Loading [MathJax]/jax/output/SVG/jax.js
Research article Special Issues

Motives of moduli spaces of rank 3 vector bundles and Higgs bundles on a curve

  • We prove formulas for the rational Chow motives of moduli spaces of semistable vector bundles and Higgs bundles of rank 3 and coprime degree on a smooth projective curve. Our approach involves identifying criteria to lift identities in (a completion of) the Grothendieck group of effective Chow motives to isomorphisms in the category of Chow motives. For the Higgs moduli space, we use motivic Białynicki-Birula decompositions associated with a scaling action, together with the variation of stability and wall-crossing for moduli spaces of rank 2 pairs, which occur in the fixed locus of this action.

    Citation: Lie Fu, Victoria Hoskins, Simon Pepin Lehalleur. Motives of moduli spaces of rank 3 vector bundles and Higgs bundles on a curve[J]. Electronic Research Archive, 2022, 30(1): 66-89. doi: 10.3934/era.2022004

    Related Papers:

    [1] Álvaro Antón-Sancho . A construction of Shatz strata in the polystable $ G_2 $-bundles moduli space using Hecke curves. Electronic Research Archive, 2024, 32(11): 6109-6119. doi: 10.3934/era.2024283
    [2] Lawrence Ein, Wenbo Niu, Jinhyung Park . On blowup of secant varieties of curves. Electronic Research Archive, 2021, 29(6): 3649-3654. doi: 10.3934/era.2021055
    [3] Yuri Prokhorov . Conic bundle structures on $ \mathbb{Q} $-Fano threefolds. Electronic Research Archive, 2022, 30(5): 1881-1897. doi: 10.3934/era.2022095
    [4] Frédéric Campana . Algebraicity of foliations on complex projective manifolds, applications. Electronic Research Archive, 2022, 30(4): 1187-1208. doi: 10.3934/era.2022063
    [5] Fabian Ziltener . Note on coisotropic Floer homology and leafwise fixed points. Electronic Research Archive, 2021, 29(4): 2553-2560. doi: 10.3934/era.2021001
    [6] Mingjun Zhou, Jingxue Yin . Continuous subsonic-sonic flows in a two-dimensional semi-infinitely long nozzle. Electronic Research Archive, 2021, 29(3): 2417-2444. doi: 10.3934/era.2020122
    [7] Jiaqi Huang, Kaixin Yao, Donghe Pei . Non-lightlike framed rectifying curves in Minkowski 3-space. Electronic Research Archive, 2024, 32(10): 5914-5925. doi: 10.3934/era.2024273
    [8] Jian-Tao Liu, Mei-Tong Fu . Theoretical modeling of thin binder interphases in highly filled PBX composites together with the closed form expression of the effective isotropic moduli of a simplified PBX model. Electronic Research Archive, 2025, 33(2): 1045-1069. doi: 10.3934/era.2025047
    [9] Yi Wei . The Riccati-Bernoulli subsidiary ordinary differential equation method to the coupled Higgs field equation. Electronic Research Archive, 2023, 31(11): 6790-6802. doi: 10.3934/era.2023342
    [10] Juan Gerardo Alcázar, Carlos Hermoso, Hüsnü Anıl Çoban, Uğur Gözütok . Computation of symmetries of rational surfaces. Electronic Research Archive, 2024, 32(11): 6087-6108. doi: 10.3934/era.2024282
  • We prove formulas for the rational Chow motives of moduli spaces of semistable vector bundles and Higgs bundles of rank 3 and coprime degree on a smooth projective curve. Our approach involves identifying criteria to lift identities in (a completion of) the Grothendieck group of effective Chow motives to isomorphisms in the category of Chow motives. For the Higgs moduli space, we use motivic Białynicki-Birula decompositions associated with a scaling action, together with the variation of stability and wall-crossing for moduli spaces of rank 2 pairs, which occur in the fixed locus of this action.



    Let C be a smooth projective geometrically connected curve of genus g1 over a field k. We assume that C admits a degree 1 line bundle. Let N=NC(n,d) (resp. M=MC(n,d)) denote the moduli space of semistable vector bundles (resp. Higgs bundles) of rank n and degree d on C. Throughout this paper we assume that n and d are coprime, so that semistability and stability coincide. The variety N is smooth projective of dimension n2(g1)+1 and the variety M is smooth quasi-projective of dimM=2dimN.

    The cohomology of both N and M have been extensively studied; different approaches to describe their various cohomological invariants should be both unified and refined by working with motivic invariants, which encode finer invariants, like Hodge structures on cohomology groups and also algebro-geometric invariants such as Chow groups. Let us explicitly mention some motivic descriptions of these moduli spaces. The motivic Poincaré polynomial of the vector bundle moduli space N was computed by del Baño [1] using the geometric techniques of [2]; the ideas in [2] were also used to give formulas for the stack of vector bundles on C in the Grothendieck ring of varieties [3] and in Voevodsky's triangulated category of motives over k with rational coefficients [4].

    An algorithm for computing the class of the Higgs moduli space M in the Grothendieck ring of varieties was described by García-Prada, Heinloth and Schmitt [5] using the Białynicki-Birula decomposition associated to the natural scaling action on M considered by Hitchin [6] in rank 2, Gothen [7] in rank 3, and Simpson [8], together with variation of stability for chains of vector bundle homomorphisms. This was upgraded in [9] to a motivic argument in Voevodsky's triangulated category of motives with rational coefficients and, by [9,Corollary 6.9], the motive of M is pure and lies in the tensor subcategory generated by the motive of C.

    In a recent paper [10], we thoroughly studied the rank 2 case and gave formulas for the rational Chow motives of NC(2,d) and MC(2,d), as well as moduli spaces of parabolic bundles and parabolic Higgs bundles by using explicit descriptions of variation of stability as flips.

    In this paper, we proceed to rank 3 and give formulas for the rational Chow motives of N=NC(3,d) and M=MC(3,d) for d coprime to 3. We expect that similar techniques to [10] can be used to give formulas for the motives of moduli spaces of parabolic vector bundles.

    For an integer d coprime to 3 and LPicd(C), we let NL=NC,L(3,d) denote the moduli space of semistable vector bundles with determinant isomorphic to L. The rational Chow motive h(NL) is abelian by [10,Proposition 4.1], and h(N(3,d))h(NL(3,d))h(Jac(C)) by [10,Theorem 1.1]. Hence it suffices to give a formula for the motive h(NL(3,d)).

    Theorem 1.1. Assume that C has a degree 1 line bundle and d is coprime to 3. For any LPicd(C), the rational Chow motive of NC,L(3,d) is

    h(NC,L(3,d))h(C(g1)×C(g1))(3g3)k1+k2<2g2ork1+k2=2g2andk1<g1h(C(k1)×C(k2))Lk1,k2,

    where Lk1,k2 are sums of Tate twists given by Lk1,k2=Q(k1+2k2)Q(8g82k13k2).

    This theorem upgrades a recent computation of the motivic Poincaré polynomial of NC,L(3,1) in the completion ^K0(CHMeff(k,Q)) of the Grothendieck group of effective Chow motives over k along the ideal generated by the Lefschetz motive L=Q(1) due to Gomez and Lee [11] to an isomorphism of Chow motives. In particular, Theorem 1.1 gives information about the Chow groups of NC,L(3,d) and NC(3,d) (see §6.3 for some examples), which is not captured by the previous results on the motivic Poincaré polynomial.

    In general, it is not known if either the map from isomorphism classes in CHMeff(k,Q) to K0(CHMeff(k,Q)) or the natural ring homomorphism K0(CHMeff(k,Q))^K0(CHMeff(k,Q)) are injective. However, in the case of Kimura finite dimensional motives [12] (for example, abelian motives), we show that it is possible to lift identities in ^K0(CHMeff(k,Q)) to isomorphisms in CHM(k,Q) in §2.

    This strategy would theoretically enable one to obtain formulas for the Chow motives of NC,L(n,d) and NC(n,d) in higher ranks; however, one can only apply Corollary 2.3 to lift identities in ^K0(CHMeff(k,Q)) with positive coefficients to CHM(k,Q). Since the motivic Poincaré polynomial of NC,L(n,d) is computed in [1] using a Harder–Narasimhan recursion which involves introducing negative signs, it remains to write these as positive identities in order to obtain corresponding isomorphisms of Chow motives. This appears to be a difficult combinatorial problem in general, which was solved by Gomez and Lee in [11] in rank 3.

    To study the Chow motive of the Higgs moduli space M=MC(3,d) we use the motivic Białynicki-Birula decomposition associated to the Gm-action on the Higgs moduli space given by scaling the Higgs field. In rank 3, this idea was used by Gothen [7] to compute the Poincaré polynomial of M (and of the moduli space of Higgs bundles with fixed determinant). The motive of M is expressed in terms of Tate twists of the motives of the fixed components, which come in four types: one fixed components is N where the Higgs field is zero, then there are components of Type (1, 1, 1) where the underlying bundle decomposes as a sum of line bundles E=L1L2L3 each of which is sent to the next via the Higgs field, and finally there are components of Type (1, 2) and Type (2, 1) where E decomposes as E=LF and E=FL respectively for a line bundle L and the Higgs field maps the first factor to the second.

    Gothen showed that the components of Type (1, 2) and (2, 1) are related to moduli spaces of pairs consisting of a rank 2 vector bundle and a non-zero section which are semistable with respect to an appropriate stability parameter. The variation of stability for these moduli spaces of rank 2 pairs was studied by Thaddeus [13], where he explicitly described the birational wall-crossing transformations as standard flips (or flops). From this description, it is straightforward to compute the motivic Poincaré polynomial of moduli spaces of rank 2 pairs which are semistable with respect to a generic stability parameter (i.e. where semistability and stability coincide). However, in general, these wall-crossing formulas involve negative signs. At this point, we again employ the strategy of §2: we express the motivic Poincaré polynomial of the moduli spaces of rank 2 pairs that we are interested in as a positive combination of motives, so that it can be lifted to an isomorphism in CHM(k,Q). In fact, we give two different formulas for the rational Chow motives of these moduli spaces of rank 2 degree e pairs Pie (here i indexes the chamber in which we take our stability parameter). Let us state the more compact geometric formulation here, which expresses the Chow motives of pair moduli spaces in terms of motives of symmetric powers of C and Jac(C); we refer the reader to Corollary 4.10 for the alternative formula in terms of h1(C). For a polynomial with positive integral coefficients Q(T)=kakTkN[T], we define the Tate motive Q(Q(1)):=kQ(k)akCHM(k,Q).

    Theorem 1.2. Assume that 2i<e4g5. Then the rational Chow motive of the moduli space Pie of rank 2 degree e pairs with stability given by the ith chamber is computed as follows:

    (i) If 3i<e+g, then

    h(Pie)ik=0h(Jac(C)×C(k)×Pe+g3k2)(k).

    (ii) If 3ie+g, then

    h(Pie)h(Jac(C)×Pe2g+1×C(g1))(g1)2g3ik=0h(Jac(C)×C(k)×Pe+g3k2)(k)h(Jac(C)2)Qi,e,g(Q(1))g2k=2g2ih(Jac(C)×C(k)×Pe2g+1)(Q(3g32k)+Q(k)),

    where Qi,e,g(T)N[T] is defined as follows

    Qi,e,g(T):=(TgTe+g12i)(1Tig+1)(1Tig+2)(1T)2(1T2).

    Finally, here is the formula we then obtain for the motive of moduli spaces of rank 3 Higgs bundles. Recall that the Voevodsky motive of this quasi-projective moduli space turns out to be pure ([9,Corollary 6.9]), thus it makes sense to speak of its Chow motive.

    Theorem 1.3. Assume that C has a degree 1 line bundle and d is coprime to 3. The rational Chow motive of the Higgs moduli space MC(3,d) is given by the following expression.

    h(MC(3,d))h(NC(3,d))g2l=0h(Jac(C))[h(P2g2l44g3l6)(2g+3l)h(P2g2l34g3l5)(2g+3l1)](m1,m2)N22m1+m2<6g62m2+m1<6g6m2m1+1mod3h(Jac(C))h(C(m1)×C(m2))(8g8m1m2).

    where h(NC(3,d))h(NC,L(3,d))h(Jac(C)) and the Chow motives of the moduli space NC,L(3,d) of vector bundles with fixed determinant and the pair moduli spaces Pie appearing here are calculated by Theorem 1.1 and Theorem 1.2 (or Corollary 4.10) respectively.

    By plugging in the formulas from Theorem 1.1 and Theorem 1.2, we see that the motive of MC(3,d) is expressed in terms of motives of Jac(C) and symmetric powers of C.

    Theorem 1.3 can be viewed as a lifting of the formula of García-Prada–Heinloth–Schmitt [5,§8] for the class of M in a certain completion of the Grothendieck ring of varieties. Actually, it takes some straightforward but tedious computation to see that our isomorphism indeed recovers the formula in [5].

    We note that the relationship between the Higgs moduli space M and the Higgs moduli space ML with fixed determinant is not as simple as the case for N and NL given by [10,Theorem 1.1]; this was already observed on the level of cohomology in rank n=2 by Hitchin [6] and in rank 3 by Gothen [7]. In fact, in Proposition 5.7, we show that for a general smooth projective complex curve C, the rational Chow motive of ML,C(n,d) for any n and any d coprime to n is not contained in the tensor subcategory generated by the motive of C.

    Finally, we give some explicit formulas in low genus and applications to Chow groups in §6.

    Throughout C denotes a smooth projective geometrically connected curve over a field k which we assume admits a degree 1 line bundle. We let C(m) denote the m-fold symmetric power of C and let Jac(C) denote the Jacobian of C.

    We write CHM(k,Q) for the category of Chow motives over k with coefficients in Q and we follow a homological convention for morphisms. With this convention, we have a covariant functor h:SmProjkCHM(k,Q) associating to a smooth projective k-variety X its rational Chow motive h(X). In particular, for a smooth k-variety X whose motive is pure, the rational Chow groups of X can be computed as homomorphism groups in CHM(k,Q) as follows

    CHi(X)Q=HomCHM(k,Q)(h(X),Q(i)). (1.1)

    Since the Higgs moduli space M is only quasi-projective, the natural way to associate a motive to M is via the triangulated category DM(k,Q) of Voevodsky motives over k with rational coefficients. However, by [9,Corollary 6.9], this motive is pure and thus we can view it as a Chow motive by identifying CHM(k,Q) with a full subcategory of DM(k,Q) via the fundamental embedding theorem of Voevodsky [14] (see [10,§2.2]).

    Definition 2.1. The motivic Poincaré polynomial χ(X) of a smooth projective k-variety X is the image of the rational Chow motive h(X) in the completion ^K0(CHMeff(k,Q)) of the Grothendieck ring of effective rational Chow motives over k along the ideal generated by the Lefschetz motive L=[Q(1)].

    This notion was introduced in [1], because power series in L occur naturally and unavoidably in his computations. In general, it is not known if either the natural ring homomorphism K0(CHMeff(k,Q))^K0(CHMeff(k,Q)) or the map from isomorphism classes in CHMeff(k,Q) to K0(CHMeff(k,Q)) are injective. However, with Kimura's assumption on finite dimensionality [12], we have the following result (already appeared in [23,Lemme 13.2.1.1] and exploited in [10,Theorem 4.3]).

    Proposition 2.2. Given effective Chow motives N,MCHMeff(k,Q) which are Kimura finite dimensional and whose classes in ^K0(CHMeff(k,Q)) coincide, there is an isomorphism NM in CHMeff(k,Q).

    Proof. The equality in ^K0(CHMeff(k,Q)) also determines a corresponding isomorphism in the category Meffnum(k,Q) of effective numerical motives (because Meffnum(k,Q) is semisimple [15], see the proof of [10,Theorem 4.3]). In particular, the equality holds in Mnum(k,Q). Since the restriction of the functor from Chow motives to numerical motives to the subcategory of Kimura finite dimensional Chow motives is full and conservative (see [16]), we deduce that the isomorphism also holds in CHM(k,Q).

    We note that the above isomorphism is not explicit. More precisely, we can lift positive identities in ^K0(CHMeff(k,Q)) to isomorphisms in CHM(k,Q), when the terms appearing are Kimura finite dimensional, as in the following corollary.

    Corollary 2.3. Let X be a smooth projective variety, whose Chow motive h(X) is Kimura finite dimensional (for example, h(X) is an abelian motive). Given any effective identity in ^K0(CHMeff(k,Q)) expressing the motivic Poincaré polynomial χ(X) as a polynomial in L

    χ(X)=Ni=0χ(Xi)Li

    whose coefficients are motivic Poincaré polynomials of smooth projective varieties Xi with h(Xi) being Kimura finite dimensional, there is a corresponding isomorphism in CHM(k,Q); that is,

    h(X)Ni=0h(Xi)(i).

    This corollary also holds when X and Xi are varieties (not necessarily smooth or projective) whose motives are pure.

    For two coprime positive integers n and d, let N=NC(n,d) denote the moduli space of semistable vector bundles of rank n and degree d on C. If L is a degree d line bundle on C, we can also consider the moduli space NL=NC,L(n,d) of rank n semistable vector bundles with determinant LPicd(C). In [10], we computed the rational motives of N and NL for n=2. In this section, we will consider the case of rank n=3.

    Our starting point is a formula for the motivic Poincaré polynomial χ(NL) recently established by Gomez and Lee [11,Theorem 1.3], which goes back to the work of del Baño [1] on the motive of NL.

    Theorem 3.1 (Gomez–Lee). Let L be a degree 1 line bundle on C. The motivic Poincaré polynomial of NL(3,1) is as follows:

    χ(NL(3,1))=χ(C(g1)×C(g1))L3g3+k1+k2<2g2ork1+k2=2g2andk1<g1χ(C(k1)×C(k2))Lk1,k2

    where Lk1,k2=Lk1+2k2+L8g82k13k2.

    Remark 3.2 (Independency on the degree d in rank 3). Note that the operation of taking dual bundles EE preserves stability, hence gives rise to an isomorphism of moduli spaces NL(n,d)NL(n,d) and N(n,d)N(n,d). Now specializing to rank n=3 and assuming the existence of a degree 1 line bundle on C, we have N(3,1)N(3,1) and N(3,d)N(3,d+3). Hence when Pic1(C), the isomorphism class of N(3,d) is independent of d, provided that (3,d)=1.

    We use a similar trick to [10,Theorem 4.3] as described in §2 above to upgrade Gomez–Lee's identity in ^K0(CHMeff(k,Q)) to an isomorphism in the category CHM(k,Q).

    Theorem 3.3. Let C be a smooth projective curve defined over k admitting a degree 1 line bundle. For any dZ which is coprime to 3 and for any LPicd(C), the rational Chow motive of NC,L(3,d) is

    h(NC,L(3,d))h(C(g1)×C(g1))(3g3)k1+k2<2g2ork1+k2=2g2andk1<g1h(C(k1)×C(k2))Lk1,k2,

    where Lk1,k2 are sums of Tate twists given by Lk1,k2=Q(k1+2k2)Q(8g82k13k2).

    The rational Chow motive of N=NC(3,d) is

    h(N(3,d))h(NL(3,d))h(Jac(C)).

    Proof. In view of Remark 3.2, we can assume without loss of generality that d=1.

    Since the formula of Gomez and Lee in ^K0(CHMeff(k,Q)) is an equality between virtual motives with positive coefficients and the Chow motive h(NL(3,d)) is abelian by [10,Theorem 4.1] (and thus Kimura finite dimensional [16,Théorème 2.8]), we can apply Corollary 2.3 to deduce the claimed isomorphism in CHM(k,Q).

    The final isomorphism follows from [10,Theorem 1.1].

    Moduli of pairs (V,ϕ) consisting of a vector bundle V on C and a non-zero section ϕH0(C,V) have been studied by Bradlow [17] and Thaddeus [13], who gave a GIT construction of pair moduli spaces depending on a stability parameter σQ>0. In this section, we focus on moduli spaces of rank 2 pairs, as in our later application to Higgs bundles, rank 2 pairs are related to rank 3 Higgs bundles via a Białynicki-Birula decomposition studied by Gothen [7] (see §5.3.2 and §5.3.3 below).

    Definition 4.1. A rank 2 pair (V,ϕ) is σ-semistable if for all line subbundles MV, we have

    μ(M)μ(V)ϵ(M,ϕ)σwhere ϵ(M,ϕ):={1if ϕH0(C,M)1else.

    If this equality is strict for all M, we say that (V,ϕ) is σ-stable.

    Fix a stability parameter σ and a degree e>0 (resp. a degree e line bundle L on C); then there is a projective moduli space Pσss=PσssC(2,e) (resp. PσssL) of σ-semistable pairs on C of rank 2 and degree e (resp. with determinant isomorphic to L) constructed as a GIT quotient [13]. For generic σ (where semistability and stability coincide), the pair moduli spaces are smooth and have dimension

    dim(PσssC(2,e))=e+2g2.

    The motives of moduli spaces of pairs will naturally appear in §5.3.2 and §5.3.3 below. To study their motives, we use Thaddeus' description [13] of the birational transformations between these moduli spaces as the stability parameter σ varies, as explicit standard flips. This immediately gives rise to formulas for the motivic Poincaré polynomials of moduli spaces of pairs in the Grothendieck ring of Chow motives and then we apply Proposition 2.2 by finding a positive expression for the motivic Poincaré polynomials of moduli spaces of pairs.

    Let us first recall the notion of standard flips/flops.

    Definition 4.2 (Standard flip). Let S be a smooth projective variety and ϕ:XX be a birational transformation between smooth projective varieties. We say that ϕ is a standard flip of type (m,l) with centre S if there are closed smooth subvarieties ZX and ZX which are projective bundles over S of relative dimensions m and l respectively such that the blow-up ˜X of X along Z coincides with the blow-up of X along Z with common exceptional divisor E. This is summarised by the following diagram

    where the top two squares are blow-up squares and the outer square is cartesian. When m=l, we call this a standard flop.

    Thaddeus studied variation of stability for rank 2 degree e pairs (V,ϕ) in [13]. The space of stability parameters Q>0 admits a wall and chamber decomposition given by considering how the notion of (semi)stability changes as σ varies. The moduli space Pσ(2,e) is non-empty if and only if σe/2 by [13,(1.3)], and so we can restrict our attention to the interval (0,e/2]. There is a finite set W(0,e/2] of walls; that is, critical values of σ for which semistability and stability do not coincide (i.e. there is a line subbundle of degree e with e=e/2±σ). The walls are given by σ0>>σm where m=(e1)/2 and σi:=e/2i by purely numerical considerations. The connected components of (0,e/2]W are called chambers which we also label from right to left as Ci=(σi+1,σi), where for notational convenience, we set σm+1:=0 (which is not a stability parameter). In each chamber Ci, semistability and stability coincide and the corresponding moduli space of pairs is smooth and only depends on the chamber; thus we write Pie:=Pσss(2,e) (resp. PiL:=PσssL(2,e)) for the moduli space of pairs (resp. with determinant L) which are stable with respect to σCi.

    Theorem 4.3 (Thaddeus [13]). For degree e3, let m=(e1)/2 and let P0L,,PmL be the moduli spaces of stable pairs of rank 2 vector bundles with determinant a degree e line bundle L and for stability parameters appearing in each of the C0,,Cm chambers introduced above.

    (i) The extremal moduli space P0L is the moduli space of non-split extensions of L by OC and consequently we have P0LP(H1(C,L1))Pe+g2.

    (ii) The opposite extremal moduli space PmL admits a natural map π:PmLNL=NL(2,e) given by forgetting the section. If e>2g2, then π is surjective with fibre P(H0(C,E)) over ENL. If e>4g4, then π is a Pe2g+1-bundle.

    (iii) There is a standard flip Pi1LPiL of type (i1,e+g2(i+1)) with centre C(i).

    If one does not fix the determinant L, then there is a similar picture where (i) P0ePice(C) is a Pe+g2-fibration, (ii) there is a forgetful map π:PmeN which is a Pe2g+1-fibration for e>4g4 and (iii) one replaces the centres of the flips C(i) with Picei(C)×C(i) (see [25,§8]). More precisely, the relationship between these moduli spaces of stable pairs is illustrated by the following diagram

    We can easily calculate the motivic Poincaré polynomial of Pie.

    Lemma 4.4. We have

    χ(Pie)=ij=0χ(Picej(C)×C(j))Le+g2j1LjL1.

    Proof. This follows directly from Theorem 4.3 (see the above diagram).

    Corollary 4.5. When 3ie+g1, we have an isomorphism in CHMeff(k,Q):

    h(Pie)h(Jac(C))(ij=0e+g2j2k=jh(C(j))(k)).

    Proof. The change in integral Chow motives of smooth projective varieties under a standard flip is described by a recent result of Jiang [18]. Combined with Theorem 4.3 (note that the canonical class is always increasing along the flips, under the numerical hypothesis), we get the formula in the statement, even in CHM(k,Z).

    We give here a quick proof without using the somewhat difficult result of Jiang. Note that the motives in the formula in Lemma 4.4 are all Kimura finite dimensional and all coefficients are positive, when 3ie+g1. Hence we can apply Corollary 2.3 to deduce that

    h(Pie)ij=0h(Picej(C)×C(j))(e+g2j2k=jQ(k)).

    In order to get the desired form, it suffices to identify Picej(C) with Jac(C).

    Observe that the formula in Lemma 4.4 contains terms with negative coefficients, when 3i>e+g1. The main goal of the next two sections is to deal with this case. In fact, we will give two formulas for the rational Chow motive of Pie. Just as in the second proof of Corollary 4.5, our strategy is to work in the Grothendieck ring of Chow motives and establish an expression of the motivic Poincaré polynomial of these pairs moduli spaces in terms of Kimura finite dimensional motives with positive coefficients in order to apply Proposition 2.2 or Corollary 2.3.

    Choosing a zero-cycle z of degree 1 on C (its existence is guaranteed by the hypothesis that Pic1(C)), we have

    h(C)Qh1(C)Q(1),

    in the category CHMeff(k,Q), where h1(C):=(C,ΔCz×CC×z), which can be appropriately called the Jacobian motive of C. In some sense, h1(C) is the most fundamental indecomposable building block for objects in the tensor subcategory of CHM(k,Q) generated by h(C). The purpose of this section is to give a formula of the rational Chow motive of the pair moduli space Pie in terms of h1(C).

    The following facts will be the main ingredient:

    Lemma 4.6 (Künnemann [19]). Let g be the genus of C and b a positive integer.

    (i) Symb(h1(C))=0 if b>2g.

    (ii) For any gb2g, we have in CHMeff(k,Q),

    Symb(h1(C))Sym2gbh1(C)Q(bg).

    Hence [Symbh1(C)]=[Sym2gbh1(C)]Lbg in K0(CHMeff(k,Q)).

    Proposition 4.7. The following identity holds in ^K0(CHM(k,Q)).

    χ(Pie)=χ(Jac(C))ib=0[Symb(h1(C))](LbLe+g12i)(1Lib+1)(1Lib+2)(1L)2(1L2)

    Proof. Note that in CHM(k,Q),

    h(C(j))Symj(h(C))Symj(Qh1(C)Q(1))a+b+c=jSymbh1(C)Q(c).

    Taking their classes in K0(CHM(k,Q)), we obtain that

    χ(C(j))=a+b+c=j[Symbh1(C)]Lc.

    After plugging this into the formula in Lemma 4.4 and exchanging the two summations, we obtain that

    χ(Pie)=χ(Jac(C))ib=0[Symb(h1(C))]ij=b(1Ljb+1)(LjLe+g2j1)(1L)2.

    We then compute

    (1L2)ij=b(1Ljb+1)(LjLe+g2j1)=Lb+Lb+1Li+1Li+2Lb+1+L2ib+3Le+g2i1+Le+g2b+2+Le+gbi+Le+gbi+1Le+g2b+2Le+g2=(LbLe+g12i)(1Lib+1)(1Lib+2)

    which proves the claimed formula.

    Definition 4.8. Fix g2. Let i,e,b be positive integers satisfying bi<e/2. Define

    Qi,e,b(T):=(TbTe+g12i)(1Tib+1)(1Tib+2)(1T)2(1T2)Z[T], (4.1)

    which is a polynomial with integral coefficients. The coefficients are positive if e+g12i>b and are negative if e+g12i<b.

    The following elementary result is crucial for our purpose:

    Lemma 4.9. Assume that e+g12i<bi<e22g3, which implies that bg+1. The polynomial

    Ri,e,b(T):=TbgQi,e,b(T)+Qi,e,2gb(T)

    has positive coefficients.

    Proof. Define a partial order on Z[T] by claiming that P(T)0 if and only if all coefficients of P(T) are positive. Then

    TbgQi,e,b(T)+Qi,e,2gb(T)=(T2gbTe+g12i)(1Ti2g+b+1)(1Ti2g+b+2)Tbg(Te+g12iTb)(1Tib+1)(1Tib+2)(1T)2(1T2)(T2gbTe+g12i)(1Ti2g+b+1)(1Tib+2)Tbg(Te+g12iTb)(1Tib+1)(1Tib+2)(1T)2(1T2)=(1Tib+2)(1T)2(1T2)[(T2gbTe+g12i)(1Ti2g+b+1)Tbg(Te+g12iTb)(1Tib+1)](1Tib+2)(1T)2(1T2)[(T2gbTg)(1Ti2g+b+1)Tbg(TgTb)(1Tib+1)]=(1Tib+2)T2gb(1T)2(1T2)[(1Tbg)(1Ti2g+b+1)(T2b2gT3b3g)(1Tib+1)]=(1Tib+2)T2gb(1Tbg)(1T2b2g)(1T)2(1T2)0,

    where the first inequality uses b>g and the second inequality uses e2i1.

    In the sequel, for a polynomial P(T)=nj=0mjTj with positive integral coefficients, we denote by P(Q(1)) the effective Tate motive nj=0Q(j)mj.

    Corollary 4.10. Assume that i<e22g3, then the rational Chow motive of Pie is as follows:

    (i) If 3ie+g1, then

    h(Pie)h(Jac(C))(ib=0Symb(h1(C))Qi,e,b(Q(1))).

    (ii) If 3i>e+g1, then 0<2gige+2i<g<g+e2ii, and

    h(Pie)h(Jac(C))(b<2gior|bg|<e2iSymb(h1(C))Qi,e,b(Q(1))ge+2ib=2giSymb(h1(C))Ri,e,2gb(Q(1))).

    Here Qi,e,b is the polynomial in Definition 4.8 and Ri,e,2gb is the polynomial defined in Lemma 4.9.

    Proof. By Proposition 2.2, it suffices to check that both sides agree in K0(CHM(k,Q)). For case (i), it follows directly from Proposition 4.7 and the definition of Qi,e,b in Definition 4.8. For case (ii), the non-positive part in the expression of χ(Pie) in Proposition 4.7 is

    χ(Jac(C))ib=g+e2i[Symb(h1(C))]Qi,e,b(L).

    It can be absorbed by the following effective part of χ(Pie) with b running in the symmetric range with respect to g:

    χ(Jac(C))ge+2ib=2gi[Symb(h1(C))]Qi,e,b(L).

    Indeed, for any b[e+g2i,i], by Lemma 4.6,

    [Symb(h1(C))]Qi,e,b(L)+[Sym2gb(h1(C))]Qi,e,2gb(L)=[Sym2gb(h1(C))]LbgQi,e,b(L)+[Sym2gb(h1(C))]Qi,e,2gb(L)=[Sym2gb(h1(C))]Ri,e,b(L),

    which is a positive integral linear combination of effective motives by Lemma 4.9.

    In this section, we compute the rational Chow motive of Pie again, but in terms of symmetric powers C(k) and Jac(C). The following basic fact will be our key tool:

    Lemma 4.11. ([11,Proposition 1.6(i)]). For any gj2g2, we have the following identity in K0(CHM(k,Q)):

    χ(C(j))=χ(C(2g2j))Lj+1g+χ(Jac(C))χ(Pjg).

    Remark 4.12. Corollary 2.3 allows one to lift the equality in Lemma 4.11 to an isomorphism in the category of rational Chow motives. Note that the result for integral Chow groups is recent obtained by Jiang [18,Section 5.1].

    In the sequel, we impose the numerical constraint that

    2i<e4g5,

    which will be sufficient for all the pair moduli spaces appearing in Theorem 1.3. In view of Corollary 4.5, we assume furthermore that

    3i>e+g1,

    which implies that ig and e2g+1. To summarise, from now on, we work under the following hypothesis

    3ie+g and 2g2i<e4g5. (4.2)

    Proposition 4.13. Under the above numerical assumptions, the following identity holds in ^K0(CHMeff(k,Q)) :

    χ(Pie)=χ(Jac(C))χ(C(g1))Lg1Leg+11L+χ(Jac(C))2g3ik=0χ(C(k))LkLe+g2k11L+χ(Jac(C))g2k=2g2iχ(C(k))(L3g32k+Lk)1Le2g+21L+χ(Jac(C)2)Lg(1Le2i1)(1Li+1g)(1Li+2g)(1L)2(1L2).

    Proof. Note that under these assumptions, we have gi2g2. Therefore, we apply Lemma 4.11 to the symmetric powers C(j) in the formula in Lemma 4.4 with gji. It is then a straightforward computation to obtain the following formula

    χ(Pie)=χ(Jac(C))g1k=0χ(C(k))LkLe+g2k11L+χ(Jac(C))g2k=2g2iχ(C(k))L3g32kLe2g+2+k1L+χ(Jac(C)2)igk=0(1Lk+1)(Lk+gLeg12k)(1L)2=χ(Jac(C))χ(C(g1))Lg1Leg+11L+χ(Jac(C))2g3ik=0χ(C(k))LkLe+g2k11L+χ(Jac(C))g2k=2g2iχ(C(k))(L3g32kLe2g+2+k1L+LkLe+g2k11L)+χ(Jac(C)2)igk=0(1Lk+1)(Lk+gLeg12k)(1L)2.

    Note that

    L3g32kLe2g+2+k1L+LkLe+g2k11L=(L3g32k+Lk)1Le2g+21L.

    It remains to check that

    igk=0(1Lk+1)(Lk+gLeg12k)(1L)2=Lg(1Le2i1)(1Li+1g)(1Li+2g)(1L)2(1L2),

    which follows as in the computation at the end of Proposition 4.7.

    We are now able to prove Theorem 1.2.

    Proof of Theorem 1.2. The formula in the first case is just a reformulation of Corollary 4.5. In the second case, we apply Proposition 2.2 to Proposition 4.13.

    We recall that a Higgs bundle on C is a pair (E,Φ) consisting of a vector bundle E and a Higgs field Φ:EEωC which is a OC-linear homomorphism. There is a notion of semistability for Higgs bundles which involves verifying an inequality of slopes for Higgs subbundles (i.e., vector subbundles which are invariant under the Higgs field). This enables the construction of the moduli space M=M(n,d) of semistable rank n degree d Higgs bundles on C as a quasi-projective variety via Geometric Invariant Theory. In the case where n and d are coprime, semistability and stability coincide and M is smooth; moreover M is a non-compact hyper-Kähler manifold over k=C [6].

    There is a Gm-action on M given by scaling the Higgs field which was used by Hitchin [6] and Simpson [8] to study the geometry of M. They established that this Gm-action is semi-projective in the sense that

    ● the fixed locus is proper and

    ● the limit of tGm acting on any point in M exists as t tends to zero;

    for details on the proof, see [24,Section 9]. The flow under this action induces an associated Białynicki-Birula decomposition [20] and, when M is smooth, this is a deformation retract to the fixed locus. Consequently, the Voevodsky motive of M is pure [9,Corollary 6.9] and we can consider its associated Chow motive (for details, see [10,Theorem 2.4 and §6.1.1]).

    For a point (E,Φ)M fixed by the Gm-action, either the Higgs field Φ is zero (in which case the underlying vector bundle is a semistable vector bundle) or the Higgs field is non-zero and so there is GmAut(E) inducing a weight decomposition E=iEi and with respect to this decomposition Φ is given by non-trivial homomorphisms EiEi+1ωC. Consequently, if Φ0, we obtain a chain of vector bundle homomorphisms

    Ei0Ei0+1ωCEi0+2ω2CEi0+mωmC.

    The fixed components with Φ0 are then indexed by the discrete invariants of this chain (this is equivalent to fixing the ranks and degrees of the Ei).

    Once one fixes discrete invariants for chains (i.e. a tuple n_ and d_ corresponding to the ranks and degrees of the vector bundles in the chain), one can construct projective moduli spaces of chains which are semistable with respect to a stability parameter α (a tuple of real numbers indexed by the vector bundles in the chain) via Geometric Invariant Theory [21]. The deformation theory and wall-crossing for chains were studied in [22], as well as the relationship between stability for chains and Higgs bundles. In particular, the connected components of the fixed point set of the Gm-action on M are moduli spaces of αH-semistable chains for different discrete invariants, where αH is a Higgs stability parameter satisfying αH,iαH,i+1=2g2 for all i (see [8] and [9,Corollary 2.6]). Provided n and d are coprime, the Higgs stability parameter is generic for the discrete invariants for chains appearing as fixed loci components (i.e., semistability and stability coincide and these chain moduli spaces are smooth projective varieties). Hence, the fixed locus consists of the moduli space N of semistable vector bundles and moduli spaces of αH-semistable chains with various discrete invariants.

    For small values of n and for values of d coprime to n, this Gm-action has been used to calculate the Poincaré polynomial of M in rank n=2 by Hitchin [6] and in rank n=3 by Gothen [7]; in these low rank computations, the fixed loci are related to symmetric powers of C, the Jacobian of C and moduli spaces of pairs (consisting of a vector bundle and a section) studied by Bradlow [17] and Thaddeus [13], which depend on a stability parameter.

    This scaling action is also used in the study the class of M in the Grothendieck ring of varieties in [5] and the Voevodsky motive of M in [9], where wall-crossing for chains plays an important role. In rank n=2 and odd degree, we obtained a formula for the integral motive of M in [10,Theorem 1.4] in terms of N.

    In order to compute the motive of the Higgs bundle moduli space in rank 3 and coprime degree d, we will use the motivic Białynicki-Birula decomposition associated to the Gm-action on M and Gothen's description of the fixed components [7]. Since the motive of M is pure, we can view the motivic Białynicki-Birula decomposition as an isomorphism in CHM(k,Q). For this calculation, we need to describe the motive of each component in the fixed locus. By specifying the ranks of the vector bundles in the chain, we split the possible fixed components into the following types:

    Type (1, 1, 1): (E,Φ) with E=L1L2L3 a sum of three line bundles and Φi:LiLi+1ωC,

    Type (1, 2): (E,Φ) with E=LF for a line bundle L with Φ:LFωC,

    Type (2, 1): (E,Φ) with E=FL for a line bundle L with Φ:FLωC,

    Type (3): (E,Φ) with Φ=0 and E a rank 3 semistable vector bundle.

    In the last case, Type (3), there is only one fixed component: the moduli space N=NC(3,d) of semistable vector bundles of rank n=3 and degree d on C. For all the other types, there are different components indexed by the possible degrees of the vector bundles in the chain. We modify Gothen's description of the fixed components of each type for Higgs bundles with fixed determinant to arbitrary determinant in the following sections.

    The Chow motive of the Higgs moduli space will be, via the motivic Białynicki-Birula decomposition, a sum of motives corresponding to each type:

    h(MC(3,d))=h(NC(3,d))M(1,1,1)M(2,1)M(1,2) (5.1)

    where the Chow motives M(1,1,1), M(2,1) and M(1,2) will be each computed in turn below. Note that a priori, these motives depend on d. Each of these motives is a direct sum of Tate twists of the motives of the fixed components of that type. The Tate twist appearing with a fixed component F is the codimension of the corresponding Białynicki-Birula stratum F+ (which retracts onto F via the downwards flow); since the downward flow is Lagrangian,

    codim(F+)=12dim(M(3,d))dim(F)=9(g1)+1dim(F).

    Suppose that (E,Φ) is a stable Higgs bundle fixed by the scaling action of Type (1, 1, 1); then E=L1L2L3 and

    Φ=(000ϕ1000ϕ20)

    where ϕi:LiLi+1ωC are non-zero. Let li:=deg(Li); then d=l1+l2+l3. The non-zero homomorphisms ϕi correspond to non-zero sections of the line bundle Mi=L1iLi+1ωC, which has degree mi=li+1li+2g20. Given M1 and M2 and one of the three line bundles (say L2), we can determine the other two line bundles (L1=L2M11ωC and L2=L3M12ωC). Hence, the fixed points (L1L2L3,Φ) with degrees (l1,l2,l3) are parametrised by

    Picl1(C)×C(l2l1+2g2)×C(d2l2l1+2g2).

    The possible ranges for (l1,l2) are determined by ϕi being non-zero and stability of (E,Φ): the Φ-invariant subbundles of E are L2L3 and L3 and stability of (E,Φ) implies

    l2+l32<d3andl3<d3.

    If we equivalently phrase these inequalities in terms of mi, we get

    2m1+m2<6g6andm1+2m2<6g6

    and we recover the li by noting that 3l2=d+m1m2. Hence, we need dm2m1 modulo 3; we note that this last constraint was accidentally omitted by Gothen and consequently resulted in an error in the formula for the Poincaré polynomial stated in [7]; this was later corrected in [24,§10] and in the formula for the virtual motivic class in [5,Appendix].

    Corollary 5.1. The fixed locus components of Type (1, 1, 1) are given by

    F(1,1,1)=(m1,m2)N2max(2m1+m2,m1+2m2)<6g6dm2m1mod3Pic(d+m1m2)/3(C)×C(m1)×C(m2).

    Thus the contribution M(1,1,1) in (5.1) to the Chow motive of the Higgs bundle moduli space is

    M(1,1,1)=(m1,m2)N2max(2m1+m2,m1+2m2)<6g6dm2m1mod3h(Pic(d+m1m2)/3(C))h(C(m1))h(C(m2))(8g8m1m2).

    Remark 5.2. A priori F(1,1,1) depends on d and so we should really write F(d)(1,1,1). However, assuming that C has a degree 1 line bundle, the map (m1,m2)(m2,m1) determines an isomorphism

    F(d)(1,1,1)F(d)(1,1,1).

    Suppose that (E,Φ) is a stable Higgs bundle fixed by the scaling action of Type (1, 2); then E=LF and Φ is determined by a non-zero homomorphism LFωC. Equivalently, we can think of this non-zero homomorphism as a non-zero section ϕ of the vector bundle V:=L1FωC. Gothen bounded the possible values of l:=deg(L) as follows

    d3<l<d3+g1 (5.2)

    using stability of (E,Φ) and the fact that the homomorphism LFωC is non-zero. Hence (E,Φ) determines a line bundle L of degree l and a pair (V,ϕ) consisting of a rank 2 vector bundle of degree e:=d3l+4g4 and a non-zero section. Gothen [7] showed that Higgs stability of (E,Φ) corresponds to pair stability of (V,ϕ) for a particular value of the stability parameter σ.

    Proposition 5.3 ([7,Proposition 2.5]). The component of the Gm-fixed locus consisting of Higgs bundles (E=LF,Φ:LFωC) of Type (1, 2) with deg(L)=l satisfying Eq (5.2) is isomorphic to the product Picl(C)×Pσd,lss(2,ed,l) where ed,l:=d3l+4g4 and σd,l=l2d6.

    Consequently, we obtain the following description of the fixed locus components of Type (1, 2) and the motivic contribution M(1,2) in Eq (5.1).

    Corollary 5.4. The fixed locus components in MGm of Type (1, 2) are given by

    F(1,2)=d3<l<d3+g1Picl(C)×Pσd,lss(2,ed,l)

    where ed,l:=d3l+4g4 and σd,l=l2d6. Hence, the contribution M(1,2) in Eq (5.1) to the Chow motive of the Higgs bundle moduli space is

    M(1,2)=d3<l<d3+g1h(Picl(C))h(Pσd,lss(2,ed,l))(2g2d+3l).

    If we make a change of variables k=ld31, then 3ld=3k+3x where x{1,2} satisfies xd mod 3. Hence, we have

    M(1,2)=g2k=0h(Pick+1+dx3(C))h(P(k+12x6)ss(2,4g3k7+x))(2g+3k+1x). (5.3)

    For 0kg2, pairs of degree e(k,x):=4g3k7+x have different moduli spaces Pje(k,x) corresponding to the different chambers Cj in which the stability parameter lies (see Theorem 4.3). The stability parameter k+12x6 lies in the chamber Cik where ik=2g2k5+x and so

    P(k+12x6)ss(2,4g3k7+x))P2g2k5+x4g3k7+x

    and the Chow motive of this pairs moduli space is calculated by Corollary 4.10 above.

    The dual of a Higgs bundle (E,Φ) is given by (E,ΦIdωC) and preserves stability. Furthermore, the dual of a stable Higgs bundle of Type (2, 1) is a stable Higgs bundle of Type (1, 2). More precisely, if we write the fixed loci as depending on d as F(d)(1,2) and F(d)(2,1), then dualising gives an isomorphism F(d)(2,1)F(d)(1,2). Therefore, the fixed components of Type (2, 1) with degree d are indexed by

    d3+1g<j<d3 (5.4)

    Proposition 5.5 ([7,Proposition 2.9]). The component of the Gm-fixed locus consisting Higgs bundles (E=FL,Φ:FLωC) of Type (2, 1) with deg(L)=j satisfying Eq (5.4) is isomorphic to the product Picj(C)×Pσd,jss(2,fd,j) where fd,j:=3jd+4g4 and σd,j:=d6j2.

    Corollary 5.6. The fixed locus components of Type (2, 1) are

    F(2,1)=d3+1g<j<d3Picj(C)×Pσd,jss(2,fd,j)

    where fd,j:=3jd+4g4 and σd,j:=d6j2. Hence, the contribution M(2,1) in Eq (5.1) to the Chow motive of the Higgs bundle moduli space is

    M(2,1)=d3+1g<j<d3h(Picj(C))h(Pσd,jss(2,fd,j))(2g23j+d).

    If we make a change of variables k=d3j, then d3j=3k+x where x{1,2} satisfies xd mod 3. Then we have

    M(2,1)=g2k=0h(Picdx3k(C))h(P(k2+x6)ss(2,4g3k4x))(2g+3k2+x). (5.5)

    For 0kg2 and degree f(k,x):=4g3k4x, the pairs stability parameter k2+x6 lies in the chamber Ci(k) where i(k)=2g2k2x and so

    P(k+12x6)ss(2,4g3k7+x))P2g2k2x4g43kx.

    In this section, by putting the results in the previous sections together, we compute the Chow motive of MC(3,d), the moduli spaces of rank 3 stable Higgs bundles of degree d, which is coprime to 3.

    Proof of Theorem 1.3. Analogously to Remark 3.2, by taking dual Higgs bundles and tensoring with line bundles, we see that the isomorphism class of the moduli space M(3,d) is independent of d as long as (3,d)=1 and Pic1(C)(k). Therefore, without loss of generality, we can assume that d=1, and identify Picj(C) with Jac(C).

    We apply the motivic Białynicki-Birula decomposition in the form of [9,Theorem A.4 (i)]: the statement follows from Eq (5.1) and the combination of Corollaries 5.1, 5.4 and 5.6 (see also Eqs (5.3) and (5.5) and note that we now take d=1 so x=1).

    The rational Chow motive of M(n,d) for any rank n and coprime degree d lies in in the thick tensor subcategory generated by the motive of C [9]. As observed in the rank 2 case in [10,Proposition 6.3], for a line bundle L of odd degree d on a general complex curve C, the rational Chow motive of ML(2,d) is not in the thick tensor subcategory generated by the motive of C. We have a similar phenomenon in any rank n.

    Proposition 5.7. If C is a general complex curve, then for a line bundle L of degree d coprime to n, the rational Chow motive of ML(n,d) is not in the thick tensor subcategory generated by the motive of C.

    Proof. Consider the fixed loci of the scaling action on ML=ML(n,d). Similarly to Gothen's description in rank 3, we have fixed components of Type (1,,1) consisting of Higgs bundles (E,Φ) where E=ni=1Li is a sum of line bundles and the Higgs field is given by non-zero homomorphisms ϕi:LiLi+1ωC. Without fixing the determinant, this data is parametrised by a Picard group and n1 copies of symmetric powers of C (one symmetric power for each ϕi). Fixing the determinant, results in fixed loci of Type (1,,1) the form

    ~C(m1)××C(mn1),

    which is the degree n2g étale cover of C(m1)××C(mn1) obtained as the pullback of the isogeny Jac(C)nJac(C). For the fixed determinant case, these fixed loci are discussed in rank n=2 in [6] and n=3 in [7]. The range of possible values of mi is bounded by degree reasons and stability of the Higgs pair (E,Φ). In particular (taking all but one mi to be zero and mi=1), the motive of ˜C appears as a direct summand in the motive of ML by the motivic Białynicki-Birula decomposition.

    We claim that h(˜C) (hence ML also) does not belong to the tensor subcategory generated by h(C). Indeed, the same argument in [10,Proposition 6.3] shows that Jac(˜C) is isogenous to the product

    tH1(C,Z/nZ)At,

    where At is the complement abelian variety of Jac(C) in Jac(Ct) associated with the not necessarily connected étale n-fold cover CtC determined by t. Therefore, it suffices to show that for some t, the Hodge structure H1(At,Q) is not in the tensor subcategory H1(C,Q)QHS of the category of rational Hodge structures generated by H1(C,Q). To this end, observe that for the n-fold covers of the form At=(n2j=1C)CC with CC a connected étale double cover, At is isogenous to Jac(C)n2×Prym(C/C), where Prym(C/C) is the Prym variety associated with the double cover C/C. By an argument using the representation theory of speical Mumford–Tate groups in [10,Proposition 6.3], we know that H1(Prym(C/C),Q)H1(C,Q)QHS provided that C is general.

    In this section, we give formulas for the motives of MC(3,d) when g=2,3, as well as the resulting Hodge numbers (which were already implicitly known in rank 3 and arbitrary genus by [5,Appendix]). The Hodge diamonds in this section were generated using Belmans' Hodge diamond cutter [26].

    For ease of notation, for integers m1<m2<<mr, let

    Tm1,m2,,mr=Q(m1)Q(m2)Q(mr)andT[m1,m2]=m2i=m1Q(i).

    We also let J:=Jac(C) denote the Jacobian of C.

    For a curve C of genus g=2, the rational Chow motive of NC(3,d) and MC(3,d), for d coprime to 3, are given as follows.

    h(NC(3,d))h(J)(T0,8h(C)T1,2,5,6h(C(2))T2,4h(C2)(3));h(MC(3,d))h(J)(T0,8h(C)T1,2,5,6,7h(C(2))T2,4,6h(C2)(3)h(C×C(2))(5))h(J2)(T[3,6]T[4,6]h(C)(4)).

    The resulting Hodge numbers of the pure Hodge structure on the cohomology of M(3,d) are given by:

    (12100000000256520000001616221661000005224554412050000216541041269644122000641126222246177802020012096246390390239821200054417739050839416830000012802393943691843800002208216818410424000002123038246)

    For a curve C of genus g=3, the rational Chow motive of NC(3,d) and MC(3,d), for d coprime to 3, are given as follows.

    h(NC(3,d))h(J)(T0,16h(C)T1,2,13,14h(C(2))T2,4,10,12h(C2)T3,11h(C(3))T3,6,7,10h(C×C(2))T4,5,8,9h(C(4))T4,8h(C×C(3))T5,7h(C(2)×C(2))(6));
    h(MC(3,d))h(J)(T0,16h(C)T1,2,13,14,15h(C(2))T2,4,10,12,14h(C2)T3,11h(C(3))T3,6,7,10h(C×C(2))T4,5,8,9,13h(C(4))T4,8,12h(C×C(3))T5,7,12h(C(2)×C(2))(6)h(C(5))(11)h(C(2)×C(3))(11)h(C×C(5))(10)h(C(2)×C(4))(10)h(C(3)×C(4))(9))h(J2)(T[5,13]T[6,13]T[8,13]T[9,13]h(C)(T[6,11]T[7,11]T[9,11])h(C(2))(T[8,9]T[7,9])).

    The Hodge diamond of the pure Hodge structure of MC(3,d) for g=3 is already quite large and difficult to display properly. Since the motive h(MC(3,d)) is a multiple of the motive h(J) and the Hodge structure of H(J) is well-known, we give the Hodge diamond of "h(MC(3,d))/h(J)" (which coincides with the Hodge diamond of the moduli space of PGL3-Higgs bundles on a curve of genus 3):

    (1000000000000000001300000000000000033630000000000000061312121000000000000312343021100000000000001230637845213000000000012178122147994112000000000010451472422611958021300000000021992614474563301564260000000034119545673177753725172121000000012803307771151117379836210215100000002115653711731659158710204171021200000003422517981587206917769903244500000000672362102017762003140754993000000000121024179901407116753710200000000011510232454953727660000000000011245931026015)

    The formulas in Theorems 1.1 and 1.3 directly imply formulas for the Chow groups of NC(3,d), NC,L(3,d) and MC(3,d) via the representability of Chow groups in the categories of Chow and Voevodsky motives; see Eq (1.1). We make these formulas explicit in low (co)dimension. For simplicity, in order to exclude degenerate cases, we assume that g2.

    The following results for NC,L(3,d) are similar to those in [10,§4.3.1] in rank 2.

    Corollary 6.1.

    (i) CH1(NC,L(3,d))Z.

    (ii) CH2(NC,L(3,d))QQ2CH0(C)Q.

    (iii) CH3(NC,L(3,d))Q{Q2CH0(C)QPic(Jac(C))Qifg=2,Q3CH0(C)QPic(Jac(C))Qifg3.

    (iv) CH0(NC,L(3,d))QQ.

    (v) CH1(NC,L(3,d))QCH0(C)Q.

    (vi) CH2(NC,L(3,d))QQCH0(C)QCH0(C(2))Q.

    Proof. First of all, the variety NC,L(3,d) is a smooth projective Fano variety, hence its Picard group is torsion-free, which means that it suffices to prove (i) (and all the other statements) with rational coefficients.

    By inspecting the indices in the formula of Theorem 1.1, we see that we can write

    h(NC,L(3,d))=Q(0)h(C)(1)(h(C)h(C(2)))(2)(h(C2)(h(C2)h(C(3))ϵ(3)P(4)h(C(2))(8g12)h(C)(8g11)h(C)(8g10)Q(8g8)

    where ϵ=0 for g=2 and ϵ=1 otherwise, and P is a sum of direct factors of motives of smooth projective varieties of dimensions 8g15 (we have P=0 for g=2, and P can be read off the formula above for g=3). This ensures that the term P(4) does not contribute to the Chow groups in the ranges we are considering. All the formulas then follow from this together with the fact that

    Pic(Sym2(C))QQPic(Jac(C))Q.

    which is deduced from the decomposition h(C)=Q(0)h1(C)Q(1).

    For NC(3,d) and MC(3,d), the situation is complicated by the Jacobian factor h(Jac(C)). Here are some groups which are still reasonably simple to write down.

    Corollary 6.2.

    (i) CH1(NC(3,d))QCH1(MC(3,d))QPic(Jac(C))QQ.

    (ii) CH2(NC(3,d)QCH2(MC(3,d))QCH2(Jac(C))QPic(Jac(C)×C)QQ2.

    Proof. For these two Chow groups, the direct summands of h(MC(3,d)) other than h(NC(3,d)) in the decomposition of Theorem 1.3 do not contribute, so it remains to do the computation for NC(3,d), which follows from the formula in Theorem 1.1 in a straightforward way.

    L. F. is supported by the Radboud Excellence Initiative programme, and the Agence Nationale de la Recherche (ANR), under project numbers ANR-16-CE40-0011 and ANR-20-CE40-0023. S. P. L. is supported by The Netherlands Organisation for Scientific Research (NWO), under project number 613.001.752.

    The authors declare there is no conflict of interest.



    [1] S. del Baño, On the Chow motive of some moduli spaces, J. Reine Angew. Math., 532 (2001), 105–132. https://doi.org/10.1515/crll.2001.019 doi: 10.1515/crll.2001.019
    [2] E. Bifet, F. Ghione, M. Letizia, On the Abel-Jacobi map for divisors of higher rank on a curve, Math. Ann., 299 (1994), 641–672. https://doi.org/10.1007/BF01459804 doi: 10.1007/BF01459804
    [3] K. Behrend, A. Dhillon, On the motivic class of the stack of bundles, Adv. Math., 212 (2007), 617–644. https://doi.org/10.1016/j.aim.2006.11.003 doi: 10.1016/j.aim.2006.11.003
    [4] V. Hoskins, S. Pepin Lehalleur, A formula for the Voevodsky motive of the moduli stack of vector bundles on a curve, (2020), preprint, arXiv: 1809.02150.
    [5] O. García-Prada, J. Heinloth, A. Schmitt, On the motives of moduli of chains and Higgs bundles, J. Eur. Math. Soc., 16 (2014), 2617–2668. https://doi.org/10.4171/JEMS/494 doi: 10.4171/JEMS/494
    [6] N. J. Hitchin, The self-duality equations on a Riemann surface, Proc. London Math. Soc., 55 (1987), 59–126. https://doi.org/10.1112/plms/s3-55.1.59 doi: 10.1112/plms/s3-55.1.59
    [7] P. Gothen, The Betti numbers of the moduli space of stable rank 3 Higgs bundles on a Riemann surface, Internat. J. Math., 5 (1994), 861–875. https://doi.org/10.1142/S0129167X94000449 doi: 10.1142/S0129167X94000449
    [8] C. Simpson, The Hodge filtration on nonabelian cohomology, preprint, arXiv: alg-geom/9604005.
    [9] V. Hoskins, S. Pepin Lehalleur, On the Voevodsky motive of the moduli space of higgs bundles on a curve, Sel. Math., 27 (2021), 1–37. https://doi.org/10.1007/s00029-020-00610-5 doi: 10.1007/s00029-020-00610-5
    [10] L. Fu, V. Hoskins, S. Pepin Lehalleur, Motives of moduli spaces of bundles on curves via variation of stability and flips, preprint, arXiv: 2011.14872.
    [11] T. Gómez, K. S. Lee, Motivic decompositions of moduli spaces of vector bundles on curves, preprint, arXiv: 2007.06067.
    [12] S. I. Kimura, Chow groups are finite dimensional, in some sense, Math. Ann., 331 (2005), 173–201. https://doi.org/10.1007/s00208-004-0577-3 doi: 10.1007/s00208-004-0577-3
    [13] M. Thaddeus, Stable pairs, linear systems and the Verlinde formula, Invent. Math., 117 (1994), 317–353. https://doi.org/10.1007/BF01232244 doi: 10.1007/BF01232244
    [14] V. Voevodsky, Triangulated categories of motives over a field, Ann. Math. Stud., 143 (2000), 188–238.
    [15] U. Jannsen, Motives, numerical equivalence, and semi-simplicity, Invent. Math., 107 (1992), 447–452. https://doi.org/10.1007/BF01231898
    [16] Y. André, Motifs de dimension finie, Séminaire Bourbaki., 299 (2005), 115–145.
    [17] S. Bradlow, Special metrics and stability for holomorphic bundles with global sections, J. Differ. Geom., 33 (1991), 169–213. https://doi.org/10.4310/jdg/1214446034 doi: 10.4310/jdg/1214446034
    [18] Q. Jiang, On the Chow theory of projectivization, preprint, arXiv: 1910.06730.
    [19] K. Künnemann, A Lefschetz decomposition for Chow motives of abelian schemes, Invent. Math., 113 (1993), 85–102. https://doi.org/10.1007/BF01244303 doi: 10.1007/BF01244303
    [20] A. Białynicki-Birula, Some theorems on actions of algebraic groups, Ann. of Math., 98 (1973), 480–497. https://doi.org/10.24033/asens.2105 doi: 10.24033/asens.2105
    [21] A. Schmitt, Moduli for decorated tuples of sheaves and representation spaces for quivers, Proc. Indian Acad. Sci. Math. Sci., 115 (2005), 15–49. https://doi.org/10.1007/BF02829837 doi: 10.1007/BF02829837
    [22] L. Álvarez Cónsul, O. García-Prada, A. H. W. Schmitt, On the geometry of moduli spaces of holomorphic chains over compact Riemann surfaces, Int. Math. Res. Pap., 2006 (2006), 73597. https://doi.org/10.1155/IMRP/2006/73597 doi: 10.1155/IMRP/2006/73597
    [23] Y. André, Une introduction aux motifs (motifs purs, motifs mixtes, périodes), Société mathématique de France, (2004).
    [24] T. Hausel, M. Thaddeus, Mirror symmetry, Langlands duality, and the Hitchin system, Invent. Math., 153 (2003), 197–229. https://doi.org/10.1007/s00222-003-0286-7
    [25] M. Thaddeus, Geometric invariant theory and flips, J. Amer. Math. Soc., 9 (1996), 691–723. https://doi.org/10.1090/S0894-0347-96-00204-4 doi: 10.1090/S0894-0347-96-00204-4
    [26] P. Belmans, pbelmans/hodge-diamond-cutter: Initial release, Zenodo, v1.0 (2020). https://doi.org/10.5281/zenodo.3893510
  • This article has been cited by:

    1. Qingyuan Jiang, ON THE CHOW THEORY OF PROJECTIVIZATIONS, 2021, 1474-7480, 1, 10.1017/S1474748021000451
    2. Lie Fu, Victoria Hoskins, Simon Pepin Lehalleur, Motives of moduli spaces of bundles on curves via variation of stability and flips, 2023, 108, 0024-6107, 1, 10.1112/jlms.12739
    3. Sumit Roy, On motives of parabolic Higgs bundles and parabolic connections, 2024, 14, 1664-3607, 10.1142/S1664360724500012
    4. Kyoung-Seog Lee, Han-Bom Moon, Derived categories of symmetric products and moduli spaces of vector bundles on a curve, 2025, 197, 00217824, 103694, 10.1016/j.matpur.2025.103694
  • Reader Comments
  • © 2022 the Author(s), licensee AIMS Press. This is an open access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0)
通讯作者: 陈斌, bchen63@163.com
  • 1. 

    沈阳化工大学材料科学与工程学院 沈阳 110142

  1. 本站搜索
  2. 百度学术搜索
  3. 万方数据库搜索
  4. CNKI搜索

Metrics

Article views(2652) PDF downloads(219) Cited by(4)

Other Articles By Authors

/

DownLoad:  Full-Size Img  PowerPoint
Return
Return

Catalog