Changes between Version 39 and Version 40 of SMEFT

Timestamp:

Sep 18, 2017, 11:27:20 AM (7 years ago)

Author:

Ilaria Brivio

Comment:

--

SMEFT

@@ -16 +16 @@
 
 
-The SMEFT is constructed out of a series of SU(3),,C,, × SU(2),,L,, × U(1),,Y,, invariant (local and analytic) higher dimensional operators L,,6,,, L,,7,,, ... built out of the SM fields.[[BR]]
-The SMEFTsim package provides a complete implementation of the dimension-6 Lagrangian adopting the Warsaw basis [https://arxiv.org/abs/1008.4884/ arXiv:1008.4884]
+The Standard Model Effective Field Theory (SMEFT) is constructed out of a series of SU(3),,C,, × SU(2),,L,, × U(1),,Y,, invariant (local and analytic) higher dimensional operators L,,6,,, L,,7,,, ... built out of the SM fields.[[BR]]
+The SMEFTsim package provides a complete implementation of the lepton and baryon number conserving dimension-6 Lagrangian adopting the Warsaw basis [https://arxiv.org/abs/1008.4884/ arXiv:1008.4884]
 
-The SM Lagrangian is extended with the inclusion of the complete set of baryon-number-conserving operators of the Warsaw basis and of the SM loop-induced  Higgs couplings to gg, γγ and Zγ. [[BR]]
-Importantly, field rotations required to have canonically normalized kinetic terms and parameter redefinitions following from the choice of an input parameters set are automatically applied in the Lagrangian.
+The SM Lagrangian [link] is included and extended with the SM loop-induced  Higgs couplings to gg, γγ and Zγ. [[BR]]
 
 
@@ -28 +27 @@
 * The flavour general case
 * The U(3)^5^ flavor symmetric case, with possible non-SM CP-violating phases
-* A linear Minimal flavor violation (MFV) ansatz, in which non-SM CP-violating effects are neglected, but flavor-violation spurion insertions are allowed in quark currents
+* A linear Minimal flavor violation (MFV) ansatz [Gino's paper], in which non-SM CP-violating effects are neglected, but linear flavor-violating spurion insertions are allowed in quark currents
 
 For each model it is possible to choose between two input parameters sets for the electroweak sector, namely:
 * α scheme: {α,,em,,, m,,Z,, , G,,f,,} 
-* m,,W,, scheme: {m,,W,,, m,,Z,, , G,,f,,}
+* m,,W,, scheme: {m,,W,,, m,,Z,, , G,,f,,} 
+
+Importantly, field rotations required to have canonically normalized kinetic terms and parameter redefinitions following from the choice of an input parameters set are automatically applied in the Lagrangian.
 
 Two independent models sets (A and B) are supplied. Each set contains a main file, a number of subroutines and restriction files. 
@@ -39 +40 @@
 
 
-We appreciate if you could report us any inconsistency or bugs. 
+We would appreciate if you could report to us any inconsistency or bugs.