Диссертация (1145387), страница 42
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— 1995. — Vol. 51. —P. 4891. — arXiv : hep-ex/9412289.[36] Mirkes E. Ohnemus J. Polarisation effects in Drell – Yan type processes h1 + h2 →(W, Z, γ ∗ , J/Ψ) + X. — 1994. — arXiv : hep-ex/9408402.[37] Aaltonen T. et al., CDF collaboration. First Measurement of the Angular Coefficients√of Drell – Yan e+ e− Pairs in the Z Mass Region from pp Collisions at s = 1.96TeV //Phys. Rev. Lett. — 2011. — June. — Vol. 106.
— P. 241801. — arXiv : hep-ex/1103.5699.[38] A. Sirlin. Universal Renormalization in Leptonic and Semileptonic Amplitudes // Phys.Rev. D. — 1980. — Vol. 22. — P. 971.2[39] T. Aaltonen et al., CDF Collaboration. Indirect measurement of sinθWusing e+ e−pairs from γ ∗ /Z bosons produced in pp̄ collisions at a centre-of-momentum energy of1.96 TeV // Phys. Rev. D. — 2013. — Vol.
88. — P. 072002. — arXiv : hep-ex/1402.2239.2002[40] T. Aaltonen et al., CDF Collaboration. Indirect measurement of sinθWusing µ+ µ−pairs from γ ∗ /Z bosons produced in pp̄ collisions at a centre-of-momentum energy of1.96 TeV // Phys. Rev. D. — 2014. — Vol. 89. — P. 072005. — arXiv : hep-ex/1402.2239.[41] Aad G. et al., ATLAS Collaboration. Measurement of the forward-backward asymmetry√of electron and muon pair-production in pp collisions at s = 7 TeV with the ATLASdetector // JHEP.
— 2015. — Vol. 09. — P. 049. — arXiv : hep-ex/1503.03709.[42] Z. Bern et al. Left-handed W bosons at the LHC // Phys. Rev. D. — 2011. — Vol. 84. —P. 034008. — arXiv : hep-ex/1103.5445.[43] Karlberg A., Re E., Zanderighi G. NNLOPS accurate Drell – Yan production //JHEP. — 2014.
— Vol. 09. — P. 134. — arXiv : hep-ph/1407.2940.[44] Aad G. et al., ATLAS Collaboration. Measurement of the transverse momentum and√φ∗η distributions of Drell–Yan lepton pairs in proton-proton collisions at s = 8 TeVwith the ATLAS detector // Eur. Phys. J. C. — 2016. — Vol. 76.
— P. 1. — arXiv :hep-ex/1512.02192.[45] Aad G. et al., ATLAS Collaboration. Measurement of the Z/γ ∗ boson transverse√momentum distribution in pp collisions at s = 7 TeV with the ATLAS detector //JHEP. — 2014. — Vol. 09. — P. 145. — arXiv : hep-ex/1406.3660.[46] Khachatryan V.
et al., CMS Collaboration. Angular coefficients of Z bosons produced√in pp collisions at s = 8 TeV and decaying to µ+ µ− as a function of transversemomentum and rapidity // Phys. Lett. B. — 2015. — Vol. 750. — P. 154. — arXiv :hep-ex/1504.03512.[47] Lam C.S., Tung W-K. A Systematic Approach to Inclusive Lepton Pair Production inHadronic Collisions // Phys.
Rev. — 1978. — Vol. D18. — P. 2447.[48] Hagiwara K., Hikasa K., Kai N. Parity-Odd Asymmetries in W-Jet Events at HadronColliders // Phys. Rev. Lett. — 1984. — Vol. 52. — P. 1076.[49] Jadach S., Was Z. Suppression of QED interference contributions to the chargeasymmetry at the Z resonance // Phys. Lett. B.
— 1989. — Vol. 219. — P. 103.[50] Jadach S., Pietrzyk B. et al. Initial final state interference in the Z line shape // Phys.Lett. B. — 1999. — Vol. 465. — P. 254. — arXiv : hep-ph/9907547.[51] Collins J. C., Soper D. E. Angular distribution of dileptons in high-energy hadroncollisions // Phys.
Rev. D. — 1977. — Vol. 16. — P. 2219.201[52] Gottfried K., Jackson J. D. On the connection between production mechanism anddecay of resonances at high energies // Nuovo Cim. — 1964. — Vol. 33. — P. 309.[53] Stirling W., Vryonidou E. Electroweak gauge boson polarisation at the LHC //JHEP. — 2012. — Vol. 07. — P. 124. — arXiv : hep-ph/1204.6427.[54] Gao J., Guzzi M. et al.
CT10 next-to-next-to-leading order global analysis of QCD //Phys. Rev. D. — 2014. — Vol. 89, no. 3. — P. 033009. — arXiv : hep-ph/1302.6246.[55] Dittmaier S., Kramer M. Electroweak radiative corrections to W-boson production athadron colliders // Phys. Rev. D. — 2002. — Vol. 65. — P. 073007. — arXiv : hepph/0109062.[56] Olive K.
A. et al., Particle Data Group. Review of Particle Physics // Chin. Phys. —2014. — Vol. C38. — P. 090001.[57] Lam C. S., Tung W-K. Structure Function Relations at Large Transverse Momenta inLepton Pair Production Processes // Phys. Lett. B. — 1979. — Vol. 80. — P. 228.[58] Lam C. S., Tung W-K.
A Parton Model Relation Sans QCD Modifications in LeptonPair Productions // Phys. Rev. D. — 1980. — Vol. 21. — P. 2712.[59] Nason P. A New method for combining NLO QCD with shower Monte Carloalgorithms // JHEP. — 2004. — Vol. 11. — P.
040. — arXiv : hep-ph/0409146.[60] Alioli S. et al. A general framework for implementing NLO calculations in shower MonteCarlo programs: the POWHEG BOX // JHEP. — 2010. — Vol. 06. — P. 043. — arXiv :hep-ph/1002.2581.[61] Hamilton K., Nason P., Zanderighi G.
MiNLO: Multi-Scale Improved NLO // JHEP. —2012. — Vol. 10. — P. 155. — arXiv : hep-ph/1206.3572.[62] Hamilton K., Nason P., Oleari C., Zanderighi G. Merging H/W/Z + 0 and 1 jet atNLO with no merging scale: a path to parton shower + NNLO matching // JHEP. —2013. — Vol. 05. — P. 082. — arXiv : hep-ex/1212.4504.[63] Martin A. D., Stirling W. J., Thorne R. S., Watt G. Parton distributions for the LHC //Eur.
Phys. J. — 2009. — Vol. C63. — P. 189. — arXiv : hep-ph/0901.0002.[64] Ball R. D., Bertone V., Cerutti F., et al. Impact of Heavy Quark Masses on PartonDistributions and LHC // Nucl. Phys. B. — 2011. — Vol. 849. — P. 296. — arXiv :hep-ph/1101.1300.202[65] Sjostrand T., Mrenna S., Skands P. Z.
A Brief Introduction to PYTHIA 8.1 // Comput.Phys. Commun. — 2008. — Vol. 178. — P. 852. — arXiv : hep-ph/0710.3820.[66] Corcella G. et al. HERWIG 6: An Event generator for hadron emission reactionswith interfering gluons (including supersymmetric processes) // JHEP. — 2001. — Vol.0101. — P.
010. — arXiv : hep-ph/hep-ph/0011363.[67] Gleisberg T. et. al. Event generation with Sherpa 1.1 // JHEP. — 2009. — Vol. 02. —P. 007. — arXiv : hep-ph/0811.4622.[68] Catani S., Krauss F., Kuhn R., Webber B. R. QCD Matrix Elements + PartonShowers // JHEP. — 2001. — Vol. 11. — P. 063. — arXiv : hep-ph/0109231.[69] Hoeche S., Krauss F., Schumann S., Siegert F. QCD matrix elements and truncatedshowers // JHEP. — 2009. — Vol. 05. — P. 053.
— arXiv : hep-ph/0903.1219.[70] Hoeche S., Krauss F., Siegert F. NLO matrix elements and truncated showers //JHEP. — 2011. — Vol. 08. — P. 123. — arXiv : hep-ph/1009.1127.[71] Gleisberg T., Hoeche S. Comix, a new matrix element generator // JHEP. — 2008. —Vol. 0812. — P.
039. — arXiv : hep-ph/0808.3674.[72] Gleisberg T., Hoeche S. Automating dipole subtraction for QCD NLO calculations //Eur. Phys. J. C. — 2008. — Vol. 53. — P. 502. — arXiv : hep-ph/0709.2881.[73] Gottschalk T. D. A realistic model for `+ `− annihilation including partonbremsstrahlung effects // Nucl. Phys. B. — 1983. — Vol. 214.
— P. 201.[74] Gottschalk T. D. An improved description of hadronization in the QCD cluster modelfor `+ `− annihilation // Nucl. Phys. B. — 1984. — Vol. 239. — P. 349.[75] Webber B. R. A QCD model for jet fragmentation including soft gluon interference //Nucl. Phys.
B. — 1984. — Vol. 238. — P. 492.[76] Gottschalk T. D., Morris D. A. A new model for hadronization and `+ `− annihilation //Nucl. Phys. B. — 1987. — Vol. 288. — P. 729.[77] Hoche S., Krauss F., Schonherr M., Siegert F. A critical appraisal of NLO+PS matchingmethods // JHEP. — 2012. — Vol. 09. — P. 49. — arXiv : hep-ex/111.1220.[78] Hoche S., Krauss F., Schonherr M., Siegert F. QCD matrix elements + parton showers:The NLO case // JHEP. — 2013. — Vol. 04.
— P. 027. — arXiv : hep-ex/1207.5030.203[79] Hoche S., Krauss F., Schonherr M., Siegert F. NLO QCD matrix elements + partonshowers in e+ e− → hadrons // JHEP. — 2013. — Vol. 01. — P. 144. — arXiv : hepex/1207.5031.[80] Abat E. et al., TRT Collaborations. The ATLAS Transition Radiation Tracker (TRT)proportional drift tube: design and performance // JINST. — 2008.
— Vol. 3. —P. P02013.[81] Akesson T. et al. Operation of the ATLAS transition radiation tracker under very highirradiation at the CERN LHC // Nucl. Instrum. Meth. — 2005. — Vol. A522. — P. 1185.[82] Capeans M. et al. Recent ageing studies for the ATLAS transition radiation detectors //IEEE Trans. Nucl. Sci. — 2004. — Vol. 51. — P. 960.[83] Sprachmann G. et al. Ageing effects in the ATLAS transition radiation tracker and gasfiltration studies // IEEE Nucl.
Sci. Symp. Conf. Rec. — 2005. — Vol. 2. — P. 1185.[84] E. Abat et al., TRT Collaboration. The ATLAS TRT barrel detector // JINST. —2008. — Vol. 3. — P. P20014.[85] Abat E. et al., TRT Collaboration. The ATLAS TRT end-cap detectors // JINST. —2008. — Vol. 3. — P. P10003.[86] Fedin O. Reconstruction and identification of photons and electrons with the ATLASdetector // Nucl. Instr. and Meth. in Phys.
Res. A. — 2010. — Vol. 623. — P. 306.[87] Lampl W. et al. Calorimeter Clustering Algorithms: Description and Performance. —ATL-LARG-PUB-2008-002, 2008. —URL: http://cdsweb.cern.ch/record/1099735.[88] Cornelissen T. et al. Concepts, design and implementation of the ATLAS newtracking (NEWT). — ATL-SOFT-PUB-2007-007, 2007. — URL: https://cds.cern.ch/record/1020106.[89] Cornelissen T. et al. The global χ2 track fitter in ATLAS // J. Phys. Conf. Ser. —2008. — Vol. 119. — P. 032013.
— URL: http://iopscience.iop.org/1742-6596/119/3/03201.[90] Aad G. et al., ATLAS Collaboration. Improved electron reconstruction in ATLAS usingthe Gaussian Sum Filter-based model for bremsstrahlung. — ATLAS-CONF-2012-047,2012. — URL: http://cdsweb.cern.ch/record/1449796.204[91] Aad G. et al., ATLAS Collaboration. Electron and photon energy calibration with theATLAS detector using LHC Run 1 data // Eur.
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