Generically log smooth families via generators and relations
Simon Felten
TL;DR
This work develops an algorithmic toolkit for studying generically log smooth degenerations of affine and projective families by encoding the total space with a generators-and-relations presentation and leveraging log geometry. It introduces an explicit, computable GLS criterion (including dkink and Ext^1-based obstructions) that certifies when a flat family is generically log smooth, and it generalizes the framework to toroidal crossing schemes with a refined classifying map via $\eta_V^{(\ell)}$. Central results include a differential-log-smoothness perspective, finite determinacy of log structures on the central fiber, and a tight correspondence between GLS data and toroidal crossing structures, enabling practical computations (and a Macaulay2 implementation). The theory yields both affine and projective variants, provides practical checks using infinitesimal thickenings, and establishes how log structures on the central fiber can be compared or identified across families through kink data. Collectively, these contributions offer a robust, implementable approach for analyzing log singularities and smoothing degenerations in explicit examples, with potential impact on log Gromov–Witten theory and mirror symmetry constructions.
Abstract
Let $f\colon X \to \mathbb{A}^1_t$ be an affine flat morphism of finite type, and let $V = f^{-1}(0)$. Then, we obtain a morphism of log schemes $f\colon (X|V) \to (\mathbb{A}^1_t|0)$. In this article, we develop algorithmic tools to study the log-geometric properties of $f$ by means of a presentation \[Γ(X,\mathcal{O}_X) = \Bbbk[t,x_1,\ldots,x_n]/(f_1,\ldots,f_r).\] We obtain similar tools for projective flat morphisms when the homogeneous coordinate ring is given by generators and relations. We provide an implementation of our algorithms in Macaulay2. In a slightly different direction, we give some results on the sheaf $\mathcal{LS}_V$ of log smooth structures on a toroidal crossing scheme $(V,\mathcal{P},\barρ)$.
