Single top quark production as a probe of anomalous tqγ and tqZ couplings at the FCC-ee
暂无分享,去创建一个
Mojtaba Mohammadi Najafabadi | M. M. Najafabadi | Hamzeh Khanpour | S. Khatibi | M. K. Yanehsari | Hamzeh Khanpour | Sara Khatibi | Morteza Khatiri Yanehsari
[1] M. Cacciari,et al. Dispelling the N3 myth for the kt jet-finder , 2005, hep-ph/0512210.
[2] P. Speckmayer,et al. The toolkit for multivariate data analysis, TMVA 4 , 2010 .
[3] C. Yue,et al. Search for anomalous couplings via single top quark production in association with a photon at LHC , 2016, 1603.00604.
[4] Claude Duhr,et al. A comprehensive approach to new physics simulations , 2009, 0906.2474.
[5] A. Mertens. New features in Delphes 3 , 2015 .
[6] S. Glashow,et al. Weak Interactions with Lepton-Hadron Symmetry , 1970 .
[7] Ellis,et al. Successive combination jet algorithm for hadron collisions. , 1993, Physical review. D, Particles and fields.
[8] Alfio Lazzaro,et al. The RooStats Project , 2010, 1009.1003.
[9] M. M. Najafabadi,et al. Probing the Anomalous FCNC Interactions in Top-Higgs Final State and Charge Ratio Approach , 2014, 1402.3073.
[10] R. K. Shivpuri,et al. Search for flavor changing neutral currents in decays of top quarks , 2011 .
[11] S. Stapnes,et al. The CLIC programme: Towards a staged $e^{+}e^{−}$ linear collider exploring the terascale : CLIC conceptual design report , 2012, 1209.2543.
[12] Zeus Collaboration. Search for single-top production in ep collisions at HERA , 2003, 1111.3901.
[13] M. Stanitzki,et al. Physics at the $$e^+ e^-$$e+e- linear collider , 2015, 1504.01726.
[14] V. M. Ghete,et al. Search for flavor-changing neutral currents in top-quark decays t → Zq in pp collisions at sqrt[s] = 8 TeV. , 2014, Physical review letters.
[15] Claude Duhr,et al. Introducing an interface between FeynRules and WHIZARD , 2012 .
[16] H. Hesari,et al. Probing the Top Quark Flavour-Changing Neutral Current at a Future Electron-Positron Collider , 2014, Advances in High Energy Physics.
[17] S. Chatrchyan. Search for flavor changing neutral currents in top quark decays in pp collis , 2013 .
[18] F. Dulat,et al. Limit setting procedures and theoretical uncertainties in Higgs boson searches , 2012, 1204.3851.
[19] J. T. Childers,et al. Search for top quark decays t → qH with H → γγ using the ATLAS detector , 2014, 1403.6293.
[20] topcolor-assisted technicolor , 2008 .
[21] Searches for anomalous top-quark interaction at the LEP-2 collider , 1997, hep-ph/9712394.
[22] et al,et al. ILC Reference Design Report Volume 1 - Executive Summary , 2007, 0712.1950.
[23] Lan V. Truong,et al. Search for single top-quark production via flavour-changing neutral currents at 8 TeV with the ATLAS detector , 2015, The European Physical Journal. C, Particles and Fields.
[24] Claude Duhr,et al. A superspace module for the FeynRules package , 2011, Comput. Phys. Commun..
[25] S. Béjar,et al. FCNC-induced heavy-quark events at the LHC from supersymmetry , 2008, 0805.0973.
[26] H. S. Bansil,et al. Search for flavour-changing neutral current top-quark decays to $$\varvec{qZ}$$qZ in $$\varvec{pp}$$pp collision data collected with the ATLAS detector at $$\varvec{\sqrt{s}=8}$$s=8 TeV , 2012 .
[27] D. Whiteson,et al. Snowmass 2013 Top quark working group report , 2013, 1311.2028.
[28] Marcelino B. Santos,et al. CMS Physics Technical Design Report, Volume II: Physics Performance , 2007 .
[29] J. A. Aguilar-Saavedra. A minimal set of top anomalous couplings , 2008, 0811.3842.
[30] Daniel Schulte,et al. A Multi-TeV linear collider based on CLIC technology : CLIC Conceptual Design Report , 2012 .
[31] Y. Gouz,et al. Double top production at hadronic colliders , 1998, hep-ph/9811330.
[32] Benjamin Fuks,et al. BEYOND THE MINIMAL SUPERSYMMETRIC STANDARD MODEL: FROM THEORY TO PHENOMENOLOGY , 2012, 1202.4769.
[33] J. A. Aguilar-Saavedra. Zt, γt and t production at hadron colliders via strong flavour-changing neutral couplings , 2010, 1003.3173.
[34] Claude Duhr,et al. FeynRules 2.0 - A complete toolbox for tree-level phenomenology , 2013, Comput. Phys. Commun..
[35] Kyoungchul Kong,et al. TASI 2011: CalcHEP and PYTHIA Tutorials , 2012, 1208.0035.
[36] A. Read. Presentation of search results: the CLs technique , 2002 .
[37] D. d’Enterria. Physics at the FCC-ee , 2016, 1602.05043.
[38] J. A. Aguilar-Saavedra. Top flavor-changing neutral interactions: Theoretical expectations and experimental detection , 2004, hep-ph/0409342.
[39] Search for single top production via FCNC at LEP at root s=189-208 GeV , 2004, hep-ex/0404014.
[40] Marcel Stanitzki,et al. Physics and Detectors at CLIC: CLIC Conceptual Design Report , 2012 .
[41] P. Skands,et al. Tuning PYTHIA 8.1: the Monash 2013 tune , 2014, 1404.5630.
[42] C. Dionisi,et al. Search for Single Top Production at LEP , 2002 .
[43] Claude Duhr,et al. UFO - The Universal FeynRules Output , 2011, Comput. Phys. Commun..
[44] Jin Min Yang,et al. R-parity violating effects in top quark flavor-changing neutral-current production at LHC , 2009 .
[45] A. Onofre,et al. MEtop—a generator for single top production via FCNC interactions , 2012, 1207.7026.
[46] M. Vos,et al. Top quark precision physics at the International Linear Collider , 2013, 1307.8265.
[47] M. Cacciari,et al. FastJet user manual , 2011, 1111.6097.
[48] M. Seymour,et al. Longitudinally-invariant k ⊥ -clustering algorithms for hadron-hadron collisions , 1993 .
[49] J. Brau,et al. The Physics Case for an e+e- Linear Collider , 2012, 1210.0202.
[50] R. Frederix,et al. The automated computation of tree-level and next-to-leading order differential cross sections, and their matching to parton shower simulations , 2014, 1405.0301.