Changes between Version 26 and Version 27 of HeavyN


Ignore:
Timestamp:
Feb 23, 2016, 6:02:04 PM (9 years ago)
Author:
Richard Ruiz
Comment:

Minor updates for references to Refs.

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  • HeavyN

    v26 v27  
    77
    88In collaboration with
    9 Daniel Alva and Tao Han, and Celine Degrande, Olivier Mattelear, and Jessica Turner.
     9Daniel Alva and Tao Han [ [#Alva 1] ], and Celine Degrande, Olivier Mattelear, and Jessica Turner [ [#Degrande 2] ].
    1010
    1111
    1212== Model Description ==
    13 This effective model extends the Standard Model (SM) field content by introducing three right-handed (RH) neutrinos, which are singlets under the SM gauge symmetry (no color, weak isospin, or weak hypercharge charges). Each RH neutrino possesses one RH Majorana mass. After electroweak symmetry breaking, the Lagrangian with three heavy Majorana neutrinos ''N''i (for i=1,2,3) is given by [ [#Atre 1] ]
     13This effective model extends the Standard Model (SM) field content by introducing three right-handed (RH) neutrinos, which are singlets under the SM gauge symmetry (no color, weak isospin, or weak hypercharge charges). Each RH neutrino possesses one RH Majorana mass. After electroweak symmetry breaking, the Lagrangian with three heavy Majorana neutrinos ''N''i (for i=1,2,3) is given by [ [#Atre 3] ]
    1414{{{
    1515#!latex
    … …  
    8080  * Nine mixing parameters: V''lk'' for ''l'' = ''e, mu, tau'' and ''k'' = 1,2,3. Default values are V''lk'' = Identity(3x3), i.e., Ve1 = Vmu2 = Vta3 = 1 and all others zero.
    8181  * '''Note''': VlN are restricted to be real in the model file.
    82   * '''Note''': Default parameters are set so "out-of-the-box" comparisons can be performed with [ [#Degrande 2] ] and [ [#Alva 3] ].
     82  * '''Note''': Default parameters are set so "out-of-the-box" checks can be made with [ [#Alva 1] ] and [ [#Degrande 2] ].
    8383
    8484
    8585== Validation ==
    86 * The model file was validated at LO in  [ [#Alva 2] ]; see Tables 2 and 5 for further validation checks.
    87 * The model file was validated at NLO in [ [#Degrande 3] ]; see Table 1 for further validation checks.
     86* The model file was validated at LO in  [ [#Alva 1] ]; see Tables 2 and 5 for further validation checks.
     87* The model file was validated at NLO in [ [#Degrande 2] ]; see Table 1 for further validation checks.
    8888* For very large masses, this model has been constructed to satisfy the Goldstone Equivalence Theorem:
    8989{{{
    … …  
    103103
    104104== References ==
    105 * Please cite [ 1 ] for model and [ 2-3 ] for the FR/UFO model files.
     105* Please cite [ 3 ] for the model and [ 1-2 ] for the FR/UFO files.
    106106
    107 [=#Atre] [1] A. Atre, T. Han, S. Pascoli and B. Zhang, ''The Search for Heavy Majorana Neutrinos,'' JHEP '''0905''', 030 (2009),  arXiv:0901.3589 [hep-ph]
     107[=#Alva] [1] D. Alva, T. Han, R. Ruiz, ''Heavy Majorana neutrinos from {{{$W\gamma$}}} ''fusion at hadron colliders,'' JHEP '''1502''', 072 (2015), arXiv:1411.7305 [hep-ph]
    108108
    109109[=#Degrande] [2] C. Degrande, O. Mattelear, R. Ruiz, J. Turner, ''Fully-Automated Precision Predictions for Heavy Neutrino Production Mechanisms at Hadron Colliders,'' arXiv:1602.00000 [hep-ph]
    110110
    111 [=#Alva] [3] D. Alva, T. Han, R. Ruiz, ''Heavy Majorana neutrinos from {{{$W\gamma$}}} ''fusion at hadron colliders,'' JHEP '''1502''', 072 (2015), arXiv:1411.7305 [hep-ph]
    112 
     111[=#Atre] [3] A. Atre, T. Han, S. Pascoli and B. Zhang, ''The Search for Heavy Majorana Neutrinos,'' JHEP '''0905''', 030 (2009),  arXiv:0901.3589 [hep-ph]