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On the Lipschitz Saturation of Toric Singularities

Daniel Duarte, Arturo E. Giles Flores
Abstract

We begin the study of Lipschitz saturation for germs of toric singularities. By looking at their associated analytic algebras, we prove that if (X,0)(X,0) is a germ of toric singularity with smooth normalization then its Lipschitz saturation is again toric. Finally we show how to calculate the Lipschitz saturation for some families of toric singularities starting from the semigroup that defines them.

Introduction

For a germ (X,0)(n,0)(X,0)\subset(\mathbb{C}^{n},0) of reduced complex analytic singularity, the algebra of germs of Lipschitz meromorphic functions is an analytic algebra that sits between OX,0O_{X,0} and its normalization OX,0¯\overline{O_{X,0}}. The definition is algebraic, and was inspired by Zariski’s theory of saturation, whose objective was to establish the foundations for an algebraic theory of equisingularity as seen in [27], [28], [29] and [30]. It was first studied by Pham and Teissier in [21], where they prove that Lipschitz saturation and Zariski saturation coincide for hypersurfaces. In this paper they also introduced a relative notion of Lipschitz saturation whose algebraic treatment was further studied in [4], [5], [18]. Beyond the algebraic relevance of the construction, the associated germ (Xs,0)(X^{s},0) is important in the study of biLipschitz equisingularity. The case of curves is pretty well understood and described in [6], [9], [12], [13], [20], [21]. However not much is known in higher dimensions. In this work we begin the study of the Lipschitz saturation for toric singularities of arbitrary dimension.

Our study is inspired by the fact that the Lipschitz saturation of a germ of irreducible curve is a toric curve, i.e., is parametrized by monomials. Moreover, there exists an explicit procedure for calculating its corresponding numerical semigroup starting from the semigroup of the curve. Although there is no reason to believe that the Lipschitz saturation of a germ of arbitrary dimension has toric structure, we may still ask the following question: starting with a toric singularity, is the Lipschitz saturation also toric? If so, is there a procedure for computing the corresponding affine semigroup from the semigroup of the toric singularity?

We answer the first question in the situation that naturally generalizes the case of toric curves, that is, toric varieties having smooth normalization. Regarding the question of the description of the corresponding semigroup, we provide an answer for some families of toric singularities. An interesting semigroup theory aspect still lingers. The numerical semigroup of the Lipschitz saturation of a germ of toric curve can be calculated via the semigroup theoretic saturation as described in [22]. One can ask: if we start with a toric germ (X,0)(X,0), is there an analogous operation on affine semigroups that calculates the affine semigroup of (Xs,0)(X^{s},0)? We conclude the paper by exhibiting examples showing that some properties of Lipschitz saturation of curves are no longer true in higher dimension. For instance, the embedding dimension has a different behavior.

The paper is divided as follows. In section 1 we recall the general construction of Lipschitz saturation and its main properties. We also recall some known facts in the case of curves. Furthermore, we prove that if a germ (Y,0)(Y,0) can be seen as the generic linear projection of another germ (X,0)(X,0), then their Lipschitz saturations are isomorphic (proposition 1.4). This proposition has important consequences, for instance, it allows us to build examples of singularities that are not isomorphic to (X,0)(X,0) with toric Lipschitz saturation isomorphic to (Xs,0)(X^{s},0) and toric normalization isomorphic to (X¯,0)(\overline{X},0).

In section 2 we establish what we mean by a toric singularity (X,0)(X,0), which is basically taking the germ at the origin of an affine toric variety. We summarize some important facts about the passage from the algebraic toric variety to the germ of analytic space. The results of this section are essentially known (see, for instance, [15]). We include them here for the sake of completeness.

In section 3 we prove our first main theorem: the Lipschitz saturation (Xs,0)(X^{s},0) of a toric singularity whose normalization is smooth is again toric (theorem 3.2). The key idea towards this result is that for every f𝒪X,0sf\in\mathcal{O}_{X,0}^{s} all of its monomials are also in 𝒪X,0s\mathcal{O}_{X,0}^{s}. We believe this result is true for toric singularities in general. However, the smooth normalization hypothesis is there for technical reasons (remark 3.4). As a first application, we show that the Whitney Umbrella singularity is Lipschitz saturated (see example 3.6).

In section 4 we use the tools previously developed to give a combinatorial description of the Lipschitz saturation (Xs,0)(X^{s},0) for some families of toric singularities. More concretely, given the semigroup Γ\Gamma corresponding to the toric singularity (X,0)(X,0), we explicitly describe the semigroup Γs\Gamma^{s} of its Lipschitz saturation (see proposition 4.1 and theorem 4.5). As a byproduct we can compute the embedding dimension of (Xs,0)(X^{s},0) in these cases (see corollaries 4.2 and 4.6). We conclude by illustrating all these results in several examples.

1 Lipschitz saturation of complex analytic germs

The definition of Lipschitz saturation of a reduced complex analytic algebra 𝒪X,0\mathcal{O}_{X,0} is based on the concept of integral dependence on an ideal. Given an element rr and an ideal II in a ring RR, we say that r\mathit{r} is integral over I\mathit{I} if rr satisfies a relation of the form

rm+a1rm1+a2rm2++am1r+am=0,r^{m}+a_{1}r^{m-1}+a_{2}r^{m-2}+\cdots+a_{m-1}r+a_{m}=0,

for some integer m>0m>0, with ajIja_{j}\in I^{j} for j=1,2,,mj=1,2,\ldots,m. The set I¯\overline{I} consisting of those elements of RR which are integral over II is an ideal called the integral closure of II in RR (see [16], [19]).

Let us assume for simplicity that (X,0)(X,0) is irreducible and let n:𝒪X,0𝒪X,0¯n^{*}:\mathcal{O}_{X,0}\hookrightarrow\overline{\mathcal{O}_{X,0}} be the integral closure of 𝒪X,0\mathcal{O}_{X,0} in its field of fractions. Geometrically, this corresponds to the normalization map n:(X¯,0)(X,0)n:(\overline{X},0)\to(X,0) and if we consider the holomorphic map

(X¯×XX¯,(0,0))(X¯×X¯,(0,0),)\left(\overline{X}\times_{X}\overline{X},(0,0)\right)\hookrightarrow\left(\overline{X}\times\overline{X},(0,0),\right)

we get a surjective map of analytic algebras

Ψ:𝒪X,0¯\widearc𝒪X,0¯𝒪X,0¯\widearc𝒪X,0𝒪X,0¯,\Psi:\overline{\mathcal{O}_{X,0}}\widearc{\otimes}_{\mathbb{C}}\overline{\mathcal{O}_{X,0}}\longrightarrow\overline{\mathcal{O}_{X,0}}\widearc{\otimes}_{\mathcal{O}_{X,0}}\overline{\mathcal{O}_{X,0}},

where \widearc\widearc{\otimes} denotes the analytic tensor product which is the operation on the analytic algebras that corresponds to the fibre product of analytic spaces (for more details see [2] and [13]).

Definition 1.1.

Let IΔI_{\Delta} be the kernel of the morphism Ψ\Psi above. We define the Lipschitz saturation 𝒪X,0s\mathcal{O}_{X,0}^{s} of 𝒪X,0\mathcal{O}_{X,0} as the algebra

𝒪X,0s:={f𝒪X,0¯|f\widearc11\widearcfIΔ¯}.\mathcal{O}_{X,0}^{s}:=\left\{f\in\overline{\mathcal{O}_{X,0}}\,|\,f\widearc{\otimes}_{\mathbb{C}}1-1\widearc{\otimes}_{\mathbb{C}}f\in\overline{I_{\Delta}}\right\}.
Remark 1.2.

A detailed discussion of the following facts can be found in [21, 13, 23]:

  1. 1.

    𝒪X,0s\mathcal{O}_{X,0}^{s} is an analytic algebra and coincides with the ring of germs of meromorphic functions on (X,0)(X,0) which are locally Lipschitz with respect to the ambient metric.

  2. 2.

    We have injective ring morphisms

    𝒪X,0𝒪X,0s𝒪X,0¯.\mathcal{O}_{X,0}\hookrightarrow\mathcal{O}_{X,0}^{s}\hookrightarrow\overline{\mathcal{O}_{X,0}}.
  3. 3.

    The corresponding Lipschitz saturation map

    ζ:(Xs,0)(X,0)\zeta:(X^{s},0)\to(X,0)

    is a biLipschitz homeomorphism, induces an isomorphism outside the non-normal locus of XX and preserves the multiplicity, i.e.

    mult (Xs,0)= mult (X,0).\textrm{mult }(X^{s},0)=\textrm{ mult }(X,0).

    Moreover, it can be realized as a generic linear projection in the sense of [13, Def. 8.4.2].

  4. 4.

    𝒪X,0s¯=𝒪X,0¯\overline{\mathcal{O}_{X,0}^{s}}=\overline{\mathcal{O}_{X,0}} and the holomorphic map induced by 𝒪X,0s𝒪X,0¯\mathcal{O}_{X,0}^{s}\hookrightarrow\overline{\mathcal{O}_{X,0}},

    X¯nsXs,\overline{X}\stackrel{{\scriptstyle n_{s}}}{{\longrightarrow}}X^{s},

    is the normalization map of XsX^{s}. Moreover the map

    n=ζns:X¯Xn=\zeta\circ n_{s}:\overline{X}\to X

    is the normalization map of XX.

Aside from these facts, little else is known in the general case. However, in the case of curves, the saturation has some very interesting equisingularity properties. First, Pham and Teissier proved that for a plane curve (X,0)(2,0)(X,0)\subset(\mathbb{C}^{2},0) the Lipschitz saturation 𝒪X,0s\mathcal{O}_{X,0}^{s} determines and is determined by the characteristic exponents of its branches and their intersection multiplicities, in particular the curve (Xs,0)(X^{s},0) is an invariant of the equisingularity class of (X,0)(X,0) (See [21] and [6, Prop. VI.3.2]).

In the irreducible case (branches) they also prove that the the curve (Xs,0)(X^{s},0) is always a toric curve, (i.e parametrized by monomials), and if we have a parametrization of (X,0)(2,0)(X,0)\subset(\mathbb{C}^{2},0)

t(φ1(t),φ2(t));φ1,φ2{t},t\longmapsto\left(\varphi_{1}(t),\varphi_{2}(t)\right);\hskip 14.45377pt\varphi_{1},\varphi_{2}\in\mathbb{C}\{t\},

then there is a simple procedure to calculate a parametrization of (Xs,0)(X^{s},0).

  1. 1.

    Calculate the set of characteristic exponents E:={β0,β1,,βg}E:=\{\beta_{0},\beta_{1},\ldots,\beta_{g}\} of (X,0)(X,0).

  2. 2.

    Calculate the smallest saturated numerical semigroup E~\tilde{E}\subset\mathbb{N} containing EE as follows [22, Chapter 3, Section 2]:

    E0~:=Eβ0;\widetilde{E_{0}}:=E\cup\beta_{0}\cdot\mathbb{N};
    E1~:=E0~{β1+ke1|k},e1= gcd {β0,β1};\widetilde{E_{1}}:=\widetilde{E_{0}}\cup\left\{\beta_{1}+ke_{1}\,|\,k\in\mathbb{N}\right\},\hskip 14.45377pte_{1}=\textrm{ gcd }\{\beta_{0},\beta_{1}\};
    Ej+1~:=Ej~{βj+1+kej+1|k},ej+1= gcd {ej,βj+1};\widetilde{E_{j+1}}:=\widetilde{E_{j}}\cup\left\{\beta_{j+1}+ke_{j+1}\,|\,k\in\mathbb{N}\right\},\hskip 14.45377pte_{j+1}=\textrm{ gcd }\{e_{j},\beta_{j+1}\};
    E~=Eg~.\tilde{E}=\widetilde{E_{g}}.
  3. 3.

    If {a1,,aβ0}\{a_{1},\ldots,a_{\beta_{0}}\} is the minimal system of generators of E~\tilde{E} then

    t(ta1,,taβ0)t\longmapsto\left(t^{a_{1}},\ldots,t^{a_{\beta_{0}}}\right)

    is a parametrization of (Xs,0)(X^{s},0). Recall that in this setting β0\beta_{0} is the multiplicity of (X,0)(X,0) and so we get that the embedding dimension of (Xs,0)(X^{s},0) is equal to the multiplicity of (X,0)(X,0).

These results extend well beyond the plane curve case: in [6, Thm VI.0.2, Prop. VI.3.1] the authors prove that for a curve (X,0)(n,0)(X,0)\subset(\mathbb{C}^{n},0), and a generic lineal projection π:(n,0)(2,0)\pi:(\mathbb{C}^{n},0)\to(\mathbb{C}^{2},0) the Lipschitz saturations 𝒪X,0\mathcal{O}_{X,0} of (X,0)(X,0) and Oπ(X),0sO_{\pi(X),0}^{s} of the plane curve (π(X),0)(2,0)(\pi(X),0)\subset(\mathbb{C}^{2},0) are isomorphic. Even more, by [12, Thm. 4.12] we get that two germs of curves (X,0)(X,0) and (Y,0)(Y,0) are bi-Lipschitz equivalent if and only if their Lipschitz saturations are isomorphic. In this sense the saturated curve (Xs,0)(X^{s},0) can be seen as a canonical representative of the bi-Lipschitz equivalence class of (X,0)(X,0).

Example 1.3.

Let (X,0)(3,0)(X,0)\subset(\mathbb{C}^{3},0) be the space curve with normalization map

η:(,0)\displaystyle\eta:(\mathbb{C},0) (X,0)\displaystyle\longrightarrow(X,0)
t\displaystyle t (t6,t11t9,t11+t9).\displaystyle\longmapsto(t^{6},t^{11}-t^{9},t^{11}+t^{9}).

For this curve, the projection on the first two coordinates is generic, giving us the plane curve

t(t6,t11t9)t\longmapsto(t^{6},t^{11}-t^{9})

with characteristic exponents E={6,9,11}E=\{6,9,11\}.

Following the procedure described above, we get the saturated numerical semigroup E~\tilde{E} with minimal system of generators {6,9,11,13,14,16}\{6,9,11,13,14,16\}. This determines a parametrization of the saturated curve (Xs,0)(6,0)(X^{s},0)\subset(\mathbb{C}^{6},0) of the form:

ηs:(,0)\displaystyle\eta^{s}:(\mathbb{C},0) (Xs,0)\displaystyle\longrightarrow(X^{s},0)
τ\displaystyle\tau (τ6,τ9,τ11,τ13,τ14,τ16).\displaystyle\mapsto(\tau^{6},\tau^{9},\tau^{11},\tau^{13},\tau^{14},\tau^{16}).

Going back to the general case, we can prove that, just as in the case of curves, the Lipschitz saturation remains unchanged under generic linear projections.

Proposition 1.4.

Let (X,0)(n,0)(X,0)\subset(\mathbb{C}^{n},0) be a germ of reduced and irreducible singularity, and let π:(n,0)(m,0)\pi:(\mathbb{C}^{n},0)\to(\mathbb{C}^{m},0) be a generic linear projection with respect to (X,0)(X,0). Then (X,0)(X,0) and its image germ (π(X),0)(\pi(X),0) have isomorphic Lipschitz saturations, i.e.:

𝒪X,0s𝒪π(X),0s.\mathcal{O}_{X,0}^{s}\cong\mathcal{O}_{\pi(X),0}^{s}.

Before going through the proof, recall that the cone C5(X,0)C_{5}(X,0), constructed by taking limits of bi-secants to XX at 0, is an algebraic cone defined by H. Whitney in [25]. A linear projection π:(n,0)(m,0)\pi:(\mathbb{C}^{n},0)\to(\mathbb{C}^{m},0) with kernel DD is called C5C_{5}-general (or generic) with respect to (X,0)(X,0) if it is transversal to the cone C5(X,0)C_{5}(X,0), meaning DC5(X,0)={0}D\bigcap C_{5}(X,0)=\{0\}. When π\pi is generic, it induces a homeomorphism between (X,0)(X,0) and its image (π(X),0)(\pi(X),0), and these two germs have the same multiplicity, for a detailed explanation see [13, Section 8.4].

Proof.

(of proposition 1.4)

After a linear change of coordinates we can assume that the linear projection π:(n,0)(m,0)\pi:(\mathbb{C}^{n},0)\to(\mathbb{C}^{m},0) is the projection on the first mm coordinates (z1,,zn)(z1,,zm)(z_{1},\ldots,z_{n})\mapsto(z_{1},\ldots,z_{m}). Let J𝒪X×X,(0,0)J\subset\mathcal{O}_{X\times X,(0,0)} denote the ideal defining the diagonal of X×XX\times X

J=z1w1,,znwn𝒪X×X,(0,0)J=\left<z_{1}-w_{1},\ldots,z_{n}-w_{n}\right>\mathcal{O}_{X\times X,(0,0)}

Denote Jπ=z1w1,,zmwm𝒪X×X,(0,0)J_{\pi}=\left<z_{1}-w_{1},\ldots,z_{m}-w_{m}\right>\mathcal{O}_{X\times X,(0,0)}. Then by [13, Proposition 8.5.11] the genericity of π\pi is equivalent to the equality of integral closures J¯=Jπ¯\overline{J}=\overline{J_{\pi}} in 𝒪X×X,(0,0)\mathcal{O}_{X\times X,(0,0)}.

On the other hand, since π:(X,0)(π(X),0)\pi:(X,0)\to(\pi(X),0) is a finite, generically 1-1 and surjective map, then the morphism

π:𝒪π(X),0𝒪X,0\pi^{*}:\mathcal{O}_{\pi(X),0}\to\mathcal{O}_{X,0}

is injective, makes 𝒪X,0\mathcal{O}_{X,0} a finitely generated 𝒪π(X),0\mathcal{O}_{\pi(X),0}-module and induces an isomorphism of the corresponding field of fractions Q(𝒪X,0)Q(\mathcal{O}_{X,0}). All these together imply that 𝒪X,0\mathcal{O}_{X,0} and 𝒪π(X),0\mathcal{O}_{\pi(X),0} have isomorphic integral closures in Q(𝒪X,0)Q(\mathcal{O}_{X,0}) and so if η:(X¯,0)(X,0)\eta:(\overline{X},0)\to(X,0) denotes the normalization of (X,0)(X,0) then the composition

(X¯,0)η(X,0)π(π(X),0)(\overline{X},0)\stackrel{{\scriptstyle\eta}}{{\longrightarrow}}(X,0)\stackrel{{\scriptstyle\pi}}{{\longrightarrow}}(\pi(X),0)

is a normalization of (π(X),0)(\pi(X),0).

Note that the ideal IΔI_{\Delta} of definition 1.1 is defined by the “coordinate functions” of the normalization map

(X¯,0)η(X,0)π(π(X),0)(\overline{X},0)\stackrel{{\scriptstyle\eta}}{{\longrightarrow}}(X,0)\stackrel{{\scriptstyle\pi}}{{\longrightarrow}}(\pi(X),0)
y¯(η1(y),,ηn(y))(η1(y),,ηm(y)),\underline{y}\mapsto\left(\eta_{1}(y),\ldots,\eta_{n}(y)\right)\mapsto\left(\eta_{1}(y),\ldots,\eta_{m}(y)\right),

that is (see [13, Section 8.5.2]),

IΔX=η1(y)η1(x),,ηn(y)ηn(x)𝒪X¯×X¯,(0,0)I_{\Delta_{X}}=\left<\eta_{1}(y)-\eta_{1}(x),\ldots,\eta_{n}(y)-\eta_{n}(x)\right>\mathcal{O}_{\overline{X}\times\overline{X},(0,0)}
IΔπ(X)=η1(y)η1(x),,ηm(y)ηm(x)𝒪X¯×X¯,(0,0).I_{\Delta_{\pi(X)}}=\left<\eta_{1}(y)-\eta_{1}(x),\ldots,\eta_{m}(y)-\eta_{m}(x)\right>\mathcal{O}_{\overline{X}\times\overline{X},(0,0)}.

To prove the desired result it is enough to prove the equality of the integral closures IΔX¯=IΔπ(X)¯\overline{I_{\Delta_{X}}}=\overline{I_{\Delta_{\pi(X)}}}. But the germ map:

η×η:(X¯×X¯,(0,0))(X×X,(0,0))\eta\times\eta:\left(\overline{X}\times\overline{X},(0,0)\right)\longrightarrow\left(X\times X,(0,0)\right)

induces a morphism of analytic algebras:

(η×η):𝒪X×X,(0,0)𝒪X¯×X¯,(0,0)(\eta\times\eta)^{*}:\mathcal{O}_{X\times X,(0,0)}\longrightarrow\mathcal{O}_{\overline{X}\times\overline{X},(0,0)}

such that:

(η×η)(J)=IΔX\left<\left(\eta\times\eta\right)^{*}(J)\right>=I_{\Delta_{X}}
(η×η)(Jπ)=IΔπ(X)\left<\left(\eta\times\eta\right)^{*}(J_{\pi})\right>=I_{\Delta_{\pi(X)}}

and since J¯=Jπ¯\overline{J}=\overline{J_{\pi}} in 𝒪X×X,(0,0)\mathcal{O}_{X\times X,(0,0)} the result follows. ∎

Note that in the course of the proof we have shown that the germ (X,0)(X,0) and its general projection (π(X),0)(\pi(X),0) have isomorphic normalizations. On the downside, it will no longer be true in general that bi-Lipschitz equivalent germs will have isomorphic Lipschitz saturations. This is because a germ (X,0)(X,0) and its Lipschitz saturation (Xs,0)(X^{s},0) always have the same multiplicity, however in [3] the authors prove that in dimension bigger than two, multiplicity of singularities is not a bi-Lipschitz invariant.

2 Toric singularities

In this section we establish what we mean by a toric singularity. We also introduce the notation we use regarding toric varieties.

Let 𝒜={γ1,,γn}d\mathcal{A}=\{\gamma_{1},\ldots,\gamma_{n}\}\subset\mathbb{Z}^{d}, Γ=𝒜={iaiγi|ai}\Gamma=\mathbb{N}\mathcal{A}=\big{\{}\sum_{i}a_{i}\gamma_{i}|a_{i}\in\mathbb{N}\big{\}}, and σˇ=0𝒜\check{\sigma}=\mathbb{R}_{\geq 0}\mathcal{A}. Assume that the group generated by 𝒜\mathcal{A} is d\mathbb{Z}^{d} and that σˇ\check{\sigma} is a strongly convex cone. Consider the following homomorphism of semigroups,

π:\displaystyle\pi: nΓ\displaystyle\mathbb{N}^{n}\to\Gamma
αiαiγi,\displaystyle\alpha\mapsto\sum_{i}\alpha_{i}\gamma_{i},

and the induced \mathbb{C}-algebra homomorphism,

φ:\displaystyle\varphi: [z1,,zn][t1±,,td±]\displaystyle\mathbb{C}[z_{1},\ldots,z_{n}]\to\mathbb{C}[t_{1}^{\pm},\ldots,t_{d}^{\pm}]
zitγi=t1γi,1tdγi,d\displaystyle\hskip 42.67912ptz_{i}\mapsto t^{\gamma_{i}}=t_{1}^{\gamma_{i,1}}\cdots t_{d}^{\gamma_{i,d}}
zαtπ(α).\displaystyle\hskip 42.67912ptz^{\alpha}\mapsto t^{\pi(\alpha)}.

Let IΓ=kerφI_{\Gamma}=\ker\varphi. Recall that IΓI_{\Gamma} is a prime ideal and IΓ=zαzβ|π(α)=π(β).I_{\Gamma}=\langle z^{\alpha}-z^{\beta}|\pi(\alpha)=\pi(\beta)\rangle. Let XnX\subset\mathbb{C}^{n} be the affine variety defined by IΓI_{\Gamma}. Then XX is a dd-dimensional affine toric variety containing the origin. Let [X]\mathbb{C}[X] be the ring of regular functions on XX and [Γ]\mathbb{C}[\Gamma] the \mathbb{C}-algebra of the semigroup Γ\Gamma. Recall that [X][Γ]=[tγ1,,tγn][z1,,zn]/IΓ\mathbb{C}[X]\cong\mathbb{C}[\Gamma]=\mathbb{C}[t^{\gamma_{1}},\ldots,t^{\gamma_{n}}]\cong\mathbb{C}[z_{1},\ldots,z_{n}]/I_{\Gamma} [7, Chapter 1].

Next we discuss some basic results on the passage from the algebraic toric variety XX to the germ of analytic space (X,0)(X,0). Throughout this section we use the following notation.

  • [[Γ]]\mathbb{C}[[\Gamma]] denotes the ring of formal power series with exponents in Γ\Gamma.

  • {Γ}\mathbb{C}\{\Gamma\} denotes the subring of [[Γ]]\mathbb{C}[[\Gamma]] consisting of convergent series in a neighborhood of 0X0\in X.

  • 𝒪X,0\mathcal{O}_{X,0} denotes the algebra of germs of holomorphic functions on 0X0\in X.

Remark 2.1.

Notice that [[Γ]]\mathbb{C}[[\Gamma]] is indeed a ring since Γ\Gamma is contained in a strongly convex cone which implies that every element of Γ\Gamma can be written as a sum of elements of Γ\Gamma in finitely many different ways.

Lemma 2.2.

With the previous notation,

𝒪X,0{Γ}{z1,,zn}/IΓ{z1,,zn}.\mathcal{O}_{X,0}\cong\mathbb{C}\{\Gamma\}\cong\mathbb{C}\{z_{1},\ldots,z_{n}\}/I_{\Gamma}\mathbb{C}\{z_{1},\ldots,z_{n}\}.
Proof.

The first isomorphism is proved in [15, Lemme 1] or [14, Lemma 1.1]. The proof given there is for normal toric varieties. However, the same proof holds in the non-normal case.

We prove the second isomorphism. Consider the following exact sequence:

0IΓ[z1,,zn]φ[Γ]0.\lx@xy@svg{\hbox{\raise 0.0pt\hbox{\kern 5.5pt\hbox{\ignorespaces\ignorespaces\ignorespaces\hbox{\vtop{\kern 0.0pt\offinterlineskip\halign{\entry@#!@&&\entry@@#!@\cr&&&&\crcr}}}\ignorespaces{\hbox{\kern-5.5pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise 0.0pt\hbox{$\textstyle{0\ignorespaces\ignorespaces\ignorespaces\ignorespaces}$}}}}}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{\hbox{\lx@xy@droprule}}\ignorespaces{\hbox{\kern 29.5pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}{\hbox{\kern 29.5pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise 0.0pt\hbox{$\textstyle{I_{\Gamma}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}$}}}}}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{\hbox{\lx@xy@droprule}}\ignorespaces{\hbox{\kern 68.18054pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}{\hbox{\kern 68.18054pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise 0.0pt\hbox{$\textstyle{\mathbb{C}[z_{1},\ldots,z_{n}]\ignorespaces\ignorespaces\ignorespaces\ignorespaces}$}}}}}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern 118.52934pt\raise 5.1875pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-0.8264pt\hbox{$\scriptstyle{\varphi}$}}}\kern 3.0pt}}}}}}\ignorespaces{\hbox{\kern 142.02246pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}{\hbox{\kern 142.02246pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise 0.0pt\hbox{$\textstyle{\mathbb{C}[\Gamma]\ignorespaces\ignorespaces\ignorespaces\ignorespaces}$}}}}}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{\hbox{\lx@xy@droprule}}\ignorespaces{\hbox{\kern 191.05026pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}{\hbox{\kern 191.05026pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise 0.0pt\hbox{$\textstyle{0}$}}}}}}}\ignorespaces}}}}\ignorespaces.

Let 𝔪=z1,,zn\mathfrak{m}=\langle z_{1},\ldots,z_{n}\rangle. Taking completions with respect to 𝔪\mathfrak{m} we obtain the following exact sequence:

0IΓ^[[z1,,zn]]φf[[Γ]]0.\lx@xy@svg{\hbox{\raise 0.0pt\hbox{\kern 5.5pt\hbox{\ignorespaces\ignorespaces\ignorespaces\hbox{\vtop{\kern 0.0pt\offinterlineskip\halign{\entry@#!@&&\entry@@#!@\cr&&&&\crcr}}}\ignorespaces{\hbox{\kern-5.5pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise 0.0pt\hbox{$\textstyle{0\ignorespaces\ignorespaces\ignorespaces\ignorespaces}$}}}}}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{\hbox{\lx@xy@droprule}}\ignorespaces{\hbox{\kern 29.5pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}{\hbox{\kern 29.5pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise 0.0pt\hbox{$\textstyle{\hat{I_{\Gamma}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}$}}}}}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{\hbox{\lx@xy@droprule}}\ignorespaces{\hbox{\kern 65.05557pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}{\hbox{\kern 65.05557pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise 0.0pt\hbox{$\textstyle{\mathbb{C}[[z_{1},\ldots,z_{n}]]\ignorespaces\ignorespaces\ignorespaces\ignorespaces}$}}}}}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern 119.7655pt\raise 5.59027pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-0.42361pt\hbox{$\scriptstyle{\varphi_{f}}$}}}\kern 3.0pt}}}}}}\ignorespaces{\hbox{\kern 144.45306pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}{\hbox{\kern 144.45306pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise 0.0pt\hbox{$\textstyle{\mathbb{C}[[\Gamma]]\ignorespaces\ignorespaces\ignorespaces\ignorespaces}$}}}}}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{\hbox{\lx@xy@droprule}}\ignorespaces{\hbox{\kern 199.03644pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}{\hbox{\kern 199.03644pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise 0.0pt\hbox{$\textstyle{0}$}}}}}}}\ignorespaces}}}}\ignorespaces.

On the other hand, IΓ^IΓ[[z1,,zn]]\hat{I_{\Gamma}}\cong I_{\Gamma}\mathbb{C}[[z_{1},\ldots,z_{n}]] [1, Proposition 10.15]. Denote φa=φf|{z1,,zn}\varphi_{a}=\varphi_{f}|_{\mathbb{C}\{z_{1},\ldots,z_{n}\}}. In the proof of [14, Lemma 1.1], alternatively [15, Lemme 1] it is shown that Im φa={Γ}\mbox{Im }\varphi_{a}=\mathbb{C}\{\Gamma\}. It remains to prove that kerφa=IΓ{z1,,zn}\ker\varphi_{a}=I_{\Gamma}\mathbb{C}\{z_{1},\ldots,z_{n}\}.

Since kerφf=IΓ[[z1,,zn]]\ker\varphi_{f}=I_{\Gamma}\mathbb{C}[[z_{1},\ldots,z_{n}]], it follows that IΓ{z1,,zn}kerφaI_{\Gamma}\mathbb{C}\{z_{1},\ldots,z_{n}\}\subset\ker\varphi_{a}. Let F{z1,,zn}F\in\mathbb{C}\{z_{1},\ldots,z_{n}\} be such that 0=φa(F)=φf(F)0=\varphi_{a}(F)=\varphi_{f}(F). We conclude that F{z1,,zn}IΓ[[z1,,zn]]=IΓ{z1,,zn}F\in\mathbb{C}\{z_{1},\ldots,z_{n}\}\cap I_{\Gamma}\mathbb{C}[[z_{1},\ldots,z_{n}]]=I_{\Gamma}\mathbb{C}\{z_{1},\ldots,z_{n}\} (these ideals are equal by [8, Exercise 8.1.5]). ∎

Lemma 2.3.

Let X¯\bar{X} be the (algebraic) normalization of XX. Then (X¯,0)(\bar{X},0) is the (analytic) normalization of (X,0)(X,0). Moreover, 𝒪X¯,0{σˇd}.\mathcal{O}_{\bar{X},0}\cong\mathbb{C}\{\check{\sigma}\cap\mathbb{Z}^{d}\}.

Proof.

Let η:X¯X\eta:\bar{X}\to X be the normalization. Recall that X¯\bar{X} is the toric variety defined by the semigroup σˇd\check{\sigma}\cap\mathbb{Z}^{d} and that η\eta is induced by the inclusion of semigroups Γσˇd\Gamma\subset\check{\sigma}\cap\mathbb{Z}^{d} [7, Proposition 1.3.8]. In particular, η\eta is a toric morphism.

Being the normalization, η\eta is an isomorphism on dense open sets. In addition, η1(0)=0\eta^{-1}(0)=0. Indeed, let qX¯q\in\bar{X} be such that η(q)=0\eta(q)=0. Recall that points in toric varieties correspond to homomorphisms of semigroups. Hence, the homomorphism corresponding to η(q)\eta(q) sends every non-zero element of Γ\Gamma to 0. On the other hand, for every mσˇdm\in\check{\sigma}\cap\mathbb{Z}^{d} there is k1k\geq 1 such that kmΓkm\in\Gamma. Since η\eta is induced by the inclusion Γσˇd\Gamma\subset\check{\sigma}\cap\mathbb{Z}^{d}, it follows that q=0q=0.

By the previous paragraph, the induced germ of an analytic function η:(X¯,0)(X,0)\eta:(\bar{X},0)\to(X,0) is finite and generically 1-1. On the other hand, it is known that X¯\bar{X} normal implies that (X¯,0)(\bar{X},0) normal [17, Satz 4]. By the uniqueness of normalization we conclude that η:(X¯,0)(X,0)\eta:(\bar{X},0)\to(X,0) is the normalization of (X,0)(X,0).

Finally, 𝒪X¯,0{σˇd}\mathcal{O}_{\bar{X},0}\cong\mathbb{C}\{\check{\sigma}\cap\mathbb{Z}^{d}\} follows using lemma 2.2. ∎

Corollary 2.4.

(X,0)(X,0) is irreducible as a germ.

Proof.

By a well-known theorem of Zariski [26], X¯\bar{X} irreducible and normal at 0 implies that the completion of the local ring at 0 is an integral domain. Hence, (X¯,0)(\bar{X},0) is irreducible by lemma 2.2. Hence, the germ (X,0)(X,0) must also be irreducible. ∎

Definition 2.5.

Let (X,0)(X,0) be a germ of an analytic space. We say that (X,0)(X,0) is a germ of a toric singularity if there exists a finitely generated semigroup Γd\Gamma\subset\mathbb{Z}^{d} contained in a strongly convex cone such that 𝒪X,0{Γ}\mathcal{O}_{X,0}\cong\mathbb{C}\{\Gamma\}. Equivalently, let XΓX_{\Gamma} be the affine toric variety defined by Γ\Gamma. Then (X,0)(X,0) is a toric singularity if it is isomorphic, as germs, to (XΓ,0)(X_{\Gamma},0).

Example 2.6.

Let XnX\subset\mathbb{C}^{n} be a toric variety containing the origin. Then (X,0)(X,0) is a germ of a toric singularity by lemma 2.2.

3 Lipschitz saturation of toric singularities

We have seen that for a toric singularity the analytic algebra 𝒪X,0\mathcal{O}_{X,0} is generated by monomials. With this in mind, the main idea to prove that the Lipschitz saturation of a toric singularity is again toric, consists of showing that every monomial of an element of the saturation also belongs to the saturation. The first step towards that goal is the study of the integral closure of homogeneous ideals in the ring of power series.

It is well known that the integral closure of a homogeneous ideal in a polynomial ring is again a homogeneous ideal ([24, Prop. (f), pg 38]). However we need this to be true for ideals generated by homogeneous polynomials in power series rings. That is the content of the following proposition, whose proof was kindly communicated to us by Professors Irena Swanson and Craig Huneke.

Note that an ideal {z1,,zn}\mathcal{I}\subset\mathbb{C}\{z_{1},\ldots,z_{n}\} is generated by homogeneous polynomials if and only if ff\in\mathcal{I} implies that every homogeneous component of ff is also in \mathcal{I}.

Proposition 3.1.

Let {z1,,zn}\mathcal{I}\subset\mathbb{C}\{z_{1},\ldots,z_{n}\} be an ideal generated by homogeneous polynomials in the ring of convergent power series. Then its integral closure ¯\overline{\mathcal{I}} is also generated by homogeneous polynomials.

Proof.

Let R:={z1,,zn}R:=\mathbb{C}\{z_{1},\ldots,z_{n}\} denote the ring of convergent power series in nn-variables over the field of complex numbers with maximal ideal 𝔪=z1,,zn\mathfrak{m}=\left<z_{1},\ldots,z_{n}\right>, and let =f1,,fmR\mathcal{I}=\left<f_{1},\ldots,f_{m}\right>R where each fjA:=[z1,,zn]Rf_{j}\in A:=\mathbb{C}[z_{1},\ldots,z_{n}]\subset R is a homogeneous polynomial.

Let K=f1,,fmAK=\left<f_{1},\ldots,f_{m}\right>A be the ideal generated by the fjf_{j}’s in the polynomial ring AA, so =KR\mathcal{I}=\left<K\right>R. Suppose that \mathcal{I} contains a power of 𝔪\mathfrak{m}, i.e. there exists k1k\geq 1 such that 𝔪k\mathfrak{m}^{k}\subset\mathcal{I}, and let sRs\in R be in the integral closure of \mathcal{I}. We can write

s=p+s,s=p+s^{\prime},

where pAp\in A is a polynomial and s𝔪k¯s^{\prime}\in\mathfrak{m}^{k}\subset\mathcal{I}\subset\overline{\mathcal{I}} is a series of order greater than or equal to kk. Note that p=ss¯p=s-s^{\prime}\in\overline{\mathcal{I}}.

Since the ring extension A𝔪RA_{\mathfrak{m}}\rightarrow R is faithfully flat ([11, Lemma B.3.4]) then ¯A𝔪=KA𝔪¯\overline{\mathcal{I}}\cap A_{\mathfrak{m}}=\overline{\left<K\right>A_{\mathfrak{m}}} ([16, Prop.1.6.2]), in particular p/1KA𝔪¯p/1\in\overline{\left<K\right>A_{\mathfrak{m}}}. This means that in the localized polynomial ring A𝔪A_{\mathfrak{m}} we have an equation of integral dependence of the form:

pr1+b1c1pr11++br1cr1p1+brcr=01,\frac{p^{r}}{1}+\frac{b_{1}}{c_{1}}\frac{p^{r-1}}{1}+\cdots+\frac{b_{r-1}}{c_{r-1}}\frac{p}{1}+\frac{b_{r}}{c_{r}}=\frac{0}{1},

where bjKjb_{j}\in K^{j} and cj𝔪c_{j}\notin\mathfrak{m}. Letting u=c1crAu=c_{1}\cdots c_{r}\in A and multiplying this equation by the unit ur1\frac{u^{r}}{1} of A𝔪A_{\mathfrak{m}} we get the following equality in A𝔪A_{\mathfrak{m}}:

(up)r+b1~(up)r1++br1~(up)+br~1=01.\frac{(up)^{r}+\widetilde{b_{1}}(up)^{r-1}+\cdots+\widetilde{b_{r-1}}(up)+\widetilde{b_{r}}}{1}=\frac{0}{1}.

Since A is an integral domain we get an integral dependence equation in AA

(up)r+b1~(up)r1++br1~(up)+br~=0,(up)^{r}+\widetilde{b_{1}}(up)^{r-1}+\cdots+\widetilde{b_{r-1}}(up)+\widetilde{b_{r}}=0,

that is, upK¯Aup\in\overline{K}\subset A. The inclusions 𝔪kKK¯\mathfrak{m}^{k}\subset K\subset\overline{K} imply that K¯\overline{K} is an 𝔪\mathfrak{m}-primary ideal of AA and since u𝔪u\notin\mathfrak{m} then pK¯p\in\overline{K}. Since KK is a homogeneous ideal in the polynomial ring AA then K¯\overline{K} is also homogeneous ([24, Prop. (f), pg 38]) and so each homogeneous component of pp is also in K¯¯\overline{K}\subset\overline{\mathcal{I}}. This implies that ¯\overline{\mathcal{I}} is also generated by homogeneous polynomials.

Now let R\mathcal{I}\subset R be an arbitrary ideal generated by homogeneous polynomials, and let ss be in the integral closure ¯\overline{\mathcal{I}} as before. Let s0s_{0} be the initial form of ss, s0s_{0} is the non-zero homogeneous component of ss of lowest degree. For all jj\in\mathbb{N}, ss is in the integral closure of +𝔪j\mathcal{I}+\mathfrak{m}^{j}. We proved in the previous paragraph that the integral closure +𝔪j¯\overline{\mathcal{I}+\mathfrak{m}^{j}} of +𝔪j\mathcal{I}+\mathfrak{m}^{j} in RR is generated by homogeneous polynomials for all jj\in\mathbb{N}. In particular, s0s_{0} is in the integral closure +𝔪j¯\overline{\mathcal{I}+\mathfrak{m}^{j}} for all jj. But by [16, Corollary 6.8.5] this implies that s0s_{0} is in the integral closure ¯\overline{\mathcal{I}}. Now we start over with s=ss0¯s^{\prime}=s-s_{0}\in\overline{\mathcal{I}} and in this way we get that all homogeneous components of ss are in ¯\overline{\mathcal{I}} which is what we wanted to prove. ∎

Theorem 3.2.

Let (X,0)(X,0) be a dd-dimensional toric singularity with smooth normalization. Then the Lipschitz saturated germ (Xs,0)(X^{s},0) is also a toric singularity.

We will do this proof in several steps starting with the following lemma.

Lemma 3.3.

Let (X,0)(X,0) be a dd-dimensional toric singularity with smooth normalization and let f𝒪X,0¯f\in\overline{\mathcal{O}_{X,0}} be a homogeneous polynomial such that f𝒪X,0sf\in\mathcal{O}_{X,0}^{s}. Then every monomial of ff is also in 𝒪X,0s\mathcal{O}_{X,0}^{s}.

Proof.

Let Γd\Gamma\subset\mathbb{Z}^{d} be the semigroup defining (X,0)(X,0). Recall that σˇ=0Γ\check{\sigma}=\mathbb{R}_{\geq 0}\Gamma is a strongly convex cone. This fact, together with the condition of smooth normalization allows us to assume, up to a change of coordinates, that Γd\Gamma\subset\mathbb{N}^{d} and σˇd=d\check{\sigma}\cap\mathbb{Z}^{d}=\mathbb{N}^{d} (see lemma 2.3).

Let 𝒜={a1,,an}d\mathcal{A}=\{a_{1},\ldots,a_{n}\}\subset\mathbb{N}^{d} be the minimal generating set of Γ\Gamma defining the toric singularity (X,0)(X,0). The normalization map can be realized as the monomial morphism:

n:(d,0)\displaystyle n:(\mathbb{C}^{d},0) (X,0)\displaystyle\longrightarrow(X,0)
(u1,,ud)\displaystyle\left(u_{1},\ldots,u_{d}\right) (ua1,,uan).\displaystyle\mapsto\left(u^{a_{1}},\ldots,u^{a_{n}}\right).

The ideal IΔI_{\Delta} of definition 1.1 is a homogeneous, binomial ideal in the ring of convergent power series {x1,,xd,y1,,yd}\mathbb{C}\{x_{1},\ldots,x_{d},y_{1},\ldots,y_{d}\}:

IΔ=xa1ya1,,xanyan.I_{\Delta}=\left<x^{a_{1}}-y^{a_{1}},\ldots,x^{a_{n}}-y^{a_{n}}\right>.

For any point τ=(t1,,td)()d\tau=(t_{1},\ldots,t_{d})\in\left(\mathbb{C}^{*}\right)^{d} we have an automorphism

φτ:{x1,,xd,y1,,yd}\varphi_{\tau}:\mathbb{C}\{x_{1},\ldots,x_{d},y_{1},\ldots,y_{d}\}\circlearrowleft

defined by xjtjxjx_{j}\mapsto t_{j}x_{j} and yjtjyjy_{j}\mapsto t_{j}y_{j}, such that φτ(IΔ)=IΔ\varphi_{\tau}\left(I_{\Delta}\right)=I_{\Delta}.

Now let f𝒪X,0¯{u1,,ud}f\in\overline{\mathcal{O}_{X,0}}\cong\mathbb{C}\{u_{1},\ldots,u_{d}\} be a homogeneous polynomial such that f𝒪X,0sf\in\mathcal{O}_{X,0}^{s}. Then f(x)f(y)IΔ¯f(x)-f(y)\in\overline{I_{\Delta}} and it satisfies an integral dependence equation of the form:

(f(x)f(y))m+h1(x,y)(f(x)f(y))m1++hm(x,y)=0,\left(f(x)-f(y)\right)^{m}+h_{1}(x,y)\left(f(x)-f(y)\right)^{m-1}+\cdots+h_{m}(x,y)=0,

where hj(x,y)IΔjh_{j}(x,y)\in I_{\Delta}^{j}. By applying the morphism φτ\varphi_{\tau} to the previous equation we get:

(f(τx)f(τy))m+h1(τx,τy)(f(τx)f(τy))m1++hm(τx,τy)=0,\left(f(\tau x)-f(\tau y)\right)^{m}+h_{1}(\tau x,\tau y)\left(f(\tau x)-f(\tau y)\right)^{m-1}+\cdots+h_{m}(\tau x,\tau y)=0,

where hj(τx,τy)IΔjh_{j}(\tau x,\tau y)\in I_{\Delta}^{j}, and so we get that gτ:=f(t1u1,,tdud)𝒪X,0sg_{\tau}:=f(t_{1}u_{1},\ldots,t_{d}u_{d})\in\mathcal{O}_{X,0}^{s}.

Since ff is a homogeneous polynomial, say of order kk, then we can write it in the form

f(u1,,ud)=α1++αd=kbαuα,f(u_{1},\ldots,u_{d})=\sum_{\alpha_{1}+\cdots+\alpha_{d}=k}b_{\alpha}u^{\alpha},

where bαb_{\alpha}\in\mathbb{C} and α=(α1,,αd)\alpha=(\alpha_{1},\ldots,\alpha_{d}). Then we have an expression for gτg_{\tau} of the form

gτ=f(t1u1,,tdud)\displaystyle g_{\tau}=f(t_{1}u_{1},\ldots,t_{d}u_{d}) =α1++αd=kταbαuα\displaystyle=\sum_{\alpha_{1}+\cdots+\alpha_{d}=k}\tau^{\alpha}b_{\alpha}u^{\alpha}
=(τα1,,ταN),(bα1uα1,,bαNuαN).\displaystyle=\left<\left(\tau^{\alpha^{1}},\ldots,\tau^{\alpha^{N}}\right),\left(b_{\alpha^{1}}u^{\alpha^{1}},\ldots,b_{\alpha^{N}}u^{\alpha^{N}}\right)\right>.

By choosing τ1,,τN\tau_{1},\ldots,\tau_{N} generic points in ()d\left(\mathbb{C}^{*}\right)^{d} we get

(gτ1gτN)=(τ1α1τ1αNτNα1τNαN)(bα1uα1bαNuαN),\begin{pmatrix}g_{\tau_{1}}\\ \vdots\\ g_{\tau_{N}}\end{pmatrix}=\begin{pmatrix}\tau_{1}^{\alpha^{1}}&\ldots&\tau_{1}^{\alpha^{N}}\\ \vdots&\cdots&\vdots\\ \tau_{N}^{\alpha^{1}}&\ldots&\tau_{N}^{\alpha^{N}}\end{pmatrix}\begin{pmatrix}b_{\alpha^{1}}u^{\alpha^{1}}\\ \vdots\\ b_{\alpha^{N}}u^{\alpha^{N}}\end{pmatrix},

where the ii-th row of the matrix corresponds to the image of the point τi()d\tau_{i}\in\left(\mathbb{C}^{*}\right)^{d} of the Veronese map νk:d1N1\nu_{k}:\mathbb{P}^{d-1}\to\mathbb{P}^{N-1} of degree kk. Since the image of the Veronese map is a nondegenerate projective variety, in the sense that it is not contained in any hyperplane, then these NN points are in general position. This implies that the matrix is invertible, and so we have

(bα1uα1bαNuαN)=(τ1α1τ1αNτNα1τNαN)1(gτ1gτN)\begin{pmatrix}b_{\alpha^{1}}u^{\alpha^{1}}\\ \vdots\\ b_{\alpha^{N}}u^{\alpha^{N}}\end{pmatrix}=\begin{pmatrix}\tau_{1}^{\alpha^{1}}&\ldots&\tau_{1}^{\alpha^{N}}\\ \vdots&\cdots&\vdots\\ \tau_{N}^{\alpha^{1}}&\ldots&\tau_{N}^{\alpha^{N}}\end{pmatrix}^{-1}\begin{pmatrix}g_{\tau_{1}}\\ \vdots\\ g_{\tau_{N}}\end{pmatrix}

In particular we have that bαjuαj𝒪X,0sb_{\alpha^{j}}u^{\alpha^{j}}\in\mathcal{O}_{X,0}^{s} which is what we wanted to prove. ∎

Proof.

(of theorem 3.2 )
We want to prove that there exists a finitely generated semigroup Γsd\Gamma^{s}\subset\mathbb{N}^{d} such that

𝒪X,0s{Γs}.\mathcal{O}_{X,0}^{s}\cong\mathbb{C}\{\Gamma^{s}\}.

As we mentioned before, in this setting the ideal IΔI_{\Delta} is a homogeneous, binomial ideal in the ring of convergent power series {x1,,xd,y1,,yd}\mathbb{C}\{x_{1},\ldots,x_{d},y_{1},\ldots,y_{d}\}, and by proposition 3.1 the ideal IΔ¯\overline{I_{\Delta}} is also generated by homogeneous polynomials. This means that if a series f{u1,ud}f\in\mathbb{C}\{u_{1}\ldots,u_{d}\} is in 𝒪X,0s\mathcal{O}_{X,0}^{s},

f=fm+fm+1++fN+,f=f_{m}+f_{m+1}+\cdots+f_{N}+\cdots,

then every homogeneous component fjf_{j} of ff is in 𝒪X,0s\mathcal{O}_{X,0}^{s}. But by lemma 3.3 this implies that every monomial of degree jj with a non-zero coefficient in fjf_{j} is also in 𝒪X,0s\mathcal{O}_{X,0}^{s}. Let Γs\Gamma^{s} be the semigroup defined by

Γs={αd|uα𝒪X,0s}.\Gamma^{s}=\{\alpha\in\mathbb{N}^{d}\,|\,u^{\alpha}\in\mathcal{O}_{X,0}^{s}\}.

We have that

𝒪X,0s{Γs}{u1,,ud}.\mathcal{O}_{X,0}^{s}\subset\mathbb{C}\{\Gamma^{s}\}\subset\mathbb{C}\{u_{1},\ldots,u_{d}\}.

We have to prove that Γs\Gamma^{s} is finitely generated and the equality 𝒪X,0s={Γs}\mathcal{O}_{X,0}^{s}=\mathbb{C}\{\Gamma^{s}\}.

To begin with the latter, take g{Γs}g\in\mathbb{C}\{\Gamma^{s}\}. For every k0k\geq 0, write g=gk+gk~g=g_{\leq k}+\widetilde{g_{k}} where gkg_{\leq k} is the truncation of gg to degree kk, and since it is a finite sum of monomials of 𝒪X,0s\mathcal{O}_{X,0}^{s}, by definition of Γs\Gamma^{s}, we have that gk𝒪X,0sg_{\leq k}\in\mathcal{O}_{X,0}^{s}. This means that

gk(x)gk(y)IΔ¯g_{\leq k}(x)-g_{\leq k}(y)\in\overline{I_{\Delta}}

and since gk~(x)gk~(y)𝔪k+1{x,y}\widetilde{g_{k}}(x)-\widetilde{g_{k}}(y)\in\mathfrak{m}^{k+1}\mathbb{C}\{x,y\} we have that

g(x)g(y)IΔ¯+𝔪k+1IΔ+𝔪k+1¯.g(x)-g(y)\in\overline{I_{\Delta}}+\mathfrak{m}^{k+1}\subset\overline{I_{\Delta}+\mathfrak{m}^{k+1}}.

In particular,

g(x)g(y)kIΔ+𝔪k+1¯=IΔ¯ by [16, Corollary 6.8.5]g(x)-g(y)\in\bigcap_{k\in\mathbb{N}}\overline{I_{\Delta}+\mathfrak{m}^{k+1}}=\overline{I_{\Delta}}\textrm{ by \cite[cite]{[\@@bibref{}{HS06}{}{}, Corollary 6.8.5]}}

then g𝒪X,0sg\in\mathcal{O}_{X,0}^{s} and we have the equality we wanted.

Now we prove that Γs\Gamma^{s} is a finitely generated semigroup. Let \leq be a monomial order in [u1,,ud]\mathbb{C}[u_{1},\ldots,u_{d}]. We order the elements of Γs\Gamma^{s} and write them as {βj|j}\{\beta^{j}\,|\,j\in\mathbb{N}\}, where 0=β0<β1<β2<0=\beta^{0}<\beta^{1}<\beta^{2}<\cdots. Consider the following ascending chain of ideals in 𝒪X,0s\mathcal{O}_{X,0}^{s}:

uβ1uβ1,uβ2uβ1,uβ2,uβ3\langle u^{\beta^{1}}\rangle\subset\langle u^{\beta^{1}},u^{\beta^{2}}\rangle\subset\langle u^{\beta^{1}},u^{\beta^{2}},u^{\beta^{3}}\rangle\subset\cdots

Since 𝒪X,0s\mathcal{O}_{X,0}^{s} is Noetherian, we have uβjuβ1,,uβmu^{\beta^{j}}\in\langle u^{\beta^{1}},\ldots,u^{\beta^{m}}\rangle, for some mm\in\mathbb{N} and for all jj\in\mathbb{N}. We claim that Γs=(β1,,βm)\Gamma^{s}=\mathbb{N}(\beta^{1},\ldots,\beta^{m}).

Indeed, let uβj=i=1mFiuβiu^{\beta^{j}}=\sum_{i=1}^{m}F_{i}u^{\beta^{i}}, for some Fi𝒪X,0sF_{i}\in\mathcal{O}_{X,0}^{s}. Since 𝒪X,0s{u1,,ud}\mathcal{O}_{X,0}^{s}\subset\mathbb{C}\{u_{1},\ldots,u_{d}\} it follows that uβj=uβuβiu^{\beta^{j}}=u^{\beta}u^{\beta^{i}}, for some ii and some monomial uβu^{\beta} of FiF_{i}. As before, we have βΓs\beta\in\Gamma^{s}. Hence, βj\beta^{j} is the sum of βi\beta^{i} plus an element βΓs\beta\in\Gamma^{s} and β<βj\beta<\beta^{j}. Continuing this way, we obtain that βj(β1,,βm)\beta^{j}\in\mathbb{N}(\beta^{1},\ldots,\beta^{m}). ∎

Remark 3.4.

The smooth normalization hypothesis plays a key role in the proofs of lemma 3.3 and theorem 3.2 since it implies that the ideal IΔI_{\Delta} is a homogeneous ideal in the ring of convergent power series {x1,,xd,y1,,yd}\mathbb{C}\{x_{1},\ldots,x_{d},y_{1},\ldots,y_{d}\} and allows us to use proposition 3.1.

We now know that for a germ (X,0)(X,0) of toric singularity with smooth normalization and associated semigroup Γ\Gamma, the Lipschitz saturated germ (Xs,0)(X^{s},0) is again a toric singularity with associated semigroup Γs\Gamma^{s}. In this setting we have ΓΓsd\Gamma\subset\Gamma^{s}\subset\mathbb{N}^{d} and we need to determine which elements αd\alpha\in\mathbb{N}^{d} we have to add to Γ\Gamma in order to obtain Γs\Gamma^{s}. Since many properties of a toric variety are encoded in its semigroup, we can use them to start discerning. This is the content of the following proposition.

Proposition 3.5.

Let (X,0)(X,0) be a germ of dd-dimensional toric singularity with smooth normalization. Let Γd\Gamma\subset\mathbb{N}^{d} be the associated semigroup and K+(Γ)K_{+}(\Gamma) the convex hull of Γ{0}\Gamma\setminus\{0\} in d\mathbb{R}^{d}. If αdK+(Γ)\alpha\in\mathbb{N}^{d}\setminus K_{+}(\Gamma) then αΓs\alpha\notin\Gamma^{s}.

Proof.

By [10, Chapter 5, theorem 3.14], the multiplicity of a toric germ is determined by the (normalized) volume of the complement of K+(Γ)K_{+}(\Gamma) in d\mathbb{N}^{d}. But we know from 1.2 that a germ (X,0)(X,0) and its Lipschitz saturation (Xs,0)(X^{s},0) have the same multiplicity, and so we must have that K+(Γ)=K+(Γs)K_{+}(\Gamma)=K_{+}(\Gamma^{s}) which finishes the proof. ∎

In the case of curves, this means that if mm is the minimal non-zero element of Γ\Gamma\subset\mathbb{N} then kk\in\mathbb{N}, with k<mk<m implies that kΓsk\notin\Gamma^{s} (see section 1). Recall that in this case mm is equal to the multiplicity of the curve.

Example 3.6.

The Whitney Umbrella.
The surface singularity (X,0)(3,0)(X,0)\subset(\mathbb{C}^{3},0) defined by the equation y2x2z=0y^{2}-x^{2}z=0 is a toric singularity with smooth normalization given by

(u,v)(u,uv,v2)(u,v)\mapsto(u,uv,v^{2})

and associated semigroup Γ2\Gamma\subset\mathbb{N}^{2} with minimal generating set {(1,0),(1,1),(0,2)}\{(1,0),(1,1),(0,2)\}. This translates to 𝒪X,0{u,uv,v2}{u,v}\mathcal{O}_{X,0}\cong\mathbb{C}\{u,uv,v^{2}\}\subset\mathbb{C}\{u,v\} and a point (a,b)Γs(a,b)\in\Gamma^{s} is identified with the monomial uavb𝒪X,0s{u,v}u^{a}v^{b}\in\mathcal{O}_{X,0}^{s}\subset\mathbb{C}\{u,v\}.

Refer to caption
Figure 1: The square points are not in Γ\Gamma.

Note that 2Γ={(0,2k+1)|k}\mathbb{N}^{2}\setminus\Gamma=\left\{(0,2k+1)\,|\,k\in\mathbb{N}\right\}. We will show that none of them are in Γs\Gamma^{s}. Hence, Γ=Γs\Gamma=\Gamma^{s}. In the proof of theorem 3.2 we showed that 𝒪X,0s={Γs}\mathcal{O}_{X,0}^{s}=\mathbb{C}\{\Gamma^{s}\}. We conclude that 𝒪X,0=𝒪X,0s\mathcal{O}_{X,0}=\mathcal{O}_{X,0}^{s} and so the Whitney Umbrella coincides with its Lipschitz saturation (Xs,0)(X^{s},0).

To begin with, the only point in 2K+(Γ)\mathbb{N}^{2}\setminus K_{+}(\Gamma) is (0,1)(0,1), and so (0,1)Γs(0,1)\notin\Gamma^{s} by the previous proposition. For the points of the form (0,r)(0,r) with r>1r>1 odd, consider the ideal

IΔ=x1y1,x1x2y1y2,x22y22{x1,x2,y1,y2}I_{\Delta}=\left<x_{1}-y_{1},x_{1}x_{2}-y_{1}y_{2},x_{2}^{2}-y_{2}^{2}\right>\mathbb{C}\left\{x_{1},x_{2},y_{1},y_{2}\right\}

Taking the arc φ:(,0)(2×2,0)\varphi:(\mathbb{C},0)\to\left(\mathbb{C}^{2}\times\mathbb{C}^{2},0\right) defined by t(tr+1,t,tr+2,t)t\mapsto(t^{r+1},t,t^{r+2},-t) we have the corresponding morphism of analytic algebras φ:{x1,x2,y1,y2}{t}\varphi^{*}:\mathbb{C}\left\{x_{1},x_{2},y_{1},y_{2}\right\}\to\mathbb{C}\{t\} such that

φ(x2ry2r)=2trφ(IΔ)=tr+1.\varphi^{*}(x_{2}^{r}-y_{2}^{r})=2t^{r}\notin\left<\varphi^{*}(I_{\Delta})\right>=\left<t^{r+1}\right>.

By [19, Thm 2.1] this implies that x2ry2rIΔ¯x_{2}^{r}-y_{2}^{r}\notin\overline{I_{\Delta}}, i.e. vr𝒪X,0sv^{r}\notin\mathcal{O}_{X,0}^{s}.

4 Some examples.

In this section we will show how to calculate the Lipschitz saturation of some families of toric singularities, starting with products of curves.

Let (X1,0)(X_{1},0) and (X2,0)(X_{2},0) be two germs of toric singularities of dimension 11 defined by the semigroups Γ1\Gamma_{1} and Γ2\Gamma_{2} with corresponding minimal generating sets 𝒜1={γ1,,γm}\mathcal{A}_{1}=\{\gamma_{1},\ldots,\gamma_{m}\} and 𝒜2={ω1,,ωn}\mathcal{A}_{2}=\{\omega_{1},\ldots,\omega_{n}\}. The germ (X,0)=(X1×X2,0)(X,0)=(X_{1}\times X_{2},0) is a toric surface singularity with semigroup Γ2\Gamma\subset\mathbb{N}^{2} generated by 𝒜={(γi,0),(0,ωj)}i,j\mathcal{A}=\left\{(\gamma_{i},0),(0,\omega_{j})\right\}_{i,j}, that is Γ=Γ1×Γ2\Gamma=\Gamma_{1}\times\Gamma_{2}. Note that the normalization of (X,0)(X,0) is smooth and the normalization map can be written as

η:(2,0)\displaystyle\eta:(\mathbb{C}^{2},0) (X,0)(m+n,0)\displaystyle\longrightarrow(X,0)\subset(\mathbb{C}^{m+n},0)
(u,v)\displaystyle(u,v) (uγ1,,uγm,vω1,,vωn).\displaystyle\mapsto\left(u^{\gamma_{1}},\ldots,u^{\gamma_{m}},v^{\omega_{1}},\ldots,v^{\omega_{n}}\right).
Proposition 4.1.

For a germ of surface singularity (X,0)=(X1×X2,0)(X,0)=(X_{1}\times X_{2},0) defined by a product of toric curves, the Lipschitz saturation (Xs,0)(X^{s},0) is a toric surface singularity with semigroup

Γs=Γ1s×Γ2s,\Gamma^{s}=\Gamma_{1}^{s}\times\Gamma_{2}^{s},

where Γ1s\Gamma_{1}^{s} and Γ2s\Gamma_{2}^{s} are the semigroups of the Lipschitz saturated curves (X1s,0)(X_{1}^{s},0) and (X2s,0)(X_{2}^{s},0) described in section 1.

Proof.

We know that 𝒪X,0s{u,v}\mathcal{O}_{X,0}^{s}\subset\mathbb{C}\{u,v\} is an analytic algebra generated by monomials, so we need to characterize them. A monomial uαvβ𝒪X,0su^{\alpha}v^{\beta}\in\mathcal{O}_{X,0}^{s} defines a meromorphic function on a neighborhood UU of the origin in XX which is locally Lipschitz with respect to the ambient metric. If we consider the normalization of (X,0)(X,0) as before

η:(2,0)\displaystyle\eta:(\mathbb{C}^{2},0) (X,0)(m+n,0)\displaystyle\longrightarrow(X,0)\subset(\mathbb{C}^{m+n},0)
(u,v)\displaystyle(u,v) (uγ1,,uγm,vω1,,vωn),\displaystyle\mapsto\left(u^{\gamma_{1}},\ldots,u^{\gamma_{m}},v^{\omega_{1}},\ldots,v^{\omega_{n}}\right),

then for any sufficiently small v0v_{0} the restriction of uαvβu^{\alpha}v^{\beta} to (X1×{v0ω},(0,v0ω))\left(X_{1}\times\{v_{0}^{\omega}\},(0,v_{0}^{\omega})\right) tells us that uαv0βu^{\alpha}v_{0}^{\beta} defines a meromorphic locally Lipschitz function on (X1,0)(X_{1},0) and so uα𝒪X1,0su^{\alpha}\in\mathcal{O}_{X_{1},0}^{s}; equivalently αΓ1s\alpha\in\Gamma_{1}^{s}. The same reasoning with the restriction to ({u0γ}×X2,(u0γ,0))\left(\{u_{0}^{\gamma}\}\times X_{2},(u_{0}^{\gamma},0)\right) tells us that βΓ2s\beta\in\Gamma_{2}^{s} and so (α,β)Γ1s×Γ2s(\alpha,\beta)\in\Gamma_{1}^{s}\times\Gamma_{2}^{s}.

On the other hand, in this setting we have the ideal IΔI_{\Delta} defined by

IΔ=x1γ1y1γ1,,x1γmy1γm,x2ω1y2ω1,,x2ωny2ωn{x1,x2,y1,y2}.I_{\Delta}=\left<x_{1}^{\gamma_{1}}-y_{1}^{\gamma_{1}},\ldots,x_{1}^{\gamma_{m}}-y_{1}^{\gamma_{m}},x_{2}^{\omega_{1}}-y_{2}^{\omega_{1}},\ldots,x_{2}^{\omega_{n}}-y_{2}^{\omega_{n}}\right>\mathbb{C}\{x_{1},x_{2},y_{1},y_{2}\}.

Let αΓ1s\alpha\in\Gamma_{1}^{s} then by definition we have

x1αy1αx1γ1y1γ1,,x1γmy1γm¯{x1,y1}.x_{1}^{\alpha}-y_{1}^{\alpha}\in\overline{\left<x_{1}^{\gamma_{1}}-y_{1}^{\gamma_{1}},\ldots,x_{1}^{\gamma_{m}}-y_{1}^{\gamma_{m}}\right>}\mathbb{C}\{x_{1},y_{1}\}.

In particular, x1αy1αIΔ¯x_{1}^{\alpha}-y_{1}^{\alpha}\in\overline{I_{\Delta}} and so uα𝒪X,0s{u,v}u^{\alpha}\in\mathcal{O}_{X,0}^{s}\subset\mathbb{C}\{u,v\}. Analogously for every βΓ2s\beta\in\Gamma_{2}^{s} we have vβ𝒪X,0sv^{\beta}\in\mathcal{O}_{X,0}^{s}. Since 𝒪X,0s\mathcal{O}_{X,0}^{s} is an analytic algebra, this implies that for every αΓ1s\alpha\in\Gamma_{1}^{s} and βΓ2s\beta\in\Gamma_{2}^{s} the monomial uαvβ𝒪X,0su^{\alpha}v^{\beta}\in\mathcal{O}_{X,0}^{s} which finishes the proof. ∎

Corollary 4.2.

Let (X,0)=(X1×X2,0)(X,0)=(X_{1}\times X_{2},0) be a product of toric curves. Then edim(Xs,0)=edim(X1s,0)+edim(X2s,0)\operatorname{edim}(X^{s},0)=\operatorname{edim}(X_{1}^{s},0)+\operatorname{edim}(X_{2}^{s},0). In addition, mult(Xs,0)=mult(X1s,0)mult(X2s,0)\operatorname{mult}(X^{s},0)=\operatorname{mult}(X_{1}^{s},0)\cdot\operatorname{mult}(X_{2}^{s},0).

Proof.

First, recall that the embedding dimension of the origin of a toric variety i.e., the dimension of its Zariski tangent space, coincides with the cardinality of the minimal generating set of the correspondig semigroup. On the other hand, the multiplicity at the origin of a toric variety is also described combinatorially in terms of the semigroup (see proposition 3.5). Hence, both assertions follow from proposition 4.1. ∎

Remark 4.3.

Notice that both proposition 4.1 and corollary 4.2 hold for the product of any finite number of toric curves, with the same proof.

Example 4.4.

Starting from the space curves (X1,0)(X_{1},0) and (X2,0)(X_{2},0) parametrized respectively by

u(u4,u6,u7),v(v6,v9,v11),u\longmapsto(u^{4},u^{6},u^{7}),\hskip 72.26999ptv\longmapsto(v^{6},v^{9},v^{11}),

we get the toric surface (X,0)(6,0)(X,0)\subset(\mathbb{C}^{6},0) of multiplicity 2424 and embedding dimension 66 defined by the ideal

IX=y2x3,c3a4b,b2a3,z2x2y{x,y,z,a,b,c}.I_{X}=\left<y^{2}-x^{3},c^{3}-a^{4}b,b^{2}-a^{3},z^{2}-x^{2}y\right>\mathbb{C}\{x,y,z,a,b,c\}.

The normalization map is given by:

η:(2,0)\displaystyle\eta:(\mathbb{C}^{2},0) (X,0)(6,0)\displaystyle\longrightarrow(X,0)\subset(\mathbb{C}^{6},0)
(u,v)\displaystyle(u,v) (u4,u6,u7,v6,v9,v11).\displaystyle\mapsto\left(u^{4},u^{6},u^{7},v^{6},v^{9},v^{11}\right).

Following the procedure described in section 1 we obtain that the semigroup Γ1s\Gamma_{1}^{s}\subset\mathbb{N} is generated by 𝒜1={4,6,7,9}\mathcal{A}_{1}=\{4,6,7,9\} and the semigroup Γ2s\Gamma_{2}^{s}\subset\mathbb{N} is generated by 𝒜2={6,9,11,13,14,16}\mathcal{A}_{2}=\{6,9,11,13,14,16\}. By proposition 4.1 the Lipschitz saturation (Xs,0)(10,0)(X^{s},0)\subset(\mathbb{C}^{10},0) is the toric singularity defined by the semigroup Γs2\Gamma^{s}\subset\mathbb{N}^{2} generated by the set

𝒜={(4,0),(6,0),(7,0),(9,0),(0,6),(0,9),(0,11),(0,13),(0,14),(0,16)},\mathcal{A}=\left\{(4,0),(6,0),(7,0),(9,0),(0,6),(0,9),(0,11),(0,13),(0,14),(0,16)\right\},

and with normalization map given by:

η:(2,0)\displaystyle\eta:(\mathbb{C}^{2},0) (Xs,0)(6,0)\displaystyle\longrightarrow(X^{s},0)\subset(\mathbb{C}^{6},0)
(u,v)\displaystyle(u,v) (u4,u6,u7,u9,v6,v9,v11,v13,v14,v16).\displaystyle\mapsto\left(u^{4},u^{6},u^{7},u^{9},v^{6},v^{9},v^{11},v^{13},v^{14},v^{16}\right).

(Xs,0)(X^{s},0) is a toric germ of multiplicity 2424 and embedding dimension 1010.

Since (X,0)(6,0)(X,0)\subset(\mathbb{C}^{6},0) is a germ of singular surface, we have that the cone C5(X,0)C_{5}(X,0) is of dimension 33 or 44 and so almost every linear projection

π:(6,0)\displaystyle\pi:(\mathbb{C}^{6},0) (4,0)\displaystyle\longrightarrow(\mathbb{C}^{4},0)
(z1z6)\displaystyle\begin{pmatrix}z_{1}\\ \vdots\\ z_{6}\end{pmatrix} (a11a16a41a46)(z1z6)\displaystyle\longmapsto\begin{pmatrix}a_{11}&\cdots&a_{16}\\ \vdots&\vdots&\vdots\\ a_{41}&\cdots&a_{46}\end{pmatrix}\begin{pmatrix}z_{1}\\ \vdots\\ z_{6}\end{pmatrix}

is generic, in the sense that it is transversal to this cone (see [13, Prop. 8.4.3]). Using proposition 1.4, for each such π\pi we get a germ of singular surface (Yπ,0):=(π(X),0)(4,0)(Y_{\pi},0):=(\pi(X),0)\subset(\mathbb{C}^{4},0) of multiplicity 2424 and embedding dimension at most 44, with normalization map (see the proof of proposition 1.4)

ηYπ:(2,0)\displaystyle\eta_{Y_{\pi}}:(\mathbb{C}^{2},0) (Yπ,0)\displaystyle\longrightarrow(Y_{\pi},0)
(u,v)\displaystyle(u,v) (a11a16a41a46)(u4u6u7v6v9v11)\displaystyle\longmapsto\begin{pmatrix}a_{11}&\cdots&a_{16}\\ \vdots&\vdots&\vdots\\ a_{41}&\cdots&a_{46}\end{pmatrix}\begin{pmatrix}u^{4}\\ u^{6}\\ u^{7}\\ v^{6}\\ v^{9}\\ v^{11}\end{pmatrix}

This gives us a family of surfaces (Yπ,0)(4,0)(Y_{\pi},0)\subset(\mathbb{C}^{4},0) that are not isomorphic to (X,0)(X,0) whose Lipschitz saturation (Yπs,0)(Y_{\pi}^{s},0) is toric and isomorphic to (Xs,0)(X^{s},0).

We will now a consider a family of hypersurfaces (X,0)(3,0)(X,0)\subset(\mathbb{C}^{3},0) with equation of the form

yNxαNzβ=0,y^{N}-x^{\alpha N}z^{\beta}=0,

where α,β1\alpha,\beta\geq 1 and  mcd(β,N)=1\text{ mcd}(\beta,N)=1. It is a family of toric surface singularities with semigroup Γ\Gamma generated by 𝒜={(1,0),(α,β),(0,N)}\mathcal{A}=\{(1,0),(\alpha,\beta),(0,N)\}.

Theorem 4.5.

Let (X,0)(3,0)(X,0)\subset(\mathbb{C}^{3},0) be the toric hypersurface singularity with normalization map given by

η:(2,0)\displaystyle\eta:(\mathbb{C}^{2},0) (X,0)\displaystyle\longrightarrow(X,0)
(u,v)\displaystyle(u,v) (u,uαvβ,vN),\displaystyle\mapsto\left(u,u^{\alpha}v^{\beta},v^{N}\right),

where α,β1\alpha,\beta\geq 1 and  mcd(β,N)=1\text{ mcd}(\beta,N)=1. Let TT\subset\mathbb{N} be the numerical semigroup generated by {N,β}\{N,\beta\}, and TsT^{s}\subset\mathbb{N} be its saturation as in section 1. The monomial uavb{u,v}u^{a}v^{b}\in\mathbb{C}\{u,v\} is in the Lipschitz saturation 𝒪X,0s\mathcal{O}_{X,0}^{s} if and only if b=mNb=mN for some mm\in\mathbb{N} or aαa\geq\alpha and bTsb\in T^{s}.

Proof.

In this setting the semigroup Γ\Gamma is generated by 𝒜={(1,0),(α,β),(0,N)}\mathcal{A}=\{(1,0),(\alpha,\beta),(0,N)\}, and by the proof of theorem 3.2 uavb𝒪X,0su^{a}v^{b}\in\mathcal{O}_{X,0}^{s} is equivalent to (a,b)Γs(a,b)\in\Gamma^{s}.

We first show that if b=mNb=mN for some mm\in\mathbb{N} or aαa\geq\alpha and bTsb\in T^{s} then (a,b)Γs(a,b)\in\Gamma^{s}. Suppose first that b=mNb=mN. Since (1,0),(0,N)Γ(1,0),(0,N)\in\Gamma, it follows that (a,b)ΓΓs(a,b)\in\Gamma\subset\Gamma^{s} for all aa\in\mathbb{N}.

Now suppose that aαa\geq\alpha and bTsb\in T^{s}. Since ΓΓs\Gamma\subset\Gamma^{s} we have that u𝒪X,0su\in\mathcal{O}_{X,0}^{s} and so it is enough to prove the statement for a=αa=\alpha. By definition uαvb𝒪X,0su^{\alpha}v^{b}\in\mathcal{O}_{X,0}^{s} if and only if x1αx2by1αy2bIΔ¯x_{1}^{\alpha}x_{2}^{b}-y_{1}^{\alpha}y_{2}^{b}\in\overline{I_{\Delta}} where

IΔ=x1y1,x1αx2βy1αy2β,x2Ny2N{x1,x2,y1,y2}.I_{\Delta}=\left<x_{1}-y_{1},x_{1}^{\alpha}x_{2}^{\beta}-y_{1}^{\alpha}y_{2}^{\beta},x_{2}^{N}-y_{2}^{N}\right>\mathbb{C}\left\{x_{1},x_{2},y_{1},y_{2}\right\}.

The assumption bTsb\in T^{s} means that vb𝒪C,0s{v}v^{b}\in\mathcal{O}_{C,0}^{s}\subset\mathbb{C}\{v\}, which can be rephrased in terms of integral closure of ideals by

x2by2bx2βy2β,x2Ny2N¯{x2,y2}.x_{2}^{b}-y_{2}^{b}\in\overline{\left<x_{2}^{\beta}-y_{2}^{\beta},x_{2}^{N}-y_{2}^{N}\right>}\mathbb{C}\{x_{2},y_{2}\}.

And so if we denote x2by2bx_{2}^{b}-y_{2}^{b} by f(x2,y2)f(x_{2},y_{2}) we have an integral dependence equation in {x2,y2}\mathbb{C}\{x_{2},y_{2}\} of the form:

fm+g1(x2,y2)fm1++gm(x2,y2)=0,f^{m}+g_{1}(x_{2},y_{2})f^{m-1}+\cdots+g_{m}(x_{2},y_{2})=0,

with gk(x2,y2)Jk=(x2Ny2N)i(x2βy2β)j|i+j=k{x2,y2}g_{k}(x_{2},y_{2})\in J^{k}=\left<(x_{2}^{N}-y_{2}^{N})^{i}(x_{2}^{\beta}-y_{2}^{\beta})^{j}\,|\,i+j=k\right>\mathbb{C}\{x_{2},y_{2}\}. Each gkg_{k} will then be of the form

gk(x2,y2)=j=0khj(x2,y2)(x2Ny2N)kj(x2βy2β)j.g_{k}(x_{2},y_{2})=\sum_{j=0}^{k}h_{j}(x_{2},y_{2})(x_{2}^{N}-y_{2}^{N})^{k-j}(x_{2}^{\beta}-y_{2}^{\beta})^{j}.

Multiplying the integral dependence equation by x1αmx_{1}^{\alpha m} we obtain:

(x1αf)m+x1αg1(x1αf)m1++x1α(m1)gm1x1αf+x1αmgm=0.(x_{1}^{\alpha}f)^{m}+x_{1}^{\alpha}g_{1}\left(x_{1}^{\alpha}f\right)^{m-1}+\cdots+x_{1}^{\alpha(m-1)}g_{m-1}x_{1}^{\alpha}f+x_{1}^{\alpha m}g_{m}=0. (1)

But now

x1αkgk(x2,y2)=j=0kx1α(kj)hj(x2,y2)(x2Ny2N)kj[x1α(x2βy2β)]j.x_{1}^{\alpha k}g_{k}(x_{2},y_{2})=\sum_{j=0}^{k}x_{1}^{\alpha(k-j)}h_{j}(x_{2},y_{2})(x_{2}^{N}-y_{2}^{N})^{k-j}\left[x_{1}^{\alpha}(x_{2}^{\beta}-y_{2}^{\beta})\right]^{j}.

Note that x1y1,x1αx2βy1αy2βIΔx_{1}-y_{1},x_{1}^{\alpha}x_{2}^{\beta}-y_{1}^{\alpha}y_{2}^{\beta}\in I_{\Delta} implies that x1α(x2βy2β)IΔx_{1}^{\alpha}(x_{2}^{\beta}-y_{2}^{\beta})\in I_{\Delta}. In particular we get

(x2Ny2N)kj[x1α(x2βy2β)]jIΔk,(x_{2}^{N}-y_{2}^{N})^{k-j}\left[x_{1}^{\alpha}(x_{2}^{\beta}-y_{2}^{\beta})\right]^{j}\in I_{\Delta}^{k},

and so x1αkgkIΔkx_{1}^{\alpha k}g_{k}\in I_{\Delta}^{k}. This implies that equation (1) is an integral dependence equation for x1αfx_{1}^{\alpha}f over IΔI_{\Delta}. Finally x1αf=x1α(x2by2b)IΔ¯x_{1}^{\alpha}f=x_{1}^{\alpha}\left(x_{2}^{b}-y_{2}^{b}\right)\in\overline{I_{\Delta}} and x1y1IΔx_{1}-y_{1}\in I_{\Delta} imply x1αx2by1αy2bIΔ¯x_{1}^{\alpha}x_{2}^{b}-y_{1}^{\alpha}y_{2}^{b}\in\overline{I_{\Delta}} which is what we wanted to prove.

Now we prove that (a,b)Γs(a,b)\in\Gamma^{s} implies b=mNb=mN for some mm\in\mathbb{N} or aαa\geq\alpha and bTsb\in T^{s}.

If b=mNb=mN for some mm\in\mathbb{N}, we are done. Assume that bmNb\neq mN for all mm\in\mathbb{N}. We show that aαa\geq\alpha and bTsb\in T^{s}.

Note that for any u00u_{0}\neq 0 we have an embedding of the plane toric curve (C,0)(C,0), with semigroup TT generated by {N,β}\{N,\beta\} and defined by yNzβ=0y^{N}-z^{\beta}=0, via the map

(C,0)\displaystyle(C,0) (X,(u0,0,0))\displaystyle\hookrightarrow\left(X,(u_{0},0,0)\right)
(y,z)\displaystyle(y,z) (u0,u0αy,z)\displaystyle\mapsto(u_{0},u_{0}^{\alpha}y,z)
(vβ,vN)\displaystyle(v^{\beta},v^{N}) (u0,u0αvβ,vN).\displaystyle\mapsto(u_{0},u_{0}^{\alpha}v^{\beta},v^{N}).

By remark 1.2 a monomial uavb𝒪X,0su^{a}v^{b}\in\mathcal{O}_{X,0}^{s} defines a locally Lipschitz meromorphic function on a small enough neighborhood UU of 0 in XX. For any small enough u0u_{0} it restricts to a locally Lipschitz meromorphic function u0avbu_{0}^{a}v^{b} on a neighborhood of (u0,0,0)(u_{0},0,0) in the embedded curve CC. In particular vb𝒪C,0sv^{b}\in\mathcal{O}_{C,0}^{s}, or equivalently bTsb\in T^{s}.

To show that aαa\geq\alpha we prove that 0a<α0\leq a<\alpha and bmNb\neq mN implies (a,b)Γs(a,b)\notin\Gamma^{s}. We consider two cases: a=0a=0 and 0<a<α0<a<\alpha.

Following example 3.6, note that all points of the form (0,k)(0,k) with k<Nk<N are in 2K+(Γ)\mathbb{N}^{2}\setminus K_{+}(\Gamma) and so they are not in Γs\Gamma^{s} by proposition 3.5. For the points of the form (0,k)(0,k) with k>Nk>N, kmNk\neq mN, consider the ideal

IΔ=x1y1,x1αx2βy1αy2β,x2Ny2N{x1,x2,y1,y2}.I_{\Delta}=\left<x_{1}-y_{1},x_{1}^{\alpha}x_{2}^{\beta}-y_{1}^{\alpha}y_{2}^{\beta},x_{2}^{N}-y_{2}^{N}\right>\mathbb{C}\left\{x_{1},x_{2},y_{1},y_{2}\right\}.

Let θ\theta\in\mathbb{C} be a primitive NN-th root of unity and consider the arc

φ:(,0)\displaystyle\varphi:(\mathbb{C},0) (2×2,0)\displaystyle\to\left(\mathbb{C}^{2}\times\mathbb{C}^{2},0\right)
t\displaystyle t (tk+1,t,tk+2,θt).\displaystyle\mapsto(t^{k+1},t,t^{k+2},\theta t).

We have the corresponding morphism of analytic algebras φ:{x1,x2,y1,y2}{t}\varphi^{*}:\mathbb{C}\left\{x_{1},x_{2},y_{1},y_{2}\right\}\to\mathbb{C}\{t\} such that

φ(IΔ){t}\displaystyle\left<\varphi^{*}(I_{\Delta})\right>\mathbb{C}\{t\} =φ(x1y1),φ(x1αx2βy1αy2β),φ(x2Ny2N)\displaystyle=\left<\varphi^{*}(x_{1}-y_{1}),\varphi^{*}(x_{1}^{\alpha}x_{2}^{\beta}-y_{1}^{\alpha}y_{2}^{\beta}),\varphi^{*}(x_{2}^{N}-y_{2}^{N})\right>
=(1t)tk+1,(1θβtα)tα(k+1)+β,0\displaystyle=\left<(1-t)t^{k+1},(1-\theta^{\beta}t^{\alpha})t^{\alpha(k+1)+\beta},0\right>
=tk+1{t}.\displaystyle=\left<t^{k+1}\right>\mathbb{C}\{t\}.

In particular,

φ(x2ky2k)=(1θk)tkφ(IΔ)=tk+1.\varphi^{*}(x_{2}^{k}-y_{2}^{k})=(1-\theta^{k})t^{k}\notin\left<\varphi^{*}(I_{\Delta})\right>=\left<t^{k+1}\right>.

By [19, Thm 2.1] this impliest that x2ky2kIΔ¯x_{2}^{k}-y_{2}^{k}\notin\overline{I_{\Delta}}, i.e. vk𝒪X,0sv^{k}\notin\mathcal{O}_{X,0}^{s}.

All that is left to prove is that for 0<a<α0<a<\alpha and bmNb\neq mN the monomial uavbu^{a}v^{b} is not in 𝒪X,0s\mathcal{O}_{X,0}^{s}. We will once again use the arc criterion for integral dependence, but this time with the arc

ψ:(,0)\displaystyle\psi:(\mathbb{C},0) (2×2,0)\displaystyle\to\left(\mathbb{C}^{2}\times\mathbb{C}^{2},0\right)
t\displaystyle t (tb+1,t,tb+1+tr,θt),\displaystyle\mapsto(t^{b+1},t,t^{b+1}+t^{r},\theta t),

where θ\theta\in\mathbb{C} is a primitive NN-th root of unity. In this setting the image of IΔI_{\Delta} by the morphism ψ\psi^{*} in {t}\mathbb{C}\{t\} is of the form:

φ(IΔ){t}\displaystyle\left<\varphi^{*}(I_{\Delta})\right>\mathbb{C}\{t\} =ψ(x1y1),ψ(x1αx2βy1αy2β),ψ(x2Ny2N)\displaystyle=\left<\psi^{*}(x_{1}-y_{1}),\psi^{*}(x_{1}^{\alpha}x_{2}^{\beta}-y_{1}^{\alpha}y_{2}^{\beta}),\psi^{*}(x_{2}^{N}-y_{2}^{N})\right>
=tr,[1θβ(1+trb1)α]tα(b+1)+β,0\displaystyle=\left<-t^{r},\left[1-\theta^{\beta}\left(1+t^{r-b-1}\right)^{\alpha}\right]t^{\alpha(b+1)+\beta},0\right>
=tα(b+1)+β{t} for r big enough.\displaystyle=\left<t^{\alpha(b+1)+\beta}\right>\mathbb{C}\{t\}\hskip 7.22743pt\text{ for }r\text{ big enough.}

On the other hand we have

ψ(x1ax2by1ay2b)=[1θb(1+trb1)a]ta(b+1)+b.\psi^{*}\left(x_{1}^{a}x_{2}^{b}-y_{1}^{a}y_{2}^{b}\right)=\left[1-\theta^{b}\left(1+t^{r-b-1}\right)^{a}\right]t^{a(b+1)+b}.

Using that 0<a<α0<a<\alpha it is straightforward to verify that for every b0b\geq 0

α(b+1)+β>a(b+1)+b\alpha(b+1)+\beta>a(b+1)+b

and so x1ax2by1ay2bIΔ¯x_{1}^{a}x_{2}^{b}-y_{1}^{a}y_{2}^{b}\notin\overline{I_{\Delta}}, i.e. uavb𝒪X,0su^{a}v^{b}\notin\mathcal{O}_{X,0}^{s}.

Corollary 4.6.

Let (X,0)(3,0)(X,0)\subset(\mathbb{C}^{3},0) be a germ of toric hypersurface singularity as in theorem 4.5. Then (Xs,0)(X^{s},0) is a toric surface singularity of multiplicity NN and embedding dimension N+1N+1.

Proof.

By the combinatorial description of multiplicity in toric geometry, it follows that N=mult(X,0)=mult(Xs,0)N=\operatorname{mult}(X,0)=\operatorname{mult}(X^{s},0). Similarly, the embedding dimension of (Xs,0)(X^{s},0) corresponds to the cardinality of the minimal set of generators of Γs\Gamma^{s}. We exhibit this minimal set of generators and show that it has cardinality N+1N+1.

Theorem 4.5 states that (a,b)Γs(a,b)\in\Gamma^{s} if and only if b=mNb=mN for some mm\in\mathbb{N} or aαa\geq\alpha and bTsb\in T^{s}. We divide the proof in two cases.

Case N<βN<\beta. Write β=kN+l\beta=kN+l, k1k\geq 1 and 0<l<N0<l<N. By the algorithm for computing TsT^{s} we obtain Ts={0,N,2N,,kN,β,β+1,β+2,}T^{s}=\{0,N,2N,\ldots,kN,\beta,\beta+1,\beta+2,\cdots\} (see section 1). Consider the sets

𝒜\displaystyle\mathcal{A} ={(1,0),(α,β),(0,N)},\displaystyle=\{(1,0),(\alpha,\beta),(0,N)\},
\displaystyle\mathcal{B} ={(α,β+1),,(α,β+N1)}{(α,(k+1)N)}.\displaystyle=\{(\alpha,\beta+1),\ldots,(\alpha,\beta+N-1)\}\setminus\{(\alpha,(k+1)N)\}.

We claim that Γs=(𝒜)\Gamma^{s}=\mathbb{N}(\mathcal{A}\cup\mathcal{B}). Firstly observe that 𝒜Γs\mathcal{A}\cup\mathcal{B}\subset\Gamma^{s}. Now let (a,b)Γs(a,b)\in\Gamma^{s}. If b=mNb=mN then (a,b)Γ=(𝒜)(𝒜)(a,b)\in\Gamma=\mathbb{N}(\mathcal{A})\subset\mathbb{N}(\mathcal{A}\cup\mathcal{B}). In particular, this holds for the element (α,(k+1)N)(\alpha,(k+1)N). Now assume that aαa\geq\alpha and bTsb\in T^{s}. Since (1,0)𝒜(1,0)\in\mathcal{A} it is enough to consider a=αa=\alpha.

  • Suppose b<βb<\beta. Then b=mNb=mN for some mm\in\mathbb{N}. Hence (α,b)(𝒜)(\alpha,b)\in\mathbb{N}(\mathcal{A}\cup\mathcal{B}).

  • Suppose b=βb=\beta. Then (α,b)𝒜(𝒜)(\alpha,b)\in\mathcal{A}\subset\mathbb{N}(\mathcal{A}\cup\mathcal{B}).

  • Suppose β+1bβ+N1\beta+1\leq b\leq\beta+N-1, b(α,(k+1)N)b\neq(\alpha,(k+1)N). Then (α,b)(𝒜)(\alpha,b)\in\mathcal{B}\subset\mathbb{N}(\mathcal{A}\cup\mathcal{B}).

  • Suppose β+Nb\beta+N\leq b. Write bβ=rN+sb-\beta=rN+s, r1r\geq 1, 0s<N0\leq s<N. Then (α,b)=(α,β+rN+s)=(α,β+s)+r(0,N)(𝒜)(\alpha,b)=(\alpha,\beta+rN+s)=(\alpha,\beta+s)+r(0,N)\in\mathbb{N}(\mathcal{A}\cup\mathcal{B}).

Now we show that 𝒜\mathcal{A}\cup\mathcal{B} is minimal as a generating set. Indeed, first notice that no element of 𝒜\mathcal{A} can be generated by \mathcal{B} and viceversa (because of the second entry of the vectors). Similarly, for each (α,β+i)(\alpha,\beta+i)\in\mathcal{B} it follows that (α,β+i)(𝒜{(α,β+i)})(\alpha,\beta+i)\notin\mathbb{N}(\mathcal{A}\cup\mathcal{B}\setminus\{(\alpha,\beta+i)\}) (because of the first entry of the vectors). Hence 𝒜\mathcal{A}\cup\mathcal{B} is the minimal generating set of Γs\Gamma^{s} and has cardinality N+1N+1.

Case β<N\beta<N. Write N=kβ+lN=k\beta+l, k1k\geq 1 and 0<l<β0<l<\beta. We compute TsT^{s} as before: Ts={0,β,,kβ,N,N+1,}T^{s}=\{0,\beta,\ldots,k\beta,N,N+1,\cdots\}. Consider the sets

𝒜=\displaystyle\mathcal{A}= {(1,0),(α,β),(0,N)},\displaystyle\{(1,0),(\alpha,\beta),(0,N)\},
=\displaystyle\mathcal{B}= {(α,2β),(α,3β),,(α,kβ)}\displaystyle\{(\alpha,2\beta),(\alpha,3\beta),\ldots,(\alpha,k\beta)\}
[{(α,N+1),,(α,N+(N1))}{(α,N+β),,(α,N+kβ)}].\displaystyle\cup\big{[}\{(\alpha,N+1),\ldots,(\alpha,N+(N-1))\}\setminus\{(\alpha,N+\beta),\ldots,(\alpha,N+k\beta)\}\big{]}.

We claim that Γs=(𝒜)\Gamma^{s}=\mathbb{N}(\mathcal{A}\cup\mathcal{B}). Firstly observe that 𝒜Γs\mathcal{A}\cup\mathcal{B}\subset\Gamma^{s}. Now let (a,b)Γs(a,b)\in\Gamma^{s}. If b=mNb=mN then (a,b)Γ=(𝒜)(𝒜)(a,b)\in\Gamma=\mathbb{N}(\mathcal{A})\subset\mathbb{N}(\mathcal{A}\cup\mathcal{B}). Now assume that aαa\geq\alpha and bTsb\in T^{s}. As before, it is enough to consider a=αa=\alpha.

  • For each i{1,,k}i\in\{1,\ldots,k\} we have (α,N+iβ)=(0,N)+(α,iβ)(𝒜)(\alpha,N+i\beta)=(0,N)+(\alpha,i\beta)\in\mathbb{N}(\mathcal{A}\cup\mathcal{B}).

  • Suppose b<Nb<N. Then b=mβb=m\beta for some mm\in\mathbb{N}. Hence (α,b)(𝒜)(\alpha,b)\in\mathbb{N}(\mathcal{A}\cup\mathcal{B}).

  • Suppose b=Nb=N. Then (α,b)(𝒜)(𝒜)(\alpha,b)\in\mathbb{N}(\mathcal{A})\subset\mathbb{N}(\mathcal{A}\cup\mathcal{B}).

  • Suppose N+1bN+(N1)N+1\leq b\leq N+(N-1), b(α,N+iβ)b\neq(\alpha,N+i\beta), i{1,,k}i\in\{1,\ldots,k\}. Then (α,b)(𝒜)(\alpha,b)\in\mathcal{B}\subset\mathbb{N}(\mathcal{A}\cup\mathcal{B}).

  • Suppose 2Nb2N\leq b. Write bN=rN+sb-N=rN+s, r1r\geq 1, 0s<N0\leq s<N. Then (α,b)=(α,N+rN+s)=r(0,N)+(α,N+s)(𝒜)(\alpha,b)=(\alpha,N+rN+s)=r(0,N)+(\alpha,N+s)\in\mathbb{N}(\mathcal{A}\cup\mathcal{B}).

A similar analysis as in the previous case shows that 𝒜\mathcal{A}\cup\mathcal{B} is the minimal generating set of Γs\Gamma^{s} and has cardinality N+1N+1. ∎

Example 4.7.

Consider the toric hypersurface singularity (X,0)(3,0)(X,0)\subset(\mathbb{C}^{3},0) with normalization map

η:(2,0)\displaystyle\eta:(\mathbb{C}^{2},0) (X,0)\displaystyle\longrightarrow(X,0)
(u,v)\displaystyle(u,v) (u,u3v11,v5).\displaystyle\mapsto\left(u,u^{3}v^{11},v^{5}\right).

It is defined by the equation y5x15z11=0y^{5}-x^{15}z^{11}=0 and so it has multiplicity 55. Following the notation of theorem 4.5 we have the semigroup TT\subset\mathbb{N} generated by {5,11}\{5,11\} and its saturation TsT^{s}\subset\mathbb{N} with minimal generating set {5,11,12,13,14}\{5,11,12,13,14\}.

Refer to caption
Figure 2: The integral points of the shaded region are contained in Γs\Gamma^{s}. The highlighted points mark the minimal generating set of Γs\Gamma^{s}.

From the previous corollary we have the semigroup Γs\Gamma^{s} associated to the Lipschitz saturation (Xs,0)(X^{s},0) with minimal generating set

𝒜s={(1,0),(3,11),(3,12),(3,13),(3,14),(0,5)},\mathcal{A}^{s}=\{(1,0),(3,11),(3,12),(3,13),(3,14),(0,5)\},

normalization map

η:(2,0)\displaystyle\eta:(\mathbb{C}^{2},0) (Xs,0)(6,0)\displaystyle\longrightarrow(X^{s},0)\subset(\mathbb{C}^{6},0)
(u,v)\displaystyle(u,v) (u,u3v11,u3v12,u3v13,u3v14,v5),\displaystyle\mapsto\left(u,u^{3}v^{11},u^{3}v^{12},u^{3}v^{13},u^{3}v^{14},v^{5}\right),

and embedding dimension 66.

Interchanging the roles of 55 and 1111 we get the following example.

Example 4.8.

Consider the toric hypersurface singularity (X,0)(3,0)(X,0)\subset(\mathbb{C}^{3},0) with normalization map

η:(2,0)\displaystyle\eta:(\mathbb{C}^{2},0) (X,0)\displaystyle\longrightarrow(X,0)
(u,v)\displaystyle(u,v) (u,u3v5,v11).\displaystyle\mapsto\left(u,u^{3}v^{5},v^{11}\right).

It is defined by the equation y11x33z5=0y^{11}-x^{33}z^{5}=0 and so it has multiplicity 1111. Following the notation of theorem 4.5 we have again the semigroup TT\subset\mathbb{N} generated by {5,11}\{5,11\} and its saturation TsT^{s}\subset\mathbb{N} with minimal generating set {5,11,12,13,14}\{5,11,12,13,14\}.

Refer to caption
Figure 3: The integral points of the shaded region are contained in Γs\Gamma^{s}. The highlighted points mark the minimal generating set of Γs\Gamma^{s}.

From the previous corollary we have the semigroup Γs\Gamma^{s} associated to the Lipschitz saturation (Xs,0)(X^{s},0) with minimal generating set

𝒜s={(1,0),(3,5),(3,10),(3,12),(3,13),(3,14),(3,15),(3,17),(3,18),(3,19),(3,20),(0,11)},\mathcal{A}^{s}=\{(1,0),(3,5),(3,10),(3,12),(3,13),(3,14),(3,15),(3,17),(3,18),(3,19),(3,20),(0,11)\},

normalization map

η:(2,0)\displaystyle\eta:(\mathbb{C}^{2},0) (Xs,0)(12,0)\displaystyle\longrightarrow(X^{s},0)\subset(\mathbb{C}^{12},0)
(u,v)\displaystyle(u,v) (u,u3v5,u3v10,u3v12,u3v13,u3v14,u3v15,u3v17,u3v18,u3v19,u3v20,v11),\displaystyle\mapsto\left(u,u^{3}v^{5},u^{3}v^{10},u^{3}v^{12},u^{3}v^{13},u^{3}v^{14},u^{3}v^{15},u^{3}v^{17},u^{3}v^{18},u^{3}v^{19},u^{3}v^{20},v^{11}\right),

and embedding dimension 1212.

Note that in both examples we have (3,10)+2Γs(3,10)+\mathbb{N}^{2}\subset\Gamma^{s}.

Remark 4.9.

Recall from section 1 that the Lipschitz saturation of an irreducible curve has multiplicity equal to its embedding dimension. The results and examples from this section shows that there is no general relation among the embedding dimension and the multiplicity of the Lipschitz saturation in higher dimensions.

Remark 4.10.

Contrary to the case of curves, for the moment it is not clear that there exists an explicit algorithm to compute the semigroup Γs\Gamma^{s} from the semigroup Γ\Gamma, in general. We proved in theorem 3.2 that Γs\Gamma^{s} is finitely generated by Noetherian arguments, hence we do not have a constructive procedure to obtain a set of generators. However, the same theorem shows that the toric structure is preserved under Lipschitz saturation so, in principle, there should be a semigroup operation that provides Γs\Gamma^{s}. It remains an open question to find an algorithm that produces generators for Γs\Gamma^{s} in general.

Acknowledgements

The authors would like to thank professors P. Gonzalez Perez, C. Huneke and I. Swanson for the fruitful e-mail exchanges that greatly helped in the preparation of this work. They also acknowledge support by PAPIIT grant IN117523 and CONAHCYT grant CF-2023-G-33. A. Giles Flores acknowledges support by UAA grants PIM21-1 and PIM24-7.

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D. Duarte, Centro de Ciencias Matemáticas, UNAM.
E-mail: adduarte@matmor.unam.mx
A. Giles Flores, Universidad Autónoma de Aguascalientes.
Email: arturo.giles@edu.uaa.mx