A generalization of the Clifford index and determinantal equations for curves and their secant varieties

Adam Ginensky

Introduction

When Brendan Hassett was a post doc at the University of Chicago I spoke to him a lot about a paper of Griffiths . which involved the concept of Shiffer variations. These are infinitesimal deformations of a curve, which have rank one when viewed (via cup product) as homomorphisms from H0(KC)⟶H1(OC)H^{0}(K_{C})\longrightarrow H^{1}(\mathcal{O}_{C}). They are in fact parametrized by points of the curve. Initially I was trying to understand on which curves CC, every rank jj infinitesimal deformations is just the sum of jj rank one Shiffer variations. Theorem 2.1 shows this holds only for j<Cliff⁡(C)j<\operatorname{Cliff}(C)

The arrangement of the thesis is as follows. In the first section we review the definition of the Clifford index and its relationship to the geometry of a curve CC. Shiffer variations are defined and then generalized to Shiffer variations supported on a divisor DD . We then prove a theorem (2.5 ) which explains how Shiffer variations are related to the Clifford index. The main result of this section is a geometric characterization of the Clifford index . Namely we show that in the bicanonical embedding, \mboxSecj(C)\mbox{Sec}^{j}(C) is in fact set theoretically the locus of all infinitesimal deformations or rank j+1j+1 if and only if j<c−1j<c-1. Recall that points in \mboxSecj(C)\mbox{Sec}^{j}(C) are the linear combinations of j+1j+1 points of CC and hence are the sum of j+1j+1 Shiffer variations. Since the sum of j+1j+1 rank one matrices is of rank at most j+1j+1 , \mboxSecj(C)\mbox{Sec}^{j}(C) consists of deformations of rank at most j+1j+1. Scheme theoretic equality which implies that \mboxSecj(C)\mbox{Sec}^{j}(C) is defined by equations of degree j+2j+2 for j<(Cliff⁡(C)−1)j<(\operatorname{Cliff}(C)-1) is true and is proven in section 6. This implies that \mboxSecj(C)\mbox{Sec}^{j}(C) is determinantally defined . The methods used are different and deferring the proof until later allows us to prove a more general result.

Up until this point the results have been on embeddings in L⊗2L^{\otimes 2} and it’s obvious factorization as L⊗LL\otimes L. In section 7 we take up the question of what happens when LL factors as L1⊗L2L_{1}\otimes L_{2}. All the machinery developed in sections 3 and 4 generalize and one can prove a theorem stating that for j<Cliff⁡(C,L1,L2)j<\operatorname{Cliff}(C,L_{1},L_{2}) the secant varieties are determinantally defined. Rarely is it the case that a divisor is ’special’ for both L1L_{1} and L2L_{2} and hence one gets improved bounds on the circumstances under which one can say that the secant varieties are determinantal. In particular for j=0j=0 that is to say for the case of the curve CC itself, one recovers the main result of in the case of smooth curves, which is if deg⁡(Li)≥2g+1\deg(L_{i})\geq 2g+1 and L1≠L2L_{1}\neq L_{2} if deg⁡(L1)=deg⁡(L2)=2g+1\deg(L_{1})=\deg(L_{2})=2g+1 then for L=L1⊗L2L=L_{1}\otimes L_{2}, CC is determinantally defined in LL.

In section 8 we discuss the results that occur when h1(L)=1h^{1}\left({L}\right)=1 . First as an application of the ideas of Clifford index we give another proof of the theorem of Green and Lazarsfeld giving a bound in terms of deg⁡(L)\deg(L) and Cliff⁡(C)\operatorname{Cliff}(C) as to when an imbedding by a very ample line bundle is quadratically normal. In essence, a very ample line bundle satisfying Cliff⁡(C,L)>0\operatorname{Cliff}(C,L)>0 is quadratically normal, and one can only realize a line bundle of clifford index zero as the projection from a linear space of dimension p−1p-1 of a line bundle of clifford index pp. A computation finishes the proof. We then take up the question of bounding when \mboxSecj(C)\mbox{Sec}^{j}(C) is determinantally defined. The same bounds hold as in the case h1(L)=0h^{1}\left({L}\right)=0 but it is much harder to prove, that for j>Cliff⁡(C,L)j>\operatorname{Cliff}(C,L) that the two varieties, the rank locus and the secant variety differ. Ironically this means that for special line bundles one is far more likely to have a stronger result than for line bundles with h1(L)=0h^{1}\left({L}\right)=0.

Finally in the last section , we consider the question of the relationship between these results and Green’s conjecture. The story here is incomplete, as one would like to be able to use these results to prove the conjecture. What we can say is that, the classes we produce in Theorem 2.5 for DD a base point free divisor, do give rise to non-trivial Koszul cohomology classes. This applies in particular to divisors which calculate the Clifford index of CC. Further these classes are ’decomposable’ (see section 9 for details) and that there are no such ’decomposable’ Koszual cohomology classes in Kp,2(C,KC)K_{p,2}(C,K_{C}) for c<Cliff⁡(C)c<\operatorname{Cliff}(C). This hardly settles the matter though.

I want to acknowledge the help I have received over the years from numerous people. Firstly, I want to express my deepest thanks to my thesis advisor, Prof. Spencer Bloch. Spencer was unstinting in his time and advice. Spencer’s remark, ‘You know I’m retiring soon, so if you want to write a thesis you should probably get it done now rather than later.’ provided the final encouragement to get things done. Spencer was a great friend and advisor. I also want to thank Professor Brendan Hassett who first brought my attention the question of the relationship between the Clifford index and determinantal embeddings. Brendan spent numerous hours discussing the problem with me and proofreading this thesis. My good friend Professor Mohan Kumar discussed this paper with me and read various version offering numerous helpful suggestions . In addition, over the years we have had so many conversations about so many mathematical topics, it is fair to say that I could/would never have kept my interest in mathematics alive without his help, advice, and information. Nicholas Passell and Mihnea Popa also read preliminary versions of the thesis offering numerous helpful suggestions.

I want to thank my wife Carol Lind for providing an environment that was very conducive to writing this thesis. I want to thank my children David Sidney Ginensky and Katherine Miriam Ginensky for being my children. I want to thank WH Trading for all their consideration in providing me with very flexible working hours while I was writing. I must also thank Mr. Tom Carrideo for his enthusiastic demonstrating of the ’wobbly H’. It helped to provide the inspiration to get this thesis done.

The Clifford Index

(Max Noether) Φ1\Phi_{1} is a projectively normal embedding unless CC is hyperelliptic.

We wish to rephrase these theorems in terms of the Clifford index of C. Recall that the Clifford index of CC, Cliff(CC) is defined as follows:

Let L be any line bundle. Cliff⁡(L)=deg⁡(L)−2(h0(C,L)−1)\operatorname{Cliff}(L)=\deg(L)-2(h^{0}\left({C,L}\right)-1)

The Clifford index of C written Cliff⁡(C)\operatorname{Cliff}(C) is min⁡{Cliff⁡(L)∣h0(L)\min\{\operatorname{Cliff}(L)|h^{0}\left({L}\right) and h1(L)≥2}\,h^{1}\left({L}\right)\geq 2\}

In this section we will give a geometric generalization of Thms A and B that characterizes the Clifford index.

To state our theorem we must recall some more notation. Recall that if ξ∈H1(C,TC)\xi\in H^{1}(C,T_{C}) then via cup product we get a map ξ:H0(C,KC)⟶H1(C,OC)\xi:H^{0}(C,K_{C})\longrightarrow H^{1}(C,\mathcal{O}_{C}) called the Kodaira-Spencer map. This induces a map

Let C be a smooth curve then, Sec⁡j−1(C)=Rj(C)\operatorname{Sec}^{j-1}(C)=R^{j}(C) for j<\mboxCliff(C)j<\mbox{Cliff}(C) and \mboxSecj(C)⊊Rj(C)\mbox{Sec}^{j}(C)\subsetneq R^{j}(C) for j≥\mboxCliff(C)j\geq\mbox{Cliff}(C).

This result is than weaker, but connected to, Green’s conjecture. We will discuss the exact relationship in the last section of this thesis. Notice in the case Cliff⁡(C)=0\operatorname{Cliff}(C)=0 our theorem merely states that Cliff⁡(C)>0⇔Ho(KC)⊗H0(KC)⟹H0(KC⊗2)\operatorname{Cliff}(C)>0\Leftrightarrow H^{o}(K_{C})\otimes H^{0}(K_{C})\Longrightarrow H^{0}(K_{C}^{\otimes 2}) is surjective and in the case \mboxCliff(C)=1\mbox{Cliff}(C)=1 we get only set theoretic and not scheme theoretic results. The theorem only asserts a set theoretic equality. Scheme theoretic equality is true, but will be discussed later as it involves some different ideas.

Recall that H0(TC(p))=0 ∀p∈CH^{0}(T_{C}(p))=0\ \forall p\in C when g≥2g\geq 2. Hence in the long exact sequence of cohomology associated to

0⟶TC⟶TC(p)⟶TC(p)∣p⟶00\longrightarrow T_{C}\longrightarrow T_{C}(p)\longrightarrow T_{C}(p)_{|p}\longrightarrow 0

We will need this same notion regarding classes in H1(OC)H^{1}(\mathcal{O}_{C}) so we note the following:

0⟶OC⟶OC(p)⟶OC(p)∣p⟶00\longrightarrow\mathcal{O}_{C}\longrightarrow\mathcal{O}_{C}(p)\longrightarrow\mathcal{O}_{C}(p)_{|p}\longrightarrow 0.

We wish to generalize the preceding definitions to reduced divisors. Let D=∑i=1dpiD=\sum_{i=1}^{d}p_{i} with the pip_{i} distinct.

⟨σi⟩⊂H1(OC)\langle\sigma_{i}\rangle\subset H^{1}(\mathcal{O}_{C}) is the vector space spanned by the σpi=σi\sigma_{p_{i}}=\sigma_{i} i.e. pick local parameters ziz_{i} around pip_{i} and let σi=∂(1zi)∈H0(OC(p)∣p)\sigma_{i}=\partial\left(\frac{1}{z_{i}}\right)\in H^{0}(\mathcal{O}_{C}(p)_{|p}), then ⟨σi⟩={∑i=1daiσi ∣ ai∈k}\langle\sigma_{i}\rangle=\left\{\sum_{i=1}^{d}a_{i}\sigma_{i}\,|\,a_{i}\in k\right\}.

Similarly let τi=∂(1zi∂∂zi)∈H0(TC(p)∣p)\tau_{i}=\partial\left(\frac{1}{z_{i}}\frac{\partial}{\partial z_{i}}\right)\in H^{0}(T_{C}(p)_{|p}) then

T(D)={∑i=1daiτi ∣ ai∈k}T(D)=\left\{\sum_{i=1}^{d}a_{i}\tau_{i}\,|\,a_{i}\in k\right\}. T(D)T(D) is the set of Shiffer variations supported on DD.

Unless the degree of DD is large, and in particular if deg⁡(D)≤2g−3\deg(D)\leq 2g-3, then H0(TC(D))H^{0}(T_{C}(D)) =0=0. Hence in this case, dim⁡T(D)=deg⁡D\dim T(D)=\deg D.

Recall that any ξ∈H1(TC)\xi\in H^{1}(T_{C}) induces ξ:H0(KC)⟶H1(OC)\xi:H^{0}(K_{C})\longrightarrow H^{1}(\mathcal{O}_{C}). In terms of Shiffer variations we can describe the action of T(D)T(D) as follows:

Pick local coordinates ziz_{i} around pip_{i} and let τi=1zi∂∂zi∈H1(TC)\tau_{i}=\frac{1}{z_{i}}\frac{\partial}{\partial z_{i}}\in H^{1}(T_{C}), σi=1zi∈H1(OC)\sigma_{i}=\frac{1}{z_{i}}\in H^{1}(\mathcal{O}_{C}). Suppose ω∈H0(KC)\omega\in H^{0}(K_{C}) has a local representation f(zi)dzif(z_{i})dz_{i} with f(0)=aif(0)=a_{i}. Then, for τ=∑i=1dτi\tau=\sum_{i=1}^{d}\tau_{i}

Both σi\sigma_{i} and τi\tau_{i} are defined in terms of boundaries (Say σi=∂(σi~) and τi=∂(τi~)\sigma_{i}=\partial(\widetilde{\sigma_{i}})\ and\ \tau_{i}=\partial(\widetilde{\tau_{i}})) ∂:H0(OD(D))⟶H1(OC) and ∂:H0(TC(D)∣D)⟶H1(TC)\partial:H^{0}(\mathcal{O}_{D}(D))\longrightarrow H^{1}(\mathcal{O}_{C})\ and\ \partial:H^{0}(T_{C}(D)_{|D})\longrightarrow H^{1}(T_{C}). As such it is clear we have a commutative diagram for any ω∈H0(KC)\omega\in H^{0}(K_{C})

But τi∪ω=1zi∂∂zi∪f(zi)dzi=f(zi)zi=aizi+\tau_{i}\cup\omega=\frac{1}{z_{i}}\frac{\partial}{\partial z_{i}}\cup f(z_{i})dz_{i}=\frac{f(z_{i})}{z_{i}}=\frac{a_{i}}{z_{i}}+ holomorphic fnc. f(zi)/zi=aizif(z_{i})/z_{i}=\frac{a_{i}}{z_{i}} in H0(Opi(pi))H^{0}(\mathcal{O}_{p_{i}}(p_{i})) so denoting by τi~=1zi∂∂z∈H0(TC(pi)∣pi)\widetilde{\tau_{i}}=\frac{1}{z_{i}}\frac{\partial}{\partial z}\in H^{0}(T_{C}(p_{i})_{|p_{i}}) τi(ω)=∂(τi~∨ω)=∂(aizi)=aiσi\tau_{i}(\omega)=\partial(\widetilde{\tau_{i}}\vee\omega)=\partial\left(\frac{a_{i}}{z_{i}}\right)=a_{i}\sigma_{i}. Since TC(D)∣D and OD(D)T_{C}(D)_{|D}\ and\ \mathcal{O}_{D}(D) are skyscraper sheaves it follows that τ(ω)=∑i=1dσi(ω)=∑i=1daiσi\tau(\omega)=\sum_{i=1}^{d}\sigma_{i}(\omega)=\sum_{i=1}^{d}a_{i}\sigma_{i} as claimed. ∎

ker (τi)=H0(KC(−pi))(\tau_{i})=H^{0}(K_{C}(-p_{i})) and for τ∈T(D)\tau\in T(D) ker(τ)⊃H0(KC(−D))(\tau)\supset H^{0}(K_{C}(-D)).

τi(ω)=aiσi\tau_{i}(\omega)=a_{i}\sigma_{i} where ω=f(zi)dzi and f(0)=ai\omega=f(z_{i})dz_{i}\ and\ f(0)=a_{i}. Hence τi(ω)=0⇔ai=0⇔ω∈H0(KC(−pi))\tau_{i}(\omega)=0\Leftrightarrow a_{i}=0\Leftrightarrow\omega\in H^{0}(K_{C}(-p_{i})). If τ=∑biτi\tau=\sum b_{i}\tau_{i} then

The rank of ξ∈H1(TC)\xi\in H^{1}(T_{C}) is the rank of ξ:H0(KC)⟶H1(OC)\xi:H^{0}(K_{C})\longrightarrow H^{1}(\mathcal{O}_{C}). Rk(C)={ξ∈H1(TC) ∣ \mboxrank(ξ)≤k}R^{k}(C)=\{\xi\in H^{1}(T_{C})\,|\,\mbox{rank}(\xi)\leq k\}.

Suppose E=kpE=kp is a divisor. Then we define generalized Shiffer variations as follows: let τpj=∂(τ~pj) 1≤j≤k\tau_{p}^{j}=\partial(\widetilde{\tau}_{p}^{j})\ 1\leq j\leq k : where τp~j=1zj∂∂z∈H0(TC(kp)∣kp){\widetilde{\tau_{p}}}^{j}=\frac{1}{z^{j}}\frac{\partial}{\partial z}\in H^{0}(T_{C}(kp)_{|kp}). If D=∑i=1d′kipiD=\sum_{i=1}^{d^{\prime}}k_{i}p_{i} then

From the definition it follows that T(D)T(D) is the linear space spanned by the divisor D. Thus the following is clear.

The purpose of this thesis is to show that the relationship between Sec⁡j−1(C)\operatorname{Sec}^{j-1}(C) and  Rj(C)\ R^{j}(C) is controlled by the Clifford index. This will follow from an analysis of Shiffer variations and classes. To that end we need to understand for any τ∈T(D)\tau\in T(D) what the possible kernels and images can be. Since \mboxker(τ)⊃H0(KC(−D))\mbox{ker}(\tau)\supset H^{0}(K_{C}(-D)) in any event set WD=W=H0(KC)/H0(KC(−D))W_{D}=W=H^{0}(K_{C})/H^{0}(K_{C}(-D)) and S=⟨σi⟩pi∈DS={\langle\sigma_{i}\rangle}_{p_{i}\in D} so τ:W⟶S\tau:W\longrightarrow S. Note dim⁡(W)=g−(g−d+r)=d−r\dim(W)=g-(g-d+r)=d-r since DD defines a gdrg^{r}_{d}. We calculate dim⁡(S)\dim(S):

∑aiσi=0⇔∃f∈H0(OC(D))\sum a_{i}\sigma_{i}=0\Leftrightarrow\exists f\in H^{0}(\mathcal{O}_{C}(D)) s.t. in the same local coordinates ziz_{i} used to define σi\sigma_{i} one has f(zi)=ai/zif(z_{i})=a_{i}/z_{i} + holomorphic function.

since ∂(H0(OD(D)))=⟨σi⟩\partial(H^{0}(\mathcal{O}_{D}(D)))=\langle\sigma_{i}\rangle so i) follows from h0(OD(D))=dh^{0}(\mathcal{O}_{D}(D))=d anddim⁡(\mboxIm(ρ))=r\dim(\mbox{Im}(\rho))=r (DD is a gdrg_{d}^{r}). ii) This is just an explication of i). Choosing local coordinates ziz_{i} around pip_{i} and identifying H0(Opi(pi))H^{0}(\mathcal{O}_{p_{i}}(p_{i})) with 1zi\frac{1}{z_{i}}. Then if f=aizif=\frac{a_{i}}{z_{i}} + holomorphic function near pip_{i} then ρ(f)=⨁i∈Daizi\rho(f)=\bigoplus_{i\in D}\frac{a_{i}}{z_{i}} so ∂(ρ(f))=0= ∑aiσi\partial(\rho(f))=0=\,\sum a_{i}\sigma_{i}. ∎

Remark: If for D=∑i=1d′kipiD=\sum_{i=1}^{d^{\prime}}k_{i}p_{i} with ∑ki=d\sum k_{i}=d and we define σ~ij  1≤j≤ki\widetilde{\sigma}_{i}^{j}\ \ 1\leq j\leq k_{i} to be the class of 1zij∈Okip(kip)  σij=∂(σ~ij)\frac{1}{z_{i}^{j}}\in\mathcal{O}_{k_{i}p}(k_{i}p)\ \ \sigma_{i}^{j}=\partial(\widetilde{\sigma}^{j}_{i}) then the lemma extends in a straight forward manner to non-reduced divisors.

The main theorem of this section is Thereom 2.1 which characterizes the rank filtration in terms of the Clifford index. I recall the statement.

\mboxSecj(C)=Rj(C)\mbox{Sec}^{j}(C)=R^{j}(C) for j<\mboxCliff(C)j<\mbox{Cliff}(C)

\mboxSecj(C)⊊Rj(C)\mbox{Sec}^{j}(C)\subsetneq R^{j}(C) for j≥\mboxCliff(C)j\geq\mbox{Cliff}(C).

This theorem is a geometric characterization of the Clifford index. Griffiths has commented upon the importance of understanding the rank filtration in terms of doing Hodge theory, but perhaps there is more to be said algebraically.

The main tool used is a theorem that characterizes the possible ranks of a generalized Shiffer variation supported on DD in terms of data about DD, in particular the Clifford index d−2rd-2r of DD. A calculation of the dimension of \mboxSecj(C)\mbox{Sec}^{j}(C) which allows one to bound the number of Shiffer variations needed to express any element of H1(TC)H^{1}(T_{C}) finishes the proof. The relationship between the rank filtration and the Clifford index is governed by:

Let τ=∑pi∈Daiτi ∈ T(D) ai≠0\tau=\sum_{p_{i}\in D}a_{i}\tau_{i}\,\in\,T(D)\ a_{i}\neq 0 be a generalized Shiffer variation. Then:

The upper bound is always achieved and the lower bound is achieved if D and\linebreak KC(−D)D\ and\linebreak\ K_{C}(-D) are base point free.

Remarks: Notice that if DD computes the Clifford index of CC then DD satisfies ii). Also note the choice of local coordinates ziz_{i} is irrelevant as different choices of ziz_{i} just scale σi\sigma_{i} and τi\tau_{i} differently.

Since τ:W⟶S\tau:W\longrightarrow S, rk⁡(τ)≤dim⁡(S)=d−r\operatorname{rk}(\tau)\leq\dim(S)=d-r. Let p1,…,pd−r∈Dp_{1},\ldots,p_{d-r}\in D be such that h0(OC(p1,…,pd−r))=1h^{0}(\mathcal{O}_{C}(p_{1},\ldots,p_{d-r}))=1. That is to say that the points p1,…,pd−rp_{1},\ldots,p_{d-r} are linearly independent. One can check easily by induction that such points exist. If we take τ=∑i=1d−rτi\tau=\sum_{i=1}^{d-r}\tau_{i} then \mboxrank τ=d−r\mbox{rank}\,\tau=d-r because if ω∈H0(KC) \omega\in H^{0}\left({K_{C}}\right)\, then τ(ω)=∑i=1d−rbiσi\tau(\omega)=\sum_{i=1}^{d-r}b_{i}\sigma_{i} where bi∈kb_{i}\in k is the value of ω\omega at ziz_{i}, that is to say that locally ω=fi(zi)dzi\omega=f_{i}(z_{i})dz_{i} where fi(0)=bif_{i}(0)=b_{i}. Thus τ(ω)=0\tau(\omega)=0 if and only if bi=0b_{i}=0 for all ii, since the σi\sigma_{i} were constructed to be linearly independent. Hence τ=∑i=1d−rτi\tau=\sum_{i=1}^{d-r}\tau_{i} achieves the upper bound.

Next we show the lower bound d−2r≤\mboxrank(τ)d-2r\leq\mbox{rank}(\tau). Recall that the action of a Shiffer variation τ\tau on one forms can be calculated by considering the action of τ~∈H0(TC(D)∣D)\widetilde{\tau}\in H^{0}(T_{C}(D)_{|D}) representing τ\tau. In fact we have the following commutative diagram.

Here rr is the restriction map and τ~\widetilde{\tau} is such that ∂(τ~)=τ\partial(\widetilde{\tau})=\tau. The key point is if D=∑i=1jkipiD=\sum_{i=1}^{j}k_{i}p_{i} and τ~=∑i=1j∑l=1kibilτil\widetilde{\tau}=\sum_{i=1}^{j}\sum_{l=1}^{k_{i}}b_{il}\tau_{i}^{l} then τ~\widetilde{\tau} is an isomorphism if and only if biki≠0 ∀ib_{ik_{i}}\neq 0\ \forall i ; i.e. the highest pole order terms are nonzero. This means that all coefficients are non-zero if DD is reduced. To see this its clearly enough to check at any point pip_{i} that the map H0(KC∣kip)⟶τ~iH0(Okip(kip))H^{0}({K_{C}}_{|k_{i}p})\stackrel{{\scriptstyle\widetilde{\tau}_{i}}}{{\longrightarrow}}H^{0}(\mathcal{O}_{k_{i}p}(k_{i}p)) is an isomorphism ⇔biki≠0\Leftrightarrow b_{ik_{i}}\neq 0. Working in local coordinates since zijτik=τik−jz_{i}^{j}\tau_{i}^{k}=\tau_{i}^{k-j} one sees that \mboxrank τij=j and \mboxIm τij=zi\mboxIm(τij+1)\mbox{rank}\,\tau_{i}^{j}=j\ and\ \mbox{Im}\,\tau_{i}^{j}=z_{i}\mbox{Im}(\tau_{i}^{j+1}) so ∑j=1kibijτij\sum_{j=1}^{k_{i}}b_{ij}\tau_{i}^{j} has \mboxrank m⇔bim≠0\mbox{rank}\,m\Leftrightarrow b_{i_{m}}\neq 0 and bij=0 j>mb_{i_{j}}=0\ j>m and hence \mboxrank τi~=ki⇔biki≠0\mbox{rank}\,\widetilde{\tau_{i}}=k_{i}\Leftrightarrow b_{ik_{i}}\neq 0.

Now returning to our diagram, the map τ~\widetilde{\tau} is an isomorphism, and rr is injective, so \mboxker(τ)=\mboxker(∂∘τ~∘r)=\mboxker(∂∣Im(τ~∘r))\mbox{ker}(\tau)=\mbox{ker}(\partial\circ\widetilde{\tau}\circ r)=\mbox{ker}(\partial_{|\rm{\scriptstyle{Im}}(\widetilde{\tau}\circ r)}). Since dim⁡(\mboxker ∂)=r≥dim⁡(\mboxker(∂∣Im(τ~∘r)))\dim(\mbox{ker}\,\partial)=r\geq\dim(\mbox{ker}(\partial_{|\rm{\scriptstyle{Im}}(\widetilde{\tau}\circ r)})) so dim⁡ \mboxker(τ)≤r\dim\,\mbox{ker}(\tau)\leq r and hence \mboxrank τ=dim⁡(W)−dim⁡(\mboxker(τ))≥(d−r)−r=d−2r\mbox{rank}\,\tau=\dim(W)-\dim(\mbox{ker}(\tau))\geq(d-r)-r=d-2r.

To finish we must show that if KC(−D)K_{C}(-D) is base point free there exists a τ\tau with \mboxrank(τ)=d−2r\mbox{rank}(\tau)=d-2r. Because DD moves and is base point free, (h0(O(D))=1h^{0}(\mathcal{O}(D))=1 is the case r=0r=0) we may find D′D^{\prime} linearly equivalent to DD and reduced, D′=∑i=1dpiD^{\prime}=\sum_{i=1}^{d}p_{i} where pi≠pjp_{i}\neq p_{j} for i≠ji\neq j. We may set D=D′D=D^{\prime} since we are only interested in existence. Now since KC(−D)K_{C}(-D) is base point free there exists ω∈Ho(KC(−D))\omega\in H^{o}(K_{C}(-D)) such that ω\omega has simple zeroes at pip_{i} for all ii. Pick local coordinates s.t. ziz_{i} on Ui∋pi′U_{i}\ni p_{i}^{\prime} with ω(zi)=zidzi\omega(z_{i})=z_{i}dz_{i} and set σi=∂(1zi)∈H1(OC)\sigma_{i}=\partial\left(\frac{1}{z_{i}}\right)\in H^{1}(\mathcal{O}_{C}) and τi=∂(1zi∂∂zi)∈H1(TC)\tau_{i}=\partial\left(\frac{1}{z_{i}}\frac{\partial}{\partial z_{i}}\right)\in H^{1}(T_{C}). Let f1…frf_{1}\ldots f_{r} be a basis for H0(OC(D))/H0(OC)H^{0}(\mathcal{O}_{C}(D))/H^{0}(\mathcal{O}_{C}). From our choices we have fiω=ηi∈H0(KC) and τi(ηj)=ai(j)f_{i}\omega=\eta_{i}\in H^{0}(K_{C})\ and\ \tau_{i}(\eta_{j})=a_{i}^{(j)} where fj∣Ui=ai(j)/zif_{j|U_{i}}=a_{i}^{(j)}/z_{i}+hol. function. Note that ηi\eta_{i} are linearly independent elements of H0(KC)H^{0}(K_{C}) because if ∑j=1rRjηj=0\sum_{j=1}^{r}R_{j}\eta_{j}=0 for Rj∈kR_{j}\in k then (∑j=1rRjfj)ω=0\left(\sum_{j=1}^{r}R_{j}f_{j}\right)\omega=0. But ω\omega is a holomorphic one form so this can only happen if ∑j=1nRjfj=0\sum_{j=1}^{n}R_{j}f_{j}=0 which contradicts the linear independence of fjf_{j}. Now let τ=∑i=1dτi\tau=\sum_{i=1}^{d}\tau_{i}. τ(ηj)=∑i=1dτi(ηj)=∑i=1dai(j)σi=0\tau(\eta_{j})=\sum_{i=1}^{d}\tau_{i}(\eta_{j})=\sum_{i=1}^{d}a_{i}^{(j)}\sigma_{i}=0 (because τi(ηj)=ai(j)\tau_{i}(\eta_{j})=a_{i}^{(j)} by Lemma 2.2). Hence we have exhibited rr linearly independent elements of \mboxker τ\mbox{ker}\,\tau i.e. \mboxrank(τ)≤d−2r\mbox{rank}(\tau)\leq d-2r hence \mboxrank(τ)=d−2r.\mbox{rank}(\tau)=d-2r. ∎

Remark: The construction of the second part is related to classical ideas about constructing quadrics containing the canonical curve. In fact general ω∈H0(KC(−D))\omega\in H^{0}(K_{C}(-D)) have simple zeroes on DD and if ω′ and ηi′{\omega}^{\prime}\ and\ \eta_{i}^{\prime} are another such choice then ηiω′−ηi′ω∈H0(KC)⊗2\eta_{i}{\omega}^{\prime}-\eta_{i}^{\prime}\omega\in H^{0}(K_{C})^{\otimes 2} is a quadric containing CC i.e. ηiω′=fiω⋅ω′=fiω′⋅ω=ηi′ω\eta_{i}{\omega}^{\prime}=f_{i}\omega\cdot{\omega}^{\prime}=f_{i}{\omega}^{\prime}\cdot\omega=\eta_{i}^{\prime}\omega so ηiω′−ηi′ω∈\mboxker(H1(KC)⊗2⟶H0(KC⊗2))\eta_{i}{\omega}^{\prime}-\eta_{i}^{\prime}\omega\in\mbox{ker}(H^{1}(K_{C})^{\otimes 2}\longrightarrow H^{0}(K_{C}^{\otimes 2})).

dim⁡(\mboxSecj(C))=min⁡(2j+1,3g−4)\dim(\mbox{Sec}^{j}(C))=\min(2j+1,3g-4)

To show π2\pi_{2} is quasifinite it is enough to show: (∗) ∃U⊂\mboxSymj(C)(\ast)\ \exists U\subset\mbox{Sym}^{j}(C) open and non-trivial s.t. for D∈U ∃D\in U\ \exists an open subset VD⊂\mboxSymj(C)V_{D}\subset\mbox{Sym}^{j}(C) such that D∈VDD\in V_{D} and ∀E∈VD  H0(TC(D+E))=0.\forall E\in V_{D}\ \ H^{0}(T_{C}(D+E))=0.

Statement (∗)(\ast) may be translated as saying for general D∈\mboxSymj(C)D\in\mbox{Sym}^{j}(C) and any nearby E⊂\mboxSymj(C)⟨D⟩∩⟨E⟩=∅E\subset\mbox{Sym}^{j}(C)\langle D\rangle\cap\langle E\rangle=\emptyset. But by (∗)(\ast) if D1D_{1} and D2∈UD_{2}\in U are distinct divisors then for pi∈πi−1(Di)p_{i}\in\pi_{i}^{-1}(D_{i}) for i=1,2i=1,2 then π2(p1)≠π2(p2)\pi_{2}(p_{1})\neq\pi_{2}(p_{2}). Hence π2\pi_{2} is quasifinite on the open set π1−1(U)\pi_{1}^{-1}(U). However (∗)(\ast) is clear. Since j≤3g−52j\leq\frac{3g-5}{2}, deg⁡(TC(E+D))≤g−3\deg(T_{C}(E+D))\leq g-3 for D,E∈Sym⁡j(C)D,E\in\operatorname{Sym}^{j}(C) and the general divisor of degree g−3g-3 is not effective. By semi-continuity for general D,ED,E h0(OC(D+E))=0h^{0}\left({\mathcal{O}_{C}(D+E)}\right)=0 once it is true for one special D,ED,E. ∎

Finally we will show how Theorem 2.6 implies Theorem 2.1.

Geometric Riemann-Roch and the Definition of the Clifford Index of a General Line Bundle

In the previous section we have proved that the Clifford index of a curve can be characterized in terms of the geometry of the curve, specifically the geometry of the bicanonical embedding. The purpose of this section is to generalize these ideas to a much wider class of line bundles. The Clifford index can be given a more geometric interpetation which allows one to make sense of the notion of a Clifford index for any very ample line bundle. In fact the definition makes sense for any line bundle, but it doesn’t seem to be useful unless the line bundle is very ample.

The main result we are aiming to prove is one that compares secant varieties of curves to certain rank loci for non special line bundles of large degree. While secant varieties have nice geometric properties, rank loci have the important property that their equations are (by definition!) determinants of a given degree. For example to say that a curve in some given embedding is a rank one locus is to say that the curve is defined by the vanishing of two by two minors of some matrix. This brings to the forefront the issue of whether the two scheme structures defined by the secant structure and the rank loci structure coincide. We show that this is true in a large range of circumstances. Finally we relate this to earlier work of Eisenbud, Koh, and Stillman on determinantal presentations of curves and their secant varieites.

The key idea is as follows. First use Geometric Riemann-Roch to define a general Clifford index. For a very ample line bundle L interpet L⊗2L^{\otimes 2} as giving an embedding of C in a space of matrices. Finally use the Clifford Index to bound from below the rank of a matrix. This allows one to say that up to a given integer dd, \mboxSecd(C)\mbox{Sec}^{d}(C) is set-theoretically a determinantal locus. Scheme theoretic equality then comes from a different argument.

Denote by D‾\overline{D} the span of DD in PP. If DD has no multiple points this is clear. In general if V⊂H0(C,L)V\subset H^{0}\left({C,L}\right) is of codimension mm the H0(C,L)⟶H0(C,L)/VH^{0}\left({C,L}\right)\longrightarrow H^{0}\left({C,L}\right)/V determines a m−1m-1 dimensional subspace. D‾\overline{D} is the space corresponding to V=H0(L(−D))V=H^{0}\left({L(-D)}\right).

If s∈H0(OC(D))s\in H^{0}\left({\mathcal{O}_{C}(D)}\right) is a section which vanishes on DD (i.e. "1"∈H0(OC)↪H0(OC(D))"1"\in H^{0}\left({\mathcal{O}_{C}}\right)\hookrightarrow H^{0}\left({\mathcal{O}_{C}(D)}\right)) then under the natural multiplication map OC(D)⊗L(−D)⟶L\mathcal{O}_{C}(D)\otimes L(-D)\longrightarrow L we can identify I(D‾)={ξ∈H0(L) ∣ ξ∣D‾=0}I(\overline{D})=\left\{{\xi\in H^{0}\left({L}\right)\,|\,\xi|_{\overline{D}}=0}\right\} with s⊗H0(L(−D))s\otimes H^{0}\left({L(-D)}\right).

This is the definition since h0(L(−D))=h0(L)−d+rh^{0}\left({L(-D)}\right)=h^{0}\left({L}\right)-d+r means that codimension of H0(L(−D))H^{0}\left({L(-D)}\right) in H0(L)H^{0}\left({L}\right) is d−rd-r.

Tensoring this with L(−D)L(-D) and taking global sections give us (ii).

Thus we may rephrase the definition of the Clifford index as

Cliff⁡(L,C)=min⁡{Cliff⁡(L,D) ∣ rL(D)>0 and the span of Dis of codimension two or greater}\operatorname{Cliff}(L,C)=\min\{\operatorname{Cliff}(L,D)\,|\,r_{L}(D)>0\text{ and the span of }D\\ \text{is of codimension two or greater}\}

Remark It is a standard notation that Cliff⁡(D)=Cliff⁡(KC,D)\operatorname{Cliff}(D)=\operatorname{Cliff}(K_{C},D). This definition is specific for curves. As far as I can tell, the important point is that DD consists of points not divisors. We now record the basic properties of rL(D)r_{L}(D) and Cliff⁡(L,D)\operatorname{Cliff}(L,D).

rL(D)=codim⁡(im⁡(H0(L)⟶H0(L,D)))r_{L}(D)=\operatorname{codim}\left(\operatorname{im}\left(H^{0}\left({L}\right)\longrightarrow H^{0}\left({L,D}\right)\right)\right).

rL(D)=h0(KC⊗L−1(D))−h0(KC⊗L−1)r_{L}(D)=h^{0}\left({K_{C}\otimes L^{-1}(D)}\right)-h^{0}\left({K_{C}\otimes L^{-1}}\right).

Cliff⁡(L,D)=Cliff⁡(L(−D))−Cliff⁡(L)\operatorname{Cliff}(L,D)=\operatorname{Cliff}(L(-D))-\operatorname{Cliff}(L).

Cliff⁡(L,D)=Cliff⁡(L,L⊗2⊗KC−1(−D))\operatorname{Cliff}(L,D)=\operatorname{Cliff}(L,L^{\otimes 2}\otimes K_{C}^{-1}(-D)).

rL(D)r_{L}(D) is defined by h0(L(−D))=h0(L)−d+rL(D)h^{0}\left({L(-D)}\right)=h^{0}\left({L}\right)-d+r_{L}(D). Using

(since H1(L∣D)=0H^{1}\left({L|_{D}}\right)=0) and h0(L∣D)=dh^{0}\left({L|_{D}}\right)=d, we see that dim⁡(im⁡(H0(L)⟶H0(L∣D)))\linebreak=d−rL(D)\dim\left(\operatorname{im}\left(H^{0}\left({L}\right)\longrightarrow H^{0}\left({L|_{D}}\right)\right)\right)\linebreak=d-r_{L}(D) which is (i).

From (i) we get rL(D)=h1(L(−D))−h1(L)r_{L}(D)=h^{1}\left({L(-D)}\right)-h^{1}\left({L}\right). Applying Serre duality the result follows.

Cliff⁡(L,D)=d−2rL(D)=(d−rL(D))−rL(D)\operatorname{Cliff}(L,D)=d-2r_{L}(D)=\left(d-r_{L}(D)\right)-r_{L}(D), which by (i) and (ii) =(h0(L)−h0(L(−D)))−(h1(L(−D))−h0(L))=(h0(L)+h1(L))−\linebreak(h0(L(−D))+h1(L(−D)))=\left(h^{0}\left({L}\right)-h^{0}\left({L(-D)}\right))-(h^{1}\left({L(-D)}\right)-h^{0}\left({L}\right)\right)=\left(h^{0}\left({L}\right)+h^{1}\left({L}\right)\right)-\linebreak\left(h^{0}\left({L(-D)}\right)+h^{1}\left({L(-D)}\right)\right). (iii) now follows from the well known

h0(L)+h1(L)=g+1−Cliff⁡(L)h^{0}\left({L}\right)+h^{1}\left({L}\right)=g+1-\operatorname{Cliff}(L).

By (iii), Cliff⁡(L,D)=Cliff⁡(L(−D))−Cliff⁡(L)=Cliff⁡(Kc⊗L−1(D))−Cliff⁡(L)\operatorname{Cliff}(L,D)=\operatorname{Cliff}(L(-D))-\operatorname{Cliff}(L)=\operatorname{Cliff}(K_{c}\otimes L^{-1}(D))-\operatorname{Cliff}(L), since Cliff⁡(L)=Cliff⁡(KC⊗L−1)\operatorname{Cliff}(L)=\operatorname{Cliff}(K_{C}\otimes L^{-1}). Now KC⊗L−1(D)=L⊗(L⊗2⊗KC(−D))−1K_{C}\otimes L^{-1}(D)=L\otimes\left(L^{\otimes 2}\otimes K_{C}(-D)\right)^{-1} and the result follows.

We first consider the case when deg⁡(L)=2g−2\deg(L)=2g-2. Depending on how “far away” LL is from KCK_{C}, its behavior becomes more “very ample”. “Far away” means more general in a sense to be explained below. I am sure that most, if not all, of this material is well known to the experts. I could not find references to these specific statements, so I am including the proofs.

Suppose deg(L)deg(L) = 2g−22g-2 and L≠KCL\neq K_{C}

LL is base-point free unless L=KC(p−q)L=K_{C}(p-q), p,q∈Cp,q\in C. KC(p−q)K_{C}(p-q) has a unique base point unless CC is hyperelliptic.

Suppose LL is base-point free, then LL is very ample unless L=KC(D−E)L=K_{C}(D-E), D,E∈Sym⁡2(C)D,E\in\operatorname{Sym}^{2}(C).

Suppose LL is very ample, then CC is not defined by quadrics if L=KC(D1−D2)L=K_{C}(D_{1}-D_{2}), where deg⁡(Di)=3\deg(D_{i})=3 and DiD_{i} is general. That is, LL has a 3-secant line.

Suppose p∈Cp\in C is a base point. Then H0(C,L)=H0(C,L(−p))H^{0}\left({C,L}\right)=H^{0}\left({C,L(-p)}\right) and hence h1(L(−p))=1h^{1}\left({L(-p)}\right)=1. As mentioned above, this means L(−p)=KC(−E)L(-p)=K_{C}(-E) (with EE effective). It follows that deg⁡(E)=1\deg(E)=1, so L(−p)=KC(−q)L(-p)=K_{C}(-q) and L=KC(p−q)L=K_{C}(p-q).

For any p,q∈Cp,q\in C, KC(p−q)K_{C}(p-q) has a base point at pp. Furthermore, if p1≠pp_{1}\neq p is another base point, then KC(p−q−p1)=KC(−q1)K_{C}(p-q-p_{1})=K_{C}(-q_{1}), so OC≅OC(p−q+q1−p1)\mathcal{O}_{C}\cong\mathcal{O}_{C}(p-q+q_{1}-p_{1}) for some choice of p1∈Cp_{1}\in C which means that there exists a function on CC with two poles, i.e. CC is hyperellipic.

If LL is not very ample, there is a divisor DD of degree 2, such that h0(L(−D))>h0(L)−2h^{0}\left({L(-D)}\right)>h^{0}\left({L}\right)-2. This is just the usual criterion that a divisor is very ample if and only if it separates any two points , including infinitely near points, on CC (see p.152) . Since LL is base-point free if D=p1+p2D=p_{1}+p_{2},

hence h1(L(−D))=1h^{1}\left({L(-D)}\right)=1 and hence L(−D)=KC(−E)L(-D)=K_{C}(-E) with deg⁡(E)=2\deg(E)=2 and EE effective, so L=KC(D−E)L=K_{C}(D-E).

The condition that L=KC(D1−D2)L=K_{C}(D_{1}-D_{2}) with DiD_{i} general is equivalent to a line which intersects CC in 3 points. This is because h0(L)=g−1h^{0}\left({L}\right)=g-1 and

so D1D_{1} is a line. Finally, any quadric containing CC contains D‾1\overline{D}_{1}, since if QQ is any such quadric #(D‾1∩Q)≥3\#(\overline{D}_{1}\cap Q)\geq 3.

The map Cd×Cd⟶Pic2d(C)C^{d}\times C^{d}\longrightarrow Pic^{2d}(C) given by (E,D)↦E−D(E,D)\mapsto E-D has 2d2d dimensional image in P2d(C)P_{2d}(C) (). So for g≥3g\geq 3, a general line bundle is base-point free, and for g≥5g\geq 5, a general bundle of degree 2g−22g-2 is very ample. This is because the above theorem shows that the space of line bundles with a base point is two dimensional and the space of non ample line bundles is of dimension 4.

Before moving on to the the Clifford index of line bundles of degree ≥2g−2\geq 2g-2, I would like to give one more application of this idea.

One says a divisor DD of degree dd defines a dd-pointed jj secant if DD is of degree dd and spans a projective space of dimension jj. By Geometric Riemann-Roch, DD spans a d−1−rd-1-r plane with r≥0r\geq 0. A general set of points has r=0r=0. One can ask what is the smallest dd such that there exists a dd-pointed d−1−rd-1-r plane. gives the formula that there exists a dd-pointed d−1−rd-1-r plane if: d≥r(h0(L)−d+r)d\geq r(h^{0}\left({L}\right)-d+r) This holds for any very ample LL such that h1(L)=0h^{1}\left({L}\right)=0. The techniques used in are sophisticated.

For r=1r=1 and deg⁡(L)=2g−2\deg(L)=2g-2, we can prove this very simply. In this case, the result is

If d≥h0(L)−d+1d\geq h^{0}\left({L}\right)-d+1, then there exists a dd-pointed d−2d-2 plane.

Rearranging terms, we need to show that if 2d≥h0(L)+12d\geq h^{0}\left({L}\right)+1, then there exists a divisor DD of degree dd, such that h1(L(−D))>0h^{1}\left({L(-D)}\right)>0. Using the same argument of as before, if gg is even, the map Sym⁡g2(C)×Sym⁡g2(C)⟶Picg(C)\operatorname{Sym}^{\frac{g}{2}}(C)\times\operatorname{Sym}^{\frac{g}{2}}(C)\longrightarrow Pic^{g}(C), or if gg is odd, the map Sym⁡g+12(C)×Sym⁡g+12(C)⟶Picg(C)\operatorname{Sym}^{\frac{g+1}{2}}(C)\times\operatorname{Sym}^{\frac{g+1}{2}}(C)\longrightarrow Pic^{g}(C) (D,ED,E) ↦D−E−p0\mapsto D-E-p_{0} for a fixed p0p_{0} are surjective. In either case we get that for any divisor L0L_{0} of degree 0, we may write L0=OC(D−E)L_{0}=\mathcal{O}_{C}(D-E), with deg⁡(D)≤g+12\deg(D)\leq\frac{g+1}{2}. Since L=KC⊗L0L=K_{C}\otimes L_{0} for some L0L_{0}, L(−D)=KC(−E)L(-D)=K_{C}(-E), and hence for the embedding given by LL, DD is a dd-secant d−2d-2 plane.

We now consider the case where deg⁡(L)≥2g+1\deg(L)\geq 2g+1. We distinguish between the case when L contains KCK_{C} as a subsheaf and when L doesn’t. Of course if deg(L) ≥3g−2\geq 3g-2, then the canonical bundle will always be a subsheaf. These results are used in calculating the bounds for which one can say that curves of high degree, and certain of their secant varieties, are determinantally defined.

If L=KC(D)L=K_{C}(D) with DD effective of degree =d≥2=d\geq 2, then Cliff⁡(L,C)=d−2\operatorname{Cliff}(L,C)=d-2. Unless CC is hyperelliptic, DD uniquely achieves this bound.

h0(L)=g−1+dh^{0}\left({L}\right)=g-1+d and h0(L(−D))=h0(KC)=gh^{0}\left({L(-D)}\right)=h^{0}\left({K_{C}}\right)=g, so DD spans a dd secant d−2d-2 plane, that is, rL(D)=1r_{L}(D)=1 and Cliff⁡(L,D)=d−2\operatorname{Cliff}(L,D)=d-2. If EE satisfies rL(E)>0r_{L}(E)>0 then h1(L(−E))>0h^{1}\left({L(-E)}\right)>0, i.e. L(−E)=KC(−E1)L(-E)=K_{C}(-E_{1}). Let e=deg⁡(E)e=\deg(E), e1=deg⁡(E1)e_{1}=\deg(E_{1}), and set h0(OC(E1))=r1+1h^{0}\left({\mathcal{O}_{C}(E_{1})}\right)=r_{1}+1. Then h1(L(−E))=h1(KC(−E1))=g−e1+r1=g+d−e+r1=g+d−1−e+(r1+1)h^{1}\left({L(-E)}\right)=h^{1}\left({K_{C}(-E_{1})}\right)=g-e_{1}+r_{1}=g+d-e+r_{1}=g+d-1-e+(r_{1}+1), and hence rL(E)=r1+1r_{L}(E)=r_{1}+1. Hence we get Cliff⁡(L,E)=deg⁡(E)−2rL(E)\operatorname{Cliff}(L,E)=\deg(E)-2r_{L}(E). d+e1−2(r1+1)=d−2+e1−2r1=d−2+Cliff⁡(E1)d+e_{1}-2(r_{1}+1)=d-2+e_{1}-2r_{1}=d-2+\operatorname{Cliff}(E_{1}). By Clifford’s theorem: Cliff⁡(E1)≥0\operatorname{Cliff}(E_{1})\geq 0, with equality ⇔E1=0\Leftrightarrow E_{1}=0, KCK_{C}, or CC is hyperelliptic and E1=ng21E_{1}=ng_{2}^{1} a multiple of the g21g_{2}^{1}. E1=0E_{1}=0 means E=DE=D; E1=KCE_{1}=K_{C} means E=LE=L. Clearly E=D+ng21E=D+ng_{2}^{1} will give a divisor with Cliff⁡(L,E)=d−2\operatorname{Cliff}(L,E)=d-2.

Suppose deg⁡(L)=2g−2+d\deg(L)=2g-2+d, L=KC(D)L=K_{C}(D), deg⁡(D)=d>1\deg(D)=d>1 and h0(OC(D))=0h^{0}\left({\mathcal{O}_{C}(D)}\right)=0 , then Cliff⁡(C,D)≥d−1\operatorname{Cliff}(C,D)\geq d-1 unless CC is hyperelliptic, in which case Cliff⁡(C,L)=d−2\operatorname{Cliff}(C,L)=d-2 is achieved.

If rL(E)>0r_{L}(E)>0, then H1(L(−E))>0H^{1}\left({L(-E)}\right)>0, so L(−E)=KC(−E1)L(-E)=K_{C}(-E_{1}), with E1E_{1} effective. Again let deg⁡(E)=e\deg(E)=e, deg⁡(E1)=e1\deg(E_{1})=e_{1}, and suppose h0(OC(E1))=r1+1h^{0}\left({\mathcal{O}_{C}(E_{1})}\right)=r_{1}+1, then rL(E)=r1+1r_{L}(E)=r_{1}+1 and Cliff⁡(L,E)=e−2rL(E)=d+e1−2(r1+1)=d−2+(e1−2r1)\operatorname{Cliff}(L,E)=e-2r_{L}(E)=d+e_{1}-2(r_{1}+1)=d-2+(e_{1}-2r_{1}). Again by Clifford’s theorem, e−2r1>0e-2r_{1}>0 unless CC is hyperelliptic. If CC is hyperelliptic, then taking L=KC(D−E)L=K_{C}(D-E) with DD general and EE a multiple of the g21g_{2}^{1} will produce LL with Cliff⁡(C,L)=d−2\operatorname{Cliff}(C,L)=d-2.

If L=KC(D)L=K_{C}(D), deg⁡(D)=d>0\deg(D)=d>0, then Cliff⁡(L,C)≥d−2\operatorname{Cliff}(L,C)\geq d-2.

Generalized Shiffer Variations

The goal of this section is to generalize Shiffer variations to an arbitrary very ample line bundle. We wish to prove the same sort of theorem for arbitrary line bundles as we have proven for KCK_{C}. That is we wish to define Shiffer variations and relate their ranks to Cliff(C,L). In this section we will show how Shiffer variations may be defined in general and discuss the geometric information that is necessary to relate a curve and its secant varieties to rank loci.

As with the case L=KCL=K_{C} it is convenient to use the geometric version of projective spaces of lines in the dual vector space. That is to say, we consider the space of lines in H0(C,L)∨=H1(C,KC⊗L−1)H^{0}\left({C,L}\right)^{\vee}=H^{1}\left({C,K_{C}\otimes L^{-1}}\right), rather than hyperplanes in H0(C,L)H^{0}\left({C,L}\right).

where the last statement follows by the exactness of the long exact sequence.

We now turn our attention to defining Shiffer variations in general. Just as elements of H1(TC)H^{1}\left({T_{C}}\right) can be considered as elements of

(via the cup product), we can consider elements of H1(C,KC⊗L−2)H^{1}\left({C,K_{C}\otimes L^{-2}}\right) =H0(C,L⊗2)∨=H^{0}\left({C,L^{\otimes 2}}\right)^{\vee} as elements of Hom⁡(H0(C,L),H1(KC⊗L−1))\operatorname{Hom}\left(H^{0}\left({C,L}\right),H^{1}\left({K_{C}\otimes L^{-1}}\right)\right). To make sense of the geometry we must assume that the map

Fact: AA is injective ⟺H0(C,L)\Longleftrightarrow H^{0}\left({C,L}\right) is quadratically normal, that is H0(L)⊗H0(L)⟶H0(L⊗2)H^{0}\left({L}\right)\otimes H^{0}\left({L}\right)\longrightarrow H^{0}\left({L^{\otimes 2}}\right) is surjective.

Hom⁡(H0(L),H1(KC⊗L−1))=H0(L)∨⊗H0(L)∨\operatorname{Hom}\left(H^{0}\left({L}\right),H^{1}\left({K_{C}\otimes L^{-1}}\right)\right)=H^{0}\left({L}\right)^{\vee}\otimes H^{0}\left({L}\right)^{\vee} by Serre duality. The natural map H1(KC⊗L−2)⟶H0(L)∨⊗H0(L)∨H^{1}\left({K_{C}\otimes L^{-2}}\right)\longrightarrow H^{0}\left({L}\right)^{\vee}\otimes H^{0}\left({L}\right)^{\vee} is injective ⟺ the dual map H0(L)⊗H0(L)⟶H1(KC⊗L−2)∨=H0(L⊗2)\Longleftrightarrow\text{ the dual map }H^{0}\left({L}\right)\otimes H^{0}\left({L}\right)\longrightarrow H^{1}\left({K_{C}\otimes L^{-2}}\right)\vee=H^{0}\left({L^{\otimes 2}}\right) is surjective.

Let TL(D)=∂(H0(KC⊗L−2(D)∣D))⊂H1(KC⊗L−2)T_{L}(D)=\partial\left(H^{0}\left({K_{C}\otimes L^{-2}(D)|_{D}}\right)\right)\subset H^{1}\left({K_{C}\otimes L^{-2}}\right).

TL(D)T_{L}(D) are the Shiffer variations (for LL) supported on DD.

Our calculations relate to rank and are independent of the choice of local parameter. We will generally proceed by choosing a local parameter and making our calculation “locally”. We need one more piece of notation.

The next theorem shows how to compute Shiffer deformations. Just as in the case of L=KCL=K_{C} they can be computed locally. and hence the exact same proof applies.

Let ξ∈TL(D)⊂H1(KC⊗L−2)\xi\in T_{L}(D)\subset H^{1}\left({K_{C}\otimes L^{-2}}\right). Denote by ρ\rho the natural restriction H0(C,L)⟶ρH0(C,L∣D)H^{0}\left({C,L}\right)\stackrel{{\scriptstyle\rho}}{{\longrightarrow}}H^{0}\left({C,L|_{D}}\right). Denote by

the boundary map in the long exact sequence of cohomology coming from the exact sequence

and denote by ∂2:H0(KC⊗L−2(D)∣D)⟶H1(KC⊗L−2)\partial_{2}:H^{0}\left({K_{C}\otimes L^{-2}(D)|_{D}}\right)\longrightarrow H^{1}\left({K_{C}\otimes L^{-2}}\right) the boundary map in the long exact sequence of cohomology coming from the short exact sequence

We can use Cěch cohomology to compute all the maps. Let V1V_{1} be an open set such that D⊂V1D\subset V_{1}, and V2=C−DV_{2}=C-D. We use this open cover. Write D=∑i=1nnipiD=\sum_{i=1}^{n}n_{i}p_{i}.

Let ξ∈TL(D)\xi\in T_{L}(D). Then ker⁡(ξ)⊃H0(L(−D))\operatorname{ker}(\xi)\supset H^{0}\left({L(-D)}\right) and im⁡(ξ)⊂SL(D)\operatorname{im}(\xi)\subset S_{L}(D), the affine cone over D‾\overline{D}.

When L=KCL=K_{C}, Theorem 2.1 characterized the Clifford index as the smallest integer jj for which Sec⁡j−1(C)\operatorname{Sec}^{j-1}(C) is not the full rank jj locus. Here is the set-up for general LL. We assume for now only that LL is very ample and quadratically normal.

(ii)(ii) is clear because any element of v(X)v(X) is of rank 1. As many people have observed the sum of kk rank 1 matrices is of rank ≤k\leq k.

The proof in the general case is exactly the same as for when d=2d=2 and XX is a curve, the case Hassett did. We include it for completeness.

If we let Λ=⟨p1,…pm⟩\Lambda=\langle p_{1},\ldots p_{m}\rangle, then H0(V,IX(d))H^{0}\left({V,I_{X}(d)}\right) vanished at pp, i.e.

Let φ:V⟶V∨\varphi:V\longrightarrow V^{\vee} be a linear map which is an isomorphism. Let W⊂VW\subset V be of codimension rr, then φ∣W:W⟶W∨\varphi|_{W}:W\longrightarrow W^{\vee} is of rank ≥d−2r\geq d-2r.

Because φ\varphi is an isomorphism, φ1:W⟶V∨\varphi_{1}:W\longrightarrow V\vee has rank d−rd-r and since π:V∨⟶W∨\pi:V\vee\longrightarrow W\vee has an rr dimensional kernel, φ∣W=π∘φ1\varphi|_{W}=\pi\circ\varphi_{1} has rank at least (d−r)−r=d−2r(d-r)-r=d-2r.

Since we are local over pp we can identify H0(C,L∣np)H^{0}\left({C,L|_{np}}\right) with k[z]/znk[z]/z^{n}, where kk is a field of definition for CC and we can identify H0(KC⊗L−1(np)∣np)H^{0}\left({K_{C}\otimes L^{-1}(np)|_{np}}\right) with ⨁j=0n−1z−jk\bigoplus_{j=0}^{n-1}z^{-j}k. Under this identification ξ=∑j=0n−1βjzj\xi=\sum_{j=0}^{n-1}\beta_{j}z^{j} corresponds to the matrix

which has determinant (βn−1)n(\beta_{n-1})^{n}.

As mentioned in Theorem 4.6 the condition βi,ni≠0\beta_{i,{n_{i}}}\neq 0 is exactly the condition that τ∈TL(D)\tau\in T_{L}(D) is not an element of TL(D′)T_{L}(D^{\prime}) for some D′⊂DD^{\prime}\subset D. That is to say that τ∈\mboxSecd−1(C)/\mboxSecd−2(C)\tau\in\mbox{Sec}^{d-1}(C)/\mbox{Sec}^{d-2}(C). Obviously elements of TL(D)T_{L}(D) can have low rank by lying in a low dimensional secant variety. For example rk⁡(τp)=1\operatorname{rk}(\tau_{p})=1 for any p∈Cp\in C. Since we are only interested in the ranks of generic elements of TL(D)T_{L}(D) we make the following definition.

TL∗(D)={τ∈TL(D)∣βi,ni≠0∀i}T_{L}^{*}(D)=\{\tau\in T_{L}(D)|\beta_{i,{n_{i}}}\neq 0\forall i\} That is TL∗(D)=TL(D)∩(\mboxSecd−1(C)/\mboxSecd−2(C))T_{L}^{*}(D)=T_{L}(D)\cap(\mbox{Sec}^{d-1}(C)/\mbox{Sec}^{d-2}(C)).

When L=KCL=K_{C} one checked, using Shiffer variations, that one had equality \mboxSecj−1(C)=Rj\mbox{Sec}^{j-1}(C)=R^{j} for j<j< Cliff(C). The same sort of result is true in general, but the results have different flavors depending on whether h1(L)>0h^{1}\left({L}\right)>0 or h1(L)=0h^{1}\left({L}\right)=0. Roughly speaking for h1(L)>2h^{1}\left({L}\right)>2, I cannot say anything general. For h1(L)=1h^{1}\left({L}\right)=1 a version of the theorem is true, but weaker, as the lower bound does not generally occur. If h1(L)=0h^{1}\left({L}\right)=0 and deg⁡(L)≥2g−2\deg(L)\geq 2g-2. one can get strong results with the strongest results being for deg⁡(L)≥2g+1\deg(L)\geq 2g+1. We first consider the case h1(L)=0h^{1}\left({L}\right)=0 and deg⁡(L)>2g+1\deg(L)>2g+1.

Geometric Characterization of the Clifford Index for Line Bundles of Large Degree

Throughout this section L will be a very ample line bundle of degree ≥2g+1\geq 2g+1. We restrict to this case because in this range LL is always a very ample, quadratically normal line bundle. Recall that in section 3 we have calculated the Clifford index of any line bundle of degree ≥2g+1\geq 2g+1. We recall this and explain its relationship with secant varieties now.

By Theorem 3.6 we know that if L=KC(D)L=K_{C}(D) with DD effective, then Cliff(C,L)= d−2d-2 and by Theorem 3.7 generically Cliff(C,L) =d−1=d-1. In both cases by Lemma 5.4 we can find special Shiffer variations of rank equal to Cliff⁡(C,L)\operatorname{Cliff}(C,L). We are only claiming set theoretic equality (and inequality) at the moment. We will break the proof down into two pieces, the equality and the inequality.

That this diagram commutes follows if LL is very ample and quadratically normal.

Suppose that j<Cliff(C,L)=cj<Cliff(C,L)=c. then as sets Sec⁡j−1(C)=Rj(C)\operatorname{Sec}^{j-1}(C)=R^{j}(C). Further if LL is generic then Sec⁡c−1(C)⫋Rc(C)\operatorname{Sec}^{c-1}(C)\subsetneqq R^{c}(C).

Let EE be any divisor on CC. Using the factorization for the map ξ∈TL(E)\xi\in T_{L}(E) given by theorem 4.2 we can factor ξ∈TL(E)\xi\in T_{L}(E) as,

If rL(D)=r>0r_{L}(D)=r>0 and rL⊗2(D)=0r_{L^{\otimes 2}}(D)=0, we can find a τ∈TL(D)\tau\in T_{L}(D), rk⁡(τ)=d−2\operatorname{rk}(\tau)=d-2.

Our assumption is that DD fails to impose independent conditions on the linear system given by LL, but does impose independent conditions of L⊗2L^{\otimes 2}. Hence TL(D)T_{L}(D) gives rise to a dd-dimensional subspace of H1(KC⊗L−2)H^{1}\left({K_{C}\otimes L^{-2}}\right), and hence we have dd rank one elements of TL(D)T_{L}(D) whose image lies in at most a (d−1)(d-1) dimensional space. In fact, τ\tau are distinct as elements of

Let x1,…,xd∈Vx_{1},\ldots,x_{d}\in V with dim⁡(V)=d−1\dim(V)=d-1, x1,…,xd−1x_{1},\dots,x_{d-1} a base, xd=∑i=1d−1aixix_{d}=\sum_{i=1}^{d-1}a_{i}x_{i}, with ai≠0a_{i}\neq 0. Then identifying Sym⁡2(V)\operatorname{Sym}^{2}(V) with Hom⁡sym(V∨,V\operatorname{Hom}^{sym}(V^{\vee,V}, there exists λ≠0\lambda\neq 0 such that rk⁡(∑i=1d−1xi2+λxd2)≤d−2\operatorname{rk}(\sum_{i=1}^{d-1}x_{i}^{2}+\lambda x_{d}^{2})\leq d-2.

Let f(λ)=det⁡(x12+⋯+xd−12+λxd2)f(\lambda)=\det(x_{1}^{2}+\cdots+x_{d-1}^{2}+\lambda x_{d}^{2}), so f(0)=1f(0)=1. Unless ff is constant there exists λ\lambda such that f(λ)=0f(\lambda)=0, i.e. rk⁡(x12+⋯+xd−12+λxd2)≤d−2\operatorname{rk}(x_{1}^{2}+\cdots+x_{d-1}^{2}+\lambda x_{d}^{2})\leq d-2 as desired. But as a polynomial in λ\lambda it has leading term λd−1∏i=1d−1ai2\lambda^{d-1}\prod_{i=1}^{d-1}a_{i}^{2}, and hence the polynomial is non-constant.

Let L=KC(D)L=K_{C}(D). ∃ τ∈TL(D)\exists\,\tau\in T_{L}(D) such that i) rk⁡(τ)=d−2\operatorname{rk}(\tau)=d-2, ii) im⁡(τ)∩C=∅\operatorname{im}(\tau)\cap C=\emptyset.

By the lemma above ∃ τ\exists\,\tau of rank <d−1<d-1 and rk⁡(τ)≥d−2=Cliff⁡(C,D)\operatorname{rk}(\tau)\geq d-2=\operatorname{Cliff}(C,D) in any event, so ∃ τ\exists\,\tau such that rk⁡(τ)=d−2\operatorname{rk}(\tau)=d-2. By Hassett’s criterion(4.5, since Sec⁡d−3=Rd−3\operatorname{Sec}^{d-3}=R^{d-3}, if τ∉Sec⁡d−2(C)\tau\notin\operatorname{Sec}^{d-2}(C), then im⁡(τ)∩C≠∅\operatorname{im}(\tau)\cap C\neq\emptyset. But if τ∉Sec⁡d−2(C)\tau\notin\operatorname{Sec}^{d-2}(C) , then ∃ τ′∈TL(D′)\exists\,\tau^{\prime}\in T_{L}(D^{\prime}) with deg⁡(D)<d−2\deg(D)<d-2 such that τ=τ′\tau=\tau^{\prime}, i.e. D′=D−RD^{\prime}=D-R, with RR effective. This would mean σ12+⋯σd−12+λσd2=∑i=1d′<dλiσi2\sigma_{1}^{2}+\cdots\sigma_{d-1}^{2}+\lambda\sigma_{d}^{2}=\sum_{i=1}^{d^{\prime}<d}\lambda_{i}\sigma_{i}^{2}, i.e. H0(KC⊗L−2(D))≠0H^{0}\left({K_{C}\otimes L^{-2}(D)}\right)\neq 0, i.e. H0(L−1)≠0H^{0}\left({L^{-1}}\right)\neq 0 which is absurd. (Any relation ∑σi∈Dλiσi2=0∈H0(KC⊗L−2)\sum_{\sigma_{i}\in D}\lambda_{i}\sigma_{i}^{2}=0\in H^{0}\left({K_{C}\otimes L^{-2}}\right) implies H0(KC⊗L−2(D))≠0H^{0}\left({K_{C}\otimes L^{-2}(D)}\right)\neq 0.)

Throughout this section LL will either be KCK_{C} or deg⁡(L)≥2g+1\deg(L)\geq 2g+1. If L=KCL=K_{C} then we will further assume that g(C)≥3g(C)\geq 3 and Cliff⁡(C)≥1\operatorname{Cliff}(C)\geq 1. In particular LL will always be very ample and quadratically normal. Let n=h0(L)n=h^{0}\left({L}\right), V=H0(C,L)∨V=H^{0}\left({C,L}\right)^{\vee} and let M2=H0(L⊗2)∨M_{2}=H^{0}\left({L^{\otimes 2}}\right)^{\vee}. Denote by

Let H=Hom⁡(V,W)\mathbf{H}=\operatorname{Hom}(V,W) where VV and WW are finite dimensional vector spaces. The space of rank p matrices in H\mathbf{H} is defined by the vanishing of all the (p+1)×(p+1)(p+1)\times(p+1) minors with respect to some choice of a basis for VV and WW. It is denoted by Hp.\mathbf{H}^{p}. It is known that Hp\mathbf{H}^{p} is Cohen–Macaulay and smooth away from Hp−1\mathbf{H}^{p-1}. The Cohen-MacCauley statement can be found in p.175 for example. The proof of the smoothness statement follows from the existence of a canonical desingularization, H~p\widetilde{\mathbf{H}}^{p}, of Hp\mathbf{H}^{p}, and the calculation of the tangent space to H~p\widetilde{\mathbf{H}}^{p} at a general point. For completeness we sketch the construction. The details may be found in .

Remark 1: In our case V=W∨=H0(C,L)V=W^{\vee}=H^{0}\left({C,L}\right) and M=H0(C,L⊗2)M=H^{0}\left({C,L^{\otimes 2}}\right) and in fact M↪Sym⁡2(W)↪Hom⁡(V,W)\mathbf{M}\hookrightarrow\operatorname{Sym}^{2}(W)\hookrightarrow\operatorname{Hom}(V,W). We will need this greater generality to deal with the scheme structures that occur in section 7.

Remark 2: We will see later that in this case, M=H0(C,L⊗2),\mathbf{M}=H^{0}\left({C,L^{\otimes 2}}\right), that Rp∖Rp−1R^{p}\setminus R^{p-1} is smooth if p<Cliff⁡(C,L)p<\operatorname{Cliff}(C,L).

With the notation of Definition 6.1, let φ∈Rp∖Rp−1\varphi\in R^{p}\setminus R^{p-1}, then Tφ,M={ ψ∈M∣ψ:ker⁡(φ)⟶im⁡(φ)T_{\varphi,\mathbf{M}}=\{\,\psi\in\mathbf{M}|\psi:\ker(\varphi)\longrightarrow\operatorname{im}(\varphi)}

Let T\mathbf{T} denote the tangent space to φ\varphi in Hom⁡(V,W)\operatorname{Hom}(V,W). We have previously identified T\mathbf{T} with {ψ∈H∣ψ:ker⁡(φ)⟶im⁡(φ)}\{\psi\in\mathbf{H}|\psi:\ker(\varphi)\longrightarrow\operatorname{im}(\varphi)\}. Since M\mathbf{M} is a subspace of H\mathbf{H}, Tφ,M={ ψ∈T ∣ψ(I)=0}T_{\varphi,\mathbf{M}}=\{\,\psi\in\mathbf{T}\,|\psi(I)=0\} where I=I(M)I=I(\mathbf{M}), is the ideal of M\mathbf{M}. Since M\mathbf{M} is a linear space, the condition on ψ\psi is that ψ∈M\psi\in\mathbf{M} ∎

We recall the notations and results of and construct a rank pp bundle Bp−1(M)B^{p-1}(M) over Sym⁡p(C)\operatorname{Sym}^{p}(C). Informally it is the rank pp bundle D↦H0(C,M∣D)D\mapsto H^{0}\left({C,M|_{D}}\right). The actual construction is given below. MM will denote any very ample line bundle with h0(M)=nh^{0}\left({M}\right)=n and satisfying h0(M(−D))=h0(M)−dh^{0}\left({M(-D)}\right)=h^{0}\left({M}\right)-d for all divisors DD with deg⁡(D)=d≤p\deg(D)=d\leq p. The last condition is that MM separates pp points.

Let Dp↪C×Sym⁡p(C)\mathcal{D}_{p}\hookrightarrow C\times\operatorname{Sym}^{p}(C) be the universal divisor, π2:C×Sym⁡p(C)⟶Sym⁡p(C)\pi_{2}:C\times\operatorname{Sym}^{p}(C)\longrightarrow\operatorname{Sym}^{p}(C), then Bp−1(M)=π2∗(π1∗(M)∣Dp)B^{p-1}(M)=\pi_{2*}\left(\pi_{1}^{*}(M)|_{\mathcal{D}_{p}}\right).

Since π2∗π1∗(M)=H0(M)⊗OSym⁡p(C)\pi_{2*}\pi_{1}^{*}(M)=H^{0}\left({M}\right)\otimes\mathcal{O}_{\operatorname{Sym}^{p}(C)} and MM separate pp points , the map H0(M)⊗OSym⁡p(L)↠Bp−1(M)H^{0}\left({M}\right)\otimes\mathcal{O}_{\operatorname{Sym}^{p}(L)}\twoheadrightarrow B^{p-1}(M) is surjective. Hence we get an inclusion of projective bundles,

Remark 1) Since Bp−1(M)B^{p-1}(M) is smooth, and so reduced, the scheme theoretic image of the projection is also reduced. See p.92 for details.

Remark 3) We have used the fact the the line bundle LL separates pp points in the definition. It is possible to define a the Secant variety without this extra condition, see for example .

For the rest of this section LL will also satisfy Cliff⁡(C,L)>p\operatorname{Cliff}(C,L)>p. Notice that if Cliff⁡(C,L)>p\operatorname{Cliff}(C,L)>p then LL separates pp points. Recall that RpR^{p} is defined in equation 1.

We have a scheme theoretic inclusion \mboxSecp−1(L)↪Rp\mbox{Sec}^{p-1}(L)\hookrightarrow R^{p}.

To show scheme theoretic inclusion we need to show an inclusion of the ideal sheaves: IRp↪ISec\mathcal{I}_{R^{p}}\hookrightarrow\mathcal{I}_{Sec} . Since RpR^{p} is defined by the vanishing of all the (p+1)×(p+1)(p+1)\times(p+1) minors of the generic matrix, we need to show that \mboxSecp−1(C)\mbox{Sec}^{p-1}(C) vanishes on all (p+1)×(p+1)(p+1)\times(p+1) minors. Roughly speaking, any point x∈\mboxSecp−1(C)x\in\mbox{Sec}^{p-1}(C) is a linear sum of pp points of CC. Each point of C represents a rank one linear transformation. Hence each x∈\mboxSecp−1(C)x\in\mbox{Sec}^{p-1}(C) has a representation as the sum of pp rank one transformations and hence is of rank at most pp. Thus every point x∈\mboxSecp−1(C)x\in\mbox{Sec}^{p-1}(C) will vanish at all (p+1)×(p+1)(p+1)\times(p+1) minors and hence scheme theoretically lies in RpR^{p}. Because this point comes up frequently, I will give it a separate formal proof. The result is well-known (see () for example).

First we fix some notation. Let W⊂Hom⁡(V1,V2)W\subset\operatorname{Hom}(V_{1},V_{2}) be a linear space and let R⊂WR\subset W be a subset consisting of rank one transformations. This means that for every r∈Rr\in R, the kernel of rr is of codimension one and that the image of rr is of dimension one. By \mboxSecp−1(R)\mbox{Sec}^{p-1}(R) we mean all linear combinations of pp elements of RR.

Every element rp∈\mboxSecp−1(R)r_{p}\in\mbox{Sec}^{p-1}(R) is of rank at most pp. That is if we fix a basis for V1V_{1} and V2V_{2} every (p+1)×(p+1)(p+1)\times(p+1) minor of rpr_{p} vanishes. Informally: every sum of at most pp rank one matrices is of rank at most pp.

If p+1>min⁡(dim⁡(V1),dim⁡(V2)p+1>\min(\dim(V_{1}),\dim(V_{2}) the result is trivial. So we assume that p+1≤min⁡(dim⁡(V1),dim⁡(V2)p+1\leq\min(\dim(V_{1}),\dim(V_{2}) Once we have picked a basis we can represent any r∈Rr\in R as a matrix (aij)(a_{ij}) with a unique aij≠0a_{ij}\neq 0. Hence any rp∈\mboxSecp−1r_{p}\in\mbox{Sec}^{p-1} can have at most pp columns (or rows) with a non-zero entry. If we take a (p+1)×(p+1)(p+1)\times(p+1) submatrix and expand along a column (or row) with all zeros we see that the determinant vanishes. ∎

Since \mboxSecp−1(C)\mbox{Sec}^{p-1}(C) and RpR^{p} agree as sets, if RpR^{p} is reduced then since RpR^{p} is a thickening of \mboxSecp−1(C)\mbox{Sec}^{p-1}(C) both varieties are isomorphic having the reduced scheme structure.

There is a fair amount of literature on the scheme structure of \mboxSecp(C)\mbox{Sec}^{p}(C). See , , for example. It is known to be normal in many circumstances. The first theorem on the subject is due to Bertram.

If LL separates 2p2p points then \mboxSecp−1(C)\mbox{Sec}^{p-1}(C) is normal and smooth away from \mboxSecp−2(C)\mbox{Sec}^{p-2}(C).

Remark: In case L=KCL=K_{C} or deg⁡(L)≥2g+1\deg(L)\geq 2g+1 and p<Cliff⁡(C,L)p<\operatorname{Cliff}(C,L), one easily checks that L⊗2L^{\otimes 2} separates 2p2p points and hence that \mboxSecp−1(C)\mbox{Sec}^{p-1}(C) is normal.

The fact that \mboxSecp−1(C)=Rp\mbox{Sec}^{p-1}(C)=R^{p}, a rank locus, may suggest that in fact these varieties are Cohen-Macauley. Very little is known about this. Recently Sidman and Vermeire have proven that if deg⁡(L)≥2g+3\deg(L)\geq 2g+3 then Sec⁡1(C)\operatorname{Sec}^{1}(C) is Cohen-Macauley. Further Vermeire in has shown that if deg⁡(L)\deg(L) is sufficiently large, then \mboxSec(C)\mbox{Sec}(C) is generated by cubics. His bound is better than ours in complete analogy to the fact that, once deg⁡(L)≥2g+2\deg(L)\geq 2g+2 then CC is generated by quadrics, but one needs deg⁡(L)\deg(L) to be about 4g+44g+4 before the equations defining CC are ’determinantally presented’.

Remark If it could be directly shown that RpR^{p} is reduced, then one could conclude directly the scheme theoretic equality. Using Bertram’s Theorem, one would have normality too. I have not been able to create a simple argument to prove this simpler fact. The current proof does have the advantage of explicating the geometry of RpR^{p}. Namely, it shows that the resolution is isomorphic to the full secant variety and that it has reduced, and in fact smooth, fibers.

Suppose L=KCL=K_{C} or deg⁡(L)≥2g+1\deg(L)\geq 2g+1 ,then Cliff⁡(C,L)>p\operatorname{Cliff}(C,L)>p implies Cliff⁡(C,L⊗2)>2p\operatorname{Cliff}(C,L^{\otimes 2})>2p.

If L=KCL=K_{C}, then Cliff⁡(KC)≤g−12\operatorname{Cliff}(K_{C})\leq\frac{g-1}{2} and KC⊗2K_{C}^{\otimes 2} separates any g−1g-1 points. If L≠KCL\neq K_{C} then if deg⁡(L)=2g−2+d\deg(L)=2g-2+d with d<gd<g , then Cliff⁡(C,L)≤d−1\operatorname{Cliff}(C,L)\leq d-1 and if d≥gd\geq g then Cliff⁡(C,L)=d−2\operatorname{Cliff}(C,L)=d-2. Since deg⁡(L⊗2)=4g−4+2d\deg(L^{\otimes 2})=4g-4+2d, Cliff⁡(C,L⊗2)=2g−4+2d−2>2(d−1)\operatorname{Cliff}(C,L^{\otimes 2})=2g-4+2d-2>2(d-1) . ∎

If p<Cliff⁡(C,L)p<\operatorname{Cliff}(C,L) and φ∈Rp∖Rp−1\varphi\in R^{p}\setminus R^{p-1}, then RpR^{p} is smooth at φ\varphi. In fact Tφ,Rp=2D‾L⊗2T_{\varphi,R^{p}}=\overline{2D}_{L^{\otimes 2}}, that is, the tangent space to RpR^{p} at φ\varphi is the 2p−12p-1 dimensional space spanned by the divisor 2D2D.

H1(KC⊗L−2)⟶αH1(KC⊗L−2(2D))⟶βH^{1}\left({K_{C}\otimes L^{-2}}\right)\overset{\alpha}{\longrightarrow}H^{1}\left({K_{C}\otimes L^{-2}(2D)}\right)\overset{\beta}{\longrightarrow}

Hom⁡(H0(L(−D)),H1(KC⊗L−1(D)))\operatorname{Hom}(H^{0}\left({L(-D)}\right),H^{1}\left({K_{C}\otimes L^{-1}(D)}\right)).

Notice that ker⁡(α)=∂(H0(KC⊗L−2(2D)∣2D))\ker(\alpha)=\partial(H^{0}\left({K_{C}\otimes L^{-2}(2D)_{|2D}}\right)) that is to say 2D‾L⊗2\overline{2D}_{L^{\otimes 2}}. Since ker⁡(α)⊂ker⁡(rD)\ker(\alpha)\subset\ker(r_{D})’ to finish we need to check that β\beta is injective. We have p<Cliff⁡(C,L)p<\operatorname{Cliff}(C,L) and hence Cliff⁡(C,L(−D))≥1\operatorname{Cliff}(C,L(-D))\geq 1 . In particular L(−D)L(-D) is arithmetically normal, which is equivalent to β\beta being injective by Serre Duality. ∎

Let R~p={(φ,λ)∣im⁡(φ)⊂λ}⊂Rp×G(p,n)\widetilde{R}^{p}=\left\{(\varphi,\lambda)|\operatorname{im}\left(\varphi\right)\subset\lambda\right\}\subset R^{p}\times G(p,n). Then R~p\widetilde{R}^{p} is smooth .

With this notation R~p={(φ,λ)∣φ∪λ=0}\widetilde{R}^{p}=\left\{\left(\varphi,\lambda\right)|\varphi\cup\lambda=0\right\}. This is true as long as we are not working in characteristic 2.

Fix some λ\lambda say λ=v1∧⋯∧vp\lambda=v_{1}\wedge\dots\wedge v_{p} with vi∈Vv_{i}\in V linearly independent. Let ⟨v1…vp⟩=W⊂V\langle v_{1}\dots v_{p}\rangle=W\subset V. From equation ( 6) if φ∈Sym⁡2(W)\varphi\in\operatorname{Sym}^{2}(W) then φ∪λ=0\varphi\cup\lambda=0 since φ=∑i=0paivi2\varphi=\sum_{i=0}^{p}a_{i}v_{i}^{2} with aia_{i} constants (this is true after changing our basis of WW). So we may assume that φ\varphi contains no terms entirely in WW. Extend ⟨v1…vp⟩\langle v_{1}\dots v_{p}\rangle to a basis ⟨v1…vn⟩\langle v_{1}\dots v_{n}\rangle of VV. Write φ=∑i=p+1naili⊗vi+∑i≥j≥(p+1)bijvi⊗vj\varphi=\sum_{i=p+1}^{n}a_{i}l_{i}\otimes v_{i}+\sum_{i\geq j\geq(p+1)}b_{ij}v_{i}\otimes v_{j} with li∈Wl_{i}\in W. Then

Each of the terms are linearly independent and (as long as char(k) ≠2)\neq 2) φ∪λ\varphi\cup\lambda vanishes if and only if all the aia_{i} and all the bijb_{ij} are zero. If char(k)=2=2 then the coefficients of biib_{ii} are zero because they are divisible by two. ∎

Let g:Sym⁡p(C)⟶G(p,n)g:\operatorname{Sym}^{p}(C)\longrightarrow G(p,n) be the natural map associating D↦D‾D\mapsto\overline{D}; then for p≤Cliff⁡(L,C)p\leq\operatorname{Cliff}(L,C) this map is an embedding.

Following we construct a rank pp bundle Bp−1(L)B^{p-1}(L) over Sym⁡p(C)\operatorname{Sym}^{p}(C). Let Dp↪C×Sym⁡p(C)\mathcal{D}_{p}\hookrightarrow C\times\operatorname{Sym}^{p}(C) be the universal divisor, π2:C×Sym⁡p(C)⟶Sym⁡p(C)\pi_{2}:C\times\operatorname{Sym}^{p}(C)\longrightarrow\operatorname{Sym}^{p}(C), then E=π2∗(π1∗(L)∣Dp)\mathcal{E}=\pi_{2*}\left(\pi_{1}^{*}(L)|_{\mathcal{D}_{p}}\right). Informally this is the rank pp bundle D↦H0(C,L∣D)D\mapsto H^{0}\left({C,L|_{D}}\right). Since π2∗π1∗(L)=H0(L)⊗OSym⁡p(C)\pi_{2*}\pi_{1}^{*}(L)=H^{0}\left({L}\right)\otimes\mathcal{O}_{\operatorname{Sym}^{p}(C)} and p≤Cliff⁡(C)p\leq\operatorname{Cliff}(C) implies LL is at least (p+1)(p+1) spanned the map H0(L)⊗OSym⁡p(L)↠E∣LH^{0}\left({L}\right)\otimes\mathcal{O}_{\operatorname{Sym}^{p}(L)}\twoheadrightarrow\mathcal{E}|_{L} is surjective. Since a map g:Sym⁡p(C)⟶G(p,n)g:\operatorname{Sym}^{p}(C)\longrightarrow G(p,n) is given by a rank pp bundle and n sections generating the bundle, this gives a map g:Sym⁡p(C)⟶G(p,n)g:\operatorname{Sym}^{p}(C)\longrightarrow G(p,n). Again because LL separates atleast p+1p+1 points, D‾1≠D‾2,∀D1,D2∈Sym⁡p(C)\overline{D}_{1}\neq\overline{D}_{2},\forall D_{1},D_{2}\in\operatorname{Sym}^{p}(C) and so the map is set theoretically one to one. Using the identification of , we identify TD,Sym⁡p(C)T_{D,\operatorname{Sym}^{p}(C)} with H0(C,OD(D))H^{0}\left({C,\mathcal{O}_{D}(D)}\right) and TD,G(p,n)T_{D,G(p,n)} with Hom⁡(H0(L(−D)),H0(L∣D))\operatorname{Hom}(H^{0}\left({L(-D)}\right),H^{0}\left({L|_{D}}\right)). Then (cf. ) the map on tangent spaces, is the map “cup product”, i.e.

Since LL separates (p+1)(p+1) points, this map is an injection as required. If DD is smooth this is well known. We prove the case D=kqD=kq for completeness. Let zz be a local parameter at qq. H0(OD(D))=<z−1,…,z−k>H^{0}\left({\mathcal{O}_{D}(D)}\right)=\left<z^{-1},\dots,z^{-k}\right>, H0(L∣D)=<l,zl,…,zk−1l>H^{0}\left({L|_{D}}\right)=\left<l,zl,\dots,z^{k-1}l\right> where ll is a local section of LL at qq. Since LL is at least (k+1)(k+1) ample, there exists a section of LL which locally at qq looks like zklz^{k}l and the cup product is now multiplication. Since z−izkl=zk−ilz^{-i}z^{k}l=z^{k-i}l for 1≤i≤h1\leq i\leq h, multiplication gives rise to linearly independent elements of H0(L∣D)H^{0}\left({L|_{D}}\right) the map is injective.

Bp−1(L)B^{p-1}(L) is the pullback to Sym⁡p(C)\operatorname{Sym}^{p}(C) of the universal subbundle on G(p,n)G(p,n). That is Bp−1(L)=g∗(S)B^{p-1}(L)=g^{*}(\mathcal{S}) where S={(x,λ)∈V×∧p(V) ∣ x∧λ=0∈∧p+1(V)}\mathcal{S}=\{(x,\lambda)\in V\times\wedge^{p}(V)\,|\,x\wedge\lambda=0\in\wedge^{p+1}(V)\} . Since Bp−1(L)B^{p-1}(L) is just the restriction of S\mathcal{S} to the embedding of Sym⁡p(C)\operatorname{Sym}^{p}(C) in G(p,n)G(p,n) this is clear.

Remark: this map is not the usual Gauss map. We can include CC in Sym⁡p(C)\operatorname{Sym}^{p}(C) via the diagonal, i.e. q↦pqq\mapsto pq. As Voisin proved cf. H0(C,⋀p(Bp−1(L)))=⋀p(H0(C,L))H^{0}\left({C,\bigwedge^{p}(B^{p-1}(L))}\right)=\bigwedge^{p}(H^{0}\left({C,L}\right)) whereas the rank pp bundle associated with the Gauss map is Pp−1(L)P^{p-1}(L) (the jet bundle) and for example for p=2p=2 ⋀2(P1(L))≃L⊗2⊗KC\bigwedge^{2}\left(P^{1}(L)\right)\simeq L^{\otimes 2}\otimes K_{C} and so the two bundles have different global sections.

To finish the proof we show that RPR^{P} is normal. We use a result that we learned in namely:

Let f:X⟶Yf:X\longrightarrow Y be a proper surjective morphism of irreducible varieties over an algebraically closed field, with reduced and connected fibers. If XX is normal, then YY is normal.

Let φ∈Rk∖Rk−1\varphi\in R^{k}\setminus R^{k-1} , then p−1(φ)p^{-1}(\varphi) is scheme theoretically isomorphic to Sym⁡p−k(C)\operatorname{Sym}^{p-k}(C)

Because k≤p<Cliff⁡(C,L)k\leq p<\operatorname{Cliff}(C,L) we can write φ=∑i=1kσpi2\varphi=\sum_{i=1}^{k}\sigma_{p_{i}}^{2} where σpi2\sigma_{p_{i}}^{2} is a Shiffer variation supported at pi∈Cp_{i}\in C. Denote by DD the divisor spanned by ⟨p1,…pk⟩\langle p_{1},\dots p_{k}\rangle. We analyze p−1(φ)p^{-1}(\varphi) as follows:

φD\varphi_{D} identifies ker⁡(∪φ)∩Sym⁡p(C)\ker(\cup\varphi)\cap\operatorname{Sym}^{p}(C) with Sym⁡p−k(C)\operatorname{Sym}^{p-k}(C) because ifλ∈Sym⁡p(C)if\lambda\in\operatorname{Sym}^{p}(C), considered as a subset of G(p,n)G(p,n) then ∑i=1kσpi2∪λ=∑i=1kσi⊗σi∧λ=0\sum_{i=1}^{k}\sigma_{p_{i}}^{2}\cup\lambda=\sum_{i=1}^{k}\sigma_{i}\otimes\sigma_{i}\wedge\lambda=0 if and only if σi∧λ=0\sigma_{i}\wedge\lambda=0 for all ii. We need to see that this is an equality of schemes. By induction it will be enough to consider the case k=1k=1 because we can write a general φD\varphi_{D} as a composition of φσpi\varphi_{\sigma_{p_{i}}} for the different pi∈Dp_{i}\in D. So we assume that φ=σ2\varphi=\sigma^{2} for a specific σ=σpi\sigma=\sigma_{p_{i}} with pi∈Cp_{i}\in C.

Remark:The conclusion of the theorem is probably as strong as possible. We know for generic LL with deg⁡(L)<3g−2\deg(L)<3g-2 and for all LL with deg⁡(L)≥3g−2\deg(L)\geq 3g-2 the theorem is sharp as the two schemes do not even underly the same set in this case. It is probably the case that this is always so.

The Clifford Index of a Pair of Line Bundles and a Conjecture of Eisenbud, Koh, and Stillman

In their paper (), Eisenbud, Koh and Stillman considered the following situation. Let Li=(Li,Vi) i=1,2\mathcal{L}_{i}=(L_{i},V_{i})\,i=1,2 be two linear series on a curve – that is LiL_{i} is a line bundle on CC and Vi⊂H0(C,Li)V_{i}\subset H^{0}\left({C,L_{i}}\right) is a linear subspace. Let L1⋅L2\mathcal{L}_{1}\centerdot\mathcal{L}_{2} be the linear series (L1⊗L2,V=im⁡(V1⊗V2⟶μH0(C,L1⊗L2))(L_{1}\otimes L_{2},V=\operatorname{im}(V_{1}\otimes V_{2}\stackrel{{\scriptstyle\mu}}{{\longrightarrow}}H^{0}\left({C,L_{1}\otimes L_{2}}\right)). That is L1⋅L2\mathcal{L}_{1}\centerdot\mathcal{L}_{2} represents the line bundle L1⊗L2L_{1}\otimes L_{2} with the sub- linear series generated by V1⊗V2V_{1}\otimes V_{2}. By the linear series generated by V1⊗V2V_{1}\otimes V_{2} we mean the natural map H0(C,L1)⊗H0(C,L2)⟶μH0(C,L1⊗L2)H^{0}\left({C,L_{1}}\right)\otimes H^{0}\left({C,L_{2}}\right)\stackrel{{\scriptstyle\mu}}{{\longrightarrow}}H^{0}\left({C,L_{1}\otimes L_{2}}\right) restricts to a map μ:V1⊗V2⟶H0(C,L1⊗L2)\mu:V_{1}\otimes V_{2}\longrightarrow H^{0}\left({C,L_{1}\otimes L_{2}}\right). μ(V1⊗V2)⊂H0(C,L1⊗L2)\mu(V_{1}\otimes V_{2})\subset H^{0}\left({C,L_{1}\otimes L_{2}}\right) is the linear series generated by V1⊗V2V_{1}\otimes V_{2}

If {ei}\{e_{i}\} and {fj}\{f_{j}\} are bases for V1V_{1} and V2V_{2}, then M={μ(ei⊗fj)}M=\{\mu(e_{i}\otimes f_{j})\} can be considered as a matrix of linear form with entries in H0(C,L1⊗L2)H^{0}\left({C,L_{1}\otimes L_{2}}\right) which represents a basis for μ(V1⊗V2)\mu(V_{1}\otimes V_{2}) . Writing I2(M)I_{2}(M) for the ideal of 2×22\times 2 minors of MM in S=Sym⁡(V)S=\operatorname{Sym}(V), one has that I2(M)⊂I2(C)I_{2}(M)\subset I_{2}(C), where I2(X)I_{2}(X) is equations of degree 2 in the ideal of XX. (Proof: Let mij=μ(ei⊗fj)m_{ij}=\mu(e_{i}\otimes f_{j}) Then the equations of I2(M)I_{2}(M) are mij⋅mkl−mik⋅mjl=0m_{ij}\centerdot m_{kl}-m_{ik}\centerdot m_{jl}=0 which clearly vanish on CC). We now assume that Vi=H0(C,Li)V_{i}=H^{0}\left({C,L_{i}}\right).

If CC is defined by quadratic equations and I2(M)=I2(C)I_{2}(M)=I_{2}(C), we say L1⋅L2\mathcal{L}_{1}\centerdot\mathcal{L}_{2} is a determinantal presentation of CC and that CC is determinantally presented.

We explain how this result is related to our theorem and how their result can be extended to Sec⁡k(C)\operatorname{Sec}^{k}(C) in an appropriate range of kk.

We can create a diagram for L12L_{12} which generalizes our standard diagram.

In general, we will define the rank jj locus for j≤min⁡{dim⁡(V1),dim⁡(V2)}j\leq\min\{\dim(V_{1}),\dim(V_{2})\} as the variety defined by all the (j+1)×(j+1)(j+1)\times(j+1) minors. If L1=L2=LL_{1}=L_{2}=L, Vi=H0(C,Li)V_{i}=H^{0}\left({C,L_{i}}\right) we recover our standard diagram.

Let C be a curve of genus g, and LL a line bundle which can be factored as L=L1⊗L2L=L_{1}\otimes L_{2} for some choice of line bundles L1L_{1} and L2L_{2}.Then there is a constant k0k_{0} depending on the genus of C and the degrees of the LiL_{i} such that the variety Seck(C)Sec^{k}(C) is determinantally presented for k≤k0k\leq k_{0}.

Theorem 7.1 can be interpreted as a version of our theorem for L1≠L2L_{1}\neq L_{2} and for C=\mboxSec0(C)=R1C=\mbox{Sec}^{0}(C)=R^{1}. M.S. Ravi in gave a partial answer to this conjecture.

Suppose deg⁡(L1),deg⁡(L2)≥2g+1+k\deg(L_{1}),\deg(L_{2})\geq 2g+1+k and deg⁡(L1⊗L2)≥4g+3+2k\deg(L_{1}\otimes L_{2})\geq 4g+3+2k. Then set-theoretically, Sec⁡k(C)\operatorname{Sec}^{k}(C) is defined by Ik+2(M)I_{k+2}(M), that is, Sec⁡k(ψ(C))=Rk+1(C)\operatorname{Sec}^{k}(\psi(C))=R^{k+1}(C).

By generalizing the techniques of Shiffer variations and the Clifford index of a line bundle from the case of L⊗2=L⊗LL^{\otimes 2}=L\otimes L to the case of M=L12M=L_{12} we can improve this result.

Suppose deg⁡(L1),deg⁡(L2)≥2g+1+k\deg(L_{1}),\deg(L_{2})\geq 2g+1+k and deg⁡(L1⊗L2)≥4g+2+2k\deg(L_{1}\otimes L_{2})\geq 4g+2+2k. Then as a scheme Sec⁡k−1(C)\operatorname{Sec}^{k-1}(C) is defined by Ik+1(M)I_{k+1}(M). That is, as schemes, Sec⁡k−1(C)=Rk(C)\operatorname{Sec}^{k-1}(C)=R^{k}(C), the rank kk locus.

As in the case L1=L2L_{1}=L_{2}, the proof proceeds in a number of steps. We first define and prove the basic properties of Shiffer variations for L1≠L2L_{1}\neq L_{2}. Then one proves a set theoretic equality of the schemes \mboxSecj(C)\mbox{Sec}^{j}(C) and Rj+1R^{j+1}. As before the scheme \mboxSecj(C)\mbox{Sec}^{j}(C) is reduced and includes in Rj+1R^{j+1}, so the only issue is to show that Rj+1R^{j+1} is reduced. The proof proceeds exactly as in the case of L1=L2L_{1}=L_{2}, by showing that one has two resolutions of RpR^{p} that agree scheme theoretically. Finally since deg⁡(L)\deg(L) is very large, one can show the existence of an appropriate factorization of LL so that Theorem 7.4 is true for some choice L1L_{1} and L2L_{2} and one obtains,

We work out an example before doing things in general.

Let L1L_{1} and L2L_{2} be 2 line bundles of degree 2g+12g+1, and let D=p1+p2+p3D=p_{1}+p_{2}+p_{3}, pi∈Cp_{i}\in C. Let s1,s2,s3∈H1(KC⊗L1−1)s_{1},s_{2},s_{3}\in H^{1}\left({K_{C}\otimes L_{1}^{-1}}\right), v1,v2,v3∈H1(C,KC⊗L2−1)v_{1},v_{2},v_{3}\in H^{1}\left({C,K_{C}\otimes L_{2}^{-1}}\right), and t1,t2,t3∈H1(C,KC⊗L1−1⊗L2−1)t_{1},t_{2},t_{3}\in H^{1}\left({C,K_{C}\otimes L_{1}^{-1}\otimes L_{2}^{-1}}\right) be elements representing p1,p2,p3p_{1},p_{2},p_{3}. Recall that for any line bundle MM on CC an element of m∈H1(KC⊗M−1)=H0(M)∨m\in H^{1}\left({K_{C}\otimes M^{-1}}\right)=H^{0}\left({M}\right)^{\vee} represents the point p∈Cp\in C means that that mm kills H0(M(−p))H^{0}\left({M(-p)}\right).

The natural map H0(C,L1)⊗H0(C,L2)⟶H0(C,L1⊗L2)H^{0}\left({C,L_{1}}\right)\otimes H^{0}\left({C,L_{2}}\right)\longrightarrow H^{0}\left({C,L_{1}\otimes L_{2}}\right) dualizes to give a map:

Then as long as char⁡(k)≠2\operatorname{char}(k)\neq 2, ti=μ(si⊗vi)t_{i}=\mu(s_{i}\otimes v_{i}).

The map μ\mu can also be considered as a map

With this description it is clear that μ(si⊗vi)\mu(s_{i}\otimes v_{i}) kills H0(L1(−pi))H^{0}\left({L_{1}(-p_{i})}\right) and has image generated by viv_{i} which is the action of tit_{i}.

h0(Li(−D))=(g+2)−3=g−1h^{0}\left({L_{i}(-D)}\right)=(g+2)-3=g-1, for i=1,2i=1,2.

h0(L1(−D))=g−1h^{0}\left({L_{1}(-D)}\right)=g-1, h0(L2(−D))=gh^{0}\left({L_{2}(-D)}\right)=g.

h0(L1(−D))=h0(L2(−D))=gh^{0}\left({L_{1}(-D)}\right)=h^{0}\left({L_{2}(-D)}\right)=g.

Case (i) is the generic case. Case (ii) can occur if L1=KC(p1+p2+p3)L_{1}=K_{C}(p_{1}+p_{2}+p_{3}), with L2L_{2} general of degree 2g−22g-2. Case (iii) can occur if L1=L2=KC(p1+p2+p3)L_{1}=L_{2}=K_{C}(p_{1}+p_{2}+p_{3}).

This picture generalizes without difficulty. The notation is a bit cumbersome. Let D=∑i=1dnipiD=\sum_{i=1}^{d}n_{i}p_{i} be a divisor of degree dd. Let L1L_{1} and L2L_{2} be line bundles such that

Denote by TL12(D)=∂(H0(C,KC⊗L12−1(D)∣D))⊂H1(C,KC⊗L12−1)T_{L_{12}}(D)=\partial(H^{0}\left({C,K_{C}\otimes L_{12}^{-1}(D)|_{D}}\right))\subset H^{1}\left({C,K_{C}\otimes L_{12}^{-1}}\right).

TL12(D)T_{L_{12}}(D) are the Shiffer variation for (L1,L2)(L_{1},L_{2}) supported on DD.

Cliff⁡(L1;L2,D)=d−rL1(D)−rL2(D)\operatorname{Cliff}(L_{1};L_{2},D)=d-r_{L_{1}}(D)-r_{L_{2}}(D).

Cliff⁡(C,L1;L2)=min⁡{Cliff⁡(L1;L2,D) ∣ rL1(D)>0 or rL2(D)>0}\operatorname{Cliff}(C,L_{1};L_{2})=\min\{\operatorname{Cliff}(L_{1};L_{2},D)\,|\,r_{L_{1}}(D)>0\text{ or }r_{L_{2}}(D)>0\}.

min⁡{Cliff⁡(C,L1),Cliff⁡(C,L2)}≤Cliff⁡(C,L1;L2)\min\{\operatorname{Cliff}(C,L_{1}),\operatorname{Cliff}(C,L_{2})\}\leq\operatorname{Cliff}(C,L_{1};L_{2})

Suppose deg⁡(L1)=deg⁡(L2)\deg(L_{1})=\deg(L_{2}), then Cliff⁡(C,L1,L2)≥d−1\operatorname{Cliff}(C,L_{1},L_{2})\geq d-1, unless L1=L2=KC(D)L_{1}=L_{2}=K_{C}(D), with DD effective or CC is hyperelliptic and L1=KC(D−E1)L_{1}=K_{C}(D-E_{1}), L2=KC(D−E2)L_{2}=K_{C}(D-E_{2}), with E1E_{1}, E2E_{2} both multiples of the g21g^{1}_{2} on CC.

Suppose deg(L1)=deg(L2)≤3g−3deg(L_{1})=deg(L_{2})\leq 3g-3 and L1≠L2L_{1}\neq L_{2} are generic line bundles, then Cliff⁡(C,L1,L2)≥d−1\operatorname{Cliff}(C,L_{1},L_{2})\geq d-1.

Suppose Cliff⁡(C,L1;L2)\operatorname{Cliff}(C,L_{1};L_{2}) is computed by DD. Then if rL1(D)≤rL2(D)r_{L_{1}}(D)\leq r_{L_{2}}(D), then

Follows from (i) and Corollary 3.8 since those are the only cases, for which Cliff⁡(C,L1)\linebreak=d−2\operatorname{Cliff}(C,L_{1})\linebreak=d-2. Notice that if L1=KC(D1)L_{1}=K_{C}(D_{1}) and L2=KC(D2)L_{2}=K_{C}(D_{2}) with D1≠D2D_{1}\neq D_{2} then for example, rL1(D2)=0r_{L_{1}}(D_{2})=0 so that Cliff⁡(C,L1,L2)=d−1\operatorname{Cliff}(C,L_{1},L_{2})=d-1

We must eliminate the cases in (ii) which are possible exceptions. The only case to consider is CC is hyperelliptic and Li=KC(D−Ei)L_{i}=K_{C}(D-E_{i}) where DD computes Cliff⁡(C,L1,L2)\operatorname{Cliff}(C,L_{1},L_{2}). But deg⁡(L1)=deg⁡(L2)\deg(L_{1})=\deg(L_{2}) forces deg⁡(E1)=deg⁡(E2)\deg(E_{1})=\deg(E_{2}) which means that E1=E2E_{1}=E_{2} since the g21g_{2}^{1} is unique on CC. Hence L1=L2L_{1}=L_{2}.

The results about the rank of a matrix in TL12T_{L_{12}}, and the relationship between Rj(C)R^{j}(C) and Sec⁡j−1(C)\operatorname{Sec}^{j-1}(C) are the same as in the case L1=L2L_{1}=L_{2}. We will state the results and sketch the proofs.

Let ξ∈TL12(D)⊂H1(C,KC⊗L12−1)\xi\in T_{L_{12}}(D)\subset H^{1}\left({C,K_{C}\otimes L_{12}^{-1}}\right). Denote by ρ\rho the natural restriction H0(C,L1)⟶H0(C,L1∣D)H^{0}\left({C,L_{1}}\right)\longrightarrow H^{0}\left({C,L_{1}|_{D}}\right). Denote by ∂1:H0(KC⊗L2−1(D)∣D)⟶H1(KC⊗L2−1)\partial_{1}:H^{0}\left({K_{C}\otimes L_{2}^{-1}(D)|_{D}}\right)\longrightarrow H^{1}\left({K_{C}\otimes L_{2}^{-1}}\right) the boundary map in the long exact sequence

and denote by ∂2:H0(KC⊗L12−1(D)∣D)⟶H1(KC⊗L12−1)\partial_{2}:H^{0}\left({K_{C}\otimes L_{12}^{-1}(D)|_{D}}\right)\longrightarrow H^{1}\left({K_{C}\otimes L_{12}^{-1}}\right) the boundary map in the definition of TL12(D)T_{L_{12}}(D). Let ξ~∈H0(C,KC⊗L12−1(D)∣D)\widetilde{\xi}\in H^{0}\left({C,K_{C}\otimes L_{12}^{-1}(D)|D}\right) be an element lifting ξ\xi, i.e. ∂2(ξ~)=ξ\partial_{2}(\widetilde{\xi})=\xi. Then ∪ξ:H0(C,L1)⟶H1(C,KC⊗L2−1)\cup\xi:H^{0}\left({C,L_{1}}\right)\longrightarrow H^{1}\left({C,K_{C}\otimes L_{2}^{-1}}\right) factors as:

The proof is exactly the same. Pick an affine open cover of CC by V1V_{1} such that V1⊃DV_{1}\supset D and V2=C−DV_{2}=C-D. If one uses this Cěch cover to compute the cup product then ξ∈Γ(V1∩V2,KC⊗L1−1⊗L2−1)\xi\in\Gamma\left(V_{1}\cap V_{2},K_{C}\otimes L_{1}^{-1}\otimes L_{2}^{-1}\right) is given by ξ^\hat{\xi} where ξ^\hat{\xi} is a lifting of ξ~\widetilde{\xi} to Γ(V1∩V2,Kc⊗L1−1⊗L2−1)\Gamma\left(V_{1}\cap V_{2},K_{c}\otimes L_{1}^{-1}\otimes L_{2}^{-1}\right). So given s1∈H0(C,L1)s_{1}\in H^{0}\left({C,L_{1}}\right), s1∪ξs_{1}\cup\xi is represented by s1⋅ξ∈Γ(V1∩V2,KC⊗L2−1)s_{1}\cdot\xi\in\Gamma\left(V_{1}\cap V_{2},K_{C}\otimes L_{2}^{-1}\right) which is ∂1(ξ~⋅s1)\partial_{1}(\widetilde{\xi}\cdot s_{1}). ∎

This follows from Theorem 4.1 and the above description. ∎

The next theorem calculates the rank of an element τ∈TL12(D)\tau\in T_{L_{12}}(D). Suppose that rL2(D)=r2≥rL1(D)=r1r_{L_{2}}(D)=r_{2}\geq r_{L_{1}}(D)=r_{1}.

The condition that ξ∈TL12∗(D)\xi\in T_{L_{12}}^{*}(D) is: write D=∑i=1nnipiD=\sum_{i=1}^{n}n_{i}p_{i} and choose ziz_{i} a local parameter at pip_{i}, then we can write a lifting of ξ\xi to H0(KC⊗L1−1⊗L2−1(D)∣D)H^{0}\left({K_{C}\otimes L_{1}^{-1}\otimes L_{2}^{-1}(D)|_{D}}\right) as ξ~=∑i=1n(∑j=1niβijzij)\widetilde{\xi}=\sum_{i=1}^{n}\left(\sum_{j=1}^{n_{i}}\beta_{ij}z_{i}^{j}\right) with βi,ni≠0\beta_{i,n_{i}}\neq 0 for 1≤i≤n1\leq i\leq n. By cor 7.9 im⁡(ξ)⊂SL(D)\operatorname{im}(\xi)\subset S_{L}(D), which is a linear space of dimension d−r2d-r_{2} . This gives the upper bound. ∪ξ~\cup\widetilde{\xi} is an isomorphism by the same argument as in Theorem 4.6 so we are done by the following algebraic fact. ∎

Let φ:V1⟶V2\varphi:V_{1}\longrightarrow V_{2} be a linear isomorphism between two vector spaces of dimension dd. Let W1⊂V1W_{1}\subset V_{1} be a subspace of codimension r1r_{1} and let V2⟶W2V_{2}\longrightarrow W_{2} be a surjection onto a space of dimension d−r2d-r_{2}. Then φ‾:W1⟶W2\overline{\varphi}:W_{1}\longrightarrow W_{2} has rank ≥d−r1−r2\geq d-r_{1}-r_{2}.

Because φ\varphi is an isomorphism, φ‾1:W1⟶V2\overline{\varphi}_{1}:W_{1}\longrightarrow V_{2} has rank d−r1d-r_{1} and p:V2⟶W2p:V_{2}\longrightarrow W_{2} has kernel of rank r2r_{2}. ker⁡(p∘φ‾1)⊂ker⁡(p)\operatorname{ker}\left(p\circ\overline{\varphi}_{1}\right)\subset\ker(p) since φ‾1\overline{\varphi}_{1} is injective and hence dim⁡(ker⁡φ‾)≤r2\dim\left(\ker\overline{\varphi}\right)\leq r_{2} and so rk⁡(φ‾)=rk⁡(φ‾1)−dim⁡ker⁡(p∘φ‾1)≥d−r1−r2\operatorname{rk}\left(\overline{\varphi}\right)=\operatorname{rk}\left(\overline{\varphi}_{1}\right)-\dim\ker\left(p\circ\overline{\varphi}_{1}\right)\geq d-r_{1}-r_{2}. ∎

We next show set-theoretic equality of the appropriate secant varieties and rank-loci. Having established the generalized notation, the proofs go exactly as in the case of L1=L2L_{1}=L_{2}. Recall our setup

Suppose Cliff⁡(C,L1,L2)=c≥2\operatorname{Cliff}(C,L_{1},L_{2})=c\geq 2. Then, as sets, Sec⁡j−1(C)=Rj\operatorname{Sec}^{j-1}(C)=R^{j} for j<cj<c.

The proof is essentially identical to the case L1=L2L_{1}=L_{2}. For completeness we give details.

Since dim⁡(Sec⁡j(C))=2j+1\dim\left(\operatorname{Sec}^{j}(C)\right)=2j+1,

for k≥h0(C,L12)+12k\geq\frac{h^{0}\left({C,L_{12}}\right)+1}{2}. In other words, every element can be written as a Shiffer variation in some TL12(D)T_{L_{12}}(D) for some DD of degree kk. Let

be the elements of maximal rank. Set r1=rL1(D)r_{1}=r_{L_{1}}(D) and r2=rL2(D)r_{2}=r_{L_{2}}(D). By Theorem 7.10, if t∈TL12∗(D)t\in T^{*}_{L_{12}}(D),

If r1=r2=0r_{1}=r_{2}=0, then rk⁡(t)=d\operatorname{rk}(t)=d. That is t∈\mboxSecd−1(C)t\in\mbox{Sec}^{d-1}(C) as desired. We have r1=r2=0r_{1}=r_{2}=0 for deg⁡(D)<c\deg(D)<c. Further, if r1>0r_{1}>0 or r2>0r_{2}>0, then d−r1−r2≥cd-r_{1}-r_{2}\geq c so any t∈H1(KC⊗L1−1⊗L2−1)t\in H^{1}\left({K_{C}\otimes L_{1}^{-1}\otimes L_{2}^{-1}}\right) with rk⁡(t)<c\operatorname{rk}(t)<c can be written as the sum of rk⁡(t)\operatorname{rk}(t) matrices of rank 1. This is the statement Sec⁡j−1(C)=Rj\operatorname{Sec}^{j-1}(C)=R^{j} for j<cj<c. ∎

Finally we need to check that the set theoretic equality is a scheme theoretic equality.

Sec⁡j−1(C)=Rj\operatorname{Sec}^{j-1}(C)=R^{j} as schemes for j<cj<c.

Sec⁡j−1(C)\operatorname{Sec}^{j-1}(C) is normal and smooth away from Sec⁡j−2(C)\operatorname{Sec}^{j-2}(C) with tangent space generated by the span of the divisor 2D2D for qq a general point in the span of DD. The exact same proof holds.

By exactly the same argument as in Lemma 6.2 we get an inclusion of schemes: \mboxSecp−1↪RP\mbox{Sec}^{p-1}\hookrightarrow R^{P} .

and the fibers are linear spaces. Since p<Cliff⁡(C,L1,L2)p<\operatorname{Cliff}(C,L_{1},L_{2}), we can identify R~p\widetilde{R}^{p} with the incidence correspondence defining the full secant variety,Bp−1(L12)B^{p-1}(L_{12}). Again as in the case L1=L2L_{1}=L_{2} it follows that the projections are the same and that \mboxSecp−1(C)=Rp\mbox{Sec}^{p-1}(C)=R^{p}.

Since \mboxSecp−1=RP\mbox{Sec}^{p-1}=R^{P} as schemes they have the same tangent spaces at all points. We present an independent calculation of the tangent space to RpR^{p} at a smooth point, which is to say, at a point of rank exactly pp

Let p<Cliff⁡(C,L)p<\operatorname{Cliff}(C,L) φ∈Rp∖Rp−1\varphi\in R^{p}\setminus R^{p-1}, so φ∈TL12∗(D)\varphi\in T_{L_{12}}^{*}(D) for some DD of degree pp. The tangent space Tφ,RpT_{\varphi,R_{p}} is the projectivization of

Let T~⊂H1(KC⊗L1−1⊗L2−1)\widetilde{T}\subset H^{1}\left({K_{C}\otimes L_{1}^{-1}\otimes L_{2}^{-1}}\right) be the cone over Tφ,RpT_{\varphi,R^{p}}. Then T~\widetilde{T} is the tangent space to the affine rank pp locus. For φ∈Rp∖Rp−1\varphi\in R^{p}\setminus R^{p-1} this tangent space is described in (() see page 68) as the matrices which map the kernel of φ\varphi into the image of φ\varphi. That is to say: T~={ψ∈H1(KC⊗L1−1⊗L2−1)∣ψ:ker⁡φ⟶im⁡φ}\widetilde{T}=\left\{\psi\in H^{1}\left({K_{C}\otimes L_{1}^{-1}\otimes L_{2}^{-1}}\right)|\psi:\ker\varphi\longrightarrow\operatorname{im}\varphi\right\}. But, ker⁡φ=H0(C,L1(−D))\ker\varphi=H^{0}\left({C,L_{1}(-D)}\right) and im⁡φ=({x∈H1(KC⊗L1−1)∣x∣H0(L(−D))=0}\operatorname{im}\varphi=\left(\{x\in H^{1}\left({K_{C}\otimes L_{1}^{-1}}\right)|x|_{H^{0}\left({L(-D)}\right)}=0\right\} so

is injective or by Serre duality (and using Hom⁡(A∨,B)=A⊗B\operatorname{Hom}(A\vee,B)=A\otimes B) that

is surjective, which is true since deg⁡(Li(−D))≥2g−1\deg(L_{i}(-D))\geq 2g-1. ∎

RpR^{p} is smooth at φ∈Rp∖Rp−1\varphi\in R^{p}\setminus R^{p-1}

Since p<Cliff⁡(C,L)p<\operatorname{Cliff}(C,L) by the above argument Tφ,Rp=TL12(D)T_{\varphi,R^{p}}=T_{L_{12}}(D) which is of dimension 2p+12p+1. ∎

This concludes the proof of Theorem 7.4, since for any factorization L=L1⊗L2L=L_{1}\otimes L_{2} with deg⁡(Li)≥2g+1+k\deg(L_{i})\geq 2g+1+k one has Cliff⁡(C,Li)≥k+1\operatorname{Cliff}(C,L_{i})\geq k+1. For the case L1=L2L_{1}=L_{2} the result is sharp. By Lemma 5.5 we can for L1=L2=L=KC(D)L_{1}=L_{2}=L=K_{C}(D) find an element τ∈TL12∗(D)\tau\in T_{L_{12}}^{*}(D) with d−2=rk⁡(τ)<deg⁡(τ)=d−1d-2=\operatorname{rk}(\tau)<\deg(\tau)=d-1. In the language of Theorem 7.4 d=k+3d=k+3 and Cliff⁡(C,L)=k+1\operatorname{Cliff}(C,L)=k+1. In particular, for k=0k=0 this gives a weaker result than 7.1, the result proved in (). However, the theorem can be ’tweaked’ to get,

If L1≠L2L_{1}\neq L_{2},but deg⁡(Li)≥2g+k+1\deg(L_{i})\geq 2g+k+1 , then \mboxSecj(C)=Rj\mbox{Sec}^{j}(C)=R^{j} for j≤(k+1)j\leq(k+1) then

By Proposition 7.7 (iii) we have Cliff⁡(C,L1,L2)≥k+2\operatorname{Cliff}(C,L_{1},L_{2})\geq k+2 .The lemma follows from Theorem 7.13 ∎

Throughout this section we will write L=KC(−P)L=K_{C}(-P), where PP is an effective divisor of degree p<c=Cliff⁡(C)p<c=\operatorname{Cliff}(C). Since deg⁡(P)<c\deg(P)<c, h0(OC(P))=1h^{0}\left({\mathcal{O}_{C}(P)}\right)=1 (else Cliff⁡(C)≤p−2\operatorname{Cliff}(C)\leq p-2), so h1(L)=h0(KC⊗L−1)=h0(OC(P))=1h^{1}\left({L}\right)=h^{0}\left({K_{C}\otimes L^{-1}}\right)=h^{0}\left({\mathcal{O}_{C}(P)}\right)=1. This is the only case we will discuss as it is the only situation in which I can say something meaningful about Cliff⁡(C,L)\operatorname{Cliff}(C,L).

Suppose that L=KC(−P)L=K_{C}(-P) with deg⁡(P)=p<c\deg(P)=p<c then

Cliff⁡(L,D)=Cliff⁡(D+P)−p\operatorname{Cliff}(L,D)=\operatorname{Cliff}(D+P)-p.

c−p≤Cliff⁡(C,L)≤cc-p\leq\operatorname{Cliff}(C,L)\leq c.

Cliff⁡(C,L)=c−p\operatorname{Cliff}(C,L)=c-p, except possibly in the case where Cliff⁡(C)=[g−12]\operatorname{Cliff}(C)=[\frac{g-1}{2}] and p=Cliff⁡(C)−1p=\operatorname{Cliff}(C)-1

First notice that rL(D)=rKC(D+P)r_{L}(D)=r_{K_{C}}(D+P) since

Suppose DD computes Cliff⁡(C)\operatorname{Cliff}(C) and deg⁡(D)<[g−12]\deg(D)<[\frac{g-1}{2}]. Consider the divisor L(−D)L(-D). It is effective except possibly in the case when Cliff⁡(C)=[g−12]\operatorname{Cliff}(C)=[\frac{g-1}{2}] and p=Cliff⁡(C)−1p=\operatorname{Cliff}(C)-1. By 1, Cliff⁡(C,L(−D))=c−p\operatorname{Cliff}(C,L(-D))=c-p.

Remark: In general I would not expect it to be the case these divisors give rise to Shiffer variations of low rank. This is in complete analogy to the fact that a curve being non-arithmetically normal gives rise to a divisor of degree 2n+22n+2, spanning nn planes, but the existence of an 2n+22n+2 pointed nn plane do not necessarily imply that the embedding is not arithmetically normal.

Remark: We postpone the discussion of the possible pathology that can occur until after our one positive result.

Notice that when L=KC(−P)L=K_{C}(-P), LL is always very ample. If DD was a divisor of degree 2 such that h0(L(−D))≥h0(L)−1h^{0}\left({L(-D)}\right)\geq h^{0}\left({L}\right)-1, then h1(L(−D))≥2h^{1}\left({L(-D)}\right)\geq 2, and hence Cliff⁡(P+D)≤p+2−2=p<Cliff⁡(C)\operatorname{Cliff}(P+D)\leq p+2-2=p<\operatorname{Cliff}(C). Since

P+DP+D is eligible to compute Cliff⁡(C)\operatorname{Cliff}(C), and we would have a contradiction since p<cp<c.

To apply our standard setup we need to know that LL is quadratically normal. This is a special case of a theorem of Green and Lazarsfeld proven in

Suppose LL is very ample with deg⁡(L)≥2g+1−2h1(L)−Cliff⁡(C)\deg(L)\geq 2g+1-2h^{1}\left({L}\right)-\operatorname{Cliff}(C), then LL is projectively normal.

In our case h1(L)=1h^{1}\left({L}\right)=1 and deg⁡(L)=2g−2−p>2g−2−Cliff⁡(C)\deg(L)=2g-2-p>2g-2-\operatorname{Cliff}(C). We will actually give a proof of the theorem, as the use of Shiffer deformation and Clifford index gives (to us!) a conceptual proof of the theorem. As [G-L] points out, cubic and higher normality follow from the base-point-free pencil trick and the only issue is to prove quadratic normality.

A simple argument will show that the failure of quadratic normality implies the existence of a divisor of Clifford index zero. From our point of view it is natural to restate the inequality of the theorem as

This makes clear the basic idea, the only way to get a divisor of Clifford index zero is as the “projection” from a plane of dimension (c−1)(c-1) of a divisor of Clifford index cc. This is the geometry behind the proof. Incidentally one can check that the inequality of the theorem implies h1(L)≤1h^{1}\left({L}\right)\leq 1.

Firstly, if LL is not quadratically normal, then the map

is not injective. If ξ∈H1(KC⊗L−2)\xi\in H^{1}\left({K_{C}\otimes L^{-2}}\right) is in the kernel of this map, then, viewing ξ\xi as a matrix in Hom⁡(H0(L),H1(KC⊗L−1))\operatorname{Hom}(H^{0}\left({L}\right),H^{1}\left({K_{C}\otimes L^{-1}}\right)) we have rk⁡(ξ)=0\operatorname{rk}(\xi)=0. Viewing ξ\xi as a Shiffer variation, there is a divisor DD on CC such that ξ∈TL(D)\xi\in T_{L}(D) and setting d=deg⁡(D)d=\deg(D), r=rL(D)r=r_{L}(D), we have d−2r≤0d-2r\leq 0. Adding points to DD if necessary we have a divisor DD such that Cliff⁡(L,D)=0\operatorname{Cliff}(L,D)=0.

We consider separately the cases of h1(L)=0h^{1}\left({L}\right)=0 and h1(L)=1h^{1}\left({L}\right)=1. If h1(L)=1h^{1}\left({L}\right)=1, L=KC(−P)L=K_{C}(-P), where PP is a divisor of degree pp and our inequality is that p<c=Cliff⁡(C)p<c=\operatorname{Cliff}(C). Cliff⁡(L,D)=0\operatorname{Cliff}(L,D)=0 means d−2rL(D)=0d-2r_{L}(D)=0 and rL(D)=h0(OC(D+P))−1=d2r_{L}(D)=h^{0}\left({\mathcal{O}_{C}(D+P)}\right)-1=\frac{d}{2}, and hence Cliff⁡(KC,OC(D+P))=d+p−2(d2)=p<c\operatorname{Cliff}(K_{C},\mathcal{O}_{C}(D+P))=d+p-2\left(\frac{d}{2}\right)=p<c. Thus D+PD+P cannot be used to compute Cliff⁡(C)\operatorname{Cliff}(C) and hence must span a hyperplane. That is, h0(KC(−D−P))=1h^{0}\left({K_{C}(-D-P)}\right)=1 and so Cliff⁡(KC(−D−P)=deg⁡(KC(−D−P)\operatorname{Cliff}(K_{C}(-D-P)=\deg(K_{C}(-D-P) . But then

and hence Cliff⁡(L,D)=Cliff⁡(OC(D+P)−p>Cliff⁡(C)−p>0\operatorname{Cliff}(L,D)=\operatorname{Cliff}(\mathcal{O}_{C}(D+P)-p>\operatorname{Cliff}(C)-p>0. This is a contradiction.

So Cliff⁡(E)≥g+12≥Cliff⁡(C)\operatorname{Cliff}(E)\geq\frac{g+1}{2}\geq\operatorname{Cliff}(C) and so

Suppose LL is very ample, deg⁡(L)=2g\deg(L)=2g and LL is not arithmetically normal. Then CC is hyperelliptic.

From the proof of the theorem we see that deg⁡(L)=2g\deg(L)=2g implies e−2r=0e-2r=0. By Clifford’s theorem, after easily ruling out the cases of E=OCE=\mathcal{O}_{C} or KCK_{C}, we see that CC is hyperelliptic and EE is a multiple of the g21g^{1}_{2} on CC.

When L=KCL=K_{C} we have seen that Cliff⁡(C)\operatorname{Cliff}(C) characterizes on the nose the degree to which secant varieties are rank loci. For L=KC(−P)L=K_{C}(-P) this is no longer true. We can always guarantee the same bound, but unlike for LL with h1(L)=0h^{1}\left({L}\right)=0 or L=KCL=K_{C}, the existence of a divisor with Cliff⁡(L,D)=c\operatorname{Cliff}(L,D)=c does not seem to imply there exists a ξ∈TL(D)\xi\in T_{L}(D) with rk⁡(ξ)=Cliff⁡(L,D)\operatorname{rk}(\xi)=\operatorname{Cliff}(L,D). Nonetheless, the more important lower bound always holds. Consider the standard diagram:

Suppose j<Cliff⁡(C,L)j<\operatorname{Cliff}(C,L); then Rj(C)=Sec⁡j−1(C)R^{j}(C)=\operatorname{Sec}^{j-1}(C) as sets.

We use the same argument as before in the case L=KCL=K_{C}. As in the proof of the quadratic normality, any ξ∈H1(KC⊗L−2)\xi\in H^{1}\left({K_{C}\otimes L^{-2}}\right) can be written as ξ∈TL(D)\xi\in T_{L}(D) where deg⁡(D)≤(3g−5)/2−p\deg(D)\leq(3g-5)/2-p. If DD is eligible to compute Cliff⁡(C,L)\operatorname{Cliff}(C,L) then Cliff⁡(L,D)≥Cliff⁡(C,L)\operatorname{Cliff}(L,D)\geq\operatorname{Cliff}(C,L). If DD is not eligible to compute Cliff⁡(C,L)\operatorname{Cliff}(C,L) then either rL(D)=0r_{L}(D)=0 or h1(L(−D))≤1h^{1}\left({L(-D)}\right)\leq 1. In the first case, ξ∈\mboxSecd−1(C)∖Sec⁡d−2(C)\xi\in\mbox{Sec}^{d-1}(C)\setminus\operatorname{Sec}^{d-2}(C). In the later case we may assume rL(D)>0r_{L}(D)>0. Again exactly as in the proof of quadratic normality theorem and recalling KC⊗L−1=OC(P)K_{C}\otimes L^{-1}=\mathcal{O}_{C}(P) we see that

Scheme theoretic equality should follow exactly as in the cases of L=KCL=K_{C} or h1(L)=0h^{1}\left({L}\right)=0. I have not checked the details.

2. In case L=KCL=K_{C} the existence of ξ\xi with rk⁡(ξ)=Cliff⁡(C)\operatorname{rk}(\xi)=\operatorname{Cliff}(C) was delicate. If DD computed Cliff⁡(C)\operatorname{Cliff}(C) one could find an η∈H0(KC(−D)\eta\in H^{0}\left({K_{C}(-D}\right) such that there was a τ∈TKC(D)\tau\in T_{K_{C}}(D) with the property that τ\tau vanished on 1⊗H0(KC(−D))1\otimes H^{0}\left({K_{C}(-D)}\right) as well as vanishing on fi⊗η1f_{i}\otimes\eta_{1} for 1<i≤n1<i\leq n and so rk⁡(τ)=Cliff⁡(D)=Cliff⁡(C)\operatorname{rk}(\tau)=\operatorname{Cliff}(D)=\operatorname{Cliff}(C).

If DD computes Cliff⁡(C)\operatorname{Cliff}(C) then KC(−D)K_{C}(-D) is base point free and that is the key point.

In the case L=KC(−P)L=K_{C}(-P) it is the twisted linear system, KC⊗L−1(D)K_{C}\otimes L^{-1}(D), not OC(D)\mathcal{O}_{C}(D) which comes into play. One needs the base point freeness of L⊗2⊗KC−1(−D)=L(−D−P)L^{\otimes 2}\otimes K_{C}^{-1}(-D)=L(-D-P).

In the case of the divisor used to compute Cliff⁡(C,L)\operatorname{Cliff}(C,L) being D=L(−E)D=L(-E) where EE computes Cliff⁡(C)\operatorname{Cliff}(C) and deg⁡(E)\deg(E) small, L⊗2⊗KC−1(−D)=E−PL^{\otimes 2}\otimes K_{C}^{-1}(-D)=E-P which satisfies h0(OC(E−P))<1h^{0}\left({\mathcal{O}_{C}(E-P)}\right)<1. I cannot provide a proof, but I think that these divisors do not give rise to Shiffer variations τ\tau, satisfying rk⁡(τ)=Cliff⁡(L,D)\operatorname{rk}(\tau)=\operatorname{Cliff}(L,D). I suspect that on a general line bundle L=KC(−P)L=K_{C}(-P) that \mboxSecj−1(C)=Rj\mbox{Sec}^{j-1}(C)=R^{j} for j≤Cliff⁡(C)−2j\leq\operatorname{Cliff}(C)-2 as opposed to holding for j≤Cliff⁡(C)−p−1j\leq\operatorname{Cliff}(C)-p-1. The moral is that projecting from a general point should not affect the Clifford index, but projection from special points should. Here is a small positive result.

Suppose deg⁡(E)<(g−1)\deg(E)<(g-1), h0(OC(E))≥2h^{0}\left({\mathcal{O}_{C}(E)}\right)\geq 2. Suppose , L(−E)L(-E) is base point free, h0(OC(E−P))=1h^{0}\left({\mathcal{O}_{C}(E-P)}\right)=1 and deg⁡(P)<Cliff⁡(C)\deg(P)<\operatorname{Cliff}(C). Let D=E−PD=E-P, L=KC(−P)L=K_{C}(-P). Then

Cliff⁡(L,D)=Cliff⁡(E)−p\operatorname{Cliff}(L,D)=\operatorname{Cliff}(E)-p.

There exists a Shiffer variation ξ\xi, of rank c=Cliff⁡(L,D)c=\operatorname{Cliff}(L,D), but such that ξ∉\mboxSecc−1(C)\xi\notin\mbox{Sec}^{c-1}(C).

Since KC⊗L−1(D)=EK_{C}\otimes L^{-1}(D)=E, Cliff⁡(L,D)=Cliff⁡(E)−p\operatorname{Cliff}(L,D)=\operatorname{Cliff}(E)-p. By degree considerations DD cannot span a hyperplane and rL(D)=rKC(E)r_{L}(D)=r_{K_{C}}(E)

L(−E)L(-E) is base point free so the same argument as for L=KCL=K_{C} works. We can find η∈H0(L(−E))\eta\in H^{0}\left({L(-E)}\right) which vanishes on exactly EE. If {1,f1,…,fn}\{1,f_{1},\dots,f_{n}\} is a basis for H0(OC(E))H^{0}\left({\mathcal{O}_{C}(E)}\right) then since E−D=PE-D=P and any Shiffer variations in TL(D)T_{L}(D) kills H0(L(−D))⊃H0(L(−E))H^{0}\left({L(-D)}\right)\supset H^{0}\left({L(-E)}\right) and η⊗fi\eta\otimes f_{i} are not in H0(L(−D))H^{0}\left({L(-D)}\right) and killed by some τ∈TL(D)\tau\in T_{L}(D), specifically by τ=∑pi∈Dτpi\tau=\sum_{p_{i}\in D}\tau_{p_{i}}.

Remark: I believe that one should have L(−E)L(-E) base point free always when deg⁡(E)<g−1\deg(E)<g-1 and EE computes Cliff⁡(C)\operatorname{Cliff}(C). I do not have a proof.

In general the technique will fail since L(−E)L(-E) need not be base point free. To produce this example, we also give an example of a divisor not in the Petri locus. That is a curve CC and a divisor DD such that (r+1)(g−d+r)>g(r+1)(g-d+r)>g but the Petri map is not surjective. After conversations with L. Ein and I. Coskun it is clearly not hard to find such examples. I do not know of examples in the literature though. Firstly we prove:

Suppose DD is base point free. The following two assertions are equivalent:

The Petri map H0(OC(D))⊗H0(KC(−D))⟶H0(KC)H^{0}\left({\mathcal{O}_{C}(D)}\right)\otimes H^{0}\left({K_{C}(-D)}\right)\longrightarrow H^{0}\left({K_{C}}\right) is not surjective.

The natural map H0(OC(D))⊗H0(OC(D))⟶H0(OC(2D))H^{0}\left({\mathcal{O}_{C}(D)}\right)\otimes H^{0}\left({\mathcal{O}_{C}(D)}\right)\longrightarrow H^{0}\left({\mathcal{O}_{C}(2D)}\right) is not surjective.

Now by the base point free pencil trick c.f. [ACGH, p126] we have an exact sequence:

and mm is the Petri map. So h0(m)h^{0}\left({m}\right) is not surjective if and only if h1(ι)h^{1}\left({\iota}\right) is not injective if and only if (by Serre duality) H0(OC(D))⊕2⟶H0(OC(2D))H^{0}\left({\mathcal{O}_{C}(D)}\right)^{\oplus 2}\longrightarrow H^{0}\left({\mathcal{O}_{C}(2D)}\right) is not surjective. ∎

I speculate that the curves carrying a gn1g^{1}_{n} such that the Petri map is not surjective will be represented by a cohomology class in Mg,nM_{g,n} that is not an intersection of divisors or in the cohomology ring of ordinary Brill-Noether loci.

Suppose CC is any curve with a gn1g^{1}_{n} (n≥4n\geq 4), call it FF, and such that h0(OC(2F))=5h^{0}\left({\mathcal{O}_{C}(2F)}\right)=5. Let ∑i=1nPi∈∣F∣\sum_{i=1}^{n}P_{i}\in|F|, and set P=∑i=1n−3PiP=\sum_{i=1}^{n-3}P_{i}, D=∑i=n−2nPiD=\sum_{i=n-2}^{n}P_{i}, and L=KC(−P)L=K_{C}(-P). Then in general LL will be very ample and if LL is very ample, h0(L)=g−n+3h^{0}\left({L}\right)=g-n+3, h0(L(−D))=g−n+1h^{0}\left({L(-D)}\right)=g-n+1, so DD spans a 3-secant line.

By construction h0(KC(−F−P))=g−2n+4=h0(KC(−2E))h^{0}\left({K_{C}(-F-P)}\right)=g-2n+4=h^{0}\left({K_{C}(-2E)}\right), so L(−F)L(-F) has base points on DD, and hence the map

lands in H0(L(−D))H^{0}\left({L(-D)}\right). For such a curve and linear system, the method of construction of Shiffer variations used in the case of L=KCL=K_{C} won’t work!

We now construct such CC and FF. We merely iterate the previous construction. Namely on CC we have the linear system g∗(O(1))g^{*}(\mathcal{O}(1)), which is of degree 32. We take the 4-fold cyclic cover of CC branched on g∗(O(1))g^{*}(\mathcal{O}(1)) , call this C2C_{2}. By Hurwitz formula we calculate g(C2)=4(16)+3(32)2+1=81g(C_{2})=\frac{4(16)+3(32)}{2}+1=81. Let ff be the composed map,

so setting F=f∗(O(1))F=f^{*}(\mathcal{O}(1)) we see that h0(OC(F))=2h^{0}\left({\mathcal{O}_{C}(F)}\right)=2, h0(OC(2F))=5h^{0}\left({\mathcal{O}_{C}(2F)}\right)=5. Since FF is a g161g^{1}_{16} we get H0(KC(−F))=81−16+1=66H^{0}\left({K_{C}(-F)}\right)=81-16+1=66, and h0(KC(−2F))\linebreak=81−32+4=53h^{0}\left({K_{C}(-2F)}\right)\linebreak=81-32+4=53. In particular, FF imposes 13 conditions on the linear system KC(−F)K_{C}(-F). Take F=∑i=116PiF=\sum_{i=1}^{16}P_{i} and P=∑i=113PiP=\sum_{i=1}^{13}P_{i}, such that PP imposes independent conditions on KC(−F)K_{C}(-F). Let L=KC(−P)L=K_{C}(-P). LL is very ample because if not there would be a divisor AA of degree 2, such that h0(OC(F−P+A))=2h^{0}\left({\mathcal{O}_{C}(F-P+A)}\right)=2. This would mean these 15 points are linearly dependent. Exactly as in the case of showing KCK_{C} is very ample, the 15 points cannot lie on one fiber, and if they lie on different fibers, they clearly are linearly independent. This completes the proof.

While pathological behavior occurs, the generic case is fine. For example, we have seen that if rL(D)=1r_{L}(D)=1, for simple linear algebra reasons we can construct a τ∈TL(D)\tau\in T_{L}(D) with rk⁡(τ)=Cliff⁡(L,D)=d−2\operatorname{rk}(\tau)=\operatorname{Cliff}(L,D)=d-2. So if D computes Cliff⁡(C,L)\operatorname{Cliff}(C,L) we can construct a Shiffer variation of rank equal to Cliff⁡(C,L)\operatorname{Cliff}(C,L).

Connections with Koszul Cohomology and Green’s Conjecture

The standard reference for Koszul cohomology is . However I have also profited from reading , , and . We will not define these groups in their greatest generality. We begin by reviewing with brief proofs some of the basic facts about Koszul cohomology. We will assume throughout that k is an algebraically closed field of characteristic ≠2,3\neq 2,3.

Let W be a vector space over k and let S=⨁k=0∞Sym⁡k(W)S=\bigoplus_{k=0}^{\infty}\operatorname{Sym}^{k}(W) be the symmetric algebra. Thus k is the quotient of S by the irrelevant ideal. Let M=⨁q=o∞MqM=\bigoplus_{q=o}^{\infty}M^{q} be a graded S module. Define

One checks that δ2=0\delta^{2}=0 by a direct computation. Therefore we get a complex and we can compute cohomology.

The Koszul cohomology group Kp,q(S,M)K_{p,q}(S,M) is the cohomology of the complex:

The most common case is when W=H0(C,L)W=H^{0}\left({C,L}\right) and Mq=H0(C,L⊗q)M^{q}=H^{0}\left({C,L^{\otimes q}}\right). In that case we will denote the Koszul cohomology group as Kp,q(C,L)K_{p,q}(C,L). Koszul cohomology groups are useful because they can be used to compute free resolutions of graded modules over S. For completeness we include a brief description of this phenomena. The information can be found in any of the sources mentioned above, as well as Eisenbuds book,’Commutative Algebra’ .

A free resolution F\mbox\textbulletF^{\mbox{\textbullet}} of M is an exact sequence of the form:

The maps Fi+1⟶FiF_{i+1}\longrightarrow F_{i} are given by a matrix of homogenous polynomials, call it fif_{i}. The most important case is when the maps are given by non constant polynomials.

A free resolution is said to be minimal if all the matrices fif_{i} contain no non-zero constant terms.

Let M=∑i=0i=∞MiM=\sum_{i=0}^{i=\infty}M_{i} be a graded S module with a free resolution F\mbox\textbulletF^{\mbox{\textbullet}} with Fp=∑q(Vp,q⊗S(−q))F_{p}=\sum_{q}(V_{p,q}\otimes S(-q)): ie Vp,qV_{p,q} is a vector space that keeps track of how many S(−q)S(-q)’s appear in FpF_{p}.

The proof of this is well known and in all the above sources. I will sketch it for the sake of completeness. Firstly one has the Koszul resolution of k:

One can tensor this resolution with M and one sees by inspection that the maps are the boundary maps δ\delta from equation 7. Hence one has Kp,q(S,M)K_{p,q}(S,M) = Torpp+q(M,k)Tor_{p}^{p+q}(M,k). On the other hand, we can take the free resolution F\mbox\textbulletF^{\mbox{\textbullet}} of MM and tensor it with k (viewed as the quotient of S by its maximal ideal). By the commutivity of Tor, this gives the same answer as above. On the other hand, since F\mbox\textbulletF^{\mbox{\textbullet}} is minimal, when we tensor with k all the boundary maps are zero and hence we get Vp,p+q⊗SV_{p,p+q}\otimes S is the degree p+qp+q piece of FpF_{p}. ∎

To relate our work to Koszul cohomology we introduce some new notation. This is needed as we are going to work with the dual of the Koszul complex. This is the complex which, term by term, is the vector space dual of the Koszul complex. There is another notion of a dual Koszul complex which involves divided powers (see the appendix to for details). As long as char(k) is sufficiently large, these are the same. The reason we do this is that our Shiffer variations live naturally in the dual of the Koszul complex we describe .

Let V=W∗V=W^{*}, W=H0(C,L)W=H^{0}\left({C,L}\right) where L is a very ample line bundle. We denote by MiM_{i} the dual of H0(C,L⊗i)H^{0}\left({C,L^{\otimes i}}\right) so that M1=V.M_{1}=V.

We also assume that the line bundle L is quadratically normal which means that M2↪Sym⁡2(V)M_{2}\hookrightarrow\operatorname{Sym}^{2}(V) is injective. We frequently consider φ∈M2\varphi\in M_{2} as an element of Sym⁡2(V)\operatorname{Sym}^{2}(V) or equivalently as an element of Hom⁡\mboxsym(W,V)\operatorname{Hom}^{\mbox{s}ym}(W,V).

The Koszul cohomology group can be calculated as the cohomology of:

and so the dual cohomology groups are calculated by the complex:

We are generally only interested in determining if these groups are zero or non-zero, so calculating the dual group is good enough. Any v=φ⊗λ∈M2⊗⋀p(V)v=\varphi\otimes\lambda\in M_{2}\otimes\bigwedge^{p}(V) can be viewed as an element of Hom⁡(⋀p(W),M2)\operatorname{Hom}(\bigwedge^{p}(W),M_{2}) and δ(v)\delta(v) as an element of Hom⁡(⋀p+1(W),V)\operatorname{Hom}(\bigwedge^{p+1}(W),V). If w∈⋀p+1(W)w\in\bigwedge^{p+1}(W) then δ(v)(w)\delta(v)(w) is calculated by first contracting λ∧w\lambda\wedge w via the standard map ⋀p(V)⊗⋀p+1(W)⟶W\bigwedge^{p}(V)\otimes\bigwedge^{p+1}(W)\longrightarrow W (recall that W and V are dual) and then letting φ\varphi act on λ∧ν\lambda\wedge\nu.

Let φ∈M2\varphi\in M_{2} and let λ∈⋀p(V)\lambda\in\bigwedge^{p}(V) be decomposable. If Im(φ)⊂λIm(\varphi)\subset\lambda, then δ(φ⊗λ)=0\delta(\varphi\otimes\lambda)=0.

By λ\lambda decomposable we mean that λ=v1∧⋯∧vp\lambda=v_{1}\wedge\dots\wedge v_{p} and hence defines a subspace Vp⊂VV_{p}\subset V. We mean that viewing φ\varphi as an element of Hom⁡(W,V)\operatorname{Hom}(W,V), that φ(W)⊂Vp\varphi(W)\subset V_{p}. First extend v1…,vpv_{1}\dots,v_{p} to a basis ⟨v1…vn⟩\langle v_{1}\dots v_{n}\rangle, of VV. Let w1,…,wp,…,wnw_{1},\dots,w_{p},\dots,w_{n} be a dual basis so that vi(wj)=δijv_{i}(w_{j})=\delta_{ij}. First note that because φ\varphi is symmetric, ker⁡(φ)⊃⟨wp+1…wn⟩\ker(\varphi)\supset\langle w_{p+1}\dots w_{n}\rangle. Further, one has v1∧…vp∧wj=0v_{1}\wedge\dots v_{p}\wedge w_{j}=0(under the standard contraction) if j>pj>p, and so λ∧wi1⋯∧win=0\lambda\wedge w_{i_{1}}\dots\wedge w_{i_{n}}=0 unless ⟨wi1…win⟩=⟨w1…wp,wj⟩\langle w_{i_{1}}\dots w_{i_{n}}\rangle=\langle w_{1}\dots w_{p},w_{j}\rangle with j>pj>p. Then λ∧⋀p+1(W)⊂W>p\lambda\wedge\bigwedge^{p+1}(W)\subset W_{>p}, the subspace of WW generated by ⟨wp+1…wn⟩\langle w_{p+1}\dots w_{n}\rangle and hence is killed by φ\varphi.

Let D compute Cliff(C) and let φ∈TKC(D)\varphi\in T_{K_{C}}(D) be a Shiffer variation in Sec⁡d−1(C)/Sec⁡d−2(C)\operatorname{Sec}^{d-1}(C)/\operatorname{Sec}^{d-2}(C) with rk⁡(τ)=Cliff⁡(C)\operatorname{rk}(\tau)=\operatorname{Cliff}(C). Let Im(φ)=⟨σ1,…,σc⟩⊂VIm(\varphi)=\langle\sigma_{1},\dots,\sigma_{c}\rangle\subset V and set σ=σ1∧⋯∧σc\sigma=\sigma_{1}\wedge\dots\wedge\sigma_{c}. Then φ⊗σ\varphi\otimes\sigma represents a non-trivial Koszul cohomology class in Kp,2(C,KC)K_{p,2}(C,K_{C}).

We comment on how this compares to the construction of Green and Lazarsfeld in the appendix to . Their idea is that if one can factor a line bundle L as L1⊗L2L_{1}\otimes L_{2} , where h0(L1)=r1+1h^{0}\left({L_{1}}\right)=r_{1}+1 and h0(L2)=r2+1h^{0}\left({L_{2}}\right)=r_{2}+1 with ri≥1r_{i}\geq 1 then one can produce a non-trivial class in Kr1+r2−1,1(C,L)K_{r_{1}+r_{2}-1,1}(C,L) .

There is a duality of Koszul cohomology groups and for L=KCL=K_{C} the group Kg−p−2,1K_{g-p-2,1} is dual to Kp,2K_{p,2}. If L1=OC(D)L_{1}=\mathcal{O}_{C}(D), then L2=KC(−D)L_{2}=K_{C}(-D) and by Riemann-Roch r2=g−d+r1−1r_{2}=g-d+r_{1}-1 so that r1+r2−1=g−d+2r1−2=g−Cliff⁡(D)−2r_{1}+r_{2}-1=g-d+2r_{1}-2=g-\operatorname{Cliff}(D)-2. If DD computes Cliff⁡(C)=c\operatorname{Cliff}(C)=c the cohomology class lives in Kg−c−2,1(C,L)K_{g-c-2,1}(C,L) which is dual to Kc,2(C,L)K_{c,2}(C,L). Their construction amounts to the following: if si∈H0(C,Li)s_{i}\in H^{0}\left({C,L_{i}}\right) corresponds to a divisor DiD_{i} then the linear space corresponding to D1∩D2D_{1}\cap D_{2} is used to construct the cohomology class in Kr1+r2−1,1(C,L)K_{r_{1}+r_{2}-1,1}(C,L). Eisenbud ( ch.8) has given a different version of their construction.

The class I have constructed also lies in a group dual to Kc,2K_{c,2}. This is the situation of Theorem 9.3. Let DD be a divisor used to compute Cliff(C). If H0(OC(D))={f0,…,fr}H^{0}\left({\mathcal{O}_{C}(D)}\right)=\{f_{0},\dots,f_{r}\} and H0(KC(D))={η1,…,ηg−d+r}H^{0}\left({K_{C}(_{D})}\right)=\{\eta_{1},\dots,\eta_{g-d+r}\} then we constucted a Shiffer variation which vanished on {f0⊗ηi} 1≤i≤(g−d+r)\{f_{0}\otimes\eta_{i}\}\,1\leq i\leq(g-d+r) and{fi⊗η1}\{f_{i}\otimes\eta_{1}\} 1≤i≤r1\leq i\leq r which is exactly the intersection of the linear spaces spanned by DD and KC(−D)K_{C}(-D). By this I mean that the {fi}\{f_{i}\} generate the ideal of the linear space corresponding to KC(−D)K_{C}(-D) and the {ηi}\{\eta_{i}\} generate the ideal of the linear space corresponding to DD.

Remark 2 Notice how the formula: h0(OC(D))+h0(KC(−D))=g+1−Cliff⁡(D)h^{0}\left({\mathcal{O}_{C}(D)}\right)+h^{0}\left({K_{C}(-D)}\right)=g+1-\operatorname{Cliff}(D) comes into play in these constructions. In essence, whenever we factor KCK_{C} as OC(D)⊗KC(−D)\mathcal{O}_{C}(D)\otimes K_{C}(-D), we should expect to find a linear subspace of dimension = Cliff(D) and a Shiffer variation supported on this subspace. Our construction will produce such a Shiffer variation and hence such a cohomology class as long as one of the line bundles is base point free. We have discussed this more extensivly in the section line bundles with h1(L)=1h^{1}\left({L}\right)=1. As long as that is the case, we can non-trivial Koszul cohomology classes. They should be essentially the same as the classes constructed by Green and Lazarsfeld.

Remark 3 The construction of is not the only way to construct non-trivial classes. For example a more general construction is presented. In all these cases the natural location of these classes is in a group of the form Kp,1K_{p,1}. Our classes always live in Kp,2∗.K_{p,2}^{*}. Thus all previous methods speak to the lenght of the linear strand of the minimal free resolution of SCS_{C}, whereas our methods possibly give information on where the quadratic strand may start. Recall that the linear strand of a variety (defined by quadrics) is the piece in degree pp composed of O(−p−1)\mathcal{O}(-p-1)’s and the quadratic strand is the piece composed of O(−p−2)\mathcal{O}(-p-2)’s In the special case L=KCL=K_{C} there is duality between Kp,2K{p,2} and Kg−p−2,1K_{g-p-2,1} which doesn’t exist for other line bundles allows one to translate results about the linear strand to results about the quadratic strand.

We also do not always require that the bundle factor as the tensor product of two bundles, both of which have at least 2 sections. This is necessary for the construction of Green and Lazarsfeld. For example, let L=KC(D)L=K_{C}(D) where D is effective. Then by Theorem 3.6 Cliff⁡(C,L)=d−2\operatorname{Cliff}(C,L)=d-2 and by 5.4 there exists a τ∈TL(D)\tau\in T_{L}(D) of rank d−2d-2 such that τ∈Sec⁡d−1\tau\in\operatorname{Sec}^{d-1} but τ∉Sec⁡d−2\tau\notin\operatorname{Sec}^{d-2}. If D is general of with deg⁡(D)<g\deg(D)<g, then H0(OC(D))=0H^{0}\left({\mathcal{O}_{C}(D)}\right)=0 so the method of Green and Lazarsfeld doesn’t produce anything interesting. However:

The class τ\tau produced above gives a nontrivial cohomology class in Kd−2,2K_{d-2,2}.

The proof goes exactly as in Theorem 9.3. Namely by Hassett’s criteria, the d−2d-2 plane, Im(τ)Im(\tau) cannot meet C. This means for any expression τ=∑=1i=d−2ti2\tau=\sum_{=1}^{i=d-2}t_{i}^{2}, the ti3t_{i}^{3} cannot lie in M3M_{3} and hence τ\tau cannot be a boundary.

The final issue to be discussed in this thesis is the relationship between our theorems and Green’s conjecture. Because K0,2(C,KC)=0K_{0,2}(C,K_{C})=0 if and only if Cliff⁡(C)>0\operatorname{Cliff}(C)>0 and if K0,2(C,KC)=0K_{0,2}(C,K_{C})=0, then K1,2(C,KC)=0K_{1,2}(C,K_{C})=0 iff Cliff⁡(C)>1\operatorname{Cliff}(C)>1, Green conjectured that Kp,2(C,KC)=0K_{p,2}(C,K_{C})=0 for p<Cliff⁡(C)p<\operatorname{Cliff}(C). There has been a lot of progress on this issue. After partial results mainly by Schreyer (see and ), Voisin proved Green’s conjecture for a generic curve in and . Needless to say her techniques are very different from the ones of this thesis. In particular she uses the duality between Kp,2K_{p,2} and Kg−p−2,1K_{g-p-2,1} which is particular to the case of L=KCL=K_{C}. She then proves the vanishing on a specific curve. Generic vanishing follows by semi-continuity. The techniques of this thesis work for a larger class of line bundles and prove results that hold for all curves carrying such a line bundle. However the results given here do not seem to prove Green’s conjecture on the nose.

We do have a positive result. Suppose p<Cliff⁡(C,L)p<\operatorname{Cliff}(C,L). We consider the dual of Kp,2(C,L)=0K_{p,2}(C,L)=0. Recall that the dual cohomology group is the cohomology of the complex:

Suppose that φ⊗λ∈M2⊗⋀P(V)\varphi\otimes\lambda\in M_{2}\otimes\bigwedge^{P}(V) with λ\lambda decomposable and that δ(φ⊗λ)=0\delta(\varphi\otimes\lambda)=0 , then φ⊗λ=δ(μ)\varphi\otimes\lambda=\delta(\mu) for some μ∈M3⊗⋀p−1(V)\mu\in M_{3}\otimes\bigwedge^{p-1}(V). That is to say, in the group dual to the Koszul cohomology group, any decomposable element is trivial.

Write λ=σ1∧⋯∧σp\lambda=\sigma_{1}\wedge\dots\wedge\sigma_{p}. We first claim that im⁡(φ)⊂⟨σ1…σp⟩\operatorname{im}(\varphi)\subset\langle\sigma_{1}\dots\sigma_{p}\rangle. If not let τ∈im⁡(φ)\tau\in\operatorname{im}(\varphi) be such that τ∧λ≠0\tau\wedge\lambda\neq 0 and let τ∨∧λ∨\tau^{\vee}\wedge\lambda^{\vee} be dual to this element. Then δ(φ⊗λ)(τ∨∧λ∨)=φ(τ∨)≠0\delta(\varphi\otimes\lambda)(\tau^{\vee}\wedge\lambda^{\vee})=\varphi(\tau^{\vee})\neq 0.

Now since rk⁡(φ)≤p\operatorname{rk}(\varphi)\leq p we can write φ=∑i=1kσpi2\varphi=\sum_{i=1}^{k}\sigma_{p_{i}}^{2} where k≤pk\leq p and σpi2\sigma_{p_{i}}^{2} is a Shiffer variation associated to the point pi∈Cp_{i}\in C. Set μ=13∑i=1k(−1)k−1σi3⊗σ1∧…σi−1∧σi+1⋯∧σk\mu=\frac{1}{3}\sum_{i=1}^{k}(-1)^{k-1}\sigma_{i}^{3}\otimes\sigma_{1}\wedge\dots\sigma_{i-1}\wedge\sigma_{i+1}\dots\wedge\sigma_{k}. Then μ∈M3⊗⋀p−1(V)\mu\in M_{3}\otimes\bigwedge^{p-1}(V) and δ(μ)=φ⊗λ\delta(\mu)=\varphi\otimes\lambda. ∎

At this point we are left with the words of Ludwig Bemelmans, “And thats all there is– there isn’t anymore”.

References