M. Aharrouche
University of Mainz
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Featured researches published by M. Aharrouche.
Journal of High Energy Physics | 2013
T. Buanes; T. Burgess; G. Eigen; A. Kastanas; W. Liebig; Anna Lipniacka; Peter Lundgaard Rosendahl; Heidi Sandaker; T. B. Sjursen; Bjarne Stugu; A. Tonoyan; M. Ugland; L. Bugge; T. Buran; D. Cameron; Z. Czyczula; B. K. Gjelsten; E. Gramstad; Esben Lund; F. Ould-Saada; K. Pajchel; Y. Pylypchenko; Alexander Lincoln Read; O. Røhne; Björn Hallvard Samset; L. Smestad; S. Stapnes; A. Strandlie; G. Aad; T. Abajyan
A bstractMass and angular distributions of dijets produced in LHC proton-proton collisions at a centre-of-mass energy
Physical Review D | 2014
G. Aad; T. Abajyan; B. Abbott; J. Abdallah; Samah Abdel Khalek; Ovsat Abdinov; R. Aben; B. Abi; M. Abolins; Hass AbouZeid; T. Buanes; O. Dale; G. Eigen; A. Kastanas; W. Liebig; Anna Lipniacka; Bertrand Martin dit Latour; Peter Lundgaard Rosendahl; Heidi Sandaker; T. B. Sjursen; Bjarne Stugu; M. Ugland; L. Bugge; Magnar Kopangen Bugge; D. Cameron; Z. Czyczula; B. K. Gjelsten; E. Gramstad; F. Ould-Saada; K. Pajchel
\sqrt{s}=7
Journal of High Energy Physics | 2013
T. Buanes; T. Burgess; G. Eigen; A. Kastanas; W. Liebig; Anna Lipniacka; Peter Lundgaard Rosendahl; Heidi Sandaker; T. B. Sjursen; Bjarne Stugu; A. Tonoyan; M. Ugland; L. Bugge; T. Buran; D. Cameron; Z. Czyczula; B. K. Gjelsten; E. Gramstad; Esben Lund; F. Ould-Saada; K. Pajchel; Y. Pylypchenko; Alexander Lincoln Read; O. Røhne; Björn Hallvard Samset; L. Smestad; S. Stapnes; A. Strandlie; G. Aad; T. Abajyan
TeV have been studied with the ATLAS detector using the full 2011 data set with an integrated luminosity of 4.8 fb−1. Dijet masses up to ~ 4.0 TeV have been probed. No resonance-like features have been observed in the dijet mass spectrum, and all angular distributions are consistent with the predictions of QCD. Exclusion limits on six hypotheses of new phenomena have been set at 95% CL in terms of mass or energy scale, as appropriate. These hypotheses include excited quarks below 2.83 TeV, colour octet scalars below 1.86 TeV, heavy W bosons below 1.68 TeV, string resonances below 3.61 TeV, quantum black holes with six extra space-time dimensions for quantum gravity scales below 4.11 TeV, and quark contact interactions below a compositeness scale of 7.6 TeV in a destructive interference scenario.
Physics Letters B | 2012
G. Aad; B. Abbott; J. Abdallah; A. A. Abdelalim; A. Abdesselam; Ovsat Abdinov; B. Abi; M. Abolins; H. Abramowicz; H. Abreu; E. Acerbi; Bobby Samir Acharya; D. L. Adams; T. N. Addy; J. Adelman; M. Aderholz; S. Adomeit; P. Adragna; T. Adye; S. Aefsky; Juan Antonio Aguilar-Saavedra; M. Aharrouche; S. P. Ahlen; F. Ahles; A. Ahmad; M. Ahsan; G. Aielli; T. Akdogan; Torsten Paul Ake Åkesson; G. Akimoto
Measurements of normalized differential cross-sections for top-quark pair production are presented as a function of the top-quark transverse momentum, and of the mass, transverse momentum, and rapidity of the tt̄ system, in proton–proton collisions at a center-of-mass energy of √ s = 7TeV. The dataset corresponds to an integrated luminosity of 4.6 fb−1, recorded in 2011 with the ATLAS detector at the CERN Large Hadron Collider. Events are selected in the lepton+jets channel, requiring exactly one lepton and at least four jets with at least one of the jets tagged as originating from a b-quark. The measured spectra are corrected for detector efficiency and resolution effects and are compared to several Monte Carlo simulations and theory calculations. The results are in fair agreement with the predictions in a wide kinematic range. Nevertheless, data distributions are softer than predicted for higher values of the mass of the tt̄ system and of the top-quark transverse momentum. The measurements can also discriminate among different sets of parton distribution functions. c
Physics Letters B | 2012
G. Aad; B. Abbott; J. Abdallah; A. A. Abdelalim; A. Abdesselam; O. Abdinov; B. Abi; M. Abolins; H. Abramowicz; H. Abreu; E. Acerbi; B. S. Acharya; 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 bstractA search for resonances produced in 7 TeV proton-proton collisions and decaying into top-quark pairs is described. In this Letter events where the top-quark decay produces two massive jets with large transverse momenta recorded with the ATLAS detector at the Large Hadron Collider are considered. Two techniques that rely on jet substructure are used to separate top-quark jets from those arising from light quarks and gluons. In addition, each massive jet is required to have evidence of an associated bottom-quark decay. The data are consistent with the Standard Model, and limits can be set on the production cross section times branching fraction of a Z′ boson and a Kaluza-Klein gluon resonance. These limits exclude, at the 95% credibility level, Z′ bosons with masses 0.70-1.00 TeV as well as 1.28-1.32 TeV and Kaluza-Klein gluons with masses 0.70-1.62 TeV.
Physical Review Letters | 2014
T. Buanes; O. Dale; G. Eigen; A. Kastanas; W. Liebig; Anna Lipniacka; Peter Lundgaard Rosendahl; Heidi Sandaker; T. B. Sjursen; L. Smestad; Bjarne Stugu; M. Ugland; L. Bugge; Magnar Kopangen Bugge; D. Cameron; J. R. Catmore; Z. Czyczula; B. K. Gjelsten; E. Gramstad; F. Ould-Saada; M. Pedersen; Y. Pylypchenko; Alexander Lincoln Read; O. Røhne; S. Stapnes; A. Strandlie; G. Aad; B. Abbott; J. Abdallah; Samah Abdel Khalek
This Letter presents measurements of the differential cross-sections for inclusive electron and muon production in proton-proton collisions at a centre-of-mass energy of root s = 7 TeV, using data collected by the ATLAS detector at the LHC. The muon cross-section is measured as a function of p(T) in the range 4 < p(T) < 100 GeV and within pseudorapidity vertical bar eta vertical bar < 2.5. In addition the electron and muon cross-sections are measured in the range 7 < p(T) < 26 GeV and within vertical bar eta vertical bar < 2.0, excluding 1.37 < vertical bar eta vertical bar < 1.52. Integrated luminosities of 1.3 pb(-1) and 1.4 pb(-1) are used for the electron and muon measurements, respectively. After subtraction of the W/Z/gamma* contribution, the differential cross-sections are found to be in good agreement with theoretical predictions for heavy-flavour production obtained from Fixed Order NLO calculations with NLL high-p(T) resummation, and to be sensitive to the effects of NLL resummation
Journal of High Energy Physics | 2013
T. Buanes; T. Burgess; G. Eigen; A. Kastanas; W. Liebig; Anna Lipniacka; Peter Lundgaard Rosendahl; Heidi Sandaker; T. B. Sjursen; Bjarne Stugu; A. Tonoyan; M. Ugland; L. Bugge; T. Buran; D. Cameron; Z. Czyczula; B. K. Gjelsten; E. Gramstad; Esben Lund; F. Ould-Saada; K. Pajchel; Y. Pylypchenko; Alexander Lincoln Read; O. Røhne; Björn Hallvard Samset; L. Smestad; S. Stapnes; A. Strandlie; G. Aad; T. Abajyan
A measurement is presented of the cross section for the produ cti n of aW boson with one or two jets, of which at least one must be a b-jet, in pp collisions at √ s = 7 TeV. Production via top decay is not included in the signal definition. The measurement is based on 35 pb −1of data collected with the ATLAS detector at the LHC. The W+b-jet cross section is defined for jets reconstructed with the anti -kt clustering algorithm with transverse momentum above 25 GeV and rapidity within±2.1. Theb-jets are identified by reconstructing secondary vertices. The fiducial cross section is measured both for the electron and muon decay chan nel of theW boson and is found to be 10.2 ± 1.9 (stat) ± 2.6 (syst) pb for one lepton flavour. The results are compared with next-to-leading order QCD calculations, which predict a cross section smaller than, though consistent wit h, the measured value.
ieee nuclear science symposium | 2008
R. Achenbach; P. Adragna; M. Aharrouche; V. Andrei; B. Åsman; B. M. Barnett; B. Bauss; M. Bendel; C. Bohm; J.R.A. Booth; J. Bracinik; I.P. Brawn; D. G. Charlton; J. T. Childers; N. J. Collins; C. J. Curtis; A.O. Davis; S. Eckweiler; E. Eisenhandler; P.J.W. Faulkner; J. Fleckner; F. Föhlisch; C. N. P. Gee; A. R. Gillman; C. Goringer; M. Groll; D. R. Hadley; P. Hanke; S. Hellman; A. Hidvegi
Measurements of four-lepton (4`, ` = e, μ) production cross sections at the Z resonance in pp collisions at the LHC with the ATLAS detector are presented. For dilepton and four-lepton invariant mass regionm`+`− > 5 GeV and 80 < m4` < 100 GeV, the measured cross sections are 76±18 (stat) ± 4 (syst) ±1.4 (lumi) fb and 107±9 (stat) ±4 (syst) ±3.0 (lumi) fb at √ s = 7 and 8 TeV, respectively. By subtracting the non-resonant 4` production contributions and normalizing with Z → μ+μ− events, the branching fraction for the Z boson decay to 4` is determined to be (3.20± 0.25 (stat)± 0.13 (syst)) × 10−6, consistent with the Standard Model prediction. c
Prepared for | 2008
D. Prieur; E.-E. Kluge; C. C. Ohm; M. C. Stockton; S. B. Silverstein; Murrough Landon; T. Kuehl; D. G. Charlton; Uli Schaefer; E. Eisenhandler; A. Hidvegi; C. Boehm; K. Schmitt; A. T. Watson; J. T. Childers; N. J. Collins; P. Adragna; Joergen Sjoelin; F. Föhlisch; U. Schäfer; M. Wessels; C.L.A. Tan; M. A. Wildt; J. Sjölin; F. Foehlisch; K. Meier; M. Groll; C. J. Curtis; P. D. Thompson; F. Mueller
A search for direct chargino production in anomaly-mediated supersymmetry breaking scenarios is performed in pp collisions at √ s = 7 TeV using 4.7 fb−1 of data collected with the ATLAS experiment at the LHC. In these models, the lightest chargino is predicted to have a lifetime long enough to be detected in the tracking detectors of collider experiments. This analysis explores such models by searching for chargino decays that result in tracks with few associated hits in the outer region of the tracking system. The transverse-momentum spectrum of candidate tracks is found to be consistent with the expectation from the Standard Model background processes and constraints on chargino properties are obtained.A bstractA search for direct chargino production in anomaly-mediated supersymmetry breaking scenarios is performed in pp collisions at
Physics Letters B | 2013
G. Aad; T. Abajyan; B. Abbott; J. Abdallah; S. Abdel Khalek; A. A. Abdelalim; O. Abdinov; R. Aben; 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; S. Adomeit; P. Adragna; T. Adye; S. Aefsky; J. A. Aguilar-Saavedra; M. Agustoni; M. Aharrouche; S. P. Ahlen; F. Ahles; A. Ahmad; M. Ahsan
\sqrt{s}=7\;\mathrm{TeV}