ScalingStacks

8. Log structures [0304]

Original official author HTML, exact retained edition. Historical TeX conversion verdicts remain unchanged. Cited-edition alignment and mathematical self-containment are not assessed.

Complete original source context · Original author HTML

8. Log structures

We review the notion of log structures of Fontaine-Illusie and Kato ([44], [49]). These play a key role in trying to understand mirror symmetry via degenerations.

Definition 8.1.

A log structure on a scheme (or analytic space) XX is a (unital) homomorphism

αX:ℳX→𝒪X\alpha_{X}:\mathcal{M}_{X}\rightarrow\mathcal{O}_{X}

of sheaves of (multiplicative and commutative) monoids inducing an isomorphism αX−1​(𝒪X×)→𝒪X×\alpha_{X}^{-1}(\mathcal{O}_{X}^{\times})\rightarrow\mathcal{O}_{X}^{\times}. The monoid structure on 𝒪X\mathcal{O}_{X} is given by multiplication. The triple (X,ℳX,αX)(X,\mathcal{M}_{X},\alpha_{X}) is then called a log space. We often write the whole package as X†X^{\dagger}.

A morphism of log spaces F:X†→Y†F:X^{\dagger}\rightarrow Y^{\dagger} consists of a morphism F¯:X→Y\underline{F}:X\rightarrow Y of underlying spaces together with a homomorphism F#:F¯−1​(ℳY)→ℳXF^{\#}:\underline{F}^{-1}(\mathcal{M}_{Y})\rightarrow\mathcal{M}_{X} commuting with the structure homomorphisms:

αX∘F#=F¯∗∘αY.\alpha_{X}\circ F^{\#}=\underline{F}^{*}\circ\alpha_{Y}.

The key examples:

Examples 8.2.

(1) Let XX be a scheme and Y⊆XY\subseteq X a closed subset of codimension one. Denote by j:X∖Y→Xj:X\setminus Y\rightarrow X the inclusion. Then the inclusion

αX:ℳX=j∗​(𝒪X∖Y×)∩𝒪X→𝒪X\alpha_{X}:\mathcal{M}_{X}=j_{*}(\mathcal{O}_{X\setminus Y}^{\times})\cap\mathcal{O}_{X}\rightarrow\mathcal{O}_{X}

of the sheaf of regular functions invertible off of YY is a log structure on XX. This is called a divisorial log structure on XX.

(2) A prelog structure, i.e., an arbitrary homomorphism of sheaves of monoids φ:𝒫→𝒪X\varphi:\mathcal{P}\rightarrow\mathcal{O}_{X}, defines an associated log structure ℳX\mathcal{M}_{X} by

ℳX=(𝒫⊕𝒪X×)/{(p,φ​(p)−1)|p∈φ−1​(𝒪X×)}\mathcal{M}_{X}=(\mathcal{P}\oplus\mathcal{O}_{X}^{\times})/\{(p,\varphi(p)^{-1})\,|\,p\in\varphi^{-1}(\mathcal{O}_{X}^{\times})\}

and αX​(p,h)=h⋅φ⁡(p)\alpha_{X}(p,h)=h\cdot\varphi(p).

(3) If f:X→Yf:X\rightarrow Y is a morphism of schemes and αY:ℳY→𝒪Y\alpha_{Y}:\mathcal{M}_{Y}\rightarrow\mathcal{O}_{Y} is a log structure on YY, then the prelog structure f−1​(ℳY)→𝒪Xf^{-1}(\mathcal{M}_{Y})\rightarrow\mathcal{O}_{X} given as the composition of αY:f−1​(ℳY)→f−1​𝒪Y\alpha_{Y}:f^{-1}(\mathcal{M}_{Y})\rightarrow f^{-1}\mathcal{O}_{Y} and f∗:f−1​𝒪Y→𝒪Xf^{*}:f^{-1}\mathcal{O}_{Y}\rightarrow\mathcal{O}_{X} defines an associated log structure on XX, the pull-back log structure.

(4) In (1) we can pull back the log structure on XX to YY using (3). Thus in particular, if 𝒳→D\mathcal{X}\rightarrow D is a toric degeneration, the inclusion 𝒳0⊆𝒳\mathcal{X}_{0}\subseteq\mathcal{X} gives a log structure on 𝒳\mathcal{X} and an induced log structure on 𝒳0\mathcal{X}_{0}. Similarly the inclusion 0∈D0\in D gives a log structure on DD and an induced one on 00. Here ℳ0=ℂ×⊕ℕ\mathcal{M}_{0}=\mathbb{C}^{\times}\oplus\mathbb{N}, where ℕ\mathbb{N} is the (additive) monoid of natural (non-negative) numbers, and

α0​(h,n)={hn=00n≠0.\alpha_{0}(h,n)=\begin{cases}h&n=0\\ 0&n\not=0.\end{cases}

0†0^{\dagger} is usually called the standard log point.

We then have log morphisms 𝒳†→D†\mathcal{X}^{\dagger}\rightarrow D^{\dagger} and 𝒳0†→0†\mathcal{X}_{0}^{\dagger}\rightarrow 0^{\dagger}.

(5) If σ⊆Mℝ=ℝn\sigma\subseteq M_{\mathbb{R}}=\mathbb{R}^{n} is a strictly convex rational polyhedral cone, σ∨⊆Nℝ{\sigma}^{\scriptscriptstyle\vee}\subseteq N_{\mathbb{R}} the dual cone, let P=σ∨∩NP={\sigma}^{\scriptscriptstyle\vee}\cap N: this is a monoid under addition. The affine toric variety defined by σ\sigma can be written as X=Spec⁡ℂ⁡[P]X=\operatorname{Spec}\mathbb{C}[P]. We then have a pre-log structure induced by the homomorphism of monoids

P→ℂ⁡[P]P\rightarrow\mathbb{C}[P]

given by p↦zpp\mapsto z^{p}. There is then an associated log structure on XX. This is in fact the same as the log structure induced by ∂X⊆X\partial X\subseteq X, where ∂X\partial X is the toric boundary of XX, i.e., the union of toric divisors of XX.

If p∈Pp\in P, then the monomial zpz^{p} defines a map f:X→Spec⁡ℂ⁡[ℕ]=𝔸1f:X\rightarrow\operatorname{Spec}\mathbb{C}[\mathbb{N}]=\mathbb{A}^{1} which is a log morphism with the log structure on Spec⁡ℂ⁡[ℕ]\operatorname{Spec}\mathbb{C}[\mathbb{N}] induced similarly by ℕ→ℂ⁡[ℕ]\mathbb{N}\rightarrow\mathbb{C}[\mathbb{N}]. The fibre X0=Spec⁡ℂ⁡[P]/(zp)X_{0}=\operatorname{Spec}\mathbb{C}[P]/(z^{p}) is a subscheme of XX, there is an induced log structure on X0X_{0}, and a map X0†→0†X_{0}^{\dagger}\rightarrow 0^{\dagger} as in (4). The log morphism ff is an example of a log smooth morphism. Essentially all log smooth morphisms are étale locally of this form (if ℕ\mathbb{N} is replaced by a more general monoid). See [48] for details.

Condition (4) of Definition 7.1 in fact implies that locally, away from ZZ, 𝒳†\mathcal{X}^{\dagger} and 𝒳0†\mathcal{X}_{0}^{\dagger} are of the above form. So we should view 𝒳†→D†\mathcal{X}^{\dagger}\rightarrow D^{\dagger} as log smooth away from ZZ, and from the log point of view, 𝒳0†\mathcal{X}_{0}^{\dagger} can be treated much like a non-singular scheme away from ZZ.

(6) Given a monoid PP as in (5) and a morphism X→Spec⁡ℂ⁡[P]X\rightarrow\operatorname{Spec}\mathbb{C}[P], we can pull back the log structure defined above on Spec⁡ℂ⁡[P]\operatorname{Spec}\mathbb{C}[P] to XX. If X†X^{\dagger} is a log scheme which étale locally can be described in this way, we say X†X^{\dagger} is a fine saturated log scheme. The adjective “fine” tells us it is locally described via maps to schemes of the form Spec⁡ℂ⁡[P]\operatorname{Spec}\mathbb{C}[P] where PP is a finitely generated integral monoid, i.e., the canonical homomorphism P→PgpP\rightarrow P^{{\operatorname{gp}}} is an injection. The adjective “saturated” tells us the monoid PP is saturated. This means that PP is integral and whenever p∈Pgpp\in P^{{\operatorname{gp}}} satisfies m​p∈Pmp\in P for some m>0m>0, p∈Pp\in P. Such monoids arise, e.g., as the intersection of a rational polyhedral cone with a lattice.

Most of the literature on log geometry tends to apply only to fine log structures. In the key example of 𝒳0†→0†\mathcal{X}_{0}^{\dagger}\rightarrow 0^{\dagger}, the log structure is fine saturated away from the set ZZ. However, it is not in general fine along ZZ, and this tends to cause many technical problems as new techniques have to be developed to deal properly with the log structure along ZZ. ∎

On a log scheme X†X^{\dagger} there is always an exact sequence

1⟶𝒪X×⟶α−1ℳX⟶ℳ¯X⟶0,1\smash{\mathop{\longrightarrow}\limits}\mathcal{O}_{X}^{\times}\smash{\mathop{\longrightarrow}\limits^{\alpha^{-1}}}\mathcal{M}_{X}\smash{\mathop{\longrightarrow}\limits}\overline{\mathcal{M}}_{X}\smash{\mathop{\longrightarrow}\limits}0,

where we write the quotient sheaf of monoids ℳ¯X\overline{\mathcal{M}}_{X} additively. We call ℳ¯X\overline{\mathcal{M}}_{X} the ghost sheaf of the log structure. I like to view ℳ¯X\overline{\mathcal{M}}_{X} as specifying the combinatorial information associated to the log structure. For example, if X†X^{\dagger} is induced by the Cartier divisor Y⊆XY\subseteq X with XX normal, then the stalk ℳ¯X,x\overline{\mathcal{M}}_{X,x} at x∈Xx\in X is the monoid of effective Cartier divisors on a neighbourhood of xx supported on YY.

It is useful for understanding pull-backs of log structures to note that if f:Y→Xf:Y\rightarrow X is a morphism with XX carrying a log structure, and YY is given the pull-back log structure, then ℳ¯Y=f−1​ℳ¯X\overline{\mathcal{M}}_{Y}=f^{-1}\overline{\mathcal{M}}_{X}. In the case that ℳX\mathcal{M}_{X} is induced by an inclusion of Y⊆XY\subseteq X, ℳ¯X\overline{\mathcal{M}}_{X} is supported on YY, so we can equate ℳ¯X\overline{\mathcal{M}}_{X} and ℳ¯Y\overline{\mathcal{M}}_{Y}, the ghost sheaves for the divisorial log structure on XX and its restriction to YY.

Exercise 8.3.

Show that in Example 8.2, (5), ℳ¯X,x=P\overline{\mathcal{M}}_{X,x}=P if dimσ=dimMℝ\dim\sigma=\dim M_{\mathbb{R}} and xx is the unique zero-dimensional torus orbit of XX. More generally,

ℳ¯X,x=τ∨∩Nτ⟂∩N=Homm​o​n​o​i​d⁡(τ∩M,ℕ),\overline{\mathcal{M}}_{X,x}={{\tau}^{\scriptscriptstyle\vee}\cap N\over\tau^{\perp}\cap N}=\operatorname{Hom}_{monoid}(\tau\cap M,\mathbb{N}),

when x∈Xx\in X is in the torus orbit corresponding to a face τ\tau of σ\sigma. In particular, τ\tau can be recovered as Homm​o​n​o​i​d⁡(ℳ¯X,x,ℝ≥0)\operatorname{Hom}_{monoid}(\overline{\mathcal{M}}_{X,x},\mathbb{R}_{\geq 0}), where ℝ≥0\mathbb{R}_{\geq 0} is the additive monoid of non-negative real numbers. ∎

In the sections which follow, the key logarithmic spaces we consider will be those arising from toric degenerations 𝒳→D\mathcal{X}\rightarrow D. As above, the central fibre 𝒳0⊆𝒳\mathcal{X}_{0}\subseteq\mathcal{X} induces a divisorial log structure on 𝒳\mathcal{X}, and restricting gives a log scheme 𝒳0†\mathcal{X}_{0}^{\dagger} along with a morphism 𝒳0†→0†\mathcal{X}_{0}^{\dagger}\rightarrow 0^{\dagger} which is log smooth off of the bad set Z⊆𝒳0Z\subseteq\mathcal{X}_{0}.

We can now elaborate on the philosophy we wish to take with the following diagram:

-model A log geometry-model B

There are two sides to mirror symmetry. The AA-model side involves counting curves: we wish to count curves in the general fibre of a toric degeneration 𝒳→D\mathcal{X}\rightarrow D. There are good reasons to believe that this count can in fact be performed on 𝒳0†\mathcal{X}_{0}^{\dagger}, using a theory of logarithmic Gromov-Witten invariants: see §9. The hope is that 𝒳0\mathcal{X}_{0} is a sufficiently combinatorial object so that such a count can be carried out in a combinatorial manner.

The BB-side involves deformations of complex structure. The idea is that to understand deformations of complex structure, we should start with the central fibre 𝒳0†\mathcal{X}_{0}^{\dagger} and try to construct smoothings, i.e., construct a toric degeneration with this central fibre. The log structure is necessary to find a unique smoothing. If this smoothing can be described sufficiently explicitly, then again one should be able to extract the necessary periods for the BB-model calculations purely in terms of combinatorics.

So log geometry will play an important role on both sides of mirror symmetry, but as the above suggests, there should be some combinatorial objects underlying both calculations.

In fact, log geometry is closely related to tropical geometry. We will explore in the following sections how tropical geometry controls both the AA- and BB-model sides of the above picture, completing the above diagram:

-model A -model B log geometry

Original mathematics by the credited authors. Source-backed reader collection; mathematical self-containment is not assessed.