--- created: 2024-05-03T00:13 updated: 2024-05-11T11:38 --- ::: remark The Baily-Borel and toroidal compactifications are defined for quotients of Hermitian symmetric spaces by actions of arithmetic subgroups of their automorphism groups, i.e. those that can be written as $\Gamma\backslash \Omega$. BB compactifications are generally small, e.g. $\dim F_2 = 19$ but $\codim \partial \bbcpt{F_2} = 18$, and this often precludes having a satisfactory modular interpretation of its boundary points. In particular, given an arc in this compactification with endpoint in the boundary, one can not generally construct a birationally unique limit. Toroidal compactifications $\torcpt{\Gamma\backslash \Omega}$ are obtained as certain blowups of $\bbcpt{\Gamma\backslash \Omega}$, and e.g. for $F_2$ some boundary components become divisors (codimension 1). However these are highly non-unique and depend on choices of fans. One might hope there are canonical such choices. The semitoric compactifications of Looijenga interpolate between $\bbcpt{\Gamma\backslash \Omega}$ and $\torcpt{\Gamma\backslash \Omega}$. ::: ## The Baily-Borel compactification ::: definition The group $G$ acts transitively on the set of boundary components $F \subseteq \partial \DD_L \da \tilde\DD_L\setminus \DD_L$, and $\Stab_G(F)\leq G$ is a maximal parabolic subgroup. Taking stabilizers establishes a bijection $$\begin{aligned} \ts{\text{Boundary components $F\subseteq \partial \DD_L$}} &\to \ts{\text{Maximal parabolic subgroups $P\leq G$}} \\ F &\mapsto P\da \Stab_G(F) \end{aligned}$$ For $G \da \SO(V)$, parabolic subgroups $P$ are stabilizers of flags of isotropic subspaces in $V$, and since $\signature(V) = (2, n)$, a flag has length at most 3 and a maximal flag is of the form $p \subseteq I\subseteq J$ where $p$ is a point, $I$ is an isotropic line, and $J$ is an isotropic plane. The only flags that define maximal parabolic subgroups of $\SO(V)$ are of length 1, consisting of either a single line or a single plane. Thus we have bijections $$\begin{aligned} \ts{\text{Rational boundary components of } (\SO_{2, n}(\RR), \SO_2(\RR) \times \SO_n(\RR)) } \\ \reflectbox{\rotatebox[origin=c]{90}{$\mapstofrom$}}\hspace{10em} \\ \ts{\text{Maximal parabolic subgroups of} \SO(V) } \\ \reflectbox{\rotatebox[origin=c]{90}{$\mapstofrom$}}\hspace{10em} \\ \ts{\text{Isotropic lines $I\subset V$ }} \union \ts{\text{Isotropic planes $J \subset V$ }} \end{aligned}$$ where a boundary component $F$ is rational if $\Stab_G(F)$ is defined over $\QQ$. For an arithmetic subgroup $\Gamma \leq G$, letting $\partial(\DD_L)_\QQ$ be the set of all rational boundary components of $\DD_L \subset \tilde \DD_L$, we produce a compactification $${\overline {\Gamma\backslash \DD_L}} = {\Gamma \backslash \DD_L} \Union_{F\in \partial\DD{L, \QQ} } {(G_F(\QQ) \intersect \Gamma) \backslash F}.$$ ::: ::: definition Let $L$ be a lattice of signature $(2, n)$ for $n\geq 1$, let $\Omega_L$ be the associated period domain, let $\Orth^+(L) \leq \Orth(L)$ be the subgroup preserving $\Omega_L$ and let $\tilde \Omega_L$ be the affine cone over $\Omega_L$. Let $n\geq 3$, let $k\in \ZZ$, and let $\Gamma \leq \Orth^+(L)$ be a finite-index subgroup with $\chi: \Gamma\to \CC^*$ a character. A holomorphic functional $f: \Omega_L \to \CC$ is called a **modular form of weight $k$ and character $\chi$ for $\Gamma$** if 1. Factor of automorphy: $f(\lambda z) = \lambda^{-k} f(z)$ for any $\lambda \in \CC^*$. 2. Equivariance: $f(\gamma z) = \chi(\gamma) f(z)$ for all $\gamma\in \Gamma$. ::: ::: definition Let $\Omega_L$ as above and let $M_k(\Gamma, \chi)$ be the $\CC\dash$vector space of such modular forms of weight $k$ for $\Gamma$ with character $\chi$. The **Baily-Borel compactification** can be defined as $$\bbcpt{\Gamma\backslash \Omega_L} \da \Proj \bigoplus_{k\geq 1} M_k(\Gamma, \chi_{\mathrm{triv}})$$ where $\chi_{\mathrm{triv}}$ is the trivial character. ::: ::: remark $\partial \bbcpt{\Gamma\backslash \Omega_L}$ decomposes into points $p_i$ and curves $C_j$, which are in bijection with $\Gamma\dash$orbits of isotropic lines $i$ and isotropic planes $j$ in $L_\QQ$. Moreover $p_i \in \overline{C_j} \iff$ one can choose representatives lines $i$ and planes $j$ such that $i \subseteq j$. ::: ::: remark A theorem of Baily-Borel gives the existence of an ample automorphic line bundle $\mcl$ on $\overline{\DD_L}$ giving it the structure of a normal projective variety isomorphic to a canonical model $\Proj \bigoplus_{k\geq 0} H^0(L^k)??$. We denote this compactification $\bbcpt{\Gamma\backslash \DD_L}$. ::: ## Toroidal and semitoroidal compactifications ::: remark A **toroidal compactification** $\torcpt{\Gamma \backslash \DD_L}$ is a certain blowup of $\bbcpt{\Gamma \backslash \DD_L}$, so there is a birational map $\torcpt{\Gamma \backslash \DD_L} \rational \bbcpt{\Gamma \backslash \DD_L}$. It is defined by a collection of admissible fans $\ts{F_i}_{i\in I}$ where $I$ ranges over an index set for all cusps. A **semitoroidal compactification** is a generalization due to Looijenga for which the cones of $F_i$ are not required to be finitely generated, and [@AE21] shows that semitoroidal compactifications are characterized as exactly the normal compactifications $\semitorcpt{M}$ fitting into a tower \begin{tikzcd} {\torcpt{M}} \\ \\ {\semitorcpt{M} } \\ \\ {\bbcpt{M} } \arrow[hook, from=5-1, to=3-1] \arrow[hook, from=3-1, to=1-1] \end{tikzcd} where $\torcpt{M}$ is some toroidal compactification of $M$. ::: ::: remark On the toroidal compactification associated with $\Gamma\backslash \Omega_L$: for a cusp $C_i$ of the BB compactification, let $F\subset L_\QQ$ be the corresponding $\Gamma\dash$orbit of an isotropic line or plane. Consider its stabilizer $S(F) \da \Stab_{\Orth^+(L_\RR)}$, and its unipotent radical $U(F)$. Then $U(F)$ is a vector space containing a lattice $U(F) \intersect \Gamma$ and an open convex cone $C(F)$. Let $\rc{C(F)}$ be the rational closure of the cone, so the union of $C(F)$ and rational rays in its closure. We then choose a fan $\Sigma(F)$ with $\supp(\Sigma(F)) = \rc{C(F)}$ which is invariant under $\Stab_{\Orth^+(L_\RR)}(F) \intersect \Gamma$ and produce an associated toric variety $X_{\Sigma(F)}$. If one does this for every $F$ to produce a $\Gamma\dash$admissible collection of polyhedra $\Sigma$, their quotients by $\Gamma$ glue to give a toroidal compactification $\torcpt{\Gamma\backslash \Omega_L}$, which has the structure of a (complex) algebraic space. There is a surjection $\torcpt{\Gamma\backslash \Omega_L} \surjects \bbcpt{\Gamma\backslash \Omega_L}$. Why $e^\perp/e$ shows up: if $e$ is an isotropic line in $L$ corresponding to a cusp $F$, there is an isomorphism of lattices $U(F) \intersect \tilde \Orth^+(L) \cong e^\perp/e$ where $\tilde \Orth^+ \da \ker\qty{\Orth^+(L) \to \Orth(\discgroup L)}$. ::: ## Misc ::: definition A **log Calabi-Yau (CY) pair** is a pair $(X, D)$ with $X$ a proper variety and $D$ an effective $\QQ\dash$Cartier divisor such that the pair is log canonical and $K_X + D \sim_\QQ 0$. A degeneration $\pi: \mcx \to \Delta$ is a CY degeneration if $\pi$ is proper, $K_{\mcx}\sim_\QQ 0$, and $(\mcx, \mcx_0)$ is dlt. This implies that $\mcx_t$ is a Calabi-Yau variety for $t\neq 0$ and $\mcx_0$ is a union of log CY pairs $(V_i, D_i)$. If $\mcx_t$ is a strict CY of dimension $n$, so $\pi_1 \mcx_t = 0$ and $h^i(\mcx_t, \OO_{\mcx_t}) = 0$ for $1 \leq i \leq n-1$, and $\dim \Gamma(\mcx_0) = n$, we say $\mcx$ is a large complex structure limit or equivalently a maximal unipotent or MUM degeneration. If $n = 2$, Kulikov shows that $\Gamma(\mcx_0)$ is always isomorphic to a 2-sphere $S^2$. Whether $\Gamma(\mcx_0) \cong S^n$ or a quotient thereof for $n\geq 3$ more generally is an open question, posed by Kontsevich-Soibelman. It has recently been shown by Kollár-Xu that in the case of degenerations of Calabi-Yau or hyperkähler manifolds, the dual complex is always a rational homology sphere. ::: ::: remark Why this is useful to us: one formulation of mirror symmetry is the formulation due to Strominger-Yau-Zaslow, aptly called SYZ mirror symmetry. Conjecturally, the general fiber $\mcx_t$ of a punctured family of CYs $\mcx^\circ \to \Delta^\circ$ can be given the structure of a special Lagrangian torus fibration $\mcx_t \to B$, one can \"dualize\" the fibration to obtain a mirror CY $\hat{\mcx_t} \to B$ over the same base. The common base $B$ of these two fibrations is conjecturally of the form $\Gamma(\mcx_0)$, the dual complex of a degeneration $\mcx\to \Delta$ extending $\mcx^\circ$. ::: ## Baily-Borel cusps and incidence diagrams ## Other compactifications ::: remark Write $F_{2d} \da \Gamma_{2d}\backslash D_{2d}$. A cusp $p_i$ of $\bbcpt{F_{2d}}$ determines a cone $C_i$. Toroidal and semitoroidal compactifications are then determined by a collection of $\Gamma_{2d}\dash$invariant fans supported on $C_i$ for $i$ ranging over an index set for all cusps. If $d=1$ (or more generally if $2d$ is squarefree), there is a single 0-cusp $p_{2d}$ whose cone $C_{2d}$ has a description as the positive light cone in the rational closure of $C_{2d}$ with respect to a certain lattice $M_{2d}$. This can be written $C^{\mathrm rc }_{2d} \da \mathrm{Conv}(\overline{C}_{2d} \intersect M_{2d}\tensor_\ZZ \RR)$. A semitoroidal compactification of $F_{2d}$ is then determined by a semitoric fan in $M_{2d, \RR}$ supported on $C_{2d}^{\mathrm rc}$ which is invariant for a particular subgroup $\Gamma^+_{2d} \leq \Orth(M_{2d})$. In this case, one can make a canonical choice for such a semitoric fan: the Coxeter fan $\Sigma_{2d}^{\mathrm{Cox} }$ whose cones are precisely the fundamental domains for a Weyl group action on $C_{2d}^{\mathrm rc}$, see AET19. :::