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Compactifications of moduli of del Pezzo surfaces via line arrangement and K-stability

Junyan Zhao 851 S Morgan St, 60607, Chicago, Illinois, USA jzhao81@uic.edu
Abstract.

In this paper, we study compactifications of the moduli of smooth del Pezzo surfaces using K-stability and the line arrangement. We construct K-moduli of log del Pezzo pairs with sum of lines as boundary divisors, and prove that for d=2,3,4d=2,3,4, these K-moduli of pairs are isomorphic to the K-moduli spaces of del Pezzo surfaces. For d=1d=1, we prove that they are different by exhibiting some walls.

1. Introduction

The moduli spaces of del Pezzo surfaces have been extensively studied thanks to the development of different approaches to construct moduli spaces.

A weighted marked del Pezzo surface is a pair (S,B)(S,B) with SS a del Pezzo surface and B=biBiB=\sum b_{i}B_{i} a boundary divisor, where bi[0,1]b_{i}\in[0,1] and BiB_{i}’s are all the finitely many lines on SS. The KSBA moduli spaces parameterizes all such pairs such that (S,B)(S,B) is semi log canonical (slc) and KS+BK_{S}+B is ample. For example, when bi=1b_{i}=1 for each ii, the moduli of such quartic del Pezzo pairs is isomorphic to the moduli M¯0,5\overline{M}_{0,5} of rational curves with 5 marked points (cf. [HKT09, HKT13]). Another interesting case is when bi=bb_{i}=b, where bb is a positive number such that (S,B)(S,B) is close to a Calabi-Yau pair (cf. [HKT09, HKT13, GKS21]).

The development of K-stability provides a moduli theory for log Fano pairs, called K-moduli spaces. The general K-moduli theory was established by a group of people in the past decade (cf. [ABHLX20, BHLLX21, BLX22, BX19, CP21, LWX21, LXZ22, XZ20]). Roughly speaking, for fixed numerical invariants, we have a projective scheme parameterizing the K-polystable log Fano pairs with these invariants. Moreover, in the surface case, there is a wall crossing structure when we vary the coefficients of the boundary divisors (cf. [ADL19, ADL21]). See Section 2 for definitions and more details. We can ask the similar questions in the K-moduli spaces setting:

Question.

Fix a degree d{1,2,3,4}d\in\{1,2,3,4\} and a rational number 0c<10\leq c<1.

  1. (1)

    Can we describe the K-moduli space M¯d,cK\overline{M}^{K}_{d,c} of K-polystable log Fano pairs (X,cD)(X,cD) admitting a \mathbb{Q}-Gorenstein smoothing to a pair (X0,cD0)(X_{0},cD_{0}), where X0X_{0} a smooth del Pezzo surface of anticanonical degree dd and D0=LiD_{0}=\sum L_{i} is the sum of lines (i.e. KX0-K_{X_{0}}-degree 11 rational curves)?

  2. (2)

    When varying cc in the range such that (X0,cD0)(X_{0},cD_{0}) is log Fano, do the K-moduli spaces of pairs in (1) change? If yes, can we determine all the values cic_{i}’s at which the moduli spaces get changed?

In particular, when c=0c=0, the K-moduli space parameterizes all the del Pezzo surfaces of a fixed degree, which admit a Kähler-Einstein metric (cf. [OSS16, MM93]).

For c>0c>0, if a pair (X,cD)(X,cD) is a K-polystable degeneration of pairs (X0,cLi)(X_{0},c\sum L_{i}), then DD is unique by the separatedness of the K-moduli spaces. In particular, when X0X_{0} has du Val singularities, the boundary divisor DD can be also written as the sum Li\sum L_{i}^{\prime} of lines, where LiL_{i}^{\prime}’s do not have to be distinct.

We prove in this article that for d=2,3,4d=2,3,4, there are no walls for the K-moduli spaces M¯d,cK\overline{M}^{K}_{d,c}, and they are all isomorphic to K-moduli of del Pezzo surfaces. For d=1d=1, we exhibit examples to see that there is indeed some walls.

Theorem 1.1.

(Corollary 3.8, Proposition 3.10, Theorem 4.12) For any fixed degree d{2,3,4}d\in\{2,3,4\}, there are no walls for the K-moduli M¯d,cK\overline{M}^{K}_{d,c} when cc varies from 0 to the log Calabi-Yau threshold, and they are isomorphic to the K-moduli space of del Pezzo surfaces of degree dd.

Theorem 1.2.

(Proposition 5.2) Let 0<c<12400<c<\frac{1}{240} be a number, and M¯1,cK\overline{M}^{K}_{1,c} be the K-moduli space defined above. Then there is a wall c=c<1288c=c^{\prime}<\frac{1}{288}, which is given by the destabilization of the surface pair, where the surface acquires an A7A_{7}-singularity.

Acknowledgements This problem was motivated when talking with Schock Nolan. I would also like to express my gratitude to Yuchen Liu for sharing some primary ideas. The author also want to thank Izzet Coskun and Schock Nolan for many stimulating discussions.

2. Preliminaries

Convention.

In this paper, we work over the field of complex numbers \mathbb{C}. By a surface, we mean a complex connected projective algebraic surface. We keep the notions on singularities of surface pairs the same as [KM98, Chapter 2 and Chapter 4]

For the reader’s convenience, we state the definitions and results in simple versions, especially in dimension 2. Most of them can be generalized to higher dimension.

Definition 2.1.

Let XX be a normal projective variety, and DD be an effective \mathbb{Q}-divisor. Then (X,D)(X,D) is called a log Fano pair if KX+DK_{X}+D is \mathbb{Q}-Cartier and (KX+D)-(K_{X}+D) is ample. A normal projective variety XX is called a \mathbb{Q}-Fano variety if (X,0)(X,0) is a klt log Fano pair.

Definition 2.2.

Let (X,D)(X,D) be an n-dimensional log Fano pair, and EE a prime divisor on a normal projective variety YY, where π:YX\pi:Y\rightarrow X is a birational morphism. Then the log discrepancy of (X,E)(X,E) with respect to EE is

A(X,D)(E):=1+coeffE(KYπ(KX+D)).A_{(X,D)}(E):=1+\operatorname{coeff}_{E}(K_{Y}-\pi^{*}(K_{X}+D)).

We define the S-invariant of (X,D)(X,D) with respect to EE to be

S(X,D)(E):=1(KXD)n0volY(π(KXD)tE)𝑑t,S_{(X,D)}(E):=\frac{1}{(-K_{X}-D)^{n}}\int_{0}^{\infty}\operatorname{vol}_{Y}(\pi^{*}(-K_{X}-D)-tE)dt,

and the β\beta-invariant of (X,D)(X,D) with respect to EE to be

β(X,D)(E):=A(X,D)(E)S(X,D)(E)\beta_{(X,D)}(E):=A_{(X,D)}(E)-S_{(X,D)}(E)

The first definition of K-(poly/semi)stability of log Fano pairs used test configurations. We refer the reader to [ADL19, Xu21]. There is an equivalent definition using valuations, which is called valuative criterion for K-stability. The advantage of this definition is that it is easier to check.

Theorem 2.3.

(cf. [Fuj19, Li17, BX19]) A log Fano pair (X,D)(X,D) is

  1. (1)

    K-semistable if and only if β(X,D)(E)0\beta_{(X,D)}(E)\geq 0 for any prime divisor EE over XX;

  2. (2)

    K-stable if and only if β(X,D)(E)>0\beta_{(X,D)}(E)>0 for any prime divisor EE over XX.

The following powerful result is called interpolation of K-stability. We only state a version that we will use later. For a more general statement, see for example [ADL19, Proposition 2.13] or [Der16, Lemma 2.6].

Theorem 2.4.

Let XX be a K-semistable \mathbb{Q}-Fano variety, and DrKXD\sim_{\mathbb{Q}}-rK_{X} be an effective divisor.

  1. (1)

    If (X,1rD)(X,\frac{1}{r}D) is klt, then (X,cD)(X,cD) is K-stable for any c(0,1r)c\in(0,\frac{1}{r});

  2. (2)

    If (X,1rD)(X,\frac{1}{r}D) is log canonical, then (X,cD)(X,cD) is K-semistable for any c(0,1r)c\in(0,\frac{1}{r}).

Theorem 2.5.

Let (X,D)(X,D) be a klt log Fano pair which isotrivially degenerates to a K-semistable log Fano pair (X0,D0)(X_{0},D_{0}). Then (X,D)(X,D) is also K-semistable.

This follows immediately from the openness of K-(semi)stability (cf. [BLX22, Xu20]), which is useful in our analysis of K-moduli spaces.

Recall that the volume of a divisor DD on an nn-dimensional normal projective variety YY is

volY(D):=limmdimH0(Y,mD)mn/n!.\operatorname{vol}_{Y}(D):=\lim_{m\to\infty}\frac{\dim H^{0}(Y,mD)}{m^{n}/n!}.

The divisor DD is big by definition if and only if volY(D)>0\operatorname{vol}_{Y}(D)>0.

Definition 2.6.

Let x(X,D)x\in(X,D) be an n-dimensional klt singularity. Let π:YX\pi:Y\rightarrow X be a birational morphism such that EYE\subseteq Y is an exceptional divisor whose center on XX is {x}\{x\}. Then the volume of (xX)(x\in X) with respect to EE is

volx,X,D(E):=limmdim𝒪X,x/{f𝒪X,x:ordE(f)m}mn/n!,\operatorname{vol}_{x,X,D}(E):=\lim_{m\to\infty}\frac{\dim\mathcal{O}_{X,x}/\{f\in\mathcal{O}_{X,x}:\operatorname{ord}_{E}(f)\geq m\}}{m^{n}/n!},

and the normalized volume of (xX)(x\in X) with respect to EE is

vol^x,X,D(E):=A(X,D)(D)volx,X,D(E).\widehat{\operatorname{vol}}_{x,X,D}(E):=A_{(X,D)}(D)\cdot\operatorname{vol}_{x,X,D}(E).

We define the local volume of x(X,D)x\in(X,D) to be

vol^(x,X,D):=infEvol^x,X,D(E),\widehat{\operatorname{vol}}(x,X,D):=\inf_{E}\widehat{\operatorname{vol}}_{x,X,D}(E),

where EE runs through all the prime divisor over XX whose center on XX is {x}\{x\}.

Theorem 2.7.

(cf. [Fuj18, LL19, Liu18]) Let (X,D)(X,D) be an n-dimensional K-semistable log Fano pair. Then for any xXx\in X, we have

(KXD)n(1+1n)nvol^(x,X,D).(-K_{X}-D)^{n}\leq\left(1+\frac{1}{n}\right)^{n}\widehat{\operatorname{vol}}(x,X,D).

Now let us briefly review some results on the K-moduli spaces of log Fano pairs. We mainly state the results in our setting. For more general statements, see [ADL19, Theorem 3.1, Remark 3.25] or [ADL21, Theorem 2.21].

Definition 2.8.

Let f:(𝒳,𝒟)Bf:(\mathcal{X},\mathcal{D})\rightarrow B be a proper flat morphism to a reduced scheme with normal, geometrically connected fibers of pure dimension nn, where 𝒟\mathcal{D} is an effective relative Mumford \mathbb{Q}-divisor (cf. [Kol19, Definition 1]) on 𝒳\mathcal{X} which does not contain any fiber of ff. Then ff is called a \mathbb{Q}-Gorenstein flat family of log Fano pairs if (K𝒳/B+𝒟)-(K_{\mathcal{X}/B}+\mathcal{D}) is \mathbb{Q}-Cartier and ample over BB.

Definition 2.9.

Let 0<c<1/r0<c<1/r be a rational number and (X,cD)(X,cD) be a log Fano pair such that DrKXD\sim-rK_{X}. A \mathbb{Q}-Gorenstein flat family of log Fano pairs f:(𝒳,c𝒟)Cf:(\mathcal{X},c\mathcal{D})\rightarrow C over a pointed smooth curve (0C)(0\in C) is called a \mathbb{Q}-Gorenstein smoothing of (X,D)(X,D) if

  1. (1)

    the divisors 𝒟\mathcal{D} and K𝒳/CK_{\mathcal{X}/C} are both \mathbb{Q}-Cartier, ff-ample, and 𝒟,frK𝒳/\mathcal{D}\sim_{\mathbb{Q},f}-rK_{\mathcal{\mathcal{X}/B}};

  2. (2)

    both ff and f|𝒟f|_{\mathcal{D}} are smooth over C{0}C\setminus\{0\}, and

  3. (3)

    (𝒳0,c𝒟0)(X,cD)(\mathcal{X}_{0},c\mathcal{D}_{0})\simeq(X,cD).

Theorem 2.10.

(cf. [ADL19]) Let χ\chi be the Hilbert polynomial of an anti-canonically polarized smooth del Pezzo surface XX of degree dd. Let rr be the positive integer, and c(0,1/r)c\in(0,1/r) be a rational number. Consider the moduli pseudo-functor sending a reduced base SS to

d,cK(S)={(𝒳,𝒟)/S|(𝒳,c𝒟)/S is a -Gorenstein smoothable log Fano family,𝒟S,𝒬rK𝒳/S,each fiber (𝒳s,c𝒟s) is K-semistable, andχ(𝒳s,𝒪𝒳s(mK𝒳s))=χ(m) for m sufficiently divisible.}.\mathcal{M}^{K}_{d,c}(S)=\left\{(\mathcal{X},\mathcal{D})/S\left|\begin{array}[]{l}(\mathcal{X},c\mathcal{D})/S\textrm{ is a $\mathbb{Q}$-Gorenstein smoothable log Fano family},\\ \leavevmode\nobreak\ \mathcal{D}\sim_{S,\mathcal{Q}}-rK_{\mathcal{X}/S},\textrm{each fiber $(\mathcal{X}_{s},c\mathcal{D}_{s})$ is K-semistable, and}\\ \textrm{$\chi(\mathcal{X}_{s},\mathcal{O}_{\mathcal{X}_{s}}(-mK_{\mathcal{X}_{s}}))=\chi(m)$ for $m$ sufficiently divisible.}\end{array}\right.\right\}.

Then there is a smooth quotient stack dK(c)\mathcal{M}^{K}_{d}(c) of a smooth scheme by a projective general linear group which represents this pseudo-functor. The \mathbb{C}-points of dK(c)\mathcal{M}^{K}_{d}(c) parameterize K-semistable \mathbb{Q}-Gorenstein smoothable log Fano pairs (X,cD)(X,cD) with Hilbert polynomial χ(X,𝒪X(mKX))=χ(m)\chi(X,\mathcal{O}_{X}(-mK_{X}))=\chi(m) for sufficiently divisible m0m\gg 0 and DrKXD\sim_{\mathbb{Q}}-rK_{X}. Moreover, the stack dK(c)\mathcal{M}^{K}_{d}(c) admits a good moduli space M¯dK(c)\overline{M}^{K}_{d}(c), which is a normal projective reduced scheme of finite type over \mathbb{C}, whose \mathbb{C}-points parameterize K-polystable log Fano pairs.

Let XX be a smooth del Pezzo surface of degree d{1,2,3,4}d\in\{1,2,3,4\}, LiL_{i}’s be the lines on XX, and rr be the integer such that LirKX\sum L_{i}\sim-rK_{X}.

Definition 2.11.

Let d,cK\mathcal{M}^{K}_{d,c} be the stack-theoretic closure of the locally closed substack of dK(c)\mathcal{M}^{K}_{d}(c) parameterizing pairs (X,cD)(X,cD), where XX is a smooth del Pezzo surface and D=LiD=\sum L_{i}, and M¯d,cK\overline{M}^{K}_{d,c} be its good moduli space.

Remark 2.12.

The good moduli space M¯d,cK\overline{M}^{K}_{d,c} is exactly the closed subscheme of M¯dK(c)\overline{M}^{K}_{d}(c), which is the scheme-theoretic closure of the locus parameterizing smooth del Pezzo surfaces with the sum of lines.

Theorem 2.13.

(cf. [ADL19, Theorem 1.2]) Keep the notation as in the last theorem. There are rational numbers

0=c0<c1<c2<<cn=1r0=c_{0}<c_{1}<c_{2}<\cdots<c_{n}=\frac{1}{r}

such that for every 0j<n0\leq j<n, the K-moduli stacks d,cK\mathcal{M}^{K}_{d,c} are independent of the choice of c(cj,cj+1)c\in(c_{j},c_{j+1}). Moreover, for every 0j<n0\leq j<n and 0<ε10<\varepsilon\ll 1, one has open immersions

d,cjεKd,cjKd,cj+εK,\mathcal{M}^{K}_{d,c_{j}-\varepsilon}\hookrightarrow\mathcal{M}^{K}_{d,c_{j}}\hookleftarrow\mathcal{M}^{K}_{d,c_{j}+\varepsilon},

which descend to projective birational morphisms

M¯d,cjεKM¯d,cjKM¯d,cj+εK.\overline{M}^{K}_{d,c_{j}-\varepsilon}\rightarrow\overline{M}^{K}_{d,c_{j}}\leftarrow\overline{M}^{K}_{d,c_{j}+\varepsilon}.

3. Cubic and quartic del Pezzo pairs

In this section, we focus on the cases when d=3,4d=3,4. The K-moduli of cubic (resp. quartic) del Pezzo surfaces are isomorphic to the GIT moduli spaces of cubics (resp. quartics) (cf. [OSS16, MM93]). In particular, the K-polystable limits of the smooth ones are still embedded in 3\mathbb{P}^{3} (resp. 4\mathbb{P}^{4}) as a cubic surface (resp. complete intersection of quadric hypersurfaces), and they have at worst A1A_{1} and A2A_{2}-singularities (resp. A1A_{1}-singularities). Thus it makes sense to discuss lines on cubic and quartic del Pezzo surfaces with these mild singularities. The lines on singular cubic surfaces were first studied in [Cay69]: they are the degeneration of the 27 lines on smooth cubic surfaces with multiplicities, which are nothing but the number of lines which reduce to a given one on a singular cubic surface.

We will prove that for all cc in the Fano region, the K-moduli spaces M¯d,cK\overline{M}^{K}_{d,c} of cubic (and quartic) del Pezzo pairs do not have wall crossings, and the moduli spaces are all isomorphic to the K-moduli space of cubic (resp. quartic) del Pezzo surfaces. The proof will proceed by first showing that for 0<c=ε10<c=\varepsilon\ll 1, we have the desired isomorphism induced by the natural forgetful map, and then showing that M¯d,cKM¯d,εK\overline{M}^{K}_{d,c}\simeq\overline{M}^{K}_{d,\varepsilon}.

3.1. The cubic case

In [OSS16], the authors essentially proved that for cubic del Pezzo surfaces, the GIT-(semi/poly)stability is equivalent to the K-(semi/poly)stability. As a consequence, the two moduli spaces are isomorphic. However, the K-moduli space was constructed only in recent years. Although this is well-known to experts, for the reader’s convenience, here we state a more recent proof using local-global volumes comparison.

Theorem 3.1.

(cf. [OSS16, Section 4.2]) A cubic surface is K-semistable if and only if it is GIT-semistable. In particular, the K-moduli space of degree 33 del Pezzo surfaces is isomorphic to the GIT moduli space of cubic surfaces.

Proof.

We know that the Fermat cubic surface is K-stable (cf. [Tia87]). By the openness of the K-stability (cf. Theorem 2.5), a general cubic surface is K-stable. Denote by M¯3K\overline{M}^{K}_{3} by the K-moduli space of cubic del Pezzo surfaces, which parameterizes K-stable smooth cubic surfaces and their K-polystable limits. Let XM¯3KX\in\overline{M}^{K}_{3} be the limit of a 1-parameter family of {Xt}tT{0}\{X_{t}\}_{t\in T\setminus\{0\}} K-semistable smooth cubics.

As the K-semistable surfaces have klt singularities (cf. [Oda13]), in particular have quotient singularities, we let (xX)(0𝔸2/Gx)(x\in X)\simeq(0\in\mathbb{A}^{2}/G_{x}) be a singular point (if it exists). Then by Theorem 2.7, we have that

3=(KX)294vol^(x,X)=944|Gx|=9|Gx|,3=(-K_{X})^{2}\leq\frac{9}{4}\widehat{\operatorname{vol}}(x,X)=\frac{9}{4}\cdot\frac{4}{|G_{x}|}=\frac{9}{|G_{x}|},

which implies that |Gx|3|G_{x}|\leq 3. If |Gx|=2|G_{x}|=2, then xx is an A1A_{1}-singularity. If |Gx|=3|G_{x}|=3, then xx is either an A2A_{2}-singularity or a 13(1,1)\frac{1}{3}(1,1)-singularity. The latter case is ruled out by [KSB88, Proposition 3.10]. We thus conclude that XX has at worst A1A_{1}- or A2A_{2}-singularities. It follows from [Fuj90, Section 2] that XX can be embedded by |KX||-K_{X}| into 3\mathbb{P}^{3} as a cubic surface.

Since for hypersurfaces the K-stability implies GIT-stability (cf. [OSS16, Theorem 3.4] or [PT09, Theorem 2]), then we get an open immersion 3K3GIT\mathcal{M}^{K}_{3}\hookrightarrow\mathcal{M}^{\operatorname{GIT}}_{3} of moduli stacks, which descends to a birational and injective morphism Φ:M¯3KM¯3GIT\Phi:\overline{M}^{K}_{3}\rightarrow\overline{M}^{\operatorname{GIT}}_{3} between good moduli spaces. Notice that the M¯3GIT\overline{M}^{\operatorname{GIT}}_{3} is normal by the properties of GIT quotients. As both of these two moduli spaces are proper, then Φ\Phi is a finite map, and thus Φ\Phi is an isomorphism by Zariski Main Theorem.

Remark 3.2.

We will frequently call M¯3K\overline{M}^{K}_{3} the K-moduli spaces of cubic surfaces, by which we mean the K-moduli compactification of smooth K-polystable cubic surfaces.

In the proof of the theorem, we deduce that a K-polystable cubic del Pezzo surface has at worst A1A_{1}- or A2A_{2}-singularities. This partially recovers the following classical result of Hilbert.

Theorem 3.3.

(cf. [Hil70]) A cubic surface X3X\subseteq\mathbb{P}^{3} is

  1. (i)

    GIT-stable if and only if it has at worst A1A_{1}-singularities;

  2. (ii)

    GIT-strictly polystable if and only if it is isomorphic to the cubic X0X_{0} defined by x03=x1x2x3x_{0}^{3}=x_{1}x_{2}x_{3};

  3. (iii)

    GIT-semistable if and only if it has at worst A1A_{1}- or A2A_{2}-singularities.

For the semistable cubic surfaces, we know how the lines degenerate. In other words, we know the multiplicities of the lines (cf. [Tu05, Table 1]).

Proposition 3.4.

Let XX be a semistable cubic surface and LiL_{i}’s be the 27 lines on it. Then the pair (X,cLi)(X,c\sum L_{i}) is log canonical for 0<c<190<c<\frac{1}{9}.

Proof.

It is proven in [GKS21, Proposition 5.8] that if XX the log canonical threshold is larger than 19\frac{1}{9} if XX has at worst A1A_{1}-singularities.

Now let us deal with the surfaces with A2A_{2}-singularities. We first give an explicit construction of the surface X0={x03=x1x2x3}X_{0}=\{x_{0}^{3}=x_{1}x_{2}x_{3}\}. Let (x:y:z)(x:y:z) be the homogeneous coordinates of 2\mathbb{P}^{2}, then blow up the tangent vector given by {y=0}\{y=0\} at (1:0:0)(1:0:0), the tangent vector given by {z=0}\{z=0\} at (0:1:0)(0:1:0), and the tangent vector given by {x=0}\{x=0\} at (0:0:1)(0:0:1). Denote by EiE_{i} and FiF_{i} the exceptional divisors on the blow-up with self-intersection 2-2 and 1-1 respectively, and HiH_{i} the (2)(-2)-curves in the class

HE12F1E2F2,HE22F2E3F3,HE32F3E1F1,H-E_{1}-2F_{1}-E_{2}-F_{2},\quad H-E_{2}-2F_{2}-E_{3}-F_{3},\quad H-E_{3}-2F_{3}-E_{1}-F_{1},

respectively, where i=1,2,3i=1,2,3. Denote this surface by X~0\widetilde{X}_{0}. Finally contract the three pairs of (2)(-2)-curves to get X0X_{0}. Notice that there are four sections of ωX~0\omega^{*}_{\widetilde{X}_{0}} coming from xyz,y2z,z2x,x2yH0(2,ω2)xyz,y^{2}z,z^{2}x,x^{2}y\in H^{0}(\mathbb{P}^{2},\omega^{*}_{\mathbb{P}^{2}}). They give rise to a morphism from X~0\widetilde{X}_{0} to 3\mathbb{P}^{3} contracting (2)(-2)-curves, with image X03X_{0}\subseteq\mathbb{P}^{3} given by x03=x1x2x3x_{0}^{3}=x_{1}x_{2}x_{3}.

Let π:X~0X0\pi:\widetilde{X}_{0}\rightarrow X_{0} be the contraction map. This surface has three A2A_{2}-singularities, and the 27 lines degenerate to the images of F1,F2,F3F_{1},F_{2},F_{3}, denoted by G1G_{1}, G2G_{2}, G3G_{3}, each of which is of multiplicity 99 (cf. [Tu05, Proposition 4.1(ii)]). Then by computing intersection numbers, we deduce that

πG1=F1+13E1+23H1+13H2+23E2,\pi^{*}G_{1}=F_{1}+\frac{1}{3}E_{1}+\frac{2}{3}H_{1}+\frac{1}{3}H_{2}+\frac{2}{3}E_{2},

and the other two relations for πG2\pi^{*}G_{2} and πG3\pi^{*}G_{3}. As a result, we obtain that

A(X0,cLj)(Fi)=A(X0,cLj)(Ei)=A(X0,cLj)(Hi)=19c>0A_{(X_{0},c\sum L_{j})}(F_{i})=A_{(X_{0},c\sum L_{j})}(E_{i})=A_{(X_{0},c\sum L_{j})}(H_{i})=1-9c>0

for 0<c<190<c<\frac{1}{9}. Thus the pair (X0,cLj)(X_{0},c\sum L_{j}) is log canonical for 0<c<190<c<\frac{1}{9}. The other pairs whose surfaces have A2A_{2}-singularities specially degenerate to this case, so we get the result we desire. ∎

Proposition 3.5.

Let 0<ε10<\varepsilon\ll 1 be a rational number. Then the forgetful map φ:3K(ε)3K\varphi:\mathcal{M}^{K}_{3}(\varepsilon)\rightarrow\mathcal{M}^{K}_{3} is proper.

Proof.

Let π:(𝒳,c𝒟)T{0}\pi^{\circ}:(\mathscr{X}^{\circ},c\mathscr{D}^{\circ})\rightarrow T\setminus\{0\} be a family of K-semistable pairs, where (𝒳,c𝒟)t(\mathscr{X}^{\circ},c\mathscr{D}^{\circ})_{t} is isomorphic to a smooth del Pezzo surface with the sum of lines, and 𝒳T\mathscr{X}\rightarrow T be an extension of 𝒳T{0}\mathscr{X}^{\circ}\rightarrow T\setminus\{0\}. It suffices to show that there exists a unique extension π:(𝒳,c𝒟)T\pi:(\mathscr{X},c\mathscr{D})\rightarrow T of π\pi^{\circ}. The uniqueness is apparent to us: as 𝒳0\mathscr{X}_{0} is normal, the filling 𝒟0\mathscr{D}_{0} must be obtained in the following way if it exists. Let 𝒳sm\mathscr{X}^{\operatorname{sm}} be the open locus of 𝒳\mathscr{X} such that π:𝒳T\pi:\mathscr{X}\rightarrow T is smooth on 𝒳sm\mathscr{X}^{\operatorname{sm}}. Taking the scheme-theoretic closure of 𝒟\mathscr{D}^{\circ}, and restricting it to 𝒳0sm\mathscr{X}^{\operatorname{sm}}_{0}, the 𝒟0\mathscr{D}_{0} is the extension (by taking closure) of this restricted divisor on 𝒳0sm\mathscr{X}^{\operatorname{sm}}_{0} to 𝒳0\mathscr{X}_{0} as a Weil divisor.

Now we only need to display such a filling. Recall that the central fiber 𝒳0\mathscr{X}_{0} has at worst A2A_{2}-singularities. It was displayed in [Cay69] that the lines on general fibers degenerate to lines on 𝒳0\mathscr{X}_{0} with multiplicities, denoted by Li,0\sum L_{i,0}. It follows from Proposition 3.4 that the pair (𝒳0,cLi,0)(\mathscr{X}_{0},c\sum L_{i,0}) is log canonical when c=19c=\frac{1}{9}. It follows from interpolation that the pair (𝒳0,cLi,0)(\mathscr{X}_{0},c\sum L_{i,0}) is K-semistable for 0<c10<c\ll 1, and this gives a desired filling. ∎

Proposition 3.6.

Let 0<ε10<\varepsilon\ll 1 be a rational number. Then there is an isomorphism M¯3,εKM¯3K\overline{M}^{K}_{3,\varepsilon}\simeq\overline{M}^{K}_{3}.

Proof.

We claim that the forgetful map φ:3,εK3K\varphi:\mathcal{M}^{K}_{3,\varepsilon}\rightarrow\mathcal{M}^{K}_{3} is finite. Since φ\varphi is representable, by Proposition 3.5, it suffices to show that it is quasi-finite. In the proof of Proposition 3.5, we in fact show that for each K-semistable pair (X,cD)(X,cD) in the stack 3,εK\mathcal{M}^{K}_{3,\varepsilon}, the divisor DD is the sum of the lines on XX counted with multiplicities. For every cubic surface XX with at worst A2A_{2}-singularities, there are only finitely many lines on XX, hence φ\varphi is quasi-finite. The finite forgetful map φ\varphi descends to a finite morphism between good moduli spaces ψ:M¯3,εKM¯3K\psi:\overline{M}^{K}_{3,\varepsilon}\rightarrow\overline{M}^{K}_{3}. As the K-moduli M¯3K\overline{M}^{K}_{3} is normal, and the morphism ψ\psi is birational and finite, it follows from the Zariski’s Main Theorem that ψ\psi is an isomorphism. ∎

Remark 3.7.

In fact, the forgetful map φ\varphi between stacks is an isomorphism: for the universal family 𝒳\mathscr{X} over 3K\mathcal{M}^{K}_{3}, as we can still define lines with multiplicities on mildly singular cubic surfaces, there is a divisor 𝒟\mathscr{D} on 𝒳\mathscr{X} such that each fiber (𝒳,𝒟)t(\mathscr{X},\mathscr{D})_{t} is a cubic with sum of lines. This gives the inverse morphism of ϕ\phi.

Corollary 3.8.

Let XX be a K-semistable cubic surface and LiL_{i}’s are the 27 lines on it. Then the pair (X,cLi)(X,c\sum L_{i}) is K-semistable for 0<c<190<c<\frac{1}{9}. In other words, there are no walls for M¯3,cK\overline{M}^{K}_{3,c} when cc varies in (0,19)(0,\frac{1}{9}). We have a natural isomorphism

M¯3,cKM¯3K\overline{M}^{K}_{3,c}\stackrel{{\scriptstyle\sim}}{{\longrightarrow}}\overline{M}^{K}_{3}

induced by the forgetful map.

Proof.

This follows immediately from Proposition 3.4 and Proposition 3.6 that there are no walls for the K-moduli spaces M¯3,cK\overline{M}^{K}_{3,c}, and they are all isomorphic to the K-moduli of cubic del Pezzo surfaces, the isomorphism being induced by the forgetful map φ\varphi.

3.2. The quartic case

The existence of Kähler-Einstein metric on quartic surfaces was studied in [MM93, OSS16].

Theorem 3.9.

(cf. [OSS16, Theorem 4.1, 4.2]) A K-semistable quartic del Pezzo surface has at worst A1A_{1}-singularities.

By [HW81, Theorem 3.4], we know that every ADE del Pezzo surface is the contraction of the (2)(-2)-curves of a blow-up of 2\mathbb{P}^{2} at points in almost general position (cf. [HW81, Definition 3.2]), that is, in the position such that no (k)(-k)-curves will be created under the blow-up for any k3k\geq 3. Also, it follows from [Fuj90, Section 2] that an ADE del Pezzo surface of degree 44 can be always anti-canonically embedded in to 4\mathbb{P}^{4} as an complete intersection of two quadric 3-folds. Therefore, similar as in the cubic case, we have a canonical choice of the degeneration of the 16 lines on those ADE del Pezzo quartic surfaces.

Proposition 3.10.

Let XX be a K-semistable quartic del Pezzo surface and LiL_{i}’s the 16 lines on it. Then the pair (X,cLi)(X,c\sum L_{i}) is K-semistable for 0<c<140<c<\frac{1}{4}. Moreover, there is a natural isomorphism M¯4,cKM¯4K\overline{M}^{K}_{4,c}\simeq\overline{M}^{K}_{4} of the K-moduli spaces, induced by the forgetful map 4,εK4K\mathcal{M}^{K}_{4,\varepsilon}\rightarrow\mathcal{M}^{K}_{4}.

Proof.

As in the proof of Corollary 3.8, we have a family (𝒳,𝒟)(\mathcal{X},\mathcal{D}) over 4K\mathcal{M}^{K}_{4} such that a general fiber is a smooth quartic with the 16 lines on it. By interpolation of K-stability (cf. Theorem 2.4), if we prove that these pairs are log canonical for 0<c140<c\leq\frac{1}{4}, then (𝒳,c𝒟)(\mathcal{X},c\mathcal{D}) has K-semistable fibers for any 0c<1/40\leq c<1/4. In particular, the same argument of the second statement of Corollary 3.8 shows that M¯4,cKM¯4K\overline{M}^{K}_{4,c}\simeq\overline{M}^{K}_{4} for any c(0,14)c\in(0,\frac{1}{4}).

Now we prove that the each fiber in the family (𝒳,c𝒟)(\mathcal{X},c\mathcal{D}) is log canonical for 0c1/40\leq c\leq 1/4. Let (X,cD=cLi)(X,cD=c\sum L_{i}) be an arbitrary fiber.

  1. (i)

    If XX is smooth, then the 16 lines are distinct and Li\sum L_{i} is normal crossing. Thus the pair is log canonical automatically.

  2. (ii)

    If XX has one A1A_{1}-singularity pp, then we claim that there exist exactly four lines of multiplicity two and eight lines of multiplicity one, and that these double lines pass through pp, while the remaining eight lines avoid it.

    First notice that a quintic del Pezzo surface XX with exactly one A1A_{1}-singularity is obtained by contracting the (2)(-2)-curve on the blow-up of 2\mathbb{P}^{2} along three distinct points p1,p2,p3p_{1},p_{2},p_{3} and a tangent vector supported at p4p_{4}. In fact, let pXp\in X be the singularity, and X~X\widetilde{X}\rightarrow X the blow-up of XX at pp with an exceptional divisor, which is a (2)(-2)-curve. By [HW81, Theorem 3.4], the surface X~\widetilde{X} is obtained from blowing up 2\mathbb{P}^{2}, thus there must be a (1)(-1)-curve CC intersecting EE. Contracting first CC, then the proper transform of EE, one get a smooth del Pezzo surface of degree 66, which is a blow-up of 2\mathbb{P}^{2} at three distinct points.

    Consider a one-parameter family of projective planes 2×𝔸1𝔸1\mathbb{P}^{2}\times\mathbb{A}^{1}\rightarrow\mathbb{A}^{1}, and let l1,,l5l_{1},...,l_{5} be five sections of 𝔸1\mathbb{A}^{1} such that over 0t𝔸10\neq t\in\mathbb{A}^{1}, l1,,l5l_{1},...,l_{5} does not intersect, while over 0, only l4l_{4} and l5l_{5} intersect transversely. Blowing up 2×𝔸1\mathbb{P}^{2}\times\mathbb{A}^{1} along l1l5l_{1}\cup\cdots\cup l_{5} with reduced scheme structure, one get a degeneration 𝔛𝔸1\mathfrak{X}\rightarrow\mathbb{A}^{1} of smooth quartic del Pezzo surfaces to a singular one with exactly one A1A_{1}-singlarity. Denote pi(t)p_{i}(t) the intersection of lil_{i} with the fiber t2\mathbb{P}^{2}_{t} over t𝔸1t\in\mathbb{A}^{1}. Then under the family 𝔛𝔸1\mathfrak{X}\rightarrow\mathbb{A}^{1}, the lines L(pi(t),p4(t))L(p_{i}(t),p_{4}(t)) and L(pi(t),p5(t))L(p_{i}(t),p_{5}(t)) (for i=1,2,3) on general fibers 𝔛t\mathfrak{X}_{t} degenerate to the same line L(pi(0),p4(0))=L(pi(0),p5(0))L(p_{i}(0),p_{4}(0))=L(p_{i}(0),p_{5}(0)), and the exceptional divisors over p4(t)p_{4}(t) and p5(t)p_{5}(t) also degenerate to the same line, which is the exceptional divisor over p4(0)=p5(0)p_{4}(0)=p_{5}(0). The other eight lines over general fibers degenerate to distinct lines on 𝔛0\mathfrak{X}_{0}. Finally observe that K𝔛/𝔸1-K_{\mathfrak{X}/\mathbb{A}^{1}} gives rise to an embedding of 𝔛\mathfrak{X} into 4×𝔸1\mathbb{P}^{4}\times\mathbb{A}^{1} over 𝔸1\mathbb{A}^{1}. Thus this degeneration indeed occurs in the Hilbert scheme.

    Let EE be the exceptional divisor of the blow-up π:X~X\pi:\widetilde{X}\rightarrow X. Then E+πLiE+\pi^{*}\sum L_{i} has simple normal crossing support. Moreover, we have that

    A(X,cLi)(E)=14c>0A_{(X,c\sum L_{i})}(E)=1-4c>0

    for any 0<c<140<c<\frac{1}{4}. As the multiplicity of the proper transform of LiL_{i} is at most two, then the pair is log canonical.

  3. (iii)

    If XX has two A1A_{1}-singularities pp and qq, then there exist one line of multiplicity four, four lines of multiplicity two and four lines of multiplicity one. This follows from the same argument as in (i), and in fact the line with multiplicity four passes through both pp and qq, the line with multiplicity two passes through either pp or qq, and the line with multiplicity one avoids both pp and qq. For each singularity, there are exactly eight lines (counted with multiplicities) passing through it. Let EE be the exceptional divisor of the blow-up at pp. Then we have that

    A(X,cLi)(E)=14c>0A_{(X,c\sum L_{i})}(E)=1-4c>0

    for any 0<c<140<c<\frac{1}{4}. As the multiplicity of the proper transform of LiL_{i} is at most four, then the pair is log canonical.

    The proof of cases (iii) and (iv) are completely the same, we will omit part of the details.

  4. (iv)

    Suppose that XX has three A1A_{1}-singularities. Then XX is obtained as follows: blow up 2\mathbb{P}^{2} at a general tangent vector and at three curvilinear points on a general line, where two of them collide, then take the ample model. There exist two lines of multiplicity four, and four lines of multiplicity two. For each singularity, there are exactly eight lines (counted with multiplicities) passing through it. For the same reason as in (ii), the pair is log canonical.

  5. (v)

    If XX has four A1A_{1}-singularities, then it is obtained as follows: blow up 2\mathbb{P}^{2} at a general point PP and at two tangent vectors whose supporting lines pass through PP, then take the ample model. There are four lines of multiplicity four. For each singularity, there are exactly eight lines (counted with multiplicities) passing through it. For the same reason as in (ii), the pair is log canonical.

In the proof of the Proposition 3.10, we can deduce the following result, which is proved in [Tu05] for cubic surface case. The explicit equations of the lines on any A1A_{1} cubic del Pezzo surface can be carried out from the normal form as a cubic hypersurface in 3\mathbb{P}^{3}. When reducing from the smooth surface to a singular one, the 27 lines on a smooth surface reduce to the lines on the corresponding singular surface. The multiplicity (cf. [Cay69]) of a line ll of a singular surface is nothing but the number of lines which reduce to ll.

Corollary 3.11.

Let X4X\subseteq\mathbb{P}^{4} be a quartic del Pezzo surface with at worst A1A_{1}-singularities, and ll is a line on it. Then

  1. (1)

    If ll does not contain any singular point, then ll is of multiplicity 1;

  2. (2)

    If ll contains exactly one singularity, then ll is of multiplicity 2;

  3. (3)

    If ll contains two singularities, then ll is of multiplicity 4.

Remark 3.12.

Using the same argument as in Theorem 3.1, one can prove that the K-moduli space of quartic del Pezzo surfaces is isomorphic to the GIT-moduli space

Gr(2,H0(4,𝒪4(2)))ss//PGL(5).\operatorname{Gr}(2,H^{0}(\mathbb{P}^{4},\mathcal{O}_{\mathbb{P}^{4}}(2)))^{ss}\mathbin{\mkern-3.0mu/\mkern-6.0mu/\mkern-3.0mu}\operatorname{PGL}(5).

See [OSS16, SS17] for details. As a consequence, each K-moduli space M¯4,cK\overline{M}^{K}_{4,c} is isomorphic to this GIT-moduli space.

4. Degree two case

In this section, we prove that there are no walls for the K-moduli spaces M¯2,cK\overline{M}^{K}_{2,c} when we vary the coefficient cc from 0 to 128\frac{1}{28}.

Recall that a smooth del Pezzo surface of degree 22 is a double cover of 2\mathbb{P}^{2} branched along a quartic curve, and the 56 lines are sent pairwise to the 28 bitangent lines of the quartic. Thus the K-stability of a degree 22 del Pezzo surface XX is equivalent to the K-stability of a del Pezzo pair (2,12C4)(\mathbb{P}^{2},\frac{1}{2}C_{4}) (cf. [ADL19, Remark 6.2]), where C4C_{4} is the quartic plane curve along which the double cover X2X\rightarrow\mathbb{P}^{2} is branched.

In [OSS16], the authors give a description of the K-moduli space of del Pezzo surfaces of degree 22. It is diffeomorphic to the blow-up of H0(2,𝒪2(4))ss//PGL(3)\mathbb{P}H^{0}(\mathbb{P}^{2},\mathcal{O}_{\mathbb{P}^{2}}(4))^{ss}\mathbin{\mkern-3.0mu/\mkern-6.0mu/\mkern-3.0mu}\operatorname{PGL}(3) at the point parameterizing the double conic. Moreover, each point [s][s] on the exceptional divisor EE represents a surface which is a double cover of (1,1,4)\mathbb{P}(1,1,4) branched along a hyperelliptic curve z2=f8(x,y)z^{2}=f_{8}(x,y), where f8f_{8} is a GIT-polystable octic binary form. In [ADL19], the authors study the wall crossing of the K-moduli of pairs (2,cC4)(\mathbb{P}^{2},cC_{4}) when cc varies from 0 to 34\frac{3}{4}. They proved that there is a unique wall c=38c=\frac{3}{8}. As a result, the K-moduli of degree 22 del Pezzo surfaces is isomorphic to a weighted blow-up of the GIT moduli space H0(2,𝒪2(4))ss//PGL(3)\mathbb{P}H^{0}(\mathbb{P}^{2},\mathcal{O}_{\mathbb{P}^{2}}(4))^{ss}\mathbin{\mkern-3.0mu/\mkern-6.0mu/\mkern-3.0mu}\operatorname{PGL}(3) at the point parameterizing the double conic. For a rigorous proof, we refer the reader to [ADL21, Proposition 6.12], where the authors prove that the K-moduli of the quartic double solids is isomorphic to the K-moduli space of K-polystable pairs (X,12D)(X,\frac{1}{2}D) which admit a \mathbb{Q}-Gorenstein smoothing to (3,12S)(\mathbb{P}^{3},\frac{1}{2}S) with S|K3|S\in|-K_{\mathbb{P}^{3}}| a smooth quartic K3 surface.

Observe that the degeneration of 2\mathbb{P}^{2} to (1,1,4)\mathbb{P}(1,1,4) can occur in (1,1,1,2)\mathbb{P}(1,1,1,2) (cf. [ADL19, Theorem 5.14]), thus there is a canonical choice of the degeneration of the curves and the bitangent lines, and the multiplicity is well-defined. Therefore, we can apply the same approach as in the degree d=3,4d=3,4 cases, to show that there are no walls. By interpolation of K-semistability, it suffices to check that the (X,128Ei)(X,\frac{1}{28}\sum E_{i}) is log canonical, where XX is a K-polystable degree quadric del Pezzo surface and EiE_{i}’s are the lines on it. It further reduces to checking that (2,12C+128Li)(\mathbb{P}^{2},\frac{1}{2}C+\frac{1}{28}\sum L_{i}) or ((1,1,4),12C+128Li)(\mathbb{P}(1,1,4),\frac{1}{2}C+\frac{1}{28}\sum L_{i}) is log canonical (cf. [KM98, Proposition 5.20]), where CC is the branched curve and LiL_{i}’s are the bitangent lines of it.

The classification of the semistable plane quartics is well-known to the experts (cf. [MFK94]). For the reader’s convenience, we state the result here.

Lemma 4.1.

(cf. [HL10, Theorem 2]) Let G=PGL(3)G=\operatorname{PGL}(3) act on the space of plane quartic. A plane quartic curve C42C_{4}\subseteq\mathbb{P}^{2} is

  1. (i)

    stable if and only if it has at worst A1A_{1} or A2A_{2} singularities;

  2. (ii)

    strictly semistable if and only it is a double conic or has a tacnode. Moreover, C4C_{4} belongs to a minimal orbit if and only if it is either a double conic or the union of two tangent conics, where at least one is smooth.

Remark 4.2.

In the case (ii), if both of the (distinct) conics are smooth, then we call it cateye; if there is a singular one, we call it ox. These are the only two types of polystable quartics with infinite stabilizers.

4.1. Singularities of plane curves with infinite stabilizers

Let us first compute the log canonical property for the special cases where the quartics have infinite stabilizers.

Lemma 4.3.

The pair (2,12(C2+C2)+cLi)(\mathbb{P}^{2},\frac{1}{2}(C_{2}+C^{\prime}_{2})+c\sum L_{i}) is log canonical for 0<c<1280<c<\frac{1}{28}, where C2C_{2} and C2C^{\prime}_{2} are two smooth conics tangential at two points pp and qq.

Proof.

First observe that the (2,C2+C2)(\mathbb{P}^{2},C_{2}+C^{\prime}_{2}) is the degeneration (in the Hilbert scheme) of pairs (2,C2(t)+C2(t))tT(\mathbb{P}^{2},C_{2}(t)+C^{\prime}_{2}(t))_{t\in T} where the boundary divisors consist of two smooth conics with a tacnode and two nodes. It follows from [CS03, Section 3.4 case 2] that the arrangement of the 28 bitangent lines of C2+C2C_{2}+C^{\prime}_{2} is Li=6Lp+6Lq+16Lpq\sum L_{i}=6L_{p}+6L_{q}+16L_{pq}, where LpL_{p} and LqL_{q} are tangent lines of the conics at pp and qq respectively, and LpqL_{pq} is the line connecting pp and qq. It follows immediately that the coefficients of 12(C2+C2)+cLi\frac{1}{2}(C_{2}+C^{\prime}_{2})+c\sum L_{i} are all smaller than 11.

Taking the minimal log resolution of (2,12(C2+C2)+cLi)(\mathbb{P}^{2},\frac{1}{2}(C_{2}+C^{\prime}_{2})+c\sum L_{i}). By symmetry, we only need to look at the log resolution at qq. Let EE and FF be the exceptional divisors over qq with self-intersection 2-2 and 1-1 respectively. Then one has A(E)=122cA(E)=1-22c and A(F)=128cA(F)=1-28c, which are positive when 0<c<1280<c<\frac{1}{28}. ∎

The ox case is similar.

Lemma 4.4.

The pair (2,12(C2+M1+M1)+cLi)(\mathbb{P}^{2},\frac{1}{2}(C_{2}+M_{1}+M_{1}^{\prime})+c\sum L_{i}) is log canonical for 0<c<1280<c<\frac{1}{28}, where C2C_{2} is a smooth conic, and M1,M1M_{1},M_{1}^{\prime} are two distinct lines tangential to C2C_{2} at two points pp and qq respectively.

Proof.

First observe that the (2,C2+M1+M1)(\mathbb{P}^{2},C_{2}+M_{1}+M_{1}^{\prime}) is the degeneration (in the Hilbert scheme) of pairs (2,C2(t)+M1(t)+M1(t))tT(\mathbb{P}^{2},C_{2}(t)+M_{1}(t)+M_{1}^{\prime}(t))_{t\in T} where the boundary divisors consist of two distinct lines M1(t)M_{1}(t), M1(t)M_{1}^{\prime}(t) and a smooth conic C2(t)C_{2}(t) tangent to M1(t)M_{1}(t) at a point p(t)p(t) and meeting M1(t)M_{1}^{\prime}(t) transversely. It follows from [CS03, Section 3.4 case 10] that the arrangement of the 28 bitangent lines of C2+M1+M1C_{2}+M_{1}+M_{1}^{\prime} is Li=6M1+6M1+16Lpq\sum L_{i}=6M_{1}+6M_{1}^{\prime}+16L_{pq}, where LpqL_{pq} is the line connecting pp and qq. It follows immediately that the coefficients of 12(C2+C2)+cLi\frac{1}{2}(C_{2}+C^{\prime}_{2})+c\sum L_{i} are all smaller than 11.

Taking the minimal log resolution of (2,12(C2+M1+M1)+cLi)(\mathbb{P}^{2},\frac{1}{2}(C_{2}+M_{1}+M_{1}^{\prime})+c\sum L_{i}). By symmetry, we only need to look at the log resolution at qq. Let EE and FF be the exceptional divisors over qq with self-intersection 2-2 and 1-1 respectively. Then one has A(E)=122cA(E)=1-22c and A(F)=128cA(F)=1-28c, which are positive when 0<c<1280<c<\frac{1}{28}. ∎

4.2. Singularities of reducible plane curves with finite stabilizers

Now we consider the reducible quartics with finite stabilizers.

Proposition 4.5.

Let C4C_{4} be a reducible quartic curve in 2\mathbb{P}^{2} with finite stabilizers under the PGL(3)\operatorname{PGL}(3)-action, and LiL_{i}’s are the degeneration on C4C_{4} of the 28 bitangent lines of smooth quartics. Then (2,12C4+cLi)(\mathbb{P}^{2},\frac{1}{2}C_{4}+c\sum L_{i}) is log canonical for 0c1280\leq c\leq\frac{1}{28}.

Proof.

The classification of C4C_{4} is listed in [CS03, Section 3.4]. For each class, we can run the same argument. For simplicity, we only prove the statement for one class where C4=M1+M2+M3+M4C_{4}=M_{1}+M_{2}+M_{3}+M_{4} is the union of four general lines (forming three pairs of nodes). In this case, we have that Li=4(M1++M7)\sum L_{i}=4(M_{1}+\cdots+M_{7}), where M5,M6,M7M_{5},M_{6},M_{7} are the lines joining the three pairs of nodes (cf. [CS03, Section 3.4 case 11]). Then the blow-up of the pair (2,12C4+cLi)(\mathbb{P}^{2},\frac{1}{2}C_{4}+c\sum L_{i}) at the six nodes (with exceptional divisors E1,,E6E_{1},...,E_{6}) is log smooth. As the boundary divisors 12C4+cLi\frac{1}{2}C_{4}+c\sum L_{i} have coefficients less than 11 and A(2,12C4+cLi)(Ei)=112c>0A_{(\mathbb{P}^{2},\frac{1}{2}C_{4}+c\sum L_{i})}(E_{i})=1-12c>0, then the pair we consider is log canonical. ∎

4.3. Singularities of irreducible plane curves with finite stabilizers

Now we deal with the general case: an irreducible plane quartic C4C_{4} with at worst A1A_{1} or A2A_{2} singularities. We first assume that C4C_{4} is irreducible. Then the [CS03, Table 3.2, Lemma 3.3.1] describe how these bitangent lines degenerate. We claim that all these curves give log canonical pairs (2,12C4+cLi)(\mathbb{P}^{2},\frac{1}{2}C_{4}+c\sum L_{i}).

Lemma 4.6.

The pair (2,12C4+cLi)(\mathbb{P}^{2},\frac{1}{2}C_{4}+c\sum L_{i}) is log canonical for 0<c<1280<c<\frac{1}{28}, where C4C_{4} has three nodes.

Proof.

We know from [CS03, Lemma 3.3.1] that the 28 lines degenerate to 4 bitangent lines of multiplicity 1 not passing through the nodes, 6 tangent lines of multiplicity 2 passing through exactly one node, and 3 lines of multiplicity 4 containing two nodes. Thus for each node pp, there are 12 lines passing through it, and at most 4 lines tangential to it. One can blow up at pp twice to get a log resolution. We have A(E)=116c>0A(E)=1-16c>0 and A(F)3220c>0A(F)\geq\frac{3}{2}-20c>0 for 0<c<1/280<c<1/28, where EE and FF are the two exceptional divisors over pp with self-intersection 2-2 and 1-1 respectively. The singularities at other points are milder, thus (2,12C4+cLi)(\mathbb{P}^{2},\frac{1}{2}C_{4}+c\sum L_{i}) is log canonical as desired.

Lemma 4.7.

The pair (2,12C4+cLi)(\mathbb{P}^{2},\frac{1}{2}C_{4}+c\sum L_{i}) is log canonical for 0<c<1280<c<\frac{1}{28}, where C4C_{4} has three cusps.

Proof.

We know from [CS03, Lemma 3.3.1] that the 28 lines degenerate to 4 bitangent lines of multiplicity 1 not passing through the cusps, and 3 lines of multiplicity 9 containing two cusps. Thus for each cusp pp, there are 18 lines passing through it, and none of them are tangential to it. One can blow up at pp three times to get a log resolution. Let E,F,GE,F,G be the exceptional divisors with self-intersection 3,2,1-3,-2,-1 respectively. We have A(E)=118c>0A(E)=1-18c>0, A(F)=3218c>0A(F)=\frac{3}{2}-18c>0, and A(G)=236c>0A(G)=2-36c>0 for 0<c<1/280<c<1/28. The singularities at other points are milder, thus (2,12C4+cLi)(\mathbb{P}^{2},\frac{1}{2}C_{4}+c\sum L_{i}) is log canonical as desired.

Lemma 4.8.

The pair (2,12C4+cLi)(\mathbb{P}^{2},\frac{1}{2}C_{4}+c\sum L_{i}) is log canonical for 0<c<1280<c<\frac{1}{28}, where C4C_{4} has one node and two cusps.

Proof.

By [CS03, Lemma 3.3.1], we see that the 28 lines degenerate to one bitangent line of multiplicity 1 not passing through the singularities, 2 tangent lines of multiplicity 3 passing through exactly one cusp, 1 line of multiplicity 9 containing two cusps, and 2 lines of multiplicity 6 passing through one node and one cusp.

Thus for the node pp, there are 12 lines passing through it, and none of them are tangential to it. One can blow up at pp to get a log resolution and the log discrepancy with respect to the exceptional divisor is 112c>01-12c>0.

For each cusp qq, there are 18 lines passing through it, and at most 3 lines tangential to it. Resolving qq by blowing up three times, one gets three exceptional divisors E,F,GE,F,G with self-intersection 3,2,1-3,-2,-1 respectively. We have A(E)=118c>0A(E)=1-18c>0, A(F)3221c>0A(F)\geq\frac{3}{2}-21c>0, and A(G)239c>0A(G)\geq 2-39c>0 for 0<c<1/280<c<1/28. The singularities at other points are milder, thus (2,12C4+cLi)(\mathbb{P}^{2},\frac{1}{2}C_{4}+c\sum L_{i}) is log canonical as desired.

Lemma 4.9.

The pair (2,12C4+cLi)(\mathbb{P}^{2},\frac{1}{2}C_{4}+c\sum L_{i}) is log canonical for 0<c<1280<c<\frac{1}{28}, where C4C_{4} has one cusp and two nodes.

Proof.

By [CS03, Lemma 3.3.1], we see that the 28 lines degenerate to 2 bitangent lines of multiplicity 1 not passing through the singularities, 2 tangent lines of multiplicity 3 passing through exactly the cusp, 2 tangent lines of multiplicity 2 passing through exactly one node, 1 line of multiplicity 4 containing two nodes, and 2 lines of multiplicity 6 passing through one node and one cusp.

Thus for the cusp pp, there are 18 lines passing through it, and at most 6 of them are tangential to it. Resolving pp by blowing up three times, one gets three exceptional divisors E,F,GE,F,G with self-intersection 3,2,1-3,-2,-1 respectively. We have A(E)=118c>0A(E)=1-18c>0, A(F)3224c>0A(F)\geq\frac{3}{2}-24c>0, and A(G)242c>0A(G)\geq 2-42c>0 for 0<c<1/280<c<1/28.

For each node qq, there are 12 lines passing through it, and at most 2 lines tangential to it. One can blow up at pp twice to get a log resolution. We have A(E)=112c>0A(E^{\prime})=1-12c>0 and A(F)3214c>0A(F^{\prime})\geq\frac{3}{2}-14c>0 for 0<c<1/280<c<1/28, where EE^{\prime} and FF^{\prime} are the two exceptional divisors over pp with self-intersection 2-2 and 1-1 respectively. The singularities at other points are milder, thus (2,12C4+cLi)(\mathbb{P}^{2},\frac{1}{2}C_{4}+c\sum L_{i}) is log canonical as desired.

The other pairs with C4C_{4} irreducible have milder singularity than the four types in the above four lemmas. Applying the same argument to all these pairs, we conclude the following.

Proposition 4.10.

Let C4C_{4} be a GIT-semistable plane quartic which is not a double conic. Then the pair (2,12C4+cLi)(\mathbb{P}^{2},\frac{1}{2}C_{4}+c\sum L_{i}) is log canonical for 0<c<1280<c<\frac{1}{28}. In particular, these pairs are K-semistable for 0<c<1/280<c<1/28.

4.4. Singularities of curves in (1,1,4)\mathbb{P}(1,1,4)

We first point out an explicit degeneration of 2\mathbb{P}^{2} to (1,1,4)\mathbb{P}(1,1,4) in (1,1,1,2)\mathbb{P}(1,1,1,2). Let (x0:x1:x2:x3)(x_{0}:x_{1}:x_{2}:x_{3}) be the homogeneous coordinate of (1,1,1,2)\mathbb{P}(1,1,1,2) and then consider the the hypersurface

𝔛:={(t,(x0:x1:x2:x3)):tx3=x0x2x12}𝔸1×(1,1,1,2).\mathfrak{X}:=\left\{(t,(x_{0}:x_{1}:x_{2}:x_{3})):t\cdot x_{3}=x_{0}x_{2}-x_{1}^{2}\right\}\subseteq\mathbb{A}^{1}\times\mathbb{P}(1,1,1,2).

The natural projection π:𝔛𝔸1\pi:\mathfrak{X}\rightarrow\mathbb{A}^{1} gives a special degeneration of 2\mathbb{P}^{2} to (1,1,4)\mathbb{P}(1,1,4).

Recall that an octic binary form f8(x,y)f_{8}(x,y) is GIT-semistable if and only if each of its zeros has multiplicity at most 44 (cf. [MFK94] Section 4.1). Also notice that if the point (x:y:z)(x:y:z) is an singularity of the curve C={z2=f8(x,y)}C=\{z^{2}=f_{8}(x,y)\}, then z=0z=0 and (x:y)(x:y) is a multiple root of f8(x,y)f_{8}(x,y).

Let pip_{i} be the intersection points of CC and {z=0}\{z=0\}, where i=1,,8i=1,...,8. Another important observation is that a bitangent line of a plane quartic degenerate under π\pi to two rulings of (1,1,4)\mathbb{P}(1,1,4), each of which passes through some pip_{i}, and there are (82)=28\binom{8}{2}=28 pairs in total. Thus we only need to focus on the vertex pp of (1,1,4)\mathbb{P}(1,1,4) and the singularities of CC.

Proposition 4.11.

The pair ((1,1,4),12C+cLi)(\mathbb{P}(1,1,4),\frac{1}{2}C+c\sum L_{i}) is log canonical for 0<c<1280<c<\frac{1}{28}.

Proof.

Notice that CC does not pass through the vertex pp. Let EE be the exceptional divisor of Blp(1,1,4)(1,1,4)\operatorname{Bl}_{p}\mathbb{P}(1,1,4)\rightarrow\mathbb{P}(1,1,4). Then A(E)=1214c>0A(E)=\frac{1}{2}-14c>0 for 0<c<1280<c<\frac{1}{28}.

Suppose that pi=(x:y:0)p_{i}=(x:y:0) is a singular point of CC. We may assume that x=0x=0 and y=1y=1, and locally the equation of CC is z2=xtz^{2}=x^{t}, where t{2,3,4}t\in\{2,3,4\}. When t=4t=4, pip_{i} is a tacnode, and there are 28 lines passing through it. Let FF and GG be the exceptional divisors of the minimal resolution of pip_{i} with self-intersection 2-2 and 1-1 respectively. Then A(F)=128c>0A(F)=1-28c>0 and A(G)=128c>0A(G)=1-28c>0 for 0<c<1280<c<\frac{1}{28}. This is also true for the cases t=2t=2 and t=3t=3.

To sum up, we conclude the following by the same argument as in Corollary 3.8.

Theorem 4.12.

Let M¯2K\overline{M}^{K}_{2} be the K-moduli space of degree 22 del Pezzo surfaces. Then there are no walls for the K-moduli stacks 2,cK\mathcal{M}^{K}_{2,c}, and there is an isomorphism

M¯2,cKM¯2K\overline{M}^{K}_{2,c}\simeq\overline{M}^{K}_{2}

for any 0<c<1280<c<\frac{1}{28}.

5. Discussion on degree one case

In this section, we display some examples to show that there exist some walls for M1,cKM^{K}_{1,c} when cc varies from 0 to 1240\frac{1}{240}. The following result describes the K-polystable del Pezzo surfaces with at worst ADE singularities. For the analytic description of the K-moduli space M1KM^{K}_{1}, see [OSS16, Section 5].

Proposition 5.1.

(cf. [OSS16, Section 6.1.2]) A nodal del Pezzo surface XX of degree 11 is K-polystable if and only if it has either only AkA_{k}-singularities with k7k\leq 7, or exactly two D4D_{4}-singularities, and XX is not isomorphic to one of the surfaces parameterized by (a1:a2)1(a_{1}:a_{2})\in\mathbb{P}^{1}, which are hypersurfaces in (1,1,2,3)\mathbb{P}(1,1,2,3) defined by the equations

w2=a1z3+z2x2+zy4+a2z2y2.w^{2}=a_{1}z^{3}+z^{2}x^{2}+zy^{4}+a_{2}z^{2}y^{2}.

5.1. Degree one del Pezzo with an A7A_{7}-singularity

We aim to prove the following statement.

Proposition 5.2.

Let YY be a del Pezzo surface of degree one with an A7A_{7}-singularity, and LiL_{i}’s be the degeneration of the 240 lines. Then the pair (Y,cLi)(Y,c\sum L_{i}) is K-unstable for c1288.c\geq\frac{1}{288}.

Proof.

Let YY be a degree one del Pezzo surface with an A7A_{7}-singularity. Then YY is obtained by blowing up 2\mathbb{P}^{2} at eight curvilinear points on a smooth cubic curve supported at a single point and taking the ample model. Let E1,,E8E_{1},...,E_{8} be the eight exceptional divisor on the blow-up Y~\widetilde{Y} in the order of blow-up, and HH the class of the pull-back of 𝒪2(1)\mathcal{O}_{\mathbb{P}^{2}}(1). Then the proper transform to Y~\widetilde{Y} of the 240 lines on YY are of the following types:

  1. (a)

    E8E_{8}, intersecting E7E_{7}, of multiplicity 8;

  2. (b)

    HE12E22E32E8H-E_{1}-2E_{2}-2E_{3}-\cdots-2E_{8}, intersecting E2E_{2}, of multiplicity 28;

  3. (c)

    2HE12E23E34E45i5Ei2H-E_{1}-2E_{2}-3E_{3}-4E_{4}-5\sum_{i\geq 5}E_{i}, intersecting E5E_{5}, of multiplicity 56;

  4. (d)

    3H2E13E28E78E83H-2E_{1}-3E_{2}-\cdots-8E_{7}-8E_{8}, intersecting E1E_{1} and E7E_{7}, of multiplicity 56;

  5. (e)

    4H2E14E26E3i4(i+3)Ei4H-2E_{1}-4E_{2}-6E_{3}-\sum_{i\geq 4}(i+3)E_{i}, intersecting E3E_{3} and E8E_{8}, of multiplicity 56;

  6. (f)

    5Hi=162iEi13E714E85H-\sum_{i=1}^{6}2iE_{i}-13E_{7}-14E_{8}, intersecting E6E_{6} and E8E_{8}, of multiplicity 28;

  7. (g)

    6H3E1i2(2i+1)Ei6H-3E_{1}-\sum_{i\geq 2}(2i+1)E_{i}, intersecting E1E_{1} and intersecting E8E_{8} twice, of multiplicity 8;

Denote by LiL_{i} and lil_{i} the line and its image on YY of one of the above types, and aia_{i} be the multiplicity of the line LiL_{i}, where i=0,1,,6i=0,1,...,6 is the coefficient of HH in the class. Let π:Y~Y\pi:\widetilde{Y}\rightarrow Y be the blow-down morphism. Then we have

πl0=E8+78E7+68E6+58E5+48E4+38E3+28E2+18E1,\pi^{*}l_{0}=E_{8}+\frac{7}{8}E_{7}+\frac{6}{8}E_{6}+\frac{5}{8}E_{5}+\frac{4}{8}E_{4}+\frac{3}{8}E_{3}+\frac{2}{8}E_{2}+\frac{1}{8}E_{1},
πl1=L1+14E7+24E6+34E5+44E4+54E3+64E2+34E1,\pi^{*}l_{1}=L_{1}+\frac{1}{4}E_{7}+\frac{2}{4}E_{6}+\frac{3}{4}E_{5}+\frac{4}{4}E_{4}+\frac{5}{4}E_{3}+\frac{6}{4}E_{2}+\frac{3}{4}E_{1},
πl2=L2+58E7+108E6+158E5+128E4+98E3+68E2+38E1,\pi^{*}l_{2}=L_{2}+\frac{5}{8}E_{7}+\frac{10}{8}E_{6}+\frac{15}{8}E_{5}+\frac{12}{8}E_{4}+\frac{9}{8}E_{3}+\frac{6}{8}E_{2}+\frac{3}{8}E_{1},
πl3=L3+E7+E6+E5+E4+E3+E2+E1,\pi^{*}l_{3}=L_{3}+E_{7}+E_{6}+E_{5}+E_{4}+E_{3}+E_{2}+E_{1},
πl4=L4+38E7+68E6+98E5+128E4+158E3+108E2+58E1,\pi^{*}l_{4}=L_{4}+\frac{3}{8}E_{7}+\frac{6}{8}E_{6}+\frac{9}{8}E_{5}+\frac{12}{8}E_{4}+\frac{15}{8}E_{3}+\frac{10}{8}E_{2}+\frac{5}{8}E_{1},
πl5=L5+34E7+64E6+54E5+44E4+34E3+24E2+14E1,\pi^{*}l_{5}=L_{5}+\frac{3}{4}E_{7}+\frac{6}{4}E_{6}+\frac{5}{4}E_{5}+\frac{4}{4}E_{4}+\frac{3}{4}E_{3}+\frac{2}{4}E_{2}+\frac{1}{4}E_{1},
πl6=L6+18E7+28E6+38E5+48E4+58E3+68E2+78E1.\pi^{*}l_{6}=L_{6}+\frac{1}{8}E_{7}+\frac{2}{8}E_{6}+\frac{3}{8}E_{5}+\frac{4}{8}E_{4}+\frac{5}{8}E_{3}+\frac{6}{8}E_{2}+\frac{7}{8}E_{1}.

In particular, one gets that the log discrepancy

A(Y,caiLi)(E3)=A(Y,caiLi)(E4)=A(Y,caiLi)(E5)=1288c<0A_{(Y,c\sum a_{i}L_{i})}(E_{3})=A_{(Y,c\sum a_{i}L_{i})}(E_{4})=A_{(Y,c\sum a_{i}L_{i})}(E_{5})=1-288c<0

when 1288<c<1240\frac{1}{288}<c<\frac{1}{240}. Thus there is a wall 0<c<12880<c<\frac{1}{288} given by the degeneration of such pairs.

5.2. Degree one del Pezzo with two D4D_{4}-singularities

Proposition 5.3.

Let ZZ be a del Pezzo surface of degree one with exactly two D4D_{4}-singularities, and LiL_{i}’s be the degeneration of the 240 lines. Then the pair (Z,cLi)(Z,c\sum L_{i}) is K-stable for any 0<c<12400<c<\frac{1}{240}.

Proof.

Let ZZ be a degree one del Pezzo surface with exactly D4D_{4}-singularities. Such surfaces are weighted hypersurfaces in (1,1,2,3)\mathbb{P}(1,1,2,3) and there is a one-parameter family paramaterizing them (cf. [OSS16, Example 5.19]). For us, a description by blowing up projective plane is more useful, since we need to figure out the degeneration of the 240 lines.

We see that ZZ can be obtained by blowing up 2\mathbb{P}^{2} in the following way. Fix four distinct points p1,p2,p3,p4p_{1},p_{2},p_{3},p_{4} on a line LL in 2\mathbb{P}^{2}, and another point p2Lp\in\mathbb{P}^{2}\setminus L. Blow up 2\mathbb{P}^{2} at p1p_{1} along the tangent direction to pp with exceptional divisors E1,F1E_{1},F_{1}; at p2p_{2} along the tangent direction to pp with exceptional divisors E2,F2E_{2},F_{2}; and at the point p3p_{3} with exceptional divisors EE. Finally blow up the length 33 0-dimensional curvilinear subscheme supported on the line pp4¯\overline{pp_{4}} and concentrated at pp with exceptional divisors E3,F3,G3E_{3},F_{3},G_{3} (see Figure 1 for the blow-up procedure and Figure 2 for the configuration of the (-1)-curves and (-2)-curves on Z~\widetilde{Z}). Denote this surface by Z~\widetilde{Z}, and the ample model by ZZ.

Refer to caption
Figure 1. Blow-up of 2\mathbb{P}^{2} to get Z~\widetilde{Z}
Refer to caption
Figure 2. Configuration of the lines on Z~\widetilde{Z}

Let HH be the class of the pull-back of 𝒪2(1)\mathcal{O}_{\mathbb{P}^{2}}(1). Then the proper transform to Z~\widetilde{Z} of the 240 lines on ZZ are of the following types:

  1. (a)

    EE, of multiplicity 24;

  2. (b)

    HEE3F3G3H-E-E_{3}-F_{3}-G_{3}, of multiplicity 24;

  3. (c)

    F1F_{1}, of multiplicity 64;

  4. (d)

    F2F_{2}, of multiplicity 64;

  5. (e)

    G3G_{3}, of multiplicity 64.

Notice that the configurations of the curves in Figure 2 is symmetric: the black curves denote the (-2)-curves and the red lines denote the (-1)-curves. Using the same computation as in Section 5.1, one sees that the minimal log discrepancy of the pair (Z,caiLi)(Z,c\sum a_{i}L_{i}) is 1240c>01-240c>0, when 0<c<12400<c<\frac{1}{240}. Thus the surfaces with exactly two D4D_{4}-singularities do not contribute any wall.

Remark 5.4.

Notice that the four points p1,,p4p_{1},...,p_{4} on 1\mathbb{P}^{1} have a cross-ratio. This also explains why we have a one-dimensional family of surfaces with exactly two D4D_{4}-singularities.

5.3. Degree one del Pezzo with an A8A_{8}-singularity two 19(1,2)\frac{1}{9}(1,2)-singularities

Among all K-polystable degeneration of smooth degree 1 del Pezzo surface, there is a special one XX_{\infty} with an A8A_{8}-singularity and two 19(1,2)\frac{1}{9}(1,2)-singularities. The surface XX_{\infty} can be viewed as a degree 1818 hypersurface in (1,2,9,9)\mathbb{P}(1,2,9,9) given by the equation z3z4=z29z_{3}z_{4}=z_{2}^{9}, where (z1:z2:z3:z4)(z_{1}:z_{2}:z_{3}:z_{4}) is the coordinates of weights 1,2,9,91,2,9,9 respectively. Moreover, projecting to (1,2,9)\mathbb{P}(1,2,9) by

(z1:z2:z3:z4)(z1:z2:z3+z4)(z_{1}:z_{2}:z_{3}:z_{4})\mapsto(z_{1}:z_{2}:z_{3}+z_{4})

realizes XX_{\infty} as a double cover of (1,2,9)\mathbb{P}(1,2,9) branched along the curve C={v9=w2}C_{\infty}=\{v^{9}=w^{2}\}, where (u:v:w)(u:v:w) is the coordinate of (1,2,9)\mathbb{P}(1,2,9). In fact, this double cover map is given by the linear system |2KX||-2K_{X_{\infty}}|.

Recall that for a smooth del Pezzo surface XtX_{t} of degree one, the map given by the linear system |2KXt||-2K_{X_{t}}| is a double cover to (1,1,2)3\mathbb{P}(1,1,2)\subseteq\mathbb{P}^{3} branched along a sextic curve CtC_{t}. The 240 lines on XtX_{t} are sent pairwise to the 120 conics on (1,1,2)\mathbb{P}(1,1,2) obtained by intersecting the (1,1,2)\mathbb{P}(1,1,2) with the 120 tritangent planes of CtC_{t} in 3\mathbb{P}^{3}. See [KRSNS18] for details.

The degeneration of (1,1,2)\mathbb{P}(1,1,2) to (1,2,9)\mathbb{P}(1,2,9) can be observed in 15\mathbb{P}^{15}: they are embedded into 15\mathbb{P}^{15} by the complete linear series |𝒪(6)||\mathcal{O}(6)| and |𝒪(18)||\mathcal{O}(18)|, respectively. In particular, the 120 conics degenerate to curves in (1,2,9)\mathbb{P}(1,2,9) of degree 6. Notice that the pair ((1,2,9),12C)(\mathbb{P}(1,2,9),\frac{1}{2}C_{\infty}) is a 𝕋\mathbb{T}-variety of complexity one: there is a 𝔾m\mathbb{G}_{m}-action given by

λ(u:v:w)=(u:λ2v:λ9w).\lambda\cdot(u:v:w)=(u:\lambda^{2}v:\lambda^{9}w).

In particular, each of the 120 sextic curves is 𝔾m\mathbb{G}_{m}-invariant, and hence is defined by one of the following four equations:

u6=0,u4v=0,u2v2=0,v3=0.u^{6}=0,\quad u^{4}v=0,\quad u^{2}v^{2}=0,\quad v^{3}=0.

However, the multiplicity of them is not clear to us. We have the following partial result.

Proposition 5.5.

Let XX_{\infty} be the degree 1 del Pezzo surface as above, and LiL_{i}’s be the 240 lines on it counted with multiplicities. Then the pair (X,cLi)(X_{\infty},c\sum L_{i}) is either K-polystable for any 0<c<12400<c<\frac{1}{240} or K-unstable for any 0<c<12400<c<\frac{1}{240}. Moreover, it is K-polystable if and only if

ordu=0(lj)=240andordu=0(lj)=240,\operatorname{ord}_{u=0}\left(\sum l_{j}\right)=240\quad\textup{and}\quad\operatorname{ord}_{u=0}\left(\sum l_{j}\right)=240,

where lil_{i}’s are the 120 sextic curves in (1,2,9)\mathbb{P}(1,2,9) given by the images of LiL_{i}’s.

Proof.

The main tool here we use is equivariant K-stability (cf. [Zhu21]). Assume we are in the case when ordu=0(lj)=240\operatorname{ord}_{u=0}\left(\sum l_{j}\right)=240 and ordu=0(lj)=240\operatorname{ord}_{u=0}\left(\sum l_{j}\right)=240. By [LZ22, Theorem 1.2], it suffices to check the K-stability of the pair ((1,2,9),12C+cli)(\mathbb{P}(1,2,9),\frac{1}{2}C_{\infty}+c\sum l_{i}), which is a 𝕋\mathbb{T}-pair of complexity one. By [ACC+21, Theorem 1.3.9], we only need to compute the β\beta-invariant of the pair with respect to all 𝔾m\mathbb{G}_{m}-invariant divisors on (1,2,9)\mathbb{P}(1,2,9) (see also [Zha22, Theorem 2.9] for the statement for pairs). The divisor {u=0}\{u=0\} is the unique horizontal divisor on XX_{\infty}. We have that

A((1,2,9),12C+cli)({u=0})=1240cA_{(\mathbb{P}(1,2,9),\frac{1}{2}C_{\infty}+c\sum l_{i})}(\{u=0\})=1-240c

and that

S((1,2,9),12C+cli)({u=0})=(3720c)𝒪(1)201𝒪(1t)2𝑑t=1240c,S_{(\mathbb{P}(1,2,9),\frac{1}{2}C_{\infty}+c\sum l_{i})}(\{u=0\})=\frac{(3-720c)}{\mathcal{O}(1)^{2}}\int_{0}^{1}\mathcal{O}(1-t)^{2}dt=1-240c,

and thus β((1,2,9),12C+cli)({u=0})=0\beta_{(\mathbb{P}(1,2,9),\frac{1}{2}C_{\infty}+c\sum l_{i})}(\{u=0\})=0. For the vertical divisor {v=0}\{v=0\} we have that

A((1,2,9),12C+cli)({v=0})=1240cA_{(\mathbb{P}(1,2,9),\frac{1}{2}C_{\infty}+c\sum l_{i})}(\{v=0\})=1-240c

and that

S((1,2,9),12C+cli)({v=0})=(3720c)𝒪(1)2012𝒪(12t)2𝑑t=12(1240c).S_{(\mathbb{P}(1,2,9),\frac{1}{2}C_{\infty}+c\sum l_{i})}(\{v=0\})=\frac{(3-720c)}{\mathcal{O}(1)^{2}}\int_{0}^{\frac{1}{2}}\mathcal{O}(1-2t)^{2}dt=\frac{1}{2}(1-240c).

For other vertical divisors Dt={v9=tw2}D_{t}=\{v^{9}=tw^{2}\} with λ\lambda\in\mathbb{C}^{*}, similarly, we have that that β((1,2,9),12C+cli)(Dt)>0\beta_{(\mathbb{P}(1,2,9),\frac{1}{2}C_{\infty}+c\sum l_{i})}(D_{t})>0. This conclude for the case ordu=0(lj)=ordu=0(lj)=240\operatorname{ord}_{u=0}\left(\sum l_{j}\right)=\operatorname{ord}_{u=0}\left(\sum l_{j}\right)=240. For the other case, the β\beta-invariant for the horizontal divisor {u=0}\{u=0\} is non-zero when 0<c<12400<c<\frac{1}{240} so the pair is K-unstable.

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