Equations for secant varieties of Veronese and other varieties

J. M. Landsberg, Giorgio Ottaviani

Introduction

Show a certain Young Flattening, YFd,nYF_{d,n}, provides scheme-theoretic equations for a large class of cases where usual flattenings fail, see Theorem 1.2.3.

Determine cases where flattenings are sufficient to give defining equations (more precisely, scheme-theoretic equations), Theorem 3.2.1. Theorem 3.2.1 is primarily a consequence of work of A. Iarrobino and V. Kanev and Diesel .

Put our results in a larger context by providing a uniform formulation of all known equations for secant varieties via vector bundle methods. We use this perspective to prove some of our results, including a key induction Lemma 6.2.1. The discussion of vector bundle methods is postponed to the latter part of the paper to make the results on symmetric border rank more accessible to readers outside of algebraic geometry.

Here is a chart summarizing what is known about equations of secant varieties of Veronese varieties:

2. Young Flattenings

All the principal Pfaffians of size 88 of the this matrix coincide, up to scale, with the classical Aronhold invariant. (Redundancy occurs here is because one should really work with the submodule S21V⊂V⊗∧2V≃V⊗V∗S_{21}V\subset V{\mathord{\otimes}}\wedge^{2}V\simeq V{\mathord{\otimes}}V^{*}, where the second identification uses a choice of volume form. The Pfaffian of the map S21→S21S_{21}\to S_{21} is the desired equation.)

Now consider the inclusion V⊂∧kV∗⊗∧k+1VV\subset\wedge^{k}V^{*}{\mathord{\otimes}}\wedge^{k+1}V, given by v∈Vv\in V maps to the map ω↦v∧ω\omega\mapsto v\wedge\omega. In bases one obtains a matrix whose entries are the coefficients of vv or zero. In the special case n+1=2a+1n+1=2a+1 is odd and k=ak=a, one obtains a square matrix KnK_{n}, which is skew-symmetric for odd aa and symmetric for even aa. For example, when n=2n=2, the matrix is

Finally, consider the following generalization of both the Aronhold invariant and the KnK_{n}. Let a=⌊n2⌋a=\lfloor\frac{n}{2}\rfloor and let d=2δ+1d=2\delta+1. Map SdV→(SδV⊗∧aV∗)⊗(SδV⊗∧a+1V)S^{d}V\rightarrow(S^{\delta}V{\mathord{\otimes}}\wedge^{a}V^{*}){\mathord{\otimes}}(S^{\delta}V{\mathord{\otimes}}\wedge^{a+1}V) by first performing the inclusion SdV→SδV⊗SδV⊗VS^{d}V\rightarrow S^{\delta}V{\mathord{\otimes}}S^{\delta}V{\mathord{\otimes}}V and then using the last factor to obtain a map ∧aV→∧a+1V\wedge^{a}V\rightarrow\wedge^{a+1}V. We get:

If n+1n+1 is odd, the matrix representing YFd,n(ϕ)YF_{d,n}(\phi) is skew-symmetic, so we may take Pfaffians instead of minors.

For a decomposable wd∈SdVw^{d}\in S^{d}V, the map is

In bases, one obtains a matrix in block form, where the blocks correspond to the entries of KnK_{n} and the matrices in the blocks are the square catalecticants ±(∂ϕ∂xi)δ,δ\pm(\frac{\partial\phi}{\partial x_{i}})_{\delta,\delta} in the place of ±xi\pm x_{i}.

Just as with the Aronhold invariant above, there will be redundancies among the minors and Pfaffians of YFd,n(ϕ)YF_{d,n}(\phi). See §4 for a description without redundancies.

In the case n=2an=2a with odd aa, YFd,nYF_{d,n} is skew-symmetric (for any dd) and one may instead take the size (na)r+2{{n}\choose a}r+2 sub-pfaffians of YFd,nYF_{d,n}.

In the case n=2an=2a with even aa, YFd,nYF_{d,n} is symmetric.

The bounds given in Theorem 1.2.3 for n=2n=2 are sharp (see Proposition 4.2.3).

3. Vector bundle methods

Let EE be a vector bundle on XX of rank ee, write L=OX(1)L={\mathcal{O}}_{X}(1), so V=H0(X,L)∗V=H^{0}(X,L)^{*}. Let v∈Vv\in V and consider the linear map

where AvE(s)=A(s⊗v)A^{E}_{v}(s)=A(s{\mathord{\otimes}}v). In examples EE will be chosen so that both H0(E)H^{0}(E) and H0(E∗⊗L)H^{0}(E^{*}\otimes L) are nonzero, otherwise our construction is vacuous. A key observation (Proposition 5.1.1) is that the size (re+1)(re+1) minors of AvEA_{v}^{E} give equations for σr(X)\sigma_{r}(X).

4. Overview

Acknowledgments

We thank P. Aluffi, who pointed out the refined Bézout theorem 2.4.1. This paper grew out of questions raised at the 2008 AIM workshop Geometry and representation theory of tensors for computer science, statistics and other areas, and the authors thank AIM and the conference participants for inspiration.

Background

If G/PG/P is a rational homogeneous variety and E→G/PE\rightarrow G/P is an irreducible homogeneous vector bundle, we write E=EμE=E_{\mu} where μ\mu is the highest weight of the irreducible PP-module inducing EE. We use the conventions of regarding roots and weights of simple Lie algebras.

2. Flattenings

Given ϕ∈SdV\phi\in S^{d}V, write ϕa,d−a∈SaV⊗Sd−aV\phi_{a,d-a}\in S^{a}V{\mathord{\otimes}}S^{d-a}V for the (a,d−a)(a,d-a)-polarization of ϕ\phi. We often consider ϕa,d−a\phi_{a,d-a} as a linear map ϕa,d−a:SaV∗→Sd−aV\phi_{a,d-a}:S^{a}V^{*}\rightarrow S^{d-a}V. This notation is compatible with the more general one of Young flattenings that we will introduce in §4.

3. Inheritance

Let VV be a vector space of dimension greater than rr.

4. Results related to degree

Sometimes it is possible to conclude global information from local equations if one has information about degrees.

We need the following result about excess intersection.

This is an application of the refined Bézout theorem of [16, Thm. 12.3]. ∎

We recall the following classical formulas, due to C. Segre. For a modern reference see .

5. Conormal spaces

Let [ϕ]∈Rank(a,d−a)r(SdV)[\phi]\in Rank^{r}_{(a,d-a)}(S^{d}V) be a sufficiently general point, then

and equality holds if ϕ\phi is sufficiently general.

Symmetric Flattenings (catalecticant minors)

The following result dates back to the work of Sylvester and Gundelfinger.

Apply Proposition 2.3.1 to Theorem 3.1.1 in the case r=2r=2. ∎

C. Raicu recently proved that in Corollary 3.1.2 it is possible to replace the (2,d−2)(2,d-2) flattening with any (i,d−i)(i,d-i)-flattening such that 2≤i≤d−22\leq i\leq d-2.

The bound obtained in this theorem is the best we know of for even degree, apart from some cases of small degree listed below. Theorem 1.2.3 is an improvement of this bound in the case of odd degree.

We will have need of more than one symmetric flattening, so we make the following definitions, following , but modifying the notation:

Fix a sequence r⃗:=(r1,…,r⌞d2⌟)\vec{r}:=(r_{1},\ldots,r_{\llcorner\frac{d}{2}\lrcorner}) and let

Call a sequence r⃗\vec{r} admissible if there exists ϕ∈SdW\phi\in S^{d}W such that rank(ϕj,d−j)=rj{\rm rank}(\phi_{j,d-j})=r_{j} for all j=1,…,⌞d2⌟j=1,\ldots,\llcorner\frac{d}{2}\lrcorner. It is sufficient to consider r⃗\vec{r} that are admissible because if r⃗\vec{r} is non-admissible, the zero set of SFlatr⃗SFlat_{\vec{r}} will be contained in the union of admissible SFlatSFlat’s associated to smaller r⃗\vec{r}’s in the natural partial order. Note that SFlatr⃗(SdW)⊆Subr1(SdW)SFlat_{\vec{r}}(S^{d}W)\subseteq Sub_{r_{1}}(S^{d}W).

To remedy this, let r⃗\vec{r} be admissible, and consider

In the commutative algebra literature (e.g. ), “Gor” is short for Gorenstein, see [25, Def. 1.11] for a history.

Unfortunately, defining equations for Gor(r⃗)Gor(\vec{r}) are not known. One can test for membership of SFlatr⃗0(SdW)SFlat_{\vec{r}}^{0}(S^{d}W) by checking the required vanishing and non-vanishing of minors.

[12, Thm 1.1] If dim⁡W=3\operatorname{dim}W=3, and r⃗\vec{r} is admissible, then Gor(r⃗)Gor(\vec{r}) is irreducible.

Theorem 3.1.9 combined with Theorem 3.1.4 allows one to extend the set of secant varieties of Veronese varieties defined by flattenings.

2. Consequences of Theorems 3.1.9 and 3.1.4

The following varieties are defined scheme-theoretically by minors of flattenings:

By [47, Thm 4.2], when n≤2n\leq 2, rank(ϕs,d−s){\rm rank}(\phi_{s,d-s}) is nondecreasing in ss for 1≤s≤⌊d2⌋1\leq s\leq\lfloor\frac{d}{2}\rfloor. We will use this fact often in this section.

To prove each case, we simply show the scheme defined by the flattenings in the hypotheses coincides with the scheme of some Gor(r⃗)Gor(\vec{r}) with r⃗\vec{r} admissible and then Theorem 3.1.4 combined with Theorem 3.1.9 implies the result. The first step is to determine which r⃗\vec{r} are admissible.

The only admissible sequences r⃗\vec{r} with r1=3r_{1}=3 and ri≤5r_{i}\leq 5 are

We may assume that rank(ϕ1,d−1)=3{\rm rank}(\phi_{1,d-1})=3, otherwise we are in the case of two variables. By inheritance, it is sufficient to prove the result for n=2n=2. In this case, if rank(ϕa,d−a)≤3{\rm rank}(\phi_{a,d-a})\leq 3 for a=⌊d2⌋a=\lfloor\frac{d}{2}\rfloor, then rank(ϕa,d−a)≤3{\rm rank}(\phi_{a,d-a})\leq 3 for all aa such that 2≤a≤d−22\leq a\leq d-2, and r⃗=(3,…,3)\vec{r}=(3,\ldots,3) is admissible . ∎

Otherwise rank(ϕ2,d−2)≤5{\rm rank}(\phi_{2,d-2})\leq 5. In this case, by an extension of Lemma 3.2.3 , there are just two other possibilities for r⃗\vec{r}, namely r⃗1=(1,3,5,6…,6,5,3,1)\vec{r}_{1}=(1,3,5,6\ldots,6,5,3,1) and r⃗2=(1,3,4,5,6…,6,5,4,3,1)\vec{r}_{2}=(1,3,4,5,6\ldots,6,5,4,3,1) for d≥8d\geq 8.

Let dim⁡W=3\operatorname{dim}W=3. We will need the following facts to prove Lemma 3.2.3:

For ϕ∈SdW\phi\in S^{d}W, consider the ideal ϕ⊥\phi{}^{\perp} generated in degrees ≤d\leq d, by ker⁡(ϕa,d−a)⊂SaW∗\operatorname{ker}(\phi_{a,d-a})\subset S^{a}W^{*}, 1≤a≤d1\leq a\leq d, and the ring Aϕ:=Sym(W∗)/ϕ⊥A_{\phi}:=Sym(W^{*})/\phi{}^{\perp}. Note that the values of the Hilbert function of AϕA_{\phi}, HAϕ(j)H_{A_{\phi}}(j), are T(r⃗):=(1,r1,…,r⌞d2⌟,r⌞d2⌟,…,r1,1,0,…,0)T(\vec{r}):=(1,r_{1},\ldots,r_{\llcorner\frac{d}{2}\lrcorner},r_{\llcorner\frac{d}{2}\lrcorner},\ldots,r_{1},1,0,\ldots,0), where recall that rj=rank(ϕj,d−j)r_{j}={\rm rank}(\phi_{j,d-j}).

[5, Thm. 2.1] The ring AϕA_{\phi} has a minimal free resolution of the form

where the qjq_{j} are non-decreasing. Here Sym(W∗)(j)Sym(W^{*})(j) denotes Sym(W∗)Sym(W^{*}) with the labeling of degrees shifted by jj, so dim⁡(Sym(W∗)(j))d=(d+j+22)\operatorname{dim}(Sym(W^{*})(j))_{d}=\binom{d+j+2}{2}.

Moreover [12, Thm 1.1] there is a unique resolution with the properties q1≤d+32q_{1}\leq\frac{d+3}{2}, qi+qu−i+2=d+2q_{i}+q_{u-i+2}=d+2, 2≤i≤u+122\leq i\leq\frac{u+1}{2} having T(r⃗)T(\vec{r}) as the values of its Hilbert function.

Recall that HAϕ(j)H_{A_{\phi}}(j) is also the alternating sum of the dimensions of the degree jj term in (5) (forgetting the last term). Thus the qjq_{j} determine the rir_{i}.

[12, Thm. 3.3] Letting j0j_{0} be the smallest jj such that ϕj,d−j\phi_{j,d-j} is not injective, then u=2j0+1u=2j_{0}+1 in the resolution above.

If there are three generators in degree 22 then qi=(2,2,2,d,d)q_{i}=(2,2,2,d,d), and computing the Hilbert function via the Euler characteristic, we are in case (1) of the Lemma.

If there are two generators in degree 22 then there are the two possibilities qi=(2,2,3,n−1,n)q_{i}=(2,2,3,n-1,n) (case(2)) or qi=(2,2,4,n−2,n)q_{i}=(2,2,4,n-2,n) (case (4)). Note that qi=(2,2,5,n−3,n)q_{i}=(2,2,5,n-3,n) for n≥8n\geq 8 is impossible because otherwise r⃗=(1,3,4,5,6,…)\vec{r}=(1,3,4,5,6,\ldots) contrary to assumption. By similar arguments one shows that there are no other possibilities.

If there is one generator in degree 22 then qi=(2,3,3,n−1,n−1)q_{i}=(2,3,3,n-1,n-1) (case (3)). ∎

The result follows by solving the inequality. ∎

For the case (p,r)=(2,4)(p,r)=(2,4) see Theorem 3.2.1(2) and for the case (p,r)=(3,9)(p,r)=(3,9) see Theorem 4.2.9.

The values of the right hand side of the inequality for p=1,…4p=1,\ldots 4 are respectively 44, 112112, 2831428314, 8166215281662152.

Equality holds in Corollary 3.2.6 for the cases p=1,2,3p=1,2,3 by Proposition 2.4.2. The case p=1p=1 corresponds to the quadratic Veronese surface and the cases p=2,3p=2,3 will be considered respectively in Thm.3.2.1 (1) and Theorem 4.2.8. For p≥4p\geq 4 these numbers are out of the range of the results in (the points are too few to be fixed points of a torus action) and we do not know if equality holds.

Young flattenings for Veronese varieties

In what follows we fix n+1=dim⁡Vn+1=\operatorname{dim}V and endow VV with a volume form and thus identify (as SL(V)SL(V)-modules) S(p1,…,pn+1)VS_{(p_{1},\ldots,p_{n+1})}V with S(p1−pn+1,p2−pn+1,…,pn−pn+1,0)VS_{(p_{1}-p_{n+1},p_{2}-p_{n+1},\ldots,p_{n}-p_{n+1},0)}V. We will say (p1−pn,p2−pn,…,pn−1−pn,0)(p_{1}-p_{n},p_{2}-p_{n},\ldots,p_{n-1}-p_{n},0) is the reduced partition associated to (p1,…,pn)(p_{1},\ldots,p_{n}).

The Pieri formula states that SπV∗⊂SνV∗⊗SdV∗S_{\pi}V^{*}\subset S_{\nu}V^{*}{\mathord{\otimes}}S^{d}V^{*} iff the Young diagram of π\pi is obtained by adding dd boxes to the Young diagram of ν\nu, with no two boxes added to the same column. Moreover, if this occurs, the multiplicity of SπV∗S_{\pi}V^{*} in SνV∗⊗SdV∗S_{\nu}V^{*}{\mathord{\otimes}}S^{d}V^{*} is one.

Say SπV∗⊂SνV⊗SdV∗S_{\pi}V^{*}\subset S_{\nu}V{\mathord{\otimes}}S^{d}V^{*} and consider the map SdV→SπV⊗SνV∗S^{d}V\rightarrow S_{\pi}V{\mathord{\otimes}}S_{\nu}V^{*}. Let SμV=SνV∗S_{\mu}V=S_{\nu}V^{*} where μ\mu is the reduced partition with this property. We obtain an inclusion SdV→SπV⊗SμVS^{d}V\rightarrow S_{\pi}V{\mathord{\otimes}}S_{\mu}V.

Given ϕ∈SdV\phi\in S^{d}V, let ϕπ,μ∈SπV⊗SμV\phi_{\pi,\mu}\in S_{\pi}V{\mathord{\otimes}}S_{\mu}V denote the corresponding element. If SμV=SνV∗S_{\mu}V=S_{\nu}V^{*} as an SL(V)SL(V)-module, we will also write ϕπ,ν∗=ϕπ,μ\phi_{\pi,\nu^{*}}=\phi_{\pi,\mu} when we consider it as a linear map SνV→SπVS_{\nu}V\rightarrow S_{\pi}V.

The following proposition is an immediate consequence of the subadditivity for ranks of linear maps.

So far we have not obtained any new equations using three way symmetric flattenings and Young flattenings. We mention three-way symmetric flattenings because they may be useful in future investigations, especially when further modules of equations for secant varieties of triple Segre products are found.

Recall YFd,nrYF_{d,n}^{r} from §1.2 whose description had redundancies. We can now give an irredundant description of its defining equations:

This is a consequence of Schur’s Lemma, because the module S(δ+1,1a)VS_{(\delta+1,1^{a})}V is the only one appearing in both sides of SdV⊗SδV∗⊗∧aV→SδV⊗∧a+1VS^{d}V\otimes S^{\delta}V^{*}\otimes\wedge^{a}V\to S^{\delta}V\otimes\wedge^{a+1}V

Note that if SπV≃SμVS_{\pi}V\simeq S_{\mu}V as SL(V)SL(V)-modules and the map is symmetric, then

In this subsection fix dim⁡V=3\operatorname{dim}V=3 and a volume form Ω\Omega on VV. From the general formula for dim⁡SπV\operatorname{dim}S_{\pi}V (see, e.g., [17, p78]), we record the special case:

Let a≥ba\geq b. Write d=α+β+γd=\alpha+\beta+\gamma with α≤b\alpha\leq b, β≤a−b\beta\leq a-b so S(a+γ−α,b+β−α)V⊂Sa,bV⊗SdVS_{(a+\gamma-\alpha,b+\beta-\alpha)}V\subset S_{a,b}V{\mathord{\otimes}}S^{d}V. For ϕ∈SdV\phi\in S^{d}V, consider the induced map

In the following picture we label the first row containing aa boxes with aa and so on.

Assume we have chosen a weight basis x1,x2,x3x_{1},x_{2},x_{3} of VV and x=x3x=x_{3} is a vector of lowest weight. Consider the image of a weight basis of Sa,bVS_{a,b}V under (x33)(a,b),(a+γ−α,b+β−α)(x^{3}_{3})_{(a,b),(a+\gamma-\alpha,b+\beta-\alpha)}. Namely consider all semi-standard fillings of the Young diagram corresponding to (a,b)(a,b), and count how many do not map to zero. By construction, the images of all the vectors that do not map to zero are linearly independent, so this count indeed gives the dimension of the image.

In order to have a vector not in the kernel, the first α\alpha boxes of the first row must be filled with 11’s and the first α\alpha boxes of the second row must be filled with 22’s.

We are particularly interested in cases where (a,b)=(a+γ−α,b+β−α)(a,b)=(a+\gamma-\alpha,b+\beta-\alpha). In this case

Plugging into the conclusion of Lemma 4.2.1, the rank of the image of a dd-th power in this situation is

To keep this small, it is convenient to take d=a+bd=a+b so the rank is a−b+1a-b+1. One can then fix this number and let a,ba,b grow to study series of cases.

If (10) has rank one when d=2pd=2p, we just recover the usual symmetric flattenings as S(p,p)V=SpV∗S_{(p,p)}V=S_{p}V^{*}. We consider the next two cases in the theorems below, (a,b)=(p+1,p)(a,b)=(p+1,p) when d=2p+1d=2p+1 and (a,b)=(p+2,p)(a,b)=(p+2,p) when d=2p+2d=2p+2. Recall that (p+q,p)∗=(p+q,q)(p+q,p)^{*}=(p+q,q) in the notation of §4.1.1.

Let d=2p+1d=2p+1. The skew analog of Proposition 3.2.5 is the following proposition, which shows that the bound in the assumption of Theorem 1.2.3 is sharp.

Here is a pictorial description when p=2p=2 of ϕ31,31 ⁣:S32V→S31V\phi_{31,31}\colon S_{32}V\to S_{31}V in terms of Young diagrams:

The values of the right hand side for p=1,…4p=1,\ldots 4 are respectively 44, 140140, 6578065780, 563178924563178924.

In Corollary 4.2.4 equality holds in the cases p=1,2p=1,2 by Proposition 2.4.2. The case p=1p=1 is just the Aronhold case and the case p=2p=2 will be considered in Theorem 4.2.7 (2). For p≥3p\geq 3 these numbers are out of the range of and we do not know if equality holds.

Now let d=2p+2d=2p+2 be even, requiring π=μ\pi=\mu, the smallest possible rank((xd)π,μ){\rm rank}((x^{d})_{\pi,\mu}) is three, which we obtain with ϕ(p+2,p),(p+2,p)\phi_{(p+2,p),(p+2,p)}.

A pictorial description when p=2p=2 is as follows:

and define MϕM_{\phi} for arbitrary ϕ∈S2p+2V\phi\in S^{2p+2}V by linearity and polarization. If we take bases of S2V⊗S2(∧2V)S^{2}V{\mathord{\otimes}}S^{2}(\wedge^{2}V) as above, with indices ((i1,…,ip),(kl),(k′l′))((i_{1},\ldots,i_{p}),(kl),(k^{\prime}l^{\prime})), most of the matrix of Me12p+2M_{e_{1}^{2p+2}} is zero. The upper-right hand 6×66\times 6 block, where (i1,…,ip)=(1,…,1)(i_{1},\ldots,i_{p})=(1,\ldots,1) in both rows and columns and the order on the other indices

where all the terms in stuffstuff have partitions with at least three parts. On the other hand, from the nature of the image we conclude it is just the first factor and Mϕ∈S2(Sp+2,2V)M_{\phi}\in S^{2}(S_{p+2,2}V). ∎

is skew-symmetric if pp is even and symmetric if pp is odd.

Consider Mϕ:Sp−1V∗⊗Sq(∧2V∗)→SpV⊗Sq(∧2V)M_{\phi}:S^{p-1}V^{*}{\mathord{\otimes}}S^{q}(\wedge^{2}V^{*})\rightarrow S^{p}V{\mathord{\otimes}}S^{q}(\wedge^{2}V) given for ϕ=xp+4q−1\phi=x^{p+4q-1} by

The following is a special case of the Thm. 3.2.1(4), we include this second proof because it is very short.

det⁡(ϕ42,42)\det(\phi_{42,42}) is a polynomial of degree 27, which is not the power of a lower degree polynomial. This can be proved by cutting with a random projective line, and using Macaulay2. The two variable polynomial obtained is not the power of a lower degree polynomial.

To prove (2), we picked a polynomial ϕ\phi which is the sum of 88 random fifth powers of linear forms, and a submatrix of ϕ42,42\phi_{42,42} of order 2424 which is invertible. The matrix representing ϕ42,42\phi_{42,42} can be constructed explicitly by the package PieriMaps of Macaulay2 .

(1) can be proved in the same way. (3) is well known. ∎

(1) follows from Theorem 1.2.3. (2) is obvious. ∎

Construction of equations from vector bundles

Write e:=rank(E)e:={\rm rank}(E) and consider the determinantal varieties or rank varieties defined by the minors of AvE:H0(E)→H0(E∗⊗L)∗A^{E}_{v}:H^{0}(E)\to H^{0}(E^{*}\otimes L)^{*} (defined by equation (3)),

i.e., the size (re+1)(re+1) minors of AvEA_{v}^{E} give equations for σr(X)\sigma_{r}(X).

When EE is understood, we will write AvA_{v} for AvEA_{v}^{E}.

By (3), if x=[v]∈Xx=[v]\in X, then H0(Ix⊗E)⊆ker⁡AvH^{0}(I_{x}\otimes E)\subseteq\ker A_{v}. The subspace H0(Ix⊗E)⊆H0(E)H^{0}(I_{x}\otimes E)\subseteq H^{0}(E) has codimension at most ee in H0(E)H^{0}(E), hence the same is true for the subspace ker⁡Ax\ker A_{x} and it follows rank(Ax)≤e{\rm rank}(A_{x})\leq e. If v∈σ^r(X)v\in\hat{\sigma}_{r}(X) is a general point, then it may be expressed as v=∑i=1rxiv=\sum_{i=1}^{r}x_{i}, with xi∈X^x_{i}\in\hat{X}. Hence

as claimed. Since the inequality is a closed condition, it holds for all v∈σ^r(X)v\in\hat{\sigma}_{r}(X). ∎

The generalization of symmetric flattenings to Young flattenings for Veronese varieties is a representation-theoretic version of the generalization from line bundles to higher rank vector bundles.

A general source of examples is given by curves obtained as determinantal loci. This topic is studied in detail in . In , A. Ginensky considers the secant varieties σk(C)\sigma_{k}(C) to smooth curves CC in their bicanonical embedding. With our notations this corresponds to the symmetric pair (E,L)=(KC,KC2)(E,L)=(K_{C},K_{C}^{2}). He proves [21, Thm. 2.1] that σk(C)=Rankk(KC)\sigma_{k}(C)=Rank_{k}(K_{C}) if k<Cliff(C)k<\textrm{Cliff}(C) and σk(C)⊊Rankk(KC)\sigma_{k}(C)\subsetneq Rank_{k}(K_{C}) for larger kk. Here Cliff(C)\textrm{Cliff}(C) denotes the Clifford index of CC.

2. The construction in the symmetric and skew-symmetric cases

We say that (E,L)(E,L) is a symmetric pair if the isomorphism E⟶αE∗⊗LE\smash{\mathop{\longrightarrow}\limits^{\alpha}}E^{*}\otimes L is symmetric, that is the transpose isomorphism E⊗L∗⟶αtE∗E\otimes L^{*}\smash{\mathop{\longrightarrow}\limits^{\alpha^{t}}}E^{*}, after tensoring by LL and multiplying the map by 1L1_{L} equals α\alpha, i.e., α=αt⊗1L\alpha=\alpha^{t}\otimes 1_{L}. In this case S2ES^{2}E contains LL as a direct summand, the morphism AvA_{v} is symmetric, and Rankk(E)Rank_{k}(E) is defined by the (ke+1)(ke+1)-minors of AvA_{v}.

Similarly, (E,L)(E,L) is a skew-symmetric pair if α=−αt⊗1L\alpha=-\alpha^{t}\otimes 1_{L}. In this case ee is even, ∧2E\wedge^{2}E contains LL as a direct summand, the morphism AvA_{v} is skew-symmetric, and Rankk(E)Rank_{k}(E) is defined by the size (ke+2)(ke+2) subpfaffians of AvA_{v}, which are equations of degree ke2+1\frac{ke}{2}+1.

3. The conormal space

The results reviewed in §2.5, restated in the language of vector bundles, say the affine conormal space of Rankk(E)Rank_{k}(E) at [v]∈Rankk(E)smooth[v]\in Rank_{k}(E)_{smooth} is the image of the map

If (E,L)(E,L) is a symmetric (resp. skew symmetric) pair, there is a symmetric (resp. skew symmetric) isomorphism ker⁡Av≃Im Av⊥\ker A_{v}\simeq\textrm{Im\ }A_{v}^{\perp} and the conormal space of Rankk(E)Rank_{k}(E) at vv is given by the image of the map S2(ker⁡Av)→H0(L)S^{2}\left(\ker A_{v}\right)\to H^{0}(L), (resp. ∧2(ker⁡Av)→H0(L)\wedge^{2}\left(\ker A_{v}\right)\to H^{0}(L)).

Let v∈X^v\in\hat{X}, in the proof of Proposition 5.1.1, we saw H0(Iv⊗E)⊆ker⁡AvH^{0}(I_{v}\otimes E)\subseteq\ker A_{v}. In the same way, H0(Iv⊗E∗⊗L)⊆Im Av⊥H^{0}(I_{v}\otimes E^{*}\otimes L)\subseteq\textrm{Im\ }A_{v}^{\perp}, by taking transpose. Equality holds if EE is spanned at x=[v]x=[v]. This is generalized by the following Proposition.

Let v=∑i=1kxi∈Vv=\sum_{i=1}^{k}x_{i}\in V, with [xi]∈X[x_{i}]\in X, and let Z={[x1],…,[xk]}Z=\{[x_{1}],\ldots,[x_{k}]\}. Then

The first inclusion is an equality if H0(E∗⊗L)→H0(E∗⊗L∣Z)H^{0}(E^{*}\otimes L)\to H^{0}(E^{*}\otimes L_{|Z}) is surjective. The second inclusion is an equality if H0(E)→H0(E∣Z)H^{0}(E)\to H^{0}(E_{|Z}) is surjective.

the inclusion for the kernel follows. To see the equality assertion, if H0(E∗⊗L)→H0(E∗⊗L∣Z)H^{0}(E^{*}\otimes L)\to H^{0}(E^{*}\otimes L_{|Z}) is surjective, for every j=1,…,kj=1,\ldots,k we can choose th,j∈H0(E∗⊗L)t_{h,j}\in H^{0}(E^{*}\otimes L), for h=1,…,eh=1,\ldots,e, such that th,j(xi)=0t_{h,j}(x_{i})=0 for i≠ji\neq j, ∀h\forall h and th,jt_{h,j} span the fiber of E∗⊗LE^{*}\otimes L at xjx_{j}. It follows that if s∈ker⁡(Av)s\in\ker(A_{v}) then th,j(xj)⋅s(xj)=0t_{h,j}(x_{j})\cdot s(x_{j})=0 for every h,jh,j which implies s(xj)=0s(x_{j})=0, that is s∈H0(IZ⊗E)s\in H^{0}(I_{Z}\otimes E). The dual statement is similar. ∎

The following theorem gives a useful criterion to find local equations of secant varieties.

Let v=∑i=1rxi∈Vv=\sum_{i=1}^{r}x_{i}\in V and let Z={[x1],…,[xr]}Z=\{[x_{1}],\ldots,[x_{r}]\}, where [xj]∈X[x_{j}]\in X. If

is surjective, then σr(X)\sigma_{r}(X) is an irreducible component of Rankr(E)Rank_{r}(E).

If (E,L)(E,L) is a symmetric, resp. skew-symmetric pair, and

is surjective, then σr(X)\sigma_{r}(X) is an irreducible component of Rankr(E)Rank_{r}(E).

The surjectivity of the map in the first row implies that the rank of map in the second row is at least dim  H0(IZ2⊗L){\rm dim}\;H^{0}(I_{Z^{2}}\otimes L). By Proposition 5.4.1, ker⁡Av⊗Im Av⊥→H0(IZ2⊗L)\ker A_{v}\otimes\textrm{Im\ }A_{v}^{\perp}\to H^{0}(I_{Z^{2}}\otimes L) is surjective, so that the conormal spaces of σk(X)\sigma_{k}(X) and of Rankk(E)Rank_{k}(E) coincide at vv, proving the general case. The symmetric and skew-symmetric cases are analogous. ∎

The induction Lemma

The notion of weak defectivity, which dates back to Terracini, was applied by Ciliberto and Chiantini in to show many cases of tensors and symmetric tensors admitted a unique decomposition as a sum of rank one tensors. We review here it as it is used to prove the promised induction Lemma 6.2.1.

Notational warning: what we call kk-weakly defective is called (k−1)(k-1)-weakly defective in . We shifted the index in order to uniformize to our notion of kk-defectivity: by Terracini’s lemma, kk-defective varieties (i.e., those where dim⁡σk(X)\operatorname{dim}\sigma_{k}(X) is less than the expected dimension) are also kk-weakly defective.

The Veronese varieties which are weakly defective have been classified.

(i) the kk-defective varieties, namely (k,2,n)(k,2,n), k=2,…,(n+22)k=2,\ldots,{{n+2}\choose 2}, (5,4,2)(5,4,2), (9,4,3)(9,4,3), (14,4,4)(14,4,4), (7,3,4)(7,3,4),

If XX is not kk-weakly defective, then it is not k′k^{\prime}-weakly defective for any k′≤kk^{\prime}\leq k. Hence we may assume k′=k−1k^{\prime}=k-1. Consider the projection π\pi of XX centered at the span of k′k^{\prime} general tangent spaces at XX. The image π(X)\pi(X) is not 11-weakly defective, [10, Prop 3.6] which means that the Gauss map of π(X)\pi(X) is nondegenerate [10, Rem. 3.1 (ii)]. Consider the dual variety of π(X)\pi(X), which is contained in the discriminant, see [34, p. 810]. If the dual variety of π(X)\pi(X) were contained in a hyperplane, then π(X)\pi(X) would be a cone (see, e.g. [13, Prop. 1.1]), and thus be 11-weakly defective, which is a contradiction. Hence the linear span of the discriminant variety is the ambient space. ∎

is surjective for general Z′Z^{\prime} of length k′≤kk^{\prime}\leq k.

The analogous results hold in the symmetric and skew-symmetric cases.

It is enough to prove the case when k′=k−1k^{\prime}=k-1. Let s∈H0(IZ′2⊗L)s\in H^{0}(I_{Z^{\prime}}^{2}\otimes L). By the assumption and Proposition 6.1.3 there are sections s1,…,sts_{1},\ldots,s_{t}, with tt at most dim⁡H0(IZ′2⊗L)\operatorname{dim}H^{0}(I_{Z^{\prime}}^{2}\otimes L), with singular points respectively p1,…,ptp_{1},\ldots,p_{t} outside Z′Z^{\prime}, such that s=∑i=1tsis=\sum_{i=1}^{t}s_{i}. Let Zi=Z′∪{pi}Z_{i}=Z^{\prime}\cup\{p_{i}\} for i=1,…,ti=1,\ldots,t. We may assume that the pip_{i} are in general linear position. By assumption sis_{i} is in the image of H0(IZi⊗E)⊗H0(IZi⊗E∗⊗L)⟶ H0(IZi2⊗L)H^{0}(I_{Z_{i}}\otimes E)\otimes H^{0}(I_{Z_{i}}\otimes E^{*}\otimes L)\smash{\mathop{\longrightarrow}\limits^{\ }}H^{0}(I_{Z_{i}^{2}}\otimes L). So all sis_{i} come from H0(IZ′⊗E)⊗H0(IZ′⊗E∗⊗L)H^{0}(I_{Z^{\prime}}\otimes E)\otimes H^{0}(I_{Z^{\prime}}\otimes E^{*}\otimes L). The symmetric and skew-symmetric cases are analogous.∎

Proof of Theorem 1.2.3

By Theorem 5.4.3 it is sufficient to prove the map

is surjective. In the case n=2an=2a, aa odd we have to prove that the map

is surjective. The arguments are similar.

We need the following lemma, whose proof is given below:

Let hi∈V∗h_{i}\in V^{*} be an equation for HiH_{i}. A basis of the space of polynomials of degree 2δ+12{\delta}+1 which are singular on ZZ is given by PI,J:=(∏i∈Ihi)⋅(∏j∈Jhj)P_{I,J}:=\left(\prod_{i\in I}h_{i}\right)\cdot\left(\prod_{j\in J}h_{j}\right) where I,J⊆{1,…δ+n}I,J\subseteq\{1,\ldots{\delta}+n\} are multi-indices (without repetitions) satisfying ∣I∣=δ+1|I|={\delta+1}, ∣J∣=δ|J|={\delta}, and ∣I∩J∣≤δ−1|I\cap J|\leq{\delta}-1 (that is JJ cannot be contained in II).

We prove that the map (15) is surjective for t=(δ+nn)t={{\delta+n}\choose n} by degeneration to the case when the (δ+nn){{\delta+n}\choose n} points are the vertices of a configuration given by the union of δ+n\delta+n general hyperplanes given by linear forms h1,…,hδ+n∈V∗h_{1},\ldots,h_{\delta+n}\in V^{*}.

First consider the case nn is even. For any multi-index I⊂{1,…,δ+n}I\subset\{1,\ldots,\delta+n\} with ∣I∣=δ|I|=\delta write qI=∏k∈Ihk∈H0(O(δ))q_{I}=\prod_{k\in I}h_{k}\in H^{0}({\mathcal{O}}(\delta)) and for any multi-index HH, of length a+1a+1, let sHs_{H} be the section of ∧aQ\wedge^{a}Q represented by the linear subspace of dimension a−1a-1 given by hH={hi=0,i∈H}h_{H}=\{h_{i}=0,i\in H\}. Indeed the linear subspace is a decomposable element of ∧aV=H0(∧aQ)\wedge^{a}V=H^{0}(\wedge^{a}Q). The section sHs_{H} is represented by the Plücker coordinates of hHh_{H}.

The section qIsH∈H0(∧aQ(δ))q_{I}s_{H}\in H^{0}(\wedge^{a}Q(\delta)) vanishes on the reducible variety consisting of the linear subspace hHh_{H} of dimension a−1a-1 and the degree δ\delta hypersurface qI=0q_{I}=0. In particular, if I∩H=∅I\cap H=\emptyset, then qIsH∈H0(IZ⊗∧aQ(δ))q_{I}s_{H}\in H^{0}(I_{Z}\otimes\wedge^{a}Q(\delta)).

Let I=I0∪{u}I=I_{0}\cup\{u\} with ∣I0∣=δ|I_{0}|=\delta, consider ∣J∣=δ|J|=\delta such that u∉Ju\notin J and ∣I∩J∣≤δ−1|I\cap J|\leq\delta-1. It is possible to choose K1,K2K_{1},K_{2} such that ∣K1∣=∣K2∣=a|K_{1}|=|K_{2}|=a and such that K1∩K2=K1∩I=K2∩J=∅K_{1}\cap K_{2}=K_{1}\cap I=K_{2}\cap J=\emptyset.

We get qI0s{u}∪K1∧qJs{u}∪K2q_{I_{0}}s_{\{u\}\cup K_{1}}\wedge q_{J}s_{\{u\}\cup K_{2}} is the degree 2δ+12\delta+1 hypersurface qI0qJhu=qIqJq_{I_{0}}q_{J}h_{u}=q_{I}q_{J}. By Lemma 7.0.1 these hypersurfaces generate H0(IZ2(2δ+1))H^{0}(I_{Z}^{2}(2\delta+1)). Hence WZW_{Z} is surjective and the result is proved in the case nn is even.

When nn is odd, the morphism AϕA_{\phi} is represented by a rectangular matrix, and it induces a map B ⁣:H0(∧aQ(δ))⊗H0(∧n−aQ(δ))→H0(O(2δ+1))B\colon H^{0}(\wedge^{a}Q(\delta))\otimes H^{0}(\wedge^{n-a}Q(\delta))\to H^{0}({\mathcal{O}}(2\delta+1)).

For any multi-index HH, of length n−a+1n-a+1, let sHs_{H} be the section of ∧aQ\wedge^{a}Q represented by the linear subspace of dimension a−1a-1 given by hH={hi=0,i∈H}h_{H}=\{h_{i}=0,i\in H\}. Indeed the linear subspace is a decomposable element of ∧aV=H0(∧aQ)\wedge^{a}V=H^{0}(\wedge^{a}Q). The section sHs_{H} is represented by the Plücker coordinates of hHh_{H}.

The section qIsH∈H0(∧aQ(δ))q_{I}s_{H}\in H^{0}(\wedge^{a}Q(\delta)) vanishes on the reducible variety consisting of the linear subspace hHh_{H} of dimension a−1a-1 and the degree δ\delta hypersurface qIq_{I}. In particular, if I∩H=∅I\cap H=\emptyset, then qIsH∈H0(IZ⊗∧aQ(δ))q_{I}s_{H}\in H^{0}(I_{Z}\otimes\wedge^{a}Q(\delta)).

Let I=I0∪{u}I=I_{0}\cup\{u\} with ∣I0∣=δ|I_{0}|=\delta, consider ∣J∣=δ|J|=\delta such that u∉Ju\notin J and ∣I∩J∣≤δ−1|I\cap J|\leq\delta-1. The modification to the above proof is that it is possible to choose K1,K2K_{1},K_{2} such that ∣K1∣=n−a=a+1|K_{1}|=n-a=a+1, ∣K2∣=a|K_{2}|=a and such that K1∩K2=K1∩I=K2∩J=∅K_{1}\cap K_{2}=K_{1}\cap I=K_{2}\cap J=\emptyset.

Then qI0s{u}∪K1∈H0(∧a+1Q(δ))q_{I_{0}}s_{\{u\}\cup K_{1}}\in H^{0}(\wedge^{a+1}Q(\delta)), qJs{u}∪K2∈H0(∧aQ(δ))q_{J}s_{\{u\}\cup K_{2}}\in H^{0}(\wedge^{a}Q(\delta)),

and qI0s{u}∪K1∧qJs{u}∪K2q_{I_{0}}s_{\{u\}\cup K_{1}}\wedge q_{J}s_{\{u\}\cup K_{2}} is the degree 2δ+12\delta+1 hypersurface qI0qJhu=qIqJq_{I_{0}}q_{J}h_{u}=q_{I}q_{J}. By Lemma 7.0.1 these hypersurfaces generate H0(IZ2(2δ+1))H^{0}(I_{Z}^{2}(2\delta+1)). Hence the map (15) is surjective and the result is proved.

We begin by discussing properties of the hypersurfaces through ZZ, which may be of independent interest.

(i) For d≥δd\geq{\delta}, the products ∏i∈Ihi\prod_{i\in I}h_{i} for every I⊆{1,…,n+δ}I\subseteq\{1,\ldots,n+{\delta}\} such that ∣I∣=d|I|=d are independent in SdV∗S^{d}V^{*}.

(ii) For d≤δd\leq{\delta}, the products ∏i∈Ihi\prod_{i\in I}h_{i} for every I⊆{1,…,n+δ}I\subseteq\{1,\ldots,n+{\delta}\} such that ∣I∣=d|I|=d span SdV∗S^{d}V^{*}.

Write hI=∏∈Ihih_{I}=\prod_{\in I}h_{i}. Consider a linear combination ∑IaIhI=0\sum_{I}a_{I}h_{I}=0. Let d≥δd\geq{\delta}. If d≥n+δd\geq n+\delta the statement is vacuous, so assume d<n+δd<n+\delta. For each I0I_{0} such that ∣I0∣=d|I_{0}|=d there is a point P0∈VP_{0}\in V such that hi(P0)=0h_{i}(P_{0})=0 for i∉I0i\notin I_{0} and hi(P0)≠0h_{i}(P_{0})\neq 0 for i∈I0i\in I_{0}. The equality ∑IaIhI(P0)=0\sum_{I}a_{I}h_{I}(P_{0})=0 implies aI0=0a_{I_{0}}=0, proving (i). For d=δd={\delta}, (ii) follows as well by counting dimensions, as dim⁡SδV∗=(δ+nn)\operatorname{dim}S^{\delta}V^{*}={{{\delta}+n}\choose n}. For d≤δ−1d\leq{\delta}-1 pick f∈SdV∗f\in S^{d}V^{*}. By the case already proved, there exist coefficients aIa_{I}, bJb_{J} such that

where the first sum is over all II with ∣I∣=δ|I|={\delta} such that {1,…,δ−d}⊆I\{1,\ldots,{\delta}-d\}\subseteq I and the second sum over all JJ with ∣J∣=δ|J|={\delta} such that {1,…,δ−d}⊈J\{1,\ldots,{\delta}-d\}\not\subseteq J.

For every J0J_{0} such that ∣J0∣=δ|J_{0}|={\delta} and {1,…,δ−d}⊈J0\{1,\ldots,{\delta}-d\}\not\subseteq J_{0} there is a (unique) point [P0][P_{0}] such that hi(P0)=0h_{i}(P_{0})=0 for i∉J0i\notin J_{0} and hi(P0)≠0h_{i}(P_{0})\neq 0 for i∈J0i\in J_{0}. In particular ∏i=1δ−dhi(P0)=0\prod_{i=1}^{{\delta}-d}h_{i}(P_{0})=0 and substituting P0P_{0} into (17) shows bJ0=0b_{J_{0}}=0, for each J0J_{0}. Thus

and dividing both sides by ∏i=1δ−dhi\prod_{i=1}^{{\delta}-d}h_{i} proves (ii). ∎

Recall that the subspace of SdV∗S^{d}V^{*} of polynomials which pass through pp points and are singular through qq points has codimension ≤min⁡((n+dn),p+q(n+1))\leq\min\left({{n+d}\choose n},p+q(n+1)\right). When equality holds one says that the conditions imposed by the points are independent and that the subspace has the expected codimension.

(i) H0(IZ(d))=0H^{0}(I_{Z}(d))=0 if d≤δd\leq{\delta}.

(ii) H0(IZ(δ+1))H^{0}(I_{Z}({\delta+1})) has dimension (δ+nδ+1){{{\delta}+n}\choose{\delta+1}} and it is generated by the products hIh_{I} with ∣I∣=δ+1|I|={\delta}+1.

Since ZZ is finite, dim⁡H0(OZ(d))=(δ+nn)=deg⁡Z\operatorname{dim}H^{0}({\mathcal{O}}_{Z}(d))={{{\delta}+n}\choose n}=\deg Z for every dd.

In order to prove (ii), consider the products hIh_{I} with ∣I∣=δ+1|I|={\delta}+1, which are independent by Proposition 7.0.2.i, so they span a (δ+nδ+1){{{\delta}+n}\choose{\delta+1}}-dimensional subspace of H0(IZ(δ+1))H^{0}(I_{Z}({\delta}+1)).

The long exact sequence in cohomology implies

Notations as above. Let L0⊂{1,…,n+δ}L_{0}\subset\{1,\ldots,n+\delta\} have cardinality nn.

The space of polynomials of degree δ+1{\delta}+1 which pass through the points yLy_{L} and are singular at yL0y_{L_{0}} has a basis given by the products ∏i∈Jhi\prod_{i\in J}h_{i} for every J⊆{1,…,n+δ}J\subseteq\{1,\ldots,n+{\delta}\} such that ∣J∣=δ+1|J|={\delta}+1 and #(J∩L0)≥2\#\left(J\cap L_{0}\right)\geq 2. This space has the expected codimension (δ+nn)+n\binom{\delta+n}{n}+n.

Note that if ∣J∣=δ+1|J|={\delta}+1 then #(J∩L0)≥1\#\left(J\cap L_{0}\right)\geq 1 and equality holds just for the nn products hihL0ch_{i}h_{L_{0}^{c}} for i∈L0i\in L_{0}, where L0c={1,…,n+δ}\L0L_{0}^{c}=\{1,\ldots,n+\delta\}\backslash L_{0}. Every linear combination of the hJh_{J} which has a nonzero coefficient in these nn products is nonsingular at [yL0][y_{L_{0}}].

Hence the products which are different from these nn generate the space of polynomials of degree δ+1{\delta}+1 which pass through the points [yL][y_{L}] and are singular at [yL0][y_{L_{0}}].

There are (δ+nn−1)−n{{{\delta}+n}\choose{n-1}}-n such polynomials, which is the expected number (δ+n+1n)−(n+1)−[(δ+nn)−1]{{{\delta}+n+1}\choose n}-(n+1)-\left[{{{\delta}+n}\choose n}-1\right]. Since the codimension is always at most the expected one, it follows that these generators give a basis. ∎

In the remainder of this section, we use products hIh_{I} where II is a multi-index where repetitions are allowed. Given such a multi-index I={i1,…,i∣I∣}I=\{i_{1},\ldots,i_{|I|}\}, we write hI=h1k1⋯hn+δkn+δh_{I}=h_{1}^{k_{1}}\cdots h_{n+\delta}^{k_{n+\delta}}, where jj appears kjk_{j} times in II and we write ∣I∣=k1+⋯+kn+δ|I|=k_{1}+\cdots+k_{n+\delta}. The support s(I)s(I) of a multi-index II is the set of j⊂{1,…,n+δ}j\subset\{1,\ldots,n+\delta\} with kj>0k_{j}>0.

An immediate consequence of (ii) and (iii) of Proposition 7.0.3 is:

For d≥δ+1d\geq{\delta}+1, the vector space H0(IZ(d))H^{0}(I_{Z}(d)) is generated by the monomials hIh_{I} with ∣I∣=d|I|=d and ∣s(I)∣≥δ+1|s(I)|\geq{\delta}+1.

The space of polynomials of degree 2δ+12{\delta}+1 which contain ZZ is generated by products hIh_{I} with ∣I∣=2δ+1|I|=2\delta+1, ∣s(I)∣≥δ+1|s(I)|\geq{\delta}+1, and all the exponents in hIh_{I} are at most 22.

By Corollary 7.0.5, it just remains to prove the statement about the exponents. Let hI=∏i=1δ+nhikih_{I}=\prod_{i=1}^{{\delta}+n}h_{i}^{k_{i}} and let nj(I)=#{i∣ki=j}n_{j}(I)=\#\{i|k_{i}=j\} for j=0,…,2δ+1j=0,\ldots,2{\delta}+1. Hence ∑j≥1jnj(I)=2δ+1\sum_{j\geq 1}jn_{j}(I)=2{\delta}+1 and ∑j≥1nj(I)≥δ+1\sum_{j\geq 1}n_{j}(I)\geq{\delta}+1.

Assume that γ:=∑j≥3nj(I)>0\gamma:=\sum_{j\geq 3}n_{j}(I)>0. It is enough to show that hI=∑cJhJh_{I}=\sum c_{J}h_{J} where every JJ which appears in the sum satisfies ∣s(J)∣≥δ+1|s(J)|\geq{\delta}+1, ∣J∣=2δ+1|J|=2{\delta}+1 and ∑j≥3nj(J)<γ\sum_{j\geq 3}n_{j}(J)<\gamma.

that is, n2(I)+γ≤δ−γ≤δ−1n_{2}(I)+\gamma\leq{\delta}-\gamma\leq{\delta}-1. Hence there at least n+1n+1 forms hih_{i} which appear with exponent at most one in hIh_{I}. We can express all the remaining forms hsh_{s} as linear combinations of these n+1n+1 forms. By expressing a form with exponent at least 33 as linear combination of these n+1n+1 linear forms hih_{i}, we get hI=∑cJhJh_{I}=\sum c_{J}h_{J} where each summand has the required properties. ∎

For k=0,…,δk=0,\ldots,{\delta}, let Iδ,k,nI_{{\delta},k,n} be the linear system of hypersurfaces of degree 2δ+1−k2{\delta}+1-k which contain ZZ and are singular on the points of ZZ which lie outside ∪i=1kHi\cup_{i=1}^{k}H_{i}. The space Iδ,k,nI_{{\delta},k,n} has the expected codimension (n+1)(δ+nn)−n∑i=1k(δ+n−in−1)(n+1){{{\delta}+n}\choose n}-n\sum_{i=1}^{k}{{{\delta}+n-i}\choose{n-1}} .

For k=δk={\delta} the assertion is Proposition 7.0.4 with L0={δ+1,…,δ+n}L_{0}=\{\delta+1,\ldots,\delta+n\}. We work by induction on nn and by descending induction on kk (for fixed δ{\delta}). We restrict to the last hyperplane Hδ+nH_{{\delta}+n}.

Let Vδ,k+1,n⊇Iδ,k+1,nV_{{\delta},k+1,n}\supseteq I_{{\delta},k+1,n} denote the set of hypersurfaces of degree 2δ−k2{\delta}-k which pass through Z∖{Hδ+n∩(∪i=1kHi)}Z\setminus\{H_{{\delta}+n}\cap\left(\cup_{i=1}^{k}H_{i}\right)\} and are singular on the points of ZZ which lie outside (∪i=1kHi)∪{Hδ+n}\left(\cup_{i=1}^{k}H_{i}\right)\cup\{H_{{\delta}+n}\}. We have the exact sequence

Since by induction Iδ,k+1,nI_{{\delta},k+1,n} has the expected codimension in S2δ−kV∗S^{2{\delta}-k}V^{*} it follows that also Vδ,k+1,nV_{{\delta},k+1,n} has the expected codimension

because the conditions imposed by Vδ,k+1,nV_{{\delta},k+1,n} are a subset of the conditions imposed by Iδ,k+1,nI_{{\delta},k+1,n} and a subset of a set of independent conditions still consists of independent conditions.

The following Corollary proves Lemma 7.0.1.

The statement about the codimension is the case k=0k=0 of Proposition 7.0.7. Note that every product hIh_{I} with II such that ∣I∣=2δ+1|I|=2{\delta}+1 and s(I)≥δ+2s(I)\geq{\delta}+2 is singular at any P∈ZP\in Z because hIh_{I} contains at least two factors which vanish at PP. Let ff be a homogeneous polynomial of degree 2δ+12{\delta}+1 which is singular on ZZ. By Proposition 7.0.6 we have the decomposition f=∑∣s(I)∣≥δ+2aIhI+∑∣s(I)∣=δ+1bIhIf=\sum_{|s(I)|\geq{\delta}+2}a_{I}h_{I}+\sum_{|s(I)|={\delta+1}}b_{I}h_{I}, where all the exponents are at most 22. Let I0I_{0} be in the second summation with ∣s(I0)∣=δ+1|s(I_{0})|={\delta}+1. There is a unique hih_{i} appearing in hI0h_{I_{0}} with exponent 11 and n−1n-1 hyperplanes appearing with exponent . Let P0P_{0} be the point where these 1+(n−1)=n1+(n-1)=n hyperplanes meet. It follows that hI0h_{I_{0}} is nonsingular at P0P_{0} while, for all the other summands, hIh_{I} is singular in P0P_{0}. It follows that bI0=0b_{I_{0}}=0 and f=∑∣s(I)∣≥δ+2aIhIf=\sum_{|s(I)|\geq{\delta}+2}a_{I}h_{I} as we wanted. ∎

This map between larger, but more elementary, spaces has the same rank properties as the map Sδ+1,1n−aV∗→Sδ+1,1aVS_{\delta+1,1^{n-a}}V^{*}\rightarrow S_{\delta+1,1^{a}}V, because when one decomposes the spaces in this map as SL(V)SL(V)-modules, the other module maps are zero.

The vector bundle E=∧aQ(δ)E{=\wedge^{a}Q(\delta)} may be recovered as the image of the map

2. The general case

The key is to realize EE as the image of a map

where the LiL_{i} are direct sums of powers of MM and

By construction, for x∈X^x\in\hat{X}, rank(pE(x))=e{\rm rank}(p_{E}(x))=e. Let v∈V=H0(X,L)∗v\in V=H^{0}(X,L)^{*}. Compose the map H0(L0)⊗H0(L)∗→H0(L0∗⊗L)∗H^{0}(L_{0})\otimes H^{0}(L)^{*}\to H^{0}(L_{0}^{*}\otimes L)^{*} with the map on sections induced from pEp_{E}, to obtain

for some finite set of natural numbers a1i,a2ia^{i}_{1},a^{i}_{2}. For the examples in this paper there is just one term in the summand, e.g., in §8.1, L1=O(δ)⊕(n+1a)L_{1}={\mathcal{O}}(\delta)^{\oplus\binom{n+1}{a}}, L0=O(δ+1)⊕(n+1a+1)L_{0}={\mathcal{O}}(\delta+1)^{\oplus\binom{n+1}{a+1}}.

Let L1=⊕j=1m1O(bj)L_{1}=\oplus_{j=1}^{m_{1}}{\mathcal{O}}(b_{j}) and L0=⊕i=1m0O(ai)L_{0}=\oplus_{i=1}^{m_{0}}{\mathcal{O}}(a_{i}). Let pij∈Sai−bjW∗p_{ij}\in S^{a_{i}-b_{j}}W^{*} denote the map O(bj)→O(ai){\mathcal{O}}(b_{j})\rightarrow{\mathcal{O}}(a_{i}), given by the composition

Then, for any ϕ∈SdW\phi\in S^{d}W, PvE(ϕ)P_{v}^{E}(\phi) is obtained by taking a matrix of m1×m0m_{1}\times m_{0} blocks with the (i,j)(i,j)-th block a matrix representing the catalecticant ϕbj,d−ai∈SbjW∗⊗Sd−aiW∗⊗SdW\phi_{b_{j},d-a_{i}}\in S^{b_{j}}W^{*}\otimes S^{d-a_{i}}W^{*}\otimes S^{d}W contracted by pijp_{ij} so the new matrix is of size h0(L0∗⊗L)×h0(L1)h^{0}(L_{0}^{*}\otimes L)\times h^{0}(L_{1}) with scalar entries. See Examples 1.2.1 and 8.4.4 for explicit examples.

4. Rank and irreducible component theorems in the presentation setting

Under mild assumptions, the following proposition shows that PvEP_{v}^{E} can be used in place of AvEA_{v}^{E} in the theorems of §5.

Notations as above. Assume that H0(L1)⟶iH0(E)H^{0}(L_{1})\smash{\mathop{\longrightarrow}\limits^{i}}H^{0}(E) and H0(L0∗⊗L)⟶jH0(E∗⊗L)H^{0}(L_{0}^{*}\otimes L)\smash{\mathop{\longrightarrow}\limits^{j}}H^{0}(E^{*}\otimes L) are surjective.

Then the rank of AvEA_{v}^{E} equals the rank of PvEP_{v}^{E}, so that the size (ke+1)(ke+1)-minors of PvEP_{v}^{E} give equations for σk(X)\sigma_{k}(X).

If (E,L)(E,L) is a symmetric (resp. skew-symmetric) pair then there exists a symmetric (resp. skew-symmetric) presentation where L1≃L0∗⊗LL_{1}\simeq L_{0}^{*}\otimes L and PvEP_{v}^{E} is symmetric (resp. skew-symmetric).

The assumptions ii is surjective and jtj^{t} is injective imply rank(Av)=rank(Pv){\rm rank}(A_{v})={\rm rank}(P_{v}). The symmetric and skew assertions are clear.

With the assumptions of Proposition 8.4.1, the natural map

is surjective and the affine conormal space at vv is the image of ker⁡Pv⊗(Im Pv)⊥→H0(L)\ker P_{v}\otimes{\left(\textrm{Im\ }P_{v}\right)^{\perp}}\to H^{0}(L).

The following variant of Proposition 5.1.1 is often easy to implement in practice.

Notations as above. Let v∈σk(X)v\in\sigma_{k}(X). Assume the maps H0(L1)⟶H0(E)H^{0}(L_{1})\smash{\mathop{\longrightarrow}\limits}H^{0}(E) and H0(L0∗⊗L)⟶H0(E∗⊗L)H^{0}(L_{0}^{*}\otimes L)\smash{\mathop{\longrightarrow}\limits}H^{0}(E^{*}\otimes L) are surjective.

(i) If the rank of ker⁡Pv⊗(Im Pv)⊥⟶gH0(L)\ker P_{v}\otimes{\left(\textrm{Im\ }P_{v}\right)^{\perp}}\smash{\mathop{\longrightarrow}\limits^{g}}H^{0}(L) at vv equals the codimension of σk(X)\sigma_{k}(X), then σk(X)\sigma_{k}(X) is an irreducible component of Rankk(E)Rank_{k}(E) passing through vv.

(ii) If (E,L)(E,L) is a symmetric (resp. skew-symmetric) pair, assume that the rank of S2(ker⁡Pv)→H0(L)S^{2}\left(\ker P_{v}\right)\to H^{0}(L) (resp. of ∧2(ker⁡Pv)→H0(L)\wedge^{2}\left(\ker P_{v}\right)\to H^{0}(L)) at vv coincides with the codimension of σk(X)\sigma_{k}(X).

Then σk(X)\sigma_{k}(X) is an irreducible component of Rankk(E)Rank_{k}(E) passing through vv.

Note that in the skew-symmetric case, Rankk(E)Rank_{k}(E) is defined by sub-Pfaffians.

In Theorem 8.4.2, the rank of the maps is always bounded above by the codimension of σk(X)\sigma_{k}(X), as the rank of the maps is equal to the dimension of the conormal space of Rankk(E)Rank_{k}(E) at vv.

The previous theorem can be implemented in concrete examples. Indeed the pairing gg, appearing in the theorem, can be described as follows: given f∈ker⁡Pv⊂H0(L1)f\in\ker P_{v}\subset H^{0}(L_{1}), h∈(Im Pv)⊥⊂H0(L0∗⊗L)h\in{\left(\textrm{Im\ }P_{v}\right)^{\perp}}\subset H^{0}(L_{0}^{*}{\mathord{\otimes}}L), and ϕ∈H0(L)∗\phi\in H^{0}(L)^{*}, one has g(f,h)(ϕ)=h[Pϕ(f)]g(f,h)(\phi)=h[P_{\phi}(f)].

Note that when ϕ=x03\phi=x_{0}^{3} is a cube, then the rank of AϕEA_{\phi}^{E} and the rank of PϕP_{\phi} are both equal to 66, which is the rank of Ω2(3)\Omega^{2}(3).

Decomposition of polynomials into a sum of powers

Having a presentation for EE enables one to reduce the problem of decomposing a polynomial into a sum of powers to a problem of solving a system of polynomial equations (sometimes linear) as we explain in this section. We begin with a classical example:

For ϕ∈SdW\phi\in S^{d}W, let δ=⌊d−12⌋\delta=\lfloor\frac{d-1}{2}\rfloor, a=⌊n2⌋a=\lfloor\frac{n}{2}\rfloor, k≤(δ+nn)k\leq{{\delta+n}\choose n} and take E=∧aQ(δ)E=\wedge^{a}Q(\delta), so Aϕ ⁣:H0(∧aQ(δ))→H0(∧n−aQ(d−δ))A_{\phi}\colon H^{0}(\wedge^{a}Q(\delta))\to H^{0}(\wedge^{n-a}Q(d-\delta)), then ker⁡Aϕ=H0(IZ⊗∧aQ(δ))\ker A_{\phi}=H^{0}(I_{Z}\otimes\wedge^{a}Q(\delta)) so that ZZ can be recovered as the base locus of ker⁡Aϕ\ker A_{\phi}.

Let E=Q(2)E={Q(2)} and consider the skew-symmetric morphism AϕE ⁣:H0(Q(2))→H0(Q(2))∗A_{\phi}^{E}\colon H^{0}(Q(2))\to H^{0}(Q(2))^{*}. (Note that H0(Q(2))=S3,2VH^{0}(Q(2))=S_{3,2}V as an SL3SL_{3}-module, and that has dimension 1515.) For a general ϕ\phi the kernel of AϕA_{\phi} has dimension one and we let s∈H0(Q(2))s\in H^{0}(Q(2)) denote a section spanning it. By Proposition 5.4.1, the seven points where ss vanishes correspond to the seven summands. Explicitly, ss corresponds to a morphism f ⁣:S2W→Wf\colon S^{2}W\to W such that the set {v∈W∣f(v2)∈<v>}\{v\in W|f(v^{2})\in<v>\} consists of the seven points P1,…,P7P_{1},\ldots,P_{7}.

One way to describe the seven points is to consider the map

where the qjq_{j} are of degree two. In practice this system is easily solved with, e.g. Maple.

Grassmannians

The case k=2k=2 is well known, I(σr(G(2,W)))I(\sigma_{r}(G(2,W))) is generated in degree r+1r+1 by sub-Pfaffians of size 2r+22r+2.

Now let [E1+E2]∈σ2(G(k,W))[E_{1}+E_{2}]\in\sigma_{2}(G(k,W)). By Terracini’s lemma N^[E1+E2]∗G(k,W)=N^E1∗G(k,W)∩N^E2∗G(k,W)\hat{N}^{*}_{[E_{1}+E_{2}]}G(k,W)=\hat{N}^{*}_{E_{1}}G(k,W)\cap\hat{N}^{*}_{E_{2}}G(k,W). Let U12=E1⊥∩E2⊥U_{12}=E_{1}{}^{\perp}\cap E_{2}{}^{\perp}, and Uj=Ej⊥U_{j}=E_{j}{}^{\perp}. We have

To see this, note that each term must contain a ∧2(E1⊥)\wedge^{2}(E_{1}{}^{\perp}) and a ∧2(E2⊥)\wedge^{2}(E_{2}{}^{\perp}). The notation is designed so that ∧2(Ej⊥)\wedge^{2}(E_{j}{}^{\perp}) will appear if the jj index occurs at least twice in the UU’s. Similarly below, one takes all combinations of UU’s such that each of 1,2,31,2,3 appears twice in the expression.

We emphasize that with four or more subspaces analogous formulas are much more difficult, because four subspaces have moduli, see .

We now determine to what extent the zero sets of the skew-flattenings provide local equations for secant varieties of Grassmannians.

The first skew-flattening ∧kW⊂W⊗∧k−1W\wedge^{k}W\subset W{\mathord{\otimes}}\wedge^{k-1}W gives rise to the subspace varieties: let

it admits a description via a Kempf-Weyman “collapsing” of the vector bundle ∧kSp→G(p,W)\wedge^{k}{\mathcal{S}}_{p}\rightarrow G(p,W), where Sp{\mathcal{S}}_{p} is the tautological rank pp subspace bundle, i.e., the variety is the projectivization of the image of the total space of ∧kSp\wedge^{k}{\mathcal{S}}_{p} in ∧kW\wedge^{k}W. From this description one sees that Subp(∧kW)Sub_{p}(\wedge^{k}W) is of dimension p(n+1−p)+(pk)p(n+1-p)+\binom{p}{k} and its affine conormal space at a smooth point z∈∧kW′⊂∧kWz\in\wedge^{k}W^{\prime}\subset\wedge^{k}W is

Question

In what cases do the minors of the skew-flattenings generate the ideal of Subp(∧kW)Sub_{p}(\wedge^{k}W)?

The most relevant cases for the study of secant varieties of Grassmannians are when p=rkp=rk, as σr(G(k,W))⊂Subrk(∧kW)\sigma_{r}(G(k,W))\subset Sub_{rk}(\wedge^{k}W). Note that in general σr(G(k,W))\sigma_{r}(G(k,W)) is a much smaller subvariety than Subrk(∧kW)Sub_{rk}(\wedge^{k}W).

Now we compute ker⁡⊗Image⁡⊥\operatorname{ker}{\mathord{\otimes}}\operatorname{Image}{}^{\perp}:

For E∈G(k,W)E\in G(k,W), write Ep,k−p:∧pW∗→∧k−pWE_{p,k-p}:\wedge^{p}W^{*}\rightarrow\wedge^{k-p}W for the flattening. Then

which agrees with (19). (Note that if we had tried the (1,k−1)(1,k-1)-flattening, we would have missed the third term in (19).)

and ker⁡⊗Image⁡⊥\operatorname{ker}{\mathord{\otimes}}\operatorname{Image}{}^{\perp} does not contain last term in (20) if it is nonzero. However when we consider the (3,k−3)(3,k-3) flattening we will recover the full conormal space. In general, we obtain:

This theorem does not extend to σ4(G(k,W))\sigma_{4}(G(k,W)) because there it is possible to have e.g., sums of vectors in pairwise intersections of spaces that add to a vector in a triple intersection, which does not occur for the third secant variety.

We expect the situation to be similar to that of Veronese varieties, where for small secant varieties skew flattenings provide enough equations to cut out the variety, then for a larger range of rr the secant variety is an irreducible component of the variety of skew flattenings, and then for larger rr more equations will be needed.

2. Skew-inheritance

Equations (set-theoretic, scheme-theoretic or ideal theoretic) for σr(G(k,W))\sigma_{r}(G(k,W)) for dim⁡W>kr\operatorname{dim}W>{kr} are given by

the modules inherited from the ideal of σr(G(k,kr))\sigma_{r}(G(k,{kr})),

and the modules generating the ideal of Subkr(∧kW)Sub_{kr}(\wedge^{k}W).

Homogeneous varieties G/P𝐺𝑃G/P

2. Example: Strassen’s equations

3. Inheritance from usual Grassmannians

For example, in the case Dn/Pn−2D_{n}/P_{n-2}, Vωn−2V_{\omega_{n-2}} is a submodule of ∧2Vωn,∧2Vωn−1\wedge^{2}V_{\omega_{n}},\wedge^{2}V_{\omega_{n-1}} and ∧n−2Vω1\wedge^{n-2}V_{\omega_{1}}.

In the case of the EE series we have inclusions

Here, in each case the vector bundle EE has rank two, so we obtain minimal degree equations for the secant varieties of En/P3,En/P4,En/Pn−1E_{n}/P_{3},E_{n}/P_{4},E_{n}/P_{n-1}. The dimension of H0(E)H^{0}(E) for (e6,e7,e8)({\mathfrak{e}}_{6},{\mathfrak{e}}_{7},{\mathfrak{e}}_{8}) is respectively: (2727, 133133, 38753875) for ω3\omega_{3}, (7878, 912912, 147250147250) for ω4\omega_{4}, and (2727, 5656, 248248) for ωn−1\omega_{n-1}.

4. Other cases

References