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Radiating top quarks

Gosselink, M.

Publication date 2010

Link to publication

Citation for published version (APA):

Gosselink, M. (2010). Radiating top quarks.

http://www.nikhef.nl/pub/services/biblio/theses_pdf/thesis_M_Gosselink.pdf

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[1] P.W. Higgs, Broken Symmetries, Massless Particles and Gauge Fields, Phys. Lett. 12 (1964) 132.

[2] P.W. Higgs, Broken Symmetries and the Masses of Gauge Bosons, Phys. Rev. Lett. 13 (1964) 508.

[3] P.W. Higgs, Spontaneous Symmetry Breakdown without Massless Bosons, Phys. Lett. 145 (1966) 1156.

[4] F. Englert and R. Brout, Broken Symmetry and the Mass of Gauge Vector Mesons, Phys. Rev. Lett. 13 (1964) 321.

[5] G. S. Guralnik, C. R. Hagen, and T. W. B. Kibble, Global Conservation Laws and Massless Particles, Phys. Rev. Lett. 13 (1964) 356.

[6] S.L Glashow, Partial-symmetries of weak interactions, Nucl. Phys. 22 (1961) 579. [7] S. Weinberg, A Model of Leptons, Phys. Rev. Lett. 19 (1967) 1264.

[8] A. Salam, Weak and Electromagnetic Interactions, Originally printed in Svartholm: Elementary Particle Theory, Proceedings Of The Nobel Symposium Held 1968 At Lerum, Sweden (1968) 367.

[9] UA1 Collaboration, Experimental observation of isolated large transverse energy electrons with associated missing energy at √s = 540 GeV, Phys. Lett. B 122 (1983) 103.

[10] The UA2 Collaboration, Observation of single isolated electrons of high transverse momentum in events with missing transverse energy at the CERN p¯p collider, Phys. Lett. B 122 (1983) 476.

(3)

[11] F. Abe et al., Observation of Top Quark Production in p¯p Collisions with the Collider Detector at Fermilab, Phys. Rev. Lett. 74 (1995) 2626, arXiv:hep-ex/9503002v2.

[12] S. Abachi et al., Observation of the Top Quark, Phys. Rev. Lett. 74 (1995) 2632, arXiv:hep-ex/9503003v1.

[13] M. Kobayashi and T. Maskawa, CP-Violation in the Renormalizable Theory of Weak Interactions, Prog. Theor. Phys. 49 (1973) 652.

[14] The ATLAS Collaboration, Observation of W → ℓν and Z → ℓℓ production in proton-proton collisions at √s = 7 TeV with the ATLAS detector, 2010, ATLAS-CONF-2010-044.

[15] For the latest updates on the LHC commissioning planning see: http:// lhc-commissioning.web.cern.ch/lhc-commissioning/

[16] O.S. Br¨uning, P. Collier, P. Lebrun, S. Myers, R. Ostojic, J. Poole, and P. Proud-lock, LHC Design Report, Volume I: The LHC Main Ring, CERN, Geneva, 2004, CERN-2004-003-V-1.

[17] http://doc.cern.ch//archive/electronic/cern/others/PHO/photo-di/ 0606052.pdf

[18] http://www.fnal.gov/pub/now/tevlum.html [19] http://projects.hepforge.org/mstwpdf/

[20] J. M. Campbell and R. K. Ellis, An update on vector boson pair production at hadron colliders, Phys. Rev. D 60 (1999) 113006, arXiv:hep-ph/9905386. [21] A. D. Martin, W. J. Stirling, R. S. Thorne, and G. Watt, Parton distributions for

the LHC, Eur. Phys. J. C (2009) 189, arXiv:0901.0002v3 [hep-ph].

[22] D. Green, High PT Physics at Hadron Colliders, Cambridge University Press,

2005.

[23] G. Altarelli and M.L. Mangano, Proceedings of the workshop on standard model physics (and more) at the LHC, CERN, 2000, arXiv:hep-ph/0005025v1.

[24] J.R. Incandela, A. Quadt, W. Wagner, and D. Wicke, Status and Prospects of Top-Quark Physics, 2009, arXiv:0904.2499v1 [hep-ex].

[25] S.W. Herb et al., Observation of a Dimuon Resonance at 9.5 GeV in 400 GeV Proton-Nucleus Collisions, Phys. Rev. Lett. 39 (1977) 252.

[26] T. Aaltonen et al., First Observation of Electroweak Single Top Quark Production, Phys. Rev. Lett. 103 (2009) 092001, arXiv:0903.0885v3 [hep-ex].

(4)

[27] V.M. Abazov et al., Observation of Single Top Quark Production, Phys. Rev. Lett. 103 (2009) 092001, arXiv:0903.0850v2 [hep-ex].

[28] Tevatron Electroweak Working Group, Combination of CDF and DØ Results on the Mass of the Top Quark, 2009, arXiv:0903.2503v1 [hep-ex].

[29] M.C. Smith and S.S. Willenbrock, Top-quark Pole Mass, Phys. Rev. Lett. 79 (1997) 3825, arXiv:hep-ph/9612329v1.

[30] U. Langenfeld, S. Moch, and P. Uwer, Measuring the running top-quark mass, Phys. Rev. D 80 (2009) 054009, arXiv:0906.5273v2 [hep-ph].

[31] A.H. Hoang and I.W. Stewart, Top Mass Measurements from Jets and the Teva-tron Top-Quark Mass, Nucl. Phys. B - Proc. Sup. 185 (2008) 220, arXiv:hep-ph/0808.0222v2.

[32] P. Skands and D. Wicke, Non-perturbative QCD Effects and the Top Mass at the Tevatron, Eur. Phys. J. C 52 (2007) 133, arXiv:hep-ph/0703081v2.

[33] C. Amsler et al., Review of Particle Physics, Phys. Lett. B 667 (2008) 1.

[34] W. Bernreuther, Top quark physics at the LHC, 2008, arXiv:0805.1333v1 [hep-ph].

[35] H.S. Do, S. Groote, J.G. K¨orner, and M.C. Mauser, Electroweak and finite width corrections to top quark decays into transverse and longitudinal W -bosons, Phys. Rev. D 67 (2003) 091501, arXiv:hep-ph/0209185v2.

[36] R.K. Ellis, W.J. Stirling, and B.R. Webber, QCD and Collider Physics, Cambridge University Press, 1996.

[37] http://www-d0.fnal.gov/Run2Physics/top/top_public_web_pages/top_ feynman_diagrams.html

[38] J.C. Collins, D.E. Soper, and G. Sterman, Factorisation of the Hard Processes in QCD, Adv. Ser. Direct. HighEnergyPhys. 5 (1988) 1, arXiv:hep-ph/0409313v1. [39] J.C. Collins and D.E Soper, The Theorems of Perturbative QCD, Ann. Rev. Nucl.

Part. Sci. 37 (1987) 383.

[40] V.N. Gribov and L.N. Lipatov, Deep inelastic ep scattering in perturbation theory, Sov. J. Nucl. Phys 15 (1972) 428.

[41] L.N. Lipatov, The parton model and perturbation theory, Sov. J. Nucl. Phys 20 (1975) 94.

[42] G. Altarelli and G. Parisi, Asymptotic freedom in parton language, Nucl. Phys. B 126 (1977) 298.

(5)

[43] Y. Dokshitser, Calculation of the Structure Functions for Deep Inelastic Scattering and e+eAnnihilation by Perturbation Theory in Quantum Chromodynamics, Sov.

Phys. JETP 46 (1977) 641.

[44] Private communication with E. Laenen.

[45] M. Cacciari, S. Frixione, M.L. Mangano, P. Nason, and G. Ridolfi, Updated predic-tions for the total production cross secpredic-tions of top and heavier pairs at the Tevatron and at the LHC, JHEP 0809 (2008) 127, arXiv:0804.2800v3 [hep-ph].

[46] S. Moch and P. Uwer, Theoretical status and prospects for top-quark pair pro-duction at hadron colliders, Phys. Rev. D 78 (2008) 034003, arXiv:0804.1476 [hep-ph].

[47] W.K. Tung, H.L. Lai, A. Belyaev, J. Pumplin, D. Stump, and C.-P. Yuan, Heavy Quark Mass Effects in Deep Inelastic Scattering and Global QCD Analysis, JHEP 0702 (2007) 053, arXiv:hep-ph/0611254.

[48] N. Kidonakis, E. Laenen, S. Moch, and R. Vogt, Sudakov resummation and finite order expansions of heavy quark hadroproduction cross sections, Phys. Rev. D64 (2001) 114001, arXiv:hep-ph/0105041.

[49] S. Moch and P. Uwer, Heavy-quark pair production at two loops in QCD, Nucl. Phys. Proc. Suppl. 183 (2008) 75, arXiv:0807.2794v1 [hep-ph].

[50] N. Kidonakis and R. Vogt, The theoretical top quark cross section at the Tevatron and the LHC, Phys. Rev. D 78 (2008) 074005, arXiv:0805.3844v1 [hep-ph]. [51] U. Langenfeld, S. Moch, and P. Uwer, New results for t¯t production at hadron

colliders, To appear in the proceedings of 17th International Workshop on Deep-Inelastic Scattering and Related Subjects (DIS 2009), Madrid, Spain, 26-30 Apr 2009 (2009) , arXiv:0907.2527 [hep-ph].

[52] Latest results for summer 2009 conferences (to be published), CDF note 9913, http://www-cdf.fnal.gov/physics/new/top/public_xsection.html

[53] V. Abazov et al., Combination and interpretations of ttbar cross section measure-ments with the DØ detector, Phys. Rev. D 80 (2009) 071102, arXiv:0903.5525v1 [hep-ex].

[54] The ATLAS Collaboration, ATLAS detector and physics performance. Technical design report. Vol. 2, CERN, 1999, CERN-LHCC-99-15.

[55] The CMS Collaboration, CMS Physics Technical Design Report, Volume II: Physics Performance, J. Phys. G: Nucl. Part. Phys. 34 (2007) 995.

[56] G. Bordes and B. van Eijk, Calculating QCD corrections to single top production in hadronic interactions, Nucl. Phys. B 435 (1994) 23.

(6)

[57] B.W. Harris, E. Laenen, L. Phaf, Z. Sullivan, and S. Weinzierl, Fully differential single-top-quark cross section in next-to-leading order QCD, Phys. Rev. D 66 (2002) 054024, arXiv:hep-ph/0207055v1.

[58] W.T. Giele, S. Keller, and E. Laenen, QCD Corrections to W Boson plus Heavy Quark Production at the Tevatron, Phys. Lett. B 372 (1996) 141, arXiv:hep-ph/9511449v1.

[59] S. Zhu, Next-to-leading order QCD corrections to bg → tW− at the CERN Large

Hadron Collider, Phys. Lett. B 524 (2002) 283, erratum: Phys. Lett. B 537 (2002) 351, arXiv:hep-ph/0109269v5.

[60] A.D. Martin, R.G. Roberts, W.J. Stirling, and R.S. Thorne, Physical Gluons and High ET Jets, Phys. Lett. B 604 (2004) 61, arXiv:hep-ph/0410230v1.

[61] N. Kidonakis, Single top quark production at the Tevatron: threshold resumma-tion and finite-order soft gluon correcresumma-tions, Phys. Rev. D 74 (2006) 114012, arXiv:hep-ph/0609287v3.

[62] N. Kidonakis, Higher-order soft gluon corrections in single top quark production at the LHC, Phys. Rev. D 75 (2007) 071501, arXiv:hep-ph/0701080v1.

[63] C.D. White, S. Frixione, E. Laenen, and F. Maltoni, Isolating W t production at the LHC, arXiv:0908.0631v1 [hep-ph].

[64] S. Glazov, Measurement of DIS cross section at HERA, Braz. J. Phys. 37 (2007) 793.

[65] R.S. Thorne, A.D. Martin, W.J. Stirling, and G. Watt, Parton Distributions and QCD at LHCb, Proceedings of 16th International Workshop on Deep Inelastic Scattering and Related Subjects (DIS 2008), London, England, 7-11 Apr 2008. [66] P.M. Nadolsky, N.-L. Lai, Q.-H. Cao, Joey Huston, J. Pumplin, D. Stump, W.-K.

Tung, and C.-P. Yuan, Implications of CTEQ global analysis for collider observ-ables, Phys. Rev. D 78 (2008) 013004, arXiv:0802.0007v3 [hep-ph].

[67] L.N. Lipatov, Reggeization of the Vector Meson and the Vacuum Singularity in Nonabelian Gauge Theories, Sov. J. Phys. 23 (1976) 338.

[68] E.A. Kuraev, L.N. Lipatov, and V.S. Fadin, The Pomeranchuk Singularity in Nonabelian Gauge Theories, Sov. Phys. JETP 45 (1977) 199.

[69] I.I. Balitsky and L.N. Lipatov, The Pomeranchuk Singularity in Quantum Chro-modynamics, Sov. J. Nucl. Phys. 28 (1978) 822.

[70] M. Ciafaloni, Coherence effects in initial jets at small Q2/s, Nucl. Phys. B 296

(1988) 49.

(7)

[71] S. Catani, F. Fiorani, and G. Marchesini, QCD coherence in initial state radiation, Phys. Lett. B 234 (1990) 339.

[72] S. Catani, F. Fiorani, and G. Marchesini, Small-x behaviour of initial state radia-tion in perturbative QCD, Nucl. Phys. B 336 (1990) 18.

[73] B. Andersson, G. Gustafson, and J. Samuelsson, The linked dipole chain model for DIS, Nucl. Phys. B 467 (1996) 443.

[74] H. Kharraziha and L. L¨onnblad, The Linked Dipole Chain Monte Carlo, JHEP 9803 (1998) 006, arXiv:hep-ph/9709424.

[75] L.H. Orr and W.J. Stirling, BFKL Physics in Dijet Production at the LHC, Phys. Lett. B 436(3) (1998) 372, arXiv:hep-ph/9806371v1.

[76] C. Buttar et al., Les Houches Physics at TeV Colliders 2005, Standard Model and Higgs working group: Summary report, arXiv:hep-ph/0604120v1.

[77] J.R. Andersen, V. Del Duca, F. Maltoni, and W.J. Stirling, W Boson Production with Associated Jets at Large Rapidities, JHEP 0105 (2001) 048, arXiv:hep-ph/0105146v1.

[78] A. Sirlin, Radiative corrections in the SU(2) × U(1) theory: A simple renormal-ization framework, Phys. Rev. D 22 (1980) 971.

[79] http://lepewwg.web.cern.ch/LEPEWWG/

[80] G. Abbiendi et al., Search for the Standard Model Higgs boson at LEP, Phys. Lett. B 565 (2003) 61, arXiv:hep-ex/0306033v1.

[81] CDF and DØ collaborations, Combination of Tevatron searches for the standard model Higgs boson in the W+Wdecay mode, Phys. Rev. Lett. 104 (2010) 061802,

arXiv:1001.4162v3 [hep-ex].

[82] V.M. Abazov et al., Experimental Discrimination between Charge 2e/3 Top Quark and Charge 4e/3 Exotic Quark Production Scenarios, Phys. Rev. Lett. 98 (2007) 041801, arXiv:hep-ex/0608044v2.

[83] The CDF Collaboration, First CDF Measurement of the Top Quark Charge using the Top Decay Products, 2007, CDF note 8967.

[84] R. Frederix and F. Maltoni, Top pair invariant mass distribution: a window on new physics, JHEP 0901 (2009) 047, arXiv:0712.2355v3 [hep-ph].

[85] W. Beenakker, S. Dittmaier, M. Kr¨amer, B. Pl¨umper, M. Spira, and P.M. Zerwas, NLO QCD corrections to t¯tH production in hadron collisions, Nucl. Phys. B 653 (2003) 151, arXiv:hep-ph/0211352v1.

(8)

[86] B. Mellado, L. Nisati, D. Rebuzzi, S. Rosati, G. Unal, and Sau Lan Wu, Higgs Production Cross-Sections and Branching Ratios for the ATLAS Higgs Working Group, ATL-COM-PHYS-2007-024.

[87] M. Czakon and A. Mitov, Inclusive Heavy Flavor Hadroproduction in NLO QCD: the Exact Analytic Result, Nucl. Phys. B 824 (2010) 111, arXiv:0811.4119v1 [hep-ph].

[88] S. Dittmaier, P. Uwer, and S. Weinzierl, Hadronic top-quark pair production in association with a hard jet at next-to-leading order QCD: Phenomenological studies for the Tevatron and the LHC, Eur. Phys. J. C 59 (2009) 625, arXiv:0810.0452v2 [hep-ph].

[89] M. Czakon, Tops from light quarks: Full mass dependence at two-loops in QCD, Phys. Lett. B 664 (2008) 307, arXiv:0803.1400v3 [hep-ph].

[90] R. Bonciana and A. Ferroglia, Top Quark Production at Hadron Colliders: an Overview, arXiv:0909.2980v2 [hep-ph].

[91] A. Bredenstein, A. Denner, S. Dittmaier, and S. Pozzorini, NLO QCD cor-rections to pp → t¯tb¯b + X at the LHC, Phys. Rev. Lett. 103 (2009) 012002, arXiv:0905.0110v2 [hep-ph].

[92] G. Bevilacqua, M. Czakon, C. G. Papadopoulos, R. Pittau, and M. Worek, Assault on the NLO Wishlist: pp → t¯tb¯b, JHEP 0909 (2009) 109, arXiv:0907.4723v2 [hep-ph].

[93] T. Gleisberg, S. Hoeche, F. Krauss, M. Schoenherr, S. Schumann, F. Siegert, and J. Winter, Event generation with SHERPA 1.1, JHEP 0902 (2009) 007, arXiv:0811.4622v1 [hep-ph].

[94] T. Sj¨ostrand, S. Mrenna, and P. Skands, PYTHIA 6.4 Physics and Manual, JHEP 0605 (2006) 026, arXiv:hep-ph/0603175v2.

[95] G. Corcella, I.G. Knowles, G. Marchesini, S. Moretti, K. Odagiri, P. Richard-son, M.H. Seymour, and B.R. Webber, HERWIG 6.5: an event generator for Hadron Emission Reactions With Interfering Gluons (including supersymmetric processes), JHEP 0101 (2001) 010, ph/0011363v3, arXiv:hep-ph/0210213v2.

[96] M.L. Mangano, M. Moretti, F. Piccinini, R. Pittau, and A. Polosa, ALPGEN, a generator for hard multiparton processes in hadronic collisions, JHEP 0307 (2003) 001, arXiv:hep-ph/0206293v2.

[97] E. Barberio, B. van Eijk, and Z. Was, PHOTOS - a universal Monte Carlo for QED radiative corrections in decays, Comput. Phys. Commun. 66 (1991) 115.

(9)

[98] S. Jadach, J.H. K¨uhn, and Z. W as, TAUOLA - a library of Monte Carlo programs to simulate decays of polarized τ leptons, Comput. Phys. Commun. 64 (1991) 275. [99] K. Odagiri, Colour Connection Structure of (Supersymmetric) QCD (2 → 2)

Processes, JHEP 9810 (1998) 006, arXiv:hep-ph/9806531v2.

[100] M.L. Mangano, M. Moretti, and R. Pittau, Multijet matrix elements and shower evolution in hadronic collisions: W b¯b + n jets as a case study, Nucl. Phys. B 632 (2002) 343, arXiv:hep-ph/0108069v1.

[101] J. Alwall et al., MadGraph/MadEvent v4: The New Web Generation, JHEP 0709 (2007) 028, arXiv:0706.2334v1 [hep-ph].

[102] J. Alwall et al., A standard format for Les Houches Event Files, Comput. Phys. Commun. 176 (2007) 300, arXiv:hep-ph/0609017v1.

[103] F.A. Berends and W.T. Giele, Recursive calculations for processes with n gluons, Nucl. Phys. B 306 (1988) 759.

[104] S. Frixione and B.R. Webber, Matching NLO QCD computations and parton shower simulations, JHEP 0206 (2002) 029, arXiv:hep-ph/0204244v2.

[105] B.P. Kersevan and E. Richter-W as, The Monte Carlo Event Generator AcerMC version 3.5 with interfaces to PYTHIA 6.3, HERWIG 6.5 and ARIADNE 4.1, arXiv:hep-ph/0405247v1.

[106] V.V. Sudakov, Vertex parts at very high-energies in quantum electrodynamics, Sov. Phys. JETP 30 (1956) 65, see also: arXiv:hep-ph/0312336v1.

[107] T. Sj¨ostrand and P. Skands, Transverse-Momentum-Ordered Showers and In-terleaved Multiple Interactions, Eur. Phys. J. C 39 (2005) 129, arXiv:hep-ph/0408302v1.

[108] DØ collaboration, Evidence of Color Coherence Effects in W+jets Events from ppbar Collisions at √s = 1.8 TeV, Phys. Lett. B 464 (1999) 145, arXiv:hep-ex/9908017v1.

[109] G. Gustafson, Dual description of a confined colour field, Phys. Lett. B 175(4) (1986) 453.

[110] G. Gustafson and U. Pettersson, Dipole formulation of QCD cascades, Nucl. Phys. B 306 (1988) 746.

[111] L. L¨onnblad, ARIADNE version 4: A Program for simulation of QCD cascades implementing the color dipole model, Comput. Phys. Commun. 71 (1992) 15. [112] L. L¨onnblad, Small-x Effects in W + jets Production at the Tevatron, Nucl. Phys.

B 458 (1996) 215, arXiv:hep-ph/9508261v1.

R

(10)

[113] N. Magnussen et al., Generators for deep inelastic scattering, In *Hamburg 1991, Proceedings, Physics at HERA, vol. 3* 1167-1219.

[114] I.G Knowles and T. Sj¨ostrand, Physics at LEP2, Proceedings of the workshop Physics at LEP2 , p.103, CERN 96-01, Geneva, 1996.

[115] J. M. Butterworth, Jeffrey R. Forshaw, and M .H. Seymour, Multiparton inter-actions in photoproduction at HERA, Z. Phys. C72 (1996) 637, arXiv:hep-ph/9601371.

[116] R.D. Field, The Underlying Event in Hard Scattering Processes, contribution to Snowmass 2001.

[117] R.D. Field and R. Craig Group, Pythia Tune A, Herwig, and Jimmy in Run 2 at CDF, arXiv:hep-ph/0510198v1, 2005.

[118] R. Corke and T. Sj¨ostrand, Multiparton Interactions and Rescattering, arXiv:0911.1909v1 [hep-ph].

[119] TeV4LHC QCD Working Group, Tevatron-for-LHC Report of the QCD Working Group, 2006, arXiv:hep-ph/0610012v1.

[120] G. Corcella and M.H. Seymour, Initial State Radiation in Simulations of Vector Boson Production at Hadron Colliders, Nucl. Phys. B 565 (2000) 227, arXiv:hep-ph/9908388v2.

[121] G. Miu and T. Sj¨ostrand, W Production in an Improved Parton-Shower Approach, Phys. Lett. B 449 (1999) 313, arXiv:hep-ph/9812455v1.

[122] M.H. Seymour, Matrix-Element Corrections to Parton Shower Algorithms, Com-put. Phys. Commun. 90 (1995) 95, arXiv:hep-ph/9410414v1.

[123] S. Frixione, P. Nason, and B.R. Webber, Matching NLO QCD and Parton Showers in Heavy Flavour Production, JHEP 0308 (2003) 007, arXiv:hep-ph/0305252v2. [124] P. Torrielli and S. Frixione, Matching NLO QCD computations with PYTHIA

using MC@NLO, 2010, arXiv:1002.4293v2 [hep-ph].

[125] Stefano Frixione, Paolo Nason, and Carlo Oleari, Matching NLO QCD computa-tions with Parton Shower simulacomputa-tions: the POWHEG method, JHEP 11 (2007) 070, arXiv:0709.2092v1 [hep-ph].

[126] Stefano Frixione, Paolo Nason, and Giovanni Ridolfi, A Positive-Weight Next-to-Leading-Order Monte Carlo for Heavy Flavour Hadroproduction, JHEP 09 (2007) 126, arXiv:0707.3088v3 [hep-ph].

[127] S. Catani, F. Krauss, R. Kuhn, and B.R. Webber, QCD matrix elements + parton showers, JHEP 0111 (2001) 063, arXiv:hep-ph/0109231v1.

(11)

[128] N. Lavesson and L. L¨onnblad, W+jets Matrix Elements and the Dipole Cascade, JHEP 0507 (2005) 054, arXiv:hep-ph/0503293v2.

[129] S. Mrenna and P. Richardson, Matching Matrix Elements and Parton Showers with HERWIG and PYTHIA, JHEP 0405 (2004) 040, arXiv:hep-ph/0312274v1. [130] M.L. Mangano, http://home.fnal.gov/~mrenna/tuning/nov2002/mlm.pdf

and https://mlm.web.cern.ch/mlm/talks/lund-alpgen.pdf.

[131] S. Catani, Yu.L. Dokshitzer, M.H. Seymour, and B.R. Webber, Longitudinally-invariant k⊥-clustering algorithms for hadron-hadron collisions, Nucl. Phys. B

406 (1993) 187.

[132] F. Krauss, Matrix elements and parton showers in hadronic interactions, JHEP 0208 (2002) 015, arXiv:hep-ph/0205283v1.

[133] S. H¨oche, F. Krauss, S. Schumann, and F. Siegert, QCD matrix elements and truncated showers, arXiv:0903.1219v2 [hep-ph].

[134] N. Lavesson and L. L¨onnblad, Merging parton showers and matrix elements – back to basics, JHEP 0804 (2008) 085, arXiv:0712.2966v2 [hep-ph].

[135] J. Alwall et al., Comparative study of various algorithms for the merging of parton showers and matrix elements in hadronic collisions, Eur. Phys. J. C53 (2008) 473, arXiv:0706.2569v2 [hep-ph].

[136] J. Alwall, S. de Visscher, and F. Maltoni, QCD radiation in the production of heavy coloured particles at the LHC, JHEP 0902 (2009) 017, arXiv:0810.5350v1 [hep-ph].

[137] M.L. Mangano, M. Moretti, F. Piccinini, and M. Treccani, Matching matrix ele-ments and shower evolution for top-quark production in hadronic collisions, JHEP 0701 (2007) 013, arXiv:hep-ph/0611129v1.

[138] J. Tully K. Hamilton, P. Richardson, A Positive-Weight Next-to-Leading Order Monte Carlo Simulation for Higgs Boson Production, JHEP 0904 (2009) 116, arXiv:0903.4345v3 [hep-ph].

[139] P. Nason, Recent developments in POWHEG, 2010, arXiv:1001.2747v1 [hep-ph].

[140] DØ Collaboration, Measurement of the ratios of the Z/γ∗+ ≥ n jet production

cross sections to the total inclusive Z/γ∗ cross section in p¯p ats = 1.96 TeV,

Phys. Lett. B 658 (2008) 112, arXiv:hep-ex/0608052v3.

[141] DØ Collaboration, Measurement of differential Z/γ∗+ jet + X cross sections in p¯p

collisions at √s = 1.96 TeV, Phys. Lett. B 669 (2008) 278, arXiv:0808.1296v1 [hep-ex].

(12)

[142] DØ Collaboration, Measurements of differential cross sections of Z/γ∗+ jets + X

events in p¯p collisions at √s = 1.96 TeV, Phys. Lett. B 678 (2009) 45, arXiv:0903.1748v2 [hep-ex].

[143] DØ Collaboration, Measurements of Z/γ∗+ jets + X angular distributions in p¯p

collisions at √s = 1.96 TeV, Phys. Lett. B 682 (2010) 370, arXiv:0907.4286v2 [hep-ex].

[144] CDF Collaboration, Measurement of the ratios of the Z/γ∗+ ≥ n jet production

cross sections to the total inclusive Z/γ∗ cross section in p¯p ats = 1.96 TeV,

Phys. Rev. D 77 (2008) 011108, arXiv:0711.4044v2 [hep-ex]. [145] CDF Collaboration, Measurement of the ratios of the Z/γ∗

+ ≥ n jet production cross sections to the total inclusive Z/γ∗ cross section in p¯p ats = 1.96 TeV,

Phys. Rev. Lett. 100 (2008) 102001, arXiv:0711.3717 [hep-ex].

[146] N. Lavesson and L. L¨onnblad, Extending CKKW-merging to one-loop matrix ele-ments, JHEP 0812 (2008) 070, arXiv:0811.2912v1 [hep-ph].

[147] K. Hamilton and P. Nason, Improving NLO-parton shower matched simulation with higher order matrix elements, 2010.

[148] The ATLAS Collaboration, ATLAS detector and physics performance. Technical design report. Vol. 1, 1999, CERN-LHCC-99-14.

[149] The ATLAS Collaboration, The ATLAS Experiment at the CERN Large Hadron Collider, JINST 3 (2008) S08003.

[150] S. Catani, Yu.L. Dokshitzer, M. Olsson, G. Turnock, and B.R. Webber, New clustering algorithm for multijet cross sections in e+e- annihilation, Phys. Lett. B 269 (1991) 432.

[151] G.P. Salam and G. Soyez, A practical Seedless Infrared-Safe Cone jet algorithm, JHEP 0705 (2007) 086, arXiv:0704.0292v2 [hep-ph].

[152] M. Cacciari, G.P. Salam, and G. Soyez, The anti-kT jet clustering algorithm,

JHEP 0804 (2008) 063, arXiv:0802.1189v2 [hep-ph].

[153] G.P. Salam, Towards Jetography, arXiv:0906.1833v1 [hep-ph].

[154] L. Asquith et al., Performance of Jet Algorithms in the ATLAS Detec-tor, https://svnweb.cern.ch/trac/atlasgrp/browser/CombPerf/JetETMiss/ jetalgonote/trunk/JetAlgo.pdf, (in preparation).

[155] L. Asquith and N. Konstantinidis, Performance of jet algorithms in the channel t¯tH(H → b¯b), ATL-PHYS-INT-2009-079, ATL-COM-PHYS-2009-399.

[156] N. Ghodbane, Performance of Jet Algorithms for the Top Quark Physics at the ATLAS Experiment, ATL-PHYS-INT-2009-087, ATL-COM-PHYS-2009-432.

(13)

[157] The ATLAS Collaboration, Expected performance of the ATLAS experiment: de-tector, trigger and physics, CERN-OPEN-2008-020 (2008) , arXiv:0901.0512v4 [hep-ex].

[158] S. Bentvelsen and M. Cobal, Top studies for the ATLAS detector Commissioning, ATL-PHYS-PUB-2005-024, ATL-COM-PHYS-2005-039.

[159] W. Verkerke and I. van Vulpen, Commissioning ATLAS using top-quark pair production, ATL-COM-PHYS-2007-023.

[160] A. Doxiadis and M. Kayl, Estimating the isolated lepton rate in multi-jet events, ATL-PHYS-INT-2008-022.

[161] E.E. van der Kraaij, Uncertainties on the t¯t cross section and its ratio to the W cross section at the LHC, ATL-COM-PHYS-2006-040.

[162] A. Shibata et al., Understanding Monte Carlo Generators for Top Physics, ATL-COM-PHYS-2009-334.

[163] D. Cavalli et al., Performance of the ATLAS fast simulation ATLFAST, ATL-PHYS-INT-2007-005, ATL-COM-PHYS-2007-012.

[164] https://twiki.cern.ch/twiki/bin/view/AtlasProtected/ TopGroupCSCObjectSelection

[165] J. Pumplin et al., New Generation of Parton Distributions with Uncertainties from Global QCD Analysis, JHEP 07 (2002) 012, arXiv:hep-ph/0201195v3. [166] https://twiki.cern.ch/twiki/bin/view/Atlas/

ApprovedPlotsATLASDetector

[167] https://twiki.cern.ch/twiki/bin/view/Atlas/ EventDisplayPublicResults

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