Auxiliary counterterms and their role in effective field theory
arXiv:2603.01561 · doi:10.1140/epja/s10050-026-01836-1
Abstract
Effective field theories include contact-range interactions (or counterterms) for two reasons: representing the unknown short-range physics in a model independent manner and ensuring the cutoff independence of observables. Both are intertwined: cutoff independence alone (modulo truncation errors) already generates counterterms encoding physical information not present in the known long-range physics. Yet, there is also residual cutoff dependence, which is smaller than the uncertainties that are achievable within the effective field theory description and thus can be safely neglected in most settings. If one insists on exact cutoff independence though, new counterterms will be required, but they encode no new physical information and are thus what one could call redundant, or auxiliary, counterterms. It happens that auxiliary counterterms are still useful for solving certain inconsistencies that appear during renormalization or for improving the convergence of the effective field theory expansion. Examples of these use cases are discussed, including the interpretation of the improved actions or the relation between perturbative and non-perturbative renormalization.
arXiv comment19 pages, corresponds with published version
References in corpus (39)
- Modern Theory of Nuclear Forces
- Chiral effective field theory and nuclear forces
- Chiral Dynamics in Nucleons and Nuclei
- Effective Field Theory for Few-Nucleon Systems
- A New Expansion for Nucleon-Nucleon Interactions
- Two-Nucleon Systems from Effective Field Theory
- Nuclear effective field theory: status and perspectives
- Effective Field Theory for Short-Range Forces
- Precision nucleon-nucleon potential at fifth order in the chiral expansion
- Renormalization of One-Pion Exchange and Power Counting
- Nucleon-Nucleon Effective Field Theory Without Pions
- Local chiral effective field theory interactions and quantum Monte Carlo applications
- Power counting with one-pion exchange
- A renormalisation-group treatment of two-body scattering
- Singular Potentials and Limit Cycles
- Improving the Convergence of NN Effective Field Theory
- Regularization, renormalization and "peratization" in effective field theory for two nucleons
- Ground-State Properties of He and O Extrapolated from Lattice QCD with Pionless EFT
- A renormalisation group approach to two-body scattering in the presence of long-range forces
- Renormalization of the Deuteron with One Pion Exchange
- Power Counting of Contact-Range Currents in Effective Field Theory
- Pion-less effective field theory for atomic nuclei and lattice nuclei
- How (not) to renormalize integral equations with singular potentials in effective field theory
- Perturbative nuclear physics
- Wilsonian renormalization group versus subtractive renormalization in effective field theories for nucleon--nucleon scattering
- Power Counting and Wilsonian Renormalization in Nuclear Effective Field Theory
- Renormalization Group Analysis of Boundary Conditions in Potential Scattering
- Power counting in chiral effective field theory and nuclear binding
- Low energy universality and scaling of Van der Waals forces
- Comment on "How (not) to renormalize integral equations with singular potentials in effective field theory"
- Contact operators in renormalization of attractive singular potentials
- Perturbative Calculations of Deuteron Form Factors
- A further study on the renormalization group aspect of perturbative corrections
- Renormalization of proton-proton fusion in chiral effective field theory
- Reexamining the perturbative renormalizability of the coupled triplets
- Causality, universality, and effective field theory for van der Waals interactions
- Perturbative renormalization of chiral nuclear forces at subleading order in 3S1-3D1 channel
- Regulator constraints for the perturbative renormalizability of attractive triplets
- Feasibility of perturbative generation of bound-states from resonances or virtual states