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Ludvig Svensson

Publications and source records attributed to Ludvig Svensson.

4 recordsLinked to original sources

Gibbs polystability of Fano manifolds, stability thresholds and symmetry breaking

We extend the probabilistic approach for constructing Kähler--Einstein metrics on log Fano manifolds $(X,Δ)$ - involving random point processes - to the case of non-discrete automorphism groups, by breaking the symmetry using a moment map constraint. In particular, an algebraic notion of Gibbs polystability is introduced, ensuring that the corresponding point processes on $X$ are well-defined. We conjecture that the Gibbs polystability of $(X,Δ)$ is equivalent to the existence of a Kähler--Einstein metric and that the unique such metric with vanishing moment emerges when sampling a large number of $N$ points on $X$. The definition of Gibbs polystability is formulated in terms of a new algebro-geometric invariant, defined as a limit of certain log canonical thresholds on the GIT semistable locus of the $N$-fold products $X^N$. We conjecture that it coincides with a previously studied analytic polystability threshold, encoding the coercivity of the K-energy functional modulo automorphisms. These conjectures follow from an overarching conjectural Large Deviation Principle for the large $N$-limit. The conjectured equivalence between Gibbs polystability and K-polystability is established when $(X,Δ)$ is a log Fano curve. For Fano manifolds of any dimension, we establish an effective one-sided version of the conjecture, which yields an effective criterion for the existence of a Kähler--Einstein metric and, more generally, an effective algebraic lower bound on the analytic polystability threshold. In companion papers, applications will be given to optimal stability results for the logarithmic HLS inequality on the two-sphere, to Onsager's point vortex model on the two-sphere, and to the AdS/CFT correspondence.

math.DG

Critical temperatures and collapsing of two-dimensional Log gases

We consider the canonical ensemble of a system of point particles on the sphere interacting via a logarithmic pair potential. In this setting, we study the associated Gibbs measure and partition function, and we derive explicit formulas relating the critical temperature, at which the partition function diverges, to a certain discrete optimization problem. We further show that the asymptotic behavior of both the partition function and the Gibbs measure near the critical temperature is governed by the same optimization problem. Our approach relies on the Fulton--MacPherson compactification of configuration spaces and analytic continuation of complex powers. To illustrate the results, we apply them to well-studied systems, including the two-component plasma and the Onsager model of turbulence. In particular, for the two-component plasma with general charges, we describe the formation of dipoles close to the critical temperature, which we determine explicitly.

math-ph

A Calculus for Finite Parts and Residues of some Divergent Complex Geometric Integrals

We consider divergent integrals $\int_X ω$ of certain forms $ω$ on a reduced pure-dimensional complex space $X$. The forms $ω$ are singular along a subvariety defined by the zero set of a holomorphic section $s$ of some holomorphic vector bundle $E$. Equipping $E$ with a smooth Hermitian metric allows us to define a finite part $\mathrm{fp}\,\int_X ω$ of the divergent integral as the action of a certain current extension of $ω$. We introduce a current calculus to compute finite parts for a special class of $ω$. Our main result is a formula that decomposes the finite part of such an $ω$ into sums of products of explicit currents. Lastly, we show that, in principle, it is possible to reduce the computation of $\mathrm{fp}\,\int_X ω$ for a general $ω$ to this class.

math.CV

On Finite Parts of Divergent Complex Geometric Integrals and Their Dependence on a Choice of Hermitian Metric

Let $X$ be a reduced complex space of pure dimension. We consider divergent integrals of certain forms on $X$ that are singular along a subvariety defined by the zero set of a holomorphic section of some holomorphic vector bundle $E \rightarrow X$. Given a choice of Hermitian metric on $E$ we define a finite part of the divergent integral. Our main result is an explicit formula for the dependence on the choice of metric of the finite part.

math.CV