Magnetic moments of $A = 3$ nuclei with chiral effective field theory operators

TL;DR

This study uses chiral effective field theory to calculate the magnetic moments of Triton and Helium-3, employing systematically derived interactions and currents, and compares results with experimental data.

Contribution

It applies consistently derived LENPIC chiral interactions and currents to compute magnetic moments of $A=3$ nuclei, including derivation of the N2LO magnetic dipole operator.

Findings

Current corrections through N2LO improve agreement with experimental magnetic moments.

The approach demonstrates the effectiveness of chiral EFT in nuclear magnetic moment calculations.

Results show partial but not complete agreement with experimental data.

Abstract

Chiral effective field theory ($\chi$EFT) provides a framework for obtaining internucleon interactions in a systematically improvable fashion from first principles, while also providing for the derivation of consistent electroweak current operators. In this work, we apply consistently derived interactions and currents towards calculating the magnetic dipole moments of the $A=3$ systems Triton and Helium-3. We focus here on LENPIC interactions obtained using semilocal coordinate-space (SCS) regularization. Starting from the momentum-space representation of the LENPIC $\chi$EFT vector current, we derive the SCS-regularized magnetic dipole operator up through N2LO. We then carry out no-core shell model calculations for Triton and Helium-3 systems, using the SCS LENPIC interaction at N2LO in $\chi$EFT, and evaluate the magnetic dipole moments obtained using the consistently derived one-nucleon and two-nucleon electromagnetic currents. As anticipated by prior results with $\chi$EFT currents, the current corrections through N2LO provide improved, but not yet complete, agreement with experiment for the Triton and Helium-3 magnetic dipole moments.