We calculate the gauge terms of the one-loop anomalous dimension matrix for the
dimension-six operators of the Standard Model effective field theory (SM EFT). Combining these …

We calculate the complete order y 2 and y 4 terms of the 59× 59 one-loop anomalous
dimension matrix for the dimension-six operators of the Standard Model effective field theory, …

We calculate the order λ, λ 2 and λy 2 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 …

The gauge-invariant operators up to dimension six in the low-energy effective field theory
below the electroweak scale are classified. There are 70 Hermitian dimension-five and 3631 …

We compute the one-loop anomalous dimensions of the low-energy effective Lagrangian
below the electroweak scale, up to terms of dimension six. The theory has 70 dimension-five …

We compute the renormalization of dimension six Higgs-gauge boson operators that can
modify the h→ γγ rate at tree-level. Operator mixing is shown to lead to an important …

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 …

A geometric formulation of Higgs Effective Field Theory (HEFT) is presented. Experimental
observables are given in terms of geometric invariants of the scalar sigma model sector such …

We derive the general counting rules for a quantum effective field theory (EFT) in\(\mathsf {d}\)
dimensions. The rules are valid for strongly and weakly coupled theories, and they predict …

The S-matrix of a quantum field theory is unchanged by field redefinitions, and so it only
depends on geometric quantities such as the curvature of field space. Whether the Higgs …