Effective Field Theory Perspective On King Non-linearity

TL;DR

This paper develops an effective field theory framework to interpret King non-linearity in isotope shifts, enabling precise separation of nuclear and Standard Model effects, and improving the understanding of heavy nuclei structure.

Contribution

It introduces a systematic EFT approach to analyze King non-linearity, clarifies the role of nuclear effects, and refines the interpretation of isotope shift measurements.

Findings

Reveals the $ angle r^2 angle^2$ term arises at second-order perturbation.

Derives the long-range $1/r^4$ potential from nuclear polarizability.

Provides a classification of Standard Model sources of King NL.

Abstract

Precision spectroscopic measurements of isotope shifts have recently reached a high level of accuracy. Tests of King non-linearity (NL) along isotope chains have been proposed as a tool to search for fifth-force mediators. At the same time, these tests can potentially teach us about the structure of heavy nuclei at unprecedented precision, where King NL has already been observed in several systems. A robust interpretation of the existing data, however, is hampered by incomplete control over the Standard Model (SM) contributions. We develop a systematic effective field theory framework, matching the SM onto scalar non-relativistic QED in the infinite nuclear mass limit and then onto quantum-mechanical potentials. This approach organizes all nuclear effects into a small set of Wilson coefficients and cleanly separates short- and long-distance physics. We show that the commonly used treatment of the $\langle r^2\rangle^2$ term needs to be reconsidered, as it arises only at second-order in perturbation theory, and we derive the long-range $1/r^4$ potential from nuclear polarizability. Applying the framework to hydrogen-like systems, we provide a transparent classification of SM sources of King NL relevant for current and future isotope-shift experiments. The formalism can be applied to learn about the shape of the heavy scalar nuclei at a higher level of precision and detail than what was previously attainable.