Literature DB >> 25814885

Measurement of the top-quark mass in all-jets [Formula: see text] events in pp collisions at [Formula: see text] TeV.

S Chatrchyan1, V Khachatryan1, A M Sirunyan1, A Tumasyan1, W Adam2, T Bergauer2, M Dragicevic2, J Erö2, C Fabjan2, M Friedl2, R Frühwirth2, V M Ghete2, N Hörmann2, J Hrubec2, M Jeitler2, W Kiesenhofer2, V Knünz2, M Krammer2, I Krätschmer2, D Liko2, I Mikulec2, D Rabady2, B Rahbaran2, C Rohringer2, H Rohringer2, R Schöfbeck2, J Strauss2, A Taurok2, W Treberer-Treberspurg2, W Waltenberger2, C-E Wulz2, V Mossolov3, N Shumeiko3, J Suarez Gonzalez3, S Alderweireldt4, M Bansal4, S Bansal4, T Cornelis4, E A De Wolf4, X Janssen4, A Knutsson4, S Luyckx4, L Mucibello4, S Ochesanu4, B Roland4, R Rougny4, H Van Haevermaet4, P Van Mechelen4, N Van Remortel4, A Van Spilbeeck4, F Blekman5, S Blyweert5, J D'Hondt5, A Kalogeropoulos5, J Keaveney5, M Maes5, A Olbrechts5, S Tavernier5, W Van Doninck5, P Van Mulders5, G P Van Onsem5, I Villella5, B Clerbaux6, G De Lentdecker6, L Favart6, A P R Gay6, T Hreus6, A Léonard6, P E Marage6, A Mohammadi6, L Perniè6, T Reis6, T Seva6, L Thomas6, C Vander Velde6, P Vanlaer6, J Wang16, V Adler7, K Beernaert7, L Benucci7, A Cimmino7, S Costantini7, S Dildick7, G Garcia7, B Klein7, J Lellouch7, A Marinov7, J Mccartin7, A A Ocampo Rios7, D Ryckbosch7, M Sigamani7, N Strobbe7, F Thyssen7, M Tytgat7, S Walsh7, E Yazgan7, N Zaganidis7, S Basegmez8, C Beluffi8, G Bruno8, R Castello8, A Caudron8, L Ceard8, C Delaere8, T du Pree8, D Favart8, L Forthomme8, A Giammanco8, J Hollar8, P Jez8, V Lemaitre8, J Liao8, O Militaru8, C Nuttens8, D Pagano8, A Pin8, K Piotrzkowski8, A Popov8, M Selvaggi8, J M Vizan Garcia1, N Beliy9, T Caebergs9, E Daubie9, G H Hammad9, G A Alves10, M Correa Martins Junior10, T Martins10, M E Pol10, M H G Souza10, W L Aldá Júnior11, W Carvalho11, J Chinellato11, A Custódio11, E M Da Costa11, D De Jesus Damiao11, C De Oliveira Martins11, S Fonseca De Souza11, H Malbouisson11, M Malek11, D Matos Figueiredo11, L Mundim11, H Nogima11, W L Prado Da Silva11, A Santoro11, A Sznajder11, E J Tonelli Manganote11, A Vilela Pereira11, C A Bernardes12, F A Dias13, T R Fernandez Perez Tomei13, E M Gregores12, C Lagana13, F Marinho13, P G Mercadante12, S F Novaes13, Sandra S Padula13, V Genchev14, P Iaydjiev14, S Piperov14, M Rodozov14, G Sultanov14, M Vutova14, A Dimitrov15, R Hadjiiska15, V Kozhuharov15, L Litov15, B Pavlov15, P Petkov15, J G Bian16, G M Chen16, H S Chen16, C H Jiang16, D Liang16, S Liang16, X Meng16, J Tao16, J Wang16, X Wang16, Z Wang16, H Xiao16, M Xu16, C Asawatangtrakuldee17, Y Ban17, Y Guo17, Q Li17, W Li174, S Liu17, Y Mao181, S J Qian17, D Wang17, L Zhang17, W Zou17, C Avila18, C A Carrillo Montoya18, J P Gomez18, B Gomez Moreno18, J C Sanabria18, N Godinovic19, D Lelas19, R Plestina19, D Polic19, I Puljak19, Z Antunovic20, M Kovac20, V Brigljevic21, S Duric21, K Kadija21, J Luetic21, D Mekterovic21, S Morovic21, L Tikvica21, A Attikis22, G Mavromanolakis22, J Mousa22, C Nicolaou22, F Ptochos22, P A Razis22, M Finger23, M Finger23, A A Abdelalim24, Y Assran24, A Ellithi Kamel24, M A Mahmoud24, A Radi24, M Kadastik25, M Müntel25, M Murumaa25, M Raidal25, L Rebane25, A Tiko25, P Eerola26, G Fedi26, M Voutilainen26, J Härkönen27, V Karimäki27, R Kinnunen27, M J Kortelainen27, T Lampén27, K Lassila-Perini27, S Lehti27, T Lindén27, P Luukka27, T Mäenpää27, T Peltola27, E Tuominen27, J Tuominiemi27, E Tuovinen27, L Wendland27, A Korpela28, T Tuuva28, M Besancon29, S Choudhury29, F Couderc29, M Dejardin29, D Denegri29, B Fabbro29, J L Faure29, F Ferri29, S Ganjour29, A Givernaud29, P Gras29, G Hamel de Monchenault29, P Jarry29, E Locci29, J Malcles29, L Millischer29, A Nayak29, J Rander29, A Rosowsky29, M Titov29, S Baffioni30, F Beaudette30, L Benhabib30, L Bianchini30, M Bluj30, P Busson30, C Charlot30, N Daci30, T Dahms30, M Dalchenko30, L Dobrzynski30, A Florent30, R Granier de Cassagnac30, M Haguenauer30, P Miné30, C Mironov30, I N Naranjo30, M Nguyen30, C Ochando30, P Paganini30, D Sabes30, R Salerno30, Y Sirois30, C Veelken30, A Zabi30, J-L Agram31, J Andrea31, D Bloch31, D 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Abstract

The mass of the top quark is measured using a sample of [Formula: see text] candidate events with at least six jets in the final state. The sample is selected from data collected with the CMS detector in pp collisions at [Formula: see text] TeV in 2011 and corresponds to an integrated luminosity of 3.54 [Formula: see text]. The mass is reconstructed for each event employing a kinematic fit of the jets to a [Formula: see text] hypothesis. The top-quark mass is measured to be [Formula: see text] GeV. A combination with previously published measurements in other decay modes by CMS yields a mass of [Formula: see text] GeV.

Entities:  

Year:  2014        PMID: 25814885      PMCID: PMC4370827          DOI: 10.1140/epjc/s10052-014-2758-x

Source DB:  PubMed          Journal:  Eur Phys J C Part Fields        ISSN: 1434-6044            Impact factor:   4.590


Introduction

The mass of the top quark () is an essential parameter of the standard model. Its measurement also provides an important benchmark for the performance and calibration of the Compact Muon Solenoid (CMS) detector [1] at the CERN Large Hadron Collider (LHC). The top-quark mass has been determined with high precision at the Fermilab Tevatron [2] to be  GeV. Measurements have been carried out in several top-quark decay channels using different methods, with the most precise single measurement at the Tevatron being that performed by the CDF Collaboration [3] in the lepton+jets final state using a template method yielding  GeV. In this article a measurement is presented using a sample of candidate events with six or more reconstructed jets in the final state. It represents the first mass measurement in the all-jets channel performed by the CMS Collaboration. The all-jets decay mode has a larger signal yield than the dilepton and lepton+jets channels. However, with only jets in the final state, this channel is dominated by a multijet background and this measurement requires dedicated triggers and tight selection criteria. This measurement complements the latest measurements by the CMS Collaboration in the lepton+jets and dilepton channels that yield  GeV [4] and   GeV [5], respectively. The most precise measurement in the all-jets channel so far is by the CDF Collaboration yielding  GeV [6]. The event selection is very similar to the one used for the CMS cross section measurement in the same final state, requiring at least six jets [7]. Analogously to the CMS measurement of the top-quark mass in the lepton+jets channel [4], the analysis employs a kinematic fit of the decay products to a hypothesis and likelihood functions for each event (“ideograms”) that depend on the top-quark mass only or on both the top-quark mass and the jet energy scale.

CMS detector

The central feature of the CMS apparatus is a superconducting solenoid, of 6 m internal diameter, providing a field of 3.8 T. The bore of the solenoid is equipped with various particle detection systems. CMS uses a right-handed coordinate system, with the origin at the nominal interaction point, the axis pointing to the center of the LHC ring, the axis pointing up (perpendicular to the plane of the LHC ring), and the axis along the counterclockwise-beam direction. The polar angle, , is measured from the positive axis and the azimuthal angle, , is measured in the – plane in radians. Charged-particle trajectories are measured with silicon pixel and strip trackers, covering the pseudorapidity range , where . A lead-tungstate crystal electromagnetic calorimeter (ECAL) and a brass/scintillator hadron calorimeter (HCAL) surround the tracking volume. The HCAL, when combined with the ECAL, measures jets with a resolution . In addition to the barrel and endcap detectors, CMS has extensive forward calorimetry that extends the coverage to . Muons are measured up to using gas-ionization detectors embedded in the steel flux-return yoke outside the solenoid. A two-level trigger system selects the final states pertinent to this analysis. A detailed description of the CMS detector is available elsewhere [1].

Data samples and event selection

The analyzed data sample has been collected in 2011 in pp collisions at  TeV using two different multijet triggers and corresponds to an integrated luminosity of  [8]. The first trigger requires the presence of at least four jets built only from the energies deposited in the calorimeters with transverse momenta  GeV and the presence of a fifth calorimeter jet with  GeV. An additional requirement of a sixth calorimeter jet with  GeV was added during the data taking and this second trigger collected 3.19 fb of data. Our procedure uses simulated events to estimate the composition of the data sample, to determine and calibrate the ideograms, and to evaluate the systematic uncertainties. The signal events have been generated for nine different top-quark mass values ranging from 161.5 to 184.5 GeV with the MAD GRAPH 5.1.1.0 matrix element generator [9], PYTHIA 6.424 parton showering [10] using the Z2 tune [11], and a full GEANT4 [12] simulation of the CMS detector. The matching between the matrix elements (ME) and the parton shower evolution (PS) is done by applying the MLM prescription described in Ref. [13]. The simulation includes the effects of additional overlapping minimum-bias events (pileup) so that the distribution of the number of proton interactions per bunch crossing matches the corresponding distribution in data. Furthermore, the jet energy resolution in simulation has been scaled to match the resolution observed in data [14]. Jets are formed by clustering the particles reconstructed by a particle-flow algorithm [15] using the anti- algorithm [16, 17] with a radius parameter of 0.5. The particle-flow technique combines information from all subdetectors to reconstruct individual particles including muons, electrons, photons, charged hadrons, and neutral hadrons. It typically improves the jet energy resolution to 15 % at 10 GeV, 8 % at 100 GeV, and 4 % at 1 TeV. An additional advantage of this technique is that it facilitates pileup removal by discarding charged particles associated with vertices other than the primary and secondary vertices from the primary collision. Jet energy corrections are applied to all the jets in data and simulation [14]. These corrections are derived from simulation and are defined as a function of the transverse momentum density of an event [17-19] as well as of the and of the reconstructed jet. By these means a uniform energy response at the particle level with low pileup dependence is obtained. A residual correction, measured from the momentum balance of dijet and +jet/Z+jet events, is applied to the jets in data. To reduce the contamination by false jets from detector noise or by electrons reconstructed as jets, the fractions of the jet energy from photons, electrons, and neutral hadrons are required to be below 99 %, and the fraction of the jet energy from charged hadrons is required to be greater than zero. Since hadronically decaying top-quark pairs lead to six quarks in the final state, events are selected with at least four jets with  GeV, a fifth jet with  GeV, and a sixth jet with  GeV. Additional jets are considered only if they have  GeV. All jets are required to be within pseudorapidity of 2.4, where the tracker acceptance ends. The Combined Secondary Vertex tagger with the Tight working point (CSVT) [20] is used to tag jets originating from bottom quarks. The CSVT working point corresponds to an efficiency of approximately 60 %, while the misidentification probability for jets originating from light quarks (uds) and gluons is only 0.1 %. We require at least two b-tagged jets. After these initial event selection criteria, 26,304 candidate events are selected in the data.

Kinematic fit

For the final selection of candidate events, a kinematic least-squares fit [21] is applied. It exploits the characteristic topology of events: two W bosons that can be reconstructed from the untagged jets and two top quarks that can be reconstructed from the W bosons and the b-tagged jets. The reconstructed masses of the two top quarks are constrained to be equal. In addition, the mass of both W bosons in the event is constrained to 80.4 GeV [22] in the fit leading to degrees of freedom. Gaussian resolutions are used for the jet energies in the kinematic fit. They are separately determined for jets originating from light quarks and bottom quarks as functions of and using simulated events. To find the correct combination of jets, the fit procedure is repeated for every experimentally distinguishable jet permutation. This is done using all (six or more) jets that pass the selection. In the data, 8,810 events have exactly seven selected jets, 3,259 events have eight jets, and 1,183 events have nine or more jets. All b-tagged jets are taken as bottom-quark candidates, the untagged jets serve as light-quark candidates. If the fit converges for more than one of the possible jet permutations, the one with the smallest fit is chosen. After the kinematic fit, all events with a goodness-of-fit probability of are accepted. To further reduce the multijet background with production, an additional criterion on the separation of the two bottom-quark candidates, , is imposed. The number of events in data passing each selection step, the expected fraction of signal events in the data sample assuming a cross section of 163pb [23], and the selection efficiency for signal are given in Table 1.
Table 1

Number of events, the predicted signal fraction in the data sample, and the selection efficiency for signal after each selection step. The predicted signal fraction is derived from simulation assuming a cross section of 163 pb [23] and a top-quark mass of 172.5 GeV

Selection stepEventsSig. frac.Sel. eff. for
(%)signal (%)
At least 6 jets786,74133.48
At least two b tags26,304170.91
\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$P_\mathrm{gof} > 0.09$$\end{document}Pgof>0.09 3,691390.30
\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\Delta R_{\mathrm{b}\bar{\mathrm{b}}}$$\end{document}ΔRbb¯ 2,418510.25
Number of events, the predicted signal fraction in the data sample, and the selection efficiency for signal after each selection step. The predicted signal fraction is derived from simulation assuming a cross section of 163 pb [23] and a top-quark mass of 172.5 GeV To extract the mass, the events are weighted by their goodness-of-fit probabilities increasing the fraction of events to  % and improving the resolution of the fitted top-quark mass. We classify the events based on the jet-parton associations in simulation. Partons are matched to a jet if they are separated by less than 0.3 in – space. Three different categories are distinguished in the following way: correct permutations (27.9 %), wrong permutations (22.6 %) where at least one jet is not associated to the correct parton from the decay, and unmatched permutations (49.4 %). The last case contains events in which at least one quark from the decay cannot be matched unambiguously to a selected jet. For correct permutations, the kinematic fit and the weighting procedure improve the resolution of the fitted top-quark masses from 13.6 to 7.9 GeV. Furthermore, the requirement on the goodness-of-fit probability removes 76 % of the signal events classified as unmatched permutations enhancing the fraction of correct permutations from 10 to 27.9 %.

Background modeling

The multijet background is estimated using an event mixing technique. All events after the b-tagging selection are taken as input. The jets are mixed between the different events based on their position in a -ordered list in the event in which they were recorded; every jet in the events in the multijet background model originates from a different event in the data, with the -ordered position preserved. No duplicate jets, in terms of their -ordering, are allowed. In addition, it is required that at least two b-tagged jets are found in every new event. The kinematic fit to a hypothesis is performed on each mixed event and the same and selection is applied. This procedure was validated on particle-level jets using events generated with PYTHIA. The distributions of the fitted top-quark mass and the mean of the two reconstructed W-boson masses agree well between the generated events and the modeled events from event mixing on the same sample. As can be seen in Table 1, the input sample has an expected fraction of 17 % events. The impact of this contamination on the background prediction is evaluated with simulated events and its minor effect on the background modeling is treated as a systematic uncertainty. We normalize the simulated sample and the background prediction to data with an expected signal fraction from simulation. This signal fraction depends on the cross section and the selection efficiency for events for different top-quark masses. It varies between 50 and 55 % for top-quark masses within three standard deviations of the Tevatron average top-quark mass [2] for three different predictions of the cross section [23-25]. Adding to this the uncertainty in the luminosity and the systematic uncertainties in the selection efficiency [7], we assume  % for this analysis. Figure 1 compares data and the expectation from simulation and background for the fitted top-quark mass , the mean of the two reconstructed W-boson masses per event , the goodness-of-fit probability , and the distance between the two b-tagged jets . Overall, the agreement is good within the uncertainties.
Fig. 1

Upper left Reconstructed top-quark mass from the kinematic fit, upper right average reconstructed W-boson mass, lower left goodness-of-fit probability, and lower right the separation of the two b-tagged jets after all selection steps. The simulated signal and the background from event mixing are normalized to data. The band indicates the correlated uncertainty from the signal fraction . The top-quark mass used in the simulation is 172.5 GeV and the nominal jet energy scale is applied

Upper left Reconstructed top-quark mass from the kinematic fit, upper right average reconstructed W-boson mass, lower left goodness-of-fit probability, and lower right the separation of the two b-tagged jets after all selection steps. The simulated signal and the background from event mixing are normalized to data. The band indicates the correlated uncertainty from the signal fraction . The top-quark mass used in the simulation is 172.5 GeV and the nominal jet energy scale is applied

Ideogram method

Since the jet energy scale (JES) is the leading systematic uncertainty in previous top-quark mass measurements, we construct a likelihood function that allows the determination of the JES and the top-quark mass simultaneously by a joint fit to all selected events in data. The JES is estimated from the invariant masses of the jets associated with the W bosons exploiting the precise knowledge of the W-boson mass from previous measurements [22]. Based on this likelihood function, we perform two different estimations of the top-quark mass: one with a fixed JES (henceforth “1D analysis”) and a second with a simultaneous estimation of the JES (henceforth “2D analysis”). The 2D analysis is similar to the measurements of the top-quark mass in the all-jets channel by the CDF Collaboration [6] and in lepton+jets final states by the CMS Collaboration [4]. The observable used for measuring is the top-quark mass obtained from the fitted four-momenta of the jets after the kinematic fit. We take the mean of the two reconstructed W-boson masses before they are constrained by the kinematic fit as an estimator for measuring in situ an additional global JES beyond that of the standard CMS jet energy corrections. The likelihood calculation in the ideogram method [26-28] is done by evaluation of analytic expressions for the probability densities. These expressions are derived and calibrated using simulated events and the modeled background from event mixing. A likelihood to estimate the top-quark mass and JES given the observation of a data sample can be defined as:The event weight is introduced in order to lower the impact of unmatched and background events. The sum of all event weights is normalized to the number of events. Due to the mass constraint on the W boson in the fit, the correlation coefficient between and is only 0.08 for correct permutations in simulation. Hence, we treat and as uncorrelated and the probability from Eq. (1) is factorized intowhere with is the relative fraction of the three different permutation cases. The relative fractions and the probability density functions for signal are determined from simulated events generated for nine different top-quark mass () values and three different JES values (0.96, 1.00, and 1.04). For the probability density functions, the distributions are fitted with a Breit–Wigner function convolved with a Gaussian resolution function for the case and with the sum of a Landau function and a Gaussian function with common means for the and cases for different generated top-quark masses and jet energy scales. The corresponding distributions are distorted by the jet-selection criteria and the goodness-of-fit probability requirement and weighting because permutations with a reconstructed W-boson mass close to  GeV are preferred by the kinematic fit. The distributions are therefore fitted with asymmetric generalized Gaussian functions. The dependence of the parameters of the fitted functions on and JES is then expressed in a linear function of the generated top-quark mass, JES, and the product of the two. As the background is modeled from data, the probability density distributions for the background depend neither on the top-quark mass nor the JES. Its distribution is fitted by the sum of a Gamma function and a Landau function and its distribution by an asymmetric Gaussian function. In the 1D analysis, where the JES is not measured simultaneously, the top-quark mass is estimated from the minimization of . In the 2D analysis the most likely top-quark mass and JES are obtained by minimizing . We fit a parabola (elliptic paraboloid) to extract the minimum and uncertainty from the 1D (2D) log-likelihoods.

Analysis calibration

The method is tested for possible biases and for the correct estimation of the statistical uncertainty using pseudo-experiments. For each combination of nine different generated top-quark masses and three jet energy scales, we conduct 10,000 pseudo-experiments using simulated events and modeled background events from event mixing on data. We extract and from each pseudo-experiment, which corresponds to an integrated luminosity of . This results in 27 calibration points in the - plane. The biases are defined asBoth mass and JES bias are plotted as a function of for all three different JES values in Fig. 2. The bias is fit with a linear function for each generated JES value. Additional small corrections for calibrating the top-quark mass and the jet energy scale are derived as linear functions of both the extracted top-quark mass and JES from these fits. As shown in Fig. 3 (top), no further corrections are needed for the calibrated top-quark mass and for the calibrated jet energy scale .
Fig. 2

Difference between the extracted top-quark mass and the generated top-quark mass , (upper) and between the extracted and generated values of JES (lower) before calibration, for different generated top-quark masses and three different JES values. The lines correspond to linear fits which are used to correct the final likelihoods. The mass points for different JES values are shifted horizontally for clarity

Fig. 3

Top Difference between the calibrated top-quark mass and the generated top-quark mass , and between the calibrated and the generated values of JES after calibration for different generated top-quark masses and three different JES values; bottom width of the pull distribution for the calibrated top-quark mass and for the calibrated JES for different generated top-quark masses and three different JES values. The colored lines (top) correspond to linear fits for individual values of JES and the black line (bottom) corresponds to a constant fit to all calibration points. The mass points for different JES values are shifted horizontally for clarity

Difference between the extracted top-quark mass and the generated top-quark mass , (upper) and between the extracted and generated values of JES (lower) before calibration, for different generated top-quark masses and three different JES values. The lines correspond to linear fits which are used to correct the final likelihoods. The mass points for different JES values are shifted horizontally for clarity Top Difference between the calibrated top-quark mass and the generated top-quark mass , and between the calibrated and the generated values of JES after calibration for different generated top-quark masses and three different JES values; bottom width of the pull distribution for the calibrated top-quark mass and for the calibrated JES for different generated top-quark masses and three different JES values. The colored lines (top) correspond to linear fits for individual values of JES and the black line (bottom) corresponds to a constant fit to all calibration points. The mass points for different JES values are shifted horizontally for clarity Using pseudo-experiments with the calibrated likelihood, we fit a Gaussian function to the distribution of the pulls defined aswhere is the statistical uncertainty in an individual for a pseudo-experiment generated at . As depicted in Fig. 3 (bottom), we find a mass pull width of 1.19, meaning that our method underestimates the statistical uncertainty. We correct for this by dividing by the square of the found mass pull width. From these pseudo-experiments, the statistical uncertainty in the measured top-quark mass is expected to be  GeV for the 1D analysis and  GeV for the 2D analysis.

Systematic uncertainties

An overview of the different sources of systematic uncertainties is shown in Table 2 for the 1D analysis with a fixed JES and the 2D analysis where we estimate the top-quark mass and JES simultaneously. The effect of a source on the efficiency to select events and hence on the signal fraction is taken into account in the evaluation. In general, the largest observed shifts in the top-quark mass and JES when varying the parameters studied are quoted as systematic uncertainties. If the statistical uncertainty in a shift is larger than the observed shift value we quote the statistical uncertainty in the shift instead. The different systematic uncertainties considered as relevant for this measurement and the method to evaluate them are:
Table 2

Overview of systematic uncertainties. The total is defined by adding in quadrature the contributions from all sources, by choosing for each the larger of the estimated shift or its statistical uncertainty, as indicated by the bold script

1D analysis2D analysis
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Jet energy resolution \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\mathbf {0.15} \pm 0.06$$\end{document}0.15±0.06 \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\mathbf {0.13} \pm 0.10$$\end{document}0.13±0.10 \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\mathbf {0.003} \pm 0.001 $$\end{document}0.003±0.001
b tagging \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$0.05 \pm \mathbf {0.06}$$\end{document}0.05±0.06 \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$0.04 \pm \mathbf {0.10}$$\end{document}0.04±0.10 \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\mathbf {0.001} \pm 0.001 $$\end{document}0.001±0.001
Trigger \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\mathbf {0.24} \pm 0.06$$\end{document}0.24±0.06 \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\mathbf {0.26} \pm 0.10$$\end{document}0.26±0.10 \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\mathbf {0.006} \pm 0.001 $$\end{document}0.006±0.001
Pileup \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$0.05 \pm \mathbf {0.06}$$\end{document}0.05±0.06 \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$0.09 \pm \mathbf {0.10}$$\end{document}0.09±0.10 \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\mathbf {0.001} \pm 0.001 $$\end{document}0.001±0.001
Parton distribution functions \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$0.03 \pm \mathbf {0.06}$$\end{document}0.03±0.06 \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$0.07 \pm \mathbf {0.10}$$\end{document}0.07±0.10 \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\mathbf {0.001} \pm 0.001 $$\end{document}0.001±0.001
Renormalization and factorization scale \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$0.08 \pm \mathbf {0.22}$$\end{document}0.08±0.22 \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$0.31 \pm \mathbf {0.34}$$\end{document}0.31±0.34 \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\mathbf {0.005} \pm 0.003 $$\end{document}0.005±0.003
ME-PS matching threshold \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\mathbf {0.24} \pm 0.22$$\end{document}0.24±0.22 \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$0.29 \pm \mathbf {0.34}$$\end{document}0.29±0.34 \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$0.001 \pm \mathbf {0.003} $$\end{document}0.001±0.003
Underlying event \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\mathbf {0.20} \pm 0.12$$\end{document}0.20±0.12 \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\mathbf {0.42} \pm 0.20$$\end{document}0.42±0.20 \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\mathbf {0.004} \pm 0.002 $$\end{document}0.004±0.002
Color reconnection effects \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$0.04 \pm \mathbf {0.15}$$\end{document}0.04±0.15 \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\mathbf {0.58} \pm 0.25$$\end{document}0.58±0.25 \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\mathbf {0.006} \pm 0.002 $$\end{document}0.006±0.002
Multijet background \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\mathbf {0.13} \pm 0.06$$\end{document}0.13±0.06 \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\mathbf {0.60} \pm 0.10$$\end{document}0.60±0.10 \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\mathbf {0.006} \pm 0.001 $$\end{document}0.006±0.001
Total1.211.230.013

The total is defined by adding in quadrature the contributions from all sources, by choosing for each the larger of the estimated shift or its statistical uncertainty, as indicated by the bold script

Fit calibration: We propagate the statistical uncertainty of the calibration to the final measured quantities. Jet energy scale: The effect of the uncertainty in the jet energy corrections is estimated by scaling all jet energies up and down according to their overall uncertainty [14]. The scaling leads to an average JES shift of 1.2 %. We take the largest difference in measured top-quark mass as a systematic uncertainty. The systematic uncertainty in the measured JES for the 2D analysis is obtained by comparing the measured JES for the scaled samples with the expected JES shift of 1.2 %. b-JES: The different energy responses for jets originating from light quarks (uds), bottom quarks, and gluons have been studied in simulation. It is found that the b-jet response is intermediate between the light-quark and gluon jet responses [14]. Hence, the flavor uncertainty assumed for the JES determination [14] to cover the transition from a gluon-dominated to a light-quark-dominated sample also covers the transition from a sample of light quarks to one of bottom quarks. Thus, the energies of all b jets are scaled up and down by this flavor uncertainty in simulation that ranges from 0.2 to 1.2 %. Jet energy resolution: The jet energy resolution in simulation is degraded by 7–20 % depending on to match the resolutions found in [14]. To account for the resolution uncertainty, two additional shifts corresponding to are evaluated. b tagging: The threshold on the CSVT tagger is varied in order to reflect an uncertainty of the b-tag efficiency of 3 % [20]. Trigger: The uncertainty in the turn-on of the jet triggers in data is estimated by raising the jet cuts on the 4th, 5th, and 6th jets separately by 2 GeV in the simulation. Each increase lowers the selection efficiency by 7–10 % covering the uncertainty of 5 % found in a dedicated study for the cross section measurement in this channel [7]. We quote the quadratic sum of the observed shifts in top-quark mass and JES from each increase as systematic uncertainty. Pileup: To estimate the uncertainties associated with the determination of the number of pileup events and with the weighting procedure, the average number of expected pileup events (8.1) is varied by  %. Parton distribution functions: The simulated events have been generated using the CTEQ 6.6L parton distribution functions (PDFs) [29]. The uncertainty in this PDF set is described by up/down variation of 22 orthogonal parameters resulting in 22 pairs of additional PDFs. The events are weighted for agreement with the additional PDFs and half of the difference in top-quark mass and JES of each pair is quoted as systematic uncertainties. The systematic uncertainties stemming from each pair are added in quadrature. Renormalization and factorization scale: The dependence of the result on the renormalization and factorization scale used in the simulation is studied by varying the scale choice for the hard scattering and for parton showering by a factor 0.5 and 2.0. The variation of these parameters in simulation reflects also the uncertainty in the amount of initial state and final state radiation. ME-PS matching threshold: In the simulation, the matching threshold used for interfacing the matrix elements generated with MAD GRAPH and the PYTHIA parton showering is varied by factors of 0.5 and 2.0 compared to the default threshold. Underlying event: Non-perturbative QCD effects are taken into account by tuning PYTHIA to measurements of the underlying event [11]. The uncertainties are estimated by comparing in simulation two tunes with increased and decreased underlying event activities to a central tune (the Perugia 2011 tune to the Perugia 2011 mpiHi and Perugia 2011 Tevatron tunes [30]). Color reconnection effects: The uncertainties that arise from different modeling of color reconnection effects [31] are estimated by comparing in simulation an underlying event tune with color reconnection to a tune without it (the Perugia 2011 and Perugia 2011NoCR tunes [30]). Multijet background: After the final selection, a signal fraction of 54 % is expected from simulation. The signal fraction is varied between 49 and 59 %, corresponding to the uncertainties of the theoretical predictions of the cross section, the value of the top-quark mass, and the luminosity. In addition, we study the effect of events in the input sample used for the event mixing. To estimate the effect, the event mixing is performed in simulation on a sample and alternative probability density distributions are derived from this sample for the background. This variation also accounts for the small shape differences observed for the event mixing technique on the additional sample. Overview of systematic uncertainties. The total is defined by adding in quadrature the contributions from all sources, by choosing for each the larger of the estimated shift or its statistical uncertainty, as indicated by the bold script The total is defined by adding in quadrature the contributions from all sources, by choosing for each the larger of the estimated shift or its statistical uncertainty, as indicated by the bold script As expected, the main systematic uncertainty in the 1D analysis stems from the uncertainty in the jet energy scale and the 2D analysis reduces this uncertainty to a small - and -dependent JES uncertainty, but leads to a larger statistical uncertainty in the measured top-quark mass. Within the statistical precision of the uncertainty evaluation, most other systematic uncertainties are compatible. The variation of the signal fraction contributes 0.11 GeV (0.10 GeV) to the systematic uncertainty on the multijet background in the 1D (2D) analysis justifying that is kept fixed in the likelihood method. However, the 2D analysis has increased uncertainties for color reconnection effects and the shape of the multijet background. Due to the W-boson mass constraint in the kinematic fit, only the color reconnection effects for the b quarks affect the 1D analysis. For the 2D analysis, the JES estimation from the reconstructed W-boson masses results in an additional dependence on color reconnection effects for the light quarks and, hence, an increased systematic uncertainty. Similarly, the additional uncertainty in the modeling of the distribution of the reconstructed W-boson masses for the background gets propagated into the measured top-quark mass for the multijet background uncertainty. Overall, the systematic uncertainties for both methods are very similar in size. This is in contrast to the CMS measurement in the lepton+jets channel [4] where the simultaneous fit of the top-quark mass and the JES leads to a reduction of the systematic uncertainty by 40 %. However, the jets are required to have a higher minimum transverse momentum in the all-jets channel, which leads to a reduced uncertainty in the JES in the 1D analysis compared to the previous work [4]. In addition, the tighter jet criteria in the all-jets measurement have a stronger impact on the distribution, making the JES estimation more sensitive to changes in the simulation.

Results

From the selected 2,418 events we measure with the jet energy scale fixed to the nominal value of JES :The overall uncertainty of the presented 1D analysis is 1.39 GeV. The likelihood profile used in the 1D analysis is shown in Fig. 4 (left).
Fig. 4

Left The 1D likelihood profile with the JES fixed to unity and right the 2D likelihood. The contours correspond to , , and statistical uncertainties

Left The 1D likelihood profile with the JES fixed to unity and right the 2D likelihood. The contours correspond to , , and statistical uncertainties A simultaneous fit of the top-quark mass and JES to the same data yields:The measured JES confirms the JES for particle-flow jets in data measured in events where a Z boson or photon is produced together with one jet [14]. In the 2D analysis the overall uncertainty in the top-quark mass is 1.58 GeV. As the top-quark mass and JES are measured simultaneously, the uncertainty in the top-quark mass combines the statistical uncertainties arising from both components. Figure 4 (right) shows the 2D likelihood obtained from data. The measured top-quark masses in both analyses are in agreement, but the 1D analysis has a better precision than the 2D analysis. We use the Best Linear Unbiased Estimate technique [32] to combine the 1D result presented in this paper with the CMS measurements in the dilepton channel based on 2010 [33] and 2011 [5] data, and the measurement in the lepton+jets channel [4]. Most of the systematic uncertainties listed in Table 2 are assumed to be fully correlated among the four input measurements. Exceptions are the uncertainties in pileup, for which we assign full correlation between the 2011 analyses but no correlation with the 2010 analysis, since the pileup conditions and their treatments differ. In addition, the statistical uncertainty in the in situ fit for the JES and the uncertainties in the mass calibration, the background normalization from control samples in data in the dilepton, and the background prediction in the all-jets analysis are treated as uncorrelated systematic uncertainties. The combination of the four measurements yields a mass of  GeV. It has a of 1.4 for three degrees of freedom, which corresponds to a probability of 71 %. Figure 5 gives an overview of the input measurements and the combined result.
Fig. 5

Overview of the CMS top-quark mass measurements, their combination that is also shown as the shaded band, and the Tevatron average. The inner error bars indicate the statistical uncertainty, the outer error bars indicate the total uncertainty. The statistical uncertainty in the in situ fit for the JES is treated as a systematic uncertainty

Overview of the CMS top-quark mass measurements, their combination that is also shown as the shaded band, and the Tevatron average. The inner error bars indicate the statistical uncertainty, the outer error bars indicate the total uncertainty. The statistical uncertainty in the in situ fit for the JES is treated as a systematic uncertainty

Summary

A measurement of the top-quark mass is presented using events with at least six jets in the final state, collected by CMS in pp collisions at  TeV in 2011. The complete kinematic properties of each event are reconstructed using a constrained fit to a hypothesis. For each selected event a likelihood is calculated as a function of assumed values of the top-quark mass. From a data sample corresponding to an integrated luminosity of , 2,418 candidate events are observed and the mass of the top quark is measured to be . This result for is consistent with the Tevatron average [2], with the ATLAS measurement in the lepton+jets channel [34], and with CMS measurements in the lepton+jets [4] and dilepton [5] channels. To date, this measurement constitutes the most precise determination of the top-quark mass in the all-jets channel. A combination with the three previously published CMS measurements [4, 5, 33] yields a mass of  GeV, consistent with the Tevatron average [2] and with similar precision.
  3 in total

1.  Measurement of the top-quark mass in all-hadronic decays in pp collisions at CDF II.

Authors:  T Aaltonen; A Abulencia; J Adelman; T Affolder; T Akimoto; M G Albrow; D Ambrose; S Amerio; D Amidei; A Anastassov; K Anikeev; A Annovi; J Antos; M Aoki; G Apollinari; J-F Arguin; T Arisawa; A Artikov; W Ashmanskas; A Attal; F Azfar; P Azzi-Bacchetta; P Azzurri; N Bacchetta; W Badgett; A Barbaro-Galtieri; V E Barnes; B A Barnett; S Baroiant; V Bartsch; G Bauer; F Bedeschi; S Behari; S Belforte; G Bellettini; J Bellinger; A Belloni; D Benjamin; A Beretvas; J Beringer; T Berry; A Bhatti; M Binkley; D Bisello; R E Blair; C Blocker; B Blumenfeld; A Bocci; A Bodek; V Boisvert; G Bolla; A Bolshov; D Bortoletto; J Boudreau; A Boveia; B Brau; L Brigliadori; C Bromberg; E Brubaker; J Budagov; H S Budd; S Budd; S Budroni; K Burkett; G Busetto; P Bussey; K L Byrum; S Cabrera; M Campanelli; M Campbell; F Canelli; A Canepa; S Carillo; D Carlsmith; R Carosi; M Casarsa; A Castro; P Catastini; D Cauz; M Cavalli-Sforza; A Cerri; L Cerrito; S H Chang; Y C Chen; M Chertok; G Chiarelli; G Chlachidze; F Chlebana; I Cho; K Cho; D Chokheli; J P Chou; G Choudalakis; S H Chuang; K Chung; W H Chung; Y S Chung; M Ciljak; C I Ciobanu; M A Ciocci; A Clark; D Clark; M Coca; G Compostella; M E Convery; J Conway; B Cooper; K Copic; M Cordelli; G Cortiana; F Crescioli; C Cuenca Almenar; J Cuevas; R Culbertson; J C Cully; D Cyr; S Daronco; M Datta; S D'Auria; T Davies; M D'Onofrio; D Dagenhart; P de Barbaro; S De Cecco; A Deisher; G De Lentdecker; M Dell'orso; F Delli Paoli; L Demortier; J Deng; M Deninno; D De Pedis; P F Derwent; G P Di Giovanni; C Dionisi; B Di Ruzza; J R Dittmann; P Dituro; C Dörr; S Donati; M Donega; P Dong; J Donini; T Dorigo; S Dube; J Efron; R Erbacher; D Errede; S Errede; R Eusebi; H C Fang; S Farrington; I Fedorko; W T Fedorko; R G Feild; M Feindt; J P Fernandez; R Field; G Flanagan; A Foland; S Forrester; G W Foster; M Franklin; J C Freeman; I Furic; M Gallinaro; J Galyardt; J E Garcia; F Garberson; A F Garfinkel; C Gay; H Gerberich; D Gerdes; S Giagu; P Giannetti; A Gibson; K Gibson; J L Gimmell; C Ginsburg; N Giokaris; M Giordani; P Giromini; M Giunta; G Giurgiu; V Glagolev; D Glenzinski; M Gold; N Goldschmidt; J Goldstein; A Golossanov; G Gomez; G Gomez-Ceballos; M Goncharov; O González; I Gorelov; A T Goshaw; K Goulianos; A Gresele; M Griffiths; S Grinstein; C Grosso-Pilcher; U Grundler; J Guimaraes da Costa; Z Gunay-Unalan; C Haber; K Hahn; S R Hahn; E Halkiadakis; A Hamilton; B-Y Han; J Y Han; R Handler; F Happacher; K Hara; M Hare; S Harper; R F Harr; R M Harris; M Hartz; K Hatakeyama; J Hauser; A Heijboer; B Heinemann; J Heinrich; C Henderson; M Herndon; J Heuser; D Hidas; C S Hill; D Hirschbuehl; A Hocker; A Holloway; S Hou; M Houlden; S-C Hsu; B T Huffman; R E Hughes; U Husemann; J Huston; J Incandela; G Introzzi; M Iori; Y Ishizawa; A Ivanov; B Iyutin; E James; D Jang; B Jayatilaka; D Jeans; H Jensen; E J Jeon; S Jindariani; M Jones; K K Joo; S Y Jun; J E Jung; T R Junk; T Kamon; P E Karchin; Y Kato; Y Kemp; R Kephart; U Kerzel; V Khotilovich; B Kilminster; D H Kim; H S Kim; J E Kim; M J Kim; S B Kim; S H Kim; Y K Kim; N Kimura; L Kirsch; S Klimenko; M Klute; B Knuteson; B R Ko; K Kondo; D J Kong; J Konigsberg; A Korytov; A V Kotwal; A Kovalev; A C Kraan; J Kraus; I Kravchenko; M Kreps; J Kroll; N Krumnack; M Kruse; V Krutelyov; T Kubo; S E Kuhlmann; T Kuhr; Y Kusakabe; S Kwang; A T Laasanen; S Lai; S Lami; S Lammel; M Lancaster; R L Lander; K Lannon; A Lath; G Latino; I Lazzizzera; T Lecompte; J Lee; J Lee; Y J Lee; S W Lee; R Lefèvre; N Leonardo; S Leone; S Levy; J D Lewis; C Lin; C S Lin; M Lindgren; E Lipeles; A Lister; D O Litvintsev; T Liu; N S Lockyer; A Loginov; M Loreti; P Loverre; R-S Lu; D Lucchesi; P Lujan; P Lukens; G Lungu; L Lyons; J Lys; R Lysak; E Lytken; P Mack; D MacQueen; R Madrak; K Maeshima; K Makhoul; T Maki; P Maksimovic; S Malde; G Manca; F Margaroli; R Marginean; C Marino; C P Marino; A Martin; M Martin; V Martin; M Martínez; T Maruyama; P Mastrandrea; T Masubuchi; H Matsunaga; M E Mattson; R Mazini; P Mazzanti; K S McFarland; P McIntyre; R McNulty; A Mehta; P Mehtala; S Menzemer; A Menzione; P Merkel; C Mesropian; A Messina; T Miao; N Miladinovic; J Miles; R Miller; C Mills; M Milnik; A Mitra; G Mitselmakher; A Miyamoto; S Moed; N Moggi; B Mohr; R Moore; M Morello; P Movilla Fernandez; J Mülmenstädt; A Mukherjee; Th Muller; R Mumford; P Murat; J Nachtman; A Nagano; J Naganoma; I Nakano; A Napier; V Necula; C Neu; M S Neubauer; J Nielsen; T Nigmanov; L Nodulman; O Norniella; E Nurse; S H Oh; Y D Oh; I Oksuzian; T Okusawa; R Oldeman; R Orava; K Osterberg; C Pagliarone; E Palencia; V Papadimitriou; A A Paramonov; B Parks; S Pashapour; J Patrick; G Pauletta; M Paulini; C Paus; D E Pellett; A Penzo; T J Phillips; G Piacentino; J Piedra; L Pinera; K Pitts; C Plager; L Pondrom; X Portell; O Poukhov; N Pounder; F Prakoshyn; A Pronko; J Proudfoot; F Ptohos; G Punzi; J Pursley; J Rademacker; A Rahaman; N Ranjan; S Rappoccio; B Reisert; V Rekovic; P Renton; M Rescigno; S Richter; F Rimondi; L Ristori; A Robson; T Rodrigo; E Rogers; S Rolli; R Roser; M Rossi; R Rossin; A Ruiz; J Russ; V Rusu; H Saarikko; S Sabik; A Safonov; W K Sakumoto; G Salamanna; O Saltó; D Saltzberg; C Sánchez; L Santi; S Sarkar; L Sartori; K Sato; P Savard; A Savoy-Navarro; T Scheidle; P Schlabach; E E Schmidt; M P Schmidt; M Schmitt; T Schwarz; L Scodellaro; A L Scott; A Scribano; F Scuri; A Sedov; S Seidel; Y Seiya; A Semenov; L Sexton-Kennedy; A Sfyrla; M D Shapiro; T Shears; P F Shepard; D Sherman; M Shimojima; M Shochet; Y Shon; I Shreyber; A Sidoti; P Sinervo; A Sisakyan; J Sjolin; A J Slaughter; J Slaunwhite; K Sliwa; J R Smith; F D Snider; R Snihur; M Soderberg; A Soha; S Somalwar; V Sorin; J Spalding; F Spinella; T Spreitzer; P Squillacioti; M Stanitzki; A Staveris-Polykalas; R St Denis; B Stelzer; O Stelzer-Chilton; D Stentz; J Strologas; D Stuart; J S Suh; A Sukhanov; H Sun; T Suzuki; A Taffard; R Takashima; Y Takeuchi; K Takikawa; M Tanaka; R Tanaka; M Tecchio; P K Teng; K Terashi; J Thom; A S Thompson; E Thomson; P Tipton; V Tiwari; S Tkaczyk; D Toback; S Tokar; K Tollefson; T Tomura; D Tonelli; S Torre; D Torretta; S Tourneur; W Trischuk; R Tsuchiya; S Tsuno; N Turini; F Ukegawa; T Unverhau; S Uozumi; D Usynin; S Vallecorsa; N van Remortel; A Varganov; E Vataga; F Vázquez; G Velev; G Veramendi; V Veszpremi; R Vidal; I Vila; R Vilar; T Vine; I Vollrath; I Volobouev; G Volpi; F Würthwein; P Wagner; R G Wagner; R L Wagner; J Wagner; W Wagner; R Wallny; S M Wang; A Warburton; S Waschke; D Waters; W C Wester; B Whitehouse; D Whiteson; A B Wicklund; E Wicklund; G Williams; H H Williams; P Wilson; B L Winer; P Wittich; S Wolbers; C Wolfe; T Wright; X Wu; S M Wynne; A Yagil; K Yamamoto; J Yamaoka; T Yamashita; C Yang; U K Yang; Y C Yang; W M Yao; G P Yeh; J Yoh; K Yorita; T Yoshida; G B Yu; I Yu; S S Yu; J C Yun; L Zanello; A Zanetti; I Zaw; X Zhang; J Zhou; S Zucchelli
Journal:  Phys Rev Lett       Date:  2007-04-03       Impact factor: 9.161

2.  Precision top-quark mass measurement at CDF.

Authors:  T Aaltonen; B Alvarez González; S Amerio; D Amidei; A Anastassov; A Annovi; J Antos; G Apollinari; J A Appel; T Arisawa; A Artikov; J Asaadi; W Ashmanskas; B Auerbach; A Aurisano; F Azfar; W Badgett; T Bae; A Barbaro-Galtieri; V E Barnes; B A Barnett; P Barria; P Bartos; M Bauce; F Bedeschi; S Behari; G Bellettini; J Bellinger; D Benjamin; A Beretvas; A Bhatti; D Bisello; I Bizjak; K R Bland; B Blumenfeld; A Bocci; A Bodek; D Bortoletto; J Boudreau; A Boveia; L Brigliadori; C Bromberg; E Brucken; J Budagov; H S Budd; K Burkett; G Busetto; P Bussey; A Buzatu; A Calamba; C Calancha; S Camarda; M Campanelli; M Campbell; F Canelli; B Carls; D Carlsmith; R Carosi; S Carrillo; S Carron; B Casal; M Casarsa; A Castro; P Catastini; D Cauz; V Cavaliere; M Cavalli-Sforza; A Cerri; L Cerrito; Y C Chen; M Chertok; G Chiarelli; G Chlachidze; F Chlebana; K Cho; D Chokheli; W H Chung; Y S Chung; M A Ciocci; A Clark; C Clarke; G Compostella; M E Convery; J Conway; M Corbo; M Cordelli; C A Cox; D J Cox; F Crescioli; J Cuevas; R Culbertson; D Dagenhart; N d'Ascenzo; M Datta; P de Barbaro; M Dell'Orso; L Demortier; M Deninno; F Devoto; M d'Errico; A Di Canto; B Di Ruzza; J R Dittmann; M D'Onofrio; S Donati; P Dong; M Dorigo; T Dorigo; K Ebina; A Elagin; A Eppig; R Erbacher; S Errede; N Ershaidat; R Eusebi; S Farrington; M Feindt; J P Fernandez; R Field; G Flanagan; R Forrest; M J Frank; M Franklin; J C Freeman; Y Funakoshi; I Furic; M Gallinaro; J E Garcia; A F Garfinkel; P Garosi; H Gerberich; E Gerchtein; S Giagu; V Giakoumopoulou; P Giannetti; K Gibson; C M Ginsburg; N Giokaris; P Giromini; G Giurgiu; V Glagolev; D Glenzinski; M Gold; D Goldin; N Goldschmidt; A Golossanov; G Gomez; G Gomez-Ceballos; M Goncharov; O González; I Gorelov; A T Goshaw; K Goulianos; S Grinstein; C Grosso-Pilcher; R C Group; J Guimaraes da Costa; S R Hahn; E Halkiadakis; A Hamaguchi; J Y Han; F Happacher; K Hara; D Hare; M Hare; R F Harr; K Hatakeyama; C Hays; M Heck; J Heinrich; M Herndon; S Hewamanage; A Hocker; W Hopkins; D Horn; S Hou; R E Hughes; M Hurwitz; U Husemann; N Hussain; M Hussein; J Huston; G Introzzi; M Iori; A Ivanov; E James; D Jang; B Jayatilaka; E J Jeon; S Jindariani; M Jones; K K Joo; S Y Jun; T R Junk; T Kamon; P E Karchin; A Kasmi; Y Kato; W Ketchum; J Keung; V Khotilovich; B Kilminster; D H Kim; H S Kim; J E Kim; M J Kim; S B Kim; S H Kim; Y K Kim; Y J Kim; N Kimura; M Kirby; S Klimenko; K Knoepfel; K Kondo; D J Kong; J Konigsberg; A V Kotwal; M Kreps; J Kroll; D Krop; M Kruse; V Krutelyov; T Kuhr; M Kurata; S Kwang; A T Laasanen; S Lami; S Lammel; M Lancaster; R L Lander; K Lannon; A Lath; G Latino; T LeCompte; E Lee; H S Lee; J S Lee; S W Lee; S Leo; S Leone; J D Lewis; A Limosani; C-J Lin; M Lindgren; E Lipeles; A Lister; D O Litvintsev; C Liu; H Liu; Q Liu; T Liu; S Lockwitz; A Loginov; D Lucchesi; J Lueck; P Lujan; P Lukens; G Lungu; J Lys; R Lysak; R Madrak; K Maeshima; P Maestro; S Malik; G Manca; A Manousakis-Katsikakis; F Margaroli; C Marino; M Martínez; P Mastrandrea; K Matera; M E Mattson; A Mazzacane; P Mazzanti; K S McFarland; P McIntyre; R McNulty; A Mehta; P Mehtala; C Mesropian; T Miao; D Mietlicki; A Mitra; H Miyake; S Moed; N Moggi; M N Mondragon; C S Moon; R Moore; M J Morello; J Morlock; P Movilla Fernandez; A Mukherjee; Th Muller; P Murat; M Mussini; J Nachtman; Y Nagai; J Naganoma; I Nakano; A Napier; J Nett; C Neu; M S Neubauer; J Nielsen; L Nodulman; S Y Noh; O Norniella; L Oakes; S H Oh; Y D Oh; I Oksuzian; T Okusawa; R Orava; L Ortolan; S Pagan Griso; C Pagliarone; E Palencia; V Papadimitriou; A A Paramonov; J Patrick; G Pauletta; M Paulini; C Paus; D E Pellett; A Penzo; T J Phillips; G Piacentino; E Pianori; J Pilot; K Pitts; C Plager; L Pondrom; S Poprocki; K Potamianos; F Prokoshin; A Pranko; F Ptohos; G Punzi; A Rahaman; V Ramakrishnan; N Ranjan; I Redondo; P Renton; M Rescigno; T Riddick; F Rimondi; L Ristori; A Robson; T Rodrigo; T Rodriguez; E Rogers; S Rolli; R Roser; F Ruffini; A Ruiz; J Russ; V Rusu; A Safonov; W K Sakumoto; Y Sakurai; L Santi; K Sato; V Saveliev; A Savoy-Navarro; P Schlabach; A Schmidt; E E Schmidt; T Schwarz; L Scodellaro; A Scribano; F Scuri; S Seidel; Y Seiya; A Semenov; F Sforza; S Z Shalhout; T Shears; P F Shepard; M Shimojima; M Shochet; I Shreyber-Tecker; A Simonenko; P Sinervo; K Sliwa; J R Smith; F D Snider; A Soha; V Sorin; H Song; P Squillacioti; M Stancari; R St Denis; B Stelzer; O Stelzer-Chilton; D Stentz; J Strologas; G L Strycker; Y Sudo; A Sukhanov; I Suslov; K Takemasa; Y Takeuchi; J Tang; M Tecchio; P K Teng; J Thom; J Thome; G A Thompson; E Thomson; D Toback; S Tokar; K Tollefson; T Tomura; D Tonelli; S Torre; D Torretta; P Totaro; M Trovato; F Ukegawa; S Uozumi; A Varganov; F Vázquez; G Velev; C Vellidis; M Vidal; I Vila; R Vilar; J Vizán; M Vogel; G Volpi; P Wagner; R L Wagner; T Wakisaka; R Wallny; S M Wang; A Warburton; D Waters; W C Wester; D Whiteson; A B Wicklund; E Wicklund; S Wilbur; F Wick; H H Williams; J S Wilson; P Wilson; B L Winer; P Wittich; S Wolbers; H Wolfe; T Wright; X Wu; Z Wu; K Yamamoto; D Yamato; T Yang; U K Yang; Y C Yang; W-M Yao; G P Yeh; K Yi; J Yoh; K Yorita; T Yoshida; G B Yu; I Yu; S S Yu; J C Yun; A Zanetti; Y Zeng; C Zhou; S Zucchelli
Journal:  Phys Rev Lett       Date:  2012-10-09       Impact factor: 9.161

3.  Measurement of the top quark mass with the template method in the [Formula: see text] channel using ATLAS data.

Authors:  G Aad; B Abbott; J Abdallah; A A Abdelalim; A Abdesselam; O Abdinov; B Abi; M Abolins; O S AbouZeid; H Abramowicz; H Abreu; E Acerbi; B S Acharya; L Adamczyk; D L Adams; T N Addy; J Adelman; M Aderholz; S Adomeit; P Adragna; T Adye; S Aefsky; J A Aguilar-Saavedra; M Aharrouche; S P Ahlen; F Ahles; A Ahmad; M Ahsan; G Aielli; T Akdogan; T P A Åkesson; G Akimoto; A V Akimov; A Akiyama; M S Alam; M A Alam; J Albert; S Albrand; M Aleksa; I N Aleksandrov; F Alessandria; C Alexa; G Alexander; G Alexandre; T Alexopoulos; M Alhroob; M Aliev; G Alimonti; J Alison; M Aliyev; B M M Allbrooke; P P Allport; S E Allwood-Spiers; J Almond; A Aloisio; R Alon; A Alonso; B Alvarez Gonzalez; M G Alviggi; K Amako; P Amaral; C Amelung; V V Ammosov; A Amorim; G Amorós; N Amram; C Anastopoulos; L S Ancu; N Andari; T Andeen; C F Anders; G Anders; K J Anderson; A Andreazza; V Andrei; M-L Andrieux; X S Anduaga; A Angerami; F Anghinolfi; A Anisenkov; N Anjos; A Annovi; A Antonaki; M Antonelli; A Antonov; J Antos; F Anulli; S Aoun; L Aperio Bella; R Apolle; G Arabidze; I Aracena; Y Arai; A T H Arce; S Arfaoui; J-F Arguin; E Arik; M Arik; A J Armbruster; O Arnaez; C Arnault; A Artamonov; G Artoni; D Arutinov; S Asai; R Asfandiyarov; S Ask; B Åsman; L Asquith; K Assamagan; A Astbury; A Astvatsatourov; B Aubert; E Auge; K Augsten; M Aurousseau; G Avolio; R Avramidou; D Axen; C Ay; G Azuelos; Y Azuma; M A Baak; G Baccaglioni; C Bacci; A M Bach; H Bachacou; K Bachas; M Backes; M Backhaus; E Badescu; P Bagnaia; S Bahinipati; Y Bai; D C Bailey; T Bain; J T Baines; O K Baker; M D Baker; S Baker; E Banas; P Banerjee; Sw Banerjee; D Banfi; A Bangert; V Bansal; H S Bansil; L Barak; S P Baranov; A Barashkou; A Barbaro Galtieri; T Barber; E L Barberio; D Barberis; M Barbero; D Y Bardin; T Barillari; M Barisonzi; T Barklow; N Barlow; B M Barnett; R M Barnett; A Baroncelli; G Barone; A J Barr; F Barreiro; J Barreiro Guimarães da Costa; P Barrillon; R Bartoldus; A E Barton; V Bartsch; R L Bates; L Batkova; J R Batley; A Battaglia; M Battistin; F Bauer; H S Bawa; S Beale; B Beare; T Beau; P H Beauchemin; R Beccherle; P Bechtle; H P Beck; S Becker; M Beckingham; K H Becks; A J Beddall; A Beddall; S Bedikian; V A Bednyakov; C P Bee; M Begel; S Behar Harpaz; P K Behera; M Beimforde; C Belanger-Champagne; P J Bell; W H Bell; G Bella; L Bellagamba; F Bellina; M Bellomo; A Belloni; O Beloborodova; K Belotskiy; O Beltramello; S Ben Ami; O Benary; D Benchekroun; C Benchouk; M Bendel; N Benekos; Y Benhammou; E Benhar Noccioli; J A Benitez Garcia; D P Benjamin; M Benoit; J R Bensinger; K Benslama; S Bentvelsen; D Berge; E Bergeaas Kuutmann; N Berger; F Berghaus; E Berglund; J Beringer; P Bernat; R Bernhard; C Bernius; T Berry; C Bertella; A Bertin; F Bertinelli; F Bertolucci; M I Besana; N Besson; S Bethke; W Bhimji; R M Bianchi; M Bianco; O Biebel; S P Bieniek; K Bierwagen; J Biesiada; M Biglietti; H Bilokon; M Bindi; S Binet; A Bingul; C Bini; C Biscarat; U Bitenc; K M Black; R E Blair; J-B Blanchard; G Blanchot; T Blazek; C Blocker; J Blocki; A Blondel; W Blum; U Blumenschein; G J Bobbink; V B Bobrovnikov; S S Bocchetta; A Bocci; C R Boddy; M Boehler; J Boek; N Boelaert; J A Bogaerts; A Bogdanchikov; A Bogouch; C Bohm; V Boisvert; T Bold; V Boldea; N M Bolnet; M Bona; V G Bondarenko; M Bondioli; M Boonekamp; C N Booth; S Bordoni; C Borer; A Borisov; G Borissov; I Borjanovic; M Borri; S Borroni; V Bortolotto; K Bos; D Boscherini; M Bosman; H Boterenbrood; D Botterill; J Bouchami; J Boudreau; E V Bouhova-Thacker; D Boumediene; C Bourdarios; N Bousson; A Boveia; J Boyd; I R Boyko; N I Bozhko; I Bozovic-Jelisavcic; J Bracinik; A Braem; P Branchini; G W Brandenburg; A Brandt; G Brandt; O Brandt; U Bratzler; B Brau; J E Brau; H M Braun; B Brelier; J Bremer; R Brenner; S Bressler; D Breton; D Britton; F M Brochu; I Brock; R Brock; T J Brodbeck; E Brodet; F Broggi; C Bromberg; J Bronner; G Brooijmans; W K Brooks; G Brown; H Brown; P A Bruckman de Renstrom; D Bruncko; R Bruneliere; S Brunet; A Bruni; G Bruni; M Bruschi; T Buanes; Q Buat; F Bucci; J Buchanan; N J Buchanan; P Buchholz; R M Buckingham; A G Buckley; S I Buda; I A Budagov; B Budick; V Büscher; L Bugge; O Bulekov; M Bunse; T Buran; H Burckhart; S Burdin; T Burgess; S Burke; E Busato; P Bussey; C P Buszello; F Butin; B Butler; J M Butler; C M Buttar; J M Butterworth; W Buttinger; S Cabrera Urbán; D Caforio; O Cakir; P Calafiura; G Calderini; P Calfayan; R Calkins; L P Caloba; R Caloi; D Calvet; S Calvet; R Camacho Toro; P Camarri; M Cambiaghi; D Cameron; L M Caminada; S Campana; M Campanelli; V Canale; F Canelli; A Canepa; J Cantero; L Capasso; M D M Capeans Garrido; I Caprini; M Caprini; D Capriotti; M Capua; R Caputo; C Caramarcu; R Cardarelli; T Carli; G Carlino; L Carminati; B Caron; S Caron; G D Carrillo Montoya; A A Carter; J R Carter; J Carvalho; D Casadei; M P Casado; M Cascella; C Caso; A M Castaneda Hernandez; E Castaneda-Miranda; V Castillo Gimenez; N F Castro; G Cataldi; F Cataneo; A Catinaccio; J R Catmore; 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S De Cecco; J de Graat; N De Groot; P de Jong; C De La Taille; H De la Torre; B De Lotto; L de Mora; L De Nooij; D De Pedis; A De Salvo; U De Sanctis; A De Santo; J B De Vivie De Regie; S Dean; W J Dearnaley; R Debbe; C Debenedetti; D V Dedovich; J Degenhardt; M Dehchar; C Del Papa; J Del Peso; T Del Prete; T Delemontex; M Deliyergiyev; A Dell'Acqua; L Dell'Asta; M Della Pietra; D Della Volpe; M Delmastro; N Delruelle; P A Delsart; C Deluca; S Demers; M Demichev; B Demirkoz; J Deng; S P Denisov; D Derendarz; J E Derkaoui; F Derue; P Dervan; K Desch; E Devetak; P O Deviveiros; A Dewhurst; B DeWilde; S Dhaliwal; R Dhullipudi; A Di Ciaccio; L Di Ciaccio; A Di Girolamo; B Di Girolamo; S Di Luise; A Di Mattia; B Di Micco; R Di Nardo; A Di Simone; R Di Sipio; M A Diaz; F Diblen; E B Diehl; J Dietrich; T A Dietzsch; S Diglio; K Dindar Yagci; J Dingfelder; C Dionisi; P Dita; S Dita; F Dittus; F Djama; T Djobava; M A B do Vale; A Do Valle Wemans; T K O Doan; M Dobbs; R Dobinson; D Dobos; E Dobson; 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C Fukunaga; E Fullana Torregrosa; J Fuster; C Gabaldon; O Gabizon; T Gadfort; S Gadomski; G Gagliardi; P Gagnon; C Galea; E J Gallas; V Gallo; B J Gallop; P Gallus; K K Gan; Y S Gao; V A Gapienko; A Gaponenko; F Garberson; M Garcia-Sciveres; C García; J E García Navarro; R W Gardner; N Garelli; H Garitaonandia; V Garonne; J Garvey; C Gatti; G Gaudio; B Gaur; L Gauthier; I L Gavrilenko; C Gay; G Gaycken; J-C Gayde; E N Gazis; P Ge; C N P Gee; D A A Geerts; Ch Geich-Gimbel; K Gellerstedt; C Gemme; A Gemmell; M H Genest; S Gentile; M George; S George; P Gerlach; A Gershon; C Geweniger; H Ghazlane; N Ghodbane; B Giacobbe; S Giagu; V Giakoumopoulou; V Giangiobbe; F Gianotti; B Gibbard; A Gibson; S M Gibson; L M Gilbert; V Gilewsky; D Gillberg; A R Gillman; D M Gingrich; J Ginzburg; N Giokaris; M P Giordani; R Giordano; F M Giorgi; P Giovannini; P F Giraud; D Giugni; M Giunta; P Giusti; B K Gjelsten; L K Gladilin; C Glasman; J Glatzer; A Glazov; K W Glitza; G L Glonti; J R Goddard; J Godfrey; 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A Gupta; Y Gusakov; V N Gushchin; P Gutierrez; N Guttman; O Gutzwiller; C Guyot; C Gwenlan; C B Gwilliam; A Haas; S Haas; C Haber; H K Hadavand; D R Hadley; P Haefner; F Hahn; S Haider; Z Hajduk; H Hakobyan; D Hall; J Haller; K Hamacher; P Hamal; M Hamer; A Hamilton; S Hamilton; H Han; L Han; K Hanagaki; K Hanawa; M Hance; C Handel; P Hanke; J R Hansen; J B Hansen; J D Hansen; P H Hansen; P Hansson; K Hara; G A Hare; T Harenberg; S Harkusha; D Harper; R D Harrington; O M Harris; K Harrison; J Hartert; F Hartjes; T Haruyama; A Harvey; S Hasegawa; Y Hasegawa; S Hassani; M Hatch; D Hauff; S Haug; M Hauschild; R Hauser; M Havranek; B M Hawes; C M Hawkes; R J Hawkings; A D Hawkins; D Hawkins; T Hayakawa; T Hayashi; D Hayden; H S Hayward; S J Haywood; E Hazen; M He; S J Head; V Hedberg; L Heelan; S Heim; B Heinemann; S Heisterkamp; L Helary; C Heller; M Heller; S Hellman; D Hellmich; C Helsens; R C W Henderson; M Henke; A Henrichs; A M Henriques Correia; S Henrot-Versille; F Henry-Couannier; 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E B F G Knoops; A Knue; B R Ko; T Kobayashi; M Kobel; M Kocian; P Kodys; K Köneke; A C König; S Koenig; L Köpke; F Koetsveld; P Koevesarki; T Koffas; E Koffeman; L A Kogan; F Kohn; Z Kohout; T Kohriki; T Koi; T Kokott; G M Kolachev; H Kolanoski; V Kolesnikov; I Koletsou; J Koll; D Kollar; M Kollefrath; S D Kolya; A A Komar; Y Komori; T Kondo; T Kono; A I Kononov; R Konoplich; N Konstantinidis; A Kootz; S Koperny; K Korcyl; K Kordas; V Koreshev; A Korn; A Korol; I Korolkov; E V Korolkova; V A Korotkov; O Kortner; S Kortner; V V Kostyukhin; M J Kotamäki; S Kotov; V M Kotov; A Kotwal; C Kourkoumelis; V Kouskoura; A Koutsman; R Kowalewski; T Z Kowalski; W Kozanecki; A S Kozhin; V Kral; V A Kramarenko; G Kramberger; M W Krasny; A Krasznahorkay; J Kraus; J K Kraus; A Kreisel; F Krejci; J Kretzschmar; N Krieger; P Krieger; K Kroeninger; H Kroha; J Kroll; J Kroseberg; J Krstic; U Kruchonak; H Krüger; T Kruker; N Krumnack; Z V Krumshteyn; A Kruth; T Kubota; S Kuday; S Kuehn; A Kugel; T Kuhl; D Kuhn; 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A Marzin; L Masetti; T Mashimo; R Mashinistov; J Masik; A L Maslennikov; I Massa; G Massaro; N Massol; P Mastrandrea; A Mastroberardino; T Masubuchi; M Mathes; P Matricon; H Matsumoto; H Matsunaga; T Matsushita; C Mattravers; J M Maugain; J Maurer; S J Maxfield; D A Maximov; E N May; A Mayne; R Mazini; M Mazur; M Mazzanti; E Mazzoni; S P Mc Kee; A McCarn; R L McCarthy; T G McCarthy; N A McCubbin; K W McFarlane; J A Mcfayden; H McGlone; G Mchedlidze; R A McLaren; T Mclaughlan; S J McMahon; R A McPherson; A Meade; J Mechnich; M Mechtel; M Medinnis; R Meera-Lebbai; T Meguro; R Mehdiyev; S Mehlhase; A Mehta; K Meier; B Meirose; C Melachrinos; B R Mellado Garcia; L Mendoza Navas; Z Meng; A Mengarelli; S Menke; C Menot; E Meoni; K M Mercurio; P Mermod; L Merola; C Meroni; F S Merritt; H Merritt; A Messina; J Metcalfe; A S Mete; C Meyer; C Meyer; J-P Meyer; J Meyer; J Meyer; T C Meyer; W T Meyer; J Miao; S Michal; L Micu; R P Middleton; S Migas; L Mijović; G Mikenberg; M Mikestikova; M Mikuž; D W Miller; R J Miller; W J Mills; C Mills; A Milov; D A Milstead; D Milstein; A A Minaenko; M Miñano Moya; I A Minashvili; A I Mincer; B Mindur; M Mineev; Y Ming; L M Mir; G Mirabelli; L Miralles Verge; A Misiejuk; J Mitrevski; G Y Mitrofanov; V A Mitsou; S Mitsui; P S Miyagawa; K Miyazaki; J U Mjörnmark; T Moa; P Mockett; S Moed; V Moeller; K Mönig; N Möser; S Mohapatra; W Mohr; S Mohrdieck-Möck; A M Moisseev; R Moles-Valls; J Molina-Perez; J Monk; E Monnier; S Montesano; F Monticelli; S Monzani; R W Moore; G F Moorhead; C Mora Herrera; A Moraes; N Morange; J Morel; G Morello; D Moreno; M Moreno Llácer; P Morettini; M Morii; J Morin; A K Morley; G Mornacchi; S V Morozov; J D Morris; L Morvaj; H G Moser; M Mosidze; J Moss; R Mount; E Mountricha; S V Mouraviev; E J W Moyse; M Mudrinic; F Mueller; J Mueller; K Mueller; T A Müller; T Mueller; D Muenstermann; A Muir; Y Munwes; W J Murray; I Mussche; E Musto; A G Myagkov; M Myska; J Nadal; K Nagai; K Nagano; A Nagarkar; Y Nagasaka; M Nagel; A M Nairz; Y Nakahama; K Nakamura; T Nakamura; I Nakano; G Nanava; A Napier; R Narayan; M Nash; N R Nation; T Nattermann; T Naumann; G Navarro; H A Neal; E Nebot; P Yu Nechaeva; T J Neep; A Negri; G Negri; S Nektarijevic; A Nelson; S Nelson; T K Nelson; S Nemecek; P Nemethy; A A Nepomuceno; M Nessi; M S Neubauer; A Neusiedl; R M Neves; P Nevski; P R Newman; V Nguyen Thi Hong; R B Nickerson; R Nicolaidou; L Nicolas; B Nicquevert; F Niedercorn; J Nielsen; T Niinikoski; N Nikiforou; A Nikiforov; V Nikolaenko; K Nikolaev; I Nikolic-Audit; K Nikolics; K Nikolopoulos; H Nilsen; P Nilsson; Y Ninomiya; A Nisati; T Nishiyama; R Nisius; L Nodulman; M Nomachi; I Nomidis; M Nordberg; B Nordkvist; P R Norton; J Novakova; M Nozaki; L Nozka; I M Nugent; A-E Nuncio-Quiroz; G Nunes Hanninger; T Nunnemann; E Nurse; B J O'Brien; S W O'Neale; D C O'Neil; V O'Shea; L B Oakes; F G Oakham; H Oberlack; J Ocariz; A Ochi; S Oda; S Odaka; J Odier; H Ogren; A Oh; S H Oh; C C Ohm; T Ohshima; H Ohshita; T Ohsugi; S Okada; H Okawa; Y Okumura; T Okuyama; A Olariu; M Olcese; A G Olchevski; M Oliveira; D Oliveira Damazio; E Oliver Garcia; D Olivito; A Olszewski; J Olszowska; C Omachi; A Onofre; P U E Onyisi; C J Oram; M J Oreglia; Y Oren; D Orestano; I Orlov; C Oropeza Barrera; R S Orr; B Osculati; R Ospanov; C Osuna; G Otero Y Garzon; J P Ottersbach; M Ouchrif; E A Ouellette; F Ould-Saada; A Ouraou; Q Ouyang; A Ovcharova; M Owen; S Owen; V E Ozcan; N Ozturk; A Pacheco Pages; C Padilla Aranda; S Pagan Griso; E Paganis; F Paige; P Pais; K Pajchel; G Palacino; C P Paleari; S Palestini; D Pallin; A Palma; J D Palmer; Y B Pan; E Panagiotopoulou; B Panes; N Panikashvili; S Panitkin; D Pantea; M Panuskova; V Paolone; A Papadelis; Th D Papadopoulou; A Paramonov; W Park; M A Parker; F Parodi; J A Parsons; U Parzefall; E Pasqualucci; S Passaggio; A Passeri; F Pastore; Fr Pastore; G Pásztor; S Pataraia; N Patel; J R Pater; S Patricelli; T Pauly; M Pecsy; M I Pedraza Morales; S V Peleganchuk; H Peng; R Pengo; A Penson; J Penwell; M Perantoni; K Perez; T Perez Cavalcanti; E Perez Codina; M T Pérez García-Estañ; V Perez Reale; L Perini; H Pernegger; R Perrino; P Perrodo; S Persembe; A Perus; V D Peshekhonov; K Peters; B A Petersen; J Petersen; T C Petersen; E Petit; A Petridis; C Petridou; E Petrolo; F Petrucci; D Petschull; M Petteni; R Pezoa; A Phan; P W Phillips; G Piacquadio; E Piccaro; M Piccinini; S M Piec; R Piegaia; D T Pignotti; J E Pilcher; A D Pilkington; J Pina; M Pinamonti; A Pinder; J L Pinfold; J Ping; B Pinto; O Pirotte; C Pizio; M Plamondon; M-A Pleier; A V Pleskach; A Poblaguev; S Poddar; F Podlyski; L Poggioli; T Poghosyan; M Pohl; F Polci; G Polesello; A Policicchio; A Polini; J Poll; V Polychronakos; D M Pomarede; D Pomeroy; K Pommès; L Pontecorvo; B G Pope; G A Popeneciu; D S Popovic; A Poppleton; X Portell Bueso; C Posch; G E Pospelov; S Pospisil; I N Potrap; C J Potter; C T Potter; G Poulard; J Poveda; R Prabhu; P Pralavorio; A Pranko; S Prasad; R Pravahan; S Prell; K Pretzl; L Pribyl; D Price; J Price; L E Price; M J Price; D Prieur; M Primavera; K Prokofiev; F Prokoshin; S Protopopescu; J Proudfoot; X Prudent; M Przybycien; H Przysiezniak; S Psoroulas; E Ptacek; E Pueschel; J Purdham; M Purohit; P Puzo; Y Pylypchenko; J Qian; Z Qian; Z Qin; A Quadt; D R Quarrie; W B Quayle; F Quinonez; M Raas; V Radescu; B Radics; P Radloff; T Rador; F Ragusa; G Rahal; A M Rahimi; D Rahm; S Rajagopalan; M Rammensee; M Rammes; A S Randle-Conde; K Randrianarivony; P N Ratoff; F Rauscher; M Raymond; A L Read; D M Rebuzzi; A Redelbach; G Redlinger; R Reece; K Reeves; A Reichold; E Reinherz-Aronis; A Reinsch; I Reisinger; D Reljic; C Rembser; Z L Ren; A Renaud; P Renkel; M Rescigno; S Resconi; B Resende; P Reznicek; R Rezvani; A Richards; R Richter; E Richter-Was; M Ridel; M Rijpstra; M Rijssenbeek; A Rimoldi; L Rinaldi; R R Rios; I Riu; G Rivoltella; F Rizatdinova; E Rizvi; S H Robertson; A Robichaud-Veronneau; D Robinson; J E M Robinson; M Robinson; A Robson; J G Rocha de Lima; C Roda; D Roda Dos Santos; D Rodriguez; A Roe; S Roe; O Røhne; V Rojo; S Rolli; A Romaniouk; M Romano; V M Romanov; G Romeo; E Romero Adam; L Roos; E Ros; S Rosati; K Rosbach; A Rose; M Rose; G A Rosenbaum; E I Rosenberg; P L Rosendahl; O Rosenthal; L Rosselet; V Rossetti; E Rossi; L P Rossi; M Rotaru; I Roth; J Rothberg; D Rousseau; C R Royon; A Rozanov; Y Rozen; X Ruan; I Rubinskiy; B Ruckert; N Ruckstuhl; V I Rud; C Rudolph; G Rudolph; F Rühr; F Ruggieri; A Ruiz-Martinez; V Rumiantsev; L Rumyantsev; K Runge; Z Rurikova; N A Rusakovich; D R Rust; J P Rutherfoord; C Ruwiedel; P Ruzicka; Y F Ryabov; V Ryadovikov; P Ryan; M Rybar; G Rybkin; N C Ryder; S Rzaeva; A F Saavedra; I Sadeh; H F-W Sadrozinski; R Sadykov; F Safai Tehrani; H Sakamoto; G Salamanna; A Salamon; M Saleem; D Salihagic; A Salnikov; J Salt; B M Salvachua Ferrando; D Salvatore; F Salvatore; A Salvucci; A Salzburger; D Sampsonidis; B H Samset; A Sanchez; V Sanchez Martinez; H Sandaker; H G Sander; M P Sanders; M Sandhoff; T Sandoval; C Sandoval; R Sandstroem; S Sandvoss; D P C Sankey; A Sansoni; C Santamarina Rios; C Santoni; R Santonico; H Santos; J G Saraiva; T Sarangi; E Sarkisyan-Grinbaum; F Sarri; G Sartisohn; O Sasaki; N Sasao; I Satsounkevitch; G Sauvage; E Sauvan; J B Sauvan; P Savard; V Savinov; D O Savu; L Sawyer; D H Saxon; L P Says; C Sbarra; A Sbrizzi; O Scallon; D A Scannicchio; M Scarcella; J Schaarschmidt; P Schacht; U Schäfer; S Schaepe; S Schaetzel; A C Schaffer; D Schaile; R D Schamberger; A G Schamov; V Scharf; V A Schegelsky; D Scheirich; M Schernau; M I Scherzer; C Schiavi; J Schieck; M Schioppa; S Schlenker; J L Schlereth; E Schmidt; K Schmieden; C Schmitt; S Schmitt; M Schmitz; A Schöning; M Schott; D Schouten; J Schovancova; M Schram; C Schroeder; N Schroer; S Schuh; G Schuler; M J Schultens; J Schultes; H-C Schultz-Coulon; H Schulz; J W Schumacher; M Schumacher; B A Schumm; Ph Schune; C Schwanenberger; A Schwartzman; Ph Schwemling; R Schwienhorst; R Schwierz; J Schwindling; T Schwindt; M Schwoerer; W G Scott; J Searcy; G Sedov; E Sedykh; E Segura; S C Seidel; A Seiden; F Seifert; J M Seixas; G Sekhniaidze; K E Selbach; D M Seliverstov; B Sellden; G Sellers; M Seman; N Semprini-Cesari; C Serfon; L Serin; L Serkin; R Seuster; H Severini; M E Sevior; A Sfyrla; E Shabalina; M Shamim; L Y Shan; J T Shank; Q T Shao; M Shapiro; P B Shatalov; L Shaver; K Shaw; D Sherman; P Sherwood; A Shibata; H Shichi; S Shimizu; M Shimojima; T Shin; M Shiyakova; A Shmeleva; M J Shochet; D Short; S Shrestha; E Shulga; M A Shupe; P Sicho; A Sidoti; F Siegert; Dj Sijacki; O Silbert; J Silva; Y Silver; D Silverstein; S B Silverstein; V Simak; O Simard; Lj Simic; S Simion; B Simmons; M Simonyan; P Sinervo; N B Sinev; V Sipica; G Siragusa; A Sircar; A N Sisakyan; S Yu Sivoklokov; J Sjölin; T B Sjursen; L A Skinnari; H P Skottowe; K Skovpen; P Skubic; N Skvorodnev; M Slater; T Slavicek; K Sliwa; J Sloper; V Smakhtin; S Yu Smirnov; Y Smirnov; L N Smirnova; O Smirnova; B C Smith; D Smith; K M Smith; M Smizanska; K Smolek; A A Snesarev; S W Snow; J Snow; J Snuverink; S Snyder; M Soares; R Sobie; J Sodomka; A Soffer; C A Solans; M Solar; J Solc; E Soldatov; U Soldevila; E Solfaroli Camillocci; A A Solodkov; O V Solovyanov; N Soni; V Sopko; B Sopko; M Sosebee; R Soualah; A Soukharev; S Spagnolo; F Spanò; R Spighi; G Spigo; F Spila; R Spiwoks; M Spousta; T Spreitzer; B Spurlock; R D St Denis; J Stahlman; R Stamen; E Stanecka; R W Stanek; C Stanescu; S Stapnes; E A Starchenko; J Stark; P Staroba; P Starovoitov; A Staude; P Stavina; G Stavropoulos; G Steele; P Steinbach; P Steinberg; I Stekl; B Stelzer; H J Stelzer; O Stelzer-Chilton; H Stenzel; S Stern; K Stevenson; G A Stewart; J A Stillings; M C Stockton; K Stoerig; G Stoicea; S Stonjek; P Strachota; A R Stradling; A Straessner; J Strandberg; S Strandberg; A Strandlie; M Strang; E Strauss; M Strauss; P Strizenec; R Ströhmer; D M Strom; J A Strong; R Stroynowski; J Strube; B Stugu; I Stumer; J Stupak; P Sturm; N A Styles; D A Soh; D Su; Hs Subramania; A Succurro; Y Sugaya; T Sugimoto; C Suhr; K Suita; M Suk; V V Sulin; S Sultansoy; T Sumida; X Sun; J E Sundermann; K Suruliz; S Sushkov; G Susinno; M R Sutton; Y Suzuki; Y Suzuki; M Svatos; Yu M Sviridov; S Swedish; I Sykora; T Sykora; B Szeless; J Sánchez; D Ta; K Tackmann; A Taffard; R Tafirout; N Taiblum; Y Takahashi; H Takai; R Takashima; H Takeda; T Takeshita; Y Takubo; M Talby; A Talyshev; M C Tamsett; J Tanaka; R Tanaka; S Tanaka; S Tanaka; Y Tanaka; A J Tanasijczuk; K Tani; N Tannoury; G P Tappern; S Tapprogge; D Tardif; S Tarem; F Tarrade; G F Tartarelli; P Tas; M Tasevsky; E Tassi; M Tatarkhanov; Y Tayalati; C Taylor; F E Taylor; G N Taylor; W Taylor; M Teinturier; M Teixeira Dias Castanheira; P Teixeira-Dias; K K Temming; H Ten Kate; P K Teng; S Terada; K Terashi; J Terron; M Testa; R J Teuscher; J Thadome; J Therhaag; T Theveneaux-Pelzer; M Thioye; S Thoma; J P Thomas; E N Thompson; P D Thompson; P D Thompson; A S Thompson; E Thomson; M Thomson; R P Thun; F Tian; M J Tibbetts; T Tic; V O Tikhomirov; Y A Tikhonov; S Timoshenko; P Tipton; F J Tique Aires Viegas; S Tisserant; B Toczek; T Todorov; S Todorova-Nova; B Toggerson; J Tojo; S Tokár; K Tokunaga; K Tokushuku; K Tollefson; M Tomoto; L Tompkins; K Toms; G Tong; A Tonoyan; C Topfel; N D Topilin; I Torchiani; E Torrence; H Torres; E Torró Pastor; J Toth; F Touchard; D R Tovey; T Trefzger; L Tremblet; A Tricoli; I M Trigger; S Trincaz-Duvoid; T N Trinh; M F Tripiana; W Trischuk; A Trivedi; B Trocmé; C Troncon; M Trottier-McDonald; M Trzebinski; A Trzupek; C Tsarouchas; J C-L Tseng; M Tsiakiris; P V Tsiareshka; D Tsionou; G Tsipolitis; V Tsiskaridze; E G Tskhadadze; I I Tsukerman; V Tsulaia; J-W Tsung; S Tsuno; D Tsybychev; A Tua; A Tudorache; V Tudorache; J M Tuggle; M Turala; D Turecek; I Turk Cakir; E Turlay; R Turra; P M Tuts; A Tykhonov; M Tylmad; M Tyndel; G Tzanakos; K Uchida; I Ueda; R Ueno; M Ugland; M Uhlenbrock; M Uhrmacher; F Ukegawa; G Unal; D G Underwood; A Undrus; G Unel; Y Unno; D Urbaniec; G Usai; M Uslenghi; L Vacavant; V Vacek; B Vachon; S Vahsen; J Valenta; P Valente; S Valentinetti; S Valkar; E Valladolid Gallego; S Vallecorsa; J A Valls Ferrer; H van der Graaf; E van der Kraaij; R Van Der Leeuw; E van der Poel; D van der Ster; N van Eldik; P van Gemmeren; Z van Kesteren; I van Vulpen; M Vanadia; W Vandelli; G Vandoni; A Vaniachine; P Vankov; F Vannucci; F Varela Rodriguez; R Vari; E W Varnes; D Varouchas; A Vartapetian; K E Varvell; V I Vassilakopoulos; F Vazeille; G Vegni; J J Veillet; C Vellidis; F Veloso; R Veness; S Veneziano; A Ventura; D Ventura; M Venturi; N Venturi; V Vercesi; M Verducci; W Verkerke; J C Vermeulen; A Vest; M C Vetterli; I Vichou; T Vickey; O E Vickey Boeriu; G H A Viehhauser; S Viel; M Villa; M Villaplana Perez; E Vilucchi; M G Vincter; E Vinek; V B Vinogradov; M Virchaux; J Virzi; O Vitells; M Viti; I Vivarelli; F Vives Vaque; S Vlachos; D Vladoiu; M Vlasak; N Vlasov; A Vogel; P Vokac; G Volpi; M Volpi; G Volpini; H von der Schmitt; J von Loeben; H von Radziewski; E von Toerne; V Vorobel; A P Vorobiev; V Vorwerk; M Vos; R Voss; T T Voss; J H Vossebeld; N Vranjes; M Vranjes Milosavljevic; V Vrba; M Vreeswijk; T Vu Anh; R Vuillermet; I Vukotic; W Wagner; P Wagner; H Wahlen; J Wakabayashi; J Walbersloh; S Walch; J Walder; R Walker; W Walkowiak; R Wall; P Waller; C Wang; H Wang; H Wang; J Wang; J Wang; J C Wang; R Wang; S M Wang; A Warburton; C P Ward; M Warsinsky; P M Watkins; A T Watson; I J Watson; M F Watson; G Watts; S Watts; A T Waugh; B M Waugh; M Weber; M S Weber; P Weber; A R Weidberg; P Weigell; J Weingarten; C Weiser; H Wellenstein; P S Wells; M Wen; T Wenaus; S Wendler; Z Weng; T Wengler; S Wenig; N Wermes; M Werner; P Werner; M Werth; M Wessels; C Weydert; K Whalen; S J Wheeler-Ellis; S P Whitaker; A White; M J White; S R Whitehead; D Whiteson; D Whittington; F Wicek; D Wicke; F J Wickens; W Wiedenmann; M Wielers; P Wienemann; C Wiglesworth; L A M Wiik-Fuchs; P A Wijeratne; A Wildauer; M A Wildt; I Wilhelm; H G Wilkens; J Z Will; E Williams; H H Williams; W Willis; S Willocq; J A Wilson; M G Wilson; A Wilson; I Wingerter-Seez; S Winkelmann; F Winklmeier; M Wittgen; M W Wolter; H Wolters; W C Wong; G Wooden; B K Wosiek; J Wotschack; M J Woudstra; K W Wozniak; K Wraight; C Wright; M Wright; B Wrona; S L Wu; X Wu; Y Wu; E Wulf; R Wunstorf; B M Wynne; S Xella; M Xiao; S Xie; Y Xie; C Xu; D Xu; G Xu; B Yabsley; S Yacoob; M Yamada; H Yamaguchi; A Yamamoto; K Yamamoto; S Yamamoto; T Yamamura; T Yamanaka; J Yamaoka; T Yamazaki; Y Yamazaki; Z Yan; H Yang; U K Yang; Y Yang; Y Yang; Z Yang; S Yanush; Y Yao; Y Yasu; G V Ybeles Smit; J Ye; S Ye; M Yilmaz; R Yoosoofmiya; K Yorita; R Yoshida; C Young; S Youssef; D Yu; J Yu; J Yu; L Yuan; A Yurkewicz; B Zabinski; V G Zaets; R Zaidan; A M Zaitsev; Z Zajacova; L Zanello; P Zarzhitsky; A Zaytsev; C Zeitnitz; M Zeller; M Zeman; A Zemla; C Zendler; O Zenin; T Ženiš; Z Zinonos; S Zenz; D Zerwas; G Zevi Della Porta; Z Zhan; D Zhang; H Zhang; J Zhang; X Zhang; Z Zhang; L Zhao; T Zhao; Z Zhao; A Zhemchugov; S Zheng; J Zhong; B Zhou; N Zhou; Y Zhou; C G Zhu; H Zhu; J Zhu; Y Zhu; X Zhuang; V Zhuravlov; D Zieminska; R Zimmermann; S Zimmermann; S Zimmermann; M Ziolkowski; R Zitoun; L Živković; V V Zmouchko; G Zobernig; A Zoccoli; Y Zolnierowski; A Zsenei; M Zur Nedden; V Zutshi; L Zwalinski
Journal:  Eur Phys J C Part Fields       Date:  2012-06-21       Impact factor: 4.590

  3 in total
  4 in total

1.  Measurement of the [Formula: see text] production cross section in the all-jets final state in pp collisions at [Formula: see text][Formula: see text].

Authors:  V Khachatryan; A M Sirunyan; A Tumasyan; W Adam; E Asilar; T Bergauer; J Brandstetter; E Brondolin; M Dragicevic; J Erö; M Friedl; R Frühwirth; V M Ghete; C Hartl; N Hörmann; J Hrubec; M Jeitler; V Knünz; A König; M Krammer; I Krätschmer; D Liko; T Matsushita; I Mikulec; D Rabady; B Rahbaran; H Rohringer; J Schieck; R Schöfbeck; J Strauss; W Treberer-Treberspurg; W Waltenberger; C-E Wulz; V Mossolov; N Shumeiko; J Suarez Gonzalez; S Alderweireldt; T Cornelis; E A De Wolf; X Janssen; A Knutsson; J Lauwers; S Luyckx; M Van De Klundert; H Van Haevermaet; P Van Mechelen; N Van Remortel; A Van Spilbeeck; S Abu Zeid; F Blekman; J D'Hondt; N Daci; I De Bruyn; K Deroover; N Heracleous; J Keaveney; S Lowette; L Moreels; A Olbrechts; Q Python; D Strom; S Tavernier; W Van Doninck; P Van Mulders; G P Van Onsem; I Van Parijs; P Barria; H Brun; C Caillol; B Clerbaux; G De Lentdecker; G Fasanella; L Favart; A Grebenyuk; G Karapostoli; T Lenzi; A Léonard; T Maerschalk; A Marinov; L Perniè; A Randle-Conde; T Reis; T Seva; C Vander Velde; R Yonamine; P Vanlaer; R Yonamine; F Zenoni; F Zhang; V Adler; K Beernaert; L Benucci; A Cimmino; S Crucy; D Dobur; A Fagot; G Garcia; M Gul; J Mccartin; A A Ocampo Rios; D Poyraz; D Ryckbosch; S Salva; M Sigamani; N Strobbe; M Tytgat; W Van Driessche; E Yazgan; N Zaganidis; S Basegmez; C Beluffi; O Bondu; S Brochet; G Bruno; A Caudron; L Ceard; G G Da Silveira; C Delaere; D Favart; L Forthomme; A Giammanco; J Hollar; A Jafari; P Jez; M Komm; V Lemaitre; A Mertens; C Nuttens; L Perrini; A Pin; K Piotrzkowski; A Popov; L Quertenmont; M Selvaggi; M Vidal Marono; N Beliy; G H Hammad; W L Aldá Júnior; F L Alves; G A Alves; L Brito; M Correa Martins Junior; M Hamer; C Hensel; C Mora Herrera; A Moraes; M E Pol; P Rebello Teles; E Belchior Batista Das Chagas; W Carvalho; J Chinellato; A Custódio; E M Da Costa; D De Jesus Damiao; C De Oliveira Martins; S Fonseca De Souza; L M Huertas Guativa; H Malbouisson; D Matos Figueiredo; L Mundim; H Nogima; W L Prado Da Silva; A Santoro; A Sznajder; E J Tonelli Manganote; A Vilela Pereira; S Ahuja; C A Bernardes; A De Souza Santos; S Dogra; T R Fernandez Perez Tomei; E M Gregores; P G Mercadante; C S Moon; S F Novaes; Sandra S Padula; D Romero Abad; J C Ruiz Vargas; A Aleksandrov; R Hadjiiska; P Iaydjiev; M Rodozov; S Stoykova; G Sultanov; M Vutova; A Dimitrov; I Glushkov; L Litov; B Pavlov; P Petkov; M Ahmad; J G Bian; G M Chen; H S Chen; M Chen; T Cheng; R Du; C H Jiang; R Plestina; F Romeo; S M Shaheen; J Tao; C Wang; Z Wang; H Zhang; C Asawatangtrakuldee; Y Ban; Q Li; S Liu; Y Mao; S J Qian; D Wang; Z Xu; C Avila; A Cabrera; L F Chaparro Sierra; C Florez; J P Gomez; B Gomez Moreno; J C Sanabria; N Godinovic; D Lelas; I Puljak; P M Ribeiro Cipriano; Z Antunovic; M Kovac; V Brigljevic; K Kadija; J Luetic; S Micanovic; L Sudic; A Attikis; G Mavromanolakis; J Mousa; C Nicolaou; F Ptochos; P A Razis; H Rykaczewski; M Bodlak; M Finger; M Finger; A A Abdelalim; A Awad; M El Sawy; A Mahrous; A Radi; B Calpas; M Kadastik; 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N Lychkovskaya; V Popov; L Pozdnyakov; G Safronov; A Spiridonov; E Vlasov; A Zhokin; A Bylinkin; V Andreev; M Azarkin; I Dremin; M Kirakosyan; A Leonidov; G Mesyats; S V Rusakov; A Baskakov; A Belyaev; E Boos; V Bunichev; M Dubinin; L Dudko; A Ershov; A Gribushin; V Klyukhin; N Korneeva; I Lokhtin; I Myagkov; S Obraztsov; M Perfilov; V Savrin; I Azhgirey; I Bayshev; S Bitioukov; V Kachanov; A Kalinin; D Konstantinov; V Krychkine; V Petrov; R Ryutin; A Sobol; L Tourtchanovitch; S Troshin; N Tyurin; A Uzunian; A Volkov; P Adzic; J Milosevic; V Rekovic; J Alcaraz Maestre; C Battilana; E Calvo; M Cerrada; M Chamizo Llatas; N Colino; B De La Cruz; A Delgado Peris; D Domínguez Vázquez; A Escalante Del Valle; C Fernandez Bedoya; J P Fernández Ramos; J Flix; M C Fouz; P Garcia-Abia; O Gonzalez Lopez; S Goy Lopez; J M Hernandez; M I Josa; E Navarro De Martino; A Pérez-Calero Yzquierdo; J Puerta Pelayo; A Quintario Olmeda; I Redondo; L Romero; J Santaolalla; M S Soares; C Albajar; J F de Trocóniz; 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Journal:  Eur Phys J C Part Fields       Date:  2016-03-08       Impact factor: 4.590

2.  Measurement of the top-quark mass in the fully hadronic decay channel from ATLAS data at [Formula: see text].

Authors:  G Aad; B Abbott; J Abdallah; S Abdel Khalek; O Abdinov; R Aben; B Abi; M Abolins; O S AbouZeid; H Abramowicz; H Abreu; R Abreu; Y Abulaiti; B S Acharya; L Adamczyk; D L Adams; J Adelman; S Adomeit; T Adye; T Agatonovic-Jovin; J A Aguilar-Saavedra; M Agustoni; S P Ahlen; F Ahmadov; G Aielli; H Akerstedt; T P A Åkesson; G Akimoto; A V Akimov; G L Alberghi; J Albert; S Albrand; M J Alconada Verzini; M Aleksa; I N Aleksandrov; C Alexa; G Alexander; G Alexandre; T Alexopoulos; M Alhroob; G Alimonti; L Alio; J Alison; B M M Allbrooke; L J Allison; P P Allport; J Almond; A Aloisio; A Alonso; F Alonso; C Alpigiani; A Altheimer; B Alvarez Gonzalez; M G Alviggi; K Amako; Y Amaral Coutinho; C Amelung; D Amidei; S P Amor Dos Santos; A Amorim; S Amoroso; N Amram; G Amundsen; C Anastopoulos; L S Ancu; N Andari; T Andeen; C F Anders; G Anders; K J Anderson; A Andreazza; V Andrei; X S Anduaga; S Angelidakis; I Angelozzi; P Anger; A Angerami; F Anghinolfi; A V Anisenkov; N Anjos; A Annovi; A Antonaki; M Antonelli; A Antonov; J Antos; F Anulli; M Aoki; L Aperio Bella; R Apolle; G Arabidze; I Aracena; Y Arai; J P Araque; A T H Arce; J-F Arguin; S Argyropoulos; M Arik; A J Armbruster; O Arnaez; V Arnal; H Arnold; M Arratia; O Arslan; A Artamonov; G Artoni; S Asai; N Asbah; A Ashkenazi; B Åsman; L Asquith; K Assamagan; R Astalos; M Atkinson; N B Atlay; B Auerbach; K Augsten; M Aurousseau; G Avolio; G Azuelos; Y Azuma; M A Baak; A E Baas; C Bacci; H Bachacou; K Bachas; M Backes; M Backhaus; J Backus Mayes; E Badescu; P Bagiacchi; P Bagnaia; Y Bai; T Bain; J T Baines; O K Baker; P Balek; F Balli; E Banas; Sw Banerjee; A A E Bannoura; V Bansal; H S Bansil; L Barak; S P Baranov; E L Barberio; D Barberis; M Barbero; T Barillari; M Barisonzi; T Barklow; N Barlow; B M Barnett; R M Barnett; Z Barnovska; A Baroncelli; G Barone; A J Barr; F Barreiro; J Barreiro Guimarães da Costa; R Bartoldus; A E Barton; P Bartos; V Bartsch; A Bassalat; A Basye; R L Bates; J R Batley; M Battaglia; M Battistin; F Bauer; H S Bawa; M D Beattie; T Beau; P H Beauchemin; R Beccherle; P Bechtle; H P Beck; K Becker; S Becker; M Beckingham; C Becot; A J Beddall; A Beddall; S Bedikian; V A Bednyakov; C P Bee; L J Beemster; T A Beermann; M Begel; K Behr; C Belanger-Champagne; P J Bell; W H Bell; G Bella; L Bellagamba; A Bellerive; M Bellomo; K Belotskiy; O Beltramello; O Benary; D Benchekroun; K Bendtz; N Benekos; Y Benhammou; E Benhar Noccioli; J A Benitez Garcia; D P Benjamin; J R Bensinger; K Benslama; S Bentvelsen; D Berge; E Bergeaas Kuutmann; N Berger; F Berghaus; J Beringer; C Bernard; P Bernat; C Bernius; F U Bernlochner; T Berry; P Berta; C Bertella; G Bertoli; F Bertolucci; C Bertsche; D Bertsche; M I Besana; G J Besjes; O Bessidskaia Bylund; M Bessner; N Besson; C Betancourt; S Bethke; W Bhimji; R M Bianchi; L Bianchini; M Bianco; O Biebel; S P Bieniek; K Bierwagen; J Biesiada; M Biglietti; J Bilbao De Mendizabal; H Bilokon; M Bindi; S Binet; A Bingul; C Bini; C W Black; J E Black; K M Black; D Blackburn; R E Blair; J-B Blanchard; T Blazek; I Bloch; C Blocker; W Blum; U Blumenschein; G J Bobbink; V S Bobrovnikov; S S Bocchetta; A Bocci; C Bock; C R Boddy; M Boehler; T T Boek; J A Bogaerts; A G Bogdanchikov; A Bogouch; C Bohm; J Bohm; V Boisvert; T Bold; V Boldea; A S Boldyrev; M Bomben; M Bona; M Boonekamp; A Borisov; G Borissov; M Borri; S Borroni; J Bortfeldt; V Bortolotto; K Bos; D Boscherini; M Bosman; H Boterenbrood; J Boudreau; J Bouffard; E V Bouhova-Thacker; D Boumediene; C Bourdarios; N Bousson; S Boutouil; A Boveia; J Boyd; I R Boyko; J Bracinik; A Brandt; G Brandt; O Brandt; U Bratzler; B Brau; J E Brau; H M Braun; S F Brazzale; B Brelier; K Brendlinger; A J Brennan; R Brenner; S Bressler; K Bristow; T M Bristow; D Britton; F M Brochu; I Brock; R Brock; C Bromberg; J Bronner; G Brooijmans; T Brooks; W K Brooks; J Brosamer; E Brost; J Brown; P A Bruckman de Renstrom; D Bruncko; R Bruneliere; S Brunet; A Bruni; G Bruni; M Bruschi; L Bryngemark; T Buanes; Q Buat; F Bucci; P Buchholz; R M Buckingham; A G Buckley; S I Buda; I A Budagov; F Buehrer; L Bugge; M K Bugge; O Bulekov; A C Bundock; H Burckhart; S Burdin; B Burghgrave; S Burke; I Burmeister; E Busato; D Büscher; V Büscher; P Bussey; C P Buszello; B Butler; J M Butler; A I Butt; C M Buttar; J M Butterworth; P Butti; W Buttinger; A Buzatu; M Byszewski; S Cabrera Urbán; D Caforio; O Cakir; P Calafiura; A Calandri; G Calderini; P Calfayan; R Calkins; L P Caloba; D Calvet; S Calvet; R Camacho Toro; S Camarda; D Cameron; L M Caminada; R Caminal Armadans; S Campana; M Campanelli; A Campoverde; V Canale; A Canepa; M Cano Bret; J Cantero; R Cantrill; T Cao; M D M Capeans Garrido; I Caprini; M Caprini; M Capua; R Caputo; R Cardarelli; T Carli; G Carlino; L Carminati; S Caron; E Carquin; G D Carrillo-Montoya; J R Carter; J Carvalho; D Casadei; M P Casado; M Casolino; E Castaneda-Miranda; A Castelli; V Castillo Gimenez; N F Castro; P Catastini; A Catinaccio; J R Catmore; A Cattai; G Cattani; J Caudron; S Caughron; V Cavaliere; D Cavalli; M Cavalli-Sforza; V Cavasinni; F Ceradini; B C Cerio; K Cerny; A S Cerqueira; A Cerri; L Cerrito; F Cerutti; M Cerv; A Cervelli; S A Cetin; A Chafaq; D Chakraborty; I Chalupkova; P Chang; B Chapleau; J D Chapman; D Charfeddine; D G Charlton; C C Chau; C A Chavez Barajas; S Cheatham; A Chegwidden; S Chekanov; S V Chekulaev; G A Chelkov; M A Chelstowska; C Chen; H Chen; K Chen; L Chen; S Chen; X Chen; Y Chen; Y Chen; H C Cheng; Y Cheng; A Cheplakov; R Cherkaoui El Moursli; V Chernyatin; E Cheu; L Chevalier; V Chiarella; G Chiefari; J T Childers; A Chilingarov; G Chiodini; A S Chisholm; R T Chislett; A Chitan; M V Chizhov; S Chouridou; B K B Chow; D Chromek-Burckhart; M L Chu; J Chudoba; J J Chwastowski; L Chytka; G Ciapetti; A K Ciftci; R Ciftci; D Cinca; V Cindro; A Ciocio; P Cirkovic; Z H Citron; M Citterio; M Ciubancan; A Clark; P J Clark; R N Clarke; W Cleland; J C Clemens; C Clement; Y Coadou; M Cobal; A Coccaro; J Cochran; L Coffey; J G Cogan; J Coggeshall; B Cole; S Cole; A P Colijn; J Collot; T Colombo; G Colon; G Compostella; P Conde Muiño; E Coniavitis; M C Conidi; S H Connell; I A Connelly; S M Consonni; V Consorti; S Constantinescu; C Conta; G Conti; F Conventi; M Cooke; B D Cooper; A M Cooper-Sarkar; N J Cooper-Smith; K Copic; T Cornelissen; M Corradi; F Corriveau; A Corso-Radu; A Cortes-Gonzalez; G Cortiana; G Costa; M J Costa; D Costanzo; D Côté; G Cottin; G Cowan; B E Cox; K Cranmer; G Cree; S Crépé-Renaudin; F Crescioli; W A Cribbs; M Crispin Ortuzar; M Cristinziani; V Croft; G Crosetti; C-M Cuciuc; T Cuhadar Donszelmann; J Cummings; M Curatolo; C Cuthbert; H Czirr; P Czodrowski; Z Czyczula; S D'Auria; M D'Onofrio; M J Da Cunha Sargedas De Sousa; C Da Via; W Dabrowski; A Dafinca; T Dai; O Dale; F Dallaire; C Dallapiccola; M Dam; A C Daniells; M Dano Hoffmann; V Dao; G Darbo; S Darmora; J A Dassoulas; A Dattagupta; W Davey; C David; T Davidek; E Davies; M Davies; O Davignon; A R Davison; P Davison; Y Davygora; E Dawe; I Dawson; R K Daya-Ishmukhametova; K De; R de Asmundis; S De Castro; S De Cecco; N De Groot; P de Jong; H De la Torre; F De Lorenzi; L De Nooij; D De Pedis; A De Salvo; U De Sanctis; A De Santo; J B De Vivie De Regie; W J Dearnaley; R Debbe; C Debenedetti; B Dechenaux; D V Dedovich; I Deigaard; J Del Peso; T Del Prete; F Deliot; C M Delitzsch; M Deliyergiyev; A Dell'Acqua; L Dell'Asta; M Dell'Orso; M Della Pietra; D Della Volpe; M Delmastro; P A Delsart; C Deluca; S Demers; M Demichev; A Demilly; S P Denisov; D Derendarz; J E Derkaoui; F Derue; P Dervan; K Desch; C Deterre; P O Deviveiros; A Dewhurst; S Dhaliwal; A Di Ciaccio; L Di Ciaccio; A Di Domenico; C Di Donato; A Di Girolamo; B Di Girolamo; A Di Mattia; B Di Micco; R Di Nardo; A Di Simone; R Di Sipio; D Di Valentino; F A Dias; M A Diaz; E B Diehl; J Dietrich; T A Dietzsch; S Diglio; A Dimitrievska; J Dingfelder; C Dionisi; P Dita; S Dita; F Dittus; F Djama; T Djobava; M A B do Vale; A Do Valle Wemans; T K O Doan; D Dobos; C Doglioni; T Doherty; T Dohmae; J Dolejsi; Z Dolezal; B A Dolgoshein; M Donadelli; S Donati; P Dondero; J Donini; J Dopke; A Doria; M T Dova; A T Doyle; M Dris; J Dubbert; S Dube; E Dubreuil; E Duchovni; G Duckeck; O A Ducu; D Duda; A Dudarev; F Dudziak; L Duflot; L Duguid; M Dührssen; M Dunford; H Duran Yildiz; M Düren; A Durglishvili; M Dwuznik; M Dyndal; J Ebke; W Edson; N C Edwards; W Ehrenfeld; T Eifert; G Eigen; K Einsweiler; T Ekelof; M El Kacimi; M Ellert; S Elles; F Ellinghaus; N Ellis; J Elmsheuser; M Elsing; D Emeliyanov; Y Enari; O C Endner; M Endo; R Engelmann; J Erdmann; A Ereditato; D Eriksson; G Ernis; J Ernst; M Ernst; J Ernwein; D Errede; S Errede; E Ertel; M Escalier; H Esch; C Escobar; B Esposito; A I Etienvre; E Etzion; H Evans; A Ezhilov; L Fabbri; G Facini; R M Fakhrutdinov; S Falciano; R J Falla; J Faltova; Y Fang; M Fanti; A Farbin; A Farilla; T Farooque; S Farrell; S M Farrington; P Farthouat; F Fassi; P Fassnacht; D Fassouliotis; A Favareto; L Fayard; P Federic; O L Fedin; W Fedorko; M Fehling-Kaschek; S Feigl; L Feligioni; C Feng; E J Feng; H Feng; A B Fenyuk; S Fernandez Perez; S Ferrag; J Ferrando; A Ferrari; P Ferrari; R Ferrari; D E Ferreira de Lima; A Ferrer; D Ferrere; C Ferretti; A Ferretto Parodi; M Fiascaris; F Fiedler; A Filipčič; M Filipuzzi; F Filthaut; M Fincke-Keeler; K D Finelli; M C N Fiolhais; L Fiorini; A Firan; A Fischer; J Fischer; W C Fisher; E A Fitzgerald; M Flechl; I Fleck; P Fleischmann; S Fleischmann; G T Fletcher; G Fletcher; T Flick; A Floderus; L R Flores Castillo; A C Florez Bustos; M J Flowerdew; A Formica; A Forti; D Fortin; D Fournier; H Fox; S Fracchia; P Francavilla; M Franchini; S Franchino; D Francis; L Franconi; M Franklin; S Franz; M Fraternali; S T French; C Friedrich; F Friedrich; D Froidevaux; J A Frost; C Fukunaga; E Fullana Torregrosa; B G Fulsom; J Fuster; C Gabaldon; O Gabizon; A Gabrielli; A Gabrielli; S Gadatsch; S Gadomski; G Gagliardi; P Gagnon; C Galea; B Galhardo; E J Gallas; V Gallo; B J Gallop; P Gallus; G Galster; K K Gan; R P Gandrajula; J Gao; Y S Gao; F M Garay Walls; F Garberson; C García; J E García Navarro; M Garcia-Sciveres; R W Gardner; N Garelli; V Garonne; C Gatti; G Gaudio; B Gaur; L Gauthier; P Gauzzi; I L Gavrilenko; C Gay; G Gaycken; E N Gazis; P Ge; Z Gecse; C N P Gee; D A A Geerts; Ch Geich-Gimbel; K Gellerstedt; C Gemme; A Gemmell; M H Genest; S Gentile; M George; S George; D Gerbaudo; A Gershon; H Ghazlane; N Ghodbane; B Giacobbe; S Giagu; V Giangiobbe; P Giannetti; F Gianotti; B Gibbard; S M Gibson; M Gilchriese; T P S Gillam; D Gillberg; G Gilles; D M Gingrich; N Giokaris; M P Giordani; R Giordano; F M Giorgi; F M Giorgi; P F Giraud; D Giugni; C Giuliani; M Giulini; B K Gjelsten; S Gkaitatzis; I Gkialas; L K Gladilin; C Glasman; J Glatzer; P C F Glaysher; A Glazov; G L Glonti; M Goblirsch-Kolb; J R Goddard; J Godfrey; J Godlewski; C Goeringer; S Goldfarb; T Golling; D Golubkov; A Gomes; L S Gomez Fajardo; R Gonçalo; J Goncalves Pinto Firmino Da Costa; L Gonella; S González de la Hoz; G Gonzalez Parra; S Gonzalez-Sevilla; L Goossens; P A Gorbounov; H A Gordon; I Gorelov; B Gorini; E Gorini; A Gorišek; E Gornicki; A T Goshaw; C Gössling; M I Gostkin; M Gouighri; D Goujdami; M P Goulette; A G Goussiou; C Goy; S Gozpinar; H M X Grabas; L Graber; I Grabowska-Bold; P Grafström; K-J Grahn; J Gramling; E Gramstad; S Grancagnolo; V Grassi; V Gratchev; H M Gray; E Graziani; O G Grebenyuk; Z D Greenwood; K Gregersen; I M Gregor; P Grenier; J Griffiths; A A Grillo; K Grimm; S Grinstein; Ph Gris; Y V Grishkevich; J-F Grivaz; J P Grohs; A Grohsjean; E Gross; J Grosse-Knetter; G C Grossi; J Groth-Jensen; Z J Grout; L Guan; F Guescini; D Guest; O Gueta; C Guicheney; E Guido; T Guillemin; S Guindon; U Gul; C Gumpert; J Gunther; J Guo; S Gupta; P Gutierrez; N G Gutierrez Ortiz; C Gutschow; N Guttman; C Guyot; C Gwenlan; C B Gwilliam; A Haas; C Haber; H K Hadavand; N Haddad; P Haefner; S Hageböck; Z Hajduk; H Hakobyan; M Haleem; D Hall; G Halladjian; K Hamacher; P Hamal; K Hamano; M Hamer; A Hamilton; S Hamilton; G N Hamity; P G Hamnett; L Han; K Hanagaki; K Hanawa; M Hance; P Hanke; R Hanna; J B Hansen; J D Hansen; P H Hansen; K Hara; A S Hard; T Harenberg; F Hariri; S Harkusha; D Harper; R D Harrington; O M Harris; P F Harrison; F Hartjes; M Hasegawa; S Hasegawa; Y Hasegawa; A Hasib; S Hassani; S Haug; M Hauschild; R Hauser; M Havranek; C M Hawkes; R J Hawkings; A D Hawkins; T Hayashi; D Hayden; C P Hays; H S Hayward; S J Haywood; S J Head; T Heck; V Hedberg; L Heelan; S Heim; T Heim; B Heinemann; L Heinrich; J Hejbal; L Helary; C Heller; M Heller; S Hellman; D Hellmich; C Helsens; J Henderson; R C W Henderson; Y Heng; C Hengler; A Henrichs; A M Henriques Correia; S Henrot-Versille; C Hensel; G H Herbert; Y Hernández Jiménez; R Herrberg-Schubert; G Herten; R Hertenberger; L Hervas; G G Hesketh; N P Hessey; R Hickling; E Higón-Rodriguez; E Hill; J C Hill; K H Hiller; S Hillert; S J Hillier; I Hinchliffe; E Hines; M Hirose; D Hirschbuehl; J Hobbs; N Hod; M C Hodgkinson; P Hodgson; A Hoecker; M R Hoeferkamp; F Hoenig; J Hoffman; D Hoffmann; J I Hofmann; M Hohlfeld; T R Holmes; T M Hong; L Hooft van Huysduynen; J-Y Hostachy; S Hou; A Hoummada; J Howard; J Howarth; M Hrabovsky; I Hristova; J Hrivnac; T Hryn'ova; C Hsu; P J Hsu; S-C Hsu; D Hu; X Hu; Y Huang; Z Hubacek; F Hubaut; F Huegging; T B Huffman; E W Hughes; G Hughes; M Huhtinen; T A Hülsing; M Hurwitz; N Huseynov; J Huston; J Huth; G Iacobucci; G Iakovidis; I Ibragimov; L Iconomidou-Fayard; E Ideal; P Iengo; O Igonkina; T Iizawa; Y Ikegami; K Ikematsu; M Ikeno; Y Ilchenko; D Iliadis; N Ilic; Y Inamaru; T Ince; P Ioannou; M Iodice; K Iordanidou; V Ippolito; A Irles Quiles; C Isaksson; M Ishino; M Ishitsuka; R Ishmukhametov; C Issever; S Istin; J M Iturbe Ponce; R Iuppa; J Ivarsson; W Iwanski; H Iwasaki; J M Izen; V Izzo; B Jackson; M Jackson; P Jackson; M R Jaekel; V Jain; K Jakobs; S Jakobsen; T Jakoubek; J Jakubek; D O Jamin; D K Jana; E Jansen; H Jansen; J Janssen; M Janus; G Jarlskog; N Javadov; T Javůrek; L Jeanty; J Jejelava; G-Y Jeng; D Jennens; P Jenni; J Jentzsch; C Jeske; S Jézéquel; H Ji; J Jia; Y Jiang; M Jimenez Belenguer; S Jin; A Jinaru; O Jinnouchi; M D Joergensen; K E Johansson; P Johansson; K A Johns; K Jon-And; G Jones; R W L Jones; T J Jones; J Jongmanns; P M Jorge; K D Joshi; J Jovicevic; X Ju; C A Jung; R M Jungst; P Jussel; A Juste Rozas; M Kaci; A Kaczmarska; M Kado; H Kagan; M Kagan; E Kajomovitz; C W Kalderon; S Kama; A Kamenshchikov; N Kanaya; M Kaneda; S Kaneti; V A Kantserov; J Kanzaki; B Kaplan; A Kapliy; D Kar; K Karakostas; N Karastathis; M Karnevskiy; S N Karpov; Z M Karpova; K Karthik; V Kartvelishvili; A N Karyukhin; L Kashif; G Kasieczka; R D Kass; A Kastanas; Y Kataoka; A Katre; J Katzy; V Kaushik; K Kawagoe; T Kawamoto; G Kawamura; S Kazama; V F Kazanin; M Y Kazarinov; R Keeler; R Kehoe; M Keil; J S Keller; J J Kempster; H Keoshkerian; O Kepka; B P Kerševan; S Kersten; K Kessoku; J Keung; F Khalil-Zada; H Khandanyan; A Khanov; A Khodinov; A Khomich; T J Khoo; G Khoriauli; A Khoroshilov; V Khovanskiy; E Khramov; J Khubua; H Y Kim; H Kim; S H Kim; N Kimura; O Kind; B T King; M King; R S B King; S B King; J Kirk; A E Kiryunin; T Kishimoto; D Kisielewska; F Kiss; T Kittelmann; K Kiuchi; E Kladiva; M Klein; U Klein; K Kleinknecht; P Klimek; A Klimentov; R Klingenberg; J A Klinger; T Klioutchnikova; P F Klok; E-E Kluge; P Kluit; S Kluth; E Kneringer; E B F G Knoops; A Knue; D Kobayashi; T Kobayashi; M Kobel; M Kocian; P Kodys; P Koevesarki; T Koffas; E Koffeman; L A Kogan; S Kohlmann; Z Kohout; T Kohriki; T Koi; H Kolanoski; I Koletsou; J Koll; A A Komar; Y Komori; T Kondo; N Kondrashova; K Köneke; A C König; S König; T Kono; R Konoplich; N Konstantinidis; R Kopeliansky; S Koperny; L Köpke; A K Kopp; K Korcyl; K Kordas; A Korn; A A Korol; I Korolkov; E V Korolkova; V A Korotkov; O Kortner; S Kortner; V V Kostyukhin; V M Kotov; A Kotwal; C Kourkoumelis; V Kouskoura; A Koutsman; R Kowalewski; T Z Kowalski; W Kozanecki; A S Kozhin; V Kral; V A Kramarenko; G Kramberger; D Krasnopevtsev; M W Krasny; A Krasznahorkay; J K Kraus; A Kravchenko; S Kreiss; M Kretz; J Kretzschmar; K Kreutzfeldt; P Krieger; K Kroeninger; H Kroha; J Kroll; J Kroseberg; J Krstic; U Kruchonak; H Krüger; T Kruker; N Krumnack; Z V Krumshteyn; A Kruse; M C Kruse; M Kruskal; T Kubota; S Kuday; S Kuehn; A Kugel; A Kuhl; T Kuhl; V Kukhtin; Y Kulchitsky; S Kuleshov; M Kuna; J Kunkle; A Kupco; H Kurashige; Y A Kurochkin; R Kurumida; V Kus; E S Kuwertz; M Kuze; J Kvita; A La Rosa; L La Rotonda; C Lacasta; F Lacava; J Lacey; H Lacker; D Lacour; V R Lacuesta; E Ladygin; R Lafaye; B Laforge; T Lagouri; S Lai; H Laier; L Lambourne; S Lammers; C L Lampen; W Lampl; E Lançon; U Landgraf; M P J Landon; V S Lang; A J Lankford; F Lanni; K Lantzsch; S Laplace; C Lapoire; J F Laporte; T Lari; M Lassnig; P Laurelli; W Lavrijsen; A T Law; P Laycock; O Le Dortz; E Le Guirriec; E Le Menedeu; T LeCompte; F Ledroit-Guillon; C A Lee; H Lee; J S H Lee; S C Lee; L Lee; G Lefebvre; M Lefebvre; F Legger; C Leggett; A Lehan; M Lehmacher; G Lehmann Miotto; X Lei; W A Leight; A Leisos; A G Leister; M A L Leite; R Leitner; D Lellouch; B Lemmer; K J C Leney; T Lenz; G Lenzen; B Lenzi; R Leone; S Leone; K Leonhardt; C Leonidopoulos; S Leontsinis; C Leroy; C G Lester; C M Lester; M Levchenko; J Levêque; D Levin; L J Levinson; M Levy; A Lewis; G H Lewis; A M Leyko; M Leyton; B Li; B Li; H Li; H L Li; L Li; L Li; S Li; Y Li; Z Liang; H Liao; B Liberti; P Lichard; K Lie; J Liebal; W Liebig; C Limbach; A Limosani; S C Lin; T H Lin; F Linde; B E Lindquist; J T Linnemann; E Lipeles; A Lipniacka; M Lisovyi; T M Liss; D Lissauer; A Lister; A M Litke; B Liu; D Liu; J B Liu; K Liu; L Liu; M Liu; M Liu; Y Liu; M Livan; S S A Livermore; A Lleres; J Llorente Merino; S L Lloyd; F Lo Sterzo; E Lobodzinska; P Loch; W S Lockman; T Loddenkoetter; F K Loebinger; A E Loevschall-Jensen; A Loginov; T Lohse; K Lohwasser; M Lokajicek; V P Lombardo; B A Long; J D Long; R E Long; L Lopes; D Lopez Mateos; B Lopez Paredes; I Lopez Paz; J Lorenz; N Lorenzo Martinez; M Losada; P Loscutoff; X Lou; A Lounis; J Love; P A Love; A J Lowe; F Lu; N Lu; H J Lubatti; C Luci; A Lucotte; F Luehring; W Lukas; L Luminari; O Lundberg; B Lund-Jensen; M Lungwitz; D Lynn; R Lysak; E Lytken; H Ma; L L Ma; G Maccarrone; A Macchiolo; J Machado Miguens; D Macina; D Madaffari; R Madar; H J Maddocks; W F Mader; A Madsen; M Maeno; T Maeno; E Magradze; K Mahboubi; J Mahlstedt; S Mahmoud; C Maiani; C Maidantchik; A A Maier; A Maio; S Majewski; Y Makida; N Makovec; P Mal; B Malaescu; Pa Malecki; V P Maleev; F Malek; U Mallik; D Malon; C Malone; S Maltezos; V M Malyshev; S Malyukov; J Mamuzic; B Mandelli; L Mandelli; I Mandić; R Mandrysch; J Maneira; A Manfredini; L Manhaes de Andrade Filho; J A Manjarres Ramos; A Mann; P M Manning; A Manousakis-Katsikakis; B Mansoulie; R Mantifel; L Mapelli; L March; J F Marchand; G Marchiori; M Marcisovsky; C P Marino; M Marjanovic; C N Marques; F Marroquim; S P Marsden; Z Marshall; L F Marti; S Marti-Garcia; B Martin; B Martin; T A Martin; V J Martin; B Martin Dit Latour; H Martinez; M Martinez; S Martin-Haugh; A C Martyniuk; M Marx; F Marzano; A Marzin; L Masetti; T Mashimo; R Mashinistov; J Masik; A L Maslennikov; I Massa; L Massa; N Massol; P Mastrandrea; A Mastroberardino; T Masubuchi; P Mättig; J Mattmann; J Maurer; S J Maxfield; D A Maximov; R Mazini; L Mazzaferro; G Mc Goldrick; S P Mc Kee; A McCarn; R L McCarthy; T G McCarthy; N A McCubbin; K W McFarlane; J A Mcfayden; G Mchedlidze; S J McMahon; R A McPherson; A Meade; J Mechnich; M Medinnis; S Meehan; S Mehlhase; A Mehta; K Meier; C Meineck; B Meirose; C Melachrinos; B R Mellado Garcia; F Meloni; A Mengarelli; S Menke; E Meoni; K M Mercurio; S Mergelmeyer; N Meric; P Mermod; L Merola; C Meroni; F S Merritt; H Merritt; A Messina; J Metcalfe; A S Mete; C Meyer; C Meyer; J-P Meyer; J Meyer; R P Middleton; S Migas; L Mijović; G Mikenberg; M Mikestikova; M Mikuž; A Milic; D W Miller; C Mills; A Milov; D A Milstead; D Milstein; A A Minaenko; I A Minashvili; A I Mincer; B Mindur; M Mineev; Y Ming; L M Mir; G Mirabelli; T Mitani; J Mitrevski; V A Mitsou; S Mitsui; A Miucci; P S Miyagawa; J U Mjörnmark; T Moa; K Mochizuki; S Mohapatra; W Mohr; S Molander; R Moles-Valls; K Mönig; C Monini; J Monk; E Monnier; J Montejo Berlingen; F Monticelli; S Monzani; R W Moore; A Moraes; N Morange; D Moreno; M Moreno Llácer; P Morettini; M Morgenstern; M Morii; S Moritz; A K Morley; G Mornacchi; J D Morris; L Morvaj; H G Moser; M Mosidze; J Moss; K Motohashi; R Mount; E Mountricha; S V Mouraviev; E J W Moyse; S Muanza; R D Mudd; F Mueller; J Mueller; K Mueller; T Mueller; T Mueller; D Muenstermann; Y Munwes; J A Murillo Quijada; W J Murray; H Musheghyan; E Musto; A G Myagkov; M Myska; O Nackenhorst; J Nadal; K Nagai; R Nagai; Y Nagai; K Nagano; A Nagarkar; Y Nagasaka; M Nagel; A M Nairz; Y Nakahama; K Nakamura; T Nakamura; I Nakano; H Namasivayam; G Nanava; R Narayan; T Nattermann; T Naumann; G Navarro; R Nayyar; H A Neal; P Yu Nechaeva; T J Neep; P D Nef; A Negri; G Negri; M Negrini; S Nektarijevic; A Nelson; T K Nelson; S Nemecek; P Nemethy; A A Nepomuceno; M Nessi; M S Neubauer; M Neumann; R M Neves; P Nevski; P R Newman; D H Nguyen; R B Nickerson; R Nicolaidou; B Nicquevert; J Nielsen; N Nikiforou; A Nikiforov; V Nikolaenko; I Nikolic-Audit; K Nikolics; K Nikolopoulos; P Nilsson; Y Ninomiya; A Nisati; R Nisius; T Nobe; L Nodulman; M Nomachi; I Nomidis; S Norberg; M Nordberg; O Novgorodova; S Nowak; M Nozaki; L Nozka; K Ntekas; G Nunes Hanninger; T Nunnemann; E Nurse; F Nuti; B J O'Brien; F O'grady; D C O'Neil; V O'Shea; F G Oakham; H Oberlack; T Obermann; J Ocariz; A Ochi; M I Ochoa; S Oda; S Odaka; H Ogren; A Oh; S H Oh; C C Ohm; H Ohman; W Okamura; H Okawa; Y Okumura; T Okuyama; A Olariu; A G Olchevski; S A Olivares Pino; D Oliveira Damazio; E Oliver Garcia; A Olszewski; J Olszowska; A Onofre; P U E Onyisi; C J Oram; M J Oreglia; Y Oren; D Orestano; N Orlando; C Oropeza Barrera; R S Orr; B Osculati; R Ospanov; G Otero Y Garzon; H Otono; M Ouchrif; E A Ouellette; F Ould-Saada; A Ouraou; K P Oussoren; Q Ouyang; A Ovcharova; M Owen; V E Ozcan; N Ozturk; K Pachal; A Pacheco Pages; C Padilla Aranda; M Pagáčová; S Pagan Griso; E Paganis; C Pahl; F Paige; P Pais; K Pajchel; G Palacino; S Palestini; M Palka; D Pallin; A Palma; J D Palmer; Y B Pan; E Panagiotopoulou; J G Panduro Vazquez; P Pani; N Panikashvili; S Panitkin; D Pantea; L Paolozzi; Th D Papadopoulou; K Papageorgiou; A Paramonov; D Paredes Hernandez; M A Parker; F Parodi; J A Parsons; U Parzefall; E Pasqualucci; S Passaggio; A Passeri; F Pastore; Fr Pastore; G Pásztor; S Pataraia; N D Patel; J R Pater; S Patricelli; T Pauly; J Pearce; M Pedersen; S Pedraza Lopez; R Pedro; S V Peleganchuk; D Pelikan; H Peng; B Penning; J Penwell; D V Perepelitsa; E Perez Codina; M T Pérez García-Estañ; V Perez Reale; L Perini; H Pernegger; R Perrino; R Peschke; V D Peshekhonov; K Peters; R F Y Peters; B A Petersen; T C Petersen; E Petit; A Petridis; C Petridou; E Petrolo; F Petrucci; N E Pettersson; R Pezoa; P W Phillips; G Piacquadio; E Pianori; A Picazio; E Piccaro; M Piccinini; R Piegaia; D T Pignotti; J E Pilcher; A D Pilkington; J Pina; M Pinamonti; A Pinder; J L Pinfold; A Pingel; B Pinto; S Pires; M Pitt; C Pizio; L Plazak; M-A Pleier; V Pleskot; E Plotnikova; P Plucinski; S Poddar; F Podlyski; R Poettgen; L Poggioli; D Pohl; M Pohl; G Polesello; A Policicchio; R Polifka; A Polini; C S Pollard; V Polychronakos; K Pommès; L Pontecorvo; B G Pope; G A Popeneciu; D S Popovic; A Poppleton; X Portell Bueso; S Pospisil; K Potamianos; I N Potrap; C J Potter; C T Potter; G Poulard; J Poveda; V Pozdnyakov; P Pralavorio; A Pranko; S Prasad; R Pravahan; S Prell; D Price; J Price; L E Price; D Prieur; M Primavera; M Proissl; K Prokofiev; F Prokoshin; E Protopapadaki; S Protopopescu; J Proudfoot; M Przybycien; H Przysiezniak; E Ptacek; D Puddu; E Pueschel; D Puldon; M Purohit; P Puzo; J Qian; G Qin; Y Qin; A Quadt; D R Quarrie; W B Quayle; M Queitsch-Maitland; D Quilty; A Qureshi; V Radeka; V Radescu; S K Radhakrishnan; P Radloff; P Rados; F Ragusa; G Rahal; S Rajagopalan; M Rammensee; A S Randle-Conde; C Rangel-Smith; K Rao; F Rauscher; T C Rave; T Ravenscroft; M Raymond; A L Read; N P Readioff; D M Rebuzzi; A Redelbach; G Redlinger; R Reece; K Reeves; L Rehnisch; H Reisin; M Relich; C Rembser; H Ren; Z L Ren; A Renaud; M Rescigno; S Resconi; O L Rezanova; P Reznicek; R Rezvani; R Richter; M Ridel; P Rieck; J Rieger; M Rijssenbeek; A Rimoldi; L Rinaldi; E Ritsch; I Riu; F Rizatdinova; E Rizvi; S H Robertson; A Robichaud-Veronneau; D Robinson; J E M Robinson; A Robson; C Roda; L Rodrigues; S Roe; O Røhne; S Rolli; A Romaniouk; M Romano; E Romero Adam; N Rompotis; M Ronzani; L Roos; E Ros; S Rosati; K Rosbach; M Rose; P Rose; P L Rosendahl; O Rosenthal; V Rossetti; E Rossi; L P Rossi; R Rosten; M Rotaru; I Roth; J Rothberg; D Rousseau; C R Royon; A Rozanov; Y Rozen; X Ruan; F Rubbo; I Rubinskiy; V I Rud; C Rudolph; M S Rudolph; F Rühr; A Ruiz-Martinez; Z Rurikova; 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M Schernau; M I Scherzer; C Schiavi; J Schieck; C Schillo; M Schioppa; S Schlenker; E Schmidt; K Schmieden; C Schmitt; S Schmitt; B Schneider; Y J Schnellbach; U Schnoor; L Schoeffel; A Schoening; B D Schoenrock; A L S Schorlemmer; M Schott; D Schouten; J Schovancova; S Schramm; M Schreyer; C Schroeder; N Schuh; M J Schultens; H-C Schultz-Coulon; H Schulz; M Schumacher; B A Schumm; Ph Schune; C Schwanenberger; A Schwartzman; Ph Schwegler; Ph Schwemling; R Schwienhorst; J Schwindling; T Schwindt; M Schwoerer; F G Sciacca; E Scifo; G Sciolla; W G Scott; F Scuri; F Scutti; J Searcy; G Sedov; E Sedykh; S C Seidel; A Seiden; F Seifert; J M Seixas; G Sekhniaidze; S J Sekula; K E Selbach; D M Seliverstov; G Sellers; N Semprini-Cesari; C Serfon; L Serin; L Serkin; T Serre; R Seuster; H Severini; T Sfiligoj; F Sforza; A Sfyrla; E Shabalina; M Shamim; L Y Shan; R Shang; J T Shank; M Shapiro; P B Shatalov; K Shaw; C Y Shehu; P Sherwood; L Shi; S Shimizu; C O Shimmin; M Shimojima; M Shiyakova; A Shmeleva; 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Journal:  Eur Phys J C Part Fields       Date:  2015-04-23       Impact factor: 4.590

3.  Measurement of the top quark mass in the all-jets final state at s = 13 TeV and combination with the lepton+jets channel.

Authors:  A M Sirunyan; A Tumasyan; W Adam; F Ambrogi; E Asilar; T Bergauer; J Brandstetter; M Dragicevic; J Erö; A Escalante Del Valle; M Flechl; R Frühwirth; V M Ghete; J Hrubec; M Jeitler; N Krammer; I Krätschmer; D Liko; T Madlener; I Mikulec; N Rad; H Rohringer; J Schieck; R Schöfbeck; M Spanring; D Spitzbart; W Waltenberger; J Wittmann; C-E Wulz; M Zarucki; V Chekhovsky; V Mossolov; J Suarez Gonzalez; E A De Wolf; D Di Croce; X Janssen; J Lauwers; A Lelek; M Pieters; H Van Haevermaet; P Van Mechelen; N Van Remortel; S Abu Zeid; F Blekman; J D'Hondt; J De Clercq; K Deroover; G Flouris; D Lontkovskyi; S Lowette; I Marchesini; S Moortgat; L Moreels; Q Python; K Skovpen; S Tavernier; W Van Doninck; P Van Mulders; I Van Parijs; D Beghin; B Bilin; H Brun; B Clerbaux; G De Lentdecker; H Delannoy; B Dorney; G Fasanella; L Favart; A Grebenyuk; A K Kalsi; T Lenzi; J Luetic; N Postiau; E Starling; L Thomas; C Vander Velde; P Vanlaer; D Vannerom; Q Wang; T Cornelis; D Dobur; A Fagot; M Gul; I Khvastunov; D Poyraz; C Roskas; D Trocino; M Tytgat; W Verbeke; B Vermassen; M Vit; N Zaganidis; H Bakhshiansohi; O Bondu; G Bruno; C Caputo; P David; C Delaere; M Delcourt; A Giammanco; G Krintiras; V Lemaitre; A Magitteri; K Piotrzkowski; A Saggio; M Vidal Marono; P Vischia; J Zobec; F L Alves; G A Alves; G Correia Silva; C Hensel; A Moraes; M E Pol; P Rebello Teles; E Belchior Batista Das Chagas; W Carvalho; J Chinellato; E Coelho; E M Da Costa; G G Da Silveira; D De Jesus Damiao; C De Oliveira Martins; S Fonseca De Souza; H Malbouisson; D Matos Figueiredo; M Melo De Almeida; C Mora Herrera; L Mundim; H Nogima; W L Prado Da Silva; L J Sanchez Rosas; A Santoro; A Sznajder; M Thiel; E J Tonelli Manganote; F Torres Da Silva De Araujo; A Vilela Pereira; S Ahuja; C A Bernardes; L Calligaris; T R Fernandez Perez Tomei; E M Gregores; P G Mercadante; S F Novaes; SandraS Padula; A Aleksandrov; R Hadjiiska; P Iaydjiev; A Marinov; M Misheva; M Rodozov; M Shopova; G Sultanov; A Dimitrov; L Litov; B Pavlov; P Petkov; W Fang; X Gao; L Yuan; M Ahmad; J G Bian; G M Chen; H S Chen; M Chen; Y Chen; C H Jiang; D Leggat; H Liao; Z Liu; S M Shaheen; A Spiezia; J Tao; E Yazgan; H Zhang; S Zhang; J Zhao; Y Ban; G Chen; A Levin; J Li; L Li; Q Li; Y Mao; S J Qian; D Wang; Y Wang; C Avila; A Cabrera; C A Carrillo Montoya; L F Chaparro Sierra; C Florez; C F González Hernández; M A Segura Delgado; B Courbon; N Godinovic; D Lelas; I Puljak; T Sculac; Z Antunovic; M Kovac; V Brigljevic; D Ferencek; K Kadija; B Mesic; M Roguljic; A Starodumov; T Susa; M W Ather; A Attikis; M Kolosova; G Mavromanolakis; J Mousa; C Nicolaou; F Ptochos; P A Razis; H Rykaczewski; M Finger; M Finger; E Ayala; E Carrera Jarrin; H Abdalla; S Khalil; A Mohamed; S Bhowmik; A Carvalho Antunes De Oliveira; R K Dewanjee; K Ehataht; M Kadastik; M Raidal; C Veelken; P Eerola; H Kirschenmann; J Pekkanen; M Voutilainen; J Havukainen; J K Heikkilä; T Järvinen; V Karimäki; R Kinnunen; T Lampén; K Lassila-Perini; S Laurila; S Lehti; T Lindén; P Luukka; T Mäenpää; H Siikonen; E Tuominen; J Tuominiemi; T Tuuva; M Besancon; F Couderc; M Dejardin; D Denegri; J L Faure; F Ferri; S Ganjour; A Givernaud; P Gras; G Hamel de Monchenault; P Jarry; C Leloup; E Locci; J Malcles; G Negro; J Rander; A Rosowsky; M Ö Sahin; M Titov; A Abdulsalam; C Amendola; I Antropov; F Beaudette; P Busson; C Charlot; R Granier de Cassagnac; I Kucher; A Lobanov; J Martin Blanco; C Martin Perez; M Nguyen; C Ochando; G Ortona; P Paganini; J Rembser; R Salerno; J B Sauvan; Y Sirois; A G Stahl Leiton; A Zabi; A Zghiche; J-L Agram; J Andrea; D Bloch; G Bourgatte; J-M Brom; E C Chabert; V Cherepanov; C Collard; E Conte; J-C Fontaine; D Gelé; U Goerlach; M Jansová; A-C Le Bihan; N Tonon; P Van Hove; S Gadrat; S Beauceron; C Bernet; G Boudoul; N Chanon; R Chierici; D Contardo; P Depasse; H El Mamouni; J Fay; L Finco; S Gascon; M Gouzevitch; G Grenier; B Ille; F Lagarde; I B Laktineh; H Lattaud; M Lethuillier; L Mirabito; S Perries; A Popov; V Sordini; 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S M Heindl; U Husemann; I Katkov; S Kudella; S Mitra; M U Mozer; Th Müller; M Musich; M Plagge; G Quast; K Rabbertz; M Schröder; I Shvetsov; H J Simonis; R Ulrich; S Wayand; M Weber; T Weiler; C Wöhrmann; R Wolf; G Anagnostou; G Daskalakis; T Geralis; A Kyriakis; D Loukas; G Paspalaki; A Agapitos; G Karathanasis; P Kontaxakis; A Panagiotou; I Papavergou; N Saoulidou; K Vellidis; K Kousouris; I Papakrivopoulos; G Tsipolitis; I Evangelou; C Foudas; P Gianneios; P Katsoulis; P Kokkas; S Mallios; N Manthos; I Papadopoulos; E Paradas; J Strologas; F A Triantis; D Tsitsonis; M Bartók; M Csanad; N Filipovic; P Major; M I Nagy; G Pasztor; O Surányi; G I Veres; G Bencze; C Hajdu; D Horvath; Á Hunyadi; F Sikler; T Á Vámi; V Veszpremi; G Vesztergombi; N Beni; S Czellar; J Karancsi; A Makovec; J Molnar; Z Szillasi; P Raics; Z L Trocsanyi; B Ujvari; S Choudhury; J R Komaragiri; P C Tiwari; S Bahinipati; C Kar; P Mal; K Mandal; A Nayak; S Roy Chowdhury; D K Sahoo; S K Swain; S Bansal; S B Beri; V Bhatnagar; 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Journal:  Eur Phys J C Part Fields       Date:  2019-04-06       Impact factor: 4.590

4.  Measurement of the top quark mass in the [Formula: see text] and [Formula: see text] channels using [Formula: see text] [Formula: see text] ATLAS data.

Authors:  G Aad; B Abbott; J Abdallah; O Abdinov; R Aben; M Abolins; O S AbouZeid; H Abramowicz; H Abreu; R Abreu; Y Abulaiti; B S Acharya; L Adamczyk; D L Adams; J Adelman; S Adomeit; T Adye; A A Affolder; T Agatonovic-Jovin; J A Aguilar-Saavedra; S P Ahlen; F Ahmadov; G Aielli; H Akerstedt; T P A Åkesson; G Akimoto; A V Akimov; G L Alberghi; J Albert; S Albrand; M J Alconada Verzini; M Aleksa; I N Aleksandrov; C Alexa; G Alexander; T Alexopoulos; M Alhroob; G Alimonti; L Alio; J Alison; S P Alkire; B M M Allbrooke; P P Allport; A Aloisio; A Alonso; F Alonso; C Alpigiani; A Altheimer; B Alvarez Gonzalez; D Álvarez Piqueras; M G Alviggi; B T Amadio; K Amako; Y Amaral Coutinho; C Amelung; D Amidei; S P Amor Dos Santos; A Amorim; S Amoroso; N Amram; G Amundsen; C Anastopoulos; L S Ancu; N Andari; T Andeen; C F Anders; G Anders; J K Anders; K J Anderson; A Andreazza; V Andrei; S Angelidakis; I Angelozzi; P Anger; A Angerami; F Anghinolfi; A V Anisenkov; N Anjos; A Annovi; M Antonelli; A Antonov; J Antos; F Anulli; M Aoki; L Aperio Bella; G Arabidze; Y Arai; J P Araque; A T H Arce; F A Arduh; J-F Arguin; S Argyropoulos; M Arik; A J Armbruster; O Arnaez; V Arnal; H Arnold; M Arratia; O Arslan; A Artamonov; G Artoni; S Asai; N Asbah; A Ashkenazi; B Åsman; L Asquith; K Assamagan; R Astalos; M Atkinson; N B Atlay; B Auerbach; K Augsten; M Aurousseau; G Avolio; B Axen; M K Ayoub; G Azuelos; M A Baak; A E Baas; C Bacci; H Bachacou; K Bachas; M Backes; M Backhaus; E Badescu; P Bagiacchi; P Bagnaia; Y Bai; T Bain; J T Baines; O K Baker; P Balek; T Balestri; F Balli; E Banas; Sw Banerjee; A A E Bannoura; H S Bansil; L Barak; S P Baranov; E L Barberio; D Barberis; M Barbero; T Barillari; M Barisonzi; T Barklow; N Barlow; S L Barnes; B M Barnett; R M Barnett; Z Barnovska; A Baroncelli; G Barone; A J Barr; F Barreiro; J Barreiro Guimarães da Costa; R Bartoldus; A E Barton; P Bartos; A Bassalat; A Basye; R L Bates; S J Batista; J R Batley; M Battaglia; M Bauce; F Bauer; H S Bawa; J B Beacham; M D Beattie; T Beau; P H Beauchemin; R Beccherle; P Bechtle; H P Beck; K Becker; M Becker; S Becker; M Beckingham; C Becot; A J Beddall; A Beddall; V A Bednyakov; C P Bee; L J Beemster; T A Beermann; M Begel; J K Behr; C Belanger-Champagne; P J Bell; W H Bell; G Bella; L Bellagamba; A Bellerive; M Bellomo; K Belotskiy; O Beltramello; O Benary; D Benchekroun; M Bender; K Bendtz; N Benekos; Y Benhammou; E Benhar Noccioli; J A Benitez Garcia; D P Benjamin; J R Bensinger; S Bentvelsen; L Beresford; M Beretta; D Berge; E Bergeaas Kuutmann; N Berger; F Berghaus; J Beringer; C Bernard; N R Bernard; C Bernius; F U Bernlochner; T Berry; P Berta; C Bertella; G Bertoli; F Bertolucci; C Bertsche; D Bertsche; M I Besana; G J Besjes; O Bessidskaia Bylund; M Bessner; N Besson; C Betancourt; S Bethke; A J Bevan; W Bhimji; R M Bianchi; L Bianchini; M Bianco; O Biebel; S P Bieniek; M Biglietti; J Bilbao De Mendizabal; H Bilokon; M Bindi; S Binet; A Bingul; C Bini; C W Black; J E Black; K M Black; D Blackburn; R E Blair; J-B Blanchard; J E Blanco; T Blazek; I Bloch; C Blocker; W Blum; U Blumenschein; G J Bobbink; V S Bobrovnikov; S S Bocchetta; A Bocci; C Bock; M Boehler; J A Bogaerts; A G Bogdanchikov; C Bohm; V Boisvert; T Bold; V Boldea; A S Boldyrev; M Bomben; M Bona; M Boonekamp; A Borisov; G Borissov; S Borroni; J Bortfeldt; V Bortolotto; K Bos; D Boscherini; M Bosman; J Boudreau; J Bouffard; E V Bouhova-Thacker; D Boumediene; C Bourdarios; N Bousson; A Boveia; J Boyd; I R Boyko; I Bozic; J Bracinik; A Brandt; G Brandt; O Brandt; U Bratzler; B Brau; J E Brau; H M Braun; S F Brazzale; K Brendlinger; A J Brennan; L Brenner; R Brenner; S Bressler; K Bristow; T M Bristow; D Britton; D Britzger; F M Brochu; I Brock; R Brock; J Bronner; G Brooijmans; T Brooks; W K Brooks; J Brosamer; E Brost; J Brown; P A Bruckman de Renstrom; D Bruncko; R Bruneliere; A Bruni; G Bruni; M Bruschi; L Bryngemark; T Buanes; Q Buat; P Buchholz; A G Buckley; S I Buda; I A Budagov; F Buehrer; L Bugge; M K Bugge; O Bulekov; H Burckhart; S Burdin; B Burghgrave; S Burke; I Burmeister; E Busato; D Büscher; V Büscher; P Bussey; C P Buszello; J M Butler; A I Butt; C M Buttar; J M Butterworth; P Butti; W Buttinger; A Buzatu; R Buzykaev; S Cabrera Urbán; D Caforio; V M Cairo; O Cakir; P Calafiura; A Calandri; G Calderini; P Calfayan; L P Caloba; D Calvet; S Calvet; R Camacho Toro; S Camarda; P Camarri; D Cameron; L M Caminada; R Caminal Armadans; S Campana; M Campanelli; A Campoverde; V Canale; A Canepa; M Cano Bret; J Cantero; R Cantrill; T Cao; M D M Capeans Garrido; I Caprini; M Caprini; M Capua; R Caputo; R Cardarelli; T Carli; G Carlino; L Carminati; S Caron; E Carquin; G D Carrillo-Montoya; J R Carter; J Carvalho; D Casadei; M P Casado; M Casolino; E Castaneda-Miranda; A Castelli; V Castillo Gimenez; N F Castro; P Catastini; A Catinaccio; J R Catmore; A Cattai; J Caudron; V Cavaliere; D Cavalli; M Cavalli-Sforza; V Cavasinni; F Ceradini; B C Cerio; K Cerny; A S Cerqueira; A Cerri; L Cerrito; F Cerutti; M Cerv; A Cervelli; S A Cetin; A Chafaq; D Chakraborty; I Chalupkova; P Chang; B Chapleau; J D Chapman; D G Charlton; C C Chau; C A Chavez Barajas; S Cheatham; A Chegwidden; S Chekanov; S V Chekulaev; G A Chelkov; M A Chelstowska; C Chen; H Chen; K Chen; L Chen; S Chen; X Chen; Y Chen; H C Cheng; Y Cheng; A Cheplakov; E Cheremushkina; R Cherkaoui El Moursli; V Chernyatin; E Cheu; L Chevalier; V Chiarella; J T Childers; G Chiodini; A S Chisholm; R T Chislett; A Chitan; M V Chizhov; K Choi; S Chouridou; B K B Chow; V Christodoulou; D Chromek-Burckhart; M L Chu; J Chudoba; A J Chuinard; J J Chwastowski; L Chytka; G Ciapetti; A K Ciftci; D Cinca; V Cindro; I A Cioara; A Ciocio; Z H Citron; M Ciubancan; A Clark; B L Clark; P J Clark; R N Clarke; W Cleland; C Clement; Y Coadou; M Cobal; A Coccaro; J Cochran; L Coffey; J G Cogan; B Cole; S Cole; A P Colijn; J Collot; T Colombo; G Compostella; P Conde Muiño; E Coniavitis; S H Connell; I A Connelly; S M Consonni; V Consorti; S Constantinescu; C Conta; G Conti; F Conventi; M Cooke; B D Cooper; A M Cooper-Sarkar; T Cornelissen; M Corradi; F Corriveau; A Corso-Radu; A Cortes-Gonzalez; G Cortiana; G Costa; M J Costa; D Costanzo; D Côté; G Cottin; G Cowan; B E Cox; K Cranmer; G Cree; S Crépé-Renaudin; F Crescioli; W A Cribbs; M Crispin Ortuzar; M Cristinziani; V Croft; G Crosetti; T Cuhadar Donszelmann; J Cummings; M Curatolo; C Cuthbert; H Czirr; P Czodrowski; S D'Auria; M D'Onofrio; M J Da Cunha Sargedas De Sousa; C Da Via; W Dabrowski; A Dafinca; T Dai; O Dale; F Dallaire; C Dallapiccola; M Dam; J R Dandoy; N P Dang; A C Daniells; M Danninger; M Dano Hoffmann; V Dao; G Darbo; S Darmora; J Dassoulas; A Dattagupta; W Davey; C David; T Davidek; E Davies; M Davies; P Davison; Y Davygora; E Dawe; I Dawson; R K Daya-Ishmukhametova; K De; R de Asmundis; S De Castro; S De Cecco; N De Groot; P de Jong; H De la Torre; F De Lorenzi; L De Nooij; D De Pedis; A De Salvo; U De Sanctis; A De Santo; J B De Vivie De Regie; W J Dearnaley; R Debbe; C Debenedetti; D V Dedovich; I Deigaard; J Del Peso; T Del Prete; D Delgove; F Deliot; C M Delitzsch; M Deliyergiyev; A Dell'Acqua; L Dell'Asta; M Dell'Orso; M Della Pietra; D Della Volpe; M Delmastro; P A Delsart; C Deluca; D A DeMarco; S Demers; M Demichev; A Demilly; S P Denisov; D Derendarz; J E Derkaoui; F Derue; P Dervan; K Desch; C Deterre; P O Deviveiros; A Dewhurst; S Dhaliwal; A Di Ciaccio; L Di Ciaccio; A Di Domenico; C Di Donato; A Di Girolamo; B Di Girolamo; A Di Mattia; B Di Micco; R Di Nardo; A Di Simone; R Di Sipio; D Di Valentino; C Diaconu; M Diamond; F A Dias; M A Diaz; E B Diehl; J Dietrich; S Diglio; A Dimitrievska; J Dingfelder; F Dittus; F Djama; T Djobava; J I Djuvsland; M A B do Vale; D Dobos; M Dobre; C Doglioni; T Dohmae; J Dolejsi; Z Dolezal; B A Dolgoshein; M Donadelli; S Donati; P Dondero; J Donini; J Dopke; A Doria; M T Dova; A T Doyle; E Drechsler; M Dris; E Dubreuil; E Duchovni; G Duckeck; O A Ducu; D Duda; A Dudarev; L Duflot; L Duguid; M Dührssen; M Dunford; H Duran Yildiz; M Düren; A Durglishvili; D Duschinger; M Dyndal; C Eckardt; K M Ecker; R C Edgar; W Edson; N C Edwards; W Ehrenfeld; T Eifert; G Eigen; K Einsweiler; T Ekelof; M El Kacimi; M Ellert; S Elles; F Ellinghaus; A A Elliot; N Ellis; J Elmsheuser; M Elsing; D Emeliyanov; Y Enari; O C Endner; M Endo; R Engelmann; J Erdmann; A Ereditato; G Ernis; J Ernst; M Ernst; S Errede; E Ertel; M Escalier; H Esch; C Escobar; B Esposito; A I Etienvre; E Etzion; H Evans; A Ezhilov; L Fabbri; G Facini; R M Fakhrutdinov; S Falciano; R J Falla; J Faltova; Y Fang; M Fanti; A Farbin; A Farilla; T Farooque; S Farrell; S M Farrington; P Farthouat; F Fassi; P Fassnacht; D Fassouliotis; M Faucci Giannelli; A Favareto; L Fayard; P Federic; O L Fedin; W Fedorko; S Feigl; L Feligioni; C Feng; E J Feng; H Feng; A B Fenyuk; P Fernandez Martinez; S Fernandez Perez; S Ferrag; J Ferrando; A Ferrari; P Ferrari; R Ferrari; D E Ferreira de Lima; A Ferrer; D Ferrere; C Ferretti; A Ferretto Parodi; M Fiascaris; F Fiedler; A Filipčič; M Filipuzzi; F Filthaut; M Fincke-Keeler; K D Finelli; M C N Fiolhais; L Fiorini; A Firan; A Fischer; C Fischer; J Fischer; W C Fisher; E A Fitzgerald; M Flechl; I Fleck; P Fleischmann; S Fleischmann; G T Fletcher; G Fletcher; T Flick; A Floderus; L R Flores Castillo; M J Flowerdew; A Formica; A Forti; D Fournier; H Fox; S Fracchia; P Francavilla; M Franchini; D Francis; L Franconi; M Franklin; M Fraternali; D Freeborn; S T French; F Friedrich; D Froidevaux; J A Frost; C Fukunaga; E Fullana Torregrosa; B G Fulsom; J Fuster; C Gabaldon; O Gabizon; A Gabrielli; A Gabrielli; S Gadatsch; S Gadomski; G Gagliardi; P Gagnon; C Galea; B Galhardo; E J Gallas; B J Gallop; P Gallus; G Galster; K K Gan; J Gao; Y Gao; Y S Gao; F M Garay Walls; F Garberson; C García; J E García Navarro; M Garcia-Sciveres; R W Gardner; N Garelli; V Garonne; C Gatti; A Gaudiello; G Gaudio; B Gaur; L Gauthier; P Gauzzi; I L Gavrilenko; C Gay; G Gaycken; E N Gazis; P Ge; Z Gecse; C N P Gee; D A A Geerts; Ch Geich-Gimbel; M P Geisler; C Gemme; M H Genest; S Gentile; M George; S George; D Gerbaudo; A Gershon; H Ghazlane; B Giacobbe; S Giagu; V Giangiobbe; P Giannetti; B Gibbard; S M Gibson; M Gilchriese; T P S Gillam; D Gillberg; G Gilles; D M Gingrich; N Giokaris; M P Giordani; F M Giorgi; F M Giorgi; P F Giraud; P Giromini; D Giugni; C Giuliani; M Giulini; B K Gjelsten; S Gkaitatzis; I Gkialas; E L Gkougkousis; L K Gladilin; C Glasman; J Glatzer; P C F Glaysher; A Glazov; M Goblirsch-Kolb; J R Goddard; J Godlewski; S Goldfarb; T Golling; D Golubkov; A Gomes; R Gonçalo; J Goncalves Pinto Firmino Da Costa; L Gonella; S González de la Hoz; G Gonzalez Parra; S Gonzalez-Sevilla; L Goossens; P A Gorbounov; H A Gordon; I Gorelov; B Gorini; E Gorini; A Gorišek; E Gornicki; A T Goshaw; C Gössling; M I Gostkin; D Goujdami; A G Goussiou; N Govender; H M X Grabas; L Graber; I Grabowska-Bold; P Grafström; K-J Grahn; J Gramling; E Gramstad; S Grancagnolo; V Grassi; V Gratchev; H M Gray; E Graziani; Z D Greenwood; K Gregersen; I M Gregor; P Grenier; J Griffiths; A A Grillo; K Grimm; S Grinstein; Ph Gris; J-F Grivaz; J P Grohs; A Grohsjean; E Gross; J Grosse-Knetter; G C Grossi; Z J Grout; L Guan; J Guenther; F Guescini; D Guest; O Gueta; E Guido; T Guillemin; S Guindon; U Gul; C Gumpert; J Guo; S Gupta; P Gutierrez; N G Gutierrez Ortiz; C Gutschow; C Guyot; C Gwenlan; C B Gwilliam; A Haas; C Haber; H K Hadavand; N Haddad; P Haefner; S Hageböck; Z Hajduk; H Hakobyan; M Haleem; J Haley; D Hall; G Halladjian; G D Hallewell; K Hamacher; P Hamal; K Hamano; M Hamer; A Hamilton; S Hamilton; G N Hamity; P G Hamnett; L Han; K Hanagaki; K Hanawa; M Hance; P Hanke; R Hanna; J B Hansen; J D Hansen; M C Hansen; P H Hansen; K Hara; A S Hard; T Harenberg; F Hariri; S Harkusha; R D Harrington; P F Harrison; F Hartjes; M Hasegawa; S Hasegawa; Y Hasegawa; A Hasib; S Hassani; S Haug; R Hauser; L Hauswald; M Havranek; C M Hawkes; R J Hawkings; A D Hawkins; T Hayashi; D Hayden; C P Hays; J M Hays; H S Hayward; S J Haywood; S J Head; T Heck; V Hedberg; L Heelan; S Heim; T Heim; B Heinemann; L Heinrich; J Hejbal; L Helary; S Hellman; D Hellmich; C Helsens; J Henderson; R C W Henderson; Y Heng; C Hengler; A Henrichs; A M Henriques Correia; S Henrot-Versille; G H Herbert; Y Hernández Jiménez; R Herrberg-Schubert; G Herten; R Hertenberger; L Hervas; G G Hesketh; N P Hessey; J W Hetherly; R Hickling; E Higón-Rodriguez; E Hill; J C Hill; K H Hiller; S J Hillier; I Hinchliffe; E Hines; R R Hinman; M Hirose; D Hirschbuehl; J Hobbs; N Hod; M C Hodgkinson; P Hodgson; A Hoecker; M R Hoeferkamp; F Hoenig; M Hohlfeld; D Hohn; T R Holmes; T M Hong; L Hooft van Huysduynen; W H Hopkins; Y Horii; A J Horton; J-Y Hostachy; S Hou; A Hoummada; J Howard; J Howarth; M Hrabovsky; I Hristova; J Hrivnac; T Hryn'ova; A Hrynevich; C Hsu; P J Hsu; S-C Hsu; D Hu; Q Hu; X Hu; Y Huang; Z Hubacek; F Hubaut; F Huegging; T B Huffman; E W Hughes; G Hughes; M Huhtinen; T A Hülsing; N Huseynov; J Huston; J Huth; G Iacobucci; G Iakovidis; I Ibragimov; L Iconomidou-Fayard; E Ideal; Z Idrissi; P Iengo; O Igonkina; T Iizawa; Y Ikegami; K Ikematsu; M Ikeno; Y Ilchenko; D Iliadis; N Ilic; Y Inamaru; T Ince; P Ioannou; M Iodice; K Iordanidou; V Ippolito; A Irles Quiles; C Isaksson; M Ishino; M Ishitsuka; R Ishmukhametov; C Issever; S Istin; J M Iturbe Ponce; R Iuppa; J Ivarsson; W Iwanski; H Iwasaki; J M Izen; V Izzo; S Jabbar; B Jackson; M Jackson; P Jackson; M R Jaekel; V Jain; K Jakobs; S Jakobsen; T Jakoubek; J Jakubek; D O Jamin; D K Jana; E Jansen; R W Jansky; J Janssen; M Janus; G Jarlskog; N Javadov; T Javůrek; L Jeanty; J Jejelava; G-Y Jeng; D Jennens; P Jenni; J Jentzsch; C Jeske; S Jézéquel; H Ji; J Jia; Y Jiang; S Jiggins; J Jimenez Pena; S Jin; A Jinaru; O Jinnouchi; M D Joergensen; P Johansson; K A Johns; K Jon-And; G Jones; R W L Jones; T J Jones; J Jongmanns; P M Jorge; K D Joshi; J Jovicevic; X Ju; C A Jung; P Jussel; A Juste Rozas; M Kaci; A Kaczmarska; M Kado; H Kagan; M Kagan; S J Kahn; E Kajomovitz; C W Kalderon; S Kama; A Kamenshchikov; N Kanaya; M Kaneda; S Kaneti; V A Kantserov; J Kanzaki; B Kaplan; A Kapliy; D Kar; K Karakostas; A Karamaoun; N Karastathis; M J Kareem; M Karnevskiy; S N Karpov; Z M Karpova; K Karthik; V Kartvelishvili; A N Karyukhin; L Kashif; R D Kass; A Kastanas; Y Kataoka; A Katre; J Katzy; K Kawagoe; T Kawamoto; G Kawamura; S Kazama; V F Kazanin; M Y Kazarinov; R Keeler; R Kehoe; J S Keller; J J Kempster; H Keoshkerian; O Kepka; B P Kerševan; S Kersten; R A Keyes; F Khalil-Zada; H Khandanyan; A Khanov; A G Kharlamov; T J Khoo; V Khovanskiy; E Khramov; J Khubua; H Y Kim; H Kim; S H Kim; Y Kim; N Kimura; O M Kind; B T King; M King; R S B King; S B King; J Kirk; A E Kiryunin; T Kishimoto; D Kisielewska; F Kiss; K Kiuchi; O Kivernyk; E Kladiva; M H Klein; M Klein; U Klein; K Kleinknecht; P Klimek; A Klimentov; R Klingenberg; J A Klinger; T Klioutchnikova; P F Klok; E-E Kluge; P Kluit; S Kluth; E Kneringer; E B F G Knoops; A Knue; A Kobayashi; D Kobayashi; T Kobayashi; M Kobel; M Kocian; P Kodys; T Koffas; E Koffeman; L A Kogan; S Kohlmann; Z Kohout; T Kohriki; T Koi; H Kolanoski; I Koletsou; A A Komar; Y Komori; T Kondo; N Kondrashova; K Köneke; A C König; S König; T Kono; R Konoplich; N Konstantinidis; R Kopeliansky; S Koperny; L Köpke; A K Kopp; K Korcyl; K Kordas; A Korn; A A Korol; I Korolkov; E V Korolkova; O Kortner; S Kortner; T Kosek; V V Kostyukhin; V M Kotov; A Kotwal; A Kourkoumeli-Charalampidi; C Kourkoumelis; V Kouskoura; A Koutsman; R Kowalewski; T Z Kowalski; W Kozanecki; A S Kozhin; V A Kramarenko; G Kramberger; D Krasnopevtsev; M W Krasny; A Krasznahorkay; J K Kraus; A Kravchenko; S Kreiss; M Kretz; J Kretzschmar; K Kreutzfeldt; P Krieger; K Krizka; K Kroeninger; H Kroha; J Kroll; J Kroseberg; J Krstic; U Kruchonak; H Krüger; N Krumnack; Z V Krumshteyn; A Kruse; M C Kruse; M Kruskal; T Kubota; H Kucuk; S Kuday; S Kuehn; A Kugel; F Kuger; A Kuhl; T Kuhl; V Kukhtin; Y Kulchitsky; S Kuleshov; M Kuna; T Kunigo; A Kupco; H Kurashige; Y A Kurochkin; R Kurumida; V Kus; E S Kuwertz; M Kuze; J Kvita; T Kwan; D Kyriazopoulos; A La Rosa; J L La Rosa Navarro; L La Rotonda; C Lacasta; F Lacava; J Lacey; H Lacker; D Lacour; V R Lacuesta; E Ladygin; R Lafaye; B Laforge; T Lagouri; S Lai; L Lambourne; S Lammers; C L Lampen; W Lampl; E Lançon; U Landgraf; M P J Landon; V S Lang; J C Lange; A J Lankford; F Lanni; K Lantzsch; S Laplace; C Lapoire; J F Laporte; T Lari; F Lasagni Manghi; M Lassnig; P Laurelli; W Lavrijsen; A T Law; P Laycock; O Le Dortz; E Le Guirriec; E Le Menedeu; M LeBlanc; T LeCompte; F Ledroit-Guillon; C A Lee; S C Lee; L Lee; G Lefebvre; M Lefebvre; F Legger; C Leggett; A Lehan; G Lehmann Miotto; X Lei; W A Leight; A Leisos; A G Leister; M A L Leite; R Leitner; D Lellouch; B Lemmer; K J C Leney; T Lenz; B Lenzi; R Leone; S Leone; C Leonidopoulos; S Leontsinis; C Leroy; C G Lester; M Levchenko; J Levêque; D Levin; L J Levinson; M Levy; A Lewis; A M Leyko; M Leyton; B Li; H Li; H L Li; L Li; L Li; S Li; Y Li; Z Liang; H Liao; B Liberti; A Liblong; P Lichard; K Lie; J Liebal; W Liebig; C Limbach; A Limosani; S C Lin; T H Lin; F Linde; B E Lindquist; J T Linnemann; E Lipeles; A Lipniacka; M Lisovyi; T M Liss; D Lissauer; A Lister; A M Litke; B Liu; D Liu; J Liu; J B Liu; K Liu; L Liu; M Liu; M Liu; Y Liu; M Livan; A Lleres; J Llorente Merino; S L Lloyd; F Lo Sterzo; E Lobodzinska; P Loch; W S Lockman; F K Loebinger; A E Loevschall-Jensen; A Loginov; T Lohse; K Lohwasser; M Lokajicek; B A Long; J D Long; R E Long; K A Looper; L Lopes; D Lopez Mateos; B Lopez Paredes; I Lopez Paz; J Lorenz; N Lorenzo Martinez; M Losada; P Loscutoff; P J Lösel; X Lou; A Lounis; J Love; P A Love; N Lu; H J Lubatti; C Luci; A Lucotte; F Luehring; W Lukas; L Luminari; O Lundberg; B Lund-Jensen; D Lynn; R Lysak; E Lytken; H Ma; L L Ma; G Maccarrone; A Macchiolo; C M Macdonald; J Machado Miguens; D Macina; D Madaffari; R Madar; H J Maddocks; W F Mader; A Madsen; S Maeland; T Maeno; A Maevskiy; E Magradze; K Mahboubi; J Mahlstedt; C Maiani; C Maidantchik; A A Maier; T Maier; A Maio; S Majewski; Y Makida; N Makovec; B Malaescu; Pa Malecki; V P Maleev; F Malek; U Mallik; D Malon; C Malone; S Maltezos; V M Malyshev; S Malyukov; J Mamuzic; G Mancini; B Mandelli; L Mandelli; I Mandić; R Mandrysch; J Maneira; A Manfredini; L Manhaes de Andrade Filho; J Manjarres Ramos; A Mann; P M Manning; A Manousakis-Katsikakis; B Mansoulie; R Mantifel; M Mantoani; L Mapelli; L March; G Marchiori; M Marcisovsky; C P Marino; M Marjanovic; F Marroquim; S P Marsden; Z Marshall; L F Marti; S Marti-Garcia; B Martin; T A Martin; V J Martin; B Martin Dit Latour; M Martinez; S Martin-Haugh; V S Martoiu; A C Martyniuk; M Marx; F Marzano; A Marzin; L Masetti; T Mashimo; R Mashinistov; J Masik; A L Maslennikov; I Massa; L Massa; N Massol; P Mastrandrea; A Mastroberardino; T Masubuchi; P Mättig; J Mattmann; J Maurer; S J Maxfield; D A Maximov; R Mazini; S M Mazza; L Mazzaferro; G Mc Goldrick; S P Mc Kee; A McCarn; R L McCarthy; T G McCarthy; N A McCubbin; K W McFarlane; 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K A Parker; F Parodi; J A Parsons; U Parzefall; E Pasqualucci; S Passaggio; F Pastore; Fr Pastore; G Pásztor; S Pataraia; N D Patel; J R Pater; T Pauly; J Pearce; B Pearson; L E Pedersen; M Pedersen; S Pedraza Lopez; R Pedro; S V Peleganchuk; D Pelikan; H Peng; B Penning; J Penwell; D V Perepelitsa; E Perez Codina; M T Pérez García-Estañ; L Perini; H Pernegger; S Perrella; R Peschke; V D Peshekhonov; K Peters; R F Y Peters; B A Petersen; T C Petersen; E Petit; A Petridis; C Petridou; E Petrolo; F Petrucci; N E Pettersson; R Pezoa; P W Phillips; G Piacquadio; E Pianori; A Picazio; E Piccaro; M Piccinini; M A Pickering; R Piegaia; D T Pignotti; J E Pilcher; A D Pilkington; J Pina; M Pinamonti; J L Pinfold; A Pingel; B Pinto; S Pires; M Pitt; C Pizio; L Plazak; M-A Pleier; V Pleskot; E Plotnikova; P Plucinski; D Pluth; R Poettgen; L Poggioli; D Pohl; G Polesello; A Policicchio; R Polifka; A Polini; C S Pollard; V Polychronakos; K Pommès; L Pontecorvo; B G Pope; G A Popeneciu; D S Popovic; A Poppleton; S Pospisil; K Potamianos; I N Potrap; C J Potter; C T Potter; G Poulard; J Poveda; V Pozdnyakov; P Pralavorio; A Pranko; S Prasad; S Prell; D Price; L E Price; M Primavera; S Prince; M Proissl; K Prokofiev; F Prokoshin; E Protopapadaki; S Protopopescu; J Proudfoot; M Przybycien; E Ptacek; D Puddu; E Pueschel; D Puldon; M Purohit; P Puzo; J Qian; G Qin; Y Qin; A Quadt; D R Quarrie; W B Quayle; M Queitsch-Maitland; D Quilty; S Raddum; V Radeka; V Radescu; S K Radhakrishnan; P Radloff; P Rados; F Ragusa; G Rahal; S Rajagopalan; M Rammensee; C Rangel-Smith; F Rauscher; S Rave; T Ravenscroft; M Raymond; A L Read; N P Readioff; D M Rebuzzi; A Redelbach; G Redlinger; R Reece; K Reeves; L Rehnisch; H Reisin; M Relich; C Rembser; H Ren; A Renaud; M Rescigno; S Resconi; O L Rezanova; P Reznicek; R Rezvani; R Richter; S Richter; E Richter-Was; O Ricken; M Ridel; P Rieck; C J Riegel; J Rieger; M Rijssenbeek; A Rimoldi; L Rinaldi; B Ristić; E Ritsch; I Riu; F Rizatdinova; E Rizvi; S H Robertson; A Robichaud-Veronneau; D Robinson; J E M Robinson; A Robson; C Roda; S Roe; O Røhne; S Rolli; A Romaniouk; M Romano; S M Romano Saez; E Romero Adam; N Rompotis; M Ronzani; L Roos; E Ros; S Rosati; K Rosbach; P Rose; P L Rosendahl; O Rosenthal; V Rossetti; E Rossi; L P Rossi; R Rosten; M Rotaru; I Roth; J Rothberg; D Rousseau; C R Royon; A Rozanov; Y Rozen; X Ruan; F Rubbo; I Rubinskiy; V I Rud; C Rudolph; M S Rudolph; F Rühr; A Ruiz-Martinez; Z Rurikova; N A Rusakovich; A Ruschke; H L Russell; J P Rutherfoord; N Ruthmann; Y F Ryabov; M Rybar; G Rybkin; N C Ryder; A F Saavedra; G Sabato; S Sacerdoti; A Saddique; H F-W Sadrozinski; R Sadykov; F Safai Tehrani; M Saimpert; H Sakamoto; Y Sakurai; G Salamanna; A Salamon; M Saleem; D Salek; P H Sales De Bruin; D Salihagic; A Salnikov; J Salt; D Salvatore; F Salvatore; A Salvucci; A Salzburger; D Sampsonidis; A Sanchez; J Sánchez; V Sanchez Martinez; H Sandaker; R L Sandbach; H G Sander; M P Sanders; M Sandhoff; C Sandoval; R Sandstroem; D P C Sankey; M Sannino; A Sansoni; C Santoni; R Santonico; H Santos; I Santoyo Castillo; K Sapp; A Sapronov; J G Saraiva; B Sarrazin; O Sasaki; Y Sasaki; K Sato; G Sauvage; E Sauvan; G Savage; P Savard; C Sawyer; L Sawyer; J Saxon; C Sbarra; A Sbrizzi; T Scanlon; D A Scannicchio; M Scarcella; V Scarfone; J Schaarschmidt; P Schacht; D Schaefer; R Schaefer; J Schaeffer; S Schaepe; S Schaetzel; U Schäfer; A C Schaffer; D Schaile; R D Schamberger; V Scharf; V A Schegelsky; D Scheirich; M Schernau; C Schiavi; C Schillo; M Schioppa; S Schlenker; E Schmidt; K Schmieden; C Schmitt; S Schmitt; S Schmitt; B Schneider; Y J Schnellbach; U Schnoor; L Schoeffel; A Schoening; B D Schoenrock; E Schopf; A L S Schorlemmer; M Schott; D Schouten; J Schovancova; S Schramm; M Schreyer; C Schroeder; N Schuh; M J Schultens; H-C Schultz-Coulon; H Schulz; M Schumacher; B A Schumm; Ph Schune; C Schwanenberger; A Schwartzman; T A Schwarz; Ph Schwegler; Ph Schwemling; R Schwienhorst; J Schwindling; T Schwindt; M Schwoerer; F G Sciacca; E Scifo; G Sciolla; F Scuri; F Scutti; J Searcy; G Sedov; E Sedykh; P Seema; S C Seidel; A Seiden; F Seifert; J M Seixas; G Sekhniaidze; K Sekhon; S J Sekula; K E Selbach; D M Seliverstov; N Semprini-Cesari; C Serfon; L Serin; L Serkin; T Serre; M Sessa; R Seuster; H Severini; T Sfiligoj; F Sforza; A Sfyrla; E Shabalina; M Shamim; L Y Shan; R Shang; J T Shank; M Shapiro; P B Shatalov; K Shaw; S M Shaw; A Shcherbakova; C Y Shehu; P Sherwood; L Shi; S Shimizu; C O Shimmin; M Shimojima; M Shiyakova; A Shmeleva; D Shoaleh Saadi; M J Shochet; S Shojaii; S Shrestha; E Shulga; M A Shupe; S Shushkevich; P Sicho; O Sidiropoulou; D Sidorov; A Sidoti; F Siegert; Dj Sijacki; J Silva; Y Silver; S B Silverstein; V Simak; O Simard; Lj Simic; S Simion; E Simioni; B Simmons; D Simon; R Simoniello; P Sinervo; N B Sinev; G Siragusa; A N Sisakyan; S Yu Sivoklokov; J Sjölin; T B Sjursen; M B Skinner; H P Skottowe; P Skubic; M Slater; T Slavicek; M Slawinska; K Sliwa; V Smakhtin; B H Smart; L Smestad; S Yu Smirnov; Y Smirnov; L N Smirnova; O Smirnova; M N K Smith; M Smizanska; K Smolek; A A Snesarev; G Snidero; S Snyder; R Sobie; F Socher; A Soffer; D A Soh; C A Solans; M Solar; J Solc; E Yu Soldatov; U Soldevila; A A Solodkov; A Soloshenko; O V Solovyanov; V Solovyev; P Sommer; H Y Song; N Soni; A Sood; A Sopczak; B Sopko; V Sopko; V Sorin; D Sosa; M Sosebee; C L Sotiropoulou; R Soualah; P Soueid; A M Soukharev; D South; S Spagnolo; M Spalla; F Spanò; W R Spearman; F Spettel; R Spighi; G Spigo; L A Spiller; M Spousta; T Spreitzer; R D St Denis; S Staerz; J Stahlman; R Stamen; S Stamm; E Stanecka; C Stanescu; M Stanescu-Bellu; M M Stanitzki; S Stapnes; E A Starchenko; J Stark; P Staroba; P Starovoitov; R Staszewski; P Stavina; P Steinberg; B Stelzer; H J Stelzer; O Stelzer-Chilton; H Stenzel; S Stern; G A Stewart; J A Stillings; M C Stockton; M Stoebe; G Stoicea; P Stolte; S Stonjek; A R Stradling; A Straessner; M E Stramaglia; J Strandberg; S Strandberg; A Strandlie; E Strauss; M Strauss; P Strizenec; R Ströhmer; D M Strom; R Stroynowski; A Strubig; S A Stucci; B Stugu; N A Styles; D Su; J Su; R Subramaniam; A Succurro; Y Sugaya; C Suhr; M Suk; V V Sulin; S Sultansoy; T Sumida; S Sun; X Sun; J E Sundermann; K Suruliz; G Susinno; M R Sutton; S Suzuki; Y Suzuki; M Svatos; S Swedish; M Swiatlowski; I Sykora; T Sykora; D Ta; C Taccini; K Tackmann; J Taenzer; A Taffard; R Tafirout; N Taiblum; H Takai; R Takashima; H Takeda; T Takeshita; Y Takubo; M Talby; A A Talyshev; J Y C Tam; K G Tan; J Tanaka; R Tanaka; S Tanaka; S Tanaka; B B Tannenwald; N Tannoury; S Tapprogge; S Tarem; F Tarrade; G F Tartarelli; P Tas; M Tasevsky; T Tashiro; E Tassi; A Tavares Delgado; Y Tayalati; F E Taylor; G N Taylor; W Taylor; F A Teischinger; M Teixeira Dias Castanheira; P Teixeira-Dias; K K Temming; H Ten Kate; P K Teng; J J Teoh; F Tepel; S Terada; K Terashi; J Terron; S Terzo; M Testa; R J Teuscher; J Therhaag; T Theveneaux-Pelzer; J P Thomas; J Thomas-Wilsker; E N Thompson; P D Thompson; R J Thompson; A S Thompson; L A Thomsen; E Thomson; M Thomson; R P Thun; M J Tibbetts; R E Ticse Torres; V O Tikhomirov; Yu A Tikhonov; S Timoshenko; E Tiouchichine; P Tipton; S Tisserant; T Todorov; S Todorova-Nova; J Tojo; S Tokár; K Tokushuku; K Tollefson; E Tolley; L Tomlinson; M Tomoto; L Tompkins; K Toms; E Torrence; H Torres; E Torró Pastor; J Toth; F Touchard; D R Tovey; T Trefzger; L Tremblet; A Tricoli; I M Trigger; S Trincaz-Duvoid; M F Tripiana; W Trischuk; B Trocmé; C Troncon; M Trottier-McDonald; M Trovatelli; P True; L Truong; M Trzebinski; A Trzupek; C Tsarouchas; J C-L Tseng; P V Tsiareshka; D Tsionou; G Tsipolitis; N Tsirintanis; S Tsiskaridze; V Tsiskaridze; E G Tskhadadze; I I Tsukerman; V Tsulaia; S Tsuno; D Tsybychev; A Tudorache; V Tudorache; A N Tuna; S A Tupputi; S Turchikhin; D Turecek; R Turra; A J Turvey; P M Tuts; A Tykhonov; M Tylmad; M Tyndel; I Ueda; R Ueno; M Ughetto; M Ugland; M Uhlenbrock; F Ukegawa; G Unal; A Undrus; G Unel; F C Ungaro; Y Unno; C Unverdorben; J Urban; P Urquijo; P Urrejola; G Usai; A Usanova; L Vacavant; V Vacek; B Vachon; C Valderanis; N Valencic; S Valentinetti; A Valero; L Valery; S Valkar; E Valladolid Gallego; S Vallecorsa; J A Valls Ferrer; W Van Den Wollenberg; P C Van Der Deijl; R van der Geer; H van der Graaf; R Van Der Leeuw; N van Eldik; P van Gemmeren; J Van Nieuwkoop; I van Vulpen; M C van Woerden; M Vanadia; W Vandelli; R Vanguri; A Vaniachine; F Vannucci; G Vardanyan; R Vari; E W Varnes; T Varol; D Varouchas; A Vartapetian; K E Varvell; F Vazeille; T Vazquez Schroeder; J Veatch; F Veloso; T Velz; S Veneziano; A Ventura; D Ventura; M Venturi; N Venturi; A Venturini; V Vercesi; M Verducci; W Verkerke; J C Vermeulen; A Vest; M C Vetterli; O Viazlo; I Vichou; T Vickey; O E Vickey Boeriu; G H A Viehhauser; S Viel; R Vigne; M Villa; M Villaplana Perez; E Vilucchi; M G Vincter; V B Vinogradov; I Vivarelli; F Vives Vaque; S Vlachos; D Vladoiu; M Vlasak; M Vogel; P Vokac; G Volpi; M Volpi; H von der Schmitt; H von Radziewski; E von Toerne; V Vorobel; K Vorobev; M Vos; R Voss; J H Vossebeld; N Vranjes; M Vranjes Milosavljevic; V Vrba; M Vreeswijk; R Vuillermet; I Vukotic; Z Vykydal; P Wagner; W Wagner; H Wahlberg; S Wahrmund; J Wakabayashi; J Walder; R Walker; W Walkowiak; C Wang; F Wang; H Wang; H Wang; J Wang; J Wang; K Wang; R Wang; S M Wang; T Wang; X Wang; C Wanotayaroj; A Warburton; C P Ward; D R Wardrope; M Warsinsky; A Washbrook; C Wasicki; P M Watkins; A T Watson; I J Watson; M F Watson; G Watts; S Watts; B M Waugh; S Webb; M S Weber; S W Weber; J S Webster; A R Weidberg; B Weinert; J Weingarten; C Weiser; H Weits; P S Wells; T Wenaus; T Wengler; S Wenig; N Wermes; M Werner; P Werner; M Wessels; J Wetter; K Whalen; A M Wharton; A White; M J White; R White; S White; D Whiteson; F J Wickens; W Wiedenmann; M Wielers; P Wienemann; C Wiglesworth; L A M Wiik-Fuchs; A Wildauer; H G Wilkens; H H Williams; S Williams; C Willis; S Willocq; A Wilson; J A Wilson; I Wingerter-Seez; F Winklmeier; B T Winter; M Wittgen; J Wittkowski; S J Wollstadt; M W Wolter; H Wolters; B K Wosiek; J Wotschack; M J Woudstra; K W Wozniak; M Wu; M Wu; S L Wu; X Wu; Y Wu; T R Wyatt; B M Wynne; S Xella; D Xu; L Xu; B Yabsley; S Yacoob; R Yakabe; M Yamada; Y Yamaguchi; A Yamamoto; S Yamamoto; T Yamanaka; K Yamauchi; Y Yamazaki; Z Yan; H Yang; H Yang; Y Yang; L Yao; W-M Yao; Y Yasu; E Yatsenko; K H Yau Wong; J Ye; S Ye; I Yeletskikh; A L Yen; E Yildirim; K Yorita; R Yoshida; K Yoshihara; C Young; C J S Young; S Youssef; D R Yu; J Yu; J M Yu; J Yu; L Yuan; A Yurkewicz; I Yusuff; B Zabinski; R Zaidan; A M Zaitsev; J Zalieckas; A Zaman; S Zambito; L Zanello; D Zanzi; C Zeitnitz; M Zeman; A Zemla; K Zengel; O Zenin; T Ženiš; D Zerwas; D Zhang; F Zhang; J Zhang; L Zhang; R Zhang; X Zhang; Z Zhang; X Zhao; Y Zhao; Z Zhao; A Zhemchugov; J Zhong; B Zhou; C Zhou; L Zhou; L Zhou; N Zhou; C G Zhu; H Zhu; J Zhu; Y Zhu; X Zhuang; K Zhukov; A Zibell; D Zieminska; N I Zimine; C Zimmermann; S Zimmermann; Z Zinonos; M Zinser; M Ziolkowski; L Živković; G Zobernig; A Zoccoli; M Zur Nedden; G Zurzolo; L Zwalinski
Journal:  Eur Phys J C Part Fields       Date:  2015-07-17       Impact factor: 4.590

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