Changes between Version 10 and Version 11 of TypeIISeesaw

Timestamp:

Nov 19, 2019, 4:53:50 AM (5 years ago)

Author:

Benjamin Fuks

Comment:

--

TypeIISeesaw

@@ -18 +18 @@
 \end{equation}
 }}}
-where the extra terms respectively represents the gauge-invariant kinetic terms for the triplet, the extra pieces to the scalar potential and the Yukawa interactions giving rise to neutrino masses. The above Lagrangian was implemented in the Feynman Gauge into !FeynRules 2.3.35. QCD renormalization and R,,2,, rational counterterms were determined using [/raw-attachment/wiki/MSSMatNLO/MoGRe_v1.1.m MoGRe v1.1], NLOCT v1.02 and !FeynArts 3.9. Feynman rules were collected into a single UFO, available below. In the [/raw-attachment/wiki/TypeIISeesaw/typeII_4FNS_v1_1.ufo.tgz UFO model], four massless quarks are assumed as are zero off-diagonal CKM matrix entries.
+where the extra terms respectively represents the gauge-invariant kinetic terms for the triplet, the extra pieces to the scalar potential and the Yukawa interactions giving rise to neutrino masses. The above Lagrangian was implemented in the Feynman Gauge into !FeynRules 2.3.35. QCD renormalisation and R,,2,, rational counterterms were determined using [/raw-attachment/wiki/MSSMatNLO/MoGRe_v1.1.m MoGRe v1.1], NLOCT v1.02 and !FeynArts 3.9. Feynman rules were collected into a single UFO, available below. In the [/raw-attachment/wiki/TypeIISeesaw/typeII_4FNS_v1_2.ufo.tgz UFO model] (normal hierarchy) and [/raw-attachment/wiki/TypeIISeesaw/typeII_ih_4FNS_v1_1.ufo.tgz UFO model] (inverted hierarchy) and , four massless quarks are assumed as are zero off-diagonal CKM matrix entries.
 These additions permit tree-level calculations at LO and NLO in QCD and loop-induced calculations at LO in QCD using MadGraph_aMC@NLO.
 
@@ -26 +26 @@
  - the oscillation parameters th12 (θ,,12,,), th13 (θ,,13,,), th23 (θ,,23,,), delCP (φ,,CP,,), phiM1 (φ,,1,,), phiM2 (φ,,2,,) collected in the LH block PMNS;
  - the masses of the Higgs (PDG 125), Δ^0^ (PDG 44), Δ^±^ (PDG 38)  and Δ^±±^ (PDG 44) fields (in the LH block MASS);
- - the triplet vev v,,Δ,, (block VEVD)
+ - the triplet vev v,,Δ,, (block VEVDELTA)
  - two quartic couplings collected in the block QUARTICS
 
@@ -34 +34 @@
  - the oscillation parameters th12 (θ,,12,,), th13 (θ,,13,,), th23 (θ,,23,,), delCP (φ,,CP,,), phiM1 (φ,,1,,), phiM2 (φ,,2,,) collected in the LH block PMNS;
  - the masses of the Higgs (PDG 125), Δ^0^ (PDG 44), Δ^±^ (PDG 38)  and Δ^±±^ (PDG 44) fields (in the LH block MASS);
- - the triplet vev v,,Δ,, (block VEVD)
+ - the triplet vev v,,Δ,, (block VEVDELTA)
  - two quartic couplings collected in the block QUARTICS
 
@@ -52 +52 @@
    * [/raw-attachment/wiki/TypeIISeesaw/type_ii.fr type_ii.fr]: The !FeynRule Type II Seesaw implementation (version 1.1) to be used with a reduced SM implementation (only the modified SM parts are included in type_ii.fr).
    * [/raw-attachment/wiki/TypeIISeesaw/use-MoGre.nb use-MoGre.nb]: Illustrative Mathematica notebook using MoGRe (for NLO UFO generation and counterterm/R,,2,, calculations).
-   * [/raw-attachment/wiki/TypeIISeesaw/typeII_4FNS_v1_1.ufo.tgz typeII_4FNS_v1_1.ufo.tgz]: Standalone UFO folder.
+   * [/raw-attachment/wiki/TypeIISeesaw/typeII_4FNS_v1_2.ufo.tgz typeII_4FNS_v1_2.ufo.tgz]: Standalone UFO folder.
 
  * Files specific to an inverted neutrino mass hierarchy (Mv3 < Mv1 < Mv2):
    * [/raw-attachment/wiki/TypeIISeesaw/type_ii_ih.fr type_ii_ih.fr]: The !FeynRule Type II Seesaw implementation (version 1.1) to be used with a reduced SM implementation (only the modified SM parts are included in type_ii_ih.fr).
    * [/raw-attachment/wiki/TypeIISeesaw/use-MoGre_ih.nb use-MoGre_ih.nb]: Illustrative Mathematica notebook using MoGRe (for NLO UFO generation and counterterm/R,,2,, calculations).
-   * [/raw-attachment/wiki/TypeIISeesaw/typeII_ih_4FNS_v1_0.ufo.tgz typeII_ih_4FNS_v1_0.ufo.tgz]: Standalone UFO folder.
+   * [/raw-attachment/wiki/TypeIISeesaw/typeII_ih_4FNS_v1_1.ufo.tgz typeII_ih_4FNS_v1_1.ufo.tgz]: Standalone UFO folder.