Renormalization group evolution of the standard model dimension six operators. I: formalism and λ dependence
By E. Jenkins, A. Manohar, Michael Trott. Journal of High Energy Physics, 2013
659 citations recorded by the source corpus.
We calculate the order λ, λ2 and λy2 terms of the 59 × 59 one-loop anomalous dimension matrix of dimension-six operators, where λ and y are the Standard Model Higgs self-coupling and a generic Yukawa coupling, respectively. The dimension-six operators modify the running of the Standard Model parameters themselves, and we compute the complete one-loop result for this. We discuss how there is mixing between operators for which no direct one-particle-irreducible diagram exists, due to operator replacements by the equations of motion.
Subfields: Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/f79674bd3fc19dcd3b68f8657e3b7d33c16345fd
How researchers see this paper
The researchers whose trusted networks rank it highest, strongest advocate first. Every researcher gets a different order.
In Nuclear and High Energy Physics
- Cms Collaboration
- Atlas Collaboration
- Gudrun Heinrich
- Fabio Maltoni
- John Ellis
- T. You
- Valentin Hirschi
- R. Frederix
Citations in the corpus
- Geometry of the scalar sector (2016, background): “The independent operators at dimension six, and their renormalization [19, 20], has been worked out in detail [21–28].”
- Probing top quark neutral couplings in the Standard Model Effective Field Theory at NLO in QCD (2016, background): “The anomalous dimensions for these three operators are [14, 40–42]”
- How to use the Standard Model effective field theory (2014, methodology): “As mentioned before, the anomalous dimension matrix γij has been computed in the literature [26–31].”
- Low-energy effective field theory below the electroweak scale: operators and matching (2017, methodology): “[ 3, 18, 19], where p, r, s, t are weak-eigenstate indices, 1 and powers of 1 / Λ are included in the coefficients C .”
- Higgs Physics at the HL-LHC and HE-LHC (2019, methodology): “For the dim = 6 parametrisations we use the Warsaw basis from [41], following the notation and classification from [474].”
- Electroweak constraints on flavorful effective theories (2015, background): “The couplings in the effective Lagrangian are defined at the scale mZ ; we neglect running and mixing effect to other relevant scales as mW or mt which are subleading in our analysis, a detailed discussion on these effects can be found in [43].”