Changes between Version 3 and Version 4 of FourFermionFCNCtqll
- Timestamp:
- Mar 24, 2021, 3:08:42 PM (4 years ago)
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FourFermionFCNCtqll
v3 v4 1 == 4-fermion EFT bbll including interference with the SM1 == 4-fermion EFT tqll (q=u,c) 2 2 3 3 == Authors: … … 28 28 29 29 == Model Files: 30 * [https://feynrules.irmp.ucl.ac.be/attachment/wiki/FourFermionFCNCtqll/4fermion-tqll-models.zip 4fermion-tqll-models.zip] : the full model .30 * [https://feynrules.irmp.ucl.ac.be/attachment/wiki/FourFermionFCNCtqll/4fermion-tqll-models.zip 4fermion-tqll-models.zip] : the full model both at the 4FS and at the 5FS. In the paper we use the 5FS. 31 31 * Please note there are two models, one for t-u-l-l, and one for t-c-l-l Contact Interactions. 32 32 33 == Commands for MadGraph5_aMC@NLO, for a production of a muon and an anti-muon with a top quark and up to one more jet s:33 == Commands for MadGraph5_aMC@NLO, for a production of a muon and an anti-muon with a top quark and up to one more jet (NP only): 34 34 {{{ 35 35 define p = g u c d s b u~ c~ d~ s~ b~ … … 49 49 }}} 50 50 51 Where lambdas is the scale of new physics in GeV, fSrr is the coupling of t-u-l-l with scalar operator and right-right chirality of the fermions, etc. 51 Where lambdas is the scale of new physics in GeV, fSrr is the coupling of the t-u-l-l scalar operator with right-right chirality of the fermions, etc. For example, if we set fSrr=1 and all other couplings to 0, we get a scalar operator with: 52 {{{ 53 #!latex 54 \begin{align*} 55 {\cal L}_{tu\ell \ell} = {1\over\Lambda^2} \left( {\bar \ell} P_R \ell \right) \left( \bar t P_R u \right) 56 \end{align*} 57 }}} 52 58 59 60 Note that only operators with the couplings fSrr, fTrr, fVlr, fVrl, fVrr, fVll are generated by this UFO. 53 61 54 62