Regularization ================== The NJL model is non-renormalizable and must be regularized. This module allows the user to choose between a conventional cutoff regularization and a renormalization-group–consistent regularization [1]_, [2]_, [3]_, [4]_. Renormalization-group consistency for low-energy models, including diquark condensates, was outlined in [5]_. In the language of the functional renormalization group, it states that the effective potential in the infrared must not depend on the initial UV scale. The renormalization-group-consistent version of the NJL model allows one to avoid cutoff artifacts of the conventional regularization. This is of particular importance for the study of color-superconducting quark matter at neutron-star densities, as cutoff artifacts lead to unphysical suppression of the diquark condensates, which affects the phase structure at nonzero temperatures. References ---------- .. [1] H. Gholami, M. Hofmann, and M. Buballa, *Phys. Rev. D* **111**, 014006 (2025), `journal link `__, arXiv:`2408.06704 `_ [hep-ph]. .. [2] H. Gholami, M. Hofmann, and M. Buballa (2025), arXiv:`2508.21735 `_ [astro-ph.HE]. .. [3] H. Gholami, I. A. Rather, M. Hofmann, M. Buballa, and J. Schaffner-Bielich, *Phys. Rev. D* **111**, 103034 (2025), `journal link `__, arXiv:`2411.04064 `_ [hep-ph]. .. [4] J.-E. Christian, I. A. Rather, H. Gholami, and M. Hofmann (2025), arXiv:`2503.13626 `_ [astro-ph.HE]. .. [5] J. Braun, M. Leonhardt, and J. M. Pawlowski, *SciPost Phys.* **6**, 056 (2019), `journal link `__, arXiv:`1806.04432 `_ [hep-ph].