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Search for pair production of a heavy up-type quark decaying to a w boson and a b quark in the lepton plus jets channel with the ATLAS Detector

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Search for Pair Production of a Heavy Up-Type Quark Decaying to a

W Boson and a b Quark

in the lepton

þ jets Channel with the ATLAS Detector

G. Aad et al.* (ATLAS Collaboration)

(Received 14 February 2012; published 26 June 2012)

A search is presented for production of a heavy up-type quark (t0) together with its antiparticle, assuming subsequent decay to a W boson and a b quark, t0t0! WþbWb. The search is based on 1:04 fb1of proton-proton collisions atpffiffiffis¼ 7 TeV collected by the ATLAS detector at the CERN Large

Hadron Collider. Data are analyzed in the leptonþ jets final state, characterized by a high transverse momentum isolated electron or muon, high missing transverse momentum, and at least three jets. No significant excess of events above the background expectation is observed. A 95% C.L. lower limit of 404 GeV is set for the mass of the t0 quark.

DOI:10.1103/PhysRevLett.108.261802 PACS numbers: 14.65.Jk, 12.60.i, 13.85.Rm, 14.80.j

The discovery of the top quark [1] completed the third generation of fundamental fermions in the quark sector of the standard model (SM) of particle physics. It is natural to ask whether heavier quarks may exist. These quarks are often present in new physics models aimed at solving the limitations of the SM. For example, models with a fourth generation of heavy chiral fermions could provide new sources of CP violation to explain the matter-antimatter asymmetry in the Universe and allow for a heavier Higgs boson while remaining consistent with precision electro-weak data [2]. The latter is accomplished by keeping a small mass splitting between the heavy up-type quark (t0) and the heavy down-type quark (b0). Assuming that mt0 

mb0< mW, where mW is the W boson mass, results in the t0

quark predominantly decaying to a W boson and a down-type quark q (q ¼ d; s; b). Another possibility is the addi-tion of isospin singlets or doublets of vectorlike quarks, which appear in many extensions of the SM such as little Higgs or extra-dimensional models [3]. In both scenarios, the t0quark can decay into Wb with a large branching ratio, provided there is a significant mixing with the third gen-eration of quarks, consistent with the existing mass and mixing patterns of the known quarks.

The high center-of-mass energy and integrated luminos-ity in pp collisions available at the Large Hadron Collider (LHC) offer a unique opportunity to probe these scenarios. At the LHC, these new heavy quarks would be predomi-nantly produced in pairs via the strong interaction for masses below 1 TeV, while for larger masses electro-weak production of single heavy quarks could become the primary production mechanism, depending on the strength

of their interactions with the SM quarks and weak gauge bosons [3].

A search is presented in this Letter for t0t0 production using pp collision data atpffiffiffis¼ 7 TeV collected with the ATLAS detector. It is assumed that the t0 quark decays exclusively into Wb. The lepton þ jets final-state signature is considered, characterized by a high transverse momen-tum (pT) isolated electron or muon, high missing

trans-verse momentum (EmissT ), and at least three jets. Similar searches in this channel have been published by the CDF and D0 Collaborations [4,5]; the most stringent limits preclude the existence of a t0 quark with a mass below 358 GeV at 95% confidence level (C.L.). A search for t0t0in the dilepton final state has been performed by the ATLAS Collaboration [6], excluding a t0 quark with a mass below 350 GeV at 95% C.L. The leptonþ jets signature has also been recently exploited by the ATLAS Collaboration to search for b0b0 ! WtWþt [7].

The ATLAS detector [8] consists of an inner tracking system surrounded by a superconducting solenoid, electro-magnetic and hadronic calorimeters, and a muon spec-trometer. The inner detector is immersed in a 2 T axial magnetic field and consists of pixel and silicon microstrip detectors inside a transition radiation tracker, providing charged particle tracking in the region jj < 2:5 [9]. The electromagnetic calorimeter is based on lead–liquid-argon (LAr). Hadron calorimetry is based on two different detec-tor technologies, with scintilladetec-tor tiles or LAr as active media and with either steel, copper, or tungsten as the absorber material. The calorimeters provide coverage up to jj < 4:9. The muon spectrometer consists of super-conducting air-core toroids, a system of trigger chambers covering the rangejj < 2:4, and high-precision tracking chambers allowing muon momentum measurements withinjj < 2:7.

The data set used in this analysis was recorded between March and June 2011 by using single electron and muon triggers and includes only events collected under stable

*Full author list given at the end of the article.

Published by the American Physical Society under the terms of the Creative Commons Attribution 3.0 License. Further distri-bution of this work must maintain attridistri-bution to the author(s) and the published article’s title, journal citation, and DOI.

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beam conditions and for which all detector subsystems were fully operational. The corresponding integrated lumi-nosity is 1:04 fb1. The event selection criteria closely follow those used in recent ATLAS top quark studies, e.g., Ref. [10]. Electron candidates are required to satisfy pT> 25 GeV and jj < 2:47, excluding the transition

region 1:37 < jj < 1:52 between the barrel and end cap electromagnetic calorimeters. Muon candidates are re-quired to satisfy pT> 20 GeV and jj < 2:5. The pT

threshold requirement ensures that the selected leptons are in the efficiency plateau of the single-lepton triggers. Background from multijet production is suppressed by a requirement of EmissT > 35ð20Þ GeV [11] in the electron

(muon) channel, followed by EmissT þ mT > 60 GeV,

where mT is the transverse mass of the lepton and EmissT

[12]. The EmissT is constructed from the vector sum of all

calorimeter cells contained in topological clusters [13], calibrated at the energy scale of the associated high-pT

object, and including contributions from selected muons. Further requirements are that there be at least three jets with pT> 25 GeV and jj < 2:5, with at least one jet

satisfying pT > 60 GeV. Jets are reconstructed with the

anti-ktalgorithm [14] with radius parameter R ¼ 0:4, from

topological clusters of energy deposits in the calorimeters calibrated at the electromagnetic scale. These jets are then calibrated to the particle level [15] by using a pT- and

-dependent correction factor derived from simulated events and validated by using data. Finally, to further reduce the backgrounds, at least one jet is required to be identified as originating from the hadronization of a b quark (b tagging). This is achieved via an algorithm [16] using multivariate techniques to combine information from the impact parameters of displaced tracks as well as topo-logical properties of secondary and tertiary decay vertices reconstructed within the jet; a working point is used with 70% efficiency for b-quark jets and a rejection factor of 100 for jets originating from light quarks (u, d, s) or gluons. Events with exactly one electron or one muon and with exactly three jets or with four or more jets are ana-lyzed separately to take advantage of their different

signal-to-background ratio and background composition, as discussed below.

After event selection, the main background is tt produc-tion, followed by the production of a W boson in association with jets (W þ jets). Smaller contributions arise from mul-tijet events, single top quark, Z þ jets, and diboson produc-tion. All of the backgrounds which do not involve top quarks are significantly suppressed by the b-tagging re-quirement. Multijet events contribute to the selected sample via the misidentification of a jet or a photon as an electron or the presence of a nonprompt lepton, e.g., from a semilep-tonic b- or c-hadron decay. The normalization and shape of the multijet background kinematic distributions are esti-mated via data-driven methods [11]. For the W þ jets back-ground, the shape is estimated from the simulation, but the normalization is estimated from the asymmetry between Wþþ jets and Wþ jets production [17] in the data. All other backgrounds, as well as the signal, are estimated from the simulation and normalized to their theoretical cross sections. A summary of the background estimates in each of the four channels analyzed and a comparison with the observed yields in data are presented in TableI, showing a good agreement within the uncertainties.

Monte Carlo (MC) samples of tt and single top quark background are generated by using MC@NLO v3.41 [18], assuming a top quark mass of 172.5 GeV, using theCTEQ6.6

set of parton distribution functions (PDFs) [19], and are normalized to the approximate next-to-next-to-leading-order (NNLO) theoretical cross sections [20,21]. Samples of W=Z þ jets background are generated by usingALPGEN V2.13 [22] and the CTEQ6L1 PDF set [19]. The Z þ jets background is normalized to the NNLO theoretical cross section [23], while the W þ jets background normalization is extracted from the data. BothMC@NLOandALPGENare

interfaced toHERWIGv6.5 [24] to model the parton shower

and fragmentation, while JIMMY [25] is used to simulate

the underlying event. The diboson backgrounds are mod-eled by using HERWIGv6.5 and normalized to their NLO

theoretical cross sections [26]. The signal is modeled by usingPYTHIA6.421 [27]. Signal samples are generated for TABLE I. Number of events observed compared to the background expectation after final

event selection in each of the four channels considered. Also shown are the expected signal yields assuming mt0 ¼ 400 GeV. The quoted uncertainties are prior to the fit to data and include

both statistical and systematic contributions, taking into account correlations among processes. e þ 3 jets  þ 3 jets eþ  4 jets þ  4 jets

tt 2320  460 3000  630 4470  920 5900  1200 W þ jets 1440  790 2200  1200 830  580 1160  790 Z þ jets 92  53 118  62 86  56 83  46 Single top 382  68 554  94 262  70 325  79 Dibosons 28  7 37  11 12  5 17  5 Multijet 520  520 550  550 320  320 340  340 Total prediction 4800  1000 6500  1500 6000  1100 7800  1400 Data 4533 6421 6145 8149 t0t0ð400 GeVÞ 20:0  3:3 21:0  3:6 102:0  10:5 98:1  11:1

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a range of masses mt0 from 250 to 500 GeV in steps of

50 GeV and are normalized to the approximate NNLO theoretical cross sections [20] using the CTEQ6.6 PDF. The MC samples generated by using HERWIG or PYTHIA

use the MRST2007 LO* PDF set [28]. All MC samples

include multiple pp interactions and are processed through a full simulation [29] of the detector geometry and re-sponse using GEANT4 [30] and the same reconstruction software as the data. Simulated events are corrected to match the object identification efficiencies and resolutions determined in data control samples. The total signal detection efficiency, considering both lepton flavors and jet multiplicities analyzed, ranges from 5.2% for mt0 ¼

250 GeV to 17.3% for mt0 ¼ 500 GeV.

This analysis uses the reconstructed heavy quark mass (mreco) as the primary discriminating variable. In the case

of events with 4 jets, mrecois estimated by performing a

kinematic likelihood fit [17] to the t0t0! WþbWb ! ‘bq q0b hypothesis, imposing the constraints that t0 and t0 have the same mass and that the mass of the

lepton-neutrino system, as well as that of a jet pair, equals the nominal W boson mass. The final-state objects considered are the lepton, EmissT , and the four jets with highest pT.

Among all possible jet-parton permutations, the one yield-ing the highest likelihood value after maximization over the fit parameters is kept. In the case of events with exactly three jets, mreco is taken to be the invariant mass of the

three-jet system. In order to ensure a robust background prediction in the tail of the mreco distribution, a dynamic

binning scheme is adopted; starting from the high side and low side of the distributions, bins are merged until the statistical uncertainty in the sum of the background pre-dictions in that bin drops below 5%.

Systematic uncertainties affecting the normalization and shape of the mrecodistribution are estimated for both signal

and background, taking into account correlations among processes as well as channels. The dominant sources of uncertainty arise from the modeling of the tt background. The uncertainties on the tt background come from the theoretical uncertainty on the cross section (þ7:09:6%) as well as the effects on both normalization and shape of the mrecodistribution from a number of sources; these are

uncertainties on the fragmentation model (based on the comparison ofHERWIGandPYTHIAfragmentations), on the NLO event generator (based on the comparison of

MC@NLO and POWHEG [31]), and on the top quark mass

(taken to be1 GeV).

The uncertainty on the jet energy scale affects the nor-malization of signal (2%–12%) and backgrounds (5%– 30%) modeled through the simulation, as well as the shape of their mrecodistributions.

Uncertainties on the modeling of initial- and final-state QCD radiation, evaluated by varying corresponding generator parameters, are considered as correlated between the tt background and the t0t0 signal.

While the normalization is obtained from the asymmetry measurement, the uncertainties on the normalization of the W þ jets background are derived from measurements of W þ 2 jets dominated data samples and take into account the uncertainty on the heavy-flavor content of the samples as well as the extrapolation to higher jet multiplicities. The total uncertainty on the W þ jets normalization is 50% and 70% for events with exactly 3 jets and  4 jets, respec-tively. Uncertainties on the shape of the mreco distribution

for the W þ jets background are estimated by varying the choices of the matching scale (from 15 to 10 GeV) and the factorization scale (from 2F ¼ m2W þ

P

p2T;jet to 2F ¼

m2Wþ p2T;W) inALPGEN.

Uncertainties on the modeling of the b-tagging algo-rithms affect the identification of b=c jets (6%–8% for signal and backgrounds containing top quarks and 6%–12% for the other backgrounds) as well as the mis-identification of light jets (< 0:5% for signal and back-grounds containing top quarks and up to 5% for the other backgrounds). The Z þ jets, single top, and diboson back-grounds are varied within the uncertainty on their theoreti-cal cross sections. The uncertainty on the multijet background event normalizations is conservatively taken as 100%. Uncertainties on the shapes of the multijet back-ground are derived by varying the lepton identification criteria used to extract this background.

The uncertainties on the lepton identification and trigger efficiencies, as well as their energy scales and resolutions, impact the yields by 3% for electrons and 6% for muons.

Uncertainties on the integrated luminosity (3.7%) [32], jet reconstruction efficiency, jet resolution modeling, effect of multiple pp interactions on the modeling of the EmissT ,

and treatment of imperfections in the detector description in the MC simulation are also considered and are all found to have a very small effect on the result.

Good agreement between the data and the background prediction is observed in terms of both overall normaliza-tion and shape of the mrecodistribution. The mreco

distribu-tion is analyzed by using a log-likelihood ratio LLR ¼ 2 logðLsþb=LbÞ as a test statistic, where Lsþb

(Lb) is a Poisson likelihood to observe the data under the

signal-plus-background (background-only) hypothesis. The per-bin signal and background predictions are parame-terized in terms of 12 nuisance parameters, describing the effect of leading sources of systematic uncertainty such as jet energy scale, initial- and final-state QCD radiation, and tt, W þ jets, and QCD multijet normalizations. The impact of systematic uncertainties on the sensitivity of the search is reduced by maximizing both likelihood functions, Lsþb and Lb, with respect to these nuisance parameters,

subject to Gaussian constraints of their prior values. The set of fitted nuisance parameters is chosen based on their over-all impact on the search sensitivity, the expected constrain-ing power of the data, and their suitability to be treated as continuous parameters. The simultaneous constraint of

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several of these systematic uncertainties is possible because of the inclusion of the 3-jet channel in the analysis. The latter has a higher fraction of W þ jets background than the  4-jets channel and provides sensitivity to event migration to different jet multiplicities when varying uncertainties such as jet energy scale or initial- and final-state QCD radiation. In addition to the jet multiplicity spectrum, the jet energy scale affects the peak position of the mreco

spec-trum for tt background and can be constrained owing to the small uncertainty on the measured top quark mass [33]. Nuisance parameters associated with smaller systematic

uncertainties (e.g., lepton identification or trigger) are only weakly constrained.

Figure1shows a comparison of the postfit mreco

distri-bution between the data and the background prediction for the combined e= þ 3 jets and e=þ  4 jets channels. The fitted parameters are typically within 1 standard de-viation of their nominal values, and their uncertainties are consistent with expectations based on pseudoexperiments. Several additional studies were performed to check the integrity of the fitting procedure. The likelihood was veri-fied to be parabolic near the minimum for each of the fitted parameters and to yield reasonable fit uncertainties; the lack of sensitivity to the assumed pT and  correlation of

the jet energy scale uncertainty was verified.

In the absence of any significant data excess, either in the e þ jets or  þ jets channels individually or in their combination, 95% C.L. upper limits on the t0t0production cross section are derived by using the CLS method [34],

which employs the LLR test statistic described above. Pseudoexperiments are generated under both the signal-plus-background (s þ b) and background-only (b) hypoth-eses, taking into account per-bin statistical fluctuations of the total predictions according to Poisson statistics, as well as Gaussian fluctuations in the signal and background expectations describing the effect of systematic uncertain-ties. The fraction of s þ b and b pseudoexperiments with LLR larger than the median or observed LLR defines CLsþb and CLb for the expected or observed limits,

re-spectively. Signal cross sections for which CLs¼

CLsþb=CLb< 0:05 are deemed excluded at the 95% C.L.

The resulting observed and expected upper limits on the t0t0 production cross section are shown in Fig. 2 as a function of the t0 mass, compared to the theoretical prediction, assuming a BRðt0! WbÞ ¼ 1. As a result, an

100 200 300 400 500 0 [1/GeV] reco dN/dm 10 20 30 40 50 60 e/µ+3 jets Data ’ (400 GeV) t t’ t t W+jets Z+jets Single top Dibosons Multijets -1 L dt = 1.04 fb

= 7 TeV s ATLAS [GeV] reco m 100 200 300 400 500 600 Data-Bkg -50 0 (a) (b) 50 Evts/bin 200 250 300 350 400 450 500 0 [1/GeV] reco dN/dm 20 40 60 80 100 120 140 160 e/µ+≥4 jets Data ’ (400 GeV) t t’ t t W+jets Z+jets Single top Dibosons Multijets -1 L dt = 1.04 fb

= 7 TeV s ATLAS [GeV] reco m 100 150 200 250 300 350 400 450 500 550 Data-Bkg -50 0 50 Evts/bin

FIG. 1 (color online). mreco distribution in the combined

(a) e= þ 3 jets and (b) e=þ  4 jets channels. The data (points) are compared to the SM background predictions using the values of the nuisance parameters obtained from the fit to data under the background-only hypothesis (stacked histo-grams). In the top panels, the bin contents have been divided by bin width. The bottom panels show the background-subtracted data distribution. The underflow and overflow have been folded into the first and last bins, respectively. Also shown is the expected contribution from a signal with mass mt0 ¼

400 GeV (histogram). t’ mass [GeV] 250 300 350 400 450 500 ’ ) [pb]t t’ → (ppσ -1 10 1 10 → -1 Ldt = 1.04 fb

= 7 TeV s CDF excluded 1 s.d. ± Approx. NNLO pred. 95% C.L. observed limit 95% C.L. expected limit 1 s.d. ± Expected limit 2 s.d. ± Expected limit ATLAS

FIG. 2 (color online). Observed (solid line) and expected (dashed line) 95% C.L. upper limits on the t0t0cross section as a function of the t0mass. The surrounding shaded bands corre-spond to the 1 and 2 standard deviations (s.d.) around the expected limit. The thin line shows the theoretical prediction including its 1 s.d. uncertainty band. The shaded area is the mass region previously excluded by the CDF experiment [4].

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observed (expected) 95% C.L. lower limit of 404 (394) GeV on the mass of the t0 quark is derived.

In summary, a search for t0t0 production has been per-formed in the leptonþ jets final state under the assumption BRðt0! WbÞ ¼ 1. No significant excess of events in the tail of the mreco distribution was found, resulting in an

observed lower limit of mt0> 404 GeV at 95% C.L. This

represents the most stringent limit to date. This limit is also directly applicable to a down-type vectorlike quark with electric charge of4=3 decaying into a W boson and a b quark [3].

We thank CERN for the very successful operation of the LHC, as well as the support staff from our institutions without whom ATLAS could not be operated efficiently. We acknowledge the support of ANPCyT, Argentina; YerPhI, Armenia; ARC, Australia; BMWF, Austria; ANAS, Azerbaijan; SSTC, Belarus; CNPq and FAPESP, Brazil; NSERC, NRC, and CFI, Canada; CERN; CONICYT, Chile; CAS, MOST, and NSFC, China; COLCIENCIAS, Colombia; MSMT CR, MPO CR, and VSC CR, Czech Republic; DNRF, DNSRC, and Lundbeck Foundation, Denmark; ARTEMIS and ERC, European Union; IN2P3-CNRS, CEA-DSM/IRFU, France; GNAS, Georgia; BMBF, DFG, HGF, MPG, and AvH Foundation, Germany; GSRT, Greece; ISF, MINERVA, GIF, DIP, and Benoziyo Center, Israel; INFN, Italy; MEXT and JSPS, Japan; CNRST, Morocco; FOM and NWO, The Netherlands; RCN, Norway; MNiSW, Poland; GRICES and FCT, Portugal; MERYS (MECTS), Romania; MES of Russia and ROSATOM, Russian Federation; JINR; MSTD, Serbia; MSSR, Slovakia; ARRS and MVZT, Slovenia; DST/NRF, South Africa; MICINN, Spain; SRC and Wallenberg Foundation, Sweden; SER, SNSF, and Cantons of Bern and Geneva, Switzerland; NSC, Taiwan; TAEK, Turkey; STFC, the Royal Society, and Leverhulme Trust, United Kingdom; DOE and NSF, United States of America. The crucial computing support from all WLCG partners is acknowledged gratefully, in particular, from CERN and the ATLAS Tier-1 facilities at TRIUMF (Canada), NDGF (Denmark, Norway, Sweden), CC-IN2P3 (France), KIT/GridKA (Germany), INFN-CNAF (Italy), NL-T1 (The Netherlands), PIC (Spain), ASGC (Taiwan), RAL (United Kingdom), and BNL (USA) and in the Tier-2 facilities worldwide.

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I. Aracena,142Y. Arai,65A. T. H. Arce,44S. Arfaoui,147J-F. Arguin,14E. Arik,18a,aM. Arik,18aA. J. Armbruster,86 O. Arnaez,80C. Arnault,114A. Artamonov,94G. Artoni,131a,131bD. Arutinov,20S. Asai,154R. Asfandiyarov,171

S. Ask,27B. A˚ sman,145a,145bL. Asquith,5K. Assamagan,24A. Astbury,168A. Astvatsatourov,51B. Aubert,4 E. Auge,114K. Augsten,126M. Aurousseau,144aG. Avolio,162R. Avramidou,9D. Axen,167C. Ay,53G. Azuelos,92,e

Y. Azuma,154M. A. Baak,29G. Baccaglioni,88aC. Bacci,133a,133bA. M. Bach,14H. Bachacou,135K. Bachas,29 M. Backes,48M. Backhaus,20E. Badescu,25aP. Bagnaia,131a,131bS. Bahinipati,2Y. Bai,32aD. C. Bailey,157T. Bain,157

J. T. Baines,128O. K. Baker,174M. D. Baker,24S. Baker,76E. Banas,38P. Banerjee,92Sw. Banerjee,171D. Banfi,29 A. Bangert,149V. Bansal,168H. S. Bansil,17L. Barak,170S. P. Baranov,93A. Barashkou,64A. Barbaro Galtieri,14

T. Barber,47E. L. Barberio,85D. Barberis,49a,49bM. Barbero,20D. Y. Bardin,64T. Barillari,98M. Barisonzi,173 T. Barklow,142N. Barlow,27B. M. Barnett,128R. M. Barnett,14A. Baroncelli,133aG. Barone,48A. J. Barr,117 F. Barreiro,79J. Barreiro Guimara˜es da Costa,56P. Barrillon,114R. Bartoldus,142A. E. Barton,70V. Bartsch,148 R. L. Bates,52L. Batkova,143aJ. R. Batley,27A. Battaglia,16M. Battistin,29F. Bauer,135H. S. Bawa,142,fS. Beale,97

T. Beau,77P. H. Beauchemin,160R. Beccherle,49aP. Bechtle,20H. P. Beck,16S. Becker,97M. Beckingham,137 K. H. Becks,173A. J. Beddall,18cA. Beddall,18cS. Bedikian,174V. A. Bednyakov,64C. P. Bee,82M. Begel,24

S. Behar Harpaz,151P. K. Behera,62M. Beimforde,98C. Belanger-Champagne,84P. J. Bell,48W. H. Bell,48 G. Bella,152L. Bellagamba,19aF. Bellina,29M. Bellomo,29A. Belloni,56O. Beloborodova,106,gK. Belotskiy,95 O. Beltramello,29S. Ben Ami,151O. Benary,152D. Benchekroun,134aC. Benchouk,82M. Bendel,80N. Benekos,164 Y. Benhammou,152E. Benhar Noccioli,48J. A. Benitez Garcia,158bD. P. Benjamin,44M. Benoit,114J. R. Bensinger,22 K. Benslama,129S. Bentvelsen,104D. Berge,29E. Bergeaas Kuutmann,41N. Berger,4F. Berghaus,168E. Berglund,104 J. Beringer,14P. Bernat,76R. Bernhard,47C. Bernius,24T. Berry,75C. Bertella,82A. Bertin,19a,19bF. Bertinelli,29 F. Bertolucci,121a,121bM. I. Besana,88a,88bN. Besson,135S. Bethke,98W. Bhimji,45R. M. Bianchi,29M. Bianco,71a,71b

O. Biebel,97S. P. Bieniek,76K. Bierwagen,53J. Biesiada,14M. Biglietti,133aH. Bilokon,46M. Bindi,19a,19b S. Binet,114A. Bingul,18cC. Bini,131a,131bC. Biscarat,176U. Bitenc,47K. M. Black,21R. E. Blair,5J.-B. Blanchard,135

G. Blanchot,29T. Blazek,143aC. Blocker,22J. Blocki,38A. Blondel,48W. Blum,80U. Blumenschein,53 G. J. Bobbink,104V. B. Bobrovnikov,106S. S. Bocchetta,78A. Bocci,44C. R. Boddy,117M. Boehler,41J. Boek,173

N. Boelaert,35J. A. Bogaerts,29A. Bogdanchikov,106A. Bogouch,89,aC. Bohm,145aV. Boisvert,75T. Bold,37 V. Boldea,25aN. M. Bolnet,135M. Bona,74V. G. Bondarenko,95M. Bondioli,162M. Boonekamp,135C. N. Booth,138

S. Bordoni,77C. Borer,16A. Borisov,127G. Borissov,70I. Borjanovic,12aM. Borri,81S. Borroni,86

V. Bortolotto,133a,133bK. Bos,104D. Boscherini,19aM. Bosman,11H. Boterenbrood,104D. Botterill,128J. Bouchami,92 J. Boudreau,122E. V. Bouhova-Thacker,70D. Boumediene,33C. Bourdarios,114N. Bousson,82A. Boveia,30J. Boyd,29

I. R. Boyko,64N. I. Bozhko,127I. Bozovic-Jelisavcic,12bJ. Bracinik,17A. Braem,29P. Branchini,133a G. W. Brandenburg,56A. Brandt,7G. Brandt,117O. Brandt,53U. Bratzler,155B. Brau,83J. E. Brau,113H. M. Braun,173

B. Brelier,157J. Bremer,29R. Brenner,165S. Bressler,170D. Britton,52F. M. Brochu,27I. Brock,20R. Brock,87 T. J. Brodbeck,70E. Brodet,152F. Broggi,88aC. Bromberg,87J. Bronner,98G. Brooijmans,34W. K. Brooks,31b

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G. Brown,81H. Brown,7P. A. Bruckman de Renstrom,38D. Bruncko,143bR. Bruneliere,47S. Brunet,60A. Bruni,19a G. Bruni,19aM. Bruschi,19aT. Buanes,13Q. Buat,54F. Bucci,48J. Buchanan,117N. J. Buchanan,2P. Buchholz,140

R. M. Buckingham,117A. G. Buckley,45S. I. Buda,25aI. A. Budagov,64B. Budick,107V. Bu¨scher,80L. Bugge,116 O. Bulekov,95M. Bunse,42T. Buran,116H. Burckhart,29S. Burdin,72T. Burgess,13S. Burke,128E. Busato,33

P. Bussey,52C. P. Buszello,165F. Butin,29B. Butler,142J. M. Butler,21C. M. Buttar,52J. M. Butterworth,76 W. Buttinger,27S. Cabrera Urba´n,166D. Caforio,19a,19bO. Cakir,3aP. Calafiura,14G. Calderini,77P. Calfayan,97 R. Calkins,105L. P. Caloba,23aR. Caloi,131a,131bD. Calvet,33S. Calvet,33R. Camacho Toro,33P. Camarri,132a,132b

M. Cambiaghi,118a,118bD. Cameron,116L. M. Caminada,14S. Campana,29M. Campanelli,76V. Canale,101a,101b F. Canelli,30,hA. Canepa,158aJ. Cantero,79L. Capasso,101a,101bM. D. M. Capeans Garrido,29I. Caprini,25a M. Caprini,25aD. Capriotti,98M. Capua,36a,36bR. Caputo,80C. Caramarcu,24R. Cardarelli,132aT. Carli,29 G. Carlino,101aL. Carminati,88a,88bB. Caron,84S. Caron,103G. D. Carrillo Montoya,171A. A. Carter,74J. R. Carter,27

J. Carvalho,123a,iD. Casadei,107M. P. Casado,11M. Cascella,121a,121bC. Caso,49a,49b,a

A. M. Castaneda Hernandez,171E. Castaneda-Miranda,171V. Castillo Gimenez,166N. F. Castro,123aG. Cataldi,71a F. Cataneo,29A. Catinaccio,29J. R. Catmore,29A. Cattai,29G. Cattani,132a,132bS. Caughron,87D. Cauz,163a,163c

P. Cavalleri,77D. Cavalli,88aM. Cavalli-Sforza,11V. Cavasinni,121a,121bF. Ceradini,133a,133bA. S. Cerqueira,23b A. Cerri,29L. Cerrito,74F. Cerutti,46S. A. Cetin,18bF. Cevenini,101a,101bA. Chafaq,134aD. Chakraborty,105K. Chan,2

B. Chapleau,84J. D. Chapman,27J. W. Chapman,86E. Chareyre,77D. G. Charlton,17V. Chavda,81

C. A. Chavez Barajas,29S. Cheatham,84S. Chekanov,5S. V. Chekulaev,158aG. A. Chelkov,64M. A. Chelstowska,103 C. Chen,63H. Chen,24S. Chen,32cT. Chen,32cX. Chen,171S. Cheng,32aA. Cheplakov,64V. F. Chepurnov,64 R. Cherkaoui El Moursli,134eV. Chernyatin,24E. Cheu,6S. L. Cheung,157L. Chevalier,135G. Chiefari,101a,101b

L. Chikovani,50aJ. T. Childers,29A. Chilingarov,70G. Chiodini,71aA. S. Chisholm,17M. V. Chizhov,64 G. Choudalakis,30S. Chouridou,136I. A. Christidi,76A. Christov,47D. Chromek-Burckhart,29M. L. Chu,150 J. Chudoba,124G. Ciapetti,131a,131bK. Ciba,37A. K. Ciftci,3aR. Ciftci,3aD. Cinca,33V. Cindro,73M. D. Ciobotaru,162

C. Ciocca,19aA. Ciocio,14M. Cirilli,86M. Citterio,88aM. Ciubancan,25aA. Clark,48P. J. Clark,45W. Cleland,122 J. C. Clemens,82B. Clement,54C. Clement,145a,145bR. W. Clifft,128Y. Coadou,82M. Cobal,163a,163cA. Coccaro,171 J. Cochran,63P. Coe,117J. G. Cogan,142J. Coggeshall,164E. Cogneras,176J. Colas,4A. P. Colijn,104N. J. Collins,17 C. Collins-Tooth,52J. Collot,54G. Colon,83P. Conde Muin˜o,123aE. Coniavitis,117M. C. Conidi,11M. Consonni,103 V. Consorti,47S. Constantinescu,25aC. Conta,118a,118bF. Conventi,101a,jJ. Cook,29M. Cooke,14B. D. Cooper,76 A. M. Cooper-Sarkar,117K. Copic,14T. Cornelissen,173M. Corradi,19aF. Corriveau,84,kA. Cortes-Gonzalez,164

G. Cortiana,98G. Costa,88aM. J. Costa,166D. Costanzo,138T. Costin,30D. Coˆte´,29R. Coura Torres,23a L. Courneyea,168G. Cowan,75C. Cowden,27B. E. Cox,81K. Cranmer,107F. Crescioli,121a,121bM. Cristinziani,20

G. Crosetti,36a,36bR. Crupi,71a,71bS. Cre´pe´-Renaudin,54C.-M. Cuciuc,25aC. Cuenca Almenar,174 T. Cuhadar Donszelmann,138M. Curatolo,46C. J. Curtis,17C. Cuthbert,149P. Cwetanski,60H. Czirr,140 P. Czodrowski,43Z. Czyczula,174S. D’Auria,52M. D’Onofrio,72A. D’Orazio,131a,131bP. V. M. Da Silva,23a

C. Da Via,81W. Dabrowski,37T. Dai,86C. Dallapiccola,83M. Dam,35M. Dameri,49a,49bD. S. Damiani,136 H. O. Danielsson,29D. Dannheim,98V. Dao,48G. Darbo,49aG. L. Darlea,25bW. Davey,20T. Davidek,125 N. Davidson,85R. Davidson,70E. Davies,117,dM. Davies,92A. R. Davison,76Y. Davygora,57aE. Dawe,141 I. Dawson,138J. W. Dawson,5,aR. K. Daya-Ishmukhametova,22K. De,7R. de Asmundis,101aS. De Castro,19a,19b P. E. De Castro Faria Salgado,24S. De Cecco,77J. de Graat,97N. De Groot,103P. de Jong,104C. De La Taille,114

H. De la Torre,79B. De Lotto,163a,163cL. de Mora,70L. De Nooij,104D. De Pedis,131aA. De Salvo,131a U. De Sanctis,163a,163cA. De Santo,148J. B. De Vivie De Regie,114S. Dean,76W. J. Dearnaley,70R. Debbe,24

C. Debenedetti,45D. V. Dedovich,64J. Degenhardt,119M. Dehchar,117C. Del Papa,163a,163cJ. Del Peso,79 T. Del Prete,121a,121bT. Delemontex,54M. Deliyergiyev,73A. Dell’Acqua,29L. Dell’Asta,21M. Della Pietra,101a,j D. della Volpe,101a,101bM. Delmastro,4N. Delruelle,29P. A. Delsart,54C. Deluca,147S. Demers,174M. Demichev,64 B. Demirkoz,11,lJ. Deng,162S. P. Denisov,127D. Derendarz,38J. E. Derkaoui,134dF. Derue,77P. Dervan,72K. Desch,20

E. Devetak,147P. O. Deviveiros,104A. Dewhurst,128B. DeWilde,147S. Dhaliwal,157R. Dhullipudi,24,m A. Di Ciaccio,132a,132bL. Di Ciaccio,4A. Di Girolamo,29B. Di Girolamo,29S. Di Luise,133a,133bA. Di Mattia,171 B. Di Micco,29R. Di Nardo,46A. Di Simone,132a,132bR. Di Sipio,19a,19bM. A. Diaz,31aF. Diblen,18cE. B. Diehl,86

J. Dietrich,41T. A. Dietzsch,57aS. Diglio,85K. Dindar Yagci,39J. Dingfelder,20C. Dionisi,131a,131bP. Dita,25a S. Dita,25aF. Dittus,29F. Djama,82T. Djobava,50bM. A. B. do Vale,23cA. Do Valle Wemans,123aT. K. O. Doan,4

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J. Dolejsi,125I. Dolenc,73Z. Dolezal,125B. A. Dolgoshein,95,aT. Dohmae,154M. Donadelli,23dM. Donega,119 J. Donini,33J. Dopke,29A. Doria,101aA. Dos Anjos,171M. Dosil,11A. Dotti,121a,121bM. T. Dova,69J. D. Dowell,17

A. D. Doxiadis,104A. T. Doyle,52Z. Drasal,125J. Drees,173N. Dressnandt,119H. Drevermann,29C. Driouichi,35 M. Dris,9J. Dubbert,98S. Dube,14E. Duchovni,170G. Duckeck,97A. Dudarev,29F. Dudziak,63M. Du¨hrssen,29 I. P. Duerdoth,81L. Duflot,114M-A. Dufour,84M. Dunford,29H. Duran Yildiz,3aR. Duxfield,138M. Dwuznik,37

F. Dydak,29M. Du¨ren,51W. L. Ebenstein,44J. Ebke,97S. Eckweiler,80K. Edmonds,80C. A. Edwards,75 N. C. Edwards,52W. Ehrenfeld,41T. Ehrich,98T. Eifert,142G. Eigen,13K. Einsweiler,14E. Eisenhandler,74 T. Ekelof,165M. El Kacimi,134cM. Ellert,165S. Elles,4F. Ellinghaus,80K. Ellis,74N. Ellis,29J. Elmsheuser,97 M. Elsing,29D. Emeliyanov,128R. Engelmann,147A. Engl,97B. Epp,61A. Eppig,86J. Erdmann,53A. Ereditato,16

D. Eriksson,145aJ. Ernst,1M. Ernst,24J. Ernwein,135D. Errede,164S. Errede,164E. Ertel,80M. Escalier,114 C. Escobar,122X. Espinal Curull,11B. Esposito,46F. Etienne,82A. I. Etienvre,135E. Etzion,152D. Evangelakou,53

H. Evans,60L. Fabbri,19a,19bC. Fabre,29R. M. Fakhrutdinov,127S. Falciano,131aY. Fang,171M. Fanti,88a,88b A. Farbin,7A. Farilla,133aJ. Farley,147T. Farooque,157S. M. Farrington,117P. Farthouat,29P. Fassnacht,29 D. Fassouliotis,8B. Fatholahzadeh,157A. Favareto,88a,88bL. Fayard,114S. Fazio,36a,36bR. Febbraro,33P. Federic,143a

O. L. Fedin,120W. Fedorko,87M. Fehling-Kaschek,47L. Feligioni,82D. Fellmann,5C. Feng,32dE. J. Feng,30 A. B. Fenyuk,127J. Ferencei,143bJ. Ferland,92W. Fernando,108S. Ferrag,52J. Ferrando,52V. Ferrara,41A. Ferrari,165

P. Ferrari,104R. Ferrari,118aD. E. Ferreira de Lima,52A. Ferrer,166M. L. Ferrer,46D. Ferrere,48C. Ferretti,86 A. Ferretto Parodi,49a,49bM. Fiascaris,30F. Fiedler,80A. Filipcˇicˇ,73A. Filippas,9F. Filthaut,103M. Fincke-Keeler,168 M. C. N. Fiolhais,123a,iL. Fiorini,166A. Firan,39G. Fischer,41P. Fischer,20M. J. Fisher,108M. Flechl,47I. Fleck,140

J. Fleckner,80P. Fleischmann,172S. Fleischmann,173T. Flick,173A. Floderus,78L. R. Flores Castillo,171 M. J. Flowerdew,98M. Fokitis,9T. Fonseca Martin,16D. A. Forbush,137A. Formica,135A. Forti,81D. Fortin,158a

J. M. Foster,81D. Fournier,114A. Foussat,29A. J. Fowler,44K. Fowler,136H. Fox,70P. Francavilla,11 S. Franchino,118a,118bD. Francis,29T. Frank,170M. Franklin,56S. Franz,29M. Fraternali,118a,118bS. Fratina,119 S. T. French,27F. Friedrich,43R. Froeschl,29D. Froidevaux,29J. A. Frost,27C. Fukunaga,155E. Fullana Torregrosa,29 J. Fuster,166C. Gabaldon,29O. Gabizon,170T. Gadfort,24S. Gadomski,48G. Gagliardi,49a,49bP. Gagnon,60C. Galea,97

E. J. Gallas,117V. Gallo,16B. J. Gallop,128P. Gallus,124K. K. Gan,108Y. S. Gao,142,fV. A. Gapienko,127 A. Gaponenko,14F. Garberson,174M. Garcia-Sciveres,14C. Garcı´a,166J. E. Garcı´a Navarro,166R. W. Gardner,30 N. Garelli,29H. Garitaonandia,104V. Garonne,29J. Garvey,17C. Gatti,46G. Gaudio,118aB. Gaur,140L. Gauthier,135 I. L. Gavrilenko,93C. Gay,167G. Gaycken,20J-C. Gayde,29E. N. Gazis,9P. Ge,32dC. N. P. Gee,128D. A. A. Geerts,104

Ch. Geich-Gimbel,20K. Gellerstedt,145a,145bC. Gemme,49aA. Gemmell,52M. H. Genest,54S. Gentile,131a,131b M. George,53S. George,75P. Gerlach,173A. Gershon,152C. Geweniger,57aH. Ghazlane,134bN. Ghodbane,33 B. Giacobbe,19aS. Giagu,131a,131bV. Giakoumopoulou,8V. Giangiobbe,11F. Gianotti,29B. Gibbard,24A. Gibson,157 S. M. Gibson,29L. M. Gilbert,117V. Gilewsky,90D. Gillberg,28A. R. Gillman,128D. M. Gingrich,2,eJ. Ginzburg,152 N. Giokaris,8M. P. Giordani,163cR. Giordano,101a,101bF. M. Giorgi,15P. Giovannini,98P. F. Giraud,135D. Giugni,88a M. Giunta,92P. Giusti,19aB. K. Gjelsten,116L. K. Gladilin,96C. Glasman,79J. Glatzer,47A. Glazov,41K. W. Glitza,173

G. L. Glonti,64J. R. Goddard,74J. Godfrey,141J. Godlewski,29M. Goebel,41T. Go¨pfert,43C. Goeringer,80 C. Go¨ssling,42T. Go¨ttfert,98S. Goldfarb,86T. Golling,174A. Gomes,123a,cL. S. Gomez Fajardo,41R. Gonc¸alo,75

J. Goncalves Pinto Firmino Da Costa,41L. Gonella,20A. Gonidec,29S. Gonzalez,171S. Gonza´lez de la Hoz,166 G. Gonzalez Parra,11M. L. Gonzalez Silva,26S. Gonzalez-Sevilla,48J. J. Goodson,147L. Goossens,29 P. A. Gorbounov,94H. A. Gordon,24I. Gorelov,102G. Gorfine,173B. Gorini,29E. Gorini,71a,71bA. Gorisˇek,73

E. Gornicki,38S. A. Gorokhov,127V. N. Goryachev,127B. Gosdzik,41M. Gosselink,104M. I. Gostkin,64 I. Gough Eschrich,162M. Gouighri,134aD. Goujdami,134cM. P. Goulette,48A. G. Goussiou,137C. Goy,4 S. Gozpinar,22I. Grabowska-Bold,37P. Grafstro¨m,29K-J. Grahn,41F. Grancagnolo,71aS. Grancagnolo,15 V. Grassi,147V. Gratchev,120N. Grau,34H. M. Gray,29J. A. Gray,147E. Graziani,133aO. G. Grebenyuk,120

T. Greenshaw,72Z. D. Greenwood,24,mK. Gregersen,35I. M. Gregor,41P. Grenier,142J. Griffiths,137 N. Grigalashvili,64A. A. Grillo,136S. Grinstein,11Y. V. Grishkevich,96J.-F. Grivaz,114M. Groh,98E. Gross,170 J. Grosse-Knetter,53J. Groth-Jensen,170K. Grybel,140V. J. Guarino,5D. Guest,174C. Guicheney,33A. Guida,71a,71b

S. Guindon,53H. Guler,84,oJ. Gunther,124B. Guo,157J. Guo,34A. Gupta,30Y. Gusakov,64V. N. Gushchin,127 P. Gutierrez,110N. Guttman,152O. Gutzwiller,171C. Guyot,135C. Gwenlan,117C. B. Gwilliam,72A. Haas,142 S. Haas,29C. Haber,14H. K. Hadavand,39D. R. Hadley,17P. Haefner,98F. Hahn,29S. Haider,29Z. Hajduk,38

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S. Hamilton,160H. Han,32aL. Han,32bK. Hanagaki,115K. Hanawa,159M. Hance,14C. Handel,80P. Hanke,57a J. R. Hansen,35J. B. Hansen,35J. D. Hansen,35P. H. Hansen,35P. Hansson,142K. Hara,159G. A. Hare,136 T. Harenberg,173S. Harkusha,89D. Harper,86R. D. Harrington,45O. M. Harris,137K. Harrison,17J. Hartert,47 F. Hartjes,104T. Haruyama,65A. Harvey,55S. Hasegawa,100Y. Hasegawa,139S. Hassani,135M. Hatch,29D. Hauff,98

S. Haug,16M. Hauschild,29R. Hauser,87M. Havranek,20B. M. Hawes,117C. M. Hawkes,17R. J. Hawkings,29 A. D. Hawkins,78D. Hawkins,162T. Hayakawa,66T. Hayashi,159D. Hayden,75H. S. Hayward,72S. J. Haywood,128

E. Hazen,21M. He,32dS. J. Head,17V. Hedberg,78L. Heelan,7S. Heim,87B. Heinemann,14S. Heisterkamp,35 L. Helary,4C. Heller,97M. Heller,29S. Hellman,145a,145bD. Hellmich,20C. Helsens,11R. C. W. Henderson,70 M. Henke,57aA. Henrichs,53A. M. Henriques Correia,29S. Henrot-Versille,114F. Henry-Couannier,82C. Hensel,53

T. Henß,173C. M. Hernandez,7Y. Herna´ndez Jime´nez,166R. Herrberg,15A. D. Hershenhorn,151G. Herten,47 R. Hertenberger,97L. Hervas,29G. G. Hesketh,76N. P. Hessey,104E. Higo´n-Rodriguez,166D. Hill,5,aJ. C. Hill,27

N. Hill,5K. H. Hiller,41S. Hillert,20S. J. Hillier,17I. Hinchliffe,14E. Hines,119M. Hirose,115F. Hirsch,42 D. Hirschbuehl,173J. Hobbs,147N. Hod,152M. C. Hodgkinson,138P. Hodgson,138A. Hoecker,29

M. R. Hoeferkamp,102J. Hoffman,39D. Hoffmann,82M. Hohlfeld,80M. Holder,140S. O. Holmgren,145aT. Holy,126 J. L. Holzbauer,87Y. Homma,66T. M. Hong,119L. Hooft van Huysduynen,107T. Horazdovsky,126C. Horn,142

S. Horner,47J-Y. Hostachy,54S. Hou,150M. A. Houlden,72A. Hoummada,134aJ. Howarth,81D. F. Howell,117 I. Hristova,15J. Hrivnac,114I. Hruska,124T. Hryn’ova,4P. J. Hsu,80S.-C. Hsu,14G. S. Huang,110Z. Hubacek,126 F. Hubaut,82F. Huegging,20A. Huettmann,41T. B. Huffman,117E. W. Hughes,34G. Hughes,70R. E. Hughes-Jones,81 M. Huhtinen,29P. Hurst,56M. Hurwitz,14U. Husemann,41N. Huseynov,64,qJ. Huston,87J. Huth,56G. Iacobucci,48 G. Iakovidis,9M. Ibbotson,81I. Ibragimov,140R. Ichimiya,66L. Iconomidou-Fayard,114J. Idarraga,114P. Iengo,101a

O. Igonkina,104Y. Ikegami,65M. Ikeno,65Y. Ilchenko,39D. Iliadis,153N. Ilic,157M. Imori,154T. Ince,20 J. Inigo-Golfin,29P. Ioannou,8M. Iodice,133aV. Ippolito,131a,131bA. Irles Quiles,166C. Isaksson,165A. Ishikawa,66 M. Ishino,67R. Ishmukhametov,39C. Issever,117S. Istin,18aA. V. Ivashin,127W. Iwanski,38H. Iwasaki,65J. M. Izen,40 V. Izzo,101aB. Jackson,119J. N. Jackson,72P. Jackson,142M. R. Jaekel,29V. Jain,60K. Jakobs,47S. Jakobsen,35 J. Jakubek,126D. K. Jana,110E. Jankowski,157E. Jansen,76H. Jansen,29A. Jantsch,98M. Janus,20G. Jarlskog,78 L. Jeanty,56K. Jelen,37I. Jen-La Plante,30P. Jenni,29A. Jeremie,4P. Jezˇ,35S. Je´ze´quel,4M. K. Jha,19aH. Ji,171W. Ji,80 J. Jia,147Y. Jiang,32bM. Jimenez Belenguer,41G. Jin,32bS. Jin,32aO. Jinnouchi,156M. D. Joergensen,35D. Joffe,39

L. G. Johansen,13M. Johansen,145a,145bK. E. Johansson,145aP. Johansson,138S. Johnert,41K. A. Johns,6 K. Jon-And,145a,145bG. Jones,117R. W. L. Jones,70T. W. Jones,76T. J. Jones,72O. Jonsson,29C. Joram,29 P. M. Jorge,123aJ. Joseph,14J. Jovicevic,146T. Jovin,12bX. Ju,171C. A. Jung,42R. M. Jungst,29V. Juranek,124 P. Jussel,61A. Juste Rozas,11V. V. Kabachenko,127S. Kabana,16M. Kaci,166A. Kaczmarska,38P. Kadlecik,35

M. Kado,114H. Kagan,108M. Kagan,56S. Kaiser,98E. Kajomovitz,151S. Kalinin,173L. V. Kalinovskaya,64 S. Kama,39N. Kanaya,154M. Kaneda,29S. Kaneti,27T. Kanno,156V. A. Kantserov,95J. Kanzaki,65B. Kaplan,174 A. Kapliy,30J. Kaplon,29D. Kar,43M. Karagounis,20M. Karagoz,117M. Karnevskiy,41K. Karr,5V. Kartvelishvili,70

A. N. Karyukhin,127L. Kashif,171G. Kasieczka,57bR. D. Kass,108A. Kastanas,13M. Kataoka,4Y. Kataoka,154 E. Katsoufis,9J. Katzy,41V. Kaushik,6K. Kawagoe,66T. Kawamoto,154G. Kawamura,80M. S. Kayl,104 V. A. Kazanin,106M. Y. Kazarinov,64R. Keeler,168R. Kehoe,39M. Keil,53G. D. Kekelidze,64J. Kennedy,97 C. J. Kenney,142M. Kenyon,52O. Kepka,124N. Kerschen,29B. P. Kersˇevan,73S. Kersten,173K. Kessoku,154

J. Keung,157F. Khalil-zada,10H. Khandanyan,164A. Khanov,111D. Kharchenko,64A. Khodinov,95 A. G. Kholodenko,127A. Khomich,57aT. J. Khoo,27G. Khoriauli,20A. Khoroshilov,173N. Khovanskiy,64 V. Khovanskiy,94E. Khramov,64J. Khubua,50bH. Kim,145a,145bM. S. Kim,2S. H. Kim,159N. Kimura,169O. Kind,15

B. T. King,72M. King,66R. S. B. King,117J. Kirk,128L. E. Kirsch,22A. E. Kiryunin,98T. Kishimoto,66 D. Kisielewska,37T. Kittelmann,122A. M. Kiver,127E. Kladiva,143bJ. Klaiber-Lodewigs,42M. Klein,72U. Klein,72 K. Kleinknecht,80M. Klemetti,84A. Klier,170P. Klimek,145a,145bA. Klimentov,24R. Klingenberg,42J. A. Klinger,81 E. B. Klinkby,35T. Klioutchnikova,29P. F. Klok,103S. Klous,104E.-E. Kluge,57aT. Kluge,72P. Kluit,104S. Kluth,98

N. S. Knecht,157E. Kneringer,61J. Knobloch,29E.B.F.G. Knoops,82A. Knue,53B. R. Ko,44T. Kobayashi,154 M. Kobel,43M. Kocian,142P. Kodys,125K. Ko¨neke,29A. C. Ko¨nig,103S. Koenig,80L. Ko¨pke,80F. Koetsveld,103

P. Koevesarki,20T. Koffas,28E. Koffeman,104L. A. Kogan,117F. Kohn,53Z. Kohout,126T. Kohriki,65T. Koi,142 T. Kokott,20G. M. Kolachev,106H. Kolanoski,15V. Kolesnikov,64I. Koletsou,88aJ. Koll,87M. Kollefrath,47

S. D. Kolya,81A. A. Komar,93Y. Komori,154T. Kondo,65T. Kono,41,rA. I. Kononov,47R. Konoplich,107,s N. Konstantinidis,76A. Kootz,173S. Koperny,37K. Korcyl,38K. Kordas,153V. Koreshev,127A. Korn,117A. Korol,106

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I. Korolkov,11E. V. Korolkova,138V. A. Korotkov,127O. Kortner,98S. Kortner,98V. V. Kostyukhin,20 M. J. Kotama¨ki,29S. Kotov,98V. M. Kotov,64A. Kotwal,44C. Kourkoumelis,8V. Kouskoura,153A. Koutsman,158a

R. Kowalewski,168T. Z. Kowalski,37W. Kozanecki,135A. S. Kozhin,127V. Kral,126V. A. Kramarenko,96 G. Kramberger,73M. W. Krasny,77A. Krasznahorkay,107J. Kraus,87J. K. Kraus,20A. Kreisel,152F. Krejci,126 J. Kretzschmar,72N. Krieger,53P. Krieger,157K. Kroeninger,53H. Kroha,98J. Kroll,119J. Kroseberg,20J. Krstic,12a U. Kruchonak,64H. Kru¨ger,20T. Kruker,16N. Krumnack,63Z. V. Krumshteyn,64A. Kruth,20T. Kubota,85S. Kuday,3a

S. Kuehn,47A. Kugel,57cT. Kuhl,41D. Kuhn,61V. Kukhtin,64Y. Kulchitsky,89S. Kuleshov,31bC. Kummer,97 M. Kuna,77N. Kundu,117J. Kunkle,119A. Kupco,124H. Kurashige,66M. Kurata,159Y. A. Kurochkin,89V. Kus,124 E. S. Kuwertz,146M. Kuze,156J. Kvita,141R. Kwee,15A. La Rosa,48L. La Rotonda,36a,36bL. Labarga,79J. Labbe,4

S. Lablak,134aC. Lacasta,166F. Lacava,131a,131bH. Lacker,15D. Lacour,77V. R. Lacuesta,166E. Ladygin,64 R. Lafaye,4B. Laforge,77T. Lagouri,79S. Lai,47E. Laisne,54M. Lamanna,29C. L. Lampen,6W. Lampl,6

E. Lancon,135U. Landgraf,47M. P. J. Landon,74J. L. Lane,81C. Lange,41A. J. Lankford,162F. Lanni,24 K. Lantzsch,173S. Laplace,77C. Lapoire,20J. F. Laporte,135T. Lari,88aA. V. Larionov,127A. Larner,117C. Lasseur,29

M. Lassnig,29P. Laurelli,46V. Lavorini,36a,36bW. Lavrijsen,14P. Laycock,72A. B. Lazarev,64O. Le Dortz,77 E. Le Guirriec,82C. Le Maner,157E. Le Menedeu,9C. Lebel,92T. LeCompte,5F. Ledroit-Guillon,54H. Lee,104 J. S. H. Lee,115S. C. Lee,150L. Lee,174M. Lefebvre,168M. Legendre,135A. Leger,48B. C. LeGeyt,119F. Legger,97

C. Leggett,14M. Lehmacher,20G. Lehmann Miotto,29X. Lei,6M. A. L. Leite,23dR. Leitner,125D. Lellouch,170 M. Leltchouk,34B. Lemmer,53V. Lendermann,57aK. J. C. Leney,144bT. Lenz,104G. Lenzen,173B. Lenzi,29 K. Leonhardt,43S. Leontsinis,9C. Leroy,92J-R. Lessard,168J. Lesser,145aC. G. Lester,27A. Leung Fook Cheong,171

J. Leveˆque,4D. Levin,86L. J. Levinson,170M. S. Levitski,127A. Lewis,117G. H. Lewis,107A. M. Leyko,20 M. Leyton,15B. Li,82H. Li,171,tS. Li,32b,uX. Li,86Z. Liang,117,vH. Liao,33B. Liberti,132aP. Lichard,29 M. Lichtnecker,97K. Lie,164W. Liebig,13R. Lifshitz,151C. Limbach,20A. Limosani,85M. Limper,62S. C. Lin,150,w F. Linde,104J. T. Linnemann,87E. Lipeles,119L. Lipinsky,124A. Lipniacka,13T. M. Liss,164D. Lissauer,24A. Lister,48

A. M. Litke,136C. Liu,28D. Liu,150H. Liu,86J. B. Liu,86M. Liu,32bY. Liu,32bM. Livan,118a,118b S. S. A. Livermore,117A. Lleres,54J. Llorente Merino,79S. L. Lloyd,74E. Lobodzinska,41P. Loch,6 W. S. Lockman,136T. Loddenkoetter,20F. K. Loebinger,81A. Loginov,174C. W. Loh,167T. Lohse,15K. Lohwasser,47

M. Lokajicek,124J. Loken,117V. P. Lombardo,4R. E. Long,70L. Lopes,123aD. Lopez Mateos,56J. Lorenz,97 N. Lorenzo Martinez,114M. Losada,161P. Loscutoff,14F. Lo Sterzo,131a,131bM. J. Losty,158aX. Lou,40A. Lounis,114

K. F. Loureiro,161J. Love,21P. A. Love,70A. J. Lowe,142,fF. Lu,32aH. J. Lubatti,137C. Luci,131a,131bA. Lucotte,54 A. Ludwig,43D. Ludwig,41I. Ludwig,47J. Ludwig,47F. Luehring,60G. Luijckx,104D. Lumb,47L. Luminari,131a

E. Lund,116B. Lund-Jensen,146B. Lundberg,78J. Lundberg,145a,145bJ. Lundquist,35M. Lungwitz,80G. Lutz,98 D. Lynn,24J. Lys,14E. Lytken,78H. Ma,24L. L. Ma,171J. A. Macana Goia,92G. Maccarrone,46A. Macchiolo,98 B. Macˇek,73J. Machado Miguens,123aR. Mackeprang,35R. J. Madaras,14W. F. Mader,43R. Maenner,57cT. Maeno,24

P. Ma¨ttig,173S. Ma¨ttig,41L. Magnoni,29E. Magradze,53Y. Mahalalel,152K. Mahboubi,47G. Mahout,17 C. Maiani,131a,131bC. Maidantchik,23aA. Maio,123a,cS. Majewski,24Y. Makida,65N. Makovec,114P. Mal,135 B. Malaescu,29Pa. Malecki,38P. Malecki,38V. P. Maleev,120F. Malek,54U. Mallik,62D. Malon,5C. Malone,142

S. Maltezos,9V. Malyshev,106S. Malyukov,29R. Mameghani,97J. Mamuzic,12bA. Manabe,65L. Mandelli,88a I. Mandic´,73R. Mandrysch,15J. Maneira,123aP. S. Mangeard,87L. Manhaes de Andrade Filho,23aI. D. Manjavidze,64 A. Mann,53P. M. Manning,136A. Manousakis-Katsikakis,8B. Mansoulie,135A. Manz,98A. Mapelli,29L. Mapelli,29

L. March,79J. F. Marchand,28F. Marchese,132a,132bG. Marchiori,77M. Marcisovsky,124C. P. Marino,168 F. Marroquim,23aR. Marshall,81Z. Marshall,29F. K. Martens,157S. Marti-Garcia,166A. J. Martin,174B. Martin,29

B. Martin,87F. F. Martin,119J. P. Martin,92Ph. Martin,54T. A. Martin,17V. J. Martin,45B. Martin dit Latour,48 S. Martin-Haugh,148M. Martinez,11V. Martinez Outschoorn,56A. C. Martyniuk,168M. Marx,81F. Marzano,131a

A. Marzin,110L. Masetti,80T. Mashimo,154R. Mashinistov,93J. Masik,81A. L. Maslennikov,106I. Massa,19a,19b G. Massaro,104N. Massol,4P. Mastrandrea,131a,131bA. Mastroberardino,36a,36bT. Masubuchi,154P. Matricon,114

H. Matsumoto,154H. Matsunaga,154T. Matsushita,66C. Mattravers,117,dJ. M. Maugain,29J. Maurer,82 S. J. Maxfield,72D. A. Maximov,106,gE. N. May,5A. Mayne,138R. Mazini,150M. Mazur,20M. Mazzanti,88a S. P. Mc Kee,86A. McCarn,164R. L. McCarthy,147T. G. McCarthy,28N. A. McCubbin,128K. W. McFarlane,55

J. A. Mcfayden,138H. McGlone,52G. Mchedlidze,50bR. A. McLaren,29T. Mclaughlan,17S. J. McMahon,128 R. A. McPherson,168,kA. Meade,83J. Mechnich,104M. Mechtel,173M. Medinnis,41R. Meera-Lebbai,110 T. Meguro,115R. Mehdiyev,92S. Mehlhase,35A. Mehta,72K. Meier,57aB. Meirose,78C. Melachrinos,30

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B. R. Mellado Garcia,171L. Mendoza Navas,161Z. Meng,150,tA. Mengarelli,19a,19bS. Menke,98C. Menot,29 E. Meoni,11K. M. Mercurio,56P. Mermod,48L. Merola,101a,101bC. Meroni,88aF. S. Merritt,30H. Merritt,108 A. Messina,29J. Metcalfe,102A. S. Mete,63C. Meyer,80C. Meyer,30J-P. Meyer,135J. Meyer,172J. Meyer,53 T. C. Meyer,29W. T. Meyer,63J. Miao,32dS. Michal,29L. Micu,25aR. P. Middleton,128S. Migas,72L. Mijovic´,41

G. Mikenberg,170M. Mikestikova,124M. Mikuzˇ,73D. W. Miller,30R. J. Miller,87W. J. Mills,167C. Mills,56 A. Milov,170D. A. Milstead,145a,145bD. Milstein,170A. A. Minaenko,127M. Min˜ano Moya,166I. A. Minashvili,64

A. I. Mincer,107B. Mindur,37M. Mineev,64Y. Ming,171L. M. Mir,11G. Mirabelli,131aL. Miralles Verge,11 A. Misiejuk,75J. Mitrevski,136G. Y. Mitrofanov,127V. A. Mitsou,166S. Mitsui,65P. S. Miyagawa,138K. Miyazaki,66

J. U. Mjo¨rnmark,78T. Moa,145a,145bP. Mockett,137S. Moed,56V. Moeller,27K. Mo¨nig,41N. Mo¨ser,20 S. Mohapatra,147W. Mohr,47S. Mohrdieck-Mo¨ck,98A. M. Moisseev,127,aR. Moles-Valls,166J. Molina-Perez,29 J. Monk,76E. Monnier,82S. Montesano,88a,88bF. Monticelli,69S. Monzani,19a,19bR. W. Moore,2G. F. Moorhead,85 C. Mora Herrera,48A. Moraes,52N. Morange,135J. Morel,53G. Morello,36a,36bD. Moreno,80M. Moreno Lla´cer,166

P. Morettini,49aM. Morgenstern,43M. Morii,56J. Morin,74A. K. Morley,29G. Mornacchi,29S. V. Morozov,95 J. D. Morris,74L. Morvaj,100H. G. Moser,98M. Mosidze,50bJ. Moss,108R. Mount,142E. Mountricha,9,x S. V. Mouraviev,93E. J. W. Moyse,83M. Mudrinic,12bF. Mueller,57aJ. Mueller,122K. Mueller,20T. A. Mu¨ller,97 T. Mueller,80D. Muenstermann,29A. Muir,167Y. Munwes,152W. J. Murray,128I. Mussche,104E. Musto,101a,101b A. G. Myagkov,127M. Myska,124J. Nadal,11K. Nagai,159K. Nagano,65A. Nagarkar,108Y. Nagasaka,59M. Nagel,98

A. M. Nairz,29Y. Nakahama,29K. Nakamura,154T. Nakamura,154I. Nakano,109G. Nanava,20A. Napier,160 R. Narayan,57bM. Nash,76,dN. R. Nation,21T. Nattermann,20T. Naumann,41G. Navarro,161H. A. Neal,86E. Nebot,79

P.Yu. Nechaeva,93T. J. Neep,81A. Negri,118a,118bG. Negri,29S. Nektarijevic,48A. Nelson,162S. Nelson,142 T. K. Nelson,142S. Nemecek,124P. Nemethy,107A. A. Nepomuceno,23aM. Nessi,29,yM. S. Neubauer,164 A. Neusiedl,80R. M. Neves,107P. Nevski,24P. R. Newman,17V. Nguyen Thi Hong,135R. B. Nickerson,117 R. Nicolaidou,135L. Nicolas,138B. Nicquevert,29F. Niedercorn,114J. Nielsen,136T. Niinikoski,29N. Nikiforou,34 A. Nikiforov,15V. Nikolaenko,127K. Nikolaev,64I. Nikolic-Audit,77K. Nikolics,48K. Nikolopoulos,24H. Nilsen,47

P. Nilsson,7Y. Ninomiya,154A. Nisati,131aT. Nishiyama,66R. Nisius,98L. Nodulman,5M. Nomachi,115 I. Nomidis,153M. Nordberg,29B. Nordkvist,145a,145bP. R. Norton,128J. Novakova,125M. Nozaki,65L. Nozka,112

I. M. Nugent,158aA.-E. Nuncio-Quiroz,20G. Nunes Hanninger,85T. Nunnemann,97E. Nurse,76B. J. O’Brien,45 S. W. O’Neale,17,aD. C. O’Neil,141V. O’Shea,52L. B. Oakes,97F. G. Oakham,28,eH. Oberlack,98J. Ocariz,77 A. Ochi,66S. Oda,154S. Odaka,65J. Odier,82H. Ogren,60A. Oh,81S. H. Oh,44C. C. Ohm,145a,145bT. Ohshima,100 H. Ohshita,139T. Ohsugi,58S. Okada,66H. Okawa,162Y. Okumura,100T. Okuyama,154A. Olariu,25aM. Olcese,49a A. G. Olchevski,64S. A. Olivares Pino,31aM. Oliveira,123a,iD. Oliveira Damazio,24E. Oliver Garcia,166D. Olivito,119 A. Olszewski,38J. Olszowska,38C. Omachi,66A. Onofre,123a,zP. U. E. Onyisi,30C. J. Oram,158aM. J. Oreglia,30 Y. Oren,152D. Orestano,133a,133bI. Orlov,106C. Oropeza Barrera,52R. S. Orr,157B. Osculati,49a,49bR. Ospanov,119

C. Osuna,11G. Otero y Garzon,26J. P. Ottersbach,104M. Ouchrif,134dE. A. Ouellette,168F. Ould-Saada,116 A. Ouraou,135Q. Ouyang,32aA. Ovcharova,14M. Owen,81S. Owen,138V. E. Ozcan,18aN. Ozturk,7 A. Pacheco Pages,11C. Padilla Aranda,11S. Pagan Griso,14E. Paganis,138F. Paige,24P. Pais,83K. Pajchel,116

G. Palacino,158bC. P. Paleari,6S. Palestini,29D. Pallin,33A. Palma,123aJ. D. Palmer,17Y. B. Pan,171 E. Panagiotopoulou,9B. Panes,31aN. Panikashvili,86S. Panitkin,24D. Pantea,25aM. Panuskova,124V. Paolone,122

A. Papadelis,145aTh.D. Papadopoulou,9A. Paramonov,5D. Paredes Hernandez,33W. Park,24,aaM. A. Parker,27 F. Parodi,49a,49bJ. A. Parsons,34U. Parzefall,47E. Pasqualucci,131aS. Passaggio,49aA. Passeri,133aF. Pastore,133a,133b Fr. Pastore,75G. Pa´sztor,48,bbS. Pataraia,173N. Patel,149J. R. Pater,81S. Patricelli,101a,101bT. Pauly,29M. Pecsy,143a M. I. Pedraza Morales,171S. V. Peleganchuk,106H. Peng,32bR. Pengo,29B. Penning,30A. Penson,34J. Penwell,60

M. Perantoni,23aK. Perez,34,ccT. Perez Cavalcanti,41E. Perez Codina,11M. T. Pe´rez Garcı´a-Estan˜,166 V. Perez Reale,34L. Perini,88a,88bH. Pernegger,29R. Perrino,71aP. Perrodo,4S. Persembe,3aA. Perus,114 V. D. Peshekhonov,64K. Peters,29B. A. Petersen,29J. Petersen,29T. C. Petersen,35E. Petit,4A. Petridis,153

C. Petridou,153E. Petrolo,131aF. Petrucci,133a,133bD. Petschull,41M. Petteni,141R. Pezoa,31bA. Phan,85 P. W. Phillips,128G. Piacquadio,29A. Picazio,48E. Piccaro,74M. Piccinini,19a,19bS. M. Piec,41R. Piegaia,26 D. T. Pignotti,108J. E. Pilcher,30A. D. Pilkington,81J. Pina,123a,cM. Pinamonti,163a,163cA. Pinder,117J. L. Pinfold,2

J. Ping,32cB. Pinto,123aO. Pirotte,29C. Pizio,88a,88bM. Plamondon,168M.-A. Pleier,24A. V. Pleskach,127 A. Poblaguev,24S. Poddar,57aF. Podlyski,33L. Poggioli,114T. Poghosyan,20M. Pohl,48F. Polci,54G. Polesello,118a A. Policicchio,36a,36bA. Polini,19aJ. Poll,74V. Polychronakos,24D. M. Pomarede,135D. Pomeroy,22K. Pomme`s,29

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L. Pontecorvo,131aB. G. Pope,87G. A. Popeneciu,25aD. S. Popovic,12aA. Poppleton,29X. Portell Bueso,29 C. Posch,21G. E. Pospelov,98S. Pospisil,126I. N. Potrap,98C. J. Potter,148C. T. Potter,113G. Poulard,29J. Poveda,171

V. Pozdnyakov,64R. Prabhu,76P. Pralavorio,82A. Pranko,14S. Prasad,29R. Pravahan,7S. Prell,63K. Pretzl,16 L. Pribyl,29D. Price,60J. Price,72L. E. Price,5M. J. Price,29D. Prieur,122M. Primavera,71aK. Prokofiev,107 F. Prokoshin,31bS. Protopopescu,24J. Proudfoot,5X. Prudent,43M. Przybycien,37H. Przysiezniak,4S. Psoroulas,20

E. Ptacek,113E. Pueschel,83J. Purdham,86M. Purohit,24,aaP. Puzo,114Y. Pylypchenko,62J. Qian,86Z. Qian,82 Z. Qin,41A. Quadt,53D. R. Quarrie,14W. B. Quayle,171F. Quinonez,31aM. Raas,103V. Radescu,57bB. Radics,20

P. Radloff,113T. Rador,18aF. Ragusa,88a,88bG. Rahal,176A. M. Rahimi,108D. Rahm,24S. Rajagopalan,24 M. Rammensee,47M. Rammes,140A. S. Randle-Conde,39K. Randrianarivony,28P. N. Ratoff,70F. Rauscher,97 T. C. Rave,47M. Raymond,29A. L. Read,116D. M. Rebuzzi,118a,118bA. Redelbach,172G. Redlinger,24R. Reece,119

K. Reeves,40A. Reichold,104E. Reinherz-Aronis,152A. Reinsch,113I. Reisinger,42C. Rembser,29Z. L. Ren,150 A. Renaud,114M. Rescigno,131aS. Resconi,88aB. Resende,135P. Reznicek,97R. Rezvani,157A. Richards,76 R. Richter,98E. Richter-Was,4,ddM. Ridel,77M. Rijpstra,104M. Rijssenbeek,147A. Rimoldi,118a,118bL. Rinaldi,19a

R. R. Rios,39I. Riu,11G. Rivoltella,88a,88bF. Rizatdinova,111E. Rizvi,74S. H. Robertson,84,k A. Robichaud-Veronneau,117D. Robinson,27J. E. M. Robinson,76A. Robson,52J. G. Rocha de Lima,105 C. Roda,121a,121bD. Roda Dos Santos,29D. Rodriguez,161A. Roe,53S. Roe,29O. Røhne,116V. Rojo,1S. Rolli,160

A. Romaniouk,95M. Romano,19a,19bV. M. Romanov,64G. Romeo,26E. Romero Adam,166L. Roos,77E. Ros,166 S. Rosati,131aK. Rosbach,48A. Rose,148M. Rose,75G. A. Rosenbaum,157E. I. Rosenberg,63P. L. Rosendahl,13 O. Rosenthal,140L. Rosselet,48V. Rossetti,11E. Rossi,131a,131bL. P. Rossi,49aM. Rotaru,25aI. Roth,170J. Rothberg,137

D. Rousseau,114C. R. Royon,135A. Rozanov,82Y. Rozen,151X. Ruan,32a,eeI. Rubinskiy,41B. Ruckert,97 N. Ruckstuhl,104V. I. Rud,96C. Rudolph,43G. Rudolph,61F. Ru¨hr,6F. Ruggieri,133a,133bA. Ruiz-Martinez,63

V. Rumiantsev,90,aL. Rumyantsev,64K. Runge,47Z. Rurikova,47N. A. Rusakovich,64J. P. Rutherfoord,6 C. Ruwiedel,14P. Ruzicka,124Y. F. Ryabov,120V. Ryadovikov,127P. Ryan,87M. Rybar,125G. Rybkin,114

N. C. Ryder,117S. Rzaeva,10A. F. Saavedra,149I. Sadeh,152H.F-W. Sadrozinski,136R. Sadykov,64

F. Safai Tehrani,131aH. Sakamoto,154G. Salamanna,74A. Salamon,132aM. Saleem,110D. Salihagic,98A. Salnikov,142 J. Salt,166B. M. Salvachua Ferrando,5D. Salvatore,36a,36bF. Salvatore,148A. Salvucci,103A. Salzburger,29 D. Sampsonidis,153B. H. Samset,116A. Sanchez,101a,101bV. Sanchez Martinez,166H. Sandaker,13H. G. Sander,80 M. P. Sanders,97M. Sandhoff,173T. Sandoval,27C. Sandoval,161R. Sandstroem,98S. Sandvoss,173D. P. C. Sankey,128

A. Sansoni,46C. Santamarina Rios,84C. Santoni,33R. Santonico,132a,132bH. Santos,123aJ. G. Saraiva,123a T. Sarangi,171E. Sarkisyan-Grinbaum,7F. Sarri,121a,121bG. Sartisohn,173O. Sasaki,65N. Sasao,67 I. Satsounkevitch,89G. Sauvage,4E. Sauvan,4J. B. Sauvan,114P. Savard,157,eV. Savinov,122D. O. Savu,29 L. Sawyer,24,mD. H. Saxon,52L. P. Says,33C. Sbarra,19aA. Sbrizzi,19a,19bO. Scallon,92D. A. Scannicchio,162 M. Scarcella,149J. Schaarschmidt,114P. Schacht,98U. Scha¨fer,80S. Schaepe,20S. Schaetzel,57bA. C. Schaffer,114

D. Schaile,97R. D. Schamberger,147A. G. Schamov,106V. Scharf,57aV. A. Schegelsky,120D. Scheirich,86 M. Schernau,162M. I. Scherzer,34C. Schiavi,49a,49bJ. Schieck,97M. Schioppa,36a,36bS. Schlenker,29J. L. Schlereth,5

E. Schmidt,47K. Schmieden,20C. Schmitt,80S. Schmitt,57bM. Schmitz,20A. Scho¨ning,57bM. Schott,29 D. Schouten,158aJ. Schovancova,124M. Schram,84C. Schroeder,80N. Schroer,57cG. Schuler,29M. J. Schultens,20

J. Schultes,173H.-C. Schultz-Coulon,57aH. Schulz,15J. W. Schumacher,20M. Schumacher,47B. A. Schumm,136 Ph. Schune,135C. Schwanenberger,81A. Schwartzman,142Ph. Schwemling,77R. Schwienhorst,87R. Schwierz,43 J. Schwindling,135T. Schwindt,20M. Schwoerer,4W. G. Scott,128J. Searcy,113G. Sedov,41E. Sedykh,120E. Segura,11 S. C. Seidel,102A. Seiden,136F. Seifert,43J. M. Seixas,23aG. Sekhniaidze,101aK. E. Selbach,45D. M. Seliverstov,120

B. Sellden,145aG. Sellers,72M. Seman,143bN. Semprini-Cesari,19a,19bC. Serfon,97L. Serin,114L. Serkin,53 R. Seuster,98H. Severini,110M. E. Sevior,85A. Sfyrla,29E. Shabalina,53M. Shamim,113L. Y. Shan,32aJ. T. Shank,21

Q. T. Shao,85M. Shapiro,14P. B. Shatalov,94L. Shaver,6K. Shaw,163a,163cD. Sherman,174P. Sherwood,76 A. Shibata,107H. Shichi,100S. Shimizu,29M. Shimojima,99T. Shin,55M. Shiyakova,64A. Shmeleva,93 M. J. Shochet,30D. Short,117S. Shrestha,63E. Shulga,95M. A. Shupe,6P. Sicho,124A. Sidoti,131aF. Siegert,47

Dj. Sijacki,12aO. Silbert,170J. Silva,123aY. Silver,152D. Silverstein,142S. B. Silverstein,145aV. Simak,126 O. Simard,135Lj. Simic,12aS. Simion,114B. Simmons,76M. Simonyan,35P. Sinervo,157N. B. Sinev,113V. Sipica,140 G. Siragusa,172A. Sircar,24A. N. Sisakyan,64S.Yu. Sivoklokov,96J. Sjo¨lin,145a,145bT. B. Sjursen,13L. A. Skinnari,14 H. P. Skottowe,56K. Skovpen,106P. Skubic,110N. Skvorodnev,22M. Slater,17T. Slavicek,126K. Sliwa,160J. Sloper,29 V. Smakhtin,170B. H. Smart,45S.Yu. Smirnov,95Y. Smirnov,95L. N. Smirnova,96O. Smirnova,78B. C. Smith,56

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D. Smith,142K. M. Smith,52M. Smizanska,70K. Smolek,126A. A. Snesarev,93S. W. Snow,81J. Snow,110 J. Snuverink,104S. Snyder,24M. Soares,123aR. Sobie,168,kJ. Sodomka,126A. Soffer,152C. A. Solans,166M. Solar,126 J. Solc,126E. Soldatov,95U. Soldevila,166E. Solfaroli Camillocci,131a,131bA. A. Solodkov,127O. V. Solovyanov,127

N. Soni,2V. Sopko,126B. Sopko,126M. Sosebee,7R. Soualah,163a,163cA. Soukharev,106S. Spagnolo,71a,71b F. Spano`,75R. Spighi,19aG. Spigo,29F. Spila,131a,131bR. Spiwoks,29M. Spousta,125T. Spreitzer,157B. Spurlock,7

R. D. St. Denis,52J. Stahlman,119R. Stamen,57aE. Stanecka,38R. W. Stanek,5C. Stanescu,133aS. Stapnes,116 E. A. Starchenko,127J. Stark,54P. Staroba,124P. Starovoitov,90A. Staude,97P. Stavina,143aG. Steele,52P. Steinbach,43

P. Steinberg,24I. Stekl,126B. Stelzer,141H. J. Stelzer,87O. Stelzer-Chilton,158aH. Stenzel,51S. Stern,98 K. Stevenson,74G. A. Stewart,29J. A. Stillings,20M. C. Stockton,84K. Stoerig,47G. Stoicea,25aS. Stonjek,98

P. Strachota,125A. R. Stradling,7A. Straessner,43J. Strandberg,146S. Strandberg,145a,145bA. Strandlie,116 M. Strang,108E. Strauss,142M. Strauss,110P. Strizenec,143bR. Stro¨hmer,172D. M. Strom,113J. A. Strong,75,a R. Stroynowski,39J. Strube,128B. Stugu,13I. Stumer,24,aJ. Stupak,147P. Sturm,173N. A. Styles,41D. A. Soh,150,v

D. Su,142HS. Subramania,2A. Succurro,11Y. Sugaya,115T. Sugimoto,100C. Suhr,105K. Suita,66M. Suk,125 V. V. Sulin,93S. Sultansoy,3dT. Sumida,67X. Sun,54J. E. Sundermann,47K. Suruliz,138S. Sushkov,11 G. Susinno,36a,36bM. R. Sutton,148Y. Suzuki,65Y. Suzuki,66M. Svatos,124Yu.M. Sviridov,127S. Swedish,167 I. Sykora,143aT. Sykora,125B. Szeless,29J. Sa´nchez,166D. Ta,104K. Tackmann,41A. Taffard,162R. Tafirout,158a N. Taiblum,152Y. Takahashi,100H. Takai,24R. Takashima,68H. Takeda,66T. Takeshita,139Y. Takubo,65M. Talby,82

A. Talyshev,106,gM. C. Tamsett,24J. Tanaka,154R. Tanaka,114S. Tanaka,130S. Tanaka,65Y. Tanaka,99 A. J. Tanasijczuk,141K. Tani,66N. Tannoury,82G. P. Tappern,29S. Tapprogge,80D. Tardif,157S. Tarem,151 F. Tarrade,28G. F. Tartarelli,88aP. Tas,125M. Tasevsky,124E. Tassi,36a,36bM. Tatarkhanov,14Y. Tayalati,134d

C. Taylor,76F. E. Taylor,91G. N. Taylor,85W. Taylor,158bM. Teinturier,114M. Teixeira Dias Castanheira,74 P. Teixeira-Dias,75K. K. Temming,47H. Ten Kate,29P. K. Teng,150S. Terada,65K. Terashi,154J. Terron,79M. Testa,46 R. J. Teuscher,157,kJ. Thadome,173J. Therhaag,20T. Theveneaux-Pelzer,77M. Thioye,174S. Thoma,47J. P. Thomas,17 E. N. Thompson,34P. D. Thompson,17P. D. Thompson,157A. S. Thompson,52L. A. Thomsen,35E. Thomson,119

M. Thomson,27R. P. Thun,86F. Tian,34M. J. Tibbetts,14T. Tic,124V. O. Tikhomirov,93Y. A. Tikhonov,106,g S. Timoshenko,95P. Tipton,174F. J. Tique Aires Viegas,29S. Tisserant,82B. Toczek,37T. Todorov,4 S. Todorova-Nova,160B. Toggerson,162J. Tojo,65S. Toka´r,143aK. Tokunaga,66K. Tokushuku,65K. Tollefson,87 M. Tomoto,100L. Tompkins,30K. Toms,102G. Tong,32aA. Tonoyan,13C. Topfel,16N. D. Topilin,64I. Torchiani,29

E. Torrence,113H. Torres,77E. Torro´ Pastor,166J. Toth,82,bbF. Touchard,82D. R. Tovey,138T. Trefzger,172 L. Tremblet,29A. Tricoli,29I. M. Trigger,158aS. Trincaz-Duvoid,77T. N. Trinh,77M. F. Tripiana,69W. Trischuk,157

A. Trivedi,24,aaB. Trocme´,54C. Troncon,88aM. Trottier-McDonald,141M. Trzebinski,38A. Trzupek,38 C. Tsarouchas,29J.C-L. Tseng,117M. Tsiakiris,104P. V. Tsiareshka,89D. Tsionou,4,ffG. Tsipolitis,9V. Tsiskaridze,47

E. G. Tskhadadze,50aI. I. Tsukerman,94V. Tsulaia,14J.-W. Tsung,20S. Tsuno,65D. Tsybychev,147A. Tua,138 A. Tudorache,25aV. Tudorache,25aJ. M. Tuggle,30M. Turala,38D. Turecek,126I. Turk Cakir,3eE. Turlay,104

R. Turra,88a,88bP. M. Tuts,34A. Tykhonov,73M. Tylmad,145a,145bM. Tyndel,128G. Tzanakos,8K. Uchida,20 I. Ueda,154R. Ueno,28M. Ugland,13M. Uhlenbrock,20M. Uhrmacher,53F. Ukegawa,159G. Unal,29 D. G. Underwood,5A. Undrus,24G. Unel,162Y. Unno,65D. Urbaniec,34G. Usai,7M. Uslenghi,118a,118b L. Vacavant,82V. Vacek,126B. Vachon,84S. Vahsen,14J. Valenta,124P. Valente,131aS. Valentinetti,19a,19bS. Valkar,125

E. Valladolid Gallego,166S. Vallecorsa,151J. A. Valls Ferrer,166H. van der Graaf,104E. van der Kraaij,104 R. Van Der Leeuw,104E. van der Poel,104D. van der Ster,29N. van Eldik,83P. van Gemmeren,5Z. van Kesteren,104

I. van Vulpen,104M. Vanadia,98W. Vandelli,29G. Vandoni,29A. Vaniachine,5P. Vankov,41F. Vannucci,77 F. Varela Rodriguez,29R. Vari,131aE. W. Varnes,6D. Varouchas,14A. Vartapetian,7K. E. Varvell,149 V. I. Vassilakopoulos,55F. Vazeille,33T. Vazquez Schroeder,53G. Vegni,88a,88bJ. J. Veillet,114C. Vellidis,8 F. Veloso,123aR. Veness,29S. Veneziano,131aA. Ventura,71a,71bD. Ventura,137M. Venturi,47N. Venturi,157 V. Vercesi,118aM. Verducci,137W. Verkerke,104J. C. Vermeulen,104A. Vest,43M. C. Vetterli,141,eI. Vichou,164 T. Vickey,144b,ggO. E. Vickey Boeriu,144bG. H. A. Viehhauser,117S. Viel,167M. Villa,19a,19bM. Villaplana Perez,166 E. Vilucchi,46M. G. Vincter,28E. Vinek,29V. B. Vinogradov,64M. Virchaux,135,aJ. Virzi,14O. Vitells,170M. Viti,41

I. Vivarelli,47F. Vives Vaque,2S. Vlachos,9D. Vladoiu,97M. Vlasak,126N. Vlasov,20A. Vogel,20P. Vokac,126 G. Volpi,46M. Volpi,85G. Volpini,88aH. von der Schmitt,98J. von Loeben,98H. von Radziewski,47E. von Toerne,20 V. Vorobel,125A. P. Vorobiev,127V. Vorwerk,11M. Vos,166R. Voss,29T. T. Voss,173J. H. Vossebeld,72N. Vranjes,135

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W. Wagner,173P. Wagner,119H. Wahlen,173J. Wakabayashi,100J. Walbersloh,42S. Walch,86J. Walder,70R. Walker,97 W. Walkowiak,140R. Wall,174P. Waller,72C. Wang,44H. Wang,171H. Wang,32b,hhJ. Wang,150J. Wang,54 J. C. Wang,137R. Wang,102S. M. Wang,150A. Warburton,84C. P. Ward,27M. Warsinsky,47P. M. Watkins,17

A. T. Watson,17I. J. Watson,149M. F. Watson,17G. Watts,137S. Watts,81A. T. Waugh,149B. M. Waugh,76 M. Weber,128M. S. Weber,16P. Weber,53A. R. Weidberg,117P. Weigell,98J. Weingarten,53C. Weiser,47 H. Wellenstein,22P. S. Wells,29T. Wenaus,24D. Wendland,15S. Wendler,122Z. Weng,150,vT. Wengler,29S. Wenig,29

N. Wermes,20M. Werner,47P. Werner,29M. Werth,162M. Wessels,57aC. Weydert,54K. Whalen,28 S. J. Wheeler-Ellis,162S. P. Whitaker,21A. White,7M. J. White,85S. R. Whitehead,117D. Whiteson,162 D. Whittington,60F. Wicek,114D. Wicke,173F. J. Wickens,128W. Wiedenmann,171M. Wielers,128P. Wienemann,20

C. Wiglesworth,74L. A. M. Wiik-Fuchs,47P. A. Wijeratne,76A. Wildauer,166M. A. Wildt,41,rI. Wilhelm,125 H. G. Wilkens,29J. Z. Will,97E. Williams,34H. H. Williams,119W. Willis,34S. Willocq,83J. A. Wilson,17

M. G. Wilson,142A. Wilson,86I. Wingerter-Seez,4S. Winkelmann,47F. Winklmeier,29M. Wittgen,142 M. W. Wolter,38H. Wolters,123a,iW. C. Wong,40G. Wooden,86B. K. Wosiek,38J. Wotschack,29M. J. Woudstra,83 K. W. Wozniak,38K. Wraight,52C. Wright,52M. Wright,52B. Wrona,72S. L. Wu,171X. Wu,48Y. Wu,32b,iiE. Wulf,34

R. Wunstorf,42B. M. Wynne,45S. Xella,35M. Xiao,135S. Xie,47Y. Xie,32aC. Xu,32b,xD. Xu,138G. Xu,32a B. Yabsley,149S. Yacoob,144bM. Yamada,65H. Yamaguchi,154A. Yamamoto,65K. Yamamoto,63S. Yamamoto,154 T. Yamamura,154T. Yamanaka,154J. Yamaoka,44T. Yamazaki,154Y. Yamazaki,66Z. Yan,21H. Yang,86U. K. Yang,81 Y. Yang,60Y. Yang,32aZ. Yang,145a,145bS. Yanush,90Y. Yao,14Y. Yasu,65G. V. Ybeles Smit,129J. Ye,39S. Ye,24 M. Yilmaz,3cR. Yoosoofmiya,122K. Yorita,169R. Yoshida,5C. Young,142S. Youssef,21D. Yu,24J. Yu,7J. Yu,111

L. Yuan,32a,jjA. Yurkewicz,105B. Zabinski,38V. G. Zaets,127R. Zaidan,62A. M. Zaitsev,127Z. Zajacova,29 L. Zanello,131a,131bA. Zaytsev,106C. Zeitnitz,173M. Zeller,174M. Zeman,124A. Zemla,38C. Zendler,20O. Zenin,127

T. Zˇ enisˇ,143aZ. Zinonos,121a,121bS. Zenz,14D. Zerwas,114G. Zevi della Porta,56Z. Zhan,32dD. Zhang,32b,hh H. Zhang,87J. Zhang,5X. Zhang,32dZ. Zhang,114L. Zhao,107T. Zhao,137Z. Zhao,32bA. Zhemchugov,64S. Zheng,32a

J. Zhong,117B. Zhou,86N. Zhou,162Y. Zhou,150C. G. Zhu,32dH. Zhu,41J. Zhu,86Y. Zhu,32bX. Zhuang,97 V. Zhuravlov,98D. Zieminska,60R. Zimmermann,20S. Zimmermann,20S. Zimmermann,47M. Ziolkowski,140 R. Zitoun,4L. Zˇ ivkovic´,34V. V. Zmouchko,127,aG. Zobernig,171A. Zoccoli,19a,19bY. Zolnierowski,4A. Zsenei,29

M. zur Nedden,15V. Zutshi,105and L. Zwalinski29

(ATLAS Collaboration) 1

University at Albany, Albany, New York, USA

2Department of Physics, University of Alberta, Edmonton, Alberta, Canada 3aDepartment of Physics, Ankara University, Ankara, Turkey 3bDepartment of Physics, Dumlupinar University, Kutahya, Turkey

3cDepartment of Physics, Gazi University, Ankara, Turkey

3dDivision of Physics, TOBB University of Economics and Technology, Ankara, Turkey 3eTurkish Atomic Energy Authority, Ankara, Turkey

4LAPP, CNRS/IN2P3 and Universite´ de Savoie, Annecy-le-Vieux, France 5High Energy Physics Division, Argonne National Laboratory, Argonne, Illinois, USA

6Department of Physics, University of Arizona, Tucson, Arizona, USA 7Department of Physics, The University of Texas at Arlington, Arlington, Texas, USA

8Physics Department, University of Athens, Athens, Greece

9Physics Department, National Technical University of Athens, Zografou, Greece 10Institute of Physics, Azerbaijan Academy of Sciences, Baku, Azerbaijan

11Institut de Fı´sica d’Altes Energies and Departament de Fı´sica de la Universitat Auto`noma de Barcelona

and ICREA, Barcelona, Spain

12a

Institute of Physics, University of Belgrade, Belgrade, Serbia

12bVinca Institute of Nuclear Sciences, University of Belgrade, Belgrade, Serbia 13Department for Physics and Technology, University of Bergen, Bergen, Norway

14Physics Division, Lawrence Berkeley National Laboratory and University of California, Berkeley, California, USA 15Department of Physics, Humboldt University, Berlin, Germany

16Albert Einstein Center for Fundamental Physics and Laboratory for High Energy Physics, University of Bern, Bern, Switzerland 17School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom

18aDepartment of Physics, Bogazici University, Istanbul, Turkey 18bDivision of Physics, Dogus University, Istanbul, Turkey

Şekil

Figure 1 shows a comparison of the postfit m reco distri-

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