Renormalization group evolution of dimension-six baryon number violating operators

By R. Alonso, Hsi-Ming Chang, E. Jenkins, A. Manohar, Brian Shotwell. 2014

185 citations recorded by the source corpus.

Abstract We calculate the one-loop anomalous dimension matrix for the dimension-six baryon number violating operators of the Standard Model effective field theory, including right-handed neutrino fields. We discuss the flavor structure of the renormalization group evolution in the contexts of minimal flavor violation and unification.

Subfields: Nuclear and High Energy Physics

View Paper: https://www.semanticscholar.org/paper/aa502707c904cef68d0862ba8a25c24780c7fdd2

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In Nuclear and High Energy Physics

1. E. Jenkins
2. A. Manohar
3. P. Stoffer
4. L. Lehman
5. Michael Trott
6. Fabio Maltoni
7. R. Alonso
8. Adam Martin

Citations in the corpus

• Renormalization group evolution of the Standard Model dimension six operators III: gauge coupling dependence and phenomenology (2013, methodology): “ms in the 59 ×59 anomalous dimension matrix of the baryon number conserving operators. The anomalous dimension matrix of the dimension-six baryon number violating operators have been computed in Ref. [96]. Many of the results are lengthy, but a few important cases such as gg→h, h→γγand h→γZhave simp”
• Lepton universality violation with lepton flavor conservation in B-meson decays (2015, background): “6) from the high scale to the electro-weak vev (the full anomalous dimension matrix is given in [64–67]), and then down to the B-meson scale [52–55].”
• 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].”
• Renormalization group evolution of the Standard Model dimension six operators II: Yukawa dependence (2013, unknown): “[21].”
• Hilbert Series for Constructing Lagrangians: expanding the phenomenologist's toolbox (2015, background): “However, it has been noted that only four of these five operators are independent if the flavor structure is taken into account [37, 42].”
• Low-energy effective field theory below the electroweak scale: operators and matching (2017, background): “In addition to the 2499 dimension-six operators (for three generations of fermions), there are 273 dimension-six ∆ B = ∆ L = 1 operators (7 irreducible flavor representations), and their Hermitian conjugates [1, 2, 4–7].”
• Global approach to top-quark flavor-changing interactions (2014, background): “[79–82].”
• Extending the Standard Model Effective Field Theory with the Complete Set of Dimension-7 Operators (2014, background): “A series of papers calculated the full 59 × 59 anomalous dimension matrix for the operators that preserve baryon number [12–17], and the anomalous dimension matrix for the baryon-number violating operators followed soon after [18].”