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Gaps in the support of canonical currents on projective K3 surfaces

Simion Filip Department of Mathematics University of Chicago 5734 S University Ave Chicago, IL 60637 [email protected]  and  Valentino Tosatti Courant Institute of Mathematical Sciences New York University 251 Mercer St New York, NY 10012 [email protected]
(Date: January 2023)
Abstract.

We construct examples of canonical closed positive currents on projective K3 surfaces that are not fully supported on the complex points. The currents are the unique positive representatives in their cohomology classes and have vanishing self-intersection. The only previously known such examples were due to McMullen on non-projective K3 surfaces and were constructed using positive entropy automorphisms with a Siegel disk. Our construction is based on a Zassenhaus-type estimate for commutators of automorphisms.

Revised

1. Introduction

Let XX be a complex projective K3K3 surface and let T:XXT\colon X\to X be an automorphism with positive topological entropy h>0h>0. Thanks to a foundational result of Cantat [Can01], there are closed positive currents η±\eta_{\pm} which satisfy

Tη±=e±hη±,T^{*}\eta_{\pm}=e^{\pm h}\eta_{\pm},

and are normalized so that their cohomology classes satisfy [η+][η]=1[\eta_{+}]\cdot[\eta_{-}]=1. The classes [η±][\eta_{\pm}] belong to the boundary of the ample cone of XX and have vanishing self-intersection. These eigencurrents have Hölder continuous local potentials [DS05], and their wedge product μ=η+η\mu=\eta_{+}\wedge\eta_{-} is well-defined by Bedford–Taylor theory, and is the unique TT-invariant probability measure with maximal entropy.

When (X,T)(X,T) is not a Kummer example, it was shown by Cantat–Dupont [CD20] (with a new proof by the authors [FT21] that also covers the nonprojective case) that μ\mu is singular with respect to the Lebesgue measure dVol\operatorname{{dVol}}; therefore there exists a Borel set of zero Lebesgue measure carrying the entire mass of μ\mu. The authors conjectured (see [Tos21, Conjecture 7.3]) that the topological support suppμ\operatorname{{supp}}\mu should nonetheless be equal to all of XX, see also Cantat’s [Can18, Question 3.4]. If this were true, it would also imply the same for each of the currents: suppη±=X\operatorname{{supp}}\eta_{\pm}=X.

In [FT23] the authors showed that, under mild assumptions on XX, the eigencurrents η±\eta_{\pm} fit into a continuous family of closed positive currents with continuous local potentials whose cohomology classes sweep out the boundary of the ample cone, perhaps after blowing up the boundary at the rational rays. We called the corresponding closed positive currents the canonical currents. It is then natural to wonder whether all such canonical currents are fully supported on XX.

In this note we show that this is in fact not the case. Namely, we show in Theorem 2.3.5 below:

Theorem 1 (Gaps in the support).

There exists a projective K3 surface XX of type (2,2,2)(2,2,2), and an uncountable dense FσF_{\sigma} set of rays FAmp(X)F\subset\partial\operatorname{{Amp}}(X) in the boundary of its ample cone, such that for every fFf\in F the topological support of the unique canonical current ηf\eta_{f} is not all of XX.

Note that because the rank of the Picard group of a very general K3 surface of type (2,2,2)(2,2,2) is 33, there is no need to blow up the rational directions on the boundary. Moreover, the canonical currents in the rational directions (i.e. those where the ray spanned by ff intersects H2(X,)H^{2}(X,\mathbb{Q}) nontrivially) have full support, see § 2.3.4.

The above result can be strengthened to show that there exist K3 surfaces defined over \mathbb{R}, such that the supports of certain canonical currents are disjoint from the (nonempty) real locus (see Theorem 2.4.2):

Theorem 2 (Full gaps in the real locus).

There exists a projective K3 surface XX of type (2,2,2)(2,2,2) defied over \mathbb{R} with X()X(\mathbb{R})\neq\emptyset, and an uncountable dense FσF_{\sigma} set of rays FAmp(X)F\subset\partial\operatorname{{Amp}}(X) in the boundary of its ample cone, such that for every fFf\in F the topological support of the unique canonical current ηf\eta_{f} is disjoint from X()X(\mathbb{R}).

In the examples we construct, X()X(\mathbb{R}) is homeomorphic to a 22-sphere.

McMullen [McM02, Thm. 1.1] constructed nonprojective K3 surfaces with automorphisms whose eigencurrents η±\eta_{\pm} are not fully supported. In fact, his examples have a Siegel disc: an invariant neighborhood of a fixed point on which the dynamics is holomorphically conjugate to a rotation, and where η±\eta_{\pm} thus vanish. Let us also note that Moncet [Mon13, Thm. A] constructed a birational automorphism of a rational surface XX defined over \mathbb{R}, with positive dynamical degree and Fatou set containing X()X(\mathbb{R}).

Despite our Theorem 1 above, we do maintain hope that on projective K3 surfaces, the measure of maximal entropy (and therefore also η±\eta_{\pm}) is fully supported.

Acknowledgments

We are grateful to Roland Roeder for conversations on his work with Rebelo [RR21] that inspired this note, to Serge Cantat for detailed feedback that improved our exposition, and to the referee for useful comments. We are also grateful to Serge Cantat for suggesting to combine our methods with an example of Moncet that led to Theorem 2.

This research was partially conducted during the period the first-named author served as a Clay Research Fellow, and during the second-named author’s visit to the Center for Mathematical Sciences and Applications at Harvard University, which he would like to thank for the hospitality. This note is dedicated to the memory of Nessim Sibony, a dear colleague and friend, whose contributions to holomorphic dynamics and several complex variables remain an inspiration to us. He is greatly missed.

2. Gaps in the support of canonical currents

Outline

We recall some constructions and estimates, originally based on an idea of Ghys [Ghy93], itself inspired by the Zassenhaus lemma on commutators of small elements in Lie groups. In brief, the idea is that if two germs of holomorphic maps near the origin are close to the identity, then their commutator is even closer, and the estimates are strong enough to allow for an iteration argument.

The precise estimates that we need for Theorem 1 are contained in § 2.1.3, and we follow Rebelo–Roeder [RR21] to establish the needed bounds. We then recall some basic facts concerning the geometry of K3 surfaces in § 2.2, and establish the existence of gaps in the support of some of their canonical currents in § 2.3.

2.1. Commutator estimates

In this section we introduce notation and collect some results, stated and proved by Rebelo–Roeder [RR21] but which have also been known and used in earlier contexts, e.g. by Ghys [Ghy93]. The results are concerned with commutators of germs of holomorphic maps in a neighborhood of 0d0\in\mathbb{C}^{d}.

2.1.1. Derived series and commutators

Fix a set SS, whose elements we regard as formal symbols which can be juxtaposed to form words. Assume that SS is equipped with a fixed-point-free involution ss1s\mapsto s^{-1}, i.e. any element has a unique corresponding “inverse” in the set. Define the “derived series” of sets by

S(0):=SS(n+1):=[S(n),S(n)]S^{(0)}:=S\quad S^{(n+1)}:=\left[S^{(n)},S^{(n)}\right]

where [A,B][A,B] denotes the set of commutators [a,b]:=aba1b1[a,b]:=aba^{-1}b^{-1} with aA,bBa\in A,b\in B, and we omit the trivial commutators [a,a1][a,a^{-1}]. Denote the disjoint union by S:=n0S(n)S^{\bullet}:=\coprod_{n\geq 0}S^{(n)}. We will use the same notation in the case of a pseudogroup. We also collect the next elementary result:

2.1.2 Proposition (Fast ramification).

Let FkF_{k} denote the free group on kk generators a1,,aka_{1},\ldots,a_{k}. Set S(0):={a1,,ak,a11,,ak1}S^{(0)}:=\{a_{1},\ldots,a_{k},a_{1}^{-1},\ldots,a_{k}^{-1}\}.

Then the (k2){\binom{k}{2}} elements [ai,aj]S(1)[a_{i},a_{j}]\in S^{(1)} with i<ji<j, generate a free subgroup of rank (k2)\binom{k}{2} inside FkF_{k}.

Proof.

Observe that [ai,aj]1=[aj,ai][a_{i},a_{j}]^{-1}=[a_{j},a_{i}]. Therefore, it suffices to check that any word of the form

[ai1,aj1][ail,ajl][aiN,ajN][a_{i_{1}},a_{j_{1}}]\cdots[a_{i_{l}},a_{j_{l}}]\cdots[a_{i_{N}},a_{j_{N}}]

is never trivial, subject to the condition that no commutator is followed by its inverse. Explicitly, we assume that for any ll either ailajl+1a_{i_{l}}\neq a_{j_{l+1}} or ajlail+1a_{j_{l}}\neq a_{i_{l+1}}.

To proceed, we write out the expression in the generators aa_{\bullet}. Observe that a cancellation can only occur if ajl=ail+1a_{j_{l}}=a_{i_{l+1}} for some ll. However, subsequent cancellations are excluded by assumption so the reduced word has at least 4N2(N1)=2N+24N-2(N-1)=2N+2 letters and is nonempty. ∎

Later on, we will apply iteratively this proposition, starting with k4k\geq 4, an inequality which is preserved by k(k2)k\mapsto{\binom{k}{2}}.

2.1.3. Pseudogroup of transformations

Let B0(ε)dB_{0}(\varepsilon)\subset\mathbb{C}^{d} denote the ball of radius ε>0\varepsilon>0 centered at the origin in d\mathbb{C}^{d}. Let γ1,,γk\gamma_{1},\ldots,\gamma_{k} be injective holomorphic maps γi:B0(ε)d\gamma_{i}\colon B_{0}(\varepsilon)\to\mathbb{C}^{d}, which are thus biholomorphisms onto their ranges γi:=γi(B0(ε))\mathcal{R}_{\gamma_{i}}:=\gamma_{i}(B_{0}(\varepsilon)).

Let SS denote the set with 2k2k symbols γ1,,γk,γ11,,γk1\gamma_{1},\ldots,\gamma_{k},\gamma_{1}^{-1},\ldots,\gamma_{k}^{-1}. With SS^{\bullet} as in § 2.1.1, assign to any element γS\gamma\in S^{\bullet}, whenever possible, the holomorphic map also denoted by γ:𝒟γγ\gamma\colon\mathcal{D}_{\gamma}\to\mathcal{R}_{\gamma} with open sets 𝒟γ,γd\mathcal{D}_{\gamma},\mathcal{R}_{\gamma}\subset\mathbb{C}^{d} by expressing γ\gamma in reduced form in the letters from SS, and shrinking the domains/ranges according to the word. For certain elements γ\gamma, these might well be empty sets.

Denote by 𝟏{\bm{1}} the identity transformation and by fC0(K)\left\|f\right\|_{C^{0}(K)} the supremum norm of a function or map ff on a set KK.

2.1.4 Theorem (Common domain of definition).

For any given 0<ε10<\varepsilon\leq 1, if

γi±1𝟏C0(B0(ε))ε32, for i=1,,k\left\|\gamma_{i}^{\pm 1}-{\bm{1}}\right\|_{C^{0}(B_{0}(\varepsilon))}\leq\frac{\varepsilon}{32},\text{ for }i=1,\ldots,k

then for every n0n\geq 0 and every γS(n)\gamma\in S^{(n)}, its domain 𝒟γ\mathcal{D}_{\gamma} contains B0(ε/2)B_{0}(\varepsilon/2) and furthermore it satisfies

γ𝟏C0(B0(ε/2))ε2n32.\left\|\gamma-{\bm{1}}\right\|_{C^{0}(B_{0}(\varepsilon/2))}\leq\frac{\varepsilon}{2^{n}\cdot 32}.

This result is proved as in [RR21, Prop. 7.1] or [RR17, Prop. 3.1], which state it for k=2k=2. Indeed, the estimates in the proof only involve the estimates on the “seed” transformations γi\gamma_{i}, and not their cardinality. We include the proof for the reader’s convenience.

Note also that without further assumptions on the γi\gamma_{i}, it could happen that S(n)S^{(n)} contains only identity mappings. In our intended applications, this will be excluded as the elements will act nontrivially in cohomology.

Proof.

We will show by induction on n0n\geq 0 that for every γS(n)\gamma\in S^{(n)} its domain 𝒟γ\mathcal{D}_{\gamma} contains B0(εn)B_{0}(\varepsilon_{n}) where

εn:=εε4j=0n12jε2,\varepsilon_{n}:=\varepsilon-\frac{\varepsilon}{4}\sum_{j=0}^{n-1}2^{-j}\geq\frac{\varepsilon}{2},

and that

γ𝟏C0(B0(εn))ε2n32.\left\|\gamma-{\bm{1}}\right\|_{C^{0}(B_{0}(\varepsilon_{n}))}\leq\frac{\varepsilon}{2^{n}\cdot 32}.

The base case n=0n=0 is obvious, and for the induction step the key result that we need is the following improvement [LR03, Lemma 3.0] of a result of Ghys [Ghy93, Prop. 2.1]: given constants 0<r,δ,τ<10<r,\delta,\tau<1 with 4δ+τ<r4\delta+\tau<r, if f,g:B0(r)df,g:B_{0}(r)\to\mathbb{C}^{d} are two injective holomorphic maps which satisfy

(2.1.5) f𝟏C0(B0(r))δ,g𝟏C0(B0(r))δ,\|f-{\bm{1}}\|_{C^{0}(B_{0}(r))}\leq\delta,\quad\|g-{\bm{1}}\|_{C^{0}(B_{0}(r))}\leq\delta,

then their commutator [f,g][f,g] is defined on B0(r4δτ)B_{0}(r-4\delta-\tau) and satisfies

(2.1.6) [f,g]𝟏C0(B0(r4δτ))2τf𝟏C0(B0(r))g𝟏C0(B0(r)).\|[f,g]-{\bm{1}}\|_{C^{0}(B_{0}(r-4\delta-\tau))}\leq\frac{2}{\tau}\|f-{\bm{1}}\|_{C^{0}(B_{0}(r))}\|g-{\bm{1}}\|_{C^{0}(B_{0}(r))}.

We use this to prove the case n+1n+1 of the induction by taking

r:=εn,δ:=ε2n32,τ:=ε2n8,r:=\varepsilon_{n},\quad\delta:=\frac{\varepsilon}{2^{n}\cdot 32},\quad\tau:=\frac{\varepsilon}{2^{n}\cdot 8},

and applying it to two arbitrary f,gS(n)f,g\in S^{(n)}. These satisfy (2.1.5) by induction hypothesis, and so [f,g][f,g] is defined on the ball centered at the origin of radius

εn4ε2n32ε2n8=εn+1,\varepsilon_{n}-4\frac{\varepsilon}{2^{n}\cdot 32}-\frac{\varepsilon}{2^{n}\cdot 8}=\varepsilon_{n+1},

and by (2.1.6) it satisfies

[f,g]𝟏C0(B0(εn+1))2τδ2=δ2=ε2n+132,\|[f,g]-{\bm{1}}\|_{C^{0}(B_{0}(\varepsilon_{n+1}))}\leq\frac{2}{\tau}\delta^{2}=\frac{\delta}{2}=\frac{\varepsilon}{2^{n+1}\cdot 32},

as desired. ∎

The next result, appearing in [RR21, Lemma 7.2], will be useful in exhibiting explicit examples satisfying the assumptions of Theorem 2.1.4. We will denote by 𝟏{\bm{1}} both the identity map and the identity matrix acting on d\mathbb{C}^{d}, and by Mat\left\|-\right\|_{\rm Mat} the matrix norm on n×nn\times n matrices.

2.1.7 Proposition (Fixed points with small derivative).

For any 0<ε010<\varepsilon_{0}\leq 1 and holomorphic map γ:B0(ε0)d\gamma:B_{0}(\varepsilon_{0})\to\mathbb{C}^{d} satisfying

γ(0)=0 and Dγ(0)𝟏Mat164,\gamma(0)=0\text{ and }\left\|D\gamma(0)-{\bm{1}}\right\|_{\rm Mat}\leq\frac{1}{64},

there exists ε1>0\varepsilon_{1}>0, depending on γ\gamma, with the following property. For any ε(0,ε1)\varepsilon\in(0,\varepsilon_{1}), the map restricted to B0(ε)B_{0}(\varepsilon) satisfies

(2.1.8) γ𝟏C0(B0(ε))ε32.\left\|\gamma-{\bm{1}}\right\|_{C^{0}(B_{0}(\varepsilon))}\leq\frac{\varepsilon}{32}.
Proof.

For 0<ε<ε10<\varepsilon<\varepsilon_{1} (where ε1\varepsilon_{1} is to be determined), let Λε(z1,,zn)=(εz1,,εzn)\Lambda_{\varepsilon}(z_{1},\dots,z_{n})=(\varepsilon z_{1},\dots,\varepsilon z_{n}) be the scaling map, and let γε:=Λε1γΛε\gamma_{\varepsilon}:=\Lambda_{\varepsilon}^{-1}\circ\gamma\circ\Lambda_{\varepsilon}. This is a holomorphic map on B0(1)B_{0}(1) that satisfies

γε(0)=0 and Dγε(0)𝟏Mat164.\gamma_{\varepsilon}(0)=0\text{ and }\left\|D\gamma_{\varepsilon}(0)-{\bm{1}}\right\|_{\rm Mat}\leq\frac{1}{64}.

An application of the Taylor formula gives

γε𝟏C0(B0(1))Dγε(0)𝟏Mat+Cγε164+Cγε,\left\|\gamma_{\varepsilon}-{\bm{1}}\right\|_{C^{0}(B_{0}(1))}\leq\left\|D\gamma_{\varepsilon}(0)-{\bm{1}}\right\|_{\rm Mat}+C_{\gamma}\varepsilon\leq\frac{1}{64}+C_{\gamma}\varepsilon,

for some constant CγC_{\gamma} that depends on the size of the Hessian of γ\gamma. Thus, it suffices to choose ε1=164Cγ,\varepsilon_{1}=\frac{1}{64C_{\gamma}}, and we have

γε𝟏C0(B0(1))132,\left\|\gamma_{\varepsilon}-{\bm{1}}\right\|_{C^{0}(B_{0}(1))}\leq\frac{1}{32},

which is equivalent to (2.1.8). ∎

2.2. (2,2,2)(2,2,2)-surfaces and canonical currents

For basic background on K3 surfaces, see [BBD85, Huy16] and, for an introduction to complex automorphisms of K3 surfaces see [Fil23]. Our main examples, the (2,2,2)(2,2,2)-surfaces, were first noted by Wehler [Weh88].

2.2.1. Setup

We work over the complex numbers. Consider the 33-fold (1)3(\mathbb{P}^{1})^{3}, with its family of smooth anticanonical divisors given by degree (2,2,2)(2,2,2)-surfaces, i.e. let 𝒰27\mathcal{U}\subset\mathbb{C}^{27} denote the parameter space of coefficients of an equation

0i,j,k2cijkxiyjzk=0 in (𝔸1)3\sum_{0\leq i,j,k\leq 2}c_{ijk}x^{i}y^{j}z^{k}=0\quad\text{ in }(\mathbb{A}^{1})^{3}

that yield smooth surfaces when compactified in (1)3(\mathbb{P}^{1})^{3}. We will call these (2,2,2)(2,2,2)-surfaces. We consider for simplicity the full set of equations, without identifying surfaces equivalent under the action of (𝐏𝐆𝐋2)3(\operatorname{\mathbf{PGL}}_{2})^{3}.

2.2.2 Definition (Strict (2,2,2)(2,2,2) example).

We will say that a (2,2,2)(2,2,2)-surface is strict if the rank of its Néron–Severi group (over \mathbb{C}) is the minimal possible, i.e. 33.

Note that an at most countable dense union of codimension-one subsets in 𝒰\mathcal{U} consists of non-strict (2,2,2)(2,2,2)-surfaces. For strict (2,2,2)(2,2,2)-surfaces, the Néron–Severi group equipped with its intersection form is isometric to 1,2\mathbb{R}^{1,2} (after extension of scalars to \mathbb{R}).

2.2.3. Some recollections from topology

Recall that FσF_{\sigma}-sets are countable unions of closed sets, while GδG_{\delta}-sets are countable intersections of open ones. It follows from standard results in the moduli theory of K3 surfaces that strict (2,2,2)(2,2,2)-surfaces form a dense GδG_{\delta}-set in 𝒰\mathcal{U}, which in fact has full Lebesgue measure. Indeed, parameters giving strict (2,2,2)(2,2,2)-surfaces are the complement of countably many divisors in the full parameter space, see e.g. [Ogu03].

2.2.4. Involutions

For any u𝒰u\in\mathcal{U}, denote the associated surface by Xu(1)3X_{u}\subset(\mathbb{P}^{1})^{3}. The projection onto one of the coordinate planes Xu(1)2X_{u}\to(\mathbb{P}^{1})^{2} is two-to-one and so XuX_{u} admits an involution exchanging the two sheets. Denote by σx,σy,σz\sigma_{x},\sigma_{y},\sigma_{z} the three involutions obtained in this manner.

2.2.5. Canonical currents

We can apply [FT23, Thm. 1] to any strict (2,2,2)(2,2,2)-surface XuX_{u} with u𝒰u\in\mathcal{U}. In that theorem a certain space Ampc(Xu)\partial^{\circ}\operatorname{{Amp}}_{c}(X_{u}) appears, which on strict (2,2,2)(2,2,2)-surfaces reduces to the boundary of the ample cone Amp(Xu)\partial\operatorname{{Amp}}(X_{u}), so it consists of nef cohomology classes [η]NS(Xu)H1,1(Xu)[\eta]\in\operatorname{{NS}}_{\mathbb{R}}(X_{u})\subset H^{1,1}(X_{u}) satisfying [η]2=0[\eta]^{2}=0. Since NS(Xu)\operatorname{{NS}}_{\mathbb{R}}(X_{u}) equipped with the intersection pairing is isometric to 1,2\mathbb{R}^{1,2}, the space Amp(Xu)\partial\operatorname{{Amp}}(X_{u}) is isomorphic to one component of the null-cone in this Minkowski space. Note that in the general form of the result, one needs to replace the rational rays in Amp(Xu)\partial\operatorname{{Amp}}(X_{u}) by their blowups; since in the case of a rank 33 Néron–Severi group it would mean blowing up rays on a surface, no extra points need to be added.

Next, [FT23, Thm. 1] shows that each cohomology class [η]Amp(Xu)[\eta]\in\partial\operatorname{{Amp}}(X_{u}) has a canonical positive representative η\eta, which additionally has C0C^{0} potentials. The representative is unique when the class is irrational, and a preferred representative in the rational (also called parabolic) classes exists that makes the entire family of currents continuous in the C0C^{0}-topology of the potentials for the currents.

We will show in Theorem 2.3.5 below that some of the canonical representatives do not have full support in XuX_{u}. Specifically, we will show that there exists an open set 𝒰0𝒰\mathcal{U}_{0}\subset\mathcal{U} and a dense GδG_{\delta} set of u𝒰0u\in\mathcal{U}_{0} for which some of the canonical currents η\eta do not have full support in XuX_{u}.

But first, we will show that the set of cohomology classes [η][\eta] for which the gaps in the support are constructed contain, after projectivization, a closed uncountable set.

2.2.6. Free subgroups of automorphisms

We will consider subgroups of automorphisms of XuX_{u} freely generated by five elements. Specifically, σx,σy,σz\sigma_{x},\sigma_{y},\sigma_{z} generate a group ΓσAut(Xu)\Gamma_{\sigma}\subseteq\operatorname{{Aut}}(X_{u}) isomorphic to (/2)(/2)(/2)\left(\mathbb{Z}/2\right)*\left(\mathbb{Z}/2\right)*\left(\mathbb{Z}/2\right), in other words there are no relations between them except that σi2=𝟏\sigma_{i}^{2}={\bm{1}} for i=x,y,zi=x,y,z. This can be verified by considering the action on the hyperbolic space inside the Néron–Severi group of XuX_{u} (see for instance [Fil19, Prop.6.1] for the explicit matrices corresponding to the action in the upper half-space model).

2.2.7 Proposition (Free group on five generators).

Consider the surjective homomorphism Γσ(/2)3\Gamma_{\sigma}\twoheadrightarrow(\mathbb{Z}/2)^{\oplus 3} sending σx,σy,σz\sigma_{x},\sigma_{y},\sigma_{z} to (1,0,0),(0,1,0),(0,0,1)(1,0,0),(0,1,0),(0,0,1) respectively.

Then its kernel KσK_{\sigma} is a free group on five generators.

The above homomorphism corresponds to evaluating the derivatives of the transformations at the common fixed point of the transformations described in § 2.3.4. § 2.2.6 will provide us with a free group with five generators, each of whose derivative at the fixed point is the identity.

Proof.

We will divide our analysis by looking at the homomorphisms Γσ(/2)3/2\Gamma_{\sigma}\twoheadrightarrow(\mathbb{Z}/2)^{\oplus 3}\twoheadrightarrow\mathbb{Z}/2 where the last map sends each generator of a summand to the unique nonzero element.

Now the kernel of Γσ/2\Gamma_{\sigma}\twoheadrightarrow\mathbb{Z}/2 sending each σi\sigma_{i} to 1/21\in\mathbb{Z}/2 is the free group on two letters, generated by a:=σxσya:=\sigma_{x}\sigma_{y} and b:=σyσzb:=\sigma_{y}\sigma_{z}. Indeed this kernel is the fundamental group of the Riemann sphere with 33 points removed. This assertion follows by considering the action of Γσ\Gamma_{\sigma} on the hyperbolic plane by reflection in the sides of a geodesic triangle with vertices at infinity. The quotient surface is an orbifold triangle, while the quotient by KσK_{\sigma} corresponds to gluing two copies of the triangle along geodesic sides, to obtain a triply-punctured sphere.

Now KσK_{\sigma} is contained with finite index in the free group on a,ba,b, and is visibly given as the kernel of the surjection onto (/2)2(\mathbb{Z}/2)^{\oplus 2} sending a(1,0)a\mapsto(1,0) and b(0,1)b\mapsto(0,1). One can then work out the associated covering space and rank of free group, using the techniques in [Hat02, §1.A], and determine that KσK_{\sigma} is a free group on 55 generators.

Alternatively, the corresponding (/2)2(\mathbb{Z}/2)^{\oplus 2}-covering space of the triply punctured Riemann sphere can be visualized as a square-shaped “pillowcase” with four punctures at the corners, and two additional punctures in the center of the two faces. The involutive automorphisms are rotations by 180180^{\circ} through an axis that goes across two opposite punctures. ∎

2.2.8. Largeness of the set currents with gaps

To continue, we select γ1,γ2,γ3,γ4,γ5Kσ\gamma_{1},\gamma_{2},\gamma_{3},\gamma_{4},\gamma_{5}\subset K_{\sigma} to be five elements freely generating the group. Next, the construction of § 2.1.1 applies with S:={γ1,,γ5,γ11,γ51}S:=\{\gamma_{1},\ldots,\gamma_{5},\gamma_{1}^{-1},\ldots\gamma_{5}^{-1}\} and yields a subset SAut(Xu)S^{\bullet}\subset\operatorname{{Aut}}(X_{u}) consisting of iterated commutators. Fix a Kähler metric ω0\omega_{0} on XuX_{u}, with volume normalized to [ω0]2=1[\omega_{0}]^{2}=1, and let 2(Xu)\mathbb{H}^{2}(X_{u}) denote the hyperbolic plane of all nef cohomology classes satisfying [ω]2=1[\omega]^{2}=1.

2.2.9 Proposition (Uncountably many currents with gaps).

The intersection of the closure of the set S[ω0]2(Xu)S^{\bullet}\cdot[\omega_{0}]\subset\mathbb{H}^{2}(X_{u}) with the boundary 2(Xu)\partial\mathbb{H}^{2}(X_{u}) is an uncountable closed set.

Proof.

That the set is closed follows from its definition.

To show that the set is uncountable, we will argue on the boundary of the free group on the five initial generators, and use that the natural map from the boundary of the free group to the hyperbolic space is injective, except perhaps at the countably many parabolic points.

For this, let 𝒯\mathcal{T} denote the Cayley graph of the free group on five generators; it is a 1010-valent infinite regular tree. Define the sequence of finite subtrees 𝒯k\mathcal{T}_{k}, where 𝒯0\mathcal{T}_{0} consists of the identity vertex, and 𝒯k+1\mathcal{T}_{k+1} is obtained from 𝒯k\mathcal{T}_{k} by connecting the leaves of 𝒯k\mathcal{T}_{k} with the elements in S(k+1)S^{(k+1)}. From § 2.1.1 it follows that the number of new edges added to the leaves at each step is at least 33. Therefore, the number of infinite paths starting at the origin in 𝒯:=k0𝒯k\mathcal{T}_{\infty}:=\cup_{k\geq 0}\mathcal{T}_{k} is uncountable, and the claim follows. ∎

2.3. An example with slow commutators

2.3.1. Setup

To show that the assumptions of § 2.1.3 are satisfied in practice, we start with an explicit equation:

(2.3.2) (1+x2)(1+y2)(1+z2)+xyz=1\displaystyle(1+x^{2})(1+y^{2})(1+z^{2})+xyz=1

Let us note that Eqn. (missing) 2.3.2 determines a singular (2,2,2)(2,2,2)-surface, with a singularity at the origin 030\in\mathbb{C}^{3}. We will construct an open set 𝒰0\mathcal{U}_{0} of smooth (2,2,2)(2,2,2)-surfaces by taking perturbations of the above equation.

2.3.3. Automorphisms of ambient space

Let u027u_{0}\in\mathbb{C}^{27} denote the point corresponding to the choice of parameters as in Eqn. (missing) 2.3.2, it lies outside 𝒰\mathcal{U} but any analytic neighborhood of u0u_{0} in 27\mathbb{C}^{27} intersects 𝒰\mathcal{U} in a nonempty open set. We have three explicit involutions σu0,x,σu0,y,σu0,z\sigma_{u_{0},x},\sigma_{u_{0},y},\sigma_{u_{0},z}:

σu0,x(x,y,z)=(yz(1+y2)(1+z2)x,y,z)\sigma_{u_{0},x}(x,y,z)=\left(\frac{-yz}{(1+y^{2})(1+z^{2})}-x,y,z\right)

and similarly for σu0,y,σu0,z\sigma_{u_{0},y},\sigma_{u_{0},z}, which we view as holomorphic maps defined in a neighborhood of 030\in\mathbb{C}^{3}.

2.3.4. Fixed point and Derivatives

It is immediate from the explicit formulas that all three involutions preserve the point 030\in\mathbb{C}^{3}. Furthermore, their derivatives at that point are matrices of order two:

Dσu0,x(0,0,0)=[111] and analogously for σu0,y,σu0,z.D\sigma_{u_{0},x}(0,0,0)=\begin{bmatrix}-1&&\\ &1&\\ &&1\end{bmatrix}\text{ and analogously for }\sigma_{u_{0},y},\sigma_{u_{0},z}.

We now consider σu,x,σu,y,σu,z\sigma_{u,x},\sigma_{u,y},\sigma_{u,z} for u27u\in\mathbb{C}^{27} in a sufficiently small neighborhood of u0u_{0}. Then we can regard the σ\sigma’s as holomorphic maps defined in a neighborhood of 030\in\mathbb{C}^{3}, preserving the intersection of XuX_{u} with the fixed neighborhood.

We can now use these observations to establish:

2.3.5 Theorem (Gaps in the support of canonical currents).

There exists a nonempty open set 𝒰0\mathcal{U}_{0} in the analytic topology of smooth (2,2,2)(2,2,2)-surfaces with the following property.

For each strict K3 surface XuX_{u} with u𝒰0u\in\mathcal{U}_{0}, there exists a dense FσF_{\sigma}-set of rays FF on the boundary of the ample cone of XuX_{u} such that for any [η]F[\eta]\in F, the canonical current η\eta provided by [FT23, Thm. 1] is supported on a proper closed subset of XuX_{u}. Furthermore FF determines an uncountable set of rays.

By a “ray” we mean one orbit of the >0\mathbb{R}_{>0}-action by scaling, so that the “set of rays” is the projectivization of Amp(Xu)\partial\operatorname{{Amp}}(X_{u}). It is implicit in the the statement above that the set FF is disjoint from the countably many parabolic rays. This is justified by § 2.3.4 below.

Proof.

We keep the notation as before the statement of the theorem and will consider u𝒰u\in\mathcal{U} in a sufficiently small neighborhood of u0u_{0}.

Consider the subgroup KσAut(X)K_{\sigma}\subset\operatorname{{Aut}}(X) obtained by applying § 2.2.6 to the group generated by the three involutions. At the parameter u0u_{0} all elements in KσK_{\sigma} preserve the point with coordinate (0,0,0)(0,0,0) and have derivative equal to the identity there, see § 2.3.4. Fix now the five free generators γu,iKσ\gamma_{u,i}\in K_{\sigma} with i=1,,5i=1,\ldots,5, as per § 2.2.6. Let S(n)S^{(n)} denote the set of iterated commutators, as per § 2.1.1.

§ 2.2.8 yields for any strict XuX_{u} an uncountable closed set F0Amp(Xu)F_{0}\subset\partial\operatorname{{Amp}}(X_{u}) with the following property. Fixing ω0\omega_{0} a reference Kähler metric on XuX_{u}, for any fF0f\in F_{0} there exists a sequence {sn}\{s_{n}\} of automorphisms of XuX_{u}, with snS(n)s_{n}\in S^{(n)}, and a sequence of positive scalars λn+\lambda_{n}\to+\infty such that

f=limn+1λn(sn)[ω0].f=\lim_{n\to+\infty}\frac{1}{\lambda_{n}}(s_{n})_{*}[\omega_{0}].

Note that λn+\lambda_{n}\to+\infty since the self-intersection of (sn)[ω0](s_{n})_{*}[\omega_{0}] is 11, while the self-intersection of ff is zero. Applying [FT23, Thm. 4.2.2, pts. 4,5] then shows that in the weak sense of currents we have

ηf=limn+1λn(sn)ω0,\eta_{f}=\lim_{n\to+\infty}\frac{1}{\lambda_{n}}(s_{n})_{*}\omega_{0},

where ηf\eta_{f} is a canonical positive representative of the cohomology class ff. Furthermore, at this stage of the argument the cohomology class ff might be rational, but its canonical representative is in fact unique since we consider strict (2,2,2)(2,2,2)-surfaces. Nonetheless, see § 2.3.4 below for why, in fact, this case does not occur.

§ 2.1.3 applies to the finitely many generators γu0,i\gamma_{u_{0},i}, so Theorem 2.1.4 applies to them as well on a fixed ball B0(ε)B_{0}(\varepsilon) around 030\in\mathbb{C}^{3}. However, the assumptions of Theorem 2.1.4 are stable under a small perturbation, so they hold for γu,i\gamma_{u,i} for uu in a sufficiently small neighborhood of u0u_{0}. Therefore, by Theorem 2.1.4 the maps sns_{n} approach the identity when restricted to B0(ε/2)B_{0}(\varepsilon/2), and so the weak limit of 1λn(sn)ω0\frac{1}{\lambda_{n}}(s_{n})_{*}\omega_{0} vanishes in B0(ε/2)XuB_{0}(\varepsilon/2)\cap X_{u}. We conclude that the support of ηf\eta_{f} avoids B0(ε/2)B_{0}(\varepsilon/2).

Finally, the action of Aut(Xu)\operatorname{{Aut}}(X_{u}) on the (projectivized) boundary of the ample cone is minimal, i.e. every orbit is dense, and clearly the property of having a gap in the support is invariant under applying one automorphism. It follows that the set F:=Aut(Xu)F0F:=\operatorname{{Aut}}(X_{u})\cdot F_{0} is a dense FσF_{\sigma}-set with the required properties. ∎

2.3.6 Remark (Avoidance of parabolic points).

The set FF provided by Theorem 2.3.5 is disjoint from the countably many parabolic points. The reason is that the canonical currents at the parabolic points have full support, since they are obtained as the pullback of currents from the base 1()\mathbb{P}^{1}(\mathbb{C}) of an elliptic fibration, but the corresponding currents on 1()\mathbb{P}^{1}(\mathbb{C}) have real-analytic potentials away from the finitely many points under the singular fibers. The last assertion can be seen from following through the proof of [FT23, Thm. 3.2.14] with real-analytic data.

2.3.7 Remark (Zassenhausian points).

Recall that relative to a lattice ΓIsom(n)\Gamma\subset\operatorname{{Isom}}(\mathbb{H}^{n}) of isometries of a hyperbolic space, the boundary points in n\partial\mathbb{H}^{n} can be called “Liouvillian” or “Diophantine”. Specifically, a Liouvillian point is one for which the geodesic ray with the point as its limit on the boundary makes very long excursions into the cusps of Γ\n\Gamma\backslash\mathbb{H}^{n}, while Diophantine points are ones for which the excursions into the cusps are controlled. Both situations involve quantitative bounds.

The boundary points constructed using iterated commutators as in § 2.1.1, with group elements lying deeper and deeper in the derived series of Γ\Gamma, could then be called “Zassenhausian”. Note that in principle, geodesics with Zassenhausian boundary points will have good recurrence properties and will also be Diophantine.

It would be interesting to see if canonical currents corresponding to Liouvillian boundary points have full support or not.

2.4. An example with no support on the real locus

The above methods can be strengthened to construct an example of a current with no support on the real locus of a real projective K3 surface. The starting point is a construction due to Moncet [Mon12, §9.3], who constructed real K3 surfaces with arbitrarily small entropy on the real locus. We use some minor modifications for notational convenience, and emphasize that many different choices are possible for the initial singular real K3 surface. Let us also note that these examples have a “tropical” analogue given by PL actions on the sphere, and the analogue of the finite-order action at the singular parameter corresponds to a finite order action by reflections on the cube, see [Fil19, §6.2].

2.4.1. Setup

Let X0X_{0} denote the (singular) surface

x2+y2+z2=1x^{2}+y^{2}+z^{2}=1

compactified in (1)3(\mathbb{P}^{1})^{3}. Its real locus X0()X_{0}(\mathbb{R}) is a real 22-dimensional sphere.

As before let 𝒰27\mathcal{U}\subset\mathbb{R}^{27} be the subset of smooth (2,2,2)(2,2,2)-surfaces, parametrized by the possible coefficients, and normalized such that the parameter 0270\in\mathbb{R}^{27} corresponds to X0X_{0}. Note that 0𝒰0\notin\mathcal{U}. Let next 𝒰𝒰\mathcal{U}^{\prime}\subset\mathcal{U} denote the subset of strict (2,2,2)(2,2,2)-surfaces. By the discussion in § 2.2.3 the set 𝒰\mathcal{U}^{\prime} is the complement of countably many divisors in 𝒰\mathcal{U}, and thus forms a dense GδG_{\delta} set.

2.4.2 Theorem (Full gaps in the real locus).

There exists a nonempty open set 𝒰0𝒰n\mathcal{U}_{0}\subset\mathcal{U}\subset\mathbb{R}^{n} in the analytic topology of smooth real (2,2,2)(2,2,2)-surfaces with the following property.

For each strict K3 surface XuX_{u} with u𝒰0u\in\mathcal{U}_{0}, there exists a dense FσF_{\sigma}-set of rays FF on the boundary of the ample cone of XuX_{u} such that for any [η]F[\eta]\in F, the support of the canonical current η\eta provided by [FT23, Thm. 1] is disjoint from the real locus Xu()X_{u}(\mathbb{R}). Furthermore FF determines an uncountable set of rays.

2.4.3. Subgroup of slow automorphisms

Let us first observe that the involution σx\sigma_{x} acting on the surface X0X_{0} in § 2.4.1 is given by σx(x,y,z)=(x,y,z)\sigma_{x}(x,y,z)=(-x,y,z), and analogously for σy,σz\sigma_{y},\sigma_{z}. Therefore, let KσΓσK_{\sigma}\subset\Gamma_{\sigma} be the group from § 2.2.6 obtained as the kernel of this action; it is a free group on five generators γi\gamma_{i} and acts nontrivially on any smooth and strict (2,2,2)(2,2,2)-surface.

Even for smooth surfaces Xu(1)3X_{u}\subset(\mathbb{P}^{1})^{3}, we will be interested only in their intersection with the affine chart 3\mathbb{C}^{3}, and specifically a neighborhood of X0()X_{0}(\mathbb{R}). We will thus restrict to a neighborhood in 𝒰\mathcal{U} of u=0u=0 for which no additional real components arise.

2.4.4. Good cover

Choose a finite cover of X0()3X_{0}(\mathbb{R})\subset\mathbb{R}^{3} by open sets Vi3V_{i}\subset\mathbb{C}^{3} such that we have biholomorphisms ϕi:ViB0(1)3\phi_{i}\colon V_{i}\to B_{0}(1)\subset\mathbb{C}^{3} to a ball of radius 11 around 0, and the preimages of the smaller balls Vi:=ϕi1(B0(14))V_{i}^{\prime}:=\phi_{i}^{-1}\left(B_{0}(\tfrac{1}{4})\right) still cover X0()X_{0}(\mathbb{R}).

Choose now a sufficiently small open neighborhood of the origin 𝒰027\mathcal{U}_{0}\subset\mathbb{R}^{27} such that the following property is satisfied: For each of the five generators γj\gamma_{j} of KσK_{\sigma} and their inverses, we have for every chart ViV_{i} that γij:=ϕiγjϕi1\gamma_{ij}^{\prime}:=\phi_{i}\circ\gamma_{j}\circ\phi^{-1}_{i} satisfies:

γij:B0(12)B0(1) is well-defined and γij𝟏B0(12)164.\gamma_{ij}^{\prime}\colon B_{0}\left(\tfrac{1}{2}\right)\to B_{0}(1)\text{ is well-defined and }\left\|\gamma_{ij}^{\prime}-{\bm{1}}\right\|_{B_{0}\left(\tfrac{1}{2}\right)}\leq\tfrac{1}{64}.

Require also that for any u𝒰0u\in\mathcal{U}_{0} that Xu()X_{u}(\mathbb{R}) is nonempty and still covered by the sets {Vi}\{V_{i}^{\prime}\}.

Proof of Theorem 2.4.2.

By Theorem 2.1.4 all the commutators in the set S(n)S^{(n)} as defined in § 2.1.1 are well-defined when conjugated to any of the charts ϕi\phi_{i}, and furthermore their distance to the identity transformation goes to zero as n+n\to+\infty.

As in the proof of Theorem 2.3.5, let snS(n)s_{n}\in S^{(n)} be any sequence of such commutators such that the cohomology class 1λn(sn)[ω0]\tfrac{1}{\lambda_{n}}(s_{n})_{*}[\omega_{0}] converges to some class ff. Then the canonical current ηf\eta_{f} has no support in the neighborhoods ViV_{i}^{\prime}. Since these still cover Xu()X_{u}(\mathbb{R}) for u𝒰0u\in\mathcal{U}_{0}, the result follows. ∎

References