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arXiv:1102.2357v2 [hep-ex] 17 Feb 2011 CERN-PH-EP-2011-013, Submitted to Phys. Rev. Lett. Search for supersymmetry using final states with one lepton, jets, and missing transverse momentum with the ATLAS detector in s =7 TeV pp collisions The ATLAS Collaboration This Letter presents the first search for supersymmetry in final states containing one isolated electron or muon, jets, and missing transverse momentum from s = 7 TeV proton-proton collisions at the LHC. The data were recorded by the ATLAS experiment during 2010 and correspond to a total integrated luminosity of 35 pb -1 . No excess above the standard model background expectation is observed. Limits are set on the parameters of the minimal supergravity framework, extending previous limits. For A0 = 0 GeV, tan β = 3, μ> 0 and for equal squark and gluino masses, gluino masses below 700 GeV are excluded at 95% confidence level. PACS numbers: 12.60.Jv, 14.80.Ly Many extensions of the standard model predict the existence of new colored particles, such as the squarks q) and gluinos g) of supersymmetric (SUSY) the- ories [1], which could be accessible at the LHC. The dominant SUSY production channels are squark- (anti)squark, squark-gluino, and gluino-gluino pair pro- duction. Squarks and gluinos are expected to decay to quarks and gluons and the SUSY partners of the gauge bosons (charginos, ˜ χ ± , and neutralinos, ˜ χ 0 ), leading to events with energetic jets. In R-parity conserving SUSY models [2], the lightest supersymmetric particle (LSP) is stable and escapes detection, giving rise to events with significant missing transverse momentum. In decay chains with charginos (˜ q L q ˜ χ ± g q ¯ q ˜ χ ± ), chargino decay to the LSP can produce a high-momentum lepton. Currently, the most stringent limits on squark and gluino masses come from the LHC [3] and from the Tevatron [4– 6]. This Letter reports on a search for events with exactly one isolated high-transverse momentum (p T ) electron or muon, at least three high-p T jets, and significant missing transverse momentum. An exact definition of the signal region will be given elsewhere in this Letter. From an experimental point of view, the requirement of an iso- lated high-p T lepton suppresses the QCD multijet back- ground and facilitates triggering on interesting events. In addition to the signal region, three control regions are considered for the most important standard model backgrounds. A combined fit to the observed number of events in these four regions, together with an inde- pendent estimate of jets misidentified as leptons in QCD multijet events, is used to search for an excess of events in the signal region. The analysis is sensitive to any new physics leading to such an excess, and is not optimized for any particular model of SUSY. The results are interpreted within the MSUGRA/CMSSM (minimal supergravity/constrained minimal supersymmetric standard model) framework [7, 8] in terms of limits on the universal scalar and gaugino mass parameters m 0 and m 1/2 . These are presented for fixed values of the universal trilinear coupling parame- ter A 0 = 0 GeV, ratio of the vacuum expectation values of the two Higgs doublets tan β = 3, and Higgs mixing parameter μ> 0, in order to facilitate comparison with previous results. The ATLAS detector [9] is a multipurpose particle physics apparatus with a forward-backward symmetric cylindrical geometry and near 4π coverage in solid an- gle [10]. The inner tracking detector (ID) consists of a silicon pixel detector, a silicon microstrip detector (SCT), and a transition radiation tracker (TRT). The ID is sur- rounded by a thin superconducting solenoid providing a 2 T magnetic field, and by high-granularity liquid-argon (LAr) sampling electromagnetic calorimeters. An iron- scintillator tile calorimeter provides hadronic coverage in the central rapidity range. The end-cap and forward re- gions are instrumented with LAr calorimetry for both electromagnetic and hadronic measurements. The muon spectrometer (MS) surrounds the calorimeters and con- sists of three large superconducting toroids, a system of precision tracking chambers, and detectors for triggering. The data used in this analysis were recorded in 2010 at the LHC at a center-of-mass energy of 7 TeV. Appli- cation of beam, detector, and data-quality requirements results in a total integrated luminosity of 35 pb 1 , with an estimated uncertainty of 11% [11]. The data have been selected with single lepton (e or μ) triggers. The detailed trigger requirements vary throughout the data- taking period, but the thresholds are always low enough to ensure that leptons with p T > 20 GeV lie in the effi- ciency plateau. Fully simulated Monte Carlo event samples are used to develop and validate the analysis procedure, compute de- tector acceptance and reconstruction efficiency, and aid in the background determination. Samples of events for background processes are generated as described in de- tail in Ref. [12]. For the major backgrounds, top quark pair and W +jets production, MC@NLO [13] v3.41 and
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Page 1: Search for Supersymmetry Using Final States with One Lepton, Jets, and Missing Transverse Momentum with the ATLAS Detector in s=7TeV pp Collisions

arX

iv:1

102.

2357

v2 [

hep-

ex]

17

Feb

2011

CERN-PH-EP-2011-013, Submitted to Phys. Rev. Lett.

Search for supersymmetry using final states with one lepton, jets, and missing

transverse momentum with the ATLAS detector in√s = 7 TeV pp collisions

The ATLAS Collaboration

This Letter presents the first search for supersymmetry in final states containing one isolatedelectron or muon, jets, and missing transverse momentum from

√s = 7 TeV proton-proton collisions

at the LHC. The data were recorded by the ATLAS experiment during 2010 and correspond to atotal integrated luminosity of 35 pb−1. No excess above the standard model background expectationis observed. Limits are set on the parameters of the minimal supergravity framework, extendingprevious limits. For A0 = 0 GeV, tanβ = 3, µ > 0 and for equal squark and gluino masses, gluinomasses below 700 GeV are excluded at 95% confidence level.

PACS numbers: 12.60.Jv, 14.80.Ly

Many extensions of the standard model predict theexistence of new colored particles, such as the squarks(q) and gluinos (g) of supersymmetric (SUSY) the-ories [1], which could be accessible at the LHC.The dominant SUSY production channels are squark-(anti)squark, squark-gluino, and gluino-gluino pair pro-duction. Squarks and gluinos are expected to decay toquarks and gluons and the SUSY partners of the gaugebosons (charginos, χ

±, and neutralinos, χ

0), leading to

events with energetic jets. In R-parity conserving SUSYmodels [2], the lightest supersymmetric particle (LSP)is stable and escapes detection, giving rise to eventswith significant missing transverse momentum. In decaychains with charginos (qL → qχ

±, g → qq′χ

±), chargino

decay to the LSP can produce a high-momentum lepton.Currently, the most stringent limits on squark and gluinomasses come from the LHC [3] and from the Tevatron [4–6].

This Letter reports on a search for events with exactlyone isolated high-transverse momentum (pT) electron ormuon, at least three high-pT jets, and significant missingtransverse momentum. An exact definition of the signalregion will be given elsewhere in this Letter. From anexperimental point of view, the requirement of an iso-lated high-pT lepton suppresses the QCD multijet back-ground and facilitates triggering on interesting events.In addition to the signal region, three control regionsare considered for the most important standard modelbackgrounds. A combined fit to the observed numberof events in these four regions, together with an inde-pendent estimate of jets misidentified as leptons in QCDmultijet events, is used to search for an excess of eventsin the signal region.

The analysis is sensitive to any new physics leading tosuch an excess, and is not optimized for any particularmodel of SUSY. The results are interpreted within theMSUGRA/CMSSM (minimal supergravity/constrainedminimal supersymmetric standard model) framework [7,8] in terms of limits on the universal scalar and gaugino

mass parameters m0 and m1/2. These are presented forfixed values of the universal trilinear coupling parame-ter A0 = 0 GeV, ratio of the vacuum expectation valuesof the two Higgs doublets tanβ = 3, and Higgs mixingparameter µ > 0, in order to facilitate comparison withprevious results.

The ATLAS detector [9] is a multipurpose particlephysics apparatus with a forward-backward symmetriccylindrical geometry and near 4π coverage in solid an-gle [10]. The inner tracking detector (ID) consists of asilicon pixel detector, a silicon microstrip detector (SCT),and a transition radiation tracker (TRT). The ID is sur-rounded by a thin superconducting solenoid providing a2 T magnetic field, and by high-granularity liquid-argon(LAr) sampling electromagnetic calorimeters. An iron-scintillator tile calorimeter provides hadronic coverage inthe central rapidity range. The end-cap and forward re-gions are instrumented with LAr calorimetry for bothelectromagnetic and hadronic measurements. The muonspectrometer (MS) surrounds the calorimeters and con-sists of three large superconducting toroids, a system ofprecision tracking chambers, and detectors for triggering.

The data used in this analysis were recorded in 2010at the LHC at a center-of-mass energy of 7 TeV. Appli-cation of beam, detector, and data-quality requirementsresults in a total integrated luminosity of 35 pb−1, withan estimated uncertainty of 11% [11]. The data havebeen selected with single lepton (e or µ) triggers. Thedetailed trigger requirements vary throughout the data-taking period, but the thresholds are always low enoughto ensure that leptons with pT > 20 GeV lie in the effi-ciency plateau.

Fully simulated Monte Carlo event samples are used todevelop and validate the analysis procedure, compute de-tector acceptance and reconstruction efficiency, and aidin the background determination. Samples of events forbackground processes are generated as described in de-tail in Ref. [12]. For the major backgrounds, top quarkpair and W+jets production, MC@NLO [13] v3.41 and

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2

ALPGEN [14] v2.13 are used. Further samples includeQCD multijet events, single top production, diboson pro-duction, and Drell-Yan dilepton events.Monte Carlo signal events are generated with Her-

wig++ [15] v2.4.2. The SUSY particle spectra and de-cay modes are calculated with ISAJET [16] v7.75. TheSUSY samples are normalized using next-to-leading or-der (NLO) cross sections as determined by Prospino [17]v2.1. All signal and background samples are producedusing the ATLAS MC09 parameter tune [18] and aGEANT4 based [19] detector simulation [20].Criteria for electron and muon identification closely

follow those described in Ref. [21]. Electrons in the signalregion are required to pass the “tight” selection criteria,with pT > 20 GeV and |η| < 2.47. Events are alwaysvetoed if a “medium” electron is found in the electromag-netic calorimeter transition region, 1.37 < |η| < 1.52.Muons are required to be identified either in both ID

and MS systems (combined muons) or as a match be-tween an extrapolated ID track and one or more segmentsin the MS. The ID track is required to have at least onepixel hit, more than five SCT hits, and a number of TRThits that varies with η. For combined muons, a goodmatch between ID and MS tracks is required, and the pTvalues measured by these two systems must be compat-ible within the resolution. The summed pT of other IDtracks within a distance ∆R =

(∆η)2 + (∆φ)2 < 0.2around the muon track is required to be less than 1.8GeV. Only muons with pT > 20 GeV and |η| < 2.4 areconsidered. For the final selection, the distance betweenthe z coordinate of the primary vertex and that of theextrapolated muon track at the point of closest approachto the primary vertex must be less than 10 mm.Jets are reconstructed using the anti-kt jet cluster-

ing algorithm [22] with a radius parameter R = 0.4.The inputs to this algorithm are clusters of calorimetercells seeded by cells with energy significantly above themeasured noise. Jets are constructed by performing afour-vector sum over these clusters, treating each clusteras an (E, ~p) four-vector with zero mass. Jets are cor-rected for calorimeter non-compensation, upstream ma-terial and other effects using pT- and η-dependent cali-bration factors obtained from Monte Carlo and validatedwith extensive test-beam and collision-data studies [23].Only jets with pT > 20 GeV and |η| < 2.5 are consid-ered. If a jet and a “medium” electron are both identifiedwithin a distance ∆R < 0.2 of each other, the jet is dis-carded. Furthermore, identified “medium” electrons ormuons are only considered if they satisfy ∆R > 0.4 withrespect to the closest remaining jet. Events are discardedif they contain any jet failing basic quality selection cri-teria, which reject detector noise and non-collision back-grounds [24].The calculation of the missing transverse momentum,

EmissT , is based on the modulus of the vectorial sum of the

pT of the reconstructed objects (jets with pT > 20 GeV,

but over the full calorimeter coverage |η| < 4.9, and theselected lepton), any additional non–isolated muons andthe calorimeter clusters not belonging to reconstructedobjects.

Events are required to have at least one reconstructedprimary vertex with at least five associated tracks. Theselection criteria for signal and control regions are basedon Monte Carlo studies prior to examining the data. Thesignal region is defined as follows. At least one identifiedelectron or muon with pT > 20 GeV is required. Eventsare rejected if they contain a second identified lepton withpT > 20 GeV, because they are the subject of a futureanalysis. At least three jets with pT > 30 GeV are re-quired, the leading one of which must have pT > 60 GeV.In order to reduce the background of events with fakeEmiss

T from mismeasured jets, the missing transverse mo-

mentum vector ~EmissT is required not to point in the di-

rection of any of the three leading jets: ∆φ(jeti, ~EmissT ) >

0.2 (i = 1, 2, 3). The transverse mass between the leptonand the missing transverse momentum vector, mT =√

2 · pℓT · EmissT · (1− cos(∆φ(ℓ, Emiss

T ))), is required to be

larger than 100 GeV. EmissT must exceed 125 GeV and

must satisfy EmissT > 0.25meff, where the effective mass

meff is the scalar sum of the pT of the three leading jets,the pT of the lepton, and Emiss

T . Finally, a cut is appliedon the effective mass: meff > 500 GeV. The efficiency forthe SUSY signal in the MSUGRA/CMSSM model de-fined earlier varies between 0.01% for m1/2 = 100 GeVand 4% for m1/2 = 350 GeV, with a smaller dependenceon m0, for the electron channel and the muon channelseparately. The inefficiency is dominated by the leptonicbranching fractions in the SUSY signal.

Backgrounds from several standard model processescould contaminate the signal region. Top quark pairproduction and W+jets production backgrounds are es-timated from a combined fit to the number of observedevents in three control regions, using Monte Carlo sim-ulations to derive the background in the signal regionfrom the control regions. The background determina-tion of QCD multijet production with a jet misidentifiedas an isolated lepton is purely data driven. Remainingbackgrounds from other sources are estimated with sim-ulations.

The three control regions have identical lepton and jetselection criteria as the signal region. The top controlregion is defined by a window in the two-dimensionalplane of 30 GeV < Emiss

T < 80 GeV and 40 GeV < mT <

80 GeV and by requiring that at least one of the threeleading jets is tagged as a b-quark jet. For the b-tagging,the secondary vertex algorithm SV0 [25] is used, which,for pT = 60 GeV jets, provides an efficiency of 50% for b-quark jets and a mistag rate of 0.5% for light-quark jets.The W control region is defined by the same windowin the Emiss

T −mT plane, but with the requirement thatnone of the three hardest jets is b-tagged. The QCD mul-

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tijet control region is defined by demanding low missingtransverse momentum, Emiss

T < 40 GeV, and low trans-verse mass, mT < 40 GeV. This QCD control region isonly used to estimate the QCD multijet background con-tribution to other background regions but not to the sig-nal region. Instead, the electron and muon identificationcriteria are relaxed, obtaining a “loose” control samplethat is dominated by QCD jets. A loose-tight matrixmethod, in close analogy to that described in Ref. [12], isthen used to estimate the number of QCD multijet eventswith fake leptons in the signal region after final selectioncriteria: 0.0+0.5

−0.0 in the muon channel and 0.0+0.3−0.0 in the

electron channel.

Data are compared to expectations in Figure 1. Thestandard model backgrounds in the figure are normalizedto the theoretical cross sections, except for the multi-jet background which is normalized to data in the QCDmultijet control region. The data are in good agreementwith the standard model expectations. After final selec-tion, one event remains in the signal region in the elec-tron channel and one event remains in the muon chan-nel. Figure 1 also shows the expected distributions forthe MSUGRA/CMSSM model point m0 = 360 GeV andm1/2 = 280 GeV.

A combined fit to the number of observed events inthe signal and control regions is performed. The as-sumption that the Monte Carlo is able to predict thebackgrounds in the signal region from the control re-gions is validated by checking additional control regionsat low mT and at low Emiss

T . The defined control re-gions are not completely pure, and the combined fit takesthe expected background cross-contaminations into ac-count. The likelihood function of the fit can be writtenas: L(n|s,b, θ) = PS × PW × PT × PQ × CSyst, where nrepresents the number of observed events in data, s is theSUSY signal to be tested, b is the background, and θ rep-resents the systematic uncertainties, which are treated asnuisance parameters with a Gaussian probability densityfunction. The four P functions in the right hand sideare Poisson probability distributions for event counts inthe defined signal (S) and control regions (W, T, and Qfor W , top pair and QCD multijets respectively), andCSyst represents the constraints on systematic uncertain-ties, including correlations.The dominant sources of systematic uncertainties in

the background estimates arise from Monte Carlo mod-eling of the shape of the Emiss

T and mT distributions insignal and control regions. These uncertainties are de-termined by variation of the Monte Carlo generator, aswell as by variations of internal generator parameters. Fi-nite statistics in the background control regions also con-tributes to the uncertainty. Experimental uncertaintiesare varied within their determined range and are domi-nated by the jet energy scale uncertainty [26], b-tagginguncertainties, and the uncertainty on the luminosity.Systematic uncertainties on the SUSY signal are esti-

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FIG. 1: Top: EmissT distribution after lepton and jet selection.

Center: mT distribution after lepton and jet selection. Bot-tom: Effective mass distribution after final selection criteriaexcept for the cut on the effective mass itself. All plots aremade for the electron and muon channel combined. Yellowbands indicate the uncertainty on the Monte Carlo predic-tion from finite Monte Carlo statistics and from the jet energyscale uncertainty.

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mated by variation of the factorization and renormaliza-tion scales in Prospino and by including the parton den-sity function (PDF) uncertainties using the eigenvectorsets provided by CTEQ6 [27]. Uncertainties are calcu-lated separately for the individual production processes.Within the relevant kinematic range, typical uncertain-ties resulting from scale variations are 10–16%, whereasPDF uncertainties vary from 5% for qq production to15–30% for gg production.

The result of the combined fit to signal and control re-gions, leaving the number of signal events free in the sig-nal region while not allowing for a signal contaminationin the other regions, is shown in Table I. The observednumber of events in data is consistent with the standardmodel expectation.

Limits are set on contributions of new physics to thesignal region. These limits are obtained from a secondcombined fit to the four regions, this time allowing for asignal in all four regions, and leaving all nuisance parame-ters free. The limits are then derived from the profile like-

lihood ratio, Λ(s) = −2(lnL(n|s, ˆb, ˆθ) − lnL(n|s, b, θ)),where s, b and θ maximize the likelihood function and

ˆb

andˆθ maximize the likelihood for a given choice of s. In

the fit, s and s are constrained to be non-negative. Thetest statistic is Λ(s). The exclusion p-values are obtainedfrom this using pseudo-experiments and the limits set areone-sided upper limits [28].

From the fit to a model with signal events only in thesignal region, a 95% CL upper limit on the number ofevents from new physics in the signal region can be de-rived. This number is 2.2 in the electron channel and 2.5in the muon channel. This corresponds to a 95% CL up-per limit on the effective cross section for new processesin the signal region, including the effects of experimen-tal acceptance and efficiency, of 0.065 pb for the electronchannel and 0.073 pb for the muon channel.

Within the MSUGRA/CMSSM framework, the resultsare interpreted as limits in the m0−m1/2 plane, as shownin Figure 2. For the model considered and for equalsquark and gluino masses, gluino masses below 700 GeVare excluded at 95% CL. The limits depend only moder-ately on tanβ.

In summary, the first ATLAS results on searches forsupersymmetry with an isolated electron or muon, jets,and missing transverse momentum have been presented.In a data sample corresponding to 35 pb−1, no sig-nificant deviations from the standard model expecta-tion are observed. Limits on the cross section for newprocesses within the experimental acceptance and effi-ciency are set. For a chosen set of parameters withinMSUGRA/CMSSM, and for equal squark and gluinomasses, gluino masses below 700 GeV are excluded at95% CL. These ATLAS results exceed previous limits setby other experiments [3–6].

We wish to thank CERN for the efficient commission-

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±χ∼D0 -1<0, 2.1 fbµ, q~, g~D0

-1=5, 2 fbβ, tanq~, g~CDF

FIG. 2: Observed and expected 95% CL exclusion limits, aswell as the ±1σ variation on the expected limit, in the com-bined electron and muon channels. Also shown are the pub-lished limits from CMS [3], CDF [4], and D0 [5, 6], and theresults from the LEP experiments [29].

ing and operation of the LHC during this initial high-energy data-taking period as well as the support stafffrom our institutions without whom ATLAS could notbe 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; CON-ICYT, Chile; CAS, MOST and NSFC, China; COL-CIENCIAS, Colombia; MSMT CR, MPO CR and VSCCR, Czech Republic; DNRF, DNSRC and LundbeckFoundation, Denmark; ARTEMIS, European Union;IN2P3-CNRS, CEA-DSM/IRFU, France; GNAS, Geor-gia; BMBF, DFG, HGF, MPG and AvH Foundation,Germany; GSRT, Greece; ISF, MINERVA, GIF, DIP andBenoziyo 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 Rus-sia and ROSATOM, Russian Federation; JINR; MSTD,Serbia; MSSR, Slovakia; ARRS and MVZT, Slovenia;DST/NRF, South Africa; MICINN, Spain; SRC andWallenberg Foundation, Sweden; SER, SNSF and Can-tons of Bern and Geneva, Switzerland; NSC, Taiwan;TAEK, Turkey; STFC, the Royal Society and Lever-hulme Trust, United Kingdom; DOE and NSF, UnitedStates of America.The crucial computing support from all WLCG part-

ners is acknowledged gratefully, in particular fromCERN 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 (Tai-wan), RAL (UK) and BNL (USA) and in the Tier-2 fa-cilities worldwide.

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TABLE I: Numbers of observed events in the signal and background control regions, as well as their estimated values from thefit (see text), for the electron (top part) and muon (bottom part) channels. The central values of the fitted sum of backgroundsin the control regions agree with the observations by construction. For comparison, nominal Monte Carlo expectations aregiven in parentheses for the signal region, the top control region and the W control region.

Electron channel Signal region Top region W region QCD region

Observed events 1 80 202 1464

Fitted top events 1.34± 0.52 (1.29) 65 ± 12 (63) 32± 16 (31) 40± 11

Fitted W/Z events 0.47± 0.40 (0.46) 11.2± 4.6 (10.2) 161 ± 27 (146) 170 ± 34

Fitted QCD events 0.0+0.3

−0.03.7± 7.6 9± 20 1254 ± 51

Fitted sum of background events 1.81± 0.75 80± 9 202± 14 1464 ± 38

Muon channel Signal region Top region W region QCD region

Observed events 1 93 165 346

Fitted top events 1.76 ± 0.67 (1.39) 85± 11 (67) 42± 19 (33) 50± 10

Fitted W/Z events 0.49 ± 0.36 (0.71) 7.7± 3.3 (11.6) 120 ± 26 (166) 71± 16

Fitted QCD events 0.0+0.5

−0.00.3± 1.2 3± 12 225 ± 22

Fitted sum of background events 2.25± 0.94 93± 10 165± 13 346 ± 19

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S08003.[10] ATLAS uses a right-handed coordinate system with its

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The ATLAS Collaboration

G. Aad48, B. Abbott112, J. Abdallah11,A.A. Abdelalim49, A. Abdesselam119, O. Abdinov10,B. Abi113, M. Abolins89, H. Abramowicz154,H. Abreu116, E. Acerbi90a,90b, B.S. Acharya165a,165b,D.L. Adams24, T.N. Addy56, J. Adelman176,M. Aderholz100, S. Adomeit99, P. Adragna75,T. Adye130, S. Aefsky22, J.A. Aguilar-Saavedra125b,a,M. Aharrouche82, S.P. Ahlen21, F. Ahles48,A. Ahmad149, M. Ahsan40, G. Aielli134a,134b,T. Akdogan18a, T.P.A. Akesson80, G. Akimoto156,A.V. Akimov 95, M.S. Alam1, M.A. Alam76,S. Albrand55, M. Aleksa29, I.N. Aleksandrov65,M. Aleppo90a,90b, F. Alessandria90a, C. Alexa25a,G. Alexander154, G. Alexandre49, T. Alexopoulos9,M. Alhroob20, M. Aliev15, G. Alimonti90a, J. Alison121,M. Aliyev10, P.P. Allport73, S.E. Allwood-Spiers53,J. Almond83, A. Aloisio103a,103b, R. Alon172,A. Alonso80, M.G. Alviggi103a,103b, K. Amako66,P. Amaral29, C. Amelung22, V.V. Ammosov129,A. Amorim125a,b, G. Amoros168, N. Amram154,C. Anastopoulos140, T. Andeen34, C.F. Anders20,K.J. Anderson30, A. Andreazza90a,90b, V. Andrei58a,M-L. Andrieux55, X.S. Anduaga70, A. Angerami34,F. Anghinolfi29, N. Anjos125a, A. Annovi47,A. Antonaki8, M. Antonelli47, S. Antonelli19a,19b,J. Antos145b, F. Anulli133a, S. Aoun84, L. Aperio Bella4,R. Apolle119, G. Arabidze89, I. Aracena144, Y. Arai66,A.T.H. Arce44, J.P. Archambault28, S. Arfaoui29,c,J-F. Arguin14, E. Arik18a,∗, M. Arik18a,A.J. Armbruster88, O. Arnaez82, C. Arnault116,A. Artamonov96, G. Artoni133a,133b, D. Arutinov20,S. Asai156, R. Asfandiyarov173, S. Ask27,B. Asman147a,147b, L. Asquith5, K. Assamagan24,A. Astbury170, A. Astvatsatourov52, G. Atoian176,B. Aubert4, B. Auerbach176, E. Auge116,K. Augsten128, M. Aurousseau4, N. Austin73,R. Avramidou9, D. Axen169, C. Ay54, G. Azuelos94,d,Y. Azuma156, M.A. Baak29, G. Baccaglioni90a,C. Bacci135a,135b, A.M. Bach14, H. Bachacou137,K. Bachas29, G. Bachy29, M. Backes49, M. Backhaus20,E. Badescu25a, P. Bagnaia133a,133b, S. Bahinipati2,Y. Bai32a, D.C. Bailey159, T. Bain159, J.T. Baines130,O.K. Baker176, M.D. Baker24, S. Baker77,F. Baltasar Dos Santos Pedrosa29, E. Banas38,P. Banerjee94, Sw. Banerjee170, D. Banfi29,A. Bangert138, V. Bansal170, H.S. Bansil17, L. Barak172,S.P. Baranov95, A. Barashkou65, A. Barbaro Galtieri14,T. Barber27, E.L. Barberio87, D. Barberis50a,50b,M. Barbero20, D.Y. Bardin65, T. Barillari100,M. Barisonzi175, T. Barklow144, N. Barlow27,B.M. Barnett130, R.M. Barnett14, A. Baroncelli135a,A.J. Barr119, F. Barreiro81, J. Barreiro Guimaraes daCosta57, P. Barrillon116, R. Bartoldus144,A.E. Barton71, D. Bartsch20, R.L. Bates53,

L. Batkova145a, J.R. Batley27, A. Battaglia16,M. Battistin29, G. Battistoni90a, F. Bauer137,H.S. Bawa144, B. Beare159, T. Beau79,P.H. Beauchemin119, R. Beccherle50a, P. Bechtle41,H.P. Beck16, M. Beckingham48, K.H. Becks175,A.J. Beddall18c, A. Beddall18c, V.A. Bednyakov65,C. Bee84, M. Begel24, S. Behar Harpaz153,P.K. Behera63, M. Beimforde100,C. Belanger-Champagne167, P.J. Bell49, W.H. Bell49,G. Bella154, L. Bellagamba19a, F. Bellina29,G. Bellomo90a,90b, M. Bellomo120a, A. Belloni57,K. Belotskiy97, O. Beltramello29, S. Ben Ami153,O. Benary154, D. Benchekroun136a, C. Benchouk84,M. Bendel82, B.H. Benedict164, N. Benekos166,Y. Benhammou154, D.P. Benjamin44, M. Benoit116,J.R. Bensinger22, K. Benslama131, S. Bentvelsen106,D. Berge29, E. Bergeaas Kuutmann41, N. Berger4,F. Berghaus170, E. Berglund49, J. Beringer14,K. Bernardet84, P. Bernat77, R. Bernhard48,C. Bernius24, T. Berry76, A. Bertin19a,19b,F. Bertinelli29, F. Bertolucci123a,123b,M.I. Besana90a,90b, N. Besson137, S. Bethke100,W. Bhimji45, R.M. Bianchi29, M. Bianco72a,72b,O. Biebel99, S.P. Bieniek77, J. Biesiada14,M. Biglietti133a,133b, H. Bilokon47, M. Bindi19a,19b,A. Bingul18c, C. Bini133a,133b, C. Biscarat178,U. Bitenc48, K.M. Black21, R.E. Blair5,J.-B. Blanchard116, G. Blanchot29, C. Blocker22,J. Blocki38, A. Blondel49, W. Blum82,U. Blumenschein54, G.J. Bobbink106,V.B. Bobrovnikov108, A. Bocci44, C.R. Boddy119,M. Boehler41, J. Boek175, N. Boelaert35, S. Boser77,J.A. Bogaerts29, A. Bogdanchikov108, A. Bogouch91,∗,C. Bohm147a, V. Boisvert76, T. Bold164,e, V. Boldea25a,M. Bona75, V.G. Bondarenko97, M. Boonekamp137,G. Boorman76, C.N. Booth140, P. Booth140,S. Bordoni79, C. Borer16, A. Borisov129, G. Borissov71,I. Borjanovic12a, S. Borroni133a,133b, K. Bos106,D. Boscherini19a, M. Bosman11, H. Boterenbrood106,D. Botterill130, J. Bouchami94, J. Boudreau124,E.V. Bouhova-Thacker71, C. Boulahouache124,C. Bourdarios116, N. Bousson84, A. Boveia30, J. Boyd29,I.R. Boyko65, N.I. Bozhko129, I. Bozovic-Jelisavcic12b,J. Bracinik17, A. Braem29, E. Brambilla72a,72b,P. Branchini135a, G.W. Brandenburg57, A. Brandt7,G. Brandt15, O. Brandt54, U. Bratzler157, B. Brau85,J.E. Brau115, H.M. Braun175, B. Brelier159,J. Bremer29, R. Brenner167, S. Bressler153,D. Breton116, N.D. Brett119, P.G. Bright-Thomas17,D. Britton53, F.M. Brochu27, I. Brock20, R. Brock89,T.J. Brodbeck71, E. Brodet154, F. Broggi90a,C. Bromberg89, G. Brooijmans34, W.K. Brooks31b,G. Brown83, E. Brubaker30,P.A. Bruckman de Renstrom38, D. Bruncko145b,R. Bruneliere48, S. Brunet61, A. Bruni19a, G. Bruni19a,M. Bruschi19a, T. Buanes13, F. Bucci49, J. Buchanan119,

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N.J. Buchanan2, P. Buchholz142, R.M. Buckingham119,A.G. Buckley45, S.I. Buda25a, I.A. Budagov65,B. Budick109, V. Buscher82, L. Bugge118,D. Buira-Clark119, E.J. Buis106, O. Bulekov97,M. Bunse42, T. Buran118, H. Burckhart29, S. Burdin73,T. Burgess13, S. Burke130, E. Busato33, P. Bussey53,C.P. Buszello167, F. Butin29, B. Butler144,J.M. Butler21, C.M. Buttar53, J.M. Butterworth77,W. Buttinger27, T. Byatt77, S. Cabrera Urban168,M. Caccia90a,90b, D. Caforio19a,19b, O. Cakir3a,P. Calafiura14, G. Calderini79, P. Calfayan99,R. Calkins107, L.P. Caloba23a, R. Caloi133a,133b,D. Calvet33, S. Calvet33, R. Camacho Toro33,A. Camard79, P. Camarri134a,134b,M. Cambiaghi120a,120b, D. Cameron118, J. Cammin20,S. Campana29, M. Campanelli77, V. Canale103a,103b,F. Canelli30, A. Canepa160a, J. Cantero81,L. Capasso103a,103b, M.D.M. Capeans Garrido29,I. Caprini25a, M. Caprini25a, D. Capriotti100,M. Capua36a,36b, R. Caputo149, C. Caramarcu25a,R. Cardarelli134a, T. Carli29, G. Carlino103a,L. Carminati90a,90b, B. Caron160a, S. Caron48,C. Carpentieri48, G.D. Carrillo Montoya173,A.A. Carter75, J.R. Carter27, J. Carvalho125a,f ,D. Casadei109, M.P. Casado11, M. Cascella123a,123b,C. Caso50a,50b,∗, A.M. Castaneda Hernandez173,E. Castaneda-Miranda173, V. Castillo Gimenez168,N.F. Castro125b,a, G. Cataldi72a, F. Cataneo29,A. Catinaccio29, J.R. Catmore71, A. Cattai29,G. Cattani134a,134b, S. Caughron89, D. Cauz165a,165c,A. Cavallari133a,133b, P. Cavalleri79, D. Cavalli90a,M. Cavalli-Sforza11, V. Cavasinni123a,123b,A. Cazzato72a,72b, F. Ceradini135a,135b,A.S. Cerqueira23a, A. Cerri29, L. Cerrito75,F. Cerutti47, S.A. Cetin18b, F. Cevenini103a,103b,A. Chafaq136a, D. Chakraborty107, K. Chan2,B. Chapleau86, J.D. Chapman27, J.W. Chapman88,E. Chareyre79, D.G. Charlton17, V. Chavda83,S. Cheatham71, S. Chekanov5, S.V. Chekulaev160a,G.A. Chelkov65, H. Chen24, L. Chen2, S. Chen32c,T. Chen32c, X. Chen173, S. Cheng32a, A. Cheplakov65,V.F. Chepurnov65, R. Cherkaoui El Moursli136d,V. Chernyatin24, E. Cheu6, S.L. Cheung159,L. Chevalier137, F. Chevallier137, G. Chiefari103a,103b,L. Chikovani51, J.T. Childers58a, A. Chilingarov71,G. Chiodini72a, M.V. Chizhov65, G. Choudalakis30,S. Chouridou138, I.A. Christidi77, A. Christov48,D. Chromek-Burckhart29, M.L. Chu152, J. Chudoba126,G. Ciapetti133a,133b, K. Ciba37, A.K. Ciftci3a,R. Ciftci3a, D. Cinca33, V. Cindro74,M.D. Ciobotaru164, C. Ciocca19a,19b, A. Ciocio14,M. Cirilli88, M. Ciubancan25a, A. Clark49, P.J. Clark45,W. Cleland124, J.C. Clemens84, B. Clement55,C. Clement147a,147b, R.W. Clifft130, Y. Coadou84,M. Cobal165a,165c, A. Coccaro50a,50b, J. Cochran64,P. Coe119, J.G. Cogan144, J. Coggeshall166,

E. Cogneras178, C.D. Cojocaru28, J. Colas4,A.P. Colijn106, C. Collard116, N.J. Collins17,C. Collins-Tooth53, J. Collot55, G. Colon85,R. Coluccia72a,72b, G. Comune89, P. Conde Muino125a,E. Coniavitis119, M.C. Conidi11, M. Consonni105,V. Consorti48, S. Constantinescu25a, C. Conta120a,120b,F. Conventi103a,g, J. Cook29, M. Cooke14,B.D. Cooper77, A.M. Cooper-Sarkar119,N.J. Cooper-Smith76, K. Copic34, T. Cornelissen50a,50b,M. Corradi19a, F. Corriveau86,h, A. Cortes-Gonzalez166,G. Cortiana100, G. Costa90a, M.J. Costa168,D. Costanzo140, T. Costin30, D. Cote29,R. Coura Torres23a, L. Courneyea170, G. Cowan76,C. Cowden27, B.E. Cox83, K. Cranmer109,M. Cristinziani20, G. Crosetti36a,36b, R. Crupi72a,72b,S. Crepe-Renaudin55, C. Cuenca Almenar176,T. Cuhadar Donszelmann140, S. Cuneo50a,50b,M. Curatolo47, C.J. Curtis17, P. Cwetanski61,H. Czirr142, Z. Czyczula118, S. D’Auria53,M. D’Onofrio73, A. D’Orazio133a,133b,A. Da Rocha Gesualdi Mello23a, P.V.M. Da Silva23a,C. Da Via83, W. Dabrowski37, A. Dahlhoff48, T. Dai88,C. Dallapiccola85, S.J. Dallison130,∗, M. Dam35,M. Dameri50a,50b, D.S. Damiani138, H.O. Danielsson29,R. Dankers106, D. Dannheim100, V. Dao49, G. Darbo50a,G.L. Darlea25b, C. Daum106, J.P. Dauvergne 29,W. Davey87, T. Davidek127, N. Davidson87,R. Davidson71, M. Davies94, A.R. Davison77,E. Dawe143, I. Dawson140, J.W. Dawson5,∗,R.K. Daya39, K. De7, R. de Asmundis103a,S. De Castro19a,19b, P.E. De Castro Faria Salgado24,S. De Cecco79, J. de Graat99, N. De Groot105,P. de Jong106, C. De La Taille116, B. De Lotto165a,165c,L. De Mora71, L. De Nooij106, M. De Oliveira Branco29,D. De Pedis133a, P. de Saintignon55, A. De Salvo133a,U. De Sanctis165a,165c, A. De Santo150,J.B. De Vivie De Regie116, S. Dean77, D.V. Dedovich65,J. Degenhardt121, M. Dehchar119, M. Deile99,C. Del Papa165a,165c, J. Del Peso81,T. Del Prete123a,123b, A. Dell’Acqua29,L. Dell’Asta90a,90b, M. Della Pietra103a,g,D. della Volpe103a,103b, M. Delmastro29, P. Delpierre84,N. Delruelle29, P.A. Delsart55, C. Deluca149,S. Demers176, M. Demichev65, B. Demirkoz11,J. Deng164, S.P. Denisov129, D. Derendarz38,J.E. Derkaoui136c, F. Derue79, P. Dervan73, K. Desch20,E. Devetak149, P.O. Deviveiros159, A. Dewhurst130,B. DeWilde149, S. Dhaliwal159, R. Dhullipudi24,i,A. Di Ciaccio134a,134b, L. Di Ciaccio4, A. Di Girolamo29,B. Di Girolamo29, S. Di Luise135a,135b, A. Di Mattia89,B. Di Micco135a,135b, R. Di Nardo134a,134b,A. Di Simone134a,134b, R. Di Sipio19a,19b, M.A. Diaz31a,F. Diblen18c, E.B. Diehl88, H. Dietl100, J. Dietrich48,T.A. Dietzsch58a, S. Diglio116, K. Dindar Yagci39,J. Dingfelder20, C. Dionisi133a,133b, P. Dita25a,S. Dita25a, F. Dittus29, F. Djama84, R. Djilkibaev109,

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T. Djobava51, M.A.B. do Vale23a,A. Do Valle Wemans125a, T.K.O. Doan4, M. Dobbs86,R. Dobinson 29,∗, D. Dobos42, E. Dobson29,M. Dobson164, J. Dodd34, O.B. Dogan18a,∗,C. Doglioni119, T. Doherty53, Y. Doi66,∗, J. Dolejsi127,I. Dolenc74, Z. Dolezal127, B.A. Dolgoshein97,∗,T. Dohmae156, M. Donadelli23b, M. Donega121,J. Donini55, J. Dopke175, A. Doria103a, A. Dos Anjos173,M. Dosil11, A. Dotti123a,123b, M.T. Dova70,J.D. Dowell17, A.D. Doxiadis106, A.T. Doyle53,Z. Drasal127, J. Drees175, N. Dressnandt121,H. Drevermann29, C. Driouichi35, M. Dris9,J.G. Drohan77, J. Dubbert100, T. Dubbs138, S. Dube14,E. Duchovni172, G. Duckeck99, A. Dudarev29,F. Dudziak64, M. Duhrssen 29, I.P. Duerdoth83,L. Duflot116, M-A. Dufour86, M. Dunford29,H. Duran Yildiz3b, R. Duxfield140, M. Dwuznik37,F. Dydak 29, D. Dzahini55, M. Duren52,W.L. Ebenstein44, J. Ebke99, S. Eckert48,S. Eckweiler82, K. Edmonds82, C.A. Edwards76,I. Efthymiopoulos49, W. Ehrenfeld41, T. Ehrich100,T. Eifert29, G. Eigen13, K. Einsweiler14,E. Eisenhandler75, T. Ekelof167, M. El Kacimi4,M. Ellert167, S. Elles4, F. Ellinghaus82, K. Ellis75,N. Ellis29, J. Elmsheuser99, M. Elsing29, R. Ely14,D. Emeliyanov130, R. Engelmann149, A. Engl99,B. Epp62, A. Eppig88, J. Erdmann54, A. Ereditato16,D. Eriksson147a, J. Ernst1, M. Ernst24, J. Ernwein137,D. Errede166, S. Errede166, E. Ertel82, M. Escalier116,C. Escobar168, X. Espinal Curull11, B. Esposito47,F. Etienne84, A.I. Etienvre137, E. Etzion154,D. Evangelakou54, H. Evans61, L. Fabbri19a,19b,C. Fabre29, K. Facius35, R.M. Fakhrutdinov129,S. Falciano133a, A.C. Falou116, Y. Fang173,M. Fanti90a,90b, A. Farbin7, A. Farilla135a, J. Farley149,T. Farooque159, S.M. Farrington119, P. Farthouat29,D. Fasching173, P. Fassnacht29, D. Fassouliotis8,B. Fatholahzadeh159, A. Favareto90a,90b, L. Fayard116,S. Fazio36a,36b, R. Febbraro33, P. Federic145a,O.L. Fedin122, I. Fedorko29, W. Fedorko89,M. Fehling-Kaschek48, L. Feligioni84, D. Fellmann5,C.U. Felzmann87, C. Feng32d, E.J. Feng30,A.B. Fenyuk129, J. Ferencei145b, J. Ferland94,B. Fernandes125a,j , W. Fernando110, S. Ferrag53,J. Ferrando119, V. Ferrara41, A. Ferrari167, P. Ferrari106,R. Ferrari120a, A. Ferrer168, M.L. Ferrer47, D. Ferrere49,C. Ferretti88, A. Ferretto Parodi50a,50b, M. Fiascaris30,F. Fiedler82, A. Filipcic74, A. Filippas9, F. Filthaut105,M. Fincke-Keeler170, M.C.N. Fiolhais125a,f , L. Fiorini11,A. Firan39, G. Fischer41, P. Fischer 20, M.J. Fisher110,S.M. Fisher130, J. Flammer29, M. Flechl48, I. Fleck142,J. Fleckner82, P. Fleischmann174, S. Fleischmann175,T. Flick175, L.R. Flores Castillo173, M.J. Flowerdew100,F. Fohlisch58a, M. Fokitis9, T. Fonseca Martin16,D.A. Forbush139, A. Formica137, A. Forti83,D. Fortin160a, J.M. Foster83, D. Fournier116,

A. Foussat29, A.J. Fowler44, K. Fowler138, H. Fox71,P. Francavilla123a,123b, S. Franchino120a,120b,D. Francis29, T. Frank172, M. Franklin57, S. Franz29,M. Fraternali120a,120b, S. Fratina121, S.T. French27,R. Froeschl29, D. Froidevaux29, J.A. Frost27,C. Fukunaga157, E. Fullana Torregrosa29, J. Fuster168,C. Gabaldon29, O. Gabizon172, T. Gadfort24,S. Gadomski49, G. Gagliardi50a,50b, P. Gagnon61,C. Galea99, E.J. Gallas119, M.V. Gallas29, V. Gallo16,B.J. Gallop130, P. Gallus126, E. Galyaev40, K.K. Gan110,Y.S. Gao144,k, V.A. Gapienko129, A. Gaponenko14,F. Garberson176, M. Garcia-Sciveres14, C. Garcıa168,J.E. Garcıa Navarro49, R.W. Gardner30, N. Garelli29,H. Garitaonandia106, V. Garonne29, J. Garvey17,C. Gatti47, G. Gaudio120a, O. Gaumer49, B. Gaur142,L. Gauthier137, I.L. Gavrilenko95, C. Gay169,G. Gaycken20, J-C. Gayde29, E.N. Gazis9, P. Ge32d,C.N.P. Gee130, D.A.A. Geerts106, Ch. Geich-Gimbel20,K. Gellerstedt147a,147b, C. Gemme50a, A. Gemmell53,M.H. Genest99, S. Gentile133a,133b, S. George76,P. Gerlach175, A. Gershon154, C. Geweniger58a,H. Ghazlane136d, P. Ghez4, N. Ghodbane33,B. Giacobbe19a, S. Giagu133a,133b, V. Giakoumopoulou8,V. Giangiobbe123a,123b, F. Gianotti29, B. Gibbard24,A. Gibson159, S.M. Gibson29, G.F. Gieraltowski5,L.M. Gilbert119, M. Gilchriese14, V. Gilewsky92,D. Gillberg28, A.R. Gillman130, D.M. Gingrich2,d,J. Ginzburg154, N. Giokaris8, R. Giordano103a,103b,F.M. Giorgi15, P. Giovannini100, P.F. Giraud137,D. Giugni90a, P. Giusti19a, B.K. Gjelsten118,L.K. Gladilin98, C. Glasman81, J. Glatzer48,A. Glazov41, K.W. Glitza175, G.L. Glonti65,J. Godfrey143, J. Godlewski29, M. Goebel41,T. Gopfert43, C. Goeringer82, C. Gossling42,T. Gottfert100, S. Goldfarb88, D. Goldin39,T. Golling176, S.N. Golovnia129, A. Gomes125a,l,L.S. Gomez Fajardo41, R. Goncalo76, L. Gonella20,A. Gonidec29, S. Gonzalez173, S. Gonzalez de la Hoz168,M.L. Gonzalez Silva26, S. Gonzalez-Sevilla49,J.J. Goodson149, L. Goossens29, P.A. Gorbounov96,H.A. Gordon24, I. Gorelov104, G. Gorfine175,B. Gorini29, E. Gorini72a,72b, A. Gorisek74,E. Gornicki38, S.A. Gorokhov129, V.N. Goryachev129,B. Gosdzik41, M. Gosselink106, M.I. Gostkin65,M. Gouanere4, I. Gough Eschrich164, M. Gouighri136a,D. Goujdami136a, M.P. Goulette49, A.G. Goussiou139,C. Goy4, I. Grabowska-Bold164,e, V. Grabski177,P. Grafstrom29, C. Grah175, K-J. Grahn148,F. Grancagnolo72a, S. Grancagnolo15, V. Grassi149,V. Gratchev122, N. Grau34, H.M. Gray34,m,J.A. Gray149, E. Graziani135a, O.G. Grebenyuk122,D. Greenfield130, T. Greenshaw73, Z.D. Greenwood24,i,I.M. Gregor41, P. Grenier144, E. Griesmayer46,J. Griffiths139, N. Grigalashvili65, A.A. Grillo138,S. Grinstein11, P.L.Y. Gris33, Y.V. Grishkevich98,J.-F. Grivaz116, J. Grognuz29, M. Groh100, E. Gross172,

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J. Grosse-Knetter54, J. Groth-Jensen80, M. Gruwe29,K. Grybel142, V.J. Guarino5, D. Guest176,C. Guicheney33, A. Guida72a,72b, T. Guillemin4,S. Guindon54, H. Guler86,n, J. Gunther126, B. Guo159,J. Guo34, A. Gupta30, Y. Gusakov65, V.N. Gushchin129,A. Gutierrez94, P. Gutierrez112, N. Guttman154,O. Gutzwiller173, C. Guyot137, C. Gwenlan119,C.B. Gwilliam73, A. Haas144, S. Haas29, C. Haber14,R. Hackenburg24, H.K. Hadavand39, D.R. Hadley17,P. Haefner100, F. Hahn29, S. Haider29, Z. Hajduk38,H. Hakobyan177, J. Haller54, K. Hamacher175,P. Hamal114, A. Hamilton49, S. Hamilton162, H. Han32a,L. Han32b, K. Hanagaki117, M. Hance121, C. Handel82,P. Hanke58a, C.J. Hansen167, J.R. Hansen35,J.B. Hansen35, J.D. Hansen35, P.H. Hansen35,P. Hansson144, K. Hara161, G.A. Hare138,T. Harenberg175, D. Harper88, R.D. Harrington21,O.M. Harris139, K. Harrison17, J. Hartert48,F. Hartjes106, T. Haruyama66, A. Harvey56,S. Hasegawa102, Y. Hasegawa141, S. Hassani137,M. Hatch29, D. Hauff100, S. Haug16, M. Hauschild29,R. Hauser89, M. Havranek20, B.M. Hawes119,C.M. Hawkes17, R.J. Hawkings29, D. Hawkins164,T. Hayakawa67, D Hayden76, H.S. Hayward73,S.J. Haywood130, E. Hazen21, M. He32d, S.J. Head17,V. Hedberg80, L. Heelan28, S. Heim89, B. Heinemann14,S. Heisterkamp35, L. Helary4, M. Heldmann48,M. Heller116, S. Hellman147a,147b, C. Helsens11,R.C.W. Henderson71, M. Henke58a, A. Henrichs54,A.M. Henriques Correia29, S. Henrot-Versille116,F. Henry-Couannier84, C. Hensel54, T. Henß175,Y. Hernandez Jimenez168, R. Herrberg15,A.D. Hershenhorn153, G. Herten48, R. Hertenberger99,L. Hervas29, N.P. Hessey106, A. Hidvegi147a,E. Higon-Rodriguez168, D. Hill5,∗, J.C. Hill27, N. Hill5,K.H. Hiller41, S. Hillert20, S.J. Hillier17, I. Hinchliffe14,E. Hines121, M. Hirose117, F. Hirsch42,D. Hirschbuehl175, J. Hobbs149, N. Hod154,M.C. Hodgkinson140, P. Hodgson140, A. Hoecker29,M.R. Hoeferkamp104, J. Hoffman39, D. Hoffmann84,M. Hohlfeld82, M. Holder142, A. Holmes119,S.O. Holmgren147a, T. Holy128, J.L. Holzbauer89,Y. Homma67, L. Hooft van Huysduynen109,T. Horazdovsky128, C. Horn144, S. Horner48,K. Horton119, J-Y. Hostachy55, T. Hott100, S. Hou152,M.A. Houlden73, A. Hoummada136a, J. Howarth83,D.F. Howell119, I. Hristova 41, J. Hrivnac116,I. Hruska126, T. Hryn’ova4, P.J. Hsu176, S.-C. Hsu14,G.S. Huang112, Z. Hubacek128, F. Hubaut84,F. Huegging20, T.B. Huffman119, E.W. Hughes34,G. Hughes71, R.E. Hughes-Jones83, M. Huhtinen29,P. Hurst57, M. Hurwitz14, U. Husemann41,N. Huseynov65,o, J. Huston89, J. Huth57,G. Iacobucci103a, G. Iakovidis9, M. Ibbotson83,I. Ibragimov142, R. Ichimiya67,L. Iconomidou-Fayard116, J. Idarraga116, M. Idzik37,

P. Iengo4, O. Igonkina106, Y. Ikegami66, M. Ikeno66,Y. Ilchenko39, D. Iliadis155, D. Imbault79,M. Imhaeuser175, M. Imori156, T. Ince20,J. Inigo-Golfin29, P. Ioannou8, M. Iodice135a,G. Ionescu4, A. Irles Quiles168, K. Ishii66, A. Ishikawa67,M. Ishino66, R. Ishmukhametov39, T. Isobe156,C. Issever119, S. Istin18a, Y. Itoh102, A.V. Ivashin129,W. Iwanski38, H. Iwasaki66, J.M. Izen40, V. Izzo103a,B. Jackson121, J.N. Jackson73, P. Jackson144,M.R. Jaekel29, V. Jain61, K. Jakobs48, S. Jakobsen35,J. Jakubek128, D.K. Jana112, E. Jankowski159,E. Jansen77, A. Jantsch100, M. Janus20, G. Jarlskog80,L. Jeanty57, K. Jelen37, I. Jen-La Plante30, P. Jenni29,A. Jeremie4, P. Jez35, S. Jezequel4, H. Ji173, W. Ji82,J. Jia149, Y. Jiang32b, M. Jimenez Belenguer41,G. Jin32b, S. Jin32a, O. Jinnouchi158,M.D. Joergensen35, D. Joffe39, L.G. Johansen13,M. Johansen147a,147b, K.E. Johansson147a,P. Johansson140, S. Johnert41, K.A. Johns6,K. Jon-And147a,147b, G. Jones83, R.W.L. Jones71,T.W. Jones77, T.J. Jones73, O. Jonsson29, C. Joram29,P.M. Jorge125a,b, J. Joseph14, X. Ju131, V. Juranek126,P. Jussel62, V.V. Kabachenko129, S. Kabana16,M. Kaci168, A. Kaczmarska38, P. Kadlecik35,M. Kado116, H. Kagan110, M. Kagan57, S. Kaiser100,E. Kajomovitz153, S. Kalinin175, L.V. Kalinovskaya65,S. Kama39, N. Kanaya156, M. Kaneda156, T. Kanno158,V.A. Kantserov97, J. Kanzaki66, B. Kaplan176,A. Kapliy30, J. Kaplon29, D. Kar43, M. Karagoz119,M. Karnevskiy41, K. Karr5, V. Kartvelishvili71,A.N. Karyukhin129, L. Kashif173, A. Kasmi39,R.D. Kass110, A. Kastanas13, M. Kataoka4,Y. Kataoka156, E. Katsoufis9, J. Katzy41, V. Kaushik6,K. Kawagoe67, T. Kawamoto156, G. Kawamura82,M.S. Kayl106, V.A. Kazanin108, M.Y. Kazarinov65,S.I. Kazi87, J.R. Keates83, R. Keeler170, R. Kehoe39,M. Keil54, G.D. Kekelidze65, M. Kelly83, J. Kennedy99,M. Kenyon53, O. Kepka126, N. Kerschen29,B.P. Kersevan74, S. Kersten175, K. Kessoku156,C. Ketterer48, M. Khakzad28, F. Khalil-zada10,H. Khandanyan166, A. Khanov113, D. Kharchenko65,A. Khodinov149, A.G. Kholodenko129, A. Khomich58a,T.J. Khoo27, G. Khoriauli20, N. Khovanskiy65,V. Khovanskiy96, E. Khramov65, J. Khubua51,G. Kilvington76, H. Kim7, M.S. Kim2, P.C. Kim144,S.H. Kim161, N. Kimura171, O. Kind15, B.T. King73,M. King67, R.S.B. King119, J. Kirk130, G.P. Kirsch119,L.E. Kirsch22, A.E. Kiryunin100, D. Kisielewska37,T. Kittelmann124, A.M. Kiver129, H. Kiyamura67,E. Kladiva145b, J. Klaiber-Lodewigs42, M. Klein73,U. Klein73, K. Kleinknecht82, M. Klemetti86,A. Klier172, A. Klimentov24, R. Klingenberg42,E.B. Klinkby35, T. Klioutchnikova29, P.F. Klok105,S. Klous106, E.-E. Kluge58a, T. Kluge73, P. Kluit106,S. Kluth100, E. Kneringer62, J. Knobloch29,E.B.F.G. Knoops84, A. Knue54, B.R. Ko44,

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T. Kobayashi156, M. Kobel43, B. Koblitz29,M. Kocian144, A. Kocnar114, P. Kodys127, K. Koneke29,A.C. Konig105, S. Koenig82, S. Konig48, L. Kopke82,F. Koetsveld105, P. Koevesarki20, T. Koffas29,E. Koffeman106, F. Kohn54, Z. Kohout128, T. Kohriki66,T. Koi144, T. Kokott20, G.M. Kolachev108,H. Kolanoski15, V. Kolesnikov65, I. Koletsou90a,J. Koll89, D. Kollar29, M. Kollefrath48, S.D. Kolya83,A.A. Komar95, J.R. Komaragiri143, T. Kondo66,T. Kono41,p, A.I. Kononov48, R. Konoplich109,q,N. Konstantinidis77, A. Kootz175, S. Koperny37,S.V. Kopikov129, K. Korcyl38, K. Kordas155,V. Koreshev129, A. Korn14, A. Korol108, I. Korolkov11,E.V. Korolkova140, V.A. Korotkov129, O. Kortner100,S. Kortner100, V.V. Kostyukhin20, M.J. Kotamaki29,S. Kotov100, V.M. Kotov65, C. Kourkoumelis8,V. Kouskoura155, A. Koutsman106, R. Kowalewski170,T.Z. Kowalski37, W. Kozanecki137, A.S. Kozhin129,V. Kral128, V.A. Kramarenko98, G. Kramberger74,O. Krasel42, M.W. Krasny79, A. Krasznahorkay109,J. Kraus89, A. Kreisel154, F. Krejci128,J. Kretzschmar73, N. Krieger54, P. Krieger159,K. Kroeninger54, H. Kroha100, J. Kroll121,J. Kroseberg20, J. Krstic12a, U. Kruchonak65,H. Kruger20, Z.V. Krumshteyn65, A. Kruth20,T. Kubota156, S. Kuehn48, A. Kugel58c, T. Kuhl175,D. Kuhn62, V. Kukhtin65, Y. Kulchitsky91,S. Kuleshov31b, C. Kummer99, M. Kuna84,N. Kundu119, J. Kunkle121, A. Kupco126,H. Kurashige67, M. Kurata161, Y.A. Kurochkin91,V. Kus126, W. Kuykendall139, M. Kuze158, P. Kuzhir92,O. Kvasnicka126, R. Kwee15, A. La Rosa29,L. La Rotonda36a,36b, L. Labarga81, J. Labbe4,C. Lacasta168, F. Lacava133a,133b, H. Lacker15,D. Lacour79, V.R. Lacuesta168, E. Ladygin65,R. Lafaye4, B. Laforge79, T. Lagouri81, S. Lai48,E. Laisne55, M. Lamanna29, C.L. Lampen6, W. Lampl6,E. Lancon137, U. Landgraf48, M.P.J. Landon75,H. Landsman153, J.L. Lane83, C. Lange41,A.J. Lankford164, F. Lanni24, K. Lantzsch29,V.V. Lapin129,∗, S. Laplace79, C. Lapoire20,J.F. Laporte137, T. Lari90a, A.V. Larionov 129,A. Larner119, C. Lasseur29, M. Lassnig29, W. Lau119,P. Laurelli47, A. Lavorato119, W. Lavrijsen14,P. Laycock73, A.B. Lazarev65, A. Lazzaro90a,90b,O. Le Dortz79, E. Le Guirriec84, C. Le Maner159,E. Le Menedeu137, M. Leahu29, A. Lebedev64,C. Lebel94, T. LeCompte5, F. Ledroit-Guillon55,H. Lee106, J.S.H. Lee151, S.C. Lee152, L. Lee176,M. Lefebvre170, M. Legendre137, A. Leger49,B.C. LeGeyt121, F. Legger99, C. Leggett14,M. Lehmacher20, G. Lehmann Miotto29, X. Lei6,M.A.L. Leite23b, R. Leitner127, D. Lellouch172,J. Lellouch79, M. Leltchouk34, V. Lendermann58a,K.J.C. Leney146b, T. Lenz175, G. Lenzen175,B. Lenzi137, K. Leonhardt43, S. Leontsinis9, C. Leroy94,

J-R. Lessard170, J. Lesser147a, C.G. Lester27,A. Leung Fook Cheong173, J. Leveque84, D. Levin88,L.J. Levinson172, M.S. Levitski129, M. Lewandowska21,G.H. Lewis109, M. Leyton15, B. Li84, H. Li173, S. Li32b,X. Li88, Z. Liang39, Z. Liang119,r, B. Liberti134a,P. Lichard29, M. Lichtnecker99, K. Lie166, W. Liebig13,R. Lifshitz153, J.N. Lilley17, A. Limosani87,M. Limper63, S.C. Lin152,s, F. Linde106,J.T. Linnemann89, E. Lipeles121, L. Lipinsky126,A. Lipniacka13, T.M. Liss166, D. Lissauer24, A. Lister49,A.M. Litke138, C. Liu28, D. Liu152,t, H. Liu88,J.B. Liu88, M. Liu32b, S. Liu2, Y. Liu32b,M. Livan120a,120b, S.S.A. Livermore119, A. Lleres55,S.L. Lloyd75, E. Lobodzinska41, P. Loch6,W.S. Lockman138, S. Lockwitz176, T. Loddenkoetter20,F.K. Loebinger83, A. Loginov176, C.W. Loh169,T. Lohse15, K. Lohwasser48, M. Lokajicek126,J. Loken 119, V.P. Lombardo90a, R.E. Long71,L. Lopes125a,b, D. Lopez Mateos34,m, M. Losada163,P. Loscutoff14, F. Lo Sterzo133a,133b, M.J. Losty160a,X. Lou40, A. Lounis116, K.F. Loureiro163, J. Love21,P.A. Love71, A.J. Lowe144, F. Lu32a, J. Lu2, L. Lu39,H.J. Lubatti139, C. Luci133a,133b, A. Lucotte55,A. Ludwig43, D. Ludwig41, I. Ludwig48, J. Ludwig48,F. Luehring61, G. Luijckx106, D. Lumb48,L. Luminari133a, E. Lund118, B. Lund-Jensen148,B. Lundberg80, J. Lundberg147a,147b, J. Lundquist35,M. Lungwitz82, A. Lupi123a,123b, G. Lutz100, D. Lynn24,J. Lys14, E. Lytken80, H. Ma24, L.L. Ma173,J.A. Macana Goia94, G. Maccarrone47, A. Macchiolo100,B. Macek74, J. Machado Miguens125a, D. Macina49,R. Mackeprang35, R.J. Madaras14, W.F. Mader43,R. Maenner58c, T. Maeno24, P. Mattig175, S. Mattig41,P.J. Magalhaes Martins125a,f , L. Magnoni29,E. Magradze51, C.A. Magrath105, Y. Mahalalel154,K. Mahboubi48, G. Mahout17, C. Maiani133a,133b,C. Maidantchik23a, A. Maio125a,l, S. Majewski24,Y. Makida66, N. Makovec116, P. Mal6, Pa. Malecki38,P. Malecki38, V.P. Maleev122, F. Malek55, U. Mallik63,D. Malon5, S. Maltezos9, V. Malyshev108,S. Malyukov65, R. Mameghani99, J. Mamuzic12b,A. Manabe66, L. Mandelli90a, I. Mandic74,R. Mandrysch15, J. Maneira125a, P.S. Mangeard89,I.D. Manjavidze65, A. Mann54, P.M. Manning138,A. Manousakis-Katsikakis8, B. Mansoulie137,A. Manz100, A. Mapelli29, L. Mapelli29, L. March 81,J.F. Marchand29, F. Marchese134a,134b,M. Marchesotti29, G. Marchiori79, M. Marcisovsky126,A. Marin21,∗, C.P. Marino61, F. Marroquim23a,R. Marshall83, Z. Marshall34,m, F.K. Martens159,S. Marti-Garcia168, A.J. Martin176, B. Martin29,B. Martin89, F.F. Martin121, J.P. Martin94,Ph. Martin55, T.A. Martin17, B. Martin dit Latour49,M. Martinez11, V. Martinez Outschoorn57,A.C. Martyniuk83, M. Marx83, F. Marzano133a,A. Marzin112, L. Masetti82, T. Mashimo156,

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R. Mashinistov95, J. Masik83, A.L. Maslennikov108,M. Maß42, I. Massa19a,19b, G. Massaro106, N. Massol4,A. Mastroberardino36a,36b, T. Masubuchi156,M. Mathes20, P. Matricon116, H. Matsumoto156,H. Matsunaga156, T. Matsushita67, C. Mattravers119,u,J.M. Maugain29, S.J. Maxfield73, E.N. May5,A. Mayne140, R. Mazini152, M. Mazur20,M. Mazzanti90a, E. Mazzoni123a,123b, S.P. Mc Kee88,A. McCarn166, R.L. McCarthy149, T.G. McCarthy28,N.A. McCubbin130, K.W. McFarlane56,J.A. Mcfayden140, H. McGlone53, G. Mchedlidze51,R.A. McLaren29, T. Mclaughlan17, S.J. McMahon130,R.A. McPherson170,h, A. Meade85, J. Mechnich106,M. Mechtel175, M. Medinnis41, R. Meera-Lebbai112,T. Meguro117, R. Mehdiyev94, S. Mehlhase41,A. Mehta73, K. Meier58a, J. Meinhardt48, B. Meirose80,C. Melachrinos30, B.R. Mellado Garcia173,L. Mendoza Navas163, Z. Meng152,t,A. Mengarelli19a,19b, S. Menke100, C. Menot29,E. Meoni11, P. Mermod119, L. Merola103a,103b,C. Meroni90a, F.S. Merritt30, A. Messina29,J. Metcalfe104, A.S. Mete64, S. Meuser20, C. Meyer82,J-P. Meyer137, J. Meyer174, J. Meyer54, T.C. Meyer29,W.T. Meyer64, J. Miao32d, S. Michal29, L. Micu25a,R.P. Middleton130, P. Miele29, S. Migas73, L. Mijovic41,G. Mikenberg172, M. Mikestikova126, B. Mikulec49,M. Mikuz74, D.W. Miller144, R.J. Miller89,W.J. Mills169, C. Mills57, A. Milov172,D.A. Milstead147a,147b, D. Milstein172,A.A. Minaenko129, M. Minano168, I.A. Minashvili65,A.I. Mincer109, B. Mindur37, M. Mineev65, Y. Ming131,L.M. Mir11, G. Mirabelli133a, L. Miralles Verge11,A. Misiejuk76, J. Mitrevski138, G.Y. Mitrofanov129,V.A. Mitsou168, S. Mitsui66, P.S. Miyagawa83,K. Miyazaki67, J.U. Mjornmark80, T. Moa147a,147b,P. Mockett139, S. Moed57, V. Moeller27, K. Monig41,N. Moser20, S. Mohapatra149, B. Mohn13, W. Mohr48,S. Mohrdieck-Mock100, A.M. Moisseev129,∗,R. Moles-Valls168, J. Molina-Perez29, L. Moneta49,J. Monk77, E. Monnier84, S. Montesano90a,90b,F. Monticelli70, S. Monzani19a,19b, R.W. Moore2,G.F. Moorhead87, C. Mora Herrera49, A. Moraes53,A. Morais125a,b, N. Morange137, J. Morel54,G. Morello36a,36b, D. Moreno82, M. Moreno Llacer168,P. Morettini50a, M. Morii57, J. Morin75, Y. Morita66,A.K. Morley29, G. Mornacchi29, M-C. Morone49,S.V. Morozov97, J.D. Morris75, H.G. Moser100,M. Mosidze51, J. Moss110, R. Mount144,E. Mountricha9, S.V. Mouraviev95, E.J.W. Moyse85,M. Mudrinic12b, F. Mueller58a, J. Mueller124,K. Mueller20, T.A. Muller99, D. Muenstermann42,A. Muijs106, A. Muir169, Y. Munwes154,K. Murakami66, W.J. Murray130, I. Mussche106,E. Musto103a,103b, A.G. Myagkov129, M. Myska126,J. Nadal11, K. Nagai161, K. Nagano66, Y. Nagasaka60,A.M. Nairz29, Y. Nakahama116, K. Nakamura156,

I. Nakano111, G. Nanava20, A. Napier162, M. Nash77,u,N.R. Nation21, T. Nattermann20, T. Naumann41,G. Navarro163, H.A. Neal88, E. Nebot81,P.Yu. Nechaeva95, A. Negri120a,120b, G. Negri29,S. Nektarijevic49, A. Nelson64, S. Nelson144,T.K. Nelson144, S. Nemecek126, P. Nemethy109,A.A. Nepomuceno23a, M. Nessi29, S.Y. Nesterov122,M.S. Neubauer166, A. Neusiedl82, R.M. Neves109,P. Nevski24, P.R. Newman17, R.B. Nickerson119,R. Nicolaidou137, L. Nicolas140, B. Nicquevert29,F. Niedercorn116, J. Nielsen138, T. Niinikoski29,A. Nikiforov15, V. Nikolaenko129, K. Nikolaev65,I. Nikolic-Audit79, K. Nikolopoulos24, H. Nilsen48,P. Nilsson7, Y. Ninomiya 156, A. Nisati133a,T. Nishiyama67, R. Nisius100, L. Nodulman5,M. Nomachi117, I. Nomidis155, H. Nomoto156,M. Nordberg29, B. Nordkvist147a,147b, P.R. Norton130,J. Novakova127, M. Nozaki66, M. Nozicka41,I.M. Nugent160a, A.-E. Nuncio-Quiroz20,G. Nunes Hanninger20, T. Nunnemann99, E. Nurse77,T. Nyman29, B.J. O’Brien45, S.W. O’Neale17,∗,D.C. O’Neil143, V. O’Shea53, F.G. Oakham28,d,H. Oberlack100, J. Ocariz79, A. Ochi67, S. Oda156,S. Odaka66, J. Odier84, H. Ogren61, A. Oh83, S.H. Oh44,C.C. Ohm147a,147b, T. Ohshima102, H. Ohshita141,T.K. Ohska66, T. Ohsugi59, S. Okada67, H. Okawa164,Y. Okumura102, T. Okuyama156, M. Olcese50a,A.G. Olchevski65, M. Oliveira125a,f ,D. Oliveira Damazio24, E. Oliver Garcia168,D. Olivito121, A. Olszewski38, J. Olszowska38,C. Omachi67, A. Onofre125a,v, P.U.E. Onyisi30,C.J. Oram160a, G. Ordonez105, M.J. Oreglia30,F. Orellana49, Y. Oren154, D. Orestano135a,135b,I. Orlov108, C. Oropeza Barrera53, R.S. Orr159,E.O. Ortega131, B. Osculati50a,50b, R. Ospanov121,C. Osuna11, G. Otero y Garzon26, J.P Ottersbach106,M. Ouchrif136c, F. Ould-Saada118, A. Ouraou137,Q. Ouyang32a, M. Owen83, S. Owen140, A. Oyarzun31b,O.K. Øye13, V.E. Ozcan18a, N. Ozturk7,A. Pacheco Pages11, C. Padilla Aranda11,E. Paganis140, F. Paige24, K. Pajchel118, S. Palestini29,D. Pallin33, A. Palma125a,b, J.D. Palmer17, Y.B. Pan173,E. Panagiotopoulou9, B. Panes31a, N. Panikashvili88,S. Panitkin24, D. Pantea25a, M. Panuskova126,V. Paolone124, A. Paoloni134a,134b, A. Papadelis147a,Th.D. Papadopoulou9, A. Paramonov5, W. Park24,w,M.A. Parker27, F. Parodi50a,50b, J.A. Parsons34,U. Parzefall48, E. Pasqualucci133a, A. Passeri135a,F. Pastore135a,135b, Fr. Pastore29, G. Pasztor 49,x,S. Pataraia173, N. Patel151, J.R. Pater83,S. Patricelli103a,103b, T. Pauly29, M. Pecsy145a,M.I. Pedraza Morales173, S.V. Peleganchuk108,H. Peng173, R. Pengo29, A. Penson34, J. Penwell61,M. Perantoni23a, K. Perez34,m, T. Perez Cavalcanti41,E. Perez Codina11, M.T. Perez Garcıa-Estan168,V. Perez Reale34, I. Peric20, L. Perini90a,90b,

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H. Pernegger29, R. Perrino72a, P. Perrodo4,S. Persembe3a, V.D. Peshekhonov65, O. Peters106,B.A. Petersen29, J. Petersen29, T.C. Petersen35,E. Petit84, A. Petridis155, C. Petridou155,E. Petrolo133a, F. Petrucci135a,135b, D. Petschull41,M. Petteni143, R. Pezoa31b, A. Phan87, A.W. Phillips27,P.W. Phillips130, G. Piacquadio29, E. Piccaro75,M. Piccinini19a,19b, A. Pickford53, S.M. Piec41,R. Piegaia26, J.E. Pilcher30, A.D. Pilkington83,J. Pina125a,l, M. Pinamonti165a,165c, A. Pinder119,J.L. Pinfold2, J. Ping32c, B. Pinto125a,b, O. Pirotte29,C. Pizio90a,90b, R. Placakyte41, M. Plamondon170,W.G. Plano83, M.-A. Pleier24, A.V. Pleskach129,A. Poblaguev24, S. Poddar58a, F. Podlyski33,L. Poggioli116, T. Poghosyan20, M. Pohl49, F. Polci55,G. Polesello120a, A. Policicchio139, A. Polini19a,J. Poll75, V. Polychronakos24, D.M. Pomarede137,D. Pomeroy22, K. Pommes29, L. Pontecorvo133a,B.G. Pope89, G.A. Popeneciu25a, D.S. Popovic12a,A. Poppleton29, X. Portell Bueso48, R. Porter164,C. Posch21, G.E. Pospelov100, S. Pospisil128,I.N. Potrap100, C.J. Potter150, C.T. Potter86,G. Poulard29, J. Poveda173, R. Prabhu77,P. Pralavorio84, S. Prasad57, R. Pravahan7, S. Prell64,K. Pretzl16, L. Pribyl29, D. Price61, L.E. Price5,M.J. Price29, P.M. Prichard73, D. Prieur124,M. Primavera72a, K. Prokofiev109, F. Prokoshin31b,S. Protopopescu24, J. Proudfoot5, X. Prudent43,H. Przysiezniak4, S. Psoroulas20, E. Ptacek115,J. Purdham88, M. Purohit24,w, P. Puzo116,Y. Pylypchenko118, J. Qian88, Z. Qian84, Z. Qin41,A. Quadt54, D.R. Quarrie14, W.B. Quayle173,F. Quinonez31a, M. Raas105, V. Radescu58b,B. Radics20, T. Rador18a, F. Ragusa90a,90b,G. Rahal178, A.M. Rahimi110, D. Rahm24,S. Rajagopalan24, S. Rajek42, M. Rammensee48,M. Rammes142, M. Ramstedt147a,147b,K. Randrianarivony28, P.N. Ratoff71, F. Rauscher99,E. Rauter100, M. Raymond29, A.L. Read118,D.M. Rebuzzi120a,120b, A. Redelbach174, G. Redlinger24,R. Reece121, K. Reeves40, A. Reichold106,E. Reinherz-Aronis154, A. Reinsch115, I. Reisinger42,D. Reljic12a, C. Rembser29, Z.L. Ren152, A. Renaud116,P. Renkel39, B. Rensch35, M. Rescigno133a,S. Resconi90a, B. Resende137, P. Reznicek99,R. Rezvani159, A. Richards77, R. Richter100,E. Richter-Was38,y, M. Ridel79, S. Rieke82,M. Rijpstra106, M. Rijssenbeek149, A. Rimoldi120a,120b,L. Rinaldi19a, R.R. Rios39, I. Riu11, G. Rivoltella90a,90b,F. Rizatdinova113, E. Rizvi75, S.H. Robertson86,h,A. Robichaud-Veronneau49, D. Robinson27,J.E.M. Robinson77, M. Robinson115, A. Robson53,J.G. Rocha de Lima107, C. Roda123a,123b,D. Roda Dos Santos29, S. Rodier81, D. Rodriguez163,Y. Rodriguez Garcia15, A. Roe54, S. Roe29,O. Røhne118, V. Rojo1, S. Rolli162, A. Romaniouk97,

V.M. Romanov65, G. Romeo26, D. Romero Maltrana31a,L. Roos79, E. Ros168, S. Rosati139, M. Rose76,G.A. Rosenbaum159, E.I. Rosenberg64,P.L. Rosendahl13, L. Rosselet49, V. Rossetti11,E. Rossi103a,103b, L.P. Rossi50a, L. Rossi90a,90b,M. Rotaru25a, I. Roth172, J. Rothberg139,I. Rottlander20, D. Rousseau116, C.R. Royon137,A. Rozanov84, Y. Rozen153, X. Ruan116, I. Rubinskiy41,B. Ruckert99, N. Ruckstuhl106, V.I. Rud98,G. Rudolph62, F. Ruhr6, A. Ruiz-Martinez64,E. Rulikowska-Zarebska37, V. Rumiantsev92,∗,L. Rumyantsev65, K. Runge48, O. Runolfsson20,Z. Rurikova48, N.A. Rusakovich65, D.R. Rust61,J.P. Rutherfoord6, C. Ruwiedel14, P. Ruzicka126,Y.F. Ryabov122, V. Ryadovikov129, P. Ryan89,M. Rybar127, G. Rybkin116, N.C. Ryder119, S. Rzaeva10,A.F. Saavedra151, I. Sadeh154, H.F-W. Sadrozinski138,R. Sadykov65, F. Safai Tehrani133a,133b,H. Sakamoto156, G. Salamanna106, A. Salamon134a,M. Saleem112, D. Salihagic100, A. Salnikov144,J. Salt168, B.M. Salvachua Ferrando5,D. Salvatore36a,36b, F. Salvatore150, A. Salzburger29,D. Sampsonidis155, B.H. Samset118, H. Sandaker13,H.G. Sander82, M.P. Sanders99, M. Sandhoff175,P. Sandhu159, T. Sandoval27, R. Sandstroem106,S. Sandvoss175, D.P.C. Sankey130, A. Sansoni47,C. Santamarina Rios86, C. Santoni33,R. Santonico134a,134b, H. Santos125a, J.G. Saraiva125a,l,T. Sarangi173, E. Sarkisyan-Grinbaum7,F. Sarri123a,123b, G. Sartisohn175, O. Sasaki66,T. Sasaki66, N. Sasao68, I. Satsounkevitch91,G. Sauvage4, J.B. Sauvan116, P. Savard159,d,V. Savinov124, D.O. Savu29, P. Savva 9, L. Sawyer24,i,D.H. Saxon53, L.P. Says33, C. Sbarra19a,19b,A. Sbrizzi19a,19b, O. Scallon94, D.A. Scannicchio164,J. Schaarschmidt116, P. Schacht100, U. Schafer82,S. Schaetzel58b, A.C. Schaffer116, D. Schaile99,R.D. Schamberger149, A.G. Schamov108, V. Scharf58a,V.A. Schegelsky122, D. Scheirich88, M.I. Scherzer14,C. Schiavi50a,50b, J. Schieck99, M. Schioppa36a,36b,S. Schlenker29, J.L. Schlereth5, E. Schmidt48,M.P. Schmidt176,∗, K. Schmieden20, C. Schmitt82,M. Schmitz20, A. Schoning58b, M. Schott29,D. Schouten143, J. Schovancova126, M. Schram86,C. Schroeder82, N. Schroer58c, S. Schuh29, G. Schuler29,J. Schultes175, H.-C. Schultz-Coulon58a, H. Schulz15,J.W. Schumacher20, M. Schumacher48,B.A. Schumm138, Ph. Schune137, C. Schwanenberger83,A. Schwartzman144, Ph. Schwemling79,R. Schwienhorst89, R. Schwierz43, J. Schwindling137,W.G. Scott130, J. Searcy115, E. Sedykh122, E. Segura11,S.C. Seidel104, A. Seiden138, F. Seifert43, J.M. Seixas23a,G. Sekhniaidze103a, D.M. Seliverstov122, B. Sellden147a,G. Sellers73, M. Seman145b, N. Semprini-Cesari19a,19b,C. Serfon99, L. Serin116, R. Seuster100, H. Severini112,M.E. Sevior87, A. Sfyrla29, E. Shabalina54,

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M. Shamim115, L.Y. Shan32a, J.T. Shank21,Q.T. Shao87, M. Shapiro14, P.B. Shatalov96, L. Shaver6,C. Shaw53, K. Shaw165a,165c, D. Sherman176,P. Sherwood77, A. Shibata109, S. Shimizu29,M. Shimojima101, T. Shin56, A. Shmeleva95,M.J. Shochet30, D. Short119, M.A. Shupe6, P. Sicho126,A. Sidoti15, A. Siebel175, F. Siegert48, J. Siegrist14,Dj. Sijacki12a, O. Silbert172, J. Silva125a,z, Y. Silver154,D. Silverstein144, S.B. Silverstein147a, V. Simak128,O. Simard137, Lj. Simic12a, S. Simion116, B. Simmons77,M. Simonyan35, P. Sinervo159, N.B. Sinev115,V. Sipica142, G. Siragusa82, A.N. Sisakyan65,S.Yu. Sivoklokov98, J. Sjolin147a,147b, T.B. Sjursen13,L.A. Skinnari14, K. Skovpen108, P. Skubic112,N. Skvorodnev22, M. Slater17, T. Slavicek128,K. Sliwa162, T.J. Sloan71, J. Sloper29, V. Smakhtin172,S.Yu. Smirnov97, L.N. Smirnova98, O. Smirnova80,B.C. Smith57, D. Smith144, K.M. Smith53,M. Smizanska71, K. Smolek128, A.A. Snesarev95,S.W. Snow83, J. Snow112, J. Snuverink106, S. Snyder24,M. Soares125a, R. Sobie170,h, J. Sodomka128,A. Soffer154, C.A. Solans168, M. Solar128, J. Solc128,U. Soldevila168, E. Solfaroli Camillocci133a,133b,A.A. Solodkov129, O.V. Solovyanov129, J. Sondericker24,N. Soni2, V. Sopko128, B. Sopko128, M. Sorbi90a,90b,M. Sosebee7, A. Soukharev108, S. Spagnolo72a,72b,F. Spano34, R. Spighi19a, G. Spigo29, F. Spila133a,133b,E. Spiriti135a, R. Spiwoks29, M. Spousta127,T. Spreitzer159, B. Spurlock7, R.D. St. Denis53,T. Stahl142, J. Stahlman121, R. Stamen58a,E. Stanecka29, R.W. Stanek5, C. Stanescu135a,S. Stapnes118, E.A. Starchenko129, J. Stark55,P. Staroba126, P. Starovoitov92, A. Staude99,P. Stavina145a, G. Stavropoulos14, G. Steele53,P. Steinbach43, P. Steinberg24, I. Stekl128, B. Stelzer143,H.J. Stelzer41, O. Stelzer-Chilton160a, H. Stenzel52,K. Stevenson75, G.A. Stewart53, J.A. Stillings20,T. Stockmanns20, M.C. Stockton29, K. Stoerig48,G. Stoicea25a, S. Stonjek100, P. Strachota127,A.R. Stradling7, A. Straessner43, J. Strandberg88,S. Strandberg147a,147b, A. Strandlie118, M. Strang110,E. Strauss144, M. Strauss112, P. Strizenec145b,R. Strohmer174, D.M. Strom115, J.A. Strong76,∗,R. Stroynowski39, J. Strube130, B. Stugu13,I. Stumer24,∗, J. Stupak149, P. Sturm175, D.A. Soh152,r,D. Su144, S. Subramania2, Y. Sugaya117,T. Sugimoto102, C. Suhr107, K. Suita67, M. Suk127,V.V. Sulin95, S. Sultansoy3d, T. Sumida29, X. Sun55,J.E. Sundermann48, K. Suruliz165a,165b, S. Sushkov11,G. Susinno36a,36b, M.R. Sutton140, Y. Suzuki66,Yu.M. Sviridov129, S. Swedish169, I. Sykora145a,T. Sykora127, B. Szeless29, J. Sanchez168, D. Ta106,K. Tackmann29, A. Taffard164, R. Tafirout160a,A. Taga118, N. Taiblum154, Y. Takahashi102, H. Takai24,R. Takashima69, H. Takeda67, T. Takeshita141,M. Talby84, A. Talyshev108, M.C. Tamsett24,

J. Tanaka156, R. Tanaka116, S. Tanaka132, S. Tanaka66,Y. Tanaka101, K. Tani67, N. Tannoury84,G.P. Tappern29, S. Tapprogge82, D. Tardif159,S. Tarem153, F. Tarrade24, G.F. Tartarelli90a, P. Tas127,M. Tasevsky126, E. Tassi36a,36b, M. Tatarkhanov14,C. Taylor77, F.E. Taylor93, G.N. Taylor87,W. Taylor160b, M. Teixeira Dias Castanheira75,P. Teixeira-Dias76, K.K. Temming48, H. Ten Kate29,P.K. Teng152, Y.D. Tennenbaum-Katan153, S. Terada66,K. Terashi156, J. Terron81, M. Terwort41,p, M. Testa47,R.J. Teuscher159,h, C.M. Tevlin83, J. Thadome175,J. Therhaag20, T. Theveneaux-Pelzer79, M. Thioye176,S. Thoma48, J.P. Thomas17, E.N. Thompson85,P.D. Thompson17, P.D. Thompson159,A.S. Thompson53, E. Thomson121, M. Thomson27,R.P. Thun88, T. Tic126, V.O. Tikhomirov95,Y.A. Tikhonov108, C.J.W.P. Timmermans105,P. Tipton176, F.J. Tique Aires Viegas29, S. Tisserant84,J. Tobias48, B. Toczek37, T. Todorov4,S. Todorova-Nova162, B. Toggerson164, J. Tojo66,S. Tokar145a, K. Tokunaga67, K. Tokushuku66,K. Tollefson89, M. Tomoto102, L. Tompkins14,K. Toms104, A. Tonazzo135a,135b, G. Tong32a,A. Tonoyan13, C. Topfel16, N.D. Topilin65,I. Torchiani29, E. Torrence115, E. Torro Pastor168,J. Toth84,x, F. Touchard84, D.R. Tovey140,D. Traynor75, T. Trefzger174, J. Treis20, L. Tremblet29,A. Tricoli29, I.M. Trigger160a, S. Trincaz-Duvoid79,T.N. Trinh79, M.F. Tripiana70, N. Triplett64,W. Trischuk159, A. Trivedi24,w, B. Trocme55,C. Troncon90a, M. Trottier-McDonald143, A. Trzupek38,C. Tsarouchas29, J.C-L. Tseng119, M. Tsiakiris106,P.V. Tsiareshka91, D. Tsionou4, G. Tsipolitis9,V. Tsiskaridze48, E.G. Tskhadadze51, I.I. Tsukerman96,V. Tsulaia124, J.-W. Tsung20, S. Tsuno66,D. Tsybychev149, A. Tua140, J.M. Tuggle30,M. Turala38, D. Turecek128, I. Turk Cakir3e,E. Turlay106, P.M. Tuts34, A. Tykhonov74,M. Tylmad147a,147b, M. Tyndel130, D. Typaldos17,H. Tyrvainen29, G. Tzanakos8, K. Uchida20, I. Ueda156,R. Ueno28, M. Ugland13, M. Uhlenbrock20,M. Uhrmacher54, F. Ukegawa161, G. Unal29,D.G. Underwood5, A. Undrus24, G. Unel164, Y. Unno66,D. Urbaniec34, E. Urkovsky154, P. Urquijo49,P. Urrejola31a, G. Usai7, M. Uslenghi120a,120b,L. Vacavant84, V. Vacek128, B. Vachon86, S. Vahsen14,C. Valderanis100, J. Valenta126, P. Valente133a,S. Valentinetti19a,19b, S. Valkar127,E. Valladolid Gallego168, S. Vallecorsa153,J.A. Valls Ferrer168, H. van der Graaf106,E. van der Kraaij106, R. Van Der Leeuw106,E. van der Poel106, D. van der Ster29, B. Van Eijk106,N. van Eldik85, P. van Gemmeren5, Z. van Kesteren106,I. van Vulpen106, W. Vandelli29, G. Vandoni29,A. Vaniachine5, P. Vankov41, F. Vannucci79,F. Varela Rodriguez29, R. Vari133a, E.W. Varnes6,

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D. Varouchas14, A. Vartapetian7, K.E. Varvell151,V.I. Vassilakopoulos56, F. Vazeille33, G. Vegni90a,90b,J.J. Veillet116, C. Vellidis8, F. Veloso125a, R. Veness29,S. Veneziano133a, A. Ventura72a,72b, D. Ventura139,M. Venturi48, N. Venturi16, V. Vercesi120a,M. Verducci139, W. Verkerke106, J.C. Vermeulen106,A. Vest43, M.C. Vetterli143,d, I. Vichou166,T. Vickey146b,aa, G.H.A. Viehhauser119, S. Viel169,M. Villa19a,19b, M. Villaplana Perez168, E. Vilucchi47,M.G. Vincter28, E. Vinek29, V.B. Vinogradov65,M. Virchaux137,∗, S. Viret33, J. Virzi14,A. Vitale 19a,19b, O. Vitells172, M. Viti41, I. Vivarelli48,F. Vives Vaque11, S. Vlachos9, M. Vlasak128,N. Vlasov20, A. Vogel20, P. Vokac128, M. Volpi11,G. Volpini90a, H. von der Schmitt100, J. von Loeben100,H. von Radziewski48, E. von Toerne20, V. Vorobel127,A.P. Vorobiev129, V. Vorwerk11, M. Vos168, R. Voss29,T.T. Voss175, J.H. Vossebeld73, A.S. Vovenko129,N. Vranjes12a, M. Vranjes Milosavljevic12a, V. Vrba126,M. Vreeswijk106, T. Vu Anh82, R. Vuillermet29,I. Vukotic116, W. Wagner175, P. Wagner121,H. Wahlen175, J. Wakabayashi102, J. Walbersloh42,S. Walch88, J. Walder71, R. Walker99,W. Walkowiak142, R. Wall176, P. Waller73, C. Wang44,H. Wang173, J. Wang152, J. Wang32d, J.C. Wang139,R. Wang104, S.M. Wang152, A. Warburton86,C.P. Ward27, M. Warsinsky48, P.M. Watkins17,A.T. Watson17, M.F. Watson17, G. Watts139,S. Watts83, A.T. Waugh151, B.M. Waugh77, J. Weber42,M. Weber130, M.S. Weber16, P. Weber54,A.R. Weidberg119, J. Weingarten54, C. Weiser48,H. Wellenstein22, P.S. Wells29, M. Wen47, T. Wenaus24,S. Wendler124, Z. Weng152,r, T. Wengler29, S. Wenig29,N. Wermes20, M. Werner48, P. Werner29, M. Werth164,M. Wessels58a, K. Whalen28, S.J. Wheeler-Ellis164,S.P. Whitaker21, A. White7, M.J. White87, S. White24,S.R. Whitehead119, D. Whiteson164, D. Whittington61,F. Wicek116, D. Wicke175, F.J. Wickens130,W. Wiedenmann173, M. Wielers130, P. Wienemann20,C. Wiglesworth73, L.A.M. Wiik48, P.A. Wijeratne77,A. Wildauer168, M.A. Wildt41,p, I. Wilhelm127,H.G. Wilkens29, J.Z. Will99, E. Williams34,H.H. Williams121, W. Willis34, S. Willocq85,J.A. Wilson17, M.G. Wilson144, A. Wilson88,I. Wingerter-Seez4, S. Winkelmann48, F. Winklmeier29,M. Wittgen144, M.W. Wolter38, H. Wolters125a,f ,G. Wooden119, B.K. Wosiek38, J. Wotschack29,M.J. Woudstra85, K. Wraight53, C. Wright53,B. Wrona73, S.L. Wu173, X. Wu49, Y. Wu32b, E. Wulf34,R. Wunstorf42, B.M. Wynne45, L. Xaplanteris9,S. Xella35, S. Xie48, Y. Xie32a, C. Xu32b, D. Xu140,G. Xu32a, B. Yabsley151, M. Yamada66,A. Yamamoto66, K. Yamamoto64, S. Yamamoto156,T. Yamamura156, J. Yamaoka44, T. Yamazaki156,Y. Yamazaki67, Z. Yan21, H. Yang88, U.K. Yang83,Y. Yang61, Y. Yang32a, Z. Yang147a,147b, S. Yanush92,

W-M. Yao14, Y. Yao14, Y. Yasu66, J. Ye39, S. Ye24,M. Yilmaz3c, R. Yoosoofmiya124, K. Yorita171,R. Yoshida5, C. Young144, S. Youssef21, D. Yu24,J. Yu7, J. Yu32c,ab, L. Yuan32a,ac, A. Yurkewicz149,V.G. Zaets 129, R. Zaidan63, A.M. Zaitsev129,Z. Zajacova29, Yo.K. Zalite 122, L. Zanello133a,133b,P. Zarzhitsky39, A. Zaytsev108, C. Zeitnitz175,M. Zeller176, P.F. Zema29, A. Zemla38, C. Zendler20,A.V. Zenin129, O. Zenin129, T. Zenis145a,Z. Zenonos123a,123b, S. Zenz14, D. Zerwas116,G. Zevi della Porta57, Z. Zhan32d, D. Zhang32b,H. Zhang89, J. Zhang5, X. Zhang32d, Z. Zhang116,L. Zhao109, T. Zhao139, Z. Zhao32b, A. Zhemchugov65,S. Zheng32a, J. Zhong152,ad, B. Zhou88, N. Zhou164,Y. Zhou152, C.G. Zhu32d, H. Zhu41, Y. Zhu173,X. Zhuang99, V. Zhuravlov100, D. Zieminska61,B. Zilka145a, R. Zimmermann20, S. Zimmermann20,S. Zimmermann48, M. Ziolkowski142, R. Zitoun4,L. Zivkovic34, V.V. Zmouchko129,∗, G. Zobernig173,A. Zoccoli19a,19b, Y. Zolnierowski4, A. Zsenei29,M. zur Nedden15, V. Zutshi107, L. Zwalinski29.

1 University at Albany, 1400 Washington Ave, Albany,NY 12222, United States of America2 Department of Physics, University of Alberta,Edmonton AB, Canada3 Ankara University(a), Faculty of Sciences, Departmentof Physics, TR 061000 Tandogan, Ankara; DumlupinarUniversity(b), Faculty of Arts and Sciences, Departmentof Physics, Kutahya; Gazi University(c), Faculty of Artsand Sciences, Department of Physics, 06500,Teknikokullar, Ankara; TOBB University of Economicsand Technology(d), Faculty of Arts and Sciences,Division of Physics, 06560, Sogutozu, Ankara; TurkishAtomic Energy Authority(e), 06530, Lodumlu, Ankara,Turkey4 LAPP, CNRS/IN2P3 and Universite de Savoie,Annecy-le-Vieux, France5 Argonne National Laboratory, High Energy PhysicsDivision, 9700 S. Cass Avenue, Argonne IL 60439,United States of America6 University of Arizona, Department of Physics, Tucson,AZ 85721, United States of America7 The University of Texas at Arlington, Department ofPhysics, Box 19059, Arlington, TX 76019, United Statesof America8 University of Athens, Nuclear & Particle Physics,Department of Physics, Panepistimiopouli, Zografou,GR 15771 Athens, Greece9 National Technical University of Athens, PhysicsDepartment, 9-Iroon Polytechniou, GR 15780 Zografou,Greece10 Institute of Physics, Azerbaijan Academy of Sciences,H. Javid Avenue 33, AZ 143 Baku, Azerbaijan11 Institut de Fısica d’Altes Energies, IFAE, Edifici Cn,Universitat Autonoma de Barcelona, ES - 08193

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Bellaterra (Barcelona), Spain12 University of Belgrade(a), Institute of Physics, P.O.Box 57, 11001 Belgrade; Vinca Institute of NuclearSciences(b)M. Petrovica Alasa 12-14, 11000 Belgrade,Serbia, Serbia13 University of Bergen, Department for Physics andTechnology, Allegaten 55, NO - 5007 Bergen, Norway14 Lawrence Berkeley National Laboratory andUniversity of California, Physics Division, MS50B-6227,1 Cyclotron Road, Berkeley, CA 94720, United States ofAmerica15 Humboldt University, Institute of Physics, Berlin,Newtonstr. 15, D-12489 Berlin, Germany16 University of Bern, Albert Einstein Center forFundamental Physics, Laboratory for High EnergyPhysics, Sidlerstrasse 5, CH - 3012 Bern, Switzerland17 University of Birmingham, School of Physics andAstronomy, Edgbaston, Birmingham B15 2TT, UnitedKingdom18 Bogazici University(a), Faculty of Sciences,Department of Physics, TR - 80815 Bebek-Istanbul;Dogus University(b), Faculty of Arts and Sciences,Department of Physics, 34722, Kadikoy, Istanbul;(c)Gaziantep University, Faculty of Engineering,Department of Physics Engineering, 27310, Sehitkamil,Gaziantep, Turkey; Istanbul Technical University(d),Faculty of Arts and Sciences, Department of Physics,34469, Maslak, Istanbul, Turkey19 INFN Sezione di Bologna(a); Universita di Bologna,Dipartimento di Fisica(b), viale C. Berti Pichat, 6/2, IT- 40127 Bologna, Italy20 University of Bonn, Physikalisches Institut, Nussallee12, D - 53115 Bonn, Germany21 Boston University, Department of Physics, 590Commonwealth Avenue, Boston, MA 02215, UnitedStates of America22 Brandeis University, Department of Physics, MS057,415 South Street, Waltham, MA 02454, United Statesof America23 Universidade Federal do Rio De Janeiro,COPPE/EE/IF (a), Caixa Postal 68528, Ilha doFundao, BR - 21945-970 Rio de Janeiro; (b)Universidadede Sao Paulo, Instituto de Fisica, R.do Matao Trav.R.187, Sao Paulo - SP, 05508 - 900, Brazil24 Brookhaven National Laboratory, PhysicsDepartment, Bldg. 510A, Upton, NY 11973, UnitedStates of America25 National Institute of Physics and NuclearEngineering(a)Bucharest-Magurele, Str. Atomistilor407, P.O. Box MG-6, R-077125, Romania; UniversityPolitehnica Bucharest(b), Rectorat - AN 001, 313Splaiul Independentei, sector 6, 060042 Bucuresti; WestUniversity(c) in Timisoara, Bd. Vasile Parvan 4,Timisoara, Romania26 Universidad de Buenos Aires, FCEyN, Dto. Fisica,Pab I - C. Universitaria, 1428 Buenos Aires, Argentina

27 University of Cambridge, Cavendish Laboratory, J JThomson Avenue, Cambridge CB3 0HE, UnitedKingdom28 Carleton University, Department of Physics, 1125Colonel By Drive, Ottawa ON K1S 5B6, Canada29 CERN, CH - 1211 Geneva 23, Switzerland30 University of Chicago, Enrico Fermi Institute, 5640S. Ellis Avenue, Chicago, IL 60637, United States ofAmerica31 Pontificia Universidad Catolica de Chile, Facultad deFisica, Departamento de Fisica(a), Avda. VicunaMackenna 4860, San Joaquin, Santiago; UniversidadTecnica Federico Santa Marıa, Departamento deFısica(b), Avda. Espana 1680, Casilla 110-V, Valparaıso,Chile32 Institute of High Energy Physics, Chinese Academyof Sciences(a), P.O. Box 918, 19 Yuquan Road, ShijingShan District, CN - Beijing 100049; University ofScience & Technology of China (USTC), Department ofModern Physics(b), Hefei, CN - Anhui 230026; NanjingUniversity, Department of Physics(c), Nanjing, CN -Jiangsu 210093; Shandong University, High EnergyPhysics Group(d), Jinan, CN - Shandong 250100, China33 Laboratoire de Physique Corpusculaire, ClermontUniversite, Universite Blaise Pascal, CNRS/IN2P3, FR- 63177 Aubiere Cedex, France34 Columbia University, Nevis Laboratory, 136 So.Broadway, Irvington, NY 10533, United States ofAmerica35 University of Copenhagen, Niels Bohr Institute,Blegdamsvej 17, DK - 2100 Kobenhavn 0, Denmark36 INFN Gruppo Collegato di Cosenza(a); Universitadella Calabria, Dipartimento di Fisica(b), IT-87036Arcavacata di Rende, Italy37 Faculty of Physics and Applied Computer Science ofthe AGH-University of Science and Technology,(FPACS, AGH-UST), al. Mickiewicza 30, PL-30059Cracow, Poland38 The Henryk Niewodniczanski Institute of NuclearPhysics, Polish Academy of Sciences, ul.Radzikowskiego 152, PL - 31342 Krakow, Poland39 Southern Methodist University, Physics Department,106 Fondren Science Building, Dallas, TX 75275-0175,United States of America40 University of Texas at Dallas, 800 West CampbellRoad, Richardson, TX 75080-3021, United States ofAmerica41 DESY, Notkestr. 85, D-22603 Hamburg andPlatanenallee 6, D-15738 Zeuthen, Germany42 TU Dortmund, Experimentelle Physik IV, DE -44221 Dortmund, Germany43 Technical University Dresden, Institut fur Kern- undTeilchenphysik, Zellescher Weg 19, D-01069 Dresden,Germany44 Duke University, Department of Physics, Durham,NC 27708, United States of America

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45 University of Edinburgh, SUPA - School of Physicsand Astronomy, James Clerk Maxwell Building, TheKings Buildings, Mayfield Road, Edinburgh EH9 3JZ,United Kingdom46 Fachhochschule Wiener Neustadt; JohannesGutenbergstrasse 3 AT - 2700 Wiener Neustadt, Austria47 INFN Laboratori Nazionali di Frascati, via EnricoFermi 40, IT-00044 Frascati, Italy48 Albert-Ludwigs-Universitat, Fakultat furMathematik und Physik, Hermann-Herder Str. 3, D -79104 Freiburg i.Br., Germany49 Universite de Geneve, Section de Physique, 24 rueErnest Ansermet, CH - 1211 Geneve 4, Switzerland50 INFN Sezione di Genova(a); Universita di Genova,Dipartimento di Fisica(b), via Dodecaneso 33, IT -16146 Genova, Italy51 Institute of Physics of the Georgian Academy ofSciences, 6 Tamarashvili St., GE - 380077 Tbilisi;Tbilisi State University, HEP Institute, University St.9, GE - 380086 Tbilisi, Georgia52 Justus-Liebig-Universitat Giessen, II PhysikalischesInstitut, Heinrich-Buff Ring 16, D-35392 Giessen,Germany53 University of Glasgow, SUPA - School of Physics andAstronomy, Glasgow G12 8QQ, United Kingdom54 Georg-August-Universitat, II. Physikalisches Institut,Friedrich-Hund Platz 1, D-37077 Gottingen, Germany55 Laboratoire de Physique Subatomique et deCosmologie, Universite Joseph Fourier, CNRS-IN2P3,INPG, Grenoble, France, France56 Hampton University, Department of Physics,Hampton, VA 23668, United States of America57 Harvard University, Laboratory for Particle Physicsand Cosmology, 18 Hammond Street, Cambridge, MA02138, United States of America58 Ruprecht-Karls-Universitat Heidelberg:Kirchhoff-Institut fur Physik(a), Im Neuenheimer Feld227, D-69120 Heidelberg; Physikalisches Institut(b),Philosophenweg 12, D-69120 Heidelberg; ZITIRuprecht-Karls-University Heidelberg(c), Lehrstuhl furInformatik V, B6, 23-29, DE - 68131 Mannheim,Germany59 Hiroshima University, Faculty of Science, 1-3-1Kagamiyama, Higashihiroshima-shi, JP - Hiroshima739-8526, Japan60 Hiroshima Institute of Technology, Faculty ofApplied Information Science, 2-1-1 Miyake Saeki-ku,Hiroshima-shi, JP - Hiroshima 731-5193, Japan61 Indiana University, Department of Physics, SwainHall West 117, Bloomington, IN 47405-7105, UnitedStates of America62 Institut fur Astro- und Teilchenphysik,Technikerstrasse 25, A - 6020 Innsbruck, Austria63 University of Iowa, 203 Van Allen Hall, Iowa City, IA52242-1479, United States of America64 Iowa State University, Department of Physics and

Astronomy, Ames High Energy Physics Group, Ames,IA 50011-3160, United States of America65 Joint Institute for Nuclear Research, JINR Dubna,RU-141980 Moscow Region, Russia, Russia66 KEK, High Energy Accelerator ResearchOrganization, 1-1 Oho, Tsukuba-shi, Ibaraki-ken305-0801, Japan67 Kobe University, Graduate School of Science, 1-1Rokkodai-cho, Nada-ku, JP Kobe 657-8501, Japan68 Kyoto University, Faculty of Science, Oiwake-cho,Kitashirakawa, Sakyou-ku, Kyoto-shi, JP - Kyoto606-8502, Japan69 Kyoto University of Education, 1 Fukakusa, Fujimori,fushimi-ku, Kyoto-shi, JP - Kyoto 612-8522, Japan70 Universidad Nacional de La Plata, FCE,Departamento de Fısica, IFLP (CONICET-UNLP),C.C. 67, 1900 La Plata, Argentina71 Lancaster University, Physics Department, LancasterLA1 4YB, United Kingdom72 INFN Sezione di Lecce(a); Universita del Salento,Dipartimento di Fisica(b)Via Arnesano IT - 73100Lecce, Italy73 University of Liverpool, Oliver Lodge Laboratory,P.O. Box 147, Oxford Street, Liverpool L69 3BX,United Kingdom74 Jozef Stefan Institute and University of Ljubljana,Department of Physics, SI-1000 Ljubljana, Slovenia75 Queen Mary University of London, Department ofPhysics, Mile End Road, London E1 4NS, UnitedKingdom76 Royal Holloway, University of London, Departmentof Physics, Egham Hill, Egham, Surrey TW20 0EX,United Kingdom77 University College London, Department of Physicsand Astronomy, Gower Street, London WC1E 6BT,United Kingdom78 Louisville, United States of America79 Laboratoire de Physique Nucleaire et de HautesEnergies, UPMC, Universite Paris Diderot,CNRS/IN2P3, 4 place Jussieu, FR - 75252 Paris Cedex05, France80 Fysiska institutionen, Lunds universitet, Box 118, SE- 221 00 Lund, Sweden81 Universidad Autonoma de Madrid, Facultad deCiencias, Departamento de Fisica Teorica, ES - 28049Madrid, Spain82 Universitat Mainz, Institut fur Physik, StaudingerWeg 7, DE - 55099 Mainz, Germany83 University of Manchester, School of Physics andAstronomy, Manchester M13 9PL, United Kingdom84 CPPM, Aix-Marseille Universite, CNRS/IN2P3,Marseille, France85 University of Massachusetts, Department of Physics,710 North Pleasant Street, Amherst, MA 01003, UnitedStates of America86 McGill University, High Energy Physics Group, 3600

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University Street, Montreal, Quebec H3A 2T8, Canada87 University of Melbourne, School of Physics, AU -Parkville, Victoria 3010, Australia88 The University of Michigan, Department of Physics,2477 Randall Laboratory, 500 East University, AnnArbor, MI 48109-1120, United States of America89 Michigan State University, Department of Physicsand Astronomy, High Energy Physics Group, EastLansing, MI 48824-2320, United States of America90 INFN Sezione di Milano(a); Universita di Milano,Dipartimento di Fisica(b), via Celoria 16, IT - 20133Milano, Italy91 B.I. Stepanov Institute of Physics, National Academyof Sciences of Belarus, Independence Avenue 68, Minsk220072, Republic of Belarus92 National Scientific & Educational Centre for Particle& High Energy Physics, NC PHEP BSU, M.Bogdanovich St. 153, Minsk 220040, Republic ofBelarus93 Massachusetts Institute of Technology, Departmentof Physics, Room 24-516, Cambridge, MA 02139,United States of America94 University of Montreal, Group of Particle Physics,C.P. 6128, Succursale Centre-Ville, Montreal, Quebec,H3C 3J7 , Canada95 P.N. Lebedev Institute of Physics, Academy ofSciences, Leninsky pr. 53, RU - 117 924 Moscow, Russia96 Institute for Theoretical and Experimental Physics(ITEP), B. Cheremushkinskaya ul. 25, RU 117 218Moscow, Russia97 Moscow Engineering & Physics Institute (MEPhI),Kashirskoe Shosse 31, RU - 115409 Moscow, Russia98 Lomonosov Moscow State University SkobeltsynInstitute of Nuclear Physics (MSU SINP), 1(2),Leninskie gory, GSP-1, Moscow 119991 RussianFederation, Russia99 Ludwig-Maximilians-Universitat Munchen, Fakultatfur Physik, Am Coulombwall 1, DE - 85748 Garching,Germany100 Max-Planck-Institut fur Physik,(Werner-Heisenberg-Institut), Fohringer Ring 6, 80805Munchen, Germany101 Nagasaki Institute of Applied Science, 536Aba-machi, JP Nagasaki 851-0193, Japan102 Nagoya University, Graduate School of Science,Furo-Cho, Chikusa-ku, Nagoya, 464-8602, Japan103 INFN Sezione di Napoli(a); Universita di Napoli,Dipartimento di Scienze Fisiche(b), ComplessoUniversitario di Monte Sant’Angelo, via Cinthia, IT -80126 Napoli, Italy104 University of New Mexico, Department of Physicsand Astronomy, MSC07 4220, Albuquerque, NM 87131USA, United States of America105 Radboud University Nijmegen/NIKHEF,Department of Experimental High Energy Physics,Heyendaalseweg 135, NL-6525 AJ, Nijmegen,

Netherlands106 Nikhef National Institute for Subatomic Physics,and University of Amsterdam, Science Park 105, 1098XG Amsterdam, Netherlands107 Department of Physics, Northern Illinois University,LaTourette Hall Normal Road, DeKalb, IL 60115,United States of America108 Budker Institute of Nuclear Physics (BINP), RU -Novosibirsk 630 090, Russia109 New York University, Department of Physics, 4Washington Place, New York NY 10003, USA, UnitedStates of America110 Ohio State University, 191 West Woodruff Ave,Columbus, OH 43210-1117, United States of America111 Okayama University, Faculty of Science,Tsushimanaka 3-1-1, Okayama 700-8530, Japan112 University of Oklahoma, Homer L. DodgeDepartment of Physics and Astronomy, 440 WestBrooks, Room 100, Norman, OK 73019-0225, UnitedStates of America113 Oklahoma State University, Department of Physics,145 Physical Sciences Building, Stillwater, OK74078-3072, United States of America114 Palacky University, 17.listopadu 50a, 772 07Olomouc, Czech Republic115 University of Oregon, Center for High EnergyPhysics, Eugene, OR 97403-1274, United States ofAmerica116 LAL, Univ. Paris-Sud, IN2P3/CNRS, Orsay, France117 Osaka University, Graduate School of Science,Machikaneyama-machi 1-1, Toyonaka, Osaka 560-0043,Japan118 University of Oslo, Department of Physics, P.O. Box1048, Blindern, NO - 0316 Oslo 3, Norway119 Oxford University, Department of Physics, DenysWilkinson Building, Keble Road, Oxford OX1 3RH,United Kingdom120 INFN Sezione di Pavia(a); Universita di Pavia,Dipartimento di Fisica Nucleare e Teorica(b), Via Bassi6, IT-27100 Pavia, Italy121 University of Pennsylvania, Department of Physics,High Energy Physics Group, 209 S. 33rd Street,Philadelphia, PA 19104, United States of America122 Petersburg Nuclear Physics Institute, RU - 188 300Gatchina, Russia123 INFN Sezione di Pisa(a); Universita di Pisa,Dipartimento di Fisica E. Fermi(b), Largo B. Pontecorvo3, IT - 56127 Pisa, Italy124 University of Pittsburgh, Department of Physicsand Astronomy, 3941 O’Hara Street, Pittsburgh, PA15260, United States of America125 Laboratorio de Instrumentacao e FisicaExperimental de Particulas - LIP(a), Avenida EliasGarcia 14-1, PT - 1000-149 Lisboa, Portugal;Universidad de Granada, Departamento de FisicaTeorica y del Cosmos and CAFPE(b), E-18071 Granada,

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Spain126 Institute of Physics, Academy of Sciences of theCzech Republic, Na Slovance 2, CZ - 18221 Praha 8,Czech Republic127 Charles University in Prague, Faculty ofMathematics and Physics, Institute of Particle andNuclear Physics, V Holesovickach 2, CZ - 18000 Praha8, Czech Republic128 Czech Technical University in Prague, Zikova 4, CZ- 166 35 Praha 6, Czech Republic129 State Research Center Institute for High EnergyPhysics, Moscow Region, 142281, Protvino, Pobedastreet, 1, Russia130 Rutherford Appleton Laboratory, Science andTechnology Facilities Council, Harwell Science andInnovation Campus, Didcot OX11 0QX, UnitedKingdom131 University of Regina, Physics Department, Canada132 Ritsumeikan University, Noji Higashi 1 chome 1-1,JP - Kusatsu, Shiga 525-8577, Japan133 INFN Sezione di Roma I(a); Universita La Sapienza,Dipartimento di Fisica(b), Piazzale A. Moro 2, IT-00185 Roma, Italy134 INFN Sezione di Roma Tor Vergata(a); Universita diRoma Tor Vergata, Dipartimento di Fisica(b) , via dellaRicerca Scientifica, IT-00133 Roma, Italy135 INFN Sezione di Roma Tre(a); Universita Roma Tre,Dipartimento di Fisica(b), via della Vasca Navale 84,IT-00146 Roma, Italy136 Reseau Universitaire de Physique des HautesEnergies (RUPHE): Universite Hassan II, Faculte desSciences Ain Chock(a), B.P. 5366, MA - Casablanca;Centre National de l’Energie des Sciences TechniquesNucleaires (CNESTEN)(b), B.P. 1382 R.P. 10001 Rabat10001; Universite Mohamed Premier(c), LPTPM,Faculte des Sciences, B.P.717. Bd. Mohamed VI, 60000,Oujda ; Universite Mohammed V, Faculte desSciences(d)4 Avenue Ibn Battouta, BP 1014 RP, 10000Rabat, Morocco137 CEA, DSM/IRFU, Centre d’Etudes de Saclay, FR -91191 Gif-sur-Yvette, France138 University of California Santa Cruz, Santa CruzInstitute for Particle Physics (SCIPP), Santa Cruz, CA95064, United States of America139 University of Washington, Seattle, Department ofPhysics, Box 351560, Seattle, WA 98195-1560, UnitedStates of America140 University of Sheffield, Department of Physics &Astronomy, Hounsfield Road, Sheffield S3 7RH, UnitedKingdom141 Shinshu University, Department of Physics, Facultyof Science, 3-1-1 Asahi, Matsumoto-shi, JP - Nagano390-8621, Japan142 Universitat Siegen, Fachbereich Physik, D 57068Siegen, Germany143 Simon Fraser University, Department of Physics,

8888 University Drive, CA - Burnaby, BC V5A 1S6,Canada144 SLAC National Accelerator Laboratory, Stanford,California 94309, United States of America145 Comenius University, Faculty of Mathematics,Physics & Informatics(a), Mlynska dolina F2, SK -84248 Bratislava; Institute of Experimental Physics ofthe Slovak Academy of Sciences, Dept. of SubnuclearPhysics(b), Watsonova 47, SK - 04353 Kosice, SlovakRepublic146 (a)University of Johannesburg, Department ofPhysics, PO Box 524, Auckland Park, Johannesburg2006; (b)School of Physics, University of theWitwatersrand, Private Bag 3, Wits 2050,Johannesburg, South Africa, South Africa147 Stockholm University: Department of Physics(a);The Oskar Klein Centre(b), AlbaNova, SE - 106 91Stockholm, Sweden148 Royal Institute of Technology (KTH), PhysicsDepartment, SE - 106 91 Stockholm, Sweden149 Stony Brook University, Department of Physics andAstronomy, Nicolls Road, Stony Brook, NY 11794-3800,United States of America150 University of Sussex, Department of Physics andAstronomy Pevensey 2 Building, Falmer, Brighton BN19QH, United Kingdom151 University of Sydney, School of Physics, AU -Sydney NSW 2006, Australia152 Insitute of Physics, Academia Sinica, TW - Taipei11529, Taiwan153 Technion, Israel Inst. of Technology, Department ofPhysics, Technion City, IL - Haifa 32000, Israel154 Tel Aviv University, Raymond and Beverly SacklerSchool of Physics and Astronomy, Ramat Aviv, IL - TelAviv 69978, Israel155 Aristotle University of Thessaloniki, Faculty ofScience, Department of Physics, Division of Nuclear &Particle Physics, University Campus, GR - 54124,Thessaloniki, Greece156 The University of Tokyo, International Center forElementary Particle Physics and Department of Physics,7-3-1 Hongo, Bunkyo-ku, JP - Tokyo 113-0033, Japan157 Tokyo Metropolitan University, Graduate School ofScience and Technology, 1-1 Minami-Osawa, Hachioji,Tokyo 192-0397, Japan158 Tokyo Institute of Technology, Department ofPhysics, 2-12-1 O-Okayama, Meguro, Tokyo 152-8551,Japan159 University of Toronto, Department of Physics, 60Saint George Street, Toronto M5S 1A7, Ontario,Canada160 TRIUMF(a), 4004 Wesbrook Mall, Vancouver, B.C.V6T 2A3; (b)York University, Department of Physicsand Astronomy, 4700 Keele St., Toronto, Ontario, M3J1P3, Canada161 University of Tsukuba, Institute of Pure and

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Applied Sciences, 1-1-1 Tennoudai, Tsukuba-shi, JP -Ibaraki 305-8571, Japan162 Tufts University, Science & Technology Center, 4Colby Street, Medford, MA 02155, United States ofAmerica163 Universidad Antonio Narino, Centro deInvestigaciones, Cra 3 Este No.47A-15, Bogota,Colombia164 University of California, Irvine, Department ofPhysics & Astronomy, CA 92697-4575, United States ofAmerica165 INFN Gruppo Collegato di Udine(a); ICTP(b),Strada Costiera 11, IT-34014, Trieste; Universita diUdine, Dipartimento di Fisica(c), via delle Scienze 208,IT - 33100 Udine, Italy166 University of Illinois, Department of Physics, 1110West Green Street, Urbana, Illinois 61801, UnitedStates of America167 University of Uppsala, Department of Physics andAstronomy, P.O. Box 516, SE -751 20 Uppsala, Sweden168 Instituto de Fısica Corpuscular (IFIC) Centro MixtoUVEG-CSIC, Apdo. 22085 ES-46071 Valencia, Dept.Fısica At. Mol. y Nuclear; Dept. Ing. Electronica;Univ. of Valencia, and Inst. de Microelectronica deBarcelona (IMB-CNM-CSIC) 08193 Bellaterra, Spain169 University of British Columbia, Department ofPhysics, 6224 Agricultural Road, CA - Vancouver, B.C.V6T 1Z1, Canada170 University of Victoria, Department of Physics andAstronomy, P.O. Box 3055, Victoria B.C., V8W 3P6,Canada171 Waseda University, WISE, 3-4-1 Okubo,Shinjuku-ku, Tokyo, 169-8555, Japan172 The Weizmann Institute of Science, Department ofParticle Physics, P.O. Box 26, IL - 76100 Rehovot, Israel173 University of Wisconsin, Department of Physics,1150 University Avenue, WI 53706 Madison, Wisconsin,United States of America174 Julius-Maximilians-University of Wurzburg,Physikalisches Institute, Am Hubland, 97074 Wurzburg,Germany175 Bergische Universitat, Fachbereich C, Physik,Postfach 100127, Gauss-Strasse 20, D- 42097Wuppertal, Germany176 Yale University, Department of Physics, PO Box208121, New Haven CT, 06520-8121, United States ofAmerica177 Yerevan Physics Institute, Alikhanian BrothersStreet 2, AM - 375036 Yerevan, Armenia178 Centre de Calcul CNRS/IN2P3, Domainescientifique de la Doua, 27 bd du 11 Novembre 1918,69622 Villeurbanne Cedex, Francea Also at LIP, Portugalb Also at Faculdade de Ciencias, Universidade deLisboa, Lisboa, Portugalc Also at CPPM, Marseille, France.

d Also at TRIUMF, Vancouver, Canadae Also at FPACS, AGH-UST, Cracow, Polandf Also at Department of Physics, University ofCoimbra, Coimbra, Portugalg Also at Universita di Napoli Parthenope, Napoli, Italyh Also at Institute of Particle Physics (IPP), Canadai Also at Louisiana Tech University, Ruston, USAj Also at Universidade de Lisboa, Lisboa, Portugalk At California State University, Fresno, USAl Also at Faculdade de Ciencias, Universidade de Lisboaand at Centro de Fisica Nuclear da Universidade deLisboa, Lisboa, Portugalm Also at California Institute of Technology, Pasadena,USAn Also at University of Montreal, Montreal, Canadao Also at Baku Institute of Physics, Baku, Azerbaijanp Also at Institut fur Experimentalphysik, UniversitatHamburg, Hamburg, Germanyq Also at Manhattan College, New York, USAr Also at School of Physics and Engineering, SunYat-sen University, Guangzhou, Chinas Also at Taiwan Tier-1, ASGC, Academia Sinica,Taipei, Taiwant Also at School of Physics, Shandong University, Jinan,Chinau Also at Rutherford Appleton Laboratory, Didcot, UKv Also at Departamento de Fisica, Universidade deMinho, Braga, Portugalw Also at Department of Physics and Astronomy,University of South Carolina, Columbia, USAx Also at KFKI Research Institute for Particle andNuclear Physics, Budapest, Hungaryy Also at Institute of Physics, Jagiellonian University,Cracow, Polandz Also at Centro de Fisica Nuclear da Universidade deLisboa, Lisboa, Portugalaa Also at Department of Physics, Oxford University,Oxford, UKab Also at CEA, Gif sur Yvette, Franceac Also at LPNHE, Paris, Francead Also at Nanjing University, Nanjing Jiangsu, China∗ Deceased