Table 1 Characteristics of the materials considered in this work. Effective masses are taken from ref. <sup><a data-track="click" data-track-action="reference anchor" data-track-label="link" data-test="citation-ref" aria-label="Reference 8" title="Kormányos, A. et al. k⋅ p theory for two-dimensional transition metal dichalcogenide semiconductors. 2D Mater. 2, 022001 (2015)." href="/articles/s41699-024-00517-1#ref-CR8" id="ref-link-section-d344486348e997">8</a></sup>, and screening lengths from ref. <sup><a data-track="click" data-track-action="reference anchor" data-track-label="link" data-test="citation-ref" aria-label="Reference 41" title="Goryca, M. et al. Revealing exciton masses and dielectric properties of monolayer semiconductors with high magnetic fields. Nat. Commun. 10, 4172 (2019)." href="/articles/s41699-024-00517-1#ref-CR41" id="ref-link-section-d344486348e1001">41</a></sup>. Here <span class="mathjax-tex">\({E}_{{\rm{b}}}^{{\rm{X}}}\)</span> (<span class="mathjax-tex">\({E}_{{\rm{b}}}^{{\rm{T}}}\)</span>) is the calculated exciton (trion) binding energy in the absence of the magnetic field.