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Single top quark production at the LHC: Data processing and cross section measurement

Lee, H.C.

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Citation for published version (APA):Lee, H. C. (2013). Single top quark production at the LHC: Data processing and cross section measurement.

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Bibliography

[1] S. L. Glashow. Partial-symmetries of weak interactions. Nuclear Physics,22(4):579–588, 1961.

[2] S. Weinberg. A Model of Leptons. Phys. Rev. Lett., 19:1264–1266, Nov 1967.

[3] A. Salam. Elementary Particle Theory. In Proceedings of the 2005 IFIPinternational conference on Network and Parallel Computing, page 367. Almqvist& Wiksell, 1968.

[4] G. ’t Hooft and M. J. G. Veltman. Regularization and Renormalization of GaugeFields. Nucl.Phys., B44:189–213, 1972.

[5] S. Weinberg. The Quantum Theory of Fields, Volume 1: Foundations. CambridgeUniversity Press, 2005.

[6] S. W. Herb et al. Observation of a Dimuon Resonance at 9.5 GeV in 400 GeVProton-Nucleus Collisions. Phys. Rev. Lett., 39:252–255, Aug 1977.

[7] M. L. Perl et al. Evidence for Anomalous Lepton Production in e+ � e�

Annihilation. Phys. Rev. Lett., 35:1489–1492, Dec 1975.

[8] G. Arnison et al. Experimental observation of isolated large transverse energyelectrons with associated missing energy at

ps = 540 GeV. Physics Letters B,

122(1):103–116, 1983.

[9] G. Arnison et al. Experimental observation of lepton pairs of invariant massaround 95 GeV/c2 at the CERN SPS collider. Physics Letters B, 126(5):398–410,1983.

167

Bibliography

[10] ATLAS Collaboration. Observation of a new particle in the search for theStandard Model Higgs boson with the ATLAS detector at the LHC. Phys.Lett.B,2012, 1207.7214.

[11] CMS Collaboration. Observation of a new boson at a mass of 125 GeV with theCMS experiment at the LHC. Phys.Lett.B, 2012, 1207.7235.

[12] M. Kobayashi and T. Maskawa. CP -Violation in the Renormalizable Theory ofWeak Interaction. Progress of Theoretical Physics, 49(2):652–657, 1973.

[13] H. Harari. A new quark model for hadrons. Physics Letters B, 57(3):265–269,1975.

[14] T. M. Liss and A. Quadt. The Top Quark. http://pdg.lbl.gov/2012/reviews/rpp2012-rev-top-quark.pdf.

[15] http://mstwpdf.hepforge.org/.

[16] G. Sterman, J. Smith, J. C. Collins, J. Whitmore, R. Brock, J. Huston,J. Pumplin, W. K. Tung, H. Weerts, C. P. Yuan, S. Kuhlmann, S. Mishra,J. G. Morfín, F. Olness, J. Owens, J. Qiu, and D. E. Soper. Handbook ofperturbative QCD. Rev. Mod. Phys., 67:157–248, Jan 1995.

[17] N. Kidonakis and B. D. Pecjak. Top-quark production and QCD. 2011,arXiv:1108.6063.

[18] M. Aliev, H. Lacker, U. Langenfeld, S. Moch, P. Uwer, and M. Wiedermann.HATHOR - HAdronic Top and Heavy quarks crOss section calculatoR. ComputerPhysics Communications, 182(4):1034–1046, 2011.

[19] S. Moch and P. Uwer. Theoretical status and prospects for top-quark pairproduction at hadron colliders. Phys. Rev. D, 78:034003, Aug 2008.

[20] M. Cacciari, M. Czakon, M. Mangano, A. Mitov, and P. Nason. Top-pairproduction at hadron colliders with next-to-next-to-leading logarithmic soft-gluon resummation. Physics Letters B, 710(4-5):612–622, 2012.

[21] A. H. Hoang and I. W. Stewart. Top Mass Measurements from Jets andthe Tevatron Top-Quark Mass. Nuclear Physics B - Proceedings Supplements,185(0):220–226, 2008.

[22] CDF Collaboration and D0 Collaboration. Combination of the top-quark massmeasurements from the Tevatron collider. 2012, 1207.1069.

[23] B. W. Harris, E. Laenen, L. Phaf, Z. Sullivan, and S. Weinzierl. Fully differentialsingle-top-quark cross section in next-to-leading order QCD. Phys. Rev. D,66:054024, Sep 2002.

[24] N. Kidonakis. Single top quark production at the Fermilab Tevatron: Thresholdresummation and finite-order soft gluon corrections. Phys. Rev. D, 74:114012,Dec 2006.

168

Bibliography

[25] N. Kidonakis. Higher-order soft gluon corrections in single top quark productionat the CERN LHC. Phys. Rev. D, 75:071501, Apr 2007.

[26] N. Kidonakis. Next-to-next-to-leading-order collinear and soft gluon correctionsfor t-channel single top quark production. Phys. Rev. D, 83:091503, May 2011.

[27] N. Kidonakis. Next-to-next-to-leading logarithm resummation for s-channelsingle top quark production. Phys. Rev. D, 81:054028, Mar 2010.

[28] D0 Collaboration. Observation of Single Top-Quark Production. Phys. Rev.Lett., 103:092001, Aug 2009.

[29] CDF Collaboration. Observation of Electroweak Single Top-Quark Production.Phys. Rev. Lett., 103:092002, Aug 2009.

[30] CDF Collaboration. Measurement of Single Top Quark Production in 7.5 fb�1

of CDF Data Using Neural Networks. CDF Conference Note, 2012.

[31] D0 Collaboration. Model-independent measurement of t-channel single top quarkproduction in pp̄ collisions at

ps = 1.96 TeV. Physics Letters B, 705(4):313–319,

2011.

[32] CDF Collaboration and D0 Collaboration. Combination of CDF and D0 Mea-surements of the Single Top Production Cross Section, 2009, arXiv:0908.2171.

[33] ATLAS Collaboration. Measurement of the t-channel single top-quark productioncross section in pp collisions at

ps = 7 TeV with the ATLAS detector. Physics

Letters B, 717(4-5):330–350, 2012, arXiv:1205.3130.

[34] CMS Collaboration. Measurement of the single-top-quark t-channel cross sectionin pp collisions at

p

(s) = 7 TeV, 2012, arXiv:1209.4533.

[35] A. Belyaev and E. Boos. Single top quark tW + X production at the CERNLHC: A closer look. Phys. Rev. D, 63:034012, Jan 2001.

[36] T. M. P. Tait. tW� mode of single top quark production. Phys. Rev. D,61:034001, Dec 1999.

[37] S. Zhu. Next-to-leading order QCD corrections to bg ! tW� at the CERNLarge Hadron Collider. Physics Letters B, 524(3-4):283–288, 2002.

[38] N. Kidonakis. Two-loop soft anomalous dimensions for single top quark associatedproduction with a W� or H�. Phys. Rev. D, 82:054018, Sep 2010.

[39] ATLAS Collaboration. Measurement of the inclusive W± and Z/�⇤ cross sectionsin the e and µ decay channels in pp collisions at

ps = 7 TeV with the ATLAS

detector. Phys. Rev. D, 85:072004, Apr 2012.

[40] S. Mrenna and C. P. Yuan. QCD radiative decay of the top quark produced inhadron collisions. Phys. Rev. D, 46:1007–1021, Aug 1992.

169

Bibliography

[41] T. M. P. Tait and C. P. Yuan. Single top quark production as a window tophysics beyond the standard model. Phys. Rev. D, 63:014018, Dec 2000.

[42] J. Alwall, R. Frederix, J. M. Gérard, A. Giammanco, M. Herquet, S. Kalinin,E. Kou, V. Lemaitre, and F. Maltoni. Is Vtb ' 1. The European Physical JournalC - Particles and Fields, 49:791–801, 2007. 10.1140/epjc/s10052-006-0137-y.

[43] S. L. Glashow, J. Iliopoulos, and L. Maiani. Weak Interactions with Lepton-Hadron Symmetry. Phys. Rev. D, 2:1285–1292, Oct 1970.

[44] W. Bernreuther. Top quark physics at the LHC, 2008, arXiv:0805.1333.

[45] G. L. Kane, G. A. Ladinsky, and C. P. Yuan. Using the top quark for testingstandard-model polarization and CP predictions. Phys. Rev. D, 45:124–141, Jan1992.

[46] L. Evans and P. Bryant. LHC Machine. Journal of Instrumentation, 3(08):S08001,2008.

[47] Interim Summary Report on the Analysis of the 19 September 2008 Incidentat the LHC. https://edms.cern.ch/file/973073/1/Report_on_080919_incident_at_LHC__2_.pdf.

[48] The public results of the ATLAS experiment - Luminosity. https://twiki.cern.ch/twiki/bin/view/AtlasPublic/LuminosityPublicResults.

[49] ATLAS Collaboration. Improved luminosity determination in p � p collisions atps = 7 TeV using the ATLAS detector at the LHC. 2013, arXiv:1302.4393.

[50] ATLAS Collaboration. The ATLAS Experiment at the CERN Large HadronCollider. Journal of Instrumentation, 3(08):S08003, 2008.

[51] A. Ahmad et al. The silicon microstrip sensors of the ATLAS semiconductortracker. Nuclear Instruments and Methods in Physics Research Section A:Accelerators, Spectrometers, Detectors and Associated Equipment, 578(1):98–118,2007.

[52] The ATLAS TRT Collaboration. The ATLAS Transition Radiation Tracker(TRT) proportional drift tube: design and performance. Journal of Instrumen-tation, 3(02):P02013, 2008.

[53] ATLAS Collaboration. ATLAS Muon Spectrometer: Technical Design Report.ATLAS technical design report. CERN, 1997.

[54] ATLAS Collaboration. ATLAS Magnet System: Technical Design Report,1.ATLAS technical design report. CERN, 1997.

[55] T. Kono. Performance and evolution of the ATLAS TDAQ system with ppcollisions at 7 TeV. In Real Time Conference (RT), 2012 18th IEEE-NPSS,pages 1–7, 2012.

170

Bibliography

[56] G. A. Stewart, J. Boyd, J. F. da Costa, J. Tuggle, and G. Unal. Prompt datareconstruction at the ATLAS experiment. Journal of Physics: Conference Series,396(2):022049, 2012.

[57] M. H. Seymour and M. Marx. Monte Carlo Event Generators, 2013,arXiv:1304.6677.

[58] G. Altarelli and G. Parisi. Asymptotic freedom in parton language. NuclearPhysics B, 126(2):298–318, 1977.

[59] B. Andersson and G. Gustafson and G. Ingelman and T. Sjöstrand. Partonfragmentation and string dynamics. Physics Reports, 97(2-3):31–145, 1983.

[60] I. G. Knowles and G. D. Lafferty. Hadronization in Z0 decay. Journal of PhysicsG: Nuclear and Particle Physics, 23(7):731, 1997.

[61] R. Field and R. C. Group. PYTHIA tune A, HERWIG, and JIMMY in Run 2at CDF. 2005, hep-ph/0510198.

[62] T. Sjöstrand, S. Mrenna, and P. Skands. PYTHIA 6.4 physics and manual.Journal of High Energy Physics, 2006(05):026, 2006.

[63] G. Corcella, I. G. Knowles, G. Marchesini, S. Moretti, K. Odagiri, P. Richardson,M. H. Seymour, and B. R. Webber. HERWIG 6: an event generator for hadronemission reactions with interfering gluons (including supersymmetric processes).Journal of High Energy Physics, 2001(01):010, 2001.

[64] M. L. Mangano, F. P., A. D. Polosa, M. Moretti, and R. Pittau. ALPGEN, agenerator for hard multiparton processes in hadronic collisions. Journal of HighEnergy Physics, 2003(07):001, 2003.

[65] B. P. Kersevan and E. Richter-Wa̧s. The Monte Carlo event generator AcerMCversions 2.0 to 3.8 with interfaces to PYTHIA 6.4, HERWIG 6.5 and ARIADNE4.1. Computer Physics Communications, 184(3):919–985, 2013.

[66] S. Frixione, P. Nason, and B. R. Webber. Matching NLO QCD and parton show-ers in heavy flavour production. Journal of High Energy Physics, 2003(08):007,2003.

[67] S. Alioli, P. Nason, C. Oleari, and R. Re. A general framework for implementingNLO calculations in shower Monte Carlo programs: the POWHEG BOX. Journalof High Energy Physics, 2010(6):1–58, 2010.

[68] S. Agostinelli et al. Geant4 - a simulation toolkit. Nuclear Instruments andMethods in Physics Research Section A: Accelerators, Spectrometers, Detectorsand Associated Equipment, 506(3):250–303, 2003.

[69] ATLAS Collaboration. The ATLAS Simulation Infrastructure. The EuropeanPhysical Journal C, 70(3):823–874, 2010.

171

Bibliography

[70] P. M. Nadolsky, H. L. Lai, Q. H. Cao, J. Huston, J. Pumplin, D. Stump,W. K. Tung, and C. P. Yuan. Implications of CTEQ global analysis for colliderobservables. Phys. Rev. D, 78:013004, Jul 2008.

[71] J. M. Butterworth, J. R. Forshaw, and M. H. Seymour. Multiparton interactionsin photoproduction at HERA. Zeitschrift für Physik C: Particles and Fields,72(4):637–646, 1996.

[72] S. Frixione, F. Stoeckli, P. Torrielli, and B. R. Webber. NLO QCD correctionsin Herwig++ with MC@NLO. Journal of High Energy Physics, 2011(1):1–27,2011.

[73] C. D. White. Single Top Production in the Wt mode with MC@NLO, 2009,arXiv:0905.2066.

[74] J. Pumplin, D. R. Stump, J. Huston, H. L. Lai, P. M. Nadolsky, and W. K.Tung. New Generation of Parton Distributions with Uncertainties from GlobalQCD Analysis. Journal of High Energy Physics, 2002(07):012, 2002.

[75] C. Anastasiou, L. Dixon, K. Melnikov, and F. Petriello. High-precision QCDat hadron colliders: Electroweak gauge boson rapidity distributions at next-to-next-to leading order. Phys. Rev. D, 69:094008, May 2004.

[76] J. M. Campbell and R. K. Ellis. MCFM for the Tevatron and the LHC. InNuclear Physics B - Proceedings Supplements, volume 205-206, pages 10–15,2010.

[77] ATLAS collaboration. Electron performance measurements with the ATLASdetector using the 2010 LHC proton-proton collision data. The European PhysicalJournal C, 72(3), 2012.

[78] ATLAS Collaboration. Performance of the ATLAS Electron and Photon Triggerin p � p Collisions at

ps = 7 TeV. Technical Report ATLAS-CONF-2012-048,

CERN, Geneva, May 2012.

[79] ATLAS Collaboration. Expected performance of the ATLAS experiment: detector,trigger and physics. CERN, Geneva, 2009, arXiv:0901.0512.

[80] ATLAS Collaboration. Electron efficiency measurements in early 2012 data.Technical Report ATLAS-COM-PHYS-2011-783, CERN, Geneva, June 2012.

[81] ATLAS Collaboration. Electron identification efficiency dependence on pileup(update). Technical Report ATLAS-COM-PHYS-2012-260, CERN, Geneva,March 2012.

[82] ATLAS Collaboration. Object selection and calibration, background estimationsand MC samples for the Winter 2012 Top Quark analyses with 2011 data.(ATL-COM-PHYS-2012-224), May 2012.

172

Bibliography

[83] Calibrated z ! e+e� mass with 2011 data. Technical Report ATL-COM-PHYS-2011-1637, CERN, Geneva, December 2011.

[84] ALEPH Collaboration and DELPHI Collaboration and L3 Collaboration andOPAL Collaboration and LEP Electroweak Working Group and SLD ElectroweakGroup and SLD Heavy Flavour Group. Precision electroweak measurements onthe Z resonance. Physics Reports, 427(5-6):257–454, 2006, arXiv:hep-ex/0509008.

[85] Muon reconstruction efficiency in reprocessed 2010 lhc proton-proton collisiondata recorded with the atlas detector. Technical Report ATLAS-CONF-2011-063,CERN, Geneva, Apr 2011.

[86] Performance of the atlas muon trigger in 2011. Technical Report ATLAS-CONF-2012-099, CERN, Geneva, Jul 2012.

[87] The public results of the ATLAS experiment - Combined Muon Per-formance. https://twiki.cern.ch/twiki/bin/view/AtlasPublic/MuonPerformancePublicPlots.

[88] Muon momentum resolution in first pass reconstruction of p � p collision datarecorded by atlas in 2010. Technical Report ATLAS-CONF-2011-046, CERN,Geneva, Mar 2011.

[89] A. Salvucci. Measurement of muon momentum resolution of the atlas detector.Technical Report ATL-PHYS-PROC-2012-013, CERN, Geneva, Jan 2012.

[90] ATLAS Collaboration. Jet energy measurement with the ATLAS detector inproton-proton collisions at

ps = 7 TeV. The European Physical Journal C,

73:2304(3):1–118, 2013.

[91] Pile-up corrections for jets from proton-proton collisions atp

s = 7 TeV in atlasin 2011. Technical Report ATLAS-CONF-2012-064, CERN, Geneva, Jul 2012.

[92] The public results of the ATLAS experiment - Pileup offsetand JVF. https://twiki.cern.ch/twiki/bin/view/AtlasPublic/JetEtmissApproved2011PileupOffsetAndJVF.

[93] Jet energy scale and its systematic uncertainty in proton-proton collisionsat

ps = 7 TeV with atlas 2011 data. Technical Report ATLAS-CONF-2013-004,

CERN, Geneva, Jan 2013.

[94] ATLAS Collaboration. Jet energy resolution in proton-proton collisions atps = 7 TeV recorded in 2010 with the ATLAS detector. The European Physical

Journal C, 73:2306(3):1–27, 2013.

[95] ATLAS Colaboration. Performance of missing transverse momentum reconstruc-tion in proton-proton collisions at

ps = 7 TeV with ATLAS. The European

Physical Journal C, 72:1844(1):1–35, 2012.

173

Bibliography

[96] Performance of missing transverse momentum reconstruction in atlas with 2011proton-proton collisions at

ps = 7 TeV. Technical Report ATLAS-CONF-2012-

101, CERN, Geneva, Jul 2012.

[97] T. KONO and A. Tricoli. Efficiencies of electron/photon triggers using early2011 data: Approval for plhc2011. Technical Report ATL-COM-DAQ-2011-032,CERN, Geneva, May 2011.

[98] N. Makovec. Selection of jets produced in proton-proton collisions with the atlasdetector using 2011 data. Technical Report ATL-COM-PHYS-2012-067, CERN,Geneva, Jan 2012.

[99] D. W. Miller, A. Schwartzman, and D. Su. Jet-vertex association algorithm.Technical Report ATL-COM-PHYS-2008-008, CERN, Geneva, Jan 2008.

[100] J. Adelman, M. Barisonzi, W. H. Bell, G. Brooijmans, G. Cortiana, S. Farrel,P. Federic, A. Ferrari, K. Finelli, A. Gaponenko, U. Husemann, D. Kumar Jana,J. R. Lessard, A. Lleres, A. Lucotte, H. Okawa, M. A. Pleier, B. Radics, J. Searcy,A. Taffard, and D. Urbaniec. Technical aspects of the first top pair analyses:Note 8. Technical Report ATL-COM-PHYS-2010-820, CERN, Geneva, Oct 2010.Support document for top paper.

[101] ATLAS Collaboration. Commissioning of high-performance b-tagging algorithmsin pp collisions at

ps = 7 TeV with the ATLAS experiment. In Proceedings of

the Europhysics Conference on High Energy Physics-HEP, 2011. Proceedings ofScience, 2011.

[102] ATLAS Collaboration. Commissioning of high-performance b-tagging algorithmsin pp collisions at

ps = 7 TeV with the ATLAS experiment. In Proceedings of the

International Conference of High Energy Physics (ICHEP), 36th. Proceedingsof Science, 2012.

[103] Measurement of the mistag rate with 5 fb�1 of data collected by the atlasdetector. Technical Report ATLAS-CONF-2012-040, CERN, Geneva, Mar 2012.

[104] P Cortese, Federico Carminati, Christian Wolfgang Fabjan, Lodovico Riccati,and Hans de Groot. ALICE Computing: Technical Design Report. Technicalreport, CERN, Geneva, 2005.

[105] Atlas Collaboration. Atlas Computing: Technical Design Report. Technicalreport, CERN, Geneva, 2005.

[106] LHCb Collaboration. LHCb Computing: Technical Design Report. Technicalreport, CERN, Geneva, 2005.

[107] G. L. Bayatyan, M. D. Negra, Foà, A. Hervé, and A. Petrilli. CMS Computing:Technical Design Report. Technical report, CERN, Geneva, 2005.

[108] I. Forster and C. Kesselman, editors. The Grid: Blueprint for a New ComputingInfrastructure. Morgan Kaufmann, 1 edition, August 1998.

174

Bibliography

[109] European Grid Infrastructure. http://www.egi.eu.

[110] Open Science Grid. https://www.opensciencegrid.org/bin/view.

[111] NorduGrid. http://www.nordugrid.org.

[112] The CASTOR website. http://castor.web.cern.ch.

[113] The dCache website. http://www.dcache.org.

[114] A. Alvarez, A. Beche, F. Furano, M. Hellmich, O. Keeble, and R. Rocha.DPM: Future Proof Storage. Technical Report CERN-IT-Note-2012-021, CERN,Geneva, Jun 2012.

[115] The StoRM website. http://storm.forge.cnaf.infn.it.

[116] The EOS website. http://eos.cern.ch.

[117] M. Aderholz et al. Models of Networked Analysis at Regional Centres for LHCExperiments (MONARC) PHASE 2 REPORT. Technical report, CERN, April2000.

[118] E. J. Bos, E. Martelli, and P. Moroni. LHC Tier-0 and Tier-1 high-level networkarchitecture. Technical report, CERN, 2005.

[119] The WLCG Resource, Balance and Usage. http://wlcg-rebus.cern.ch/apps/topology/.

[120] I. Foster, C. Kesselman, and S. Tuecke. The Anatomy of the Grid: EnablingScalable Virtual Organization. The International Journal of High PerformanceComputing Applications, 15(3):200–222, Fall 2001.

[121] J. Frey, T. Tannenbaum, M. Livny, I. Foster, and S. Tuecke. Condor-G: a com-putation management agent for multi-institutional grids. In High PerformanceDistributed Computing, 2001. Proceedings. 10th IEEE International Symposiumon, pages 55–63, 2001.

[122] R. Raman, M. Livny, and M. Solomon. Matchmaking: Distributed ResourceManagement for High Throughput Computing. In The Seventh IEEE Interna-tional Symposium on High Performance Distributed Computing: Proceedings,July 1998.

[123] J. T. Mościcki. Understanding and Mastering Dynamics in Computing Grids:Processing Moldable Tasks with User-Level Overlay. PhD thesis, Universiteitvan Amsterdam, 2011.

[124] The job historical view dashboard. http://dashb-atlas-job.cern.ch/dashboard/request.py/dailysummary.

[125] M. Branco, D. Cameron, B. Gaidioz, V. Garonne, B. Koblitz, M. Lassnig,R. Rocha, P. Salgado, and T. Wenaus. Managing ATLAS data on a petabyte-scale with DQ2. Journal of Physics: Conference Series, 119(6):062017, 2008.

175

Bibliography

[126] T. Maeno, K. De, T. Wenaus, P. Nilsson, G. A. Stewart, R. Walker, A. Stradling,J. Caballero, M. Potekhin, D. Smith, and the Atlas Collaboration. Overview ofATLAS PanDA Workload Management. Journal of Physics: Conference Series,331(7):072024, 2011.

[127] J. Blomer, C. Aguado-Sánchez, P. Buncic, and A. Harutyunyan. DistributingLHC application software and conditions databases using the CernVM file system.Journal of Physics: Conference Series, 331(4):042003, 2011.

[128] J. Andreeva, M. D. Campos, J. T. Cros, B. Gaidioz, E. Karavakis,L. Kokoszkiewicz, E. Lanciotti, G. Maier, W. Ollivier, M. Nowotka, R. Rocha,T. Sadykov, P. Saiz, L. Sargsyan, I. Sidorova, and D. Tuckett. ExperimentDashboard for Monitoring of the LHC Distributed Computing Systems. Journalof Physics: Conference Series, 331(7):072001, 2011.

[129] Monitoring dashboards for the ATLAS distributed computing operation. http://adc-monitoring.cern.ch/.

[130] J. Elmsheuser, F. Legger, R. M. Llamas, G. Sciacca, and D. van der Ster.Improving ATLAS grid site reliability with functional tests using HammerCloud.Journal of Physics: Conference Series, 396(3):032066, 2012.

[131] S. Jézéquel and G. Stewart. Atlas distributed computing operations: Experi-ence and improvements after 2 full years of data-taking. Journal of Physics:Conference Series, 396(3):032058, 2012.

[132] B. P. Kersevan. Experiment updates: ATLAS Status and Plan. Presented atLHCC Referees, 2013.

[133] R. Brun and F. Rademakers. ROOT - An Object Oriented Data AnalysisFramework. Nuclear Instruments and Methods in Physics Research Section A:Accelerators, Spectrometers, Detectors and Associated Equipment, 389(1-2):81–86,1997. New Computing Techniques in Physics Research V.

[134] The ROOT website. http://root.cern.ch.

[135] P. Canal, B. Bockelman, and R. Brun. ROOT I/O: The Fast and Furious.Journal of Physics: Conference Series, 331(4):042005, 2011.

[136] J. T. Mościcki, F. Brochu, J. Ebke, U. Egede, J. Elmsheuser, K. Harrison, R. W. L.Jones, H. C. Lee, D. Liko, A. Maier, A. Muraru, G. N. Patrick, K. Pajchel,W. Reece, B. H. Samset, M. W. Slater, A. Soroko, C. L. Tan, D. C. van der Ster,and M. Williams. Ganga: A tool for computational-task management and easyaccess to Grid resources. Computer Physics Communications, 180(11):2303–2316,2009.

[137] J. Elmsheuser and D. van der Ster. Distributed Data Analysis in the ATLASExperiment: Challenges and Solutions. Journal of Physics: Conference Series,396(3):032035, 2012.

176

Bibliography

[138] W. Voorsluys, J. Broberg, and R. Buyya. Introduction to Cloud Computing,pages 1–44. Wiley, 2011.

[139] M. Armbrust, A. Fox, R. Griffith, A. D. Joseph, R. H. Katz, A. Konwinski,G. Lee, D. A. Patterson, A. Rabkin, I. Stoica, and M. Zaharia. Above the Clouds:A Berkeley View of Cloud Computing. Technical Report UCB/EECS-2009-28,EECS Department, University of California, Berkeley, Feb 2009.

[140] The BigGrid HPC Cloud website. https://www.surfsara.nl/systems/hpc-cloud.

[141] The KVM website. http://www.linux-kvm.org/.

[142] B. Sotomayor, R. S. Montero, I. M. Llorente, and I. Foster. Virtual InfrastructureManagement in Private and Hybrid Clouds. IEEE Internet Computing, 13:14–22,2009.

[143] The EGI federated cloud website. http://www.egi.eu/infrastructure/cloud/.

[144] M. Drescher and members of EGI-InSPIRE collaboration. EGI Federated CloudBlueprint v1. Technical Report 1773-v7, European Grid Infrastructure, June2013.

[145] L. Bauerdick, D. Benjamin, K. Bloom, B. Bockelman, D. Bradley, S. Dasu,M. Ernst, R. Gardner, A. Hanushevsky, H. Ito, D. Lesny, P. McGuigan, S. McKee,O. Rind, H. Severini, I. Sfiligoi, M. Tadel, I. Vukotic, S. Williams, F. Würthwein,A. Yagil, and W. Yang. Using Xrootd to Federate Regional Storage. Journal ofPhysics: Conference Series, 396(4):042009, 2012.

[146] F. Furano, R. B. Rocha, A. Devresse, O. Keeble, A. Á. Ayllón, and P. Fuhrmann.Dynamic federations: storage aggregation using open tools and protocols. Journalof Physics: Conference Series, 396(3):032042, 2012.

[147] A. Doxiadis. Searching for the Top: observation of the heaviest elementaryparticle at the LHC. PhD thesis, Universiteit van Amsterdam, 2010.

[148] J. M. Campbell. Overview of the theory of W/Z+jets and heavy flavor, 2008,arXiv:0808.3517.

[149] S. D. Ellis, Z. Kunszt, and D. E. Soper. Two-jet production in hadron collisionsat order ↵3

s in QCD. Phys. Rev. Lett., 69:1496–1499, Sep 1992.

[150] W. T. Giele, E. W. N. Glover, and D. A. Kosower. Higher-order corrections tojet cross sections in hadron colliders. Nuclear Physics B, 403(3):633–667, 1993.

[151] D0 Collaboration. Measurement of the tt production cross section in pp collisionsat

ps = 1.96 TeV using kinematic characteristics of lepton + jets events. Phys.

Rev. D, 76:092007, Nov 2007.

177

Bibliography

[152] S. Allwood-Spires, M. Barisonzi, H. Beauchemin, R. Bruneliere, J. Buchanan,N. F. Castro, E. Devetak, C. Feng, J. Ferrando, R. Hawkings, D. Hirschbuehl,U. Husemann, B. P. Kersevan, G. Khoriauli, T. Kuhl, T. Lenz, L. Mijovc, A. Pa-padelis, M. P. Sanders, L. Shan, P. Sturm, F. Veloso, W. Verkerke, N. Vlasov,and C. Wasicki. Monte Carlo samples used for top physics. Technical ReportATL-PHYS-INT-2010-132, CERN, Geneva, Dec 2010.

[153] D. A. A. Geerts. Estimation of uncertainties for top quark analyses on the heavyflavour content of W+jets events generated by AlpGen in ATLAS. TechnicalReport ATL-COM-PHYS-2013-876, CERN, Geneva, June 2013.

[154] C. Kom and W. J. Stirling. Charge asymmetry in W + jets production at theLHC. The European Physical Journal C, 69:67–73, 2010.

[155] K. Becker, D. Chakraborty, D. Hirschbuehl, J. Koll, R. Schwienhorst, andC. Suhr. Measurement of t-Channel Single Top Quark Production Cross Sectionwith p � p Collisions using a Cuts-Based Approach. Technical Report ATL-COM-PHYS-2012-1430, CERN, Geneva, Sep 2012.

[156] J. D. Bjorken and S. J. Brodsky. Statistical Model for Electron-Positron Annihi-lation into Hadrons. Phys. Rev. D, 1:1416–1420, Mar 1970.

[157] A. Hoecker, P. Speckmayer, J. Stelzer, J. Therhaag, E. von Toerne, andH. Voss. TMVA: Toolkit for Multivariate Data Analysis. PoS, ACAT:040,2007, physics/0703039.

[158] The Bill Tool. https://twiki.cern.ch/twiki/bin/view/AtlasProtected/BillTool.

[159] A. L. Read. Presentation of search results: the CLs technique. Journal ofPhysics G: Nuclear and Particle Physics, 28(10):2693, 2002.

[160] I. C. Brock, T. Loddenkoetter, S. Mergelmeyer, P. Seema, and J. A. Stillings.Measurement of the Wt production in the lepton+jets channel using neuralnetworks. Technical Report ATL-COM-PHYS-2011-1706, CERN, Geneva, Dec2011.

[161] ATLAS Collaboration. Evidence for the associated production of a w boson anda top quark in atlas at

ps = 7 TeV. Physics Letters B, 716(1):142–159, 2012.

[162] ATLAS Collaboration. Search for single b*-quark production with the AT-LAS detector at

ps = 7 TeV. Physics Letters B, 721(4-5):171–189, 2013,

arXiv:1301.1583.

178