnote 1 LQs can also decay to a neutrino and a quark; in this case, the branching ratio is 1−β. Pair production of scalar LQs at the LHC has been calculated at next-to-leading order (NLO) [11].
The results presented in this paper are an update of the previous ATLAS search for second generation LQs [12] and extend the bounds arising from previous direct searches performed by CMS [13], ATLAS [12], D0 [14] and OPAL [15]. A total integrated luminosity of 1.03 fb−1 of proton-proton collision data at a centre of mass energy \(\sqrt{s}=7~\mbox{TeV}\), collected with the ATLAS detector from March through July 2011, is used for the search. The final states arising from leptoquark pairs decaying into two muons and two quarks (μμjj), or into a muon, a neutrino and two quarks (μνjj), are considered. These result in experimental signatures of either two high transverse momentum (p T) muons and two high p T jets, or one high p T muon, missing transverse momentum, and two high p T jets.
Analyses for both dimuon and single muon final states start with the selection of event samples with large signal acceptance. Since background cross sections are several orders of magnitude larger than the signal cross sections, these samples are dominated by the major backgrounds: Z+jets and \(t\bar{t}\) in the μμjj case, and W+jets and \(t\bar{t}\) for the μνjj case. Further selection requirements are then applied to these samples to define control regions used to determine the normalization of the aforementioned backgrounds. The determination of the multi-jet background is performed in a fully data-driven approach, and the smaller diboson and single top-quark backgrounds are estimated using Monte Carlo (MC) simulations.
After all background contributions are determined, variables selected to enhance the discrimination between signal and background are combined into a log likelihood ratio, which is used to search for an excess of events over the SM background prediction. The searches are performed independently for each final state. The results are then combined and interpreted as lower bounds on the LQ mass for different β hypotheses.
2 The ATLAS detector
The ATLAS detector [16] is a multi-purpose detector with a forward-backward symmetric cylindrical geometry and nearly 4π coverage in solid angle.Footnote 2
The three major sub-components of ATLAS are the tracking detectors, the calorimeters and the muon spectrometer. Charged particle tracks and vertices are reconstructed with silicon-based tracking detectors that cover |η|<2.5 and a transition radiation tracker extending to |η|<2.0. The inner tracking system is immersed in a homogeneous 2 T axial magnetic field provided by a solenoid. Electron, photon, and jet energies are measured in the calorimeters. The calorimeter system is segmented into a central barrel and two endcaps, collectively covering the pseudorapidity range of |η|<4.9. A liquid-argon (LAr) electromagnetic calorimeter covers the range |η|<3.2 and an iron-scintillator tile hadronic calorimeter covers the range |η|<1.7. Endcap and forward LAr calorimeters provide both electromagnetic and hadronic measurements and cover the region 1.5<|η|<4.9.
Surrounding the calorimeters, a muon spectrometer [16] with air-core toroids, a system of precision tracking chambers, and detectors with triggering capabilities provides muon identification and precise momentum measurements. The muon spectrometer is based on three large superconducting toroids with coils arranged in an eight-fold symmetry around the calorimeters, covering a range of |η|<2.7. Over most of the η range, precision measurements of the track coordinates in the principal bending direction of the magnetic field are provided by Monitored Drift Tubes (MDTs). At large pseudorapidities (2.0<|η|<2.7), Cathode Strip Chambers (CSCs) with higher granularity are used in the innermost station.
A three-level trigger system selects events to be recorded for offline analysis. The muon trigger detectors consist of Resistive Plate Chambers (RPCs) in the barrel (|η|<1.05) and Thin Gap Chambers (TGCs) in the end-cap regions (1.05<|η|<2.4), with a small overlap in the |η|=1.05 region. The data considered in this analysis are selected from events containing at least one muon with the transverse momentum determined by the trigger system satisfying p T>18 GeV.
3 Simulated samples
Simulated event samples are used to determine all signal and some of the background yields. Signal samples for LQ masses between 200 GeV and 1000 GeV are simulated with PYTHIA 6.4.25 [17]. NLO cross sections as determined in Ref. [11], using CTEQ6.6 [18] parton distribution functions (PDFs), are used to normalize the samples at each mass point.
Samples of W and Z/γ ⋆ production in association with n partons (where n can be 0, 1, 2, 3, 4 and 5 or more) are simulated with the ALPGEN [19] generator interfaced to HERWIG [20] and JIMMY [21] to model parton showers and multiple parton interactions, respectively. The MLM [19] parton-shower matching scheme is used to form inclusive W/Z+jets samples. MC@NLO [22, 23] is used to estimate the production of single top quarks and top quark pairs. A top quark mass of 172.5 GeV is used in the simulation. Diboson events are generated using HERWIG, and the cross sections are scaled to NLO calculations [22–24].
All simulated events are passed through a full detector simulation based on GEANT4 [25] and then reconstructed with the same software chain as the data [26]. During the data-taking period considered in this search, the mean number of primary proton-proton interactions per bunch crossing was approximately six. The effect of this pile-up is taken into account in the analysis by overlaying simulated minimum bias events onto the simulated hard-scattering events. The MC samples are then reweighted such that the average number of pile-up interactions matches that seen in the data.
4 Object and event selection
Collision events are identified by requiring at least one reconstructed primary vertex candidate with at least three associated tracks with p T,track>0.4 GeV. If two or more such vertices are found, the one with the largest sum of \(p_{\mathrm{T}, \mathrm{track}}^{\mathrm{2}}\) is taken to be the primary vertex. Muons are reconstructed by matching tracks in the inner detector to track segments in the muon spectrometers, as described in Ref. [27]. In addition to the track quality requirements imposed for identification, the muon tracks must also satisfy |d 0|<0.1 mm and |z 0|<5 mm, where d 0 and z 0 are the transverse and longitudinal impact parameters measured with respect to the primary vertex. All selected muons must have p T>30 GeV and are restricted to be within |η|<2.4. Muon candidates must pass the isolation requirement \(p^{\mathrm{cone20}}_{\mathrm{T}}/p_{\mathrm{T}} < 0.2\), where \(p^{\mathrm{cone20}}_{\mathrm{T}}\) is the sum of the p T of the tracks within \(\varDelta R = \sqrt {(\varDelta \phi)^{2} + (\varDelta \eta^{2})} < 0.2\) of the muon track, excluding the muon p T contribution. Selected events must have at least one muon identified by the trigger system within a cone ΔR<0.1 centered on a selected muon.
Jets are reconstructed from calorimeter energy clusters using the anti-k t algorithm [29, 30] with a radius parameter R=0.4. Corrections are applied in order to account for the effects of the non-compensating calorimeter, upstream material and other effects, by using p T and η-dependent correction factors derived from simulation and validated with test-beam [31] and collision data studies [32]. After applying quality requirements based on shower shape and signal timing with respect to the beam crossing, the selected jets must satisfy p T>30 GeV, |η|<2.8 and must be separated from the selected candidate muons by ΔR≥0.4. The presence of neutrinos is inferred from the missing transverse momentum \(E^{\mathrm{miss}}_{\mathrm{T}}\), defined as the magnitude of the negative vector sum of the transverse momenta of reconstructed electrons, muons and jets, as well as calorimeter energy deposits not associated to reconstructed objects.
Corrections to the muon trigger and reconstruction efficiencies and to the momentum resolution are applied to the simulated events so that their kinematic distributions match those observed in data, with an impact on the predicted number of events of less than 2 %. These corrections are derived from samples of Z→μμ and W→μν decays [27], taking into account the effects of multiple scattering and the intrinsic resolution of the muon spectrometer [28]. In order to validate the corrections at high p T, the alignment of the muon spectrometer, which dominates the momentum resolution for p T larger than approximately 200 GeV, is derived from a sample of straight track data taken in special runs with the toroids turned off, resulting in agreement within the considered systematic uncertainties.
Events selected for this search are required to contain either exactly two muons and at least two jets for the μμjj final state, or exactly one muon, at least two jets and \(E^{\mathrm{miss}}_{\mathrm{T}}> 30~\mbox{GeV}\) for the μνjj final state. In the μμjj channel, only events with m μμ>40 GeV are considered. In the μνjj channel, events are required to have \(m_{\mathrm{T}}=\sqrt{2p^{\mu}_{\mathrm{T}}E^{\mathrm{miss}}_{\mathrm{T}}(1-\cos(\varDelta \phi))}>40~\mbox{GeV}\), where Δϕ is the angle between the muon and the \(E^{\mathrm{miss}}_{\mathrm{T}}\) direction in the plane perpendicular to the beam. Events with identified electrons as defined in Ref. [33], with p T>30 GeV, and |η|<2.47 are rejected. After all the selection criteria are applied the acceptance times efficiency ranges from about 60 % (55 %) for a LQ signal of m LQ=300 GeV to 65 % (60 %) for a LQ signal of m LQ=600 GeV for the μμjj (μνjj) channel.
5 Background determination
Major backgrounds in this search arise from V+jets (V=W,Z) and \(t\bar{t}\) processes. The kinematic distributions of these are determined using MC samples, and their absolute normalization is evaluated from data using control regions, which are subsets of the selected sample, designed to enhance either the V+jets or the top quark contribution. The multi-jet background is obtained directly from data and prior to the estimation of the normalization for the two main backgrounds, while the determination of the remaining backgrounds (diboson and single top quark production) relies entirely on MC simulations.
Two control regions are used in the μμjj channel. (I) Z+jets: formed by events within a narrow dimuon invariant mass m μμ window around the Z boson mass, defined by 81<m μμ<101 GeV, and at least two jets, and (II) \(t\bar{t}\): one of the muons is replaced by an electron resulting in events with a muon and an electron, and at least two jets.
Three control regions are used in the μνjj channel. (I) W+2 jets: events in the vicinity of the W boson Jacobian peak, selected by requiring 40<m T<120 GeV, exactly two jets and S T<225 GeV, where S T is the scalar summed transverse energy S T, defined as \(S_{\mathrm{T}}=p_{\mathrm{T}}^{\mathrm{\mu}}+E^{\mathrm{miss}}_{\mathrm{T}}+p_{\mathrm{T}}^{\mathrm{jet1}}+p_{\mathrm{T}}^{\mathrm{jet2}}\), (II) W+3 jets: events passing the 40<m T<120 GeV requirement, with at least three jets and S T<225 GeV, and (III) \(t\bar{t}\): events with at least four jets, with \(p_{\mathrm{T}}^{\mathrm{jet1}}>50~\mbox{GeV}\) and \(p_{\mathrm{T}}^{\mathrm{jet2}}>40~\mbox{GeV}\). In all of the control regions the expected signal yields are negligible.
The normalizations of the V+jets and \(t\bar{t}\) backgrounds are obtained by comparing data and MC yields in the control samples defined above. In the μμjj channel, each correction factor is obtained independently for each background, on account of the high purity of the two different control regions. In the μνjj channel, there is significant cross-region contamination and therefore the number of V+jets and \(t\bar{t}\) events is determined by simultaneously minimizing the χ 2 formed by the differences between the observed and predicted SM yields in the three control regions. The resulting scale factors are of the order of 10 % in the low S T region.
The multi-jet background in the selected sample and in each control sample is obtained from a fit to the m μμ and \(E^{\mathrm{miss}}_{\mathrm{T}}\) distribution in the μμjj and μνjj channels, respectively. In these fits, the relative fraction of the multi-jet background is a free parameter, and the sum of the total predicted events is constrained to be equal to the total observed number of events. The V+jets and \(t\bar{t}\) normalizations are not fixed. Multi-jet background arises predominantly from muons from secondary decays. Therefore, templates for the multi-jet background distributions are constructed from multi-jet enhanced samples of data events in which the muons fail the requirement on the transverse impact parameter or the isolation selection requirements described in Sect. 4. In the μμjj channel, the W+jets contribution is estimated together with the multi-jet background. During this procedure, the V+jets and \(t\bar{t}\) normalizations are fitted as well, providing an independent estimate. The resulting values agree with those obtained from the control regions, which are the ones used in the analysis.
After analyzing 1.03 fb−1 of data and applying the analysis requirements described in Sect. 4, good agreement is observed between the data and the SM expectation. The observed and expected yields in the selected sample are 9254 and 9300±1700 for the μμjj channel, and 97113 and 97000±19000 for the μνjj channel. For a LQ mass of 600 GeV, 8.2±0.4 and 3.9±0.2 events are expected for the μμjj and the μνjj final states, respectively. The aforementioned uncertainites fully account for (the dominant) systematic and statistical uncertainties.
6 Likelihood analysis
Several kinematic variables, selected to provide the best discrimination between LQ events and SM backgrounds, are combined in a log likelihood ratio in order to search for a LQ signal. In the μμjj channel, m μμ, \(S_{\mathrm{T}}=p_{\mathrm{T}}^{\mathrm{\mu 1}}+p_{\mathrm{T}}^{\mathrm{\mu 2}}+p_{\mathrm{T}}^{\mathrm{jet1}}+p_{\mathrm{T}}^{\mathrm{jet2}}\) and the average reconstructed leptoquark mass \(\bar{m}_{\mathrm{LQ}}\) are used. In the μνjj channel, S T, m T, the transverse leptoquark mass \(m_{\mathrm{T}}^{\mathrm{LQ}}\) and the leptoquark mass m LQ are used. The distributions of these input variables are shown in Fig. 1 and Fig. 2 for the μμjj and the μνjj final states, respectively.
In the μμjj channel, an average LQ mass \(\bar{m}_{\mathrm{LQ}}\) is defined for each event by reconstructing all possible combinations of lepton-jet pairs, using the two highest p T jets in each event. Of the four possible combinations in each event, the pairing which provides the smallest difference between the LQ masses is chosen, and their average is used in the likelihood analysis. In the μνjj final state, because the longitudinal component of the neutrino momentum is unknown, only one mass from the muon and a jet can be reconstructed, and the \(E^{\mathrm{miss}}_{\mathrm{T}}\) and the remaining jet are used to calculate the transverse mass of the other LQ. The two masses which provide the smallest absolute difference are used in the likelihood analysis. With this algorithm, the probability of picking the correct pairing is of around 90 % for both channels.
For each event, likelihoods are constructed for the background (L B) and the various signal LQ hypothesis (L S) as follows: L B≡∏b i(x ij), L S≡∏s i(x ij), where b i, s i are the probabilities of the i-th input variable from the normalized summed background and signal distributions, respectively, and x ij is the value of that variable for the j-th event in a sample. The log likelihood ratio for each tested signal, LLR=log(L S/L B), is used as the final variable to search for the LQ signal.
7 Systematic uncertainties
Systematic uncertainties originating from several sources are considered. These include uncertainties in lepton momentum, jet energy and \(E^{\mathrm{miss}}_{\mathrm{T}}\) scales and resolutions and their dependence on the number of pile-up events, the background estimations, and the LQ production cross section. For each source of uncertainty considered, the analysis is repeated with the relevant variable varied within its uncertainty, and a new LLR is built for the systematically varied sample, enabling the uncertainty in both the predicted yield and the kinematic distributions to be propagated to the final result. In this section, systematic uncertainties are described for each source of systematics, calculated assuming each source to be 100 % correlated among the different backgrounds. Uncertainties are given for the region of LLR≥2 and LLR≥7 for the μμjj and the μνjj channels, respectively, although the full LLR distribution is used to search for the LQ signal.
The jet energy scale (JES) and resolution (JER) are varied up and down by 1σ [32] for all simulated events. Their impact is estimated independently, and the corresponding variations are propagated to the \(E^{\mathrm{miss}}_{\mathrm{T}}\) in the case of the μνjj channel. The resulting effect of the JES (JER) uncertainty is 9 % (8 %) and 15 % (7 %) for the backgrounds in the μμjj and the μνjj channels, respectively. For a LQ signal of m LQ=600 GeV, both are 1 % for the μμjj channel, and 2.4 % and 1 % for the μνjj channel.
The systematic uncertainties from the muon resolution and momentum scale are derived by comparing the m μμ distribution in Z→μμ control samples to Z→μμ MC samples and are approximately 1 % [28]. These result in uncertainties of 12 % and 3 % for the total background prediction in the μμjj and the μνjj channels, respectively, and in uncertainties of 1.4 % for a LQ signal of m LQ=600 GeV for the μμjj and the μνjj channels.
Systematic uncertainties due to assumptions in the modelling of the V+jets background are estimated by using SHERPA [34–36] samples instead of the ALPGEN samples described in Sect. 3. The resulting uncertainty is 30 % for the μμjj channel and 60 % for the μνjj channel. Similarly, systematic uncertainties arising from the modelling of the \(t\bar{t}\) process are obtained by using different parameter values to simulate alternative samples to the one described in Sect. 3. These include samples in which the top quark mass is varied up and down by 2.5 GeV, generated with MC@NLO, samples where the initial and final-state radiation (ISR and FSR) contributions are varied accordingly to their uncertainties, generated with ACER MC [37], and samples generated with POWHEG [38] interfaced to PYTHIA and JIMMY. These impact the total background yields by 12 % (7 %) for the μμjj (μνjj) final state. For both V+jets and \(t\bar{t}\) backgrounds, a 10 % uncertainty on the scale factors is considered, covering the variation of the scale factors in the low and high p T regions.
Systematic uncertainties in the multi-jet background in the μμjj channel are determined by comparing results derived from fits to kinematic variables other than the nominal ones. These include the leading muon p T, the leading jet p T, the \(E^{\mathrm{miss}}_{\mathrm{T}}\) and the scalar sum of the transverse momenta of the two muons in the event. In the μνjj channel, an alternative loose-tight matrix method [39] with two different multi-jet enhanced samples obtained by inverting the isolation and the |d 0| requirements is used. Since the relevant phase space of the multi-jets in the two channels is very different, the different control regions have very different statistics which leads to a large difference in precision to which this background can be estimated. The resulting uncertainties are 90 % in the μμjj channel and 33 % in the μνjj channel.
A luminosity uncertainty of 3.7 % [40, 41] is assigned to the LQ signal yields and to the yields of background processes determined from simulation: diboson and single top quark production. Further systematic uncertainties considered arise from the finite number of events in the simulated samples, amounting to 4 %–25 % depending on the LQ mass being considered.
For the signal samples, additional systematic uncertainties originate from ISR and FSR effects, resulting in an uncertainty of 2 % for both channels. The choice of the renormalization and factorization scales, which are varied from m LQ to 2m LQ and m LQ/2, and the choice of the PDF, determined with the CTEQ eigenvectors errors and by using the MRST2007LO* PDF set [42], result in an uncertainty in the signal acceptance of 1 %–6 % for LQ masses between 300 GeV and 700 GeV.
8 Results
Figure 3 shows the LLR for the data, the predicted backgrounds and a LQ signal of 600 GeV for the μμjj and the μνjj channels. To ensure sufficient background statistics, bins with a total background yield less than twice the statistical uncertainty in that bin are merged into a single bin. There is no significant excess in data observed at large LLR values where such a signal would appear, and the data are found to be consistent with the SM background expectations (see Table 1). Upper limits are derived at 95 % confidence level (CL) for the scalar leptoquark production cross section using a modified frequentist CL s approach [43, 44]. The test statistic is defined as −2ln(Q)=−2ln(L s+b/L b), where the likelihoods L s+b and L s follow a Poisson distribution and are calculated based on the corresponding LLR distributions. Systematic uncertainties as described in Sect. 7 are treated as nuisance parameters with a Gaussian probability density function.
The 95 % CL upper bounds on the cross section for leptoquark pair production as a function of mass are shown in Fig. 4 for the μμjj and the μνjj channels at β=1.0 and β=0.5, respectively. The expected and observed limits for the combined channels are shown in the β vs. m LQ plane in Fig. 5.
9 Conclusions
The results of a search for the pair production of second generation scalar leptoquarks using 1.03 fb−1 of proton-proton collision data produced by the LHC at \(\sqrt{s}=7~\mbox{TeV}\) and recorded by the ATLAS detector are presented. The data are in good agreement with the expected SM background, and no evidence of LQ production is observed. Lower limits on leptoquark masses of m LQ>685 GeV and m LQ>594 GeV for β=1.0 and β=0.5 are obtained at 95 % CL, whereas the expected limits are m LQ>671 GeV and m LQ>605 GeV, respectively. These are the most stringent limits to date arising from direct searches for second generation scalar leptoquarks.
Notes
The λ LQ−ℓ−q coupling determines the LQ lifetime and width [10]. For LQ masses considered here, 200 GeV≤m LQ≤700 GeV, couplings greater than e×10−6, with \(e=\sqrt{4\pi\alpha}\) the electron charge, and α(M Z)=1/128, correspond to decay lengths less than roughly 1 mm. In addition, to be insensitive to the coupling, the width cannot be larger than the experimental resolution of a few GeV. This sets the approximate sensitivity to the unknown coupling strength.
ATLAS uses a right-handed coordinate system with its origin at the nominal interaction point and the z-axis along the beam pipe. Cylindrical coordinates (r,ϕ) are used in the transverse plane, with ϕ the azimuthal angle around the beam pipe. The pseudorapidity η is defined in terms of the polar angle θ by η=−lntan(θ/2).
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Acknowledgements
We thank CERN for the very successful operation of the LHC, as well as the support staff from our institutions without whom ATLAS could not be operated efficiently.
We acknowledge the support of ANPCyT, Argentina; YerPhI, Armenia; ARC, Australia; BMWF, Austria; ANAS, Azerbaijan; SSTC, Belarus; CNPq and FAPESP, Brazil; NSERC, NRC and CFI, Canada; CERN; CONICYT, Chile; CAS, MOST and NSFC, China; COLCIENCIAS, Colombia; MSMT CR, MPO CR and VSC CR, Czech Republic; DNRF, DNSRC and Lundbeck Foundation, Denmark; ARTEMIS and ERC, European Union; IN2P3-CNRS, CEA-DSM/IRFU, France; GNAS, Georgia; BMBF, DFG, HGF, MPG and AvH Foundation, Germany; GSRT, Greece; ISF, MINERVA, GIF, DIP and Benoziyo Center, Israel; INFN, Italy; MEXT and JSPS, Japan; CNRST, Morocco; FOM and NWO, Netherlands; RCN, Norway; MNiSW, Poland; GRICES and FCT, Portugal; MERYS (MECTS), Romania; MES of Russia and ROSATOM, Russian Federation; JINR; MSTD, Serbia; MSSR, Slovakia; ARRS and MVZT, Slovenia; DST/NRF, South Africa; MICINN, Spain; SRC and Wallenberg Foundation, Sweden; SER, SNSF and Cantons of Bern and Geneva, Switzerland; NSC, Taiwan; TAEK, Turkey; STFC, the Royal Society and Leverhulme Trust, United Kingdom; DOE and NSF, United States of America.
The crucial computing support from all WLCG partners is acknowledged gratefully, in particular from CERN and the ATLAS Tier-1 facilities at TRIUMF (Canada), NDGF (Denmark, Norway, Sweden), CC-IN2P3 (France), KIT/GridKA (Germany), INFN-CNAF (Italy), NL-T1 (Netherlands), PIC (Spain), ASGC (Taiwan), RAL (UK) and BNL (USA) and in the Tier-2 facilities worldwide.
Author information
Authors and Affiliations
University at Albany, Albany, NY, United States of America
M. S. Alam, J. Ernst & V. Rojo
Department of Physics, University of Alberta, Edmonton, AB, Canada
S. Bahinipati, N. J. Buchanan, K. Chan, D. M. Gingrich, M. S. Kim, R. W. Moore, J. L. Pinfold, N. Soni, HS. Subramania & F. Vives Vaque
Department of Physics, Ankara University, Ankara, Turkey
O. Cakir, A. K. Ciftci, R. Ciftci, H. Duran Yildiz, S. Kuday & S. Persembe
Department of Physics, Dumlupinar University, Kutahya, Turkey
O. Cakir
Department of Physics, Gazi University, Ankara, Turkey
M. Yilmaz
Division of Physics, TOBB University of Economics and Technology, Ankara, Turkey
S. Sultansoy
Turkish Atomic Energy Authority, Ankara, Turkey
I. Turk Cakir
LAPP, CNRS/IN2P3 and Université de Savoie, Annecy-le-Vieux, France
L. Aperio Bella, B. Aubert, N. Berger, J. Colas, M. Delmastro, L. Di Ciaccio, T. K. O. Doan, S. Elles, C. Goy, L. Helary, T. Hryn’ova, A. Jeremie, S. Jézéquel, M. Kataoka, J. Labbe, R. Lafaye, J. Levêque, V. P. Lombardo, N. Massol, P. Perrodo, E. Petit, H. Przysiezniak, E. Richter-Was, G. Sauvage, E. Sauvan, M. Schwoerer, T. Todorov, D. Tsionou, I. Wingerter-Seez & R. Zitoun
High Energy Physics Division, Argonne National Laboratory, Argonne, IL, United States of America
L. Asquith, R. E. Blair, S. Chekanov, J. W. Dawson, D. Fellmann, A. T. Goshaw, V. J. Guarino, D. Hill, N. Hill, T. LeCompte, D. Malon, E. N. May, L. Nodulman, A. Paramonov, L. E. Price, J. Proudfoot, B. M. Salvachua Ferrando, J. L. Schlereth, R. W. Stanek, D. G. Underwood, P. van Gemmeren, A. Vaniachine, R. Yoshida & J. Zhang
Department of Physics, University of Arizona, Tucson, AZ, United States of America
E. Cheu, K. A. Johns, V. Kaushik, C. L. Lampen, W. Lampl, X. Lei, P. Loch, C. P. Paleari, F. Rühr, J. P. Rutherfoord, L. Shaver, M. A. Shupe & E. W. Varnes
Department of Physics, The University of Texas at Arlington, Arlington, TX, United States of America
A. Brandt, H. Brown, K. De, A. Farbin, L. Heelan, C. M. Hernandez, P. Nilsson, N. Ozturk, E. Sarkisyan-Grinbaum, M. Sosebee, B. Spurlock, A. R. Stradling, G. Usai, A. Vartapetian, A. White & J. Yu
Physics Department, University of Athens, Athens, Greece
A. Antonaki, D. Fassouliotis, V. Giakoumopoulou, N. Giokaris, P. Ioannou, K. Iordanidou, C. Kourkoumelis, A. Manousakis-Katsikakis, G. Tzanakos & C. Vellidis
Physics Department, National Technical University of Athens, Zografou, Greece
T. Alexopoulos, R. Avramidou, M. Dris, A. Filippas, M. Fokitis, E. N. Gazis, G. Iakovidis, E. Katsoufis, S. Leontsinis, S. Maltezos, E. Mountricha, E. Panagiotopoulou, Th. D. Papadopoulou, G. Tsipolitis & S. Vlachos
Institute of Physics, Azerbaijan Academy of Sciences, Baku, Azerbaijan
O. Abdinov, M. Aliyev, F. Khalil-zada & S. Rzaeva
Institut de Física d’Altes Energies and Departament de Física de la Universitat Autònoma de Barcelona and ICREA, Barcelona, Spain
J. Abdallah, M. Bosman, M. P. Casado, M. Cavalli-Sforza, M. C. Conidi, B. Demirkoz, M. Dosil, X. Espinal Curull, P. Francavilla, V. Giangiobbe, G. Gonzalez Parra, S. Grinstein, C. Helsens, A. Juste Rozas, I. Korolkov, E. Le Menedeu, M. Martinez, E. Meoni, L. M. Mir, L. Miralles Verge, J. Nadal, C. Osuna, A. Pacheco Pages, C. Padilla Aranda, I. Riu, V. Rossetti, F. Rubbo, E. Segura, A. Succurro, S. Sushkov & V. Vorwerk
Institute of Physics, University of Belgrade, Belgrade, Serbia
I. Borjanovic, J. Krstic, D. S. Popovic, Dj. Sijacki & Lj. Simic
Vinca Institute of Nuclear Sciences, University of Belgrade, Belgrade, Serbia
I. Bozovic-Jelisavcic, T. Jovin, J. Mamuzic & M. Mudrinic
Department for Physics and Technology, University of Bergen, Bergen, Norway
T. Buanes, T. Burgess, G. Eigen, L. G. Johansen, A. Kastanas, W. Liebig, A. Lipniacka, P. L. Rosendahl, H. Sandaker, T. B. Sjursen, B. Stugu, A. Tonoyan & M. Ugland
Physics Division, Lawrence Berkeley National Laboratory and University of California, Berkeley, CA, United States of America
J-F. Arguin, A. M. Bach, A. Barbaro Galtieri, R. M. Barnett, J. Beringer, J. Biesiada, P. Calafiura, L. M. Caminada, A. Ciocio, M. Cooke, K. Copic, S. Dube, K. Einsweiler, A. Gaponenko, M. Garcia-Sciveres, C. Haber, M. Hance, B. Heinemann, I. Hinchliffe, S.-C. Hsu, M. Hurwitz, J. Joseph, W. Lavrijsen, C. Leggett, P. Loscutoff, J. Lys, R. J. Madaras, A. Ovcharova, S. Pagan Griso, A. Pranko, D. R. Quarrie, C. Ruwiedel, M. Shapiro, L. A. Skinnari, M. Tatarkhanov, M. J. Tibbetts, V. Tsulaia, S. Vahsen, D. Varouchas, J. Virzi, Y. Yao & S. Zenz
Department of Physics, Humboldt University, Berlin, Germany
M. Aliev, F. M. Giorgi, S. Grancagnolo, R. Herrberg, I. Hristova, O. Kind, H. Kolanoski, R. Kwee, H. Lacker, M. Leyton, T. Lohse, R. Mandrysch, A. Nikiforov, H. Schulz, D. Wendland & M. zur Nedden
Albert Einstein Center for Fundamental Physics and Laboratory for High Energy Physics, University of Bern, Bern, Switzerland
L. S. Ancu, A. Battaglia, H. P. Beck, C. Borer, A. Ereditato, T. Fonseca Martin, V. Gallo, S. Haug, S. Kabana, T. Kruker, K. Pretzl, C. Topfel & M. S. Weber
School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom
B. M. M. Allbrooke, H. S. Bansil, J. Bracinik, D. G. Charlton, A. S. Chisholm, N. J. Collins, C. J. Curtis, J. Garvey, D. R. Hadley, K. Harrison, C. M. Hawkes, S. J. Head, S. J. Hillier, G. Mahout, T. A. Martin, T. Mclaughlan, P. R. Newman, S. W. O’Neale, J. D. Palmer, 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
T. Akdogan, E. Arik, M. Arik, S. Istin, V. E. Ozcan & T. Rador
Division of Physics, Dogus University, Istanbul, Turkey
S. A. Cetin
Department of Physics Engineering, Gaziantep University, Gaziantep, Turkey
A. J. Beddall, A. Beddall, A. Bingul & F. Diblen
Department of Physics, Istanbul Technical University, Istanbul, Turkey
A. J. Beddall
INFN Sezione di Bologna, Bologna, Italy
L. Bellagamba, A. Bertin, M. Bindi, D. Boscherini, A. Bruni, G. Bruni, M. Bruschi, D. Caforio, C. Ciocca, M. Corradi, S. De Castro, R. Di Sipio, L. Fabbri, B. Giacobbe, P. Giusti, M. K. Jha, I. Massa, A. Mengarelli, S. Monzani, M. Piccinini, A. Polini, L. Rinaldi, M. Romano, C. Sbarra, A. Sbrizzi, N. Semprini-Cesari, R. Spighi, S. Valentinetti, M. Villa & A. Zoccoli
Dipartimento di Fisica, Università di Bologna, Bologna, Italy
A. Bertin, M. Bindi, D. Caforio, S. De Castro, R. Di Sipio, L. Fabbri, I. Massa, A. Mengarelli, S. Monzani, M. Piccinini, M. Romano, A. Sbrizzi, N. Semprini-Cesari, S. Valentinetti, M. Villa & A. Zoccoli
Physikalisches Institut, University of Bonn, Bonn, Germany
C. F. Anders, D. Arutinov, M. Backhaus, M. Barbero, P. Bechtle, I. Brock, M. Cristinziani, W. Davey, K. Desch, J. Dingfelder, P. Fischer, G. Gaycken, Ch. Geich-Gimbel, L. Gonella, M. Havranek, D. Hellmich, S. Hillert, F. Huegging, T. Ince, M. Karagounis, G. Khoriauli, P. Koevesarki, T. Kokott, V. V. Kostyukhin, J. K. Kraus, J. Kroseberg, H. Krüger, A. Kruth, C. Lapoire, M. Lehmacher, A. M. Leyko, C. Limbach, T. Loddenkoetter, M. Mazur, N. Möser, K. Mueller, G. Nanava, T. Nattermann, A.-E. Nuncio-Quiroz, T. Poghosyan, S. Psoroulas, B. Radics, S. Schaepe, K. Schmieden, M. Schmitz, M. J. Schultens, J. W. Schumacher, T. Schwindt, J. A. Stillings, J. Therhaag, J.-W. Tsung, K. Uchida, M. Uhlenbrock, N. Vlasov, A. Vogel, E. von Toerne, T. Wang, N. Wermes, P. Wienemann, C. Zendler, R. Zimmermann & S. Zimmermann
Department of Physics, Boston University, Boston, MA, United States of America
S. P. Ahlen, K. M. Black, J. M. Butler, L. Dell’Asta, E. Hazen, J. Love, N. R. Nation, C. Posch, J. T. Shank, S. P. Whitaker, Z. Yan & S. Youssef
Department of Physics, Brandeis University, Waltham, MA, United States of America
S. Aefsky, C. Amelung, J. R. Bensinger, C. Blocker, R. K. Daya-Ishmukhametova, S. Gozpinar, L. E. Kirsch, D. Pomeroy, G. Sciolla, N. Skvorodnev & H. Wellenstein
Universidade Federal do Rio De Janeiro COPPE/EE/IF, Rio de Janeiro, Brazil
L. P. Caloba, P. V. M. Da Silva, C. Maidantchik, L. Manhaes de Andrade Filho, F. Marroquim, A. A. Nepomuceno, M. Perantoni & J. M. Seixas
Federal University of Juiz de Fora (UFJF), Juiz de Fora, Brazil
A. S. Cerqueira
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, Sao Paulo, Brazil
M. Donadelli & M. A. L. Leite
Physics Department, Brookhaven National Laboratory, Upton, NY, United States of America
D. L. Adams, K. Assamagan, M. D. Baker, M. Begel, C. Bernius, H. Chen, V. Chernyatin, P. E. De Castro Faria Salgado, R. Debbe, R. Dhullipudi, M. Ernst, T. Gadfort, B. Gibbard, H. A. Gordon, Z. D. Greenwood, A. Klimentov, F. Lanni, D. Lissauer, D. Lynn, H. Ma, T. Maeno, S. Majewski, P. Nevski, K. Nikolopoulos, D. Oliveira Damazio, F. Paige, S. Panitkin, W. Park, M.-A. Pleier, A. Poblaguev, V. Polychronakos, R. Pravahan, S. Protopopescu, M. Purohit, D. Rahm, S. Rajagopalan, G. Redlinger, L. Sawyer, A. Sircar, S. Snyder, P. Steinberg, I. Stumer, H. Takai, M. C. Tamsett, A. Trivedi, A. Undrus, T. Wenaus, S. Ye & D. Yu
National Institute of Physics and Nuclear Engineering, Bucharest, Romania
C. Alexa, E. Badescu, V. Boldea, S. I. Buda, I. Caprini, M. Caprini, M. Ciubancan, S. Constantinescu, C.-M. Cuciuc, P. Dita, S. Dita, L. Micu, A. Olariu, D. Pantea, G. A. Popeneciu, M. Rotaru, G. Stoicea, A. Tudorache & V. Tudorache
University Politehnica Bucharest, Bucharest, Romania
G. L. Darlea
West University in Timisoara, Timisoara, Romania
G. L. Darlea
Departamento de Física, Universidad de Buenos Aires, Buenos Aires, Argentina
M. L. Gonzalez Silva, G. Otero y Garzon, R. Piegaia & G. Romeo
Cavendish Laboratory, University of Cambridge, Cambridge, United Kingdom
S. Ask, N. Barlow, J. R. Batley, F. M. Brochu, W. Buttinger, J. R. Carter, J. D. Chapman, C. Cowden, S. T. French, J. A. Frost, J. C. Hill, S. Kaneti, T. J. Khoo, C. G. Lester, V. Moeller, M. A. Parker, D. Robinson, T. Sandoval, M. Thomson & C. P. Ward
Department of Physics, Carleton University, Ottawa, ON, Canada
D. Gillberg, T. Koffas, C. Liu, J. F. Marchand, T. G. McCarthy, F. G. Oakham, K. Randrianarivony, F. Tarrade, R. Ueno, M. G. Vincter & K. Whalen
CERN, Geneva, Switzerland
M. Aleksa, P. Amaral, C. Anastopoulos, F. Anghinolfi, M. A. Baak, K. Bachas, D. Banfi, M. Battistin, F. Bellina, M. Bellomo, O. Beltramello, D. Berge, F. Bertinelli, R. M. Bianchi, G. Blanchot, J. A. Bogaerts, J. Boyd, A. Braem, J. Bremer, H. Burckhart, F. Butin, S. Campana, M. D. M. Capeans Garrido, T. Carli, A. Catinaccio, J. R. Catmore, A. Cattai, A. Cerri, C. A. Chavez Barajas, J. T. Childers, D. Chromek-Burckhart, J. Cook, D. Côté, H. O. Danielsson, A. Dell’Acqua, N. Delruelle, A. Di Girolamo, B. Di Girolamo, B. Di Micco, F. Dittus, R. Dobinson, D. Dobos, E. Dobson, J. Dopke, H. Drevermann, A. Dudarev, M. Dührssen, M. Dunford, F. Dydak, N. Ellis, M. Elsing, C. Fabre, P. Farthouat, P. Fassnacht, A. Foussat, D. Francis, S. Franz, R. Froeschl, D. Froidevaux, E. Fullana Torregrosa, C. Gabaldon, N. Garelli, V. Garonne, J-C. Gayde, F. Gianotti, S. M. Gibson, J. Godlewski, A. Gonidec, L. Goossens, B. Gorini, P. Grafström, H. M. Gray, S. Haas, F. Hahn, S. Haider, M. Hatch, M. Hauschild, R. J. Hawkings, M. Heller, A. M. Henriques Correia, L. Hervas, A. Hoecker, M. Huhtinen, J. Inigo-Golfin, M. R. Jaekel, H. Jansen, P. Jenni, O. Jonsson, C. Joram, R. M. Jungst, M. Kaneda, J. Kaplon, N. Kerschen, T. Klioutchnikova, J. Knobloch, K. Köneke, M. J. Kotamäki, M. Lamanna, C. Lasseur, M. Lassnig, G. Lehmann Miotto, B. Lenzi, P. Lichard, L. Magnoni, B. Malaescu, S. Malyukov, A. Mapelli, L. Mapelli, Z. Marshall, B. Martin, J. M. Maugain, R. A. McLaren, C. Menot, A. Messina, T. C. Meyer, S. Michal, J. Molina-Perez, A. K. Morley, G. Mornacchi, D. Muenstermann, A. M. Nairz, Y. Nakahama, G. Negri, M. Nessi, B. Nicquevert, T. Niinikoski, M. Nordberg, S. Palestini, T. Pauly, H. Pernegger, K. Peters, B. A. Petersen, J. Petersen, G. Piacquadio, O. Pirotte, K. Pommès, A. Poppleton, X. Portell Bueso, G. Poulard, S. Prasad, L. Pribyl, M. J. Price, M. Raymond, C. Rembser, D. Roda Dos Santos, S. Roe, D. Salek, A. Salzburger, D. O. Savu, S. Schlenker, M. Schott, G. Schuler, A. Sfyrla, S. Shimizu, J. Sloper, G. Spigo, R. Spiwoks, G. A. Stewart, B. Szeless, G. P. Tappern, H. Ten Kate, F. J. Tique Aires Viegas, I. Torchiani, L. Tremblet, A. Tricoli, C. Tsarouchas, G. Unal, D. van der Ster, W. Vandelli, G. Vandoni, F. Varela Rodriguez, R. Veness, E. Vinek, R. Voss, R. Vuillermet, P. S. Wells, T. Wengler, S. Wenig, P. Werner, H. G. Wilkens, F. Winklmeier, J. Wotschack, Z. Zajacova, A. Zsenei & L. Zwalinski
Enrico Fermi Institute, University of Chicago, Chicago, IL, United States of America
K. J. Anderson, A. Boveia, F. Canelli, G. Choudalakis, T. Costin, E. J. Feng, M. Fiascaris, R. W. Gardner, A. Gupta, I. Jen-La Plante, A. Kapliy, C. Melachrinos, F. S. Merritt, C. Meyer, D. W. Miller, P. U. E. Onyisi, M. J. Oreglia, B. Penning, J. E. Pilcher, M. J. Shochet, L. Tompkins & J. M. Tuggle
Departamento de Fisica, Pontificia Universidad Católica de Chile, Santiago, Chile
M. A. Diaz, S. A. Olivares Pino, B. Panes & F. Quinonez
Departamento de Física, Universidad Técnica Federico Santa María, Valparaíso, Chile
W. K. Brooks, E. Carquin, S. Kuleshov, R. Pezoa & F. Prokoshin
Institute of High Energy Physics, Chinese Academy of Sciences, Beijing, China
Y. Bai, S. Cheng, H. Han, S. Jin, F. Lu, Q. Ouyang, X. Ruan, L. Y. Shan, G. Tong, Y. Xie, G. Xu, Y. Yang & S. Zheng
Department of Modern Physics, University of Science and Technology of China, Anhui, China
L. Han, Y. Jiang, G. Jin, S. Li, M. Liu, Y. Liu, H. Peng, H. Wang, Y. Wu, C. Xu, D. Zhang, Z. Zhao & Y. Zhu
Department of Physics, Nanjing University, Jiangsu, China
S. Chen, T. Chen & J. Ping
School of Physics, Shandong University, Shandong, China
C. Feng, P. Ge, M. He, J. Miao, Z. Zhan, X. Zhang & C. G. Zhu
Laboratoire de Physique Corpusculaire, Clermont Université and Université Blaise Pascal and CNRS/IN2P3, Aubiere Cedex, France
D. Boumediene, E. Busato, D. Calvet, S. Calvet, R. Camacho Toro, D. Cinca, J. Donini, R. Febbraro, N. Ghodbane, C. Guicheney, H. Liao, D. Pallin, D. Paredes Hernandez, F. Podlyski, C. Santoni, L. P. Says & F. Vazeille
Nevis Laboratory, Columbia University, Irvington, NY, United States of America
T. Andeen, A. Angerami, G. Brooijmans, J. Dodd, N. Grau, J. Guo, E. W. Hughes, M. Leltchouk, N. Nikiforou, J. A. Parsons, A. Penson, K. Perez, V. Perez Reale, M. I. Scherzer, E. N. Thompson, F. Tian, P. M. Tuts, D. Urbaniec, E. Williams, W. Willis, E. Wulf & L. Živković
Niels Bohr Institute, University of Copenhagen, Kobenhavn, Denmark
N. Boelaert, M. Dam, C. Driouichi, K. Gregersen, J. R. Hansen, J. B. Hansen, J. D. Hansen, P. H. Hansen, S. Heisterkamp, S. Jakobsen, P. Jež, M. D. Joergensen, P. Kadlecik, E. B. Klinkby, J. Lundquist, R. Mackeprang, S. Mehlhase, T. C. Petersen, M. Simonyan, L. A. Thomsen & S. Xella
INFN Gruppo Collegato di Cosenza, Arcavata di Rende, Italy
M. Capua, G. Crosetti, S. Fazio, L. La Rotonda, V. Lavorini, A. Mastroberardino, G. Morello, A. Policicchio, D. Salvatore, M. Schioppa, G. Susinno & E. Tassi
Dipartimento di Fisica, Università della Calabria, Arcavata di Rende, Italy
M. Capua, G. Crosetti, S. Fazio, L. La Rotonda, V. Lavorini, A. Mastroberardino, G. Morello, A. Policicchio, D. Salvatore, M. Schioppa, G. Susinno & E. Tassi
Faculty of Physics and Applied Computer Science, AGH University of Science and Technology, Krakow, Poland
L. Adamczyk, T. Bold, W. Dabrowski, M. Dwuznik, I. Grabowska-Bold, K. Jelen, D. Kisielewska, S. Koperny, T. Z. Kowalski, B. Mindur, M. Przybycien & B. Toczek
The Henryk Niewodniczanski Institute of Nuclear Physics, Polish Academy of Sciences, Krakow, Poland
E. Banas, J. Blocki, P. A. Bruckman de Renstrom, D. Derendarz, E. Gornicki, Z. Hajduk, W. Iwanski, A. Kaczmarska, K. Korcyl, Pa. Malecki, P. Malecki, A. Olszewski, J. Olszowska, E. Stanecka, M. Trzebinski, A. Trzupek, M. Turala, M. W. Wolter, B. K. Wosiek, K. W. Wozniak, B. Zabinski & A. Zemla
Physics Department, Southern Methodist University, Dallas, TX, United States of America
K. Dindar Yagci, A. Firan, H. K. Hadavand, J. Hoffman, Y. Ilchenko, R. Ishmukhametov, D. Joffe, S. Kama, R. Kehoe, A. S. Randle-Conde, R. R. Rios, S. J. Sekula, R. Stroynowski & J. Ye
Physics Department, University of Texas at Dallas, Richardson, TX, United States of America
M. Ahsan, J. M. Izen, X. Lou, K. Reeves & W. C. Wong
DESY, Hamburg and Zeuthen, Germany
E. Bergeaas Kuutmann, M. Boehler, J. Dietrich, W. Ehrenfeld, V. Ferrara, G. Fischer, C. Friedrich, A. Glazov, M. Goebel, L. S. Gomez Fajardo, J. Goncalves Pinto Firmino Da Costa, B. Gosdzik, K-J. Grahn, I. M. Gregor, K. H. Hiller, A. Huettmann, U. Husemann, M. Jimenez Belenguer, S. Johnert, M. Karnevskiy, J. Katzy, T. Kono, T. Kuhl, C. Lange, E. Lobodzinska, D. Ludwig, S. Mättig, M. Medinnis, L. Mijović, K. Mönig, T. Naumann, T. Perez Cavalcanti, D. Petschull, S. M. Piec, R. Placakyte, Z. Qin, V. Radescu, I. Rubinskiy, G. Sedov, M. Stanescu-Bellu, P. Starovoitov, N. A. Styles, K. Tackmann, P. Vankov, M. Viti, C. Wasicki, M. A. Wildt & H. Zhu
Institut für Experimentelle Physik IV, Technische Universität Dortmund, Dortmund, Germany
M. Bunse, C. Gössling, F. Hirsch, C. A. Jung, R. Klingenberg, I. Reisinger & R. Wunstorf
Institut für Kern- und Teilchenphysik, Technical University Dresden, Dresden, Germany
P. Czodrowski, F. Friedrich, T. Göpfert, M. Kobel, K. Leonhardt, A. Ludwig, W. F. Mader, M. Morgenstern, X. Prudent, C. Rudolph, R. Schwierz, F. Seifert, P. Steinbach, A. Straessner & A. Vest
Department of Physics, Duke University, Durham, NC, United States of America
A. T. H. Arce, D. P. Benjamin, A. Bocci, W. L. Ebenstein, A. J. Fowler, B. R. Ko, A. Kotwal, S. H. Oh, C. Wang & J. Yamaoka
SUPA - School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom
W. Bhimji, A. G. Buckley, P. J. Clark, C. Debenedetti, R. D. Harrington, V. J. Martin, B. J. O’Brien, K. E. Selbach, B. H. Smart, A. Washbrook & B. M. Wynne
Fachhochschule Wiener Neustadt, Johannes Gutenbergstrasse 3, 2700, Wiener Neustadt, Austria
W. Bhimji
INFN Laboratori Nazionali di Frascati, Frascati, Italy
A. Annovi, M. Antonelli, H. Bilokon, F. Cerutti, M. Curatolo, R. Di Nardo, B. Esposito, M. L. Ferrer, C. Gatti, P. Laurelli, G. Maccarrone, A. Sansoni, M. Testa, E. Vilucchi & G. Volpi
Fakultät für Mathematik und Physik, Albert-Ludwigs-Universität, Freiburg i.Br., Germany
G. Aad, F. Ahles, T. Barber, R. Bernhard, U. Bitenc, R. Bruneliere, A. Christov, V. Consorti, M. Fehling-Kaschek, M. Flechl, J. Glatzer, J. Hartert, G. Herten, S. Horner, K. Jakobs, M. Janus, M. Kollefrath, A. I. Kononov, S. Kuehn, S. Lai, U. Landgraf, K. Lohwasser, I. Ludwig, J. Ludwig, D. Lumb, K. Mahboubi, W. Mohr, H. Nilsen, U. Parzefall, M. Rammensee, T. C. Rave, K. Runge, Z. Rurikova, E. Schmidt, M. Schumacher, F. Siegert, K. Stoerig, J. E. Sundermann, K. K. Temming, S. Thoma, V. Tsiskaridze, M. Venturi, I. Vivarelli, H. von Radziewski, T. Vu Anh, M. Warsinsky, C. Weiser, M. Werner, L. A. M. Wiik-Fuchs, S. Winkelmann, S. Xie & S. Zimmermann
Section de Physique, Université de Genève, Geneva, Switzerland
A. A. Abdelalim, G. Alexandre, M. Backes, G. Barone, P. J. Bell, W. H. Bell, E. Benhar Noccioli, A. Blondel, F. Bucci, A. Clark, V. Dao, C. Doglioni, D. Ferrere, S. Gadomski, S. Gonzalez-Sevilla, M. P. Goulette, G. Iacobucci, A. La Rosa, A. Leger, A. Lister, B. Martin dit Latour, P. Mermod, C. Mora Herrera, S. Nektarijevic, K. Nikolics, G. Pásztor, A. Picazio, M. Pohl, K. Rosbach, L. Rosselet & X. Wu
INFN Sezione di Genova, Genova, Italy
D. Barberis, R. Beccherle, C. Caso, M. Dameri, G. Darbo, A. Ferretto Parodi, G. Gagliardi, C. Gemme, P. Morettini, M. Olcese, B. Osculati, F. Parodi, S. Passaggio, L. P. Rossi & C. Schiavi
Dipartimento di Fisica, Università di Genova, Genova, Italy
D. Barberis, C. Caso, M. Dameri, A. Ferretto Parodi, G. Gagliardi, B. Osculati, F. Parodi & C. Schiavi
E.Andronikashvili Institute of Physics, Tbilisi State University, Tbilisi, Georgia
L. Chikovani & E. G. Tskhadadze
High Energy Physics Institute, Tbilisi State University, Tbilisi, Georgia
T. Djobava, J. Khubua, G. Mchedlidze & M. Mosidze
II Physikalisches Institut, Justus-Liebig-Universität Giessen, Giessen, Germany
M. Düren & H. Stenzel
SUPA - School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom
S. E. Allwood-Spiers, R. L. Bates, D. Britton, P. Bussey, C. M. Buttar, C. Collins-Tooth, S. D’Auria, T. Doherty, A. T. Doyle, N. C. Edwards, S. Ferrag, J. Ferrando, D. E. Ferreira de Lima, A. Gemmell, D. Kar, M. Kenyon, H. McGlone, A. Moraes, V. O’Shea, C. Oropeza Barrera, A. Robson, D. H. Saxon, K. M. Smith, R. D. St. Denis, G. Steele, A. S. Thompson, K. Wraight, C. Wright & M. Wright
II Physikalisches Institut, Georg-August-Universität, Göttingen, Germany
C. Ay, K. Bierwagen, U. Blumenschein, O. Brandt, J. Erdmann, D. Evangelakou, M. George, J. Grosse-Knetter, S. Guindon, J. Haller, M. Hamer, A. Henrichs, C. Hensel, M. Keil, A. Knue, F. Kohn, N. Krieger, K. Kroeninger, B. Lemmer, E. Magradze, A. Mann, J. Meyer, J. Morel, S. Pashapour, A. Quadt, A. Roe, L. Serkin, E. Shabalina, M. Uhrmacher, T. Vazquez Schroeder, P. Weber & J. Weingarten
Laboratoire de Physique Subatomique et de Cosmologie, Université Joseph Fourier and CNRS/IN2P3 and Institut National Polytechnique de Grenoble, Grenoble, France
S. Albrand, M-L. Andrieux, Q. Buat, B. Clement, J. Collot, S. Crépé-Renaudin, B. Dechenaux, T. Delemontex, P. A. Delsart, M. H. Genest, J-Y. Hostachy, E. Laisne, F. Ledroit-Guillon, A. Lleres, A. Lucotte, F. Malek, Ph. Martin, F. Polci, J. Stark, X. Sun, B. Trocmé, J. Wang & C. Weydert
Department of Physics, Hampton University, Hampton, VA, United States of America
T. N. Addy, A. Harvey, K. W. McFarlane, T. Shin & V. I. Vassilakopoulos
Laboratory for Particle Physics and Cosmology, Harvard University, Cambridge, MA, United States of America
J. Barreiro Guimarães da Costa, A. Belloni, G. W. Brandenburg, G. Conti, M. Franklin, P. Hurst, J. Huth, L. Jeanty, M. Kagan, D. Lopez Mateos, V. Martinez Outschoorn, K. M. Mercurio, C. Mills, S. Moed, M. Morii, H. P. Skottowe, B. C. Smith & G. Zevi della Porta
Kirchhoff-Institut für Physik, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
G. Anders, V. Andrei, Y. Davygora, T. A. Dietzsch, C. Geweniger, P. Hanke, M. Henke, A. Khomich, E.-E. Kluge, V. Lendermann, F. Lepold, K. Meier, F. Mueller, S. Poddar, V. Scharf, H.-C. Schultz-Coulon, R. Stamen & M. Wessels
Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
G. Kasieczka, R. Narayan, S. Schaetzel, S. Schmitt & A. Schöning
ZITI Institut für technische Informatik, Ruprecht-Karls-Universität Heidelberg, Mannheim, Germany
A. Kugel, R. Maenner & N. Schroer
Faculty of Applied Information Science, Hiroshima Institute of Technology, Hiroshima, Japan
Y. Nagasaka
Department of Physics, Indiana University, Bloomington, IN, United States of America
S. Brunet, P. Cwetanski, H. Evans, P. Gagnon, V. Jain, F. Luehring, H. Ogren, J. Penwell, D. Price, D. Whittington, Y. Yang & D. Zieminska
Institut für Astro- und Teilchenphysik, Leopold-Franzens-Universität, Innsbruck, Austria
B. Epp, P. Jussel, E. Kneringer, D. Kuhn, W. Lukas & G. Rudolph
University of Iowa, Iowa City, IA, United States of America
P. K. Behera, M. Limper, U. Mallik, Y. Pylypchenko & R. Zaidan
Department of Physics and Astronomy, Iowa State University, Ames, IA, United States of America
C. Chen, J. Cochran, F. Dudziak, N. Krumnack, A. S. Mete, W. T. Meyer, S. Prell, E. I. Rosenberg, A. Ruiz-Martinez, S. Shrestha & K. Yamamoto
Joint Institute for Nuclear Research, JINR Dubna, Dubna, Russia
I. N. Aleksandrov, A. Barashkou, D. Y. Bardin, V. A. Bednyakov, I. R. Boyko, I. A. Budagov, G. A. Chelkov, A. Cheplakov, V. F. Chepurnov, M. V. Chizhov, D. V. Dedovich, M. Demichev, G. L. Glonti, M. I. Gostkin, N. Grigalashvili, Y. Gusakov, N. Huseynov, L. V. Kalinovskaya, M. Y. Kazarinov, G. D. Kekelidze, D. Kharchenko, N. Khovanskiy, E. Khramov, V. Kolesnikov, V. M. Kotov, U. Kruchonak, Z. V. Krumshteyn, V. Kukhtin, E. Ladygin, A. B. Lazarev, I. D. Manjavidze, I. A. Minashvili, M. Mineev, K. Nikolaev, A. G. Olchevski, V. D. Peshekhonov, E. Plotnikova, V. Pozdnyakov, V. M. Romanov, L. Rumyantsev, N. A. Rusakovich, R. Sadykov, M. Shiyakova, A. N. Sisakyan, N. D. Topilin, V. B. Vinogradov & A. Zhemchugov
KEK, High Energy Accelerator Research Organization, Tsukuba, Japan
K. Amako, Y. Arai, Y. Doi, T. Haruyama, Y. Ikegami, M. Ikeno, H. Iwasaki, J. Kanzaki, T. Kohriki, T. Kondo, Y. Makida, A. Manabe, S. Mitsui, K. Nagano, M. Nozaki, S. Odaka, O. Sasaki, Y. Suzuki, Y. Takubo, S. Tanaka, S. Terada, K. Tokushuku, S. Tsuno, Y. Unno, M. Yamada, A. Yamamoto & Y. Yasu
Graduate School of Science, Kobe University, Kobe, Japan
A. Akiyama, T. Hayakawa, Y. Homma, R. Ichimiya, A. Ishikawa, M. King, T. Kishimoto, H. Kurashige, T. Matsushita, K. Miyazaki, T. Nishiyama, A. Ochi, S. Okada, C. Omachi, K. Suita, Y. Suzuki, H. Takeda, K. Tani, K. Tokunaga, Y. Yamazaki & L. Yuan
Faculty of Science, Kyoto University, Kyoto, Japan
M. Ishino, N. Sasao & T. Sumida
Kyoto University of Education, Kyoto, Japan
R. Takashima
Department of Physics, Kyushu University, Fukuoka, Japan
K. Kawagoe & J. Tojo
Instituto de Física La Plata, Universidad Nacional de La Plata and CONICET, La Plata, Argentina
X. S. Anduaga, M. T. Dova, F. Monticelli & M. F. Tripiana
Physics Department, Lancaster University, Lancaster, United Kingdom
A. E. Barton, G. Borissov, E. V. Bouhova-Thacker, T. J. Brodbeck, A. Chilingarov, R. Davidson, L. de Mora, W. J. Dearnaley, H. Fox, R. C. W. Henderson, G. Hughes, R. W. L. Jones, V. Kartvelishvili, R. E. Long, P. A. Love, P. N. Ratoff, M. Smizanska & J. Walder
INFN Sezione di Lecce, Lecce, Italy
M. Bianco, G. Cataldi, G. Chiodini, R. Crupi, E. Gorini, F. Grancagnolo, A. Guida, N. Orlando, R. Perrino, M. Primavera, S. Spagnolo & A. Ventura
Dipartimento di Fisica, Università del Salento, Lecce, Italy
M. Bianco, R. Crupi, E. Gorini, A. Guida, N. Orlando, S. Spagnolo & A. Ventura
Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom
P. P. Allport, A. C. Bundock, S. Burdin, M. D’Onofrio, P. Dervan, T. Greenshaw, C. B. Gwilliam, H. S. Hayward, M. A. Houlden, J. N. Jackson, T. J. Jones, B. T. King, M. Klein, U. Klein, T. Kluge, J. Kretzschmar, P. Laycock, S. Mahmoud, S. J. Maxfield, A. Mehta, S. Migas, J. Price, G. Sellers, J. H. Vossebeld, P. Waller & B. Wrona
Department of Physics, Jožef Stefan Institute and University of Ljubljana, Ljubljana, Slovenia
V. Cindro, M. Deliyergiyev, I. Dolenc, A. Filipčič, A. Gorišek, B. P. Kerševan, G. Kramberger, B. Maček, I. Mandić, M. Mikuž & A. Tykhonov
School of Physics and Astronomy, Queen Mary University of London, London, United Kingdom
P. Adragna, M. Bona, A. A. Carter, L. Cerrito, E. Eisenhandler, K. Ellis, J. R. Goddard, M. P. J. Landon, S. L. Lloyd, J. Morin, J. D. Morris, E. Piccaro, J. Poll, E. Rizvi, G. Salamanna, K. Stevenson, M. Teixeira Dias Castanheira & C. Wiglesworth
Department of Physics, Royal Holloway University of London, Surrey, United Kingdom
M. A. Alam, T. Berry, V. Boisvert, G. Cowan, C. A. Edwards, S. George, R. Gonçalo, D. Hayden, A. Misiejuk, Fr. Pastore, M. Rose, F. Spanò, J. A. Strong & P. Teixeira-Dias
Department of Physics and Astronomy, University College London, London, United Kingdom
S. Baker, P. Bernat, S. P. Bieniek, J. M. Butterworth, M. Campanelli, R. T. Chislett, I. A. Christidi, B. D. Cooper, A. R. Davison, S. Dean, G. G. Hesketh, E. Jansen, T. W. Jones, N. Konstantinidis, L. Lambourne, J. Monk, M. Nash, E. Nurse, R. Prabhu, A. Richards, J. E. M. Robinson, P. Sherwood, B. Simmons, C. Taylor, B. M. Waugh & P. A. Wijeratne
Laboratoire de Physique Nucléaire et de Hautes Energies, UPMC and Université Paris-Diderot and CNRS/IN2P3, Paris, France
T. Beau, M. Bomben, S. Bordoni, G. Calderini, P. Cavalleri, E. Chareyre, S. De Cecco, F. Derue, M. W. Krasny, M. Kuna, D. Lacour, B. Laforge, S. Laplace, O. Le Dortz, G. Marchiori, I. Nikolic-Audit, J. Ocariz, M. Ridel, L. Roos, Ph. Schwemling, T. Theveneaux-Pelzer, H. Torres, S. Trincaz-Duvoid, T. N. Trinh & F. Vannucci
Fysiska institutionen, Lunds universitet, Lund, Sweden
T. P. A. Åkesson, A. Alonso, S. S. Bocchetta, A. Floderus, A. D. Hawkins, V. Hedberg, G. Jarlskog, B. Lundberg, E. Lytken, B. Meirose, J. U. Mjörnmark & O. Smirnova
Departamento de Fisica Teorica C-15, Universidad Autonoma de Madrid, Madrid, Spain
V. Arnal, F. Barreiro, J. Cantero, H. De la Torre, J. Del Peso, C. Glasman, L. Labarga, T. Lagouri, J. Llorente Merino, L. March, E. Nebot & J. Terron
Institut für Physik, Universität Mainz, Mainz, Germany
M. Aharrouche, O. Arnaez, M. Bendel, W. Blum, V. Büscher, R. Caputo, S. Eckweiler, K. Edmonds, F. Ellinghaus, E. Ertel, F. Fiedler, J. Fleckner, C. Goeringer, C. Handel, M. Hohlfeld, P. J. Hsu, W. Ji, G. Kawamura, K. Kleinknecht, S. Koenig, L. Köpke, M. Lungwitz, L. Masetti, C. Meyer, D. Moreno, T. Mueller, A. Neusiedl, H. G. Sander, U. Schäfer, C. Schmitt, C. Schroeder & S. Tapprogge
School of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
J. Almond, M. Borri, G. Brown, V. Chavda, B. E. Cox, C. Da Via, I. P. Duerdoth, A. Forti, J. M. Foster, J. Howarth, R. E. Hughes-Jones, M. Ibbotson, K. D. Joshi, J. A. Klinger, S. D. Kolya, J. L. Lane, F. K. Loebinger, R. Marshall, M. Marx, J. Masik, T. J. Neep, A. Oh, M. Owen, J. R. Pater, A. D. Pilkington, C. Schwanenberger, S. W. Snow, S. Watts & U. K. Yang
CPPM, Aix-Marseille Université and CNRS/IN2P3, Marseille, France
S. Aoun, C. P. Bee, C. Bertella, N. Bousson, J. C. Clemens, Y. Coadou, F. Djama, F. Etienne, L. Feligioni, F. Henry-Couannier, D. Hoffmann, F. Hubaut, E. B. F. G. Knoops, E. Le Guirriec, B. Li, J. Maurer, E. Monnier, J. Odier, P. Pralavorio, Z. Qian, A. Rozanov, M. Talby, N. Tannoury, S. Tisserant, J. Toth, F. Touchard & L. Vacavant
Department of Physics, University of Massachusetts, Amherst, MA, United States of America
B. Brau, G. Colon, C. Dallapiccola, A. Meade, E. J. W. Moyse, P. Pais, E. Pueschel, N. van Eldik, T. Varol, S. Willocq & M. J. Woudstra
Department of Physics, McGill University, Montreal, QC, Canada
C. Belanger-Champagne, B. Caron, B. Chapleau, S. Cheatham, F. Corriveau, M. Dobbs, M-A. Dufour, H. Guler, M. Klemetti, S. H. Robertson, C. Santamarina Rios, M. Schram, M. C. Stockton, B. Vachon & A. Warburton
School of Physics, University of Melbourne, Victoria, Australia
E. L. Barberio, N. Davidson, S. Diglio, T. Kubota, A. Limosani, G. F. Moorhead, G. Nunes Hanninger, A. Phan, M. E. Sevior, Q. T. Shao, G. N. Taylor, M. Volpi & M. J. White
Department of Physics, The University of Michigan, Ann Arbor, MI, United States of America
A. J. Armbruster, S. Borroni, J. W. Chapman, M. Cirilli, T. Dai, E. B. Diehl, A. Eppig, C. Ferretti, S. Goldfarb, D. Harper, D. Levin, X. Li, H. Liu, J. B. Liu, S. P. Mc Kee, H. A. Neal, N. Panikashvili, J. Purdham, J. Qian, D. Scheirich, R. P. Thun, S. Walch, A. Wilson, G. Wooden, H. Yang, B. Zhou & J. Zhu
Department of Physics and Astronomy, Michigan State University, East Lansing, MI, United States of America
M. Abolins, B. Alvarez Gonzalez, G. Arabidze, R. Brock, C. Bromberg, S. Caughron, W. Fedorko, R. Hauser, S. Heim, J. L. Holzbauer, J. Huston, J. Koll, J. Kraus, J. T. Linnemann, P. S. Mangeard, B. Martin, R. J. Miller, B. G. Pope, P. Ryan, R. Schwienhorst, H. J. Stelzer, K. Tollefson & H. Zhang
INFN Sezione di Milano, Milano, Italy
E. Acerbi, F. Alessandria, G. Alimonti, A. Andreazza, G. Baccaglioni, M. I. Besana, F. Broggi, L. Carminati, D. Cavalli, M. Citterio, S. M. Consonni, G. Costa, M. Fanti, A. Favareto, D. Giugni, I. Koletsou, T. Lari, L. Mandelli, M. Mazzanti, F. Meloni, C. Meroni, S. Montesano, L. Perini, C. Pizio, F. Ragusa, S. Resconi, G. Rivoltella, R. Simoniello, G. F. Tartarelli, C. Troncon, R. Turra, G. Vegni & G. Volpini
Dipartimento di Fisica, Università di Milano, Milano, Italy
E. Acerbi, A. Andreazza, M. I. Besana, L. Carminati, S. M. Consonni, M. Fanti, A. Favareto, F. Meloni, S. Montesano, L. Perini, C. Pizio, F. Ragusa, G. Rivoltella, R. Simoniello, R. Turra & G. Vegni
B.I. Stepanov Institute of Physics, National Academy of Sciences of Belarus, Minsk, Republic of Belarus
A. Bogouch, S. Harkusha, Y. Kulchitsky, Y. A. Kurochkin, I. Satsounkevitch & P. V. Tsiareshka
National Scientific and Educational Centre for Particle and High Energy Physics, Minsk, Republic of Belarus
V. Gilewsky, V. Rumiantsev & S. Yanush
Department of Physics, Massachusetts Institute of Technology, Cambridge, MA, United States of America
F. E. Taylor
Group of Particle Physics, University of Montreal, Montreal, QC, Canada
G. Azuelos, P. Banerjee, J. Bouchami, M. Davies, J. Ferland, M. Giunta, C. Lebel, C. Leroy, J. A. Macana Goia, J. P. Martin, R. Mehdiyev & O. Scallon
P.N. Lebedev Institute of Physics, Academy of Sciences, Moscow, Russia
A. V. Akimov, S. P. Baranov, I. L. Gavrilenko, A. A. Komar, R. Mashinistov, S. V. Mouraviev, P. Yu. Nechaeva, A. Shmeleva, A. A. Snesarev, V. V. Sulin & V. O. Tikhomirov
Institute for Theoretical and Experimental Physics (ITEP), Moscow, Russia
A. Artamonov, P. A. Gorbounov, V. Khovanskiy, P. B. Shatalov & I. I. Tsukerman
Moscow Engineering and Physics Institute (MEPhI), Moscow, Russia
A. Antonov, K. Belotskiy, V. G. Bondarenko, O. Bulekov, B. A. Dolgoshein, V. A. Kantserov, A. Khodinov, S. V. Morozov, A. Romaniouk, E. Shulga, S. Yu. Smirnov, Y. Smirnov, E. Soldatov & S. Timoshenko
Skobeltsyn Institute of Nuclear Physics, Lomonosov Moscow State University, Moscow, Russia
L. K. Gladilin, Y. V. Grishkevich, V. A. Kramarenko, V. I. Rud, S. Yu. Sivoklokov & L. N. Smirnova
Fakultät für Physik, Ludwig-Maximilians-Universität München, München, Germany
S. Adomeit, S. Beale, S. Becker, O. Biebel, P. Calfayan, J. de Graat, G. Duckeck, J. Ebke, J. Elmsheuser, A. Engl, C. Galea, C. Heller, R. Hertenberger, J. Kennedy, C. Kummer, F. Legger, M. Lichtnecker, J. Lorenz, R. Mameghani, T. A. Müller, T. Nunnemann, L. B. Oakes, F. Rauscher, P. Reznicek, B. Ruckert, M. P. Sanders, D. Schaile, J. Schieck, C. Serfon, A. Staude, D. Vladoiu, R. Walker, J. Z. Will & X. Zhuang
Max-Planck-Institut für Physik (Werner-Heisenberg-Institut), München, Germany
M. Aderholz, T. Barillari, M. Beimforde, S. Bethke, J. Bronner, D. Capriotti, G. Cortiana, D. Dannheim, J. Dubbert, T. Ehrich, M. J. Flowerdew, P. Giovannini, T. Göttfert, P. Haefner, D. Hauff, A. Jantsch, S. Kaiser, A. E. Kiryunin, S. Kluth, O. Kortner, S. Kortner, S. Kotov, H. Kroha, G. Lutz, A. Macchiolo, A. Manz, S. Menke, S. Mohrdieck-Möck, H. G. Moser, M. Nagel, R. Nisius, H. Oberlack, G. E. Pospelov, I. N. Potrap, R. Richter, D. Salihagic, R. Sandstroem, P. Schacht, R. Seuster, S. Stern, S. Stonjek, M. Vanadia, H. von der Schmitt, J. von Loeben, P. Weigell & V. Zhuravlov
Nagasaki Institute of Applied Science, Nagasaki, Japan
M. Shimojima & Y. Tanaka
Graduate School of Science, Nagoya University, Nagoya, Japan
S. Hasegawa, L. Morvaj, T. Ohshima, Y. Okumura, H. Shichi, T. Sugimoto, Y. Takahashi, M. Tomoto & J. Wakabayashi
INFN Sezione di Napoli, Napoli, Italy
A. Aloisio, M. G. Alviggi, V. Canale, L. Capasso, G. Carlino, F. Cevenini, G. Chiefari, F. Conventi, R. de Asmundis, M. Della Pietra, D. della Volpe, A. Doria, R. Giordano, P. Iengo, V. Izzo, L. Merola, E. Musto, S. Patricelli, A. Sanchez & G. Sekhniaidze
Dipartimento di Scienze Fisiche, Università di Napoli, Napoli, Italy
A. Aloisio, M. G. Alviggi, V. Canale, L. Capasso, F. Cevenini, G. Chiefari, D. della Volpe, R. Giordano, L. Merola, E. Musto, S. Patricelli & A. Sanchez
Department of Physics and Astronomy, University of New Mexico, Albuquerque, NM, United States of America
I. Gorelov, M. R. Hoeferkamp, J. Metcalfe, S. C. Seidel, K. Toms & R. Wang
Institute for Mathematics, Astrophysics and Particle Physics, Radboud University Nijmegen/Nikhef, Nijmegen, Netherlands
S. Caron, M. A. Chelstowska, M. Consonni, N. De Groot, F. Filthaut, P. F. Klok, A. C. König, F. Koetsveld, M. Raas & A. Salvucci
Nikhef National Institute for Subatomic Physics and University of Amsterdam, Amsterdam, Netherlands
S. Bentvelsen, E. Berglund, G. J. Bobbink, K. Bos, H. Boterenbrood, A. P. Colijn, P. de Jong, L. De Nooij, P. O. Deviveiros, A. D. Doxiadis, P. Ferrari, H. Garitaonandia, D. A. A. Geerts, M. Gosselink, F. Hartjes, N. P. Hessey, O. Igonkina, M. S. Kayl, S. Klous, P. Kluit, E. Koffeman, H. Lee, T. Lenz, F. Linde, G. Luijckx, G. Massaro, J. Mechnich, I. Mussche, J. P. Ottersbach, A. Reichold, M. Rijpstra, N. Ruckstuhl, D. Ta, M. Tsiakiris, E. Turlay, H. van der Graaf, E. van der Kraaij, R. Van Der Leeuw, E. van der Poel, Z. van Kesteren, I. van Vulpen, W. Verkerke, J. C. Vermeulen, M. Vranjes Milosavljevic & M. Vreeswijk
Department of Physics, Northern Illinois University, DeKalb, IL, United States of America
R. Calkins, D. Chakraborty, J. G. Rocha de Lima, C. Suhr, A. Yurkewicz & V. Zutshi
Budker Institute of Nuclear Physics, SB RAS, Novosibirsk, Russia
A. Anisenkov, O. Beloborodova, V. B. Bobrovnikov, A. Bogdanchikov, V. A. Kazanin, G. M. Kolachev, A. Korol, V. Malyshev, A. L. Maslennikov, D. A. Maximov, I. Orlov, S. V. Peleganchuk, A. G. Schamov, K. Skovpen, A. Soukharev, A. Talyshev, Y. A. Tikhonov & A. Zaytsev
Department of Physics, New York University, New York, NY, United States of America
B. Budick, D. Casadei, K. Cranmer, L. Hooft van Huysduynen, R. Konoplich, A. Krasznahorkay, G. H. Lewis, A. I. Mincer, P. Nemethy, R. M. Neves, K. Prokofiev, A. Shibata & L. Zhao
Ohio State University, Columbus, OH, United States of America
W. Fernando, M. J. Fisher, K. K. Gan, H. Kagan, R. D. Kass, H. Merritt, J. Moss, A. Nagarkar, D. T. Pignotti, A. M. Rahimi & M. Strang
Faculty of Science, Okayama University, Okayama, Japan
I. Nakano
Homer L. Dodge Department of Physics and Astronomy, University of Oklahoma, Norman, OK, United States of America
B. Abbott, P. Gutierrez, G. S. Huang, D. K. Jana, A. Marzin, R. Meera-Lebbai, M. Saleem, H. Severini, P. Skubic, J. Snow & M. Strauss
Department of Physics, Oklahoma State University, Stillwater, OK, United States of America
B. Abi, A. Khanov, F. Rizatdinova & J. Yu
RCPTM, Palacký University, Olomouc, Czech Republic
P. Hamal & L. Nozka
Center for High Energy Physics, University of Oregon, Eugene, OR, United States of America
J. E. Brau, C. T. Potter, E. Ptacek, P. Radloff, A. Reinsch, J. Searcy, M. Shamim, N. B. Sinev, D. M. Strom & E. Torrence
LAL, Univ. Paris-Sud and CNRS/IN2P3, Orsay, France
S. Abdel Khalek, N. Andari, C. Arnault, E. Auge, P. Barrillon, M. Benoit, S. Binet, C. Bourdarios, C. De La Taille, J. B. De Vivie De Regie, L. Duflot, M. Escalier, L. Fayard, D. Fournier, J.-F. Grivaz, S. Henrot-Versille, J. Hrivnac, L. Iconomidou-Fayard, J. Idarraga, M. Kado, N. Lorenzo Martinez, A. Lounis, N. Makovec, P. Matricon, F. Niedercorn, L. Poggioli, P. Puzo, A. Renaud, D. Rousseau, G. Rybkin, J. B. Sauvan, J. Schaarschmidt, A. C. Schaffer, L. Serin, S. Simion, R. Tanaka, M. Teinturier, J. J. Veillet, I. Vukotic, F. Wicek, D. Zerwas & Z. Zhang
Graduate School of Science, Osaka University, Osaka, Japan
K. Hanagaki, M. Hirose, J. S. H. Lee, T. Meguro, M. Nomachi & Y. Sugaya
Department of Physics, University of Oslo, Oslo, Norway
L. Bugge, T. Buran, D. Cameron, B. K. Gjelsten, E. Lund, F. Ould-Saada, K. Pajchel, A. L. Read, O. Røhne, B. H. Samset, S. Stapnes & A. Strandlie
Department of Physics, Oxford University, Oxford, United Kingdom
A. Abdesselam, R. Apolle, A. J. Barr, C. R. Boddy, G. Brandt, J. Buchanan, R. M. Buckingham, P. Coe, E. Coniavitis, A. M. Cooper-Sarkar, A. Dafinca, E. Davies, S. M. Farrington, E. J. Gallas, L. M. Gilbert, C. Gwenlan, D. Hall, B. M. Hawes, D. F. Howell, T. B. Huffman, C. Issever, G. Jones, M. Karagoz, R. S. B. King, L. A. Kogan, A. Korn, N. Kundu, A. Larner, A. Lewis, Z. Liang, S. S. A. Livermore, J. Loken, C. Mattravers, R. B. Nickerson, A. Pinder, A. Robichaud-Veronneau, N. C. Ryder, D. Short, J. C-L. Tseng, G. H. A. Viehhauser, A. R. Weidberg, S. R. Whitehead, C. J. Young & J. Zhong
INFN Sezione di Pavia, Pavia, Italy
M. Cambiaghi, C. Conta, R. Ferrari, S. Franchino, M. Fraternali, G. Gaudio, M. Livan, A. Negri, G. Polesello, D. M. Rebuzzi, A. Rimoldi, M. Uslenghi & V. Vercesi
Dipartimento di Fisica, Università di Pavia, Pavia, Italy
M. Cambiaghi, C. Conta, S. Franchino, M. Fraternali, M. Livan, A. Negri, D. M. Rebuzzi, A. Rimoldi & M. Uslenghi
Department of Physics, University of Pennsylvania, Philadelphia, PA, United States of America
J. Alison, K. Brendlinger, J. Degenhardt, M. Donega, N. Dressnandt, S. Fratina, E. Hines, T. M. Hong, B. Jackson, J. Kroll, J. Kunkle, B. C. LeGeyt, C. M. Lester, E. Lipeles, F. F. Martin, D. Olivito, R. Ospanov, R. Reece, J. Saxon, D. Schaefer, J. Stahlman, E. Thomson, P. Wagner & H. H. Williams
Petersburg Nuclear Physics Institute, Gatchina, Russia
O. L. Fedin, V. Gratchev, O. G. Grebenyuk, V. P. Maleev, Y. F. Ryabov, V. A. Schegelsky, E. Sedykh & D. M. Seliverstov
INFN Sezione di Pisa, Pisa, Italy
F. Bertolucci, M. Cascella, V. Cavasinni, F. Crescioli, T. Del Prete, A. Dotti, C. Roda, F. Sarri, S. White & Z. Zinonos
Dipartimento di Fisica E. Fermi, Università di Pisa, Pisa, Italy
F. Bertolucci, M. Cascella, V. Cavasinni, F. Crescioli, T. Del Prete, A. Dotti, C. Roda, F. Sarri, S. White & Z. Zinonos
Department of Physics and Astronomy, University of Pittsburgh, Pittsburgh, PA, United States of America
J. Boudreau, W. Cleland, C. Escobar, T. Kittelmann, J. Mueller, V. Paolone, D. Prieur, V. Savinov, S. Wendler & R. Yoosoofmiya
Laboratorio de Instrumentacao e Fisica Experimental de Particulas - LIP, Lisboa, Portugal
A. Amorim, N. Anjos, J. Carvalho, N. F. Castro, P. Conde Muiño, A. Do Valle Wemans, M. C. N. Fiolhais, A. Gomes, P. M. Jorge, L. Lopes, J. Machado Miguens, A. Maio, J. Maneira, M. Oliveira, A. Onofre, A. Palma, J. Pina, B. Pinto, H. Santos, J. G. Saraiva, J. Silva, M. Soares, F. Veloso & H. Wolters
Departamento de Fisica Teorica y del Cosmos and CAFPE, Universidad de Granada, Granada, Spain
J. A. Aguilar-Saavedra
Institute of Physics, Academy of Sciences of the Czech Republic, Praha, Czech Republic
J. Bohm, J. Chudoba, P. Gallus, J. Gunther, I. Hruska, V. Juranek, O. Kepka, A. Kupco, V. Kus, L. Lipinsky, M. Lokajicek, M. Marcisovsky, M. Mikestikova, M. Myska, S. Nemecek, M. Panuskova, P. Ruzicka, J. Schovancova, P. Sicho, P. Staroba, M. Svatos, M. Tasevsky, T. Tic, J. Valenta, V. Vrba & M. Zeman
Faculty of Mathematics and Physics, Charles University in Prague, Praha, Czech Republic
I. Chalupkova, T. Davidek, J. Dolejsi, Z. Dolezal, Z. Drasal, P. Kodys, R. Leitner, J. Novakova, M. Rybar, M. Spousta, P. Strachota, M. Suk, T. Sykora, P. Tas, S. Valkar, V. Vorobel & I. Wilhelm
Czech Technical University in Prague, Praha, Czech Republic
K. Augsten, T. Holy, T. Horazdovsky, Z. Hubacek, J. Jakubek, Z. Kohout, V. Kral, F. Krejci, S. Pospisil, V. Simak, T. Slavicek, K. Smolek, J. Sodomka, M. Solar, J. Solc, V. Sopko, B. Sopko, I. Stekl, D. Turecek, V. Vacek, M. Vlasak & P. Vokac
State Research Center Institute for High Energy Physics, Protvino, Russia
V. V. Ammosov, A. Borisov, N. I. Bozhko, S. P. Denisov, R. M. Fakhrutdinov, A. B. Fenyuk, V. A. Gapienko, V. N. Goryachev, V. N. Gushchin, A. V. Ivashin, V. V. Kabachenko, A. N. Karyukhin, A. G. Kholodenko, A. M. Kiver, V. Koreshev, V. A. Korotkov, A. S. Kozhin, A. V. Larionov, M. S. Levitski, A. A. Minaenko, G. Y. Mitrofanov, A. G. Myagkov, V. Nikolaenko, A. V. Pleskach, V. Ryadovikov, A. A. Solodkov, O. V. Solovyanov, E. A. Starchenko, Yu. M. Sviridov, A. P. Vorobiev, V. G. Zaets, A. M. Zaitsev, O. Zenin & V. V. Zmouchko
Particle Physics Department, Rutherford Appleton Laboratory, Didcot, United Kingdom
T. Adye, J. T. Baines, B. M. Barnett, D. Botterill, S. Burke, R. W. Clifft, A. Dewhurst, D. Emeliyanov, B. J. Gallop, C. N. P. Gee, A. R. Gillman, S. J. Haywood, J. Kirk, N. A. McCubbin, S. J. McMahon, R. P. Middleton, W. J. Murray, P. R. Norton, P. W. Phillips, D. P. C. Sankey, W. G. Scott, J. Strube, M. Tyndel, M. Weber, F. J. Wickens & M. Wielers
Physics Department, University of Regina, Regina, SK, Canada
K. Benslama & G. V. Ybeles Smit
Ritsumeikan University, Kusatsu, Shiga, Japan
S. Tanaka
INFN Sezione di Roma I, Roma, Italy
F. Anulli, G. Artoni, P. Bagnaia, C. Bini, R. Caloi, G. Ciapetti, A. D’Orazio, D. De Pedis, A. De Salvo, G. De Zorzi, C. Dionisi, S. Falciano, P. Gauzzi, S. Gentile, S. Giagu, V. Ippolito, F. Lacava, F. Lo Sterzo, C. Luci, L. Luminari, C. Maiani, F. Marzano, P. Mastrandrea, G. Mirabelli, A. Nisati, E. Pasqualucci, E. Petrolo, L. Pontecorvo, M. Rescigno, S. Rosati, E. Rossi, F. Safai Tehrani, A. Sidoti, E. Solfaroli Camillocci, F. Spila, P. Valente, R. Vari, S. Veneziano & L. Zanello
Dipartimento di Fisica, Università La Sapienza, Roma, Italy
G. Artoni, P. Bagnaia, C. Bini, R. Caloi, G. Ciapetti, A. D’Orazio, G. De Zorzi, C. Dionisi, P. Gauzzi, S. Gentile, S. Giagu, V. Ippolito, F. Lacava, F. Lo Sterzo, C. Luci, C. Maiani, P. Mastrandrea, E. Rossi, E. Solfaroli Camillocci, F. Spila & L. Zanello
INFN Sezione di Roma Tor Vergata, Roma, Italy
G. Aielli, P. Camarri, R. Cardarelli, G. Cattani, A. Di Ciaccio, A. Di Simone, B. Liberti, F. Marchese, L. Mazzaferro, A. Salamon & R. Santonico
Dipartimento di Fisica, Università di Roma Tor Vergata, Roma, Italy
G. Aielli, P. Camarri, G. Cattani, A. Di Ciaccio, A. Di Simone, F. Marchese, L. Mazzaferro & R. Santonico
INFN Sezione di Roma Tre, Roma, Italy
C. Bacci, A. Baroncelli, M. Biglietti, V. Bortolotto, P. Branchini, F. Ceradini, S. Di Luise, A. Farilla, E. Graziani, M. Iodice, D. Orestano, A. Passeri, F. Pastore, F. Petrucci, F. Ruggieri & C. Stanescu
Dipartimento di Fisica, Università Roma Tre, Roma, Italy
C. Bacci, V. Bortolotto, F. Ceradini, S. Di Luise, D. Orestano, F. Pastore, F. Petrucci & F. Ruggieri
Faculté des Sciences Ain Chock, Réseau Universitaire de Physique des Hautes Energies - Université Hassan II, Casablanca, Morocco
D. Benchekroun, A. Chafaq, M. Gouighri, A. Hoummada & S. Lablak
Centre National de l’Energie des Sciences Techniques Nucleaires, Rabat, Morocco
H. Ghazlane
Faculté des Sciences Semlalia, Université Cadi Ayyad, LPHEA-Marrakech, Morocco
M. El Kacimi & D. Goujdami
Faculté des Sciences, Université Mohamed Premier and LPTPM, Oujda, Morocco
J. E. Derkaoui, M. Ouchrif & Y. Tayalati
Faculté des Sciences, Université Mohammed V- Agdal, Rabat, Morocco
R. Cherkaoui El Moursli
DSM/IRFU (Institut de Recherches sur les Lois Fondamentales de l’Univers), CEA Saclay (Commissariat a l’Energie Atomique), Gif-sur-Yvette, France
H. Abreu, H. Bachacou, F. Bauer, N. Besson, J.-B. Blanchard, N. M. Bolnet, M. Boonekamp, L. Chevalier, J. Ernwein, A. I. Etienvre, A. Formica, L. Gauthier, P. F. Giraud, C. Guyot, S. Hassani, W. Kozanecki, E. Lancon, J. F. Laporte, M. Legendre, P. Mal, B. Mansoulie, J-P. Meyer, N. Morange, V. Nguyen Thi Hong, R. Nicolaidou, A. Ouraou, D. M. Pomarede, B. Resende, C. R. Royon, Ph. Schune, J. Schwindling, O. Simard, M. Virchaux, N. Vranjes & M. Xiao
Santa Cruz Institute for Particle Physics, University of California Santa Cruz, Santa Cruz, CA, United States of America
S. Chouridou, D. S. Damiani, K. Fowler, A. A. Grillo, G. A. Hare, A. M. Litke, W. S. Lockman, P. M. Manning, J. Mitrevski, J. Nielsen, H. F-W. Sadrozinski, B. A. Schumm & A. Seiden
Department of Physics, University of Washington, Seattle, WA, United States of America
M. Beckingham, A. Coccaro, D. A. Forbush, A. G. Goussiou, J. Griffiths, O. M. Harris, J. S. Keller, H. J. Lubatti, P. Mockett, J. Rothberg, D. Ventura, M. Verducci, J. C. Wang, G. Watts & T. Zhao
Department of Physics and Astronomy, University of Sheffield, Sheffield, United Kingdom
C. N. Booth, D. Costanzo, T. Cuhadar Donszelmann, I. Dawson, R. Duxfield, M. C. Hodgkinson, P. Hodgson, P. Johansson, E. V. Korolkova, A. Mayne, J. A. Mcfayden, P. S. Miyagawa, L. Nicolas, S. Owen, E. Paganis, K. Suruliz, D. R. Tovey, A. Tua & D. Xu
Department of Physics, Shinshu University, Nagano, Japan
Y. Hasegawa, H. Ohshita & T. Takeshita
Fachbereich Physik, Universität Siegen, Siegen, Germany
P. Buchholz, H. Czirr, I. Fleck, B. Gaur, K. Grybel, M. Holder, I. Ibragimov, M. Rammes, O. Rosenthal, V. Sipica, W. Walkowiak & M. Ziolkowski
Department of Physics, Simon Fraser University, Burnaby, BC, Canada
E. Dawe, J. Godfrey, J. Kvita, D. C. O’Neil, M. Petteni, B. Stelzer, A. J. Tanasijczuk, M. Trottier-McDonald & M. C. Vetterli
SLAC National Accelerator Laboratory, Stanford, CA, United States of America
I. Aracena, T. Barklow, R. Bartoldus, H. S. Bawa, B. Butler, J. G. Cogan, T. Eifert, B. G. Fulsom, Y. S. Gao, P. Grenier, A. Haas, P. Hansson, C. Horn, P. Jackson, M. Kocian, T. Koi, A. J. Lowe, C. Malone, R. Mount, T. K. Nelson, A. Salnikov, A. Schwartzman, D. Silverstein, D. Smith, E. Strauss, D. Su, M. G. Wilson, M. Wittgen & C. Young
Faculty of Mathematics, Physics & Informatics, Comenius University, Bratislava, Slovak Republic
L. Batkova, T. Blazek, P. Federic, M. Pecsy, P. Stavina, I. Sykora, S. Tokár & T. Ženiš
Department of Subnuclear Physics, Institute of Experimental Physics of the Slovak Academy of Sciences, Kosice, Slovak Republic
J. Antos, D. Bruncko, J. Ferencei, E. Kladiva, M. Seman & P. Strizenec
Department of Physics, University of Johannesburg, Johannesburg, South Africa
M. Aurousseau
School of Physics, University of the Witwatersrand, Johannesburg, South Africa
A. Hamilton, K. J. C. Leney, T. Vickey, O. E. Vickey Boeriu & S. Yacoob
Department of Physics, Stockholm University, Stockholm, Sweden
B. Åsman, K. Bendtz, C. Bohm, C. Clement, D. Eriksson, K. Gellerstedt, S. Hellman, S. O. Holmgren, M. Johansen, K. E. Johansson, K. Jon-And, H. Kim, P. Klimek, J. Lesser, J. Lundberg, D. A. Milstead, T. Moa, C. C. Ohm, A. Papadelis, B. Sellden, S. B. Silverstein, J. Sjölin, S. Strandberg, M. Tylmad & Z. Yang
The Oskar Klein Centre, Stockholm, Sweden
B. Åsman, K. Bendtz, C. Clement, K. Gellerstedt, S. Hellman, M. Johansen, K. Jon-And, H. Kim, P. Klimek, J. Lundberg, D. A. Milstead, T. Moa, C. C. Ohm, J. Sjölin, S. Strandberg, M. Tylmad & Z. Yang
Physics Department, Royal Institute of Technology, Stockholm, Sweden
J. Jovicevic, E. S. Kuwertz, B. Lund-Jensen & J. Strandberg
Departments of Physics & Astronomy and Chemistry, Stony Brook University, Stony Brook, NY, United States of America
A. Ahmad, S. Arfaoui, C. Deluca, E. Devetak, B. DeWilde, R. Engelmann, J. Farley, J. J. Goodson, V. Grassi, J. A. Gray, J. Hobbs, J. Jia, R. L. McCarthy, S. Mohapatra, M. Rijssenbeek, R. D. Schamberger, J. Stupak & D. Tsybychev
Department of Physics and Astronomy, University of Sussex, Brighton, United Kingdom
V. Bartsch, A. De Santo, S. Martin-Haugh, C. J. Potter, A. Rose, F. Salvatore & M. R. Sutton
School of Physics, University of Sydney, Sydney, Australia
A. Bangert, C. Cuthbert, N. Patel, A. F. Saavedra, M. Scarcella, K. E. Varvell, I. J. Watson, A. T. Waugh & B. Yabsley
Institute of Physics, Academia Sinica, Taipei, Taiwan
M. L. Chu, S. Hou, S. C. Lee, S. C. Lin, D. Liu, R. Mazini, Z. Meng, Z. L. Ren, D. A. Soh, P. K. Teng, J. Wang, S. M. Wang, Z. Weng & Y. Zhou
Department of Physics, Technion: Israel Inst. of Technology, Haifa, Israel
S. Behar Harpaz, E. Kajomovitz, Y. Rozen, S. Tarem & S. Vallecorsa
Raymond and Beverly Sackler School of Physics and Astronomy, Tel Aviv University, Tel Aviv, Israel
H. Abramowicz, G. Alexander, N. Amram, G. Bella, O. Benary, Y. Benhammou, E. Brodet, E. Etzion, A. Gershon, J. Ginzburg, N. Guttman, N. Hod, Y. Mahalalel, Y. Munwes, Y. Oren, E. Reinherz-Aronis, I. Sadeh, Y. Silver, A. Soffer & N. Taiblum
Department of Physics, Aristotle University of Thessaloniki, Thessaloniki, Greece
D. Iliadis, K. Kordas, V. Kouskoura, I. Nomidis, A. Petridis, C. Petridou & D. Sampsonidis
International Center for Elementary Particle Physics and Department of Physics, The University of Tokyo, Tokyo, Japan
G. Akimoto, S. Asai, Y. Azuma, T. Dohmae, M. Imori, N. Kanaya, Y. Kataoka, T. Kawamoto, K. Kessoku, T. Kobayashi, Y. Komori, T. Mashimo, T. Masubuchi, H. Matsumoto, H. Matsunaga, K. Nakamura, T. Nakamura, Y. Ninomiya, S. Oda, T. Okuyama, H. Sakamoto, J. Tanaka, K. Terashi, I. Ueda, H. Yamaguchi, S. Yamamoto, T. Yamamura, T. Yamanaka & T. Yamazaki
Graduate School of Science and Technology, Tokyo Metropolitan University, Tokyo, Japan
U. Bratzler & C. Fukunaga
Department of Physics, Tokyo Institute of Technology, Tokyo, Japan
O. Jinnouchi, T. Kanno & M. Kuze
Department of Physics, University of Toronto, Toronto, ON, Canada
O. S. AbouZeid, D. C. Bailey, T. Bain, B. Brelier, S. L. Cheung, S. Dhaliwal, T. Farooque, B. Fatholahzadeh, A. Gibson, B. Guo, N. Ilic, J. Keung, N. S. Knecht, P. Krieger, C. Le Maner, F. K. Martens, R. S. Orr, R. Rezvani, G. A. Rosenbaum, P. Savard, P. Sinervo, T. Spreitzer, D. Tardif, R. J. Teuscher, P. D. Thompson, W. Trischuk & N. Venturi
TRIUMF, Vancouver, BC, Canada
A. Canepa, S. V. Chekulaev, D. Fortin, A. Koutsman, M. J. Losty, I. M. Nugent, C. J. Oram, E. Perez Codina, D. Schouten, O. Stelzer-Chilton, R. Tafirout & I. M. Trigger
Department of Physics and Astronomy, York University, Toronto, ON, Canada
J. A. Benitez Garcia, G. Palacino & W. Taylor
Institute of Pure and Applied Sciences, University of Tsukuba, 1-1-1 Tennodai, Tsukuba, Ibaraki, 305-8571, Japan
K. Hanawa, K. Hara, T. Hayashi, S. H. Kim, M. Kurata, K. Nagai & F. Ukegawa
Science and Technology Center, Tufts University, Medford, MA, United States of America
P. H. Beauchemin, S. Hamilton, A. Napier, S. Rolli, K. Sliwa, S. Todorova-Nova & J. Wetter
Centro de Investigaciones, Universidad Antonio Narino, Bogota, Colombia
M. Losada, K. F. Loureiro, L. Mendoza Navas, G. Navarro, D. Rodriguez & C. Sandoval
Department of Physics and Astronomy, University of California Irvine, Irvine, CA, United States of America
G. Avolio, M. Bondioli, J. Deng, S. Farrell, I. Gough Eschrich, D. Hawkins, A. J. Lankford, A. Nelson, H. Okawa, D. A. Scannicchio, M. Schernau, A. Taffard, B. Toggerson, G. Unel, M. Werth, S. J. Wheeler-Ellis, D. Whiteson & N. Zhou
INFN Gruppo Collegato di Udine, Udine, Italy
B. S. Acharya, M. Alhroob, D. Cauz, M. Cobal, B. De Lotto, U. De Sanctis, C. Del Papa, M. Pinamonti, K. Shaw & R. Soualah
ICTP, Trieste, Italy
B. S. Acharya
Dipartimento di Chimica, Fisica e Ambiente, Università di Udine, Udine, Italy
M. Alhroob, D. Cauz, M. Cobal, B. De Lotto, U. De Sanctis, C. Del Papa, M. P. Giordani, M. Pinamonti, K. Shaw & R. Soualah
Department of Physics, University of Illinois, Urbana, IL, United States of America
N. Benekos, J. Coggeshall, A. Cortes-Gonzalez, D. Errede, S. Errede, H. Khandanyan, K. Lie, T. M. Liss, A. McCarn, M. S. Neubauer & I. Vichou
Department of Physics and Astronomy, University of Uppsala, Uppsala, Sweden
R. Brenner, C. P. Buszello, T. Ekelof, M. Ellert, A. Ferrari, C. Isaksson & D. Pelikan
Instituto de Física Corpuscular (IFIC) and Departamento de Física Atómica, Molecular y Nuclear and Departamento de Ingeniería Electrónica and Instituto de Microelectrónica de Barcelona (IMB-CNM), University of Valencia and CSIC, Valencia, Spain
G. Amorós, S. Cabrera Urbán, V. Castillo Gimenez, M. J. Costa, A. Ferrer, L. Fiorini, J. Fuster, C. García, J. E. García Navarro, S. González de la Hoz, Y. Hernández Jiménez, E. Higón-Rodriguez, A. Irles Quiles, M. Kaci, C. Lacasta, V. R. Lacuesta, S. Marti-Garcia, M. Miñano Moya, V. A. Mitsou, R. Moles-Valls, M. Moreno Llácer, E. Oliver Garcia, M. T. Pérez García-Estañ, E. Romero Adam, E. Ros, J. Salt, V. Sanchez Martinez, C. A. Solans, U. Soldevila, J. Sánchez, E. Torró Pastor, E. Valladolid Gallego, J. A. Valls Ferrer, M. Villaplana Perez, M. Vos & A. Wildauer
Department of Physics, University of British Columbia, Vancouver, BC, Canada
D. Axen, C. Gay, Z. Gecse, C. W. Loh, W. J. Mills, S. Swedish & S. Viel
Department of Physics and Astronomy, University of Victoria, Victoria, BC, Canada
J. Albert, A. Astbury, V. Bansal, F. Berghaus, L. Courneyea, M. Fincke-Keeler, R. Keeler, R. Kowalewski, M. Lefebvre, J-R. Lessard, C. P. Marino, A. C. Martyniuk, R. A. McPherson, E. A. Ouellette, M. Plamondon & R. Sobie
Department of Physics, University of Warwick, Coventry, United Kingdom
J. Albert
Waseda University, Tokyo, Japan
N. Kimura & K. Yorita
Department of Particle Physics, The Weizmann Institute of Science, Rehovot, Israel
R. Alon, L. Barak, S. Bressler, E. Duchovni, T. Frank, O. Gabizon, E. Gross, J. Groth-Jensen, A. Klier, D. Lellouch, L. J. Levinson, G. Mikenberg, A. Milov, D. Milstein, I. Roth, O. Silbert, V. Smakhtin & O. Vitells
Department of Physics, University of Wisconsin, Madison, WI, United States of America
R. Asfandiyarov, Sw. Banerjee, G. D. Carrillo Montoya, A. M. Castaneda Hernandez, E. Castaneda-Miranda, X. Chen, A. Di Mattia, A. Dos Anjos, Y. Fang, L. R. Flores Castillo, S. Gonzalez, O. Gutzwiller, H. Ji, X. Ju, L. Kashif, H. Li, L. L. Ma, B. R. Mellado Garcia, Y. Ming, Y. B. Pan, M. I. Pedraza Morales, J. Poveda, W. B. Quayle, T. Sarangi, H. Wang, W. Wiedenmann, S. L. Wu & G. Zobernig
Fakultät für Physik und Astronomie, Julius-Maximilians-Universität, Würzburg, Germany
P. Fleischmann, J. Meyer, A. Redelbach, G. Siragusa, R. Ströhmer & T. Trefzger
Fachbereich C Physik, Bergische Universität Wuppertal, Wuppertal, Germany
M. Barisonzi, K. H. Becks, J. Boek, H. M. Braun, T. Cornelissen, J. Drees, S. Fleischmann, T. Flick, P. Gerlach, K. W. Glitza, G. Gorfine, K. Hamacher, T. Harenberg, T. Henß, D. Hirschbuehl, S. Kalinin, S. Kersten, A. Khoroshilov, S. Kohlmann, A. Kootz, K. Lantzsch, G. Lenzen, P. Mättig, M. Mechtel, S. Pataraia, M. Sandhoff, S. Sandvoss, G. Sartisohn, J. Schultes, P. Sturm, J. Thadome, T. T. Voss, W. Wagner, H. Wahlen, D. Wicke & C. Zeitnitz
Department of Physics, Yale University, New Haven, CT, United States of America
J. Adelman, O. K. Baker, S. Bedikian, C. Cuenca Almenar, Z. Czyczula, S. Demers, F. Garberson, T. Golling, D. Guest, B. Kaplan, L. Lee, A. Loginov, A. J. Martin, D. Sherman, M. Thioye, P. Tipton, R. Wall & M. Zeller
Yerevan Physics Institute, Yerevan, Armenia
H. Hakobyan
Domaine scientifique de la Doua, Centre de Calcul CNRS/IN2P3, Villeurbanne Cedex, France
C. Biscarat, E. Cogneras & G. Rahal
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The ATLAS Collaboration., Aad, G., Abbott, B. et al. Search for second generation scalar leptoquarks in pp collisions at \(\sqrt{s}=7~\mbox{TeV}\) with the ATLAS detector. Eur. Phys. J. C 72, 2151 (2012). https://doi.org/10.1140/epjc/s10052-012-2151-6
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DOI: https://doi.org/10.1140/epjc/s10052-012-2151-6
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