Single-top t-channel hadroproduction in the four-flavour scheme with POWHEG and aMC@NLO

[1]  J. A. Stillings Evidence for the associated production of a W boson and a top quark in ATLAS , 2012 .

[2]  M. L. Ferrer,et al.  Measurement of the t-channel single top-quark production cross section in pp collisions at root s=7 TeV with the ATLAS detector , 2012 .

[3]  M. L. Ferrer,et al.  Search for FCNC single top-quark production at √s = 7 TeV with the ATLAS detector , 2012 .

[4]  R. Keith Ellis,et al.  Top-Quark Processes at NLO in Production and Decay , 2012, 1204.1513.

[5]  G. Ridolfi,et al.  b-initiated processes at the LHC: a reappraisal , 2012, 1203.6393.

[6]  M. L. Ferrer,et al.  Search for FCNC single top-quark production at √s = 7 TeV with the ATLAS detector , 2012, 1203.0529.

[7]  H. Lacker,et al.  Model-independent extraction of |Vtq| matrix elements from top-quark measurements at hadron colliders , 2012, 1202.4694.

[8]  Rikkert Frederix,et al.  Four-lepton production at hadron colliders: aMC@NLO predictions with theoretical uncertainties , 2012, Journal of High Energy Physics.

[9]  Simon Plätzer,et al.  Dipole showers and automated NLO matching in Herwig++ , 2011, 1109.6256.

[10]  M. Cacciari,et al.  FastJet user manual , 2011, 1111.6097.

[11]  Frank Siegert,et al.  A critical appraisal of NLO+PS matching methods , 2011, 1111.1220.

[12]  V. M. Ghete,et al.  Measurement of the t-channel single top quark production cross section in pp collisions at √s=7  TeV. , 2011, Physical review letters.

[13]  C. Collaboration Measurement of the t-channel single top-quark production cross section in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector , 2011, 1205.3130.

[14]  R. Pittau,et al.  Scalar and pseudoscalar Higgs production in association with a top–antitop pair , 2011, 1104.5613.

[15]  N. Kidonakis Next-to-next-to-leading-order collinear and soft gluon corrections for t-channel single top quark production , 2011, 1103.2792.

[16]  F. Giannuzzi,et al.  Off-shell effects for t -channel and s -channel single-top production at next-to-leading order in QCD , 2011, 1102.5267.

[17]  E. Re Single-top Wt-channel production matched with parton showers using the POWHEG method , 2010, 1009.2450.

[18]  S. Frixione,et al.  NLO QCD corrections in Herwig++ with MC@NLO , 2010, 1010.0568.

[19]  F. Siegert,et al.  Automating the Powheg method in Sherpa , 2010, 1008.5399.

[20]  A. Signer,et al.  Production-decay interferences at NLO in QCD for t-channel single-top production , 2010, 1007.0893.

[21]  Chong-Sheng Li,et al.  Factorization and resummation of s-channel single top quark production , 2010, 1010.4509.

[22]  et al,et al.  Observation of single top quark production and measurement of vertical bar V-tb vertical bar with CDF , 2010, 1004.1181.

[23]  S. Frixione,et al.  Matching NLO QCD computations with PYTHIA using MC@NLO , 2010, 1002.4293.

[24]  E. Re,et al.  A general framework for implementing NLO calculations in shower Monte Carlo programs: the POWHEG BOX , 2010, 1002.2581.

[25]  E. al.,et al.  Measurement of the t-channel single top quark production cross section , 2009, 0907.4259.

[26]  E. Re,et al.  NLO single-top production matched with shower in POWHEG: s- and t-channel contributions , 2009, 0907.4076.

[27]  Tim Stelzer,et al.  Automation of next-to-leading order computations in QCD: the FKS subtraction , 2009, 0908.4272.

[28]  F. T. Collaboration,et al.  Combination of CDF and D0 Measurements of the Single Top Production Cross Section , 2009, 0908.2171.

[29]  R. Frederix,et al.  NLO predictions for t-channel production of single top and fourth generation quarks at hadron colliders , 2009, 0907.3933.

[30]  R. E. Hall,et al.  Observation of single top-quark production. , 2009, Physical review letters.

[31]  R. Frederix,et al.  Next-to-leading-order predictions for t-channel single-top production at hadron colliders. , 2009, Physical review letters.

[32]  A. Shibata,et al.  Top Quark Physics at the LHC , 2008, DIS 2008.

[33]  P. Motylinski,et al.  Single-top hadroproduction in association with a W boson , 2008, 0805.3067.

[34]  M. Beccaria,et al.  Complete one-loop calculation of electroweak supersymmetric effects in t-channel single top production at CERN LHC , 2008, 0802.1994.

[35]  M. Beccaria,et al.  A complete one-loop calculation of electroweak supersymmetric effects in t-channel single top production at LHC , 2008 .

[36]  E. Barrelet,et al.  Dijet cross sections and parton densities in diffractive DIS at HERA , 2007 .

[37]  P. Nason,et al.  Matching NLO QCD computations with Parton Shower simulations: the POWHEG method , 2007, 0709.2092.

[38]  R. S. Thorne,et al.  Parton distributions for the LHC , 2007, 0901.0002.

[39]  J. Wudka,et al.  Search for new physics via single-top production at the LHC , 2007, 0704.2809.

[40]  Tim Stelzer,et al.  MadGraph/MadEvent v4: The New Web Generation , 2007, 0706.2334.

[41]  S. Kalinin,et al.  Is Vtb≃1? , 2006, hep-ph/0607115.

[42]  P. Motylinski,et al.  Preprint typeset in JHEP style.- PAPER VERSION Cavendish–HEP–05/24 , 2005 .

[43]  M. Cacciari,et al.  Dispelling the N3 myth for the kt jet-finder , 2005, hep-ph/0512210.

[44]  Dimitri Bourilkov,et al.  The Les Houches accord PDFs (LHAPDF) and LHAGLUE , 2005, hep-ph/0508110.

[45]  R. Brock,et al.  Next-to-leading order corrections to single top quark production and decay at the Fermilab Tevatron. II. t-channel process , 2005, hep-ph/0504230.

[46]  P. Nason A new method for combining NLO QCD with shower Monte Carlo algorithms , 2004, hep-ph/0409146.

[47]  J. Campbell,et al.  Single top-quark production and decay at next-to-leading order , 2004, hep-ph/0408158.

[48]  S. Weinzierl,et al.  The fully differential single-top-quark cross section in next-to-leading order QCD , 2002, hep-ph/0207055.

[49]  S. Frixione,et al.  Matching NLO QCD computations and parton shower simulations , 2002, hep-ph/0204244.

[50]  F. Ferrari Large N and double scaling limits in two dimensions , 2002, hep-th/0202002.

[51]  S. Mrenna,et al.  Pythia 6.3 physics and manual , 2003, hep-ph/0308153.

[52]  Paul Koerber,et al.  The non-abelian Born-Infeld action through order $\alpha'{}^3$ , 2001 .

[53]  S. Moretti,et al.  HERWIG 6: an event generator for hadron emission reactions with interfering gluons (including supersymmetric processes) , 2001 .

[54]  S. Moretti,et al.  HERWIG 6.5: an event generator for Hadron Emission Reactions With Interfering Gluons (including supersymmetric processes) , 2000, hep-ph/0011363.

[55]  C. Yuan,et al.  Single top quark production as a window to physics beyond the standard model , 2000, hep-ph/0007298.

[56]  M. Seymour,et al.  Erratum to A general algorithm for calculating jet cross sections in NLO QCD [Nucl. Phys. B 485 (1 , 1998 .

[57]  M. Seymour,et al.  A general algorithm for calculating jet cross sections in NLO QCD , 1996, hep-ph/9605323.

[58]  Z. Kunszt,et al.  Three-jet cross sections to next-to-leading order , 1995, hep-ph/9512328.

[59]  M. Seymour,et al.  Longitudinally-invariant k ⊥ -clustering algorithms for hadron-hadron collisions , 1993 .

[60]  Ansgar Denner,et al.  Feyn Calc―computer-algebraic calculation of Feynman amplitudes , 1991 .

[61]  Dicus,et al.  Production of heavy quarks from W-gluon fusion. , 1986, Physical review. D, Particles and fields.

[62]  E. Byckling,et al.  n-particle phase space in terms of invariant momentum transfers , 1969 .