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Hodge-Deligne and Poincaré polynomials of M‾1,n\overline{\mathcal M}_{1,n}

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Abstract

By studying wall crossings of Hassett moduli spaces of weighted pointed curves, we prove a recursive formula that reduces the computation of the cohomology of M‾g,n\overline{\mathcal M}_{g,n} to that of the moduli space M‾g,(0+)n\overline{\mathcal M}_{g,(0^+)^n} of stable pointed curves of minimal weights. For g=1g=1, we further prove an explicit formula for the Hodge-Deligne and Poincaré polynomials of M‾1,(0+)n\overline{\mathcal M}_{1,(0^+)^n}. Combining these, we prove formulas that enable us to compute the cohomology of M‾1,n\overline{\mathcal M}_{1,n} efficiently.

Introduction

The moduli space M‾g,n\overline{\mathcal{M}}_{g,n} of stable curves of genus gg with nn marked points is one of the most important objects in algebraic geometry [9, 15]. It parametrizes connected projective curves CC of arithmetic genus gg with at worst nodal singularities together with nn ordered smooth marked points p1,⋯ ,pnp_1,\cdots,p_n in CC such that

(1) pip_i are all distinct and

(2) ωC(∑ipi)\omega_C\left(\sum_i p_i\right) is ample.

It is a smooth proper Deligne-Mumford stack with projective coarse moduli space. It plays a fundamental role in modern enumerative geometry and serves as a model for moduli spaces of higher dimensional varieties. For over half a century, much effort has been exerted to understand the geometry and topology of M‾g,n\overline{\mathcal{M}}_{g,n} and there has been a constant stream of new discoveries even until now [1, 2, 4, 6, 7, 8, 13].

In this paper, we focus on the cohomology of M‾1,n\overline{\mathcal{M}}_{1,n}. In principle, the cohomology H∗(M‾1,n)H^*(\overline{\mathcal{M}}_{1,n}) can be computed by [10] which gives a formula for the SnS_n-equivariant Hodge-Deligne polynomial of M‾1,n\overline{\mathcal{M}}_{1,n}. Hence we can compute the ordinary Hodge-Deligne polynomial as well as the SnS_n-action on the cohomology. Unfortunately, the formula is rather difficult to use for practical computation: We first need to compute the equivariant Hodge-Deligne polynomials of M‾1,n\overline{\mathcal{M}}_{1,n}, M‾0,n\overline{\mathcal{M}}_{0,n} and M‾0,n\overline{\mathcal{M}}_{0,n} for all nn and then expand a power series after applying the plethystic composition. As far as we know, computation for M‾1,n\overline{\mathcal{M}}_{1,n} has been worked out only for nn up to 20 [3].

In contrast, the computation of the Poincaré polynomial of M‾0,n\overline{\mathcal{M}}_{0,n} is much easier due to an explicit recursive formula [16] which can be proved by Keel’s blowup construction [14]. Therefore it seems reasonable to ask the following.

Question 1.1. Is there an explicit recursive formula for the Poincaré and Hodge-Deligne polynomials of M‾1,n\overline{\mathcal{M}}_{1,n}?

The purpose of this paper is to provide a positive answer to this question so that we get a new and effective way to compute the Hodge and Betti numbers of M‾1,n\overline{\mathcal{M}}_{1,n}.

Our computation of H∗(M‾1,n)H^*(\overline{\mathcal{M}}_{1,n}) is achieved in two stages. We first reduce the computation to a simpler moduli space M‾1,(0+)n\overline{\mathcal{M}}_{1,(0+)^n}, where 0+0^+ denotes a positive rational number sufficiently close to 0. We note that many of the strata in M‾1,n\overline{\mathcal{M}}_{1,n} disappear and the computation becomes much easier if we allow all the marked points to coincide. This happens in the moduli space M‾1,(0+)n\overline{\mathcal{M}}_{1,(0+)^n} of stable pointed curves with weight 0+0^+ for each marked point [12]. By studying wall crossings in Hassett’s moduli spaces of weighted pointed curves, we prove the following.

Theorem 1.2 (Theorem 3.1). Let g≥1g \ge1 and fix a motivic invariant H\mathbf{H} satisfying the blowup formula (2.2). Let M‾g,r∣s=M‾g,(1r,(0+)s)\overline{\mathcal{M}}_{g,r|s}=\overline{\mathcal{M}}_{g,(1^r,(0^+)^s)} be the moduli space of stable curves of genus gg with rr points of weight 11 and ss points of weight 0+0^+. Let Hr∣s:=HM‾g,r∣s\mathbf{H}_{r|s}:=\mathbf{H}_{\overline{\mathcal{M}}_{g,r|s}}. Then for r,s≥0r,s\ge0 with r+s>0r+s>0 and n>0n>0, the following hold:

Hr∣s=H0∣r+s+∑j=1min⁡(r,r+s−2)∑k=0r+s−j−2(r+s−jk)Hj∣k⋅(HPr+s−j−k−1−1).(1)\mathbf{H}_{r|s}=\mathbf{H}_{0|r+s}+\sum_{j=1}^{\min(r,r+s-2)}\sum_{k=0}^{r+s-j-2}\binom{r+s-j}{k}\mathbf{H}_{j|k}\cdot\left(\mathbf{H}_{\mathbb{P}^{r+s-j-k-1}}-1\right). \tag*{(1)}
HM‾g,n=Hn∣0=H0∣n+∑j=1n−2∑k=0n−j−2(n−jk)Hj∣k⋅(HPn−j−k−1−1).(2)\mathbf{H}_{\overline{\mathcal{M}}_{g,n}}=\mathbf{H}_{n|0}=\mathbf{H}_{0|n}+\sum_{j=1}^{n-2}\sum_{k=0}^{n-j-2}\binom{n-j}{k}\mathbf{H}_{j|k}\cdot\left(\mathbf{H}_{\mathbb{P}^{n-j-k-1}}-1\right). \tag*{(2)}

All Hr∣s\mathbf{H}_{r|s} are recursively determined by (1.1) if we know H0∣n=HM‾g,(0+)n\mathbf{H}_{0|n}=\mathbf{H}_{\overline{\mathcal{M}}_{g,(0^+)^n}} for all nn.

Next we compute the cohomology of M‾1,(0+)n\overline{\mathcal{M}}_{1,(0^+)^n} piece by piece. Let

π:M‾1,(0+)n⟶M‾1,0+=M‾1,1\pi:\overline{\mathcal{M}}_{1,(0^+)^n}\longrightarrow\overline{\mathcal{M}}_{1,0^+}=\overline{\mathcal{M}}_{1,1}

be the morphism that forgets all the marked points except the first. The inverse image In=π−1(M1,1)\mathcal{I}_n=\pi^{-1}(\mathcal{M}_{1,1}) of M1,1\mathcal{M}_{1,1} is the (n−1)(n-1)-fold fiber product of the universal curve

q:C⟶M1,1=SL⁡2(Z)\H,H={z∈C∣Im⁡z>0}q:\mathcal{C}\longrightarrow\mathcal{M}_{1,1}=\operatorname{SL}_2(\mathbb{Z})\backslash\mathbb{H},\qquad\mathbb{H}=\{z\in\mathbb{C}\mid\operatorname{Im}z>0\}

and we have

Rπ∗QIn=(Rq∗QC)⊗n−1=((Q⊕Q[−2])⊕V[−1])⊗n−1(3)R\pi_*\mathbb{Q}_{\mathcal{I}_n}=(Rq_*\mathbb{Q}_{\mathcal{C}})^{\otimes n-1}=\left((\mathbb{Q}\oplus\mathbb{Q}[-2])\oplus V[-1]\right)^{\otimes n-1} \tag*{(3)}

by the relative Künneth formula, where V=R1q∗QV=R^1q_*\mathbb{Q}. Note that Hc∗(M1,1,V⊗k)=0H_c^*(\mathcal{M}_{1,1},V^{\otimes k})=0 for kk odd by the action of the generic stabilizer −I∈SL⁡2(Z)-I\in\operatorname{SL}_2(\mathbb{Z}). By expanding the right hand side of (3) and applying the Clebsch-Gordan rule, the computation of Hc∗(In)H_c^*(\mathcal{I}_n) is reduced to that of Hc∗(M1,1,Sym⁡2jV)H_c^*(\mathcal{M}_{1,1},\operatorname{Sym}^{2j}V) which can be obtained by the Eichler-Shimura isomorphism (cf. Lemma 4.2). Combining these, we find that the Hodge-Deligne polynomial of the interior In\mathcal{I}_n is (cf. Proposition 4.1)

∑j=0⌊n−12⌋(n−12j)(uv+1)n−1−2j(αjj(uv)j+1−∑i=0j−1αij(uv)i)\sum_{j=0}^{\left\lfloor\frac{n-1}{2}\right\rfloor}\binom{n-1}{2j}(uv+1)^{n-1-2j}\left(\alpha_{jj}(uv)^{j+1}-\sum_{i=0}^{j-1}\alpha_{ij}(uv)^i\right)
−∑j=0⌊n−12⌋(n−12j)(uv+1)n−1−2j∑i=0j−1αijβ2j−2i+2(uv)i(u2j−2i+1+v2j−2i+1)(4)-\sum_{j=0}^{\left\lfloor\frac{n-1}{2}\right\rfloor}\binom{n-1}{2j}(uv+1)^{n-1-2j}\sum_{i=0}^{j-1}\alpha_{ij}\beta_{2j-2i+2}(uv)^i\left(u^{2j-2i+1}+v^{2j-2i+1}\right) \tag*{(4)}

where

αij=(2ji)−(2ji−1)\alpha_{ij}=\binom{2j}{i}-\binom{2j}{i-1}

and

βk={⌊k12⌋−1if k≡2(mod12),⌊k12⌋if k≢2(mod12).\beta_k= \begin{cases} \left\lfloor\frac{k}{12}\right\rfloor-1 & \text{if }k\equiv2\pmod{12},\\ \left\lfloor\frac{k}{12}\right\rfloor& \text{if }k\not\equiv2\pmod{12}. \end{cases}

The complement Bn=π−1(∞)=M‾1,n−In\mathcal{B}_n=\pi^{-1}(\infty)=\overline{\mathcal{M}}_{1,n}-\mathcal{I}_n consists of pointed rational nodal curves. Let Bn,j⊂M‾1,n\mathcal{B}_{n,j}\subset\overline{\mathcal{M}}_{1,n} be the locus of pointed rational curves whose dual graphs are necklaces with jj vertices. It is obvious that there are γn,j\gamma_{n,j} dual graphs with jj vertices, where

γn,j={(nj)(j−1)!2for j>2,1for j=1,2n−1−1for j=2.\gamma_{n,j}= \begin{cases} \binom{n}{j}\dfrac{(j-1)!}{2} & \text{for }j>2,\\ 1 & \text{for }j=1,\\ 2^{n-1}-1 & \text{for }j=2. \end{cases}

denotes the Stirling number of the second kind. For j≥2j\ge2, Bn,j≅(C∗)n−j\mathcal{B}_{n,j}\cong(\mathbb{C}^*)^{n-j} and hence Hc∗(Bn,j)H_c^*(\mathcal{B}_{n,j}) has Hodge-Deligne polynomial γn,j(uv−1)n−j\gamma_{n,j}(uv-1)^{n-j}. For j=1,2j=1,2, we have to consider an additional action of S2S_2 which acts on C∗\mathbb{C}^* by z↦z−1z \mapsto z^{-1}. Combining all these, we find that the Hodge-Deligne polynomial of the boundary BnB_n is

(uv+1)n−1+(uv−1)n−12+γn,2(uv+1)n−2+(uv−1)n−22+∑j=3nγn,j(uv−1)n−j.(5)\frac{(uv+1)^{n-1}+(uv-1)^{n-1}}{2}+\gamma_{n,2}\frac{(uv+1)^{n-2}+(uv-1)^{n-2}}{2}+\sum_{j=3}^{n}\gamma_{n,j}(uv-1)^{n-j}. \tag*{(5)}

By (1.4), (1.5) and (1.1), we have the following.

Theorem 1.3 (Theorem 4.4). The Hodge-Deligne polynomial H0∣n\mathbf{H}_{0\mid n} of M‾1,(0+)n=M‾1,0∣n\overline{\mathcal{M}}_{1,(0+)n}=\overline{\mathcal{M}}_{1,0\mid n} is

∑j=0⌊n−12⌋(n−12j)(uv+1)n−1−2j(αjj(uv)j+1−∑i=0j−1αij(uv)i)+(uv+1)n−1+(uv−1)n−12+γn,2(uv+1)n−2+(uv−1)n−22+∑j=3nγn,j(uv−1)n−j\begin{aligned} \sum_{j=0}^{\left\lfloor\frac{n-1}{2}\right\rfloor}\binom{n-1}{2j}(uv+1)^{n-1-2j}\left(\alpha_{jj}(uv)^{j+1}-\sum_{i=0}^{j-1}\alpha_{ij}(uv)^i\right) \\ &+\frac{(uv+1)^{n-1}+(uv-1)^{n-1}}{2}+\gamma_{n,2}\frac{(uv+1)^{n-2}+(uv-1)^{n-2}}{2}+\sum_{j=3}^{n}\gamma_{n,j}(uv-1)^{n-j} \end{aligned}
−∑j=0⌊n−12⌋(n−12j)(uv+1)n−1−2j∑i=0j−1αijβ2j−2i+2(uv)i(u2j−2i+1+v2j−2i+1).(6)-\sum_{j=0}^{\left\lfloor\frac{n-1}{2}\right\rfloor}\binom{n-1}{2j}(uv+1)^{n-1-2j}\sum_{i=0}^{j-1}\alpha_{ij}\beta_{2j-2i+2}(uv)^i(u^{2j-2i+1}+v^{2j-2i+1}). \tag*{(6)}

The Hodge-Deligne polynomial Hn∣0\mathbf{H}_{n\mid0} of M‾1,n=M‾1,n∣0\overline{\mathcal{M}}_{1,n}=\overline{\mathcal{M}}_{1,n\mid0} can be computed by the recursive formula (1.2) together with (1.1) and (1.6).

Letting u=v=−tu=v=-t, we get the Poincaré polynomial of M‾1,n\overline{\mathcal{M}}_{1,n}. Note that only the last line in (1.6) has odd degree terms.

It is straightforward to implement the above theorem into a computer program and we can compute the Hodge-Deligne and Poincaré polynomials of M‾1,n\overline{\mathcal{M}}_{1,n} for large nn within a relatively short period of time.

Motivated by recent discoveries on the cohomology of M‾0,n\overline{\mathcal{M}}_{0,n} [1, 2, 4, 6, 7, 8], we raise the following.

Question 1.4. (1) Can we refine the computations in this paper to prove a new recursive formula for the SnS_n-equivariant Hodge-Deligne polynomial of M‾1,n\overline{\mathcal{M}}_{1,n}?

(2) Is the even degree Poincaré polynomial PM‾1,neven(x)=∑i=0nxidim⁡H2i(M‾1,n)P^{\mathrm{even}}_{\overline{\mathcal{M}}_{1,n}}(x)=\sum_{i=0}^{n}x^i\dim H^{2i}(\overline{\mathcal{M}}_{1,n}) real-rooted?

(3) Do the coefficients of PM‾1,neven(x)P^{\mathrm{even}}_{\overline{\mathcal{M}}_{1,n}}(x) form a log-concave or kk-ultra log-concave sequence for some kk?

(4) Does the probability distribution of the coefficients of PM‾1,neven(x)/PM‾1,neven(1)P^{\mathrm{even}}_{\overline{\mathcal{M}}_{1,n}}(x)/P^{\mathrm{even}}_{\overline{\mathcal{M}}_{1,n}}(1) converge to a Gaussian distribution?

(5) Can we find effective estimates of the Betti numbers of M‾1,n\overline{\mathcal{M}}_{1,n} for large nn?

(6) Can we also use the method in this paper to calculate the Hodge-Deligne and Poincaré polynomials of M‾g,n\overline{\mathcal{M}}_{g,n} for g≥2g\ge2? Note that Theorem 3.1 holds for all g≥1g\ge1 and hence it suffices to calculate the Hodge-Deligne polynomial of M‾g,0∣n\overline{\mathcal{M}}_{g,0\mid n}.

In subsequent papers, we will continue our investigation to seek answers to the above questions.

Convention. All schemes and stacks in this paper are defined over the complex number field C\mathbb{C} and all cohomology groups have rational coefficients.

Acknowledgement. It is my pleasure to thank Jinwon Choi and Han-Bom Moon for useful discussions.

Moduli spaces of weighted pointed curves and Hodge-Deligne polynomials

In this section, we collect necessary facts about Hassett moduli spaces [12] and Hodge-Deligne polynomials that will be used throughout this paper.

Definition 2.1. [12] Let g,n≥0g,n \ge0. For A=(a1,⋯ ,an)∈(0,1]n\mathcal{A}=(a_1,\cdots,a_n)\in(0,1]^n with 2g−2+∑iai>02g-2+\sum_i a_i>0, an integral curve CC with marked points p1,⋯ ,pn∈Cp_1,\cdots,p_n\in C is called A\mathcal{A}-stable if

(1) CC has at worst nodal singularities and pip_i are all smooth points;

(2) if pi1=pi2=⋯=pikp_{i_1}=p_{i_2}=\cdots=p_{i_k}, then ai1+⋯+aik≤1a_{i_1}+\cdots+a_{i_k}\le1;

(3) ωC(a1p1+⋯+anpn)\omega_C(a_1p_1+\cdots+a_np_n) is ample.

Let M‾g,A\overline{\mathcal{M}}_{g,\mathcal{A}} denote the moduli stack of A\mathcal{A}-stable nn-pointed curves of genus gg. In particular, when ai>1/2a_i>1/2 for all ii, M‾g,A\overline{\mathcal{M}}_{g,\mathcal{A}} coincides with the Knudsen-Deligne-Mumford moduli stack M‾g,n\overline{\mathcal{M}}_{g,n} of stable curves of genus gg with nn marked points [9, 15].

Let us summarize useful facts about M‾g,A\overline{\mathcal{M}}_{g,\mathcal{A}} from [12].

Theorem 2.2. Let A=(a1,⋯ ,an)∈(0,1]n\mathcal{A}=(a_1,\cdots,a_n)\in(0,1]^n with 2g−2+∑i=1nai>02g-2+\sum_{i=1}^n a_i>0.

(1) M‾g,A\overline{\mathcal{M}}_{g,\mathcal{A}} is a smooth connected proper Deligne-Mumford stack of dimension 3g−3+n3g-3+n with projective coarse moduli space.

(2) If A=(a1,⋯ ,an)\mathcal{A}=(a_1,\cdots,a_n), A′=(a1′,⋯ ,an′)\mathcal{A}'=(a'_1,\cdots,a'_n) and ai≥ai′a_i\ge a'_i for all ii, then we have a natural morphism

ρA,A′:M‾g,A⟶M‾g,A′(7)\rho_{\mathcal{A},\mathcal{A}'}:\overline{\mathcal{M}}_{g,\mathcal{A}}\longrightarrow\overline{\mathcal{M}}_{g,\mathcal{A}'} \tag*{(7)}

which is obtained by contracting rational components in an A\mathcal{A}-stable curve which are not A′\mathcal{A}'-stable.

(3) For 2<r≤n2<r\le n, if ai1′+⋯+air′≤1a'_{i_1}+\cdots+a'_{i_r}\le1 and ai1+⋯+air>1a_{i_1}+\cdots+a_{i_r}>1 but any proper subset of {ai1,⋯ ,air}\{a_{i_1},\cdots,a_{i_r}\} has sum at most one while aj=aj′a_j=a'_j for j≠i1,⋯ ,irj\ne i_1,\cdots,i_r, then the morphism ρA,A′\rho_{\mathcal{A},\mathcal{A}'} is the smooth blowup along the locus M‾g,A‾′\overline{\mathcal{M}}_{g,\overline{\mathcal{A}}'} in M‾g,A′\overline{\mathcal{M}}_{g,\mathcal{A}'} where pi1=⋯=pirp_{i_1}=\cdots=p_{i_r} and A‾′\overline{\mathcal{A}}' is obtained from A′\mathcal{A}' by replacing ai1′,⋯ ,air′a'_{i_1},\cdots,a'_{i_r} by their sum.

(4) If r≤2r\le2 for any I⊂[n]I\subset[n] such that ai1+⋯+air>1a_{i_1}+\cdots+a_{i_r}>1 and ai1′+⋯+air′≤1a'_{i_1}+\cdots+a'_{i_r}\le1, then ρA,A′\rho_{\mathcal{A},\mathcal{A}'} is an isomorphism.

Proof. (1) is [12] and (2) is [12] while (3) is [12] and (4) is [12]. □

Let H\mathbf{H} be a motivic invariant with values in an integral domain RR which assigns to each variety XX over C\mathbb{C} an element HX∈R\mathbf{H}_X\in R such that

(1) HX=HX−Z+HZ\mathbf{H}_X=\mathbf{H}_{X-Z}+\mathbf{H}_Z for any closed Z⊂XZ\subset X and

(2) HX×Y=HX⋅HY\mathbf{H}_{X\times Y}=\mathbf{H}_X\cdot\mathbf{H}_Y.

If X→YX\to Y is a Zariski locally trivial morphism with YY connected, then HX=HY⋅HF\mathbf{H}_X=\mathbf{H}_Y\cdot\mathbf{H}_F where FF denotes a fiber.

In this paper, we will only consider motivic invariants satisfying the following blowup formula: If X→YX\to Y is the smooth blowup along ZZ of codimension cc, then

HX=HY+HZ⋅(HPc−1−1).(8)\mathbf{H}_X=\mathbf{H}_Y+\mathbf{H}_Z\cdot(\mathbf{H}_{\mathbb{P}^{c-1}}-1). \tag*{(8)}

Our main example is the Hodge-Deligne polynomial

HX(u,v)=∑k(−1)k∑p,qupvqdim⁡Hcp,q;k(X)∈Z[u,v],Hcp,q;k(X)=gr⁡Fpgr⁡p+qWHck(X)\mathbf{H}_X(u,v)=\sum_k(-1)^k\sum_{p,q}u^pv^q\dim H_c^{p,q;k}(X)\in\mathbb{Z}[u,v],\qquad H_c^{p,q;k}(X)=\operatorname{gr}_F^p\operatorname{gr}_{p+q}^W H_c^k(X)

where gr⁡Fp\operatorname{gr}_F^p and gr⁡p+qW\operatorname{gr}_{p+q}^W denote the graded parts with respect to the Hodge filtration and weight filtration respectively. By letting u=v=−tu=v=-t, we obtain the virtual Poincaré polynomial

PX(t)=HX(−t,−t)∈Z[t]P_X(t)=\mathbf{H}_X(-t,-t)\in\mathbb{Z}[t]

of XX which is also a motivic invariant.

Reduction to minimally weighted curves

In this section, we prove an explicit formula (Theorem 3.1) that calculates the motivic invariants of M‾g,n=M‾g,1n\overline{\mathcal{M}}_{g,n}=\overline{\mathcal{M}}_{g,1^n} from those of M‾g,(0+)n\overline{\mathcal{M}}_{g,(0+)^n} where (0+)n∈(0,1]n(0+)^n\in(0,1]^n denotes an element sufficiently close to zero, for g≥1g\geq1.

Fix g≥1g\geq1 and n≥1n\geq1. Then M‾g,A\overline{\mathcal{M}}_{g,A} is a nonempty proper smooth Deligne-Mumford stack for any A∈(0,1]nA\in(0,1]^n. For 0≤r<n0\leq r<n and 0≤s≤n−r0\leq s\leq n-r, let

Ar,s(n)=(1,…,1,sn−r,1n−r,…,1n−r)∈(0,1]n(9)A_{r,s}^{(n)}=\left(1,\ldots,1,\frac{s}{n-r},\frac{1}{n-r},\ldots,\frac{1}{n-r}\right)\in(0,1]^n \tag*{(9)}

where 1 is repeated r−1r-1 times and 1n−r\frac{1}{n-r} is repeated n−rn-r times. For instance, A0,s(n)=(1n,…,1n)A_{0,s}^{(n)}=\left(\frac{1}{n},\ldots,\frac{1}{n}\right) for any ss. Let

Yr,s(n):=M‾g,Ar,s(n).(10)Y_{r,s}^{(n)}:=\overline{\mathcal{M}}_{g,A_{r,s}^{(n)}}. \tag*{(10)}

In particular, Y0,n(n)=M‾g,(0+)nY_{0,n}^{(n)}=\overline{\mathcal{M}}_{g,(0+)^n} and

Yn−2,2(n)=Yn−1,1(n)=M‾g,n.(11)Y_{n-2,2}^{(n)}=Y_{n-1,1}^{(n)}=\overline{\mathcal{M}}_{g,n}. \tag*{(11)}

Moreover, by Theorem 2.2 (4),

Yr,n−r−1(n)=Yr,n−r(n)=M‾g,(1r,(0+)n−r)=:M‾g,r∣n−r(12)Y_{r,n-r-1}^{(n)}=Y_{r,n-r}^{(n)}=\overline{\mathcal{M}}_{g,(1^r,(0+)^{n-r})}=:\overline{\mathcal{M}}_{g,r|n-r} \tag*{(12)}

is the moduli space of stable curves of genus gg with rr heavy points and n−rn-r light points [13].

Note that if r>r′r>r' or r=r′r=r' and s>s′s>s', then Ar,s(n)−Ar′,s′(n)≥0A_{r,s}^{(n)}-A_{r',s'}^{(n)}\geq0 and hence we have the natural morphism

ρ(r,s),(r′,s′):Yr,s(n)⟶Yr′,s′(n)\rho_{(r,s),(r',s')}:Y_{r,s}^{(n)}\longrightarrow Y_{r',s'}^{(n)}

by Theorem 2.2 (2).

Fix a motivic invariant H\mathbf{H} and let

Hr∣s:=HM‾g,r∣s=HYr,s(n)(13)\mathbf{H}_{r|s}:=\mathbf{H}_{\overline{\mathcal{M}}_{g,r|s}}=\mathbf{H}_{Y_{r,s}^{(n)}} \tag*{(13)}

be the motivic invariant of M‾g,r∣s\overline{\mathcal{M}}_{g,r|s}. Then we have H0∣n=HM‾g,(0+)n\mathbf{H}_{0|n}=\mathbf{H}_{\overline{\mathcal{M}}_{g,(0+)^n}} and Hn∣0=HM‾g,n\mathbf{H}_{n|0}=\mathbf{H}_{\overline{\mathcal{M}}_{g,n}} by (3.4).

Now our goal is to reach Yn−2,2(n)=M‾g,nY_{n-2,2}^{(n)}=\overline{\mathcal{M}}_{g,n} starting from Y0,n(n)=M‾g,(0+)nY_{0,n}^{(n)}=\overline{\mathcal{M}}_{g,(0+)^n} by smooth blowups so that we can reduce the computation of Hn∣0\mathbf{H}_{n|0} to H0∣n\mathbf{H}_{0|n}. Let us first reach Y1,n−1(n)Y_{1,n-1}^{(n)}. The natural map

ρA1,1(n),A0,n(n):Y1,1(n)⟶Y0,n(n)\rho_{A_{1,1}^{(n)},A_{0,n}^{(n)}}:Y_{1,1}^{(n)}\longrightarrow Y_{0,n}^{(n)}

is the smooth blowup along the locus M‾g,1∣0=M‾g,1\overline{\mathcal{M}}_{g,1|0}=\overline{\mathcal{M}}_{g,1} of p1=p2=⋯=pnp_1=p_2=\cdots=p_n by Theorem 2.2 (3). Likewise, for 1≤k≤n−31\leq k\leq n-3, the natural map

ρA1,k+1(n),A1,k(n):Y1,k+1(n)⟶Y1,k(n)\rho_{A_{1,k+1}^{(n)},A_{1,k}^{(n)}}:Y_{1,k+1}^{(n)}\longrightarrow Y_{1,k}^{(n)}

is the smooth blowup along the locus of p1=pi1=⋯=pin−k−1p_1=p_{i_1}=\cdots=p_{i_{n-k-1}} for {i1,…,in−k−1}⊂{2,…,n}\{i_1,\ldots,i_{n-k-1}\}\subset\{2,\ldots,n\} which consists of (n−1k)\binom{n-1}{k} copies of M‾g,1∣k\overline{\mathcal{M}}_{g,1|k}. Note that Y1,n−2(n)=Y1,n−1(n)Y_{1,n-2}^{(n)}=Y_{1,n-1}^{(n)} by (3.4). By applying the blowup formula (2.2) to these morphisms, we find that

H1∣n−1=H0∣n+∑k=0n−3(n−1k)H1∣k(HPn−k−2−1).(14)\mathbf{H}_{1|n-1}=\mathbf{H}_{0|n}+\sum_{k=0}^{n-3}\binom{n-1}{k}\mathbf{H}_{1|k}\left(\mathbf{H}_{\mathbb{P}^{n-k-2}}-1\right). \tag*{(14)}

Next, let us reach Y2,n−2(n)Y_{2,n-2}^{(n)} from Y1,n−1(n)Y_{1,n-1}^{(n)}. The natural map

ρA2,1(n),A1,n−1(n):Y2,1(n)⟶Y1,n−1(n)\rho_{A_{2,1}^{(n)},A_{1,n-1}^{(n)}}:Y_{2,1}^{(n)}\longrightarrow Y_{1,n-1}^{(n)}

is the smooth blowup along the locus M‾g,2∣0=M‾g,2\overline{\mathcal{M}}_{g,2|0}=\overline{\mathcal{M}}_{g,2} of p2=p3=⋯=pnp_2=p_3=\cdots=p_n by Theorem 2.2 (3). For 1≤k≤n−41\leq k\leq n-4, the natural map

ρA‾2,k+1(n)A‾2,k+1(n):Y2,k+1(n)⟶Y2,k(n)\rho_{\overline{\mathcal{A}}_{2,k+1}^{(n)}}^{\overline{\mathcal{A}}_{2,k+1}^{(n)}}:Y_{2,k+1}^{(n)}\longrightarrow Y_{2,k}^{(n)}

is the smooth blowup along the locus of p2=pi1=⋯=pin−k−2p_2=p_{i_1}=\cdots=p_{i_{n-k-2}} for {i1,…,in−k−2}⊂{3,…,n}\{i_1,\ldots,i_{n-k-2}\}\subset\{3,\ldots,n\} which consists of (n−2k)\binom{n-2}{k} copies of M‾g,2∣k\overline{\mathcal{M}}_{g,2|k}. We have Y2,n−3(n)=Y1,n−2(n)Y_{2,n-3}^{(n)}=Y_{1,n-2}^{(n)} by (12) and the blowup formula (2.2) gives us

H2∣n−2=H1∣n−1+∑k=0n−4(n−2k)H2∣k(HPn−k−3−1).(15)\mathbf{H}_{2|n-2}=\mathbf{H}_{1|n-1}+\sum_{k=0}^{n-4}\binom{n-2}{k}\mathbf{H}_{2|k}\left(\mathbf{H}_{\mathbb{P}^{n-k-3}}-1\right). \tag*{(15)}

Repeating this way, we obtain the following.

Theorem 3.1. For r,s≥0r,s\geq0 with r+s>0r+s>0 and n>0n>0, the following hold:

Hr∣s=H0∣r+s+∑j=1min⁡(r,r+s−2)∑k=0r+s−j−2(r+s−jk)Hj∣k⋅(HPr+s−j−k−1−1).(16)\mathbf{H}_{r|s}=\mathbf{H}_{0|r+s}+\sum_{j=1}^{\min(r,r+s-2)}\sum_{k=0}^{r+s-j-2}\binom{r+s-j}{k}\mathbf{H}_{j|k}\cdot\left(\mathbf{H}_{\mathbb{P}^{r+s-j-k-1}}-1\right). \tag*{(16)}
HM‾g,n=Hn∣0=H0∣n+∑j=1n−2∑k=0n−j−2(n−jk)Hj∣k⋅(HPn−j−k−1−1).(17)\mathbf{H}_{\overline{\mathcal{M}}_{g,n}}=\mathbf{H}_{n|0}=\mathbf{H}_{0|n}+\sum_{j=1}^{n-2}\sum_{k=0}^{n-j-2}\binom{n-j}{k}\mathbf{H}_{j|k}\cdot\left(\mathbf{H}_{\mathbb{P}^{n-j-k-1}}-1\right). \tag*{(17)}

All Hr∣s\mathbf{H}_{r|s} are recursively determined by (16) if we know H0∣n=HM‾g,(0+)n\mathbf{H}_{0|n}=\mathbf{H}_{\overline{\mathcal{M}}_{g,(0+)n}} for all nn.

In particular, the motivic invariants HM‾g,n=Hn∣0\mathbf{H}_{\overline{\mathcal{M}}_{g,n}}=\mathbf{H}_{n|0} can be recursively calculated by (16) if we know the motivic invariants HM‾g,(0+)n=H0∣n\mathbf{H}_{\overline{\mathcal{M}}_{g,(0+)n}}=\mathbf{H}_{0|n} for all n≥1n\geq1. Conversely, if we know HM‾g,n=Hn∣0\mathbf{H}_{\overline{\mathcal{M}}_{g,n}}=\mathbf{H}_{n|0} for all n≥1n\geq1, we can recursively calculate HM‾g,(0+)n=H0∣n\mathbf{H}_{\overline{\mathcal{M}}_{g,(0+)n}}=\mathbf{H}_{0|n} for all positive nn by (16).

Moduli spaces of minimally weighted curves

In this section, we let g=1g=1 and let H\mathbf{H} be the Hodge-Deligne polynomial. We find an explicit formula that calculates the Hodge-Deligne polynomials of the moduli spaces M‾1,(0+)n\overline{\mathcal{M}}_{1,(0+)^n} of stable curves of genus 1 with nn marked points whose weights are ≤1/n\leq1/n. By Theorem 3.1, we can then calculate HM‾1,n\mathbf{H}_{\overline{\mathcal{M}}_{1,n}} for all n>0n>0.

Note that in M‾1,(0+)n\overline{\mathcal{M}}_{1,(0+)^n}, all the marked points are allowed to coincide as long as they stay away from the nodes. Let

π=πn:M‾1,(0+)n⟶M‾1,0+=M‾1,1\pi=\pi_n:\overline{\mathcal{M}}_{1,(0+)^n}\longrightarrow\overline{\mathcal{M}}_{1,0+}=\overline{\mathcal{M}}_{1,1}

be the morphism that forgets all the marked points except the first. Using the stratification

M‾1,1=M1,1⊔{∞}\overline{\mathcal{M}}_{1,1}=\mathcal{M}_{1,1}\sqcup\{\infty\}

where ∞\infty parameterizes the unique singular rational curve, we have the decomposition

M‾1,(0+)n=In⊔Bn,Bn=πn−1(∞),In=πn−1(M1,1)\overline{\mathcal{M}}_{1,(0+)^n}=\mathcal{I}_n\sqcup\mathcal{B}_n,\qquad\mathcal{B}_n=\pi_n^{-1}(\infty),\quad\mathcal{I}_n=\pi_n^{-1}(\mathcal{M}_{1,1})

into the interior and the boundary.

Let In=HIn\mathcal{I}_n=\mathbf{H}_{\mathcal{I}_n} and Bn=HBn\mathcal{B}_n=\mathbf{H}_{\mathcal{B}_n} be the Hodge-Deligne polynomials of In\mathcal{I}_n and Bn\mathcal{B}_n respectively so that

H0∣n=HM‾1,(0+)n=In+Bn\mathbf{H}_{0|n}=\mathbf{H}_{\overline{\mathcal{M}}_{1,(0+)^n}}=\mathcal{I}_n+\mathcal{B}_n

is the Hodge-Deligne polynomial of M‾1,(0+)n\overline{\mathcal{M}}_{1,(0+)^n}.

The Hodge-Deligne Polynomial InI_n of In\mathcal{I}_n

In this subsection, we prove the following.

Proposition 4.1. In(u,v)=Ineven(u,v)+Inodd(u,v)I_n(u,v)=I_n^{\mathrm{even}}(u,v)+I_n^{\mathrm{odd}}(u,v) with

Ineven(u,v)=∑j=0⌊n−12⌋(n−12j)(uv+1)n−1−2j(αjj(uv)j+1−∑i=0j−1αij(uv)i)I_n^{\mathrm{even}}(u,v)=\sum_{j=0}^{\left\lfloor\frac{n-1}{2}\right\rfloor}\binom{n-1}{2j}(uv+1)^{n-1-2j}\left(\alpha_{jj}(uv)^{j+1}-\sum_{i=0}^{j-1}\alpha_{ij}(uv)^i\right)
Inodd(u,v)=−∑j=0⌊n−12⌋(n−12j)(uv+1)n−1−2j∑i=0j−1αijβ2j−2i+2(uv)i(u2j−2i+1+v2j−2i+1)I_n^{\mathrm{odd}}(u,v)=-\sum_{j=0}^{\left\lfloor\frac{n-1}{2}\right\rfloor}\binom{n-1}{2j}(uv+1)^{n-1-2j}\sum_{i=0}^{j-1}\alpha_{ij}\beta_{2j-2i+2}(uv)^i(u^{2j-2i+1}+v^{2j-2i+1})

where

αij=(2ji)−(2ji−1)andβk={⌊k12⌋−1if k≡2(mod12)⌊k12⌋if k≠2(mod12).(18)\alpha_{ij}=\binom{2j}{i}-\binom{2j}{i-1} \qquad\text{and}\qquad \beta_k= \begin{cases} \left\lfloor\frac{k}{12}\right\rfloor-1 & \text{if } k\equiv2\pmod{12}\\ \left\lfloor\frac{k}{12}\right\rfloor& \text{if } k\ne2\pmod{12}. \end{cases} \tag*{(18)}

See Example 5.1 for an explicit computation of InI_n for n≤10n\le10.

Let q:C→M1,1q:\mathcal{C}\to\mathcal{M}_{1,1} denote the universal curve. By our choice of stability condition, all the marked points are allowed to coincide and hence In\mathcal{I}_n is nothing but the (n−1)(n-1)-fold fiber product

π:In=C×M1,1C×M1,1⋯×M1,1C⟶M1,1\pi:\mathcal{I}_n=\mathcal{C}\times_{\mathcal{M}_{1,1}}\mathcal{C}\times_{\mathcal{M}_{1,1}}\cdots\times_{\mathcal{M}_{1,1}}\mathcal{C}\longrightarrow\mathcal{M}_{1,1}

which is a smooth projective fibration with fiber En−1E^{n-1} for an elliptic curve E∈M1,1E\in\mathcal{M}_{1,1}.

Let V=R1q∗QV=R^1q_*\mathbb{Q}. Then VV is a local system of rank 2 over M1,1\mathcal{M}_{1,1} and

Rq∗Q≅(Q⊕Q[−2])⊕V[−1].Rq_*\mathbb{Q}\cong(\mathbb{Q}\oplus\mathbb{Q}[-2])\oplus V[-1].

Let π′=π∣In\pi'=\pi|_{\mathcal{I}_n}. By the relative Künneth theorem, we have

Rπ∗′QIn≅((Q⊕Q[−2])⊕V[−1])⊗n−1=⨁k=0n−1(n−1k)Ck⊗V⊗k[−k](19)R\pi'_*\mathbb{Q}_{\mathcal{I}_n}\cong\left((\mathbb{Q}\oplus\mathbb{Q}[-2])\oplus V[-1]\right)^{\otimes n-1}=\bigoplus_{k=0}^{n-1}\binom{n-1}{k}C_k\otimes V^{\otimes k}[-k] \tag*{(19)}

where Ck=(Q⊕Q[−2])⊗n−1−kC_k=(\mathbb{Q}\oplus\mathbb{Q}[-2])^{\otimes n-1-k}.

Since M1,1≅SL2(Z)\H\mathcal{M}_{1,1}\cong SL_2(\mathbb{Z})\backslash\mathbb{H} where H\mathbb{H} denotes the upper half plane and the generic stabilizer −I∈SL2(Z)-I\in SL_2(\mathbb{Z}) acts on V⊗kV^{\otimes k} as (−1)k(-1)^k, we have the vanishing

Hc∗(M1,1,V⊗k)=0,∀ odd k.H_c^*(\mathcal{M}_{1,1},V^{\otimes k})=0,\qquad\forall\text{ odd }k.

Hence (4.2) gives us

Hc∗(In)=Hc∗(M1,1,Rπ∗′QIn)≅⨁j=0⌊n−12⌋(n−12j)C2j⊗Hc∗(M1,1,V⊗2j)[−2j].(20)H_c^*(\mathcal{I}_n)=H_c^*(\mathcal{M}_{1,1},R\pi'_*\mathbb{Q}_{\mathcal{I}_n})\cong\bigoplus_{j=0}^{\left\lfloor\frac{n-1}{2}\right\rfloor}\binom{n-1}{2j}C_{2j}\otimes H_c^*(\mathcal{M}_{1,1},V^{\otimes2j})[-2j]. \tag*{(20)}

By the Clebsch-Gordan rule and (4.1), we have

V⊗2j≅⨁i=0j−1αijV2j−2i[2j−2i]⊕αjjQ,where V2k=Sym⁡2kV.V^{\otimes2j}\cong\bigoplus_{i=0}^{j-1}\alpha_{ij}V_{2j-2i}[2j-2i]\oplus\alpha_{jj}\mathbb{Q},\qquad\text{where }V_{2k}=\operatorname{Sym}^{2k}V.

Therefore (4.3) gives us

Hc∗(In)≅⨁j=0⌊n−12⌋(n−12j)C2j⊗(αjjHc∗(M1,1,Q)[−2j]+∑i=0j−1αijHc∗(M1,1,V2j−2i)[−2i]).(21)H_c^*(\mathcal{I}_n)\cong\bigoplus_{j=0}^{\left\lfloor\frac{n-1}{2}\right\rfloor}\binom{n-1}{2j}C_{2j}\otimes\left(\alpha_{jj}H_c^*(\mathcal{M}_{1,1},\mathbb{Q})[-2j]+\sum_{i=0}^{j-1}\alpha_{ij}H_c^*(\mathcal{M}_{1,1},V_{2j-2i})[-2i]\right). \tag*{(21)}

Since Hc∗(M1,1,Q)≅Q[−2]H_c^*(\mathcal{M}_{1,1},\mathbb{Q})\cong\mathbb{Q}[-2], Proposition 4.1 follows immediately from the following.

Lemma 4.2. For k>0k > 0, we have an isomorphism

Hc∗(M1,1,V2k)=Hc1(M1,1,V2k)≅Q⊕(S2k+2⊕S‾2k+2)H_c^*(\mathcal{M}_{1,1}, \mathbb{V}_{2k}) = H_c^1(\mathcal{M}_{1,1}, \mathbb{V}_{2k}) \cong\mathbb{Q} \oplus(S_{2k+2} \oplus\overline{S}_{2k+2})

where S2k+2S_{2k+2} denotes the space of cusp forms of weight 2k+22k+2 with respect to SL2(Z)SL_2(\mathbb{Z}). The first factor Q\mathbb{Q} has weight 0 and S2k+2S_{2k+2} is of Hodge type (2k+1,0)(2k+1,0).

Proof. Let j:M1,1→M‾1,1j:\mathcal{M}_{1,1} \to\overline{\mathcal{M}}_{1,1} denote the inclusion map. Then we have an exact triangle

j!V2k⟶j∗V2k⟶j∗V2k∣∞⟶.j_!\mathbb{V}_{2k} \longrightarrow j_*\mathbb{V}_{2k} \longrightarrow j_*\mathbb{V}_{2k}|_{\infty} \longrightarrow.

By the Eichler-Shimura isomorphism [17], we have

H∗(M‾1,1,j∗V2k)=H1(M‾1,1,j∗V2k)≅Hpar1(SL2(Z),Sym⁡2k(C2))≅S2k+2⊕S‾2k+2H^*(\overline{\mathcal{M}}_{1,1},j_*\mathbb{V}_{2k}) = H^1(\overline{\mathcal{M}}_{1,1},j_*\mathbb{V}_{2k}) \cong H^1_{\mathrm{par}}(SL_2(\mathbb{Z}),\operatorname{Sym}^{2k}(\mathbb{C}^2)) \cong S_{2k+2} \oplus\overline{S}_{2k+2}

where S2k+2S_{2k+2} has Hodge type (2k+1,0)(2k+1,0). We thus find that Hc∗(M1,1,V2k)=Hc1(M1,1,V2k)H_c^*(\mathcal{M}_{1,1},\mathbb{V}_{2k}) = H_c^1(\mathcal{M}_{1,1},\mathbb{V}_{2k}) and have an exact sequence

0⟶H0(∞,j∗V2k∣∞)⟶Hc1(M1,1,V2k)⟶S2k+2⊕S‾2k+2⟶0.0 \longrightarrow H^0(\infty,j_*\mathbb{V}_{2k}|_{\infty}) \longrightarrow H_c^1(\mathcal{M}_{1,1},\mathbb{V}_{2k}) \longrightarrow S_{2k+2} \oplus\overline{S}_{2k+2} \longrightarrow0.

As the cusp ∞\infty has the stabilizer group generated by

σ:=(1101),\sigma:= \begin{pmatrix} 1 & 1 \\ 0 & 1 \end{pmatrix},

H0(∞,j∗V2k∣∞)H^0(\infty,j_*\mathbb{V}_{2k}|_{\infty}) is the σ\sigma-invariant part (Sym⁡2kQ2)σ≅Q(\operatorname{Sym}^{2k}\mathbb{Q}^2)^\sigma\cong\mathbb{Q}. This completes the proof. □

It is well known that dim⁡S2k+2=β2k+2\dim S_{2k+2} = \beta_{2k+2} for k>0k > 0 by Riemann-Roch, using the notation of (4.1).

The Hodge-Deligne Polynomial BnB_n of Bn\mathcal{B}_n

Let γn,1=1\gamma_{n,1}=1, γn,2=2n−1−1\gamma_{n,2}=2^{n-1}-1 and for k>2k>2, let

γn,k=(nk)(k−1)!2=12k∑i=0k(−1)k−i(ki)in(22)\gamma_{n,k} = \binom{n}{k}\frac{(k-1)!}{2} = \frac{1}{2k}\sum_{i=0}^{k}(-1)^{k-i}\binom{k}{i}i^n \tag*{(22)}

where {nk}\left\{\begin{matrix} n \\ k \end{matrix}\right\} denotes the Stirling number of the second kind, i.e. the number of ways to partition [n]={1,2,…,n}[n]=\{1,2,\ldots,n\} into kk unordered subsets. In this subsection, we prove the following.

Proposition 4.3. With γn,k\gamma_{n,k} in (4.5),

Bn(u,v)=(uv+1)n−1+(uv−1)n−12+γn,2(uv+1)n−2+(uv−1)n−22+∑j=3nγn,j(uv−1)n−jB_n(u,v)=\frac{(uv+1)^{n-1}+(uv-1)^{n-1}}{2}+\gamma_{n,2}\frac{(uv+1)^{n-2}+(uv-1)^{n-2}}{2}+\sum_{j=3}^{n}\gamma_{n,j}(uv-1)^{n-j}

See Example 5.2 for the calculation of BnB_n for n≤10n \le10.

Observe that we have a decomposition

Bn=∐1≤j≤nBn,jB_n=\coprod_{1\le j\le n}B_{n,j}

where Bn,jB_{n,j} denotes the locus of curves with jj rational components i.e. the dual graph is a necklace with jj vertices.

If (C,p1,⋯ ,pn)∈Bn,1(C,p_1,\cdots,p_n)\in B_{n,1}, CC is a rational curve with normalization P1\mathbb{P}^1. Let 0,∞∈P10,\infty\in\mathbb{P}^1 map to the node of CC. Then we find that

Bn,1≅(C∗)n/(C∗×S2)≅(C∗)n−1/S2B_{n,1}\cong(\mathbb{C}^*)^n/(\mathbb{C}^*\times S_2)\cong(\mathbb{C}^*)^{n-1}/S_2

where −1∈S2-1\in S_2 acts by (z1,…,zn−1)↦(z1−1,…,zn−1−1)(z_1,\ldots,z_{n-1})\mapsto(z_1^{-1},\ldots,z_{n-1}^{-1}). Therefore, we have

Hc∗(Bn,1)≅(Hc∗(C∗)⊗n−1)S2H_c^*(B_{n,1})\cong\left(H_c^*(\mathbb{C}^*)^{\otimes n-1}\right)^{S_2}

whose Hodge-Deligne polynomial is

HBn,1(u,v)=12((uv+1)n−1+(uv−1)n−1).(23)\mathrm{H}_{\mathcal{B}_{n,1}}(u,v)=\frac{1}{2}\left((uv+1)^{n-1}+(uv-1)^{n-1}\right). \tag*{(23)}

If (C,p1,…,pn)∈Bn,2(C,p_1,\ldots,p_n)\in\mathcal{B}_{n,2}, C=C1∪C2C=C_1\cup C_2 with C1,C2≅P1C_1,C_2\cong\mathbb{P}^1. The locus Bn,2,k\mathcal{B}_{n,2,k} of such pointed curves where one component has kk marked points while the other has n−kn-k points is

((C∗)k/C∗×(C∗)n−k/C∗)/S2≅(C∗)n−2/S2\left((\mathbb{C}^*)^k/\mathbb{C}^*\times(\mathbb{C}^*)^{n-k}/\mathbb{C}^*\right)/S_2\cong(\mathbb{C}^*)^{n-2}/S_2

where S2S_2 interchanges the two nodes. We thus find that

HBn,2(u,v)=(2n−1−1)12((uv+1)n−2+(uv−1)n−2).(24)\mathrm{H}_{\mathcal{B}_{n,2}}(u,v)=(2^{n-1}-1)\frac{1}{2}\left((uv+1)^{n-2}+(uv-1)^{n-2}\right). \tag*{(24)}

For j≥3j\geq3, the number of ways to distribute nn marked points to jj components is γn,j\gamma_{n,j} in (22). For each such distribution, we have a connected component of Bn,j\mathcal{B}_{n,j} isomorphic to (C∗)n−j(\mathbb{C}^*)^{n-j}. Hence we find that

HBn,j(u,v)=γn,j(uv−1)n−j,for j≥3.(25)\mathrm{H}_{\mathcal{B}_{n,j}}(u,v)=\gamma_{n,j}(uv-1)^{n-j},\qquad\text{for }j\geq3. \tag*{(25)}

Adding (23), (24) and (25), we obtain Proposition 4.3.

The Hodge-Deligne polynomial HM‾1,(0+)n\mathrm{H}_{\overline{\mathcal{M}}_{1,(0+)^n}}

By Propositions 4.1 and 4.3, we obtain the following.

Theorem 4.4. The Hodge-Deligne polynomial HM‾1,(0+)n=H0∣n\mathrm{H}_{\overline{\mathcal{M}}_{1,(0+)^n}}=\mathrm{H}_{0|n} of M‾1,(0+)n\overline{\mathcal{M}}_{1,(0+)^n} is

H0∣n(u,v)=∑j=0⌊n−12⌋(n−12j)(uv+1)n−1−2j(αjj(uv)j+1−∑i=0j−1αij(uv)i)+(uv+1)n−1+(uv−1)n−12+γn,2(uv+1)n−2+(uv−1)n−22+∑j=3nγn,j(uv−1)n−j−∑j=0⌊n−12⌋(n−12j)(uv+1)n−1−2j∑i=0j−1αijβ2j−2i+2(uv)i(u2j−2i+1+v2j−2i+1)\begin{aligned} \mathrm{H}_{0|n}(u,v)={}&\sum_{j=0}^{\left\lfloor\frac{n-1}{2}\right\rfloor}\binom{n-1}{2j}(uv+1)^{n-1-2j}\left(\alpha_{jj}(uv)^{j+1}-\sum_{i=0}^{j-1}\alpha_{ij}(uv)^i\right)\\ &+\frac{(uv+1)^{n-1}+(uv-1)^{n-1}}{2}+\gamma_{n,2}\frac{(uv+1)^{n-2}+(uv-1)^{n-2}}{2}+\sum_{j=3}^{n}\gamma_{n,j}(uv-1)^{n-j}\\ &-\sum_{j=0}^{\left\lfloor\frac{n-1}{2}\right\rfloor}\binom{n-1}{2j}(uv+1)^{n-1-2j}\sum_{i=0}^{j-1}\alpha_{ij}\beta_{2j-2i+2}(uv)^i(u^{2j-2i+1}+v^{2j-2i+1}) \end{aligned}

where αij\alpha_{ij}, βk\beta_k and γn,k\gamma_{n,k} are constants defined by (18) and (22) respectively.

See Example 5.3 for a computation of H0∣n\mathrm{H}_{0|n} for n≤10n\leq10.

By Theorems 4.4 and 3.1, we can now calculate HM‾1,n(u,v)\mathrm{H}_{\overline{\mathcal{M}}_{1,n}}(u,v) recursively for all nn.

Computations for n10

Letting x=uvx=uv, by Proposition 4.1, we can evaluate InI_n as follows. Example 5.1.

I1(x)=xI_1(x)=x
I2(x)=x2+xI_2(x)=x^2+x
I3(x)=x3+3x2+x−1I_3(x)=x^3+3x^2+x-1
I4(x)=x4+6x3+6x2−2x−3I_4(x)=x^4+6x^3+6x^2-2x-3
I5(x)=x5+10x4+20x3+4x2−14x−7I_5(x)=x^5+10x^4+20x^3+4x^2-14x-7
I6(x)=x6+15x5+50x4+40x3−30x2−49x−15I_6(x)=x^6+15x^5+50x^4+40x^3-30x^2-49x-15
I7(x)=x7+21x6+105x5+160x4−183x2−139x−31I_7(x)=x^7+21x^6+105x^5+160x^4-183x^2-139x-31
I8(x)=x8+28x7+196x6+469x5+280x4−427x3−700x2−356x−63I_8(x)=x^8+28x^7+196x^6+469x^5+280x^4-427x^3-700x^2-356x-63
I9(x)=x9+36x8+336x7+1148x6+1386x5−406x4−2436x3−2224x2−860x−127I_9(x)=x^9+36x^8+336x^7+1148x^6+1386x^5-406x^4-2436x^3-2224x^2-860x-127
I10(x)=x10+45x9+540x8+2484x7+4662x6+1764x5−6090x4−9804x3−6372x2−2003x−255I_{10}(x)=x^{10}+45x^9+540x^8+2484x^7+4662x^6+1764x^5-6090x^4-9804x^3-6372x^2-2003x-255

By Proposition 4.3, we can evaluate BnB_n as follows with x=uvx=uv.

Example 5.2.

B1(x)=1B_1(x)=1
B2(x)=x+1B_2(x)=x+1
B3(x)=x2+3x+2B_3(x)=x^2+3x+2
B4(x)=x3+7x2+9x+4B_4(x)=x^3+7x^2+9x+4
B5(x)=x4+15x3+31x2+25x+8B_5(x)=x^4+15x^3+31x^2+25x+8
B6(x)=x5+31x4+100x3+111x2+65x+16B_6(x)=x^5+31x^4+100x^3+111x^2+65x+16
B7(x)=x6+63x5+316x4+476x3+351x2+161x+32B_7(x)=x^6+63x^5+316x^4+476x^3+351x^2+161x+32
B8(x)=x7+127x6+987x5+2178x4+1883x3+1023x2+385x+64B_8(x)=x^7+127x^6+987x^5+2178x^4+1883x^3+1023x^2+385x+64
B9(x)=x8+255x7+3053x6+10515x5+12307x4+6637x3+2815x2+897x+128B_9(x)=x^8+255x^7+3053x^6+10515x^5+12307x^4+6637x^3+2815x^2+897x+128
B10(x)=x9+511x8+9366x7+51313x6+92466x5+62065x4+21654x3+7423x2+2049x+256B_{10}(x)=x^9+511x^8+9366x^7+51313x^6+92466x^5+62065x^4+21654x^3+7423x^2+2049x+256

By adding InI_n and BnB_n, we find Tn=HM‾1,0∣nT_n=\mathrm{H}_{\overline{M}_{1,0|n}} as follows.

Example 5.3.

T1(x)=x+1T_1(x)=x+1
T2(x)=x2+2x+1T_2(x)=x^2+2x+1
T3(x)=x3+4x2+4x+1T_3(x)=x^3+4x^2+4x+1
T4(x)=x4+7x3+13x2+7x+1T_4(x)=x^4+7x^3+13x^2+7x+1
T5(x)=x5+11x4+35x3+35x2+11x+1T_5(x)=x^5+11x^4+35x^3+35x^2+11x+1
T6(x)=x6+16x5+81x4+140x3+81x2+16x+1T_6(x)=x^6+16x^5+81x^4+140x^3+81x^2+16x+1
T7(x)=x7+22x6+168x5+476x4+476x3+168x2+22x+1T_7(x)=x^7+22x^6+168x^5+476x^4+476x^3+168x^2+22x+1
T8(x)=x8+29x7+323x6+1456x5+2458x4+1456x3+323x2+29x+1T_8(x)=x^8+29x^7+323x^6+1456x^5+2458x^4+1456x^3+323x^2+29x+1
T9(x)=x9+37x8+591x7+4201x6+11901x5+11901x4+4201x3+591x2+37x+1T_9(x)=x^9+37x^8+591x^7+4201x^6+11901x^5+11901x^4+4201x^3+591x^2+37x+1
T10(x)=x10+46x9+1051x8+11850x7+55975x6+94230x5+55975x4+11850x3+1051x2+46x+1T_{10}(x)=x^{10}+46x^9+1051x^8+11850x^7+55975x^6+94230x^5+55975x^4+11850x^3+1051x^2+46x+1

Note that this matches perfectly with tbl:2 in [13] with x=uvx=uv.

By (3.8) and Theorem 4.4, we can compute Hr∣s=HM‾1,r∣s\mathbf{H}_{r|s}=\mathbf{H}_{\overline{\mathcal{M}}_{1,r|s}} as follows with x=uvx=uv.

Example 5.4.

H0∣1=H1∣0=x+1H0∣2=H1∣1=H2∣0=x2+2x+1H0∣3=x3+4x2+4x+1H1∣2=H2∣1=H3∣0=x3+5x2+5x+1H0∣4=x4+7x3+13x2+7x+1H1,3=x4+11x3+21x2+11x+1H2∣2=H3∣1=H4∣0=x4+12x3+23x2+12x+1H0∣5=x5+11x4+35x3+35x2+11x+1H1∣4=x5+22x4+79x3+79x2+22x+1H2∣3=x5+26x4+97x3+97x2+26x+1H3∣2=H4∣1=H5∣0=x5+27x4+102x3+102x2+27x+1.\begin{aligned} \mathbf{H}_{0|1}=\mathbf{H}_{1|0}&=x+1\\ \mathbf{H}_{0|2}=\mathbf{H}_{1|1}=\mathbf{H}_{2|0}&=x^2+2x+1\\ \mathbf{H}_{0|3}&=x^3+4x^2+4x+1\\ \mathbf{H}_{1|2}=\mathbf{H}_{2|1}=\mathbf{H}_{3|0}&=x^3+5x^2+5x+1\\ \mathbf{H}_{0|4}&=x^4+7x^3+13x^2+7x+1\\ \mathbf{H}_{1,3}&=x^4+11x^3+21x^2+11x+1\\ \mathbf{H}_{2|2}=\mathbf{H}_{3|1}=\mathbf{H}_{4|0}&=x^4+12x^3+23x^2+12x+1\\ \mathbf{H}_{0|5}&=x^5+11x^4+35x^3+35x^2+11x+1\\ \mathbf{H}_{1|4}&=x^5+22x^4+79x^3+79x^2+22x+1\\ \mathbf{H}_{2|3}&=x^5+26x^4+97x^3+97x^2+26x+1\\ \mathbf{H}_{3|2}=\mathbf{H}_{4|1}=\mathbf{H}_{5|0}&=x^5+27x^4+102x^3+102x^2+27x+1. \end{aligned}

Note that this matches perfectly with tbl:1 in [13] after applying the hook-length formula to extract the Hodge-Deligne polynomials.

By (3.9) and Theorem 4.4, we can compute Hn∣0=HM‾1,n\mathbf{H}_{n|0}=\mathbf{H}_{\overline{\mathcal{M}}_{1,n}} as follows with x=uvx=uv.

Example 5.5.

HM‾1,1=x+1HM‾1,2=x2+2x+1HM‾1,3=x3+5x2+5x+1HM‾1,4=x4+12x3+23x2+12x+1HM‾1,5=x5+27x4+102x3+102x2+27x+1HM‾1,6=x6+58x5+421x4+756x3+421x2+58x+1HM‾1,7=x7+121x6+1612x5+5077x4+5077x3+1612x2+121x+1HM‾1,8=x8+248x7+5802x6+31072x5+52402x4+31072x3+5802x2+248x+1HM‾1,9=x9+503x8+19925x7+175036x6+480097x5+480097x4+175036x3+19925x2+503x+1HM‾1,10=x10+1014x9+66090x8+920263x7+3975949x6+6349238x5+3975949x4+920263x3+⋯ .\begin{aligned} \mathbf{H}_{\overline{\mathcal{M}}_{1,1}}&=x+1\\ \mathbf{H}_{\overline{\mathcal{M}}_{1,2}}&=x^2+2x+1\\ \mathbf{H}_{\overline{\mathcal{M}}_{1,3}}&=x^3+5x^2+5x+1\\ \mathbf{H}_{\overline{\mathcal{M}}_{1,4}}&=x^4+12x^3+23x^2+12x+1\\ \mathbf{H}_{\overline{\mathcal{M}}_{1,5}}&=x^5+27x^4+102x^3+102x^2+27x+1\\ \mathbf{H}_{\overline{\mathcal{M}}_{1,6}}&=x^6+58x^5+421x^4+756x^3+421x^2+58x+1\\ \mathbf{H}_{\overline{\mathcal{M}}_{1,7}}&=x^7+121x^6+1612x^5+5077x^4+5077x^3+1612x^2+121x+1\\ \mathbf{H}_{\overline{\mathcal{M}}_{1,8}}&=x^8+248x^7+5802x^6+31072x^5+52402x^4+31072x^3+5802x^2+248x+1\\ \mathbf{H}_{\overline{\mathcal{M}}_{1,9}}&=x^9+503x^8+19925x^7+175036x^6+480097x^5+480097x^4+175036x^3+19925x^2+503x+1\\ \mathbf{H}_{\overline{\mathcal{M}}_{1,10}}&=x^{10}+1014x^9+66090x^8+920263x^7+3975949x^6+6349238x^5+3975949x^4+920263x^3+\cdots. \end{aligned}

Note that this matches perfectly with [3, eM1bar.txt] and [10, page 491].

By Theorems 3.1 and 4.4, it is straightforward to write up a computer program that computes the Hodge-Deligne and Poincaré polynomials of M‾1,n\overline{\mathcal{M}}_{1,n} for higher nn, quite efficiently. For n=50n=50, we get the following picture for the probability distribution

pn,i=dim⁡H2i(M‾1,n)∑k=0ndim⁡H2k(M‾1,n).(26)p_{n,i}=\frac{\dim H^{2i}(\overline{\mathcal{M}}_{1,n})}{\sum_{k=0}^{n}\dim H^{2k}(\overline{\mathcal{M}}_{1,n})}. \tag*{(26)}

The red curve in the picture is the graph of a Gaussian function.

Probability distribution

Figure 1.

In the subsequent paper [5], we will prove that indeed the probability distribution (5.1) is asymptotically Gaussian. Furthermore, we will prove a formula that gives us effective estimates of the Betti numbers for nn large and show that the Betti sequence is asymptotically 3-ultra log concave.

References

School of Mathematics, Korea Institute for Advanced Study, 85 Hoegiro, Dongdaemun-gu, Seoul 02455, Korea

Email address: [email protected]

References

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