Changes between Version 8 and Version 9 of WZPrimeAtNLO
- Timestamp:
- Jan 19, 2017, 7:55:04 PM (8 years ago)
Legend:
- Unmodified
- Added
- Removed
- Modified
-
WZPrimeAtNLO
v8 v9 30 30 \end{eqnarray} 31 31 }}} 32 Here, {{{ $i$}}} and {{{$j$}}} denote flavor indices, P,,L/R,,32 Here, {{{i}}} and {{{j}}} denote flavor indices, P,,L/R,, 33 33 are the usual left/right-handed chirality projectors, V^CKM^ is the CKM matrix, 34 and {{{ $g$}}} and {{{$\theta_W$}}} are the weak coupling constant and mixing angle respectively.35 We choose coupling normalizations facilitating the mapping to the reference Sequential Standard Model (SSM) Lagrangian {{{ ${\cal L}_{\rm SSM}$}}} [ [#Altarelli 3] ].36 The real-valued quantities {{{ $\kappa_{L,R}^q$}}} and {{{$\zeta_{L,R}^q$}}}34 and {{{g}}} and {{{\theta_W}}} are the weak coupling constant and mixing angle respectively. 35 We choose coupling normalizations facilitating the mapping to the reference Sequential Standard Model (SSM) Lagrangian {{{{\cal L}_{\rm SSM}}}} [ [#Altarelli 3] ]. 36 The real-valued quantities {{{\kappa_{L,R}^q}}} and {{{\zeta_{L,R}^q}}} 37 37 serve as overall normalization of the new interactions relative to the strength of the weak coupling constant. 38 38 39 The interactions involving charged lepton $\ell$ and massless neutrino $\nu_\ell$fields are parametrized by39 The interactions involving charged lepton \ell and massless neutrino \nu_\ell fields are parametrized by 40 40 {{{ 41 41 #!latex … … 52 52 \end{eqnarray} 53 53 }}} 54 The quantities {{{ $\kappa_L^\ell$}}} are real-valued and serve as normalizations for54 The quantities {{{\kappa_L^\ell}}} are real-valued and serve as normalizations for 55 55 leptonic coupling strengths. As no right-handed neutrinos are present in the SM, the corresponding 56 right-handed leptonic new physics couplings are omitted ({{{ $\zeta_R^\nu = \kappa_R^\ell = 0$}}}).56 right-handed leptonic new physics couplings are omitted ({{{\zeta_R^\nu = \kappa_R^\ell = 0}}}). 57 57 58 58 From our general Lagrangians, the SSM limit is obtained by imposing the coupling strengths to be equal to the SM weak couplings up to an overall normalization factor: … … 127 127 * Please cite [3,4] for the model file, [4,5] for NLO corrections, and [6] for automated veto resummation. 128 128 129 [=#Gopalakrishna] [1] S. Gopalakrishna, T. Han, I. Lewis, Z.-G. Si and Y. F. Zhou, ''Chiral Couplings of {{{ $W'$}}} and Top Quark Polarization at the LHC,'' PRD'''82''', 115020 (2010) arXiv:1008.3508 [hep-ph]129 [=#Gopalakrishna] [1] S. Gopalakrishna, T. Han, I. Lewis, Z.-G. Si and Y. F. Zhou, ''Chiral Couplings of {{{W'}}} and Top Quark Polarization at the LHC,'' PRD'''82''', 115020 (2010) arXiv:1008.3508 [hep-ph] 130 130 131 [=#Han] [2] T. Han, I. Lewis, R. Ruiz and Z.-G. Si, ''Lepton Number Violation and {{{ $W^\prime$}}} Chiral Couplings at the LHC,'' PRD'''87''', no. 3, 035011 (2013) arXiv:1211.6447 [hep-ph]131 [=#Han] [2] T. Han, I. Lewis, R. Ruiz and Z.-G. Si, ''Lepton Number Violation and {{{W'}}} Chiral Couplings at the LHC,'' PRD'''87''', no. 3, 035011 (2013) arXiv:1211.6447 [hep-ph] 132 132 133 [=#Altarelli] [3] G. Altarelli, B. Mele and M. Ruiz-Altaba, ''Searching for New Heavy Vector Bosons in $p \bar{p}$Colliders,'' Z. Phys. C'''45''', 109 (1989), doi:10.1007/BF01556677133 [=#Altarelli] [3] G. Altarelli, B. Mele and M. Ruiz-Altaba, ''Searching for New Heavy Vector Bosons in p \bar{p} Colliders,'' Z. Phys. C'''45''', 109 (1989), doi:10.1007/BF01556677 134 134 135 [=#Fuks] [4] B. Fuks, R. Ruiz, ''A Comprehensive Framework for Studying {{{ $W'$}}} and {{{$Z'$}}} Bosons at Hadron Colliders with Automated Jet Veto Resummation,'' arXiv:1701.xxxx [hep-ph]135 [=#Fuks] [4] B. Fuks, R. Ruiz, ''A Comprehensive Framework for Studying {{{W'}}} and {{{Z'}}} Bosons at Hadron Colliders with Automated Jet Veto Resummation,'' arXiv:1701.xxxx [hep-ph] 136 136 137 [=#Sullivan] [5] Z. Sullivan, ''Fully differential {{{ $W'$}}} production and decay at next-to-leading order in QCD,'' PRD'''66''', 075011 (2002), arXiv:hep-ph/0207290137 [=#Sullivan] [5] Z. Sullivan, ''Fully differential {{{W'}}} production and decay at next-to-leading order in QCD,'' PRD'''66''', 075011 (2002), arXiv:hep-ph/0207290 138 138 139 [=#Becher] [6] T. Becher, R. Frederix, M. Neubert and L. Rothen, ''Automated NNLL $+$NLO resummation for jet-veto cross sections,'' EPJC'''75''', no. 4, 154 (2015) arXiv:1412.8408 [hep-ph]139 [=#Becher] [6] T. Becher, R. Frederix, M. Neubert and L. Rothen, ''Automated NNLL + NLO resummation for jet-veto cross sections,'' EPJC'''75''', no. 4, 154 (2015) arXiv:1412.8408 [hep-ph] 140 140