Changes between Version 8 and Version 9 of WZPrimeAtNLO


Ignore:
Timestamp:
Jan 19, 2017 7:55:04 PM (17 months ago)
Author:
richardphysics
Comment:

Remove many unnecessary $$$

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  • WZPrimeAtNLO

    v8 v9  
    3030\end{eqnarray}
    3131}}}
    32 Here, {{{$i$}}} and {{{$j$}}} denote flavor indices, P,,L/R,,
     32Here, {{{i}}} and {{{j}}} denote flavor indices, P,,L/R,,
    3333are 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 {{{$\zeta_{L,R}^q$}}}
     34and {{{g}}} and {{{\theta_W}}} are the weak coupling constant and mixing angle respectively.
     35We choose coupling normalizations facilitating the mapping to the reference Sequential Standard Model (SSM) Lagrangian {{{{\cal L}_{\rm SSM}}}} [ [#Altarelli 3] ].
     36The real-valued quantities {{{\kappa_{L,R}^q}}} and {{{\zeta_{L,R}^q}}}
    3737serve as overall normalization of the new interactions relative to the strength of the weak coupling constant.
    3838
    39 The interactions involving charged lepton $\ell$ and massless neutrino $\nu_\ell$ fields are parametrized by
     39The interactions involving charged lepton \ell and massless neutrino \nu_\ell fields are parametrized by
    4040{{{
    4141#!latex
     
    5252\end{eqnarray}
    5353}}}
    54 The quantities {{{$\kappa_L^\ell$}}} are real-valued and serve as normalizations for
     54The quantities {{{\kappa_L^\ell}}} are real-valued and serve as normalizations for
    5555leptonic coupling strengths. As no right-handed neutrinos are present in the SM, the corresponding
    56 right-handed leptonic new physics couplings are omitted ({{{$\zeta_R^\nu = \kappa_R^\ell = 0$}}}).
     56right-handed leptonic new physics couplings are omitted ({{{\zeta_R^\nu = \kappa_R^\ell = 0}}}).
    5757
    5858From 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:
     
    127127* Please cite [3,4] for the model file, [4,5] for NLO corrections, and [6] for automated veto resummation.
    128128
    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]
    130130
    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]
    132132
    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/BF01556677
     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/BF01556677
    134134
    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]
    136136
    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/0207290
     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/0207290
    138138
    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]
    140140