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Axion EFT in the BMHV Scheme: Flavor Currents, Evanescent Operators and Ward Identities

Deepanshu Bisht, Sabyasachi Chakraborty, Atanu Samanta

Abstract

We present a systematic analysis of axion effective field theory within the Breitenlohner-Maison-`t Hooft-Veltman (BMHV) scheme, focusing on the renormalization of fermionic dimension-five operators and the associated chiral flavor currents. In this framework, the non-anticommuting nature of $γ_5$ in $d \neq 4$ dimensions leads to violations of naive Ward identities through the emergence of evanescent operators. We derive the bare and renormalized Ward identities for chiral currents, explicitly identifying the equation-of-motion and evanescent operator contributions. Using diagrammatic calculations, we verify the validity of these identities up to two-loop order $\mathcal{O}(α_s^2)$, including both pole and finite terms. We demonstrate how evanescent operators mix into physical operators and determine the finite renormalization required to restore four-dimensional Ward identities, recovering the expected structure of axial current renormalization and the anomaly. Our results provide a consistent and transparent framework for multi-loop computations in axion EFT and highlight the essential role of evanescent operators in maintaining scheme consistency.

Axion EFT in the BMHV Scheme: Flavor Currents, Evanescent Operators and Ward Identities

Abstract

We present a systematic analysis of axion effective field theory within the Breitenlohner-Maison-`t Hooft-Veltman (BMHV) scheme, focusing on the renormalization of fermionic dimension-five operators and the associated chiral flavor currents. In this framework, the non-anticommuting nature of in dimensions leads to violations of naive Ward identities through the emergence of evanescent operators. We derive the bare and renormalized Ward identities for chiral currents, explicitly identifying the equation-of-motion and evanescent operator contributions. Using diagrammatic calculations, we verify the validity of these identities up to two-loop order , including both pole and finite terms. We demonstrate how evanescent operators mix into physical operators and determine the finite renormalization required to restore four-dimensional Ward identities, recovering the expected structure of axial current renormalization and the anomaly. Our results provide a consistent and transparent framework for multi-loop computations in axion EFT and highlight the essential role of evanescent operators in maintaining scheme consistency.

Paper Structure

This paper contains 21 sections, 65 equations, 5 figures, 3 tables.

Figures (5)

  • Figure 1: Blob represents the tree-level operator insertion.
  • Figure 2: Diagrams at one-loop, cross represents current insertion.
  • Figure 3: Fermion self-energy diagrams at $\mathcal{O}(\alpha_s^2)$
  • Figure 4: Crosses indicate current insertions; bracketed numbers show the total possible diagrams for that topology (e.g., J2 represents one of three).
  • Figure 5: Crosses represent evanescent operator insertion, where 'EG' and 'EK' imply gluonic and kinetic evanescent insertion.