We investigate the hydrostatic equilibrium and global structure of neutron stars within symmetric teleparallel gravity, where gravitational interactions are mediated by the non-metricity scalar Q. Working within the metric-affine formulation, we adopt the regular, constant-Q branch (Q = Q_*) of $f(Q)$ gravity, which preserves regularity at the stellar centre while maintaining explicit dependence on the non-linear functional form through f(Q_*) and its derivatives. We propose three novel non-linear $f(Q)$ extensions: (i) a Born-Infeld-inspired model, (ii) a Hu--Sawicki analogue, and (iii) a Tsujikawa-inspired model. Incorporating state-of-the-art realistic unified equations of state, namely GPPVA(DD2) and SLy4, we numerically solve the modified Tolman-Oppenheimer-Volkoff equations and evaluate stellar stability via the Harrison-Zel'dovich-Novikov criterion. The Born-Infeld and Hu-Sawicki analogues smoothly recover the general relativistic limit as their control parameters increase, predicting stellar radii for low-mass objects (M < 2.0\,M_) that match observational constraints from X-ray binaries and GW170817; however, their maximum masses remain capped below 2.43\,M_ (DD2) and 2.06\,M_ (SLy4). Conversely, the Tsujikawa-inspired model significantly stiffens the effective gravitational coupling, accommodating massive compact objects up to ~ 3.36\,M_ and offering a viable physical origin for the 2.59-0.09+0.08\,M_ secondary object in GW190814, albeit at the expense of overpredicting radii for typical low-mass neutron stars. These contrasting behaviours demonstrate a key phenomenological complementarity between maximum mass and radius bounds within the constant-Q framework, highlighting the utility of multimessenger observations in constraining non-linear non-metricity gravity.
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Bhattacharjee et al. (2026) studied this question.
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