On secant varieties of Compact Hermitian Symmetric Spaces

J. M. Landsberg, Jerzy Weyman

Introduction

If the ideal of a variety XX is generated in degree two, the minimal possible degree of generators for the ideal of σ(X)\sigma(X) is three ( Cor. 3.2), although in general one does not expect generators in degree three (e.g. this almost always fails for complete intersections of quadrics). On the other hand, when XX is homogeneous, i.e., VV is an irreducible GG-module where GG is a a semisimple algebraic group and XX is the orbit of a highest weight line (so in particular, the ideal of XX is generated in degree two), in all previously known examples (mostly just the rank two compact Hermitian symmetric spaces), the ideal of σ(X)\sigma(X) was generated in degree three.

In this paper we determine the generators of the ideals of the secant varieties of rank three compact Hermitian symmetric spaces in their minimal homogeneous embeddings, which we abbreviate CHSS. There is one suprise, the ideal of the secant variety of the D7D_{7} spinor variety is not generated in degree three, which answers a question posed in , Section 3. Recently, L. Manivel has made significant progress towards determining the generators of the ideals of secant varieties of spinor varieties in general, see .

While determining the generators of the ideals of secant varieties of higher rank CHSS seems out of reach at the moment, we show that for all other CHSS other than spinor varieties, there are indeed generators in degree three. Moreover

For a vector space AA, let KS(A)⊂A ⊗ 3K_{S}(A)\subset A^{{\mathord{\,\otimes}\,}3} denote the kernel of the symmetrization map S2A ⊗ A  →  S3AS^{2}A{\mathord{\,\otimes}\,}A{\mathord{\;\rightarrow\;}}S^{3}A, it is a GL(A)GL(A)-module isomorphic to S21AS_{21}A. We let πS:(A ⊗ B) ⊗ 3  →  (A ⊗ B) ⊗ 3\pi_{S}:(A{\mathord{\,\otimes}\,}B)^{{\mathord{\,\otimes}\,}3}{\mathord{\;\rightarrow\;}}(A{\mathord{\,\otimes}\,}B)^{{\mathord{\,\otimes}\,}3} denote the symmetrization map whose image is S3(A ⊗ B)S^{3}(A{\mathord{\,\otimes}\,}B).

The degree three statement in Theorem 1.4 is a consequence of the more general result:

Theorem 1.4 and Proposition 1.5 are proven in §7.

For higher rank irreducible CHSS we have the following result, which is proved in §3:

In it is shown that D7/P7,D8/P8D_{7}/P_{7},D_{8}/P_{8} are the only spinor varieties whose secant varieties have empty ideal in degree three, thus these are the only CHSS in not having cubics in the ideal of its secant variety. (Segre products and Veronese re-embeddings of any varieties contain cubics in the ideals of their secant varieties as there are cubics in the ideals of the Segre products and Veronese embeddings of projective spaces.)

We obtain our results using the methods of , as described in Theorem 2.1 below, along with some new results about induced representations. In brief, in each case we obtain a desingularization of σ(X)\sigma(X), by exploiting that fact that each XX has a Legendrian “smaller cousin”, and apply Weyman’s method to this desingularization.

When dealing with an\mathfrak{a}_{n}-modules we sometimes use partitions to index highest weights, with the dictionary π=(p1,...,pn+1)\pi=(p_{1},...,p_{n+1}) corresponds to the weight (p1−p2)ω1+(p2−p3)ω2+⋯+(pn−pn+1)ωn(p_{1}-p_{2})\omega_{1}+(p_{2}-p_{3})\omega_{2}+\cdots+(p_{n}-p_{n+1})\omega_{n}. We write SπKnS_{\pi}K^{n} for the associated module. Sometimes we abbreviate a partition (i1,...,i1,i2,...,i2,...,ik,...,ik)=((i1)a1,(i2)a2,...,(ik)ak)(i_{1},...,i_{1},i_{2},...,i_{2},...,i_{k},...,i_{k})=((i_{1})^{a_{1}},(i_{2})^{a_{2}},...,(i_{k})^{a_{k}}) where isi_{s} occurs asa_{s} times.

Acknowledgments

We thank W. Kraśkiewicz and C. Robles for significant help with computer calculations and L. Manivel for pointing out and correcting an error in an earlier version of this paper.

Method of proof

If the sheaf cohomology groups Hi(B,Sdη)H^{i}({\mathcal{B}},S^{d}\eta) are all zero for i>0i>0 and d>0d>0 and if the linear maps H0(B,Sdη) ⊗ V∗  →  H0(B,Sd+1η)H^{0}({\mathcal{B}},S^{d}\eta){\mathord{\,\otimes}\,}V^{*}{\mathord{\;\rightarrow\;}}H^{0}({\mathcal{B}},S^{d+1}\eta) are surjective for all d≥0d\geq 0, then

Y^\hat{Y} is normal, with rational singularities

The coordinate ring K[Y^]K[\hat{Y}] satisfies K[Y^]d≃H0(B,Sdη)K[\hat{Y}]_{d}\simeq H^{0}({\mathcal{B}},S^{d}\eta).

The vector space of minimal generators of the ideal of YY in degree dd is isomorphic to Hd−1(B,Λdξ)H^{d-1}({\mathcal{B}},\Lambda^{d}\xi) which is also the homology of the complex

More generally, ⊕jHj(B,Λi+jξ)\oplus_{j}H^{j}({\mathcal{B}},\Lambda^{i+j}\xi) is isomorphic to the ii-th term in the minimal free resolution of YY.

If moreover YY is a GG-variety and the desingularization is GG-equivariant, then the identifications above are as GG-modules.

2. The basic theorem applies in our case

Notations as above, if YY is a GG variety, B=G/P{\mathcal{B}}=G/P and η\eta is induced from an irreducible PP-module, then the sheaf cohomology groups Hi(B,Sdη)H^{i}({\mathcal{B}},S^{d}\eta) are all zero for i>0i>0 and the linear maps H0(B,Sdη) ⊗ V∗  →  H0(B,Sd+1η)H^{0}({\mathcal{B}},S^{d}\eta){\mathord{\,\otimes}\,}V^{*}{\mathord{\;\rightarrow\;}}H^{0}({\mathcal{B}},S^{d+1}\eta) are surjective for all d≥0d\geq 0. In particular all the conclusions of 2.1 apply.

An irreducible homogeneous bundle can have nonzero cohomology in at most one degree, but a quotient bundle of a trivial bundle has nonzero sections, thus H0(B,η)H^{0}(B,\eta) is a nonzero irreducible module and all other Hj(B,η)H^{j}(B,\eta) are zero. Let f⊂p⊂g{\mathfrak{f}}\subset{\mathfrak{p}}\subset{\mathfrak{g}} be a semi-simple Levi factor, so the weight lattice of f{\mathfrak{f}} is a sublattice of the weight lattice of g{\mathfrak{g}}, let tc{\mathfrak{t}}^{c} denote the complement of tf{\mathfrak{t}}_{{\mathfrak{f}}} (the torus of f{\mathfrak{f}}) in tg{\mathfrak{t}}_{{\mathfrak{g}}} and let g0=f+tc{\mathfrak{g}}_{0}={\mathfrak{f}}+{\mathfrak{t}}^{c} denote the Levi factor of p{\mathfrak{p}}. η\eta is induced from an irreducible g0{\mathfrak{g}}_{0}-module UU which is a weight space for tc{\mathfrak{t}}^{c} having non-negative weight, say (w1,...,wp)(w_{1},...,w_{p}). The bundle η ⊗ d\eta^{{\mathord{\,\otimes}\,}d}, corresponds to a module which is U ⊗ dU^{{\mathord{\,\otimes}\,}d} as an f{\mathfrak{f}}-module and is a weight space with weight (dw1,...,dwp)(dw_{1},...,dw_{p}) for the action of tc{\mathfrak{t}}^{c}. Thus SdηS^{d}\eta is completely reducible and each component of SdηS^{d}\eta is very ample and in particular acyclic.

To prove the second assertion, consider the maps V∗ ⊗ H0(B,Sr−1η)  →  H0(B,Srη)V^{*}{\mathord{\,\otimes}\,}H^{0}(B,S^{r-1}\eta){\mathord{\;\rightarrow\;}}H^{0}(B,S^{r}\eta). Note that H0(B,Sjη)⊂SjV∗H^{0}(B,S^{j}\eta)\subset S^{j}V^{*}. The proof of Proposition 2.2 will be completed by Lemma 2.3 below applied to UU and each irreducible component of H0(B,Srη)H^{0}(B,S^{r}\eta).∎

Let Mg0gM^{{\mathfrak{g}}}_{{\mathfrak{g}}_{0}} denote the sub-category of the category of g0{\mathfrak{g}}_{0}-modules generated under direct sum by the irreducible g0{\mathfrak{g}}_{0} modules with highest weight in Λg+⊂Λg0+\Lambda^{+}_{{\mathfrak{g}}}\subset\Lambda^{+}_{{\mathfrak{g}}_{0}} and note that it is closed under tensor product. Let MgM_{{\mathfrak{g}}} denote the category of g{\mathfrak{g}}-modules. Define an additive functor F:Mg0g  →  Mg\mathcal{F}:M^{{\mathfrak{g}}}_{{\mathfrak{g}}_{0}}{\mathord{\;\rightarrow\;}}M_{{\mathfrak{g}}} which takes an irreducible g0{\mathfrak{g}}_{0}-module with highest weight λ\lambda to the corresponding irreducible g{\mathfrak{g}}-module with highest weight λ\lambda.

Let l⊂g{\mathfrak{l}}\subset{\mathfrak{g}} and F{\mathcal{F}} be as above. Let U,WU,W be irreducible l{\mathfrak{l}}-modules Then

Let N⊂PN\subset P denote the unipotent radical of PP. Any LL-module WW may be considered as a PP-module where NN acts trivially. Saying V=F(W)V=\mathcal{F}(W) means that VV is the GG-module parabolically induced from WW and WW is the set of NN-invariants of VV. The NN-invariants of F(U) ⊗ F(W)\mathcal{F}(U){\mathord{\,\otimes}\,}\mathcal{F}(W) contain U ⊗ WU{\mathord{\,\otimes}\,}W. ∎

Proof of Proposition 1.6

Let G=SL(n,K)G=SL(n,K) and W=ΛkKm=VωkW=\Lambda^{k}K^{m}=V_{\omega_{k}}. It follows from the Pieri formulas that the modules V2ωk−2+ωk+4V_{2\omega_{k-2}+\omega_{k+4}} and Vωk−4+2ωk+2V_{\omega_{k-4}+2\omega_{k+2}} do not occur in V2ωk ⊗ VωkV_{2\omega_{k}}{\mathord{\,\otimes}\,}V_{\omega_{k}}. To see that they occur in S3WS^{3}W, identify VωkV_{\omega_{k}} with Λk(Kn)\Lambda^{k}(K^{n}) where KnK^{n} has a basis {e1,…,en}\{e_{1},\ldots,e_{n}\}. First observe that Λ6(K6)⊂S3(Λ2(K6))\Lambda^{6}(K^{6})\subset S^{3}(\Lambda^{2}(K^{6})), in fact if (f1,...,f6)(f_{1},...,f_{6}) is a basis of K6K^{6}, then the inclusion takes it to the Pfaffian

where we sum over all permutations σ∈S6\sigma\in{\mathfrak{S}}_{6} satisfying

Now considering K6⊂KnK^{6}\subset K^{n} as the span of {ek−1,…,ek+4}\{e_{k-1},\ldots,e_{k+4}\} we can produce a highest weight vector of V2ωk−2+ωk+4V_{2\omega_{k-2}+\omega_{k+4}} by wedging each term fi∧fj=ei+k−2∧ei+k−2f_{i}\wedge f_{j}=e_{i+k-2}\wedge e_{i+k-2} in the summation with e1∧…∧ek−2e_{1}\wedge\ldots\wedge e_{k-2}. We leave it to the reader to check the resulting vector has the desired properties. The module Vωk−4+2ωk+2V_{\omega_{k-4}+2\omega_{k+2}} occurs in S3WS^{3}W as well by symmetry (or one can define an analogous map).

Desingularizations for secant varieties of Rank 3 CHSS

In our situation the desingularizations are based on the observation that in each case XX is swept out by the union of Legendrian varieties XsmallX_{small} and σ(X)\sigma(X) is the union of the σ(Xsmall)\sigma(X_{small})’s which are linear spaces.

Here is a table of X,Xsmall,BX,X_{small},{\mathcal{B}} and the desingularizing bundle EE over BB:

Lemma 4.1 combined with Theorem 2.1 and Proposition 2.2 prove Theorem 1.1.

We now proceed with a case by case study.

Case of X=G​(3,W)𝑋𝐺3𝑊X=G(3,W)

σ^(G(3,W∗))=R6(Λ3W∗)\hat{\sigma}(G(3,W^{*}))=R_{6}(\Lambda^{3}W^{*}).

A general point of σ^(G(3,W∗))\hat{\sigma}(G(3,W^{*})) is of the form v1∧v2∧v3+v4∧v5∧v6v_{1}\wedge v_{2}\wedge v_{3}+v_{4}\wedge v_{5}\wedge v_{6}, so σ^(G(3,W∗))⊆R6(Λ3W∗)\hat{\sigma}(G(3,W^{*}))\subseteq R_{6}(\Lambda^{3}W^{*}) because the latter is compact and the former connected. But both varieties are of the same dimension 6(dim W)−176(\text{dim}\,W)-17 and are reduced and irreducible so they must be equal. ∎

The last module corresponds to a partition of length seven and thus by the remark above, it is among the generators of I(R6(Λ3W∗))I(R_{6}(\Lambda^{3}W^{*})) (because the ideal in degree two of any secant variety is empty), and the rest are not as their partitions have length at most six.

To show there are no generators in degree greater than three, we need to prove exactness in the middle step of (1) which in this case is:

The largest partition that can show up in the middle has length nine, so once we have solved the problem for G(3,K9)G(3,K^{9}) we are done.

Thus one could proceed calculate Hd(G(6,K9),Λd+1ξ)H^{d}(G(6,K^{9}),\Lambda^{d+1}\xi) with the aid of a computer to conclude (although the passage from the cohomology of Λd+1gr(ξ)\Lambda^{d+1}gr(\xi) to Λd+1ξ\Lambda^{d+1}\xi might require some effort). We will proceed differently, resolving the cases of dim W=7,8,9\text{dim}\,W=7,8,9 iteratively using rank varieties with p=dim W−1p=\text{dim}\,W-1.

For dim W=7\text{dim}\,W=7, the method in , §7.3 shows that the ideal of R6(Λ3W)R_{6}(\Lambda^{3}W) is generated by S316WS_{31^{6}}W and we are done. For the next two cases we proceed indirectly, calculating the ideal of R7(Λ3K8)R_{7}(\Lambda^{3}K^{8}) (resp. R8(Λ3K9)R_{8}(\Lambda^{3}K^{9})), and show these are in the ideal generated by S316WS_{31^{6}}W to complete the proof.

The ideal of the rank variety R6(Λ3K7∗)R_{6}(\Lambda^{3}K^{7*}) is generated in degree three by S3,16K7S_{3,1^{6}}K^{7} included in S3(Λ3K7)S^{3}(\Lambda^{3}K^{7}) as described in the recipe in the proof.

The ideal of the rank variety R7(Λ3K8∗)R_{7}(\Lambda^{3}K^{8*}) is generated in degree five by S3,22,15K8S_{3,2^{2},1^{5}}K^{8} included in S5(Λ3K8)S^{5}(\Lambda^{3}K^{8}) as described in the recipe in the proof.

The ideal of the rank variety R8(Λ3K9∗)R_{8}(\Lambda^{3}K^{9*}) is generated in degrees four and five by S4,18K9S_{4,1^{8}}K^{9} and S32,22,15K9S_{3^{2},2^{2},1^{5}}K^{9} respectively included in S4(Λ3K9)S^{4}(\Lambda^{3}K^{9}) and S5(Λ3K9)S^{5}(\Lambda^{3}K^{9}) as described in the recipe in the proof.

Thanks to the irreducibility of ξ\xi and its exterior powers, determination of modules generating the ideal is a straightforward application of the methods of and is left to the reader. It remains to show the above modules are all in the ideal generated by S316WS_{31^{6}}W. To do this we give explicit descriptions of the modules as spaces of polynomials.

We will encode the representations occurring in the dd-th symmetric powers of Λ3W\Lambda^{3}W by Young tableaux of shape π=λ(D)\pi=\lambda(D) with 3d3d boxes, filled with the numbers 1,…,d1,\ldots,d with each number occurring three times. These tableaux are also assumed to be weakly increasing in rows and strictly increasing in columns. We associate to such tableau DD the map ρ(D)\rho(D)

where π′=(d1′,...,dr′)\pi^{\prime}=(d_{1}^{\prime},...,d_{r}^{\prime}) is the conjugate partition to π\pi.

The map ρ(D)\rho(D) is defined as the composition of the following maps:

a) assuming there are ei,se_{i,s} boxes filled with ss in the ii-th row, apply the embedding

b) Noting that for each ss, e1,s+⋯+er,s=3e_{1,s}+\cdots+e_{r,s}=3, wedge the factors coming from different rows corresponding to the same number ss in DD, i.e., after rearranging the factors define the projection to (Λ3W) ⊗ d(\Lambda^{3}W)^{{\mathord{\,\otimes}\,}d} by sending, for each ss,

c) Project (Λ3W) ⊗ d  →  Sd(Λ3W)(\Lambda^{3}W)^{{\mathord{\,\otimes}\,}d}{\mathord{\;\rightarrow\;}}S^{d}(\Lambda^{3}W) by symmetrizing.

We call the Young diagram DD the numbering scheme associated to the map ρ(D)\rho(D). Write λ(D)\lambda(D) for the weight of the numbering scheme whose ii-th entry is the length of the ii-th column of the Young diagram of DD - this will be the highest weight of the associated module.

The four Schur functors mentioned in the statement of the lemma correspond to four numbering schemes.

It is clear that the images of the corresponding maps are in the ideals of corresponding rank varieties because of the length of the first row of each numbering scheme.

Decomposing the domain and range of ρ(Di)\rho(D_{i}) into irreducible representations, in all four cases Sλ(Di)WS_{\lambda(D_{i})}W is the only Schur functor occurring in both the domain and range of ρ(Di)\rho(D_{i}), and it occurs there with multiplicity one. Thus it only remains to see the maps ρ(Dj)\rho(D_{j}) are nonzero, which is the purpose of the following lemma.

The numbering schemes D1,D2,D3,D4D_{1},D_{2},D_{3},D_{4} all yield nonzero modules.

is nonzero in S4(Λ3W)S_{4}(\Lambda^{3}W). The other cases are similar.

Consider the contribution to the monomial (e1∧e2∧e3)(e1∧e2∧e3)(e1∧e4∧e5)(e6∧e7∧e8)(e_{1}\wedge e_{2}\wedge e_{3})(e_{1}\wedge e_{2}\wedge e_{3})(e_{1}\wedge e_{4}\wedge e_{5})(e_{6}\wedge e_{7}\wedge e_{8}) in the image of highest weight vector ρ(D2)(e1∧e2∧e3∧e4∧e5∧e6∧e7∧e8) ⊗ (e1∧e2∧e3) ⊗ (e1)\rho(D_{2})(e_{1}\wedge e_{2}\wedge e_{3}\wedge e_{4}\wedge e_{5}\wedge e_{6}\wedge e_{7}\wedge e_{8}){\mathord{\,\otimes}\,}(e_{1}\wedge e_{2}\wedge e_{3}){\mathord{\,\otimes}\,}(e_{1}). All occurrences of this monomial can be divided to 24 classes (corresponding to permutations of {1,2,3,4}\{1,2,3,4\}) according to the order in which the factors appear in (Λ3W) ⊗ d(\Lambda^{3}W)^{{\mathord{\,\otimes}\,}d} after applying parts a) and b) of the definition of ρ(D2)\rho(D_{2}). In fact only two classes out of 24 are non-empty. The factor e6∧e7∧e8e_{6}\wedge e_{7}\wedge e_{8} has to come from the first factor, and one of the factors e1∧e2∧e3e_{1}\wedge e_{2}\wedge e_{3} has to come from the fourth factor. The factor e1∧e4∧e5e_{1}\wedge e_{4}\wedge e_{5} can come from the third factor (and this gives contribution 33 to the coefficient) or from the second factor (and this gives contribution 11 to the coefficient). Thus the coefficient is nonzero and and therefore ρ(D2)≠0\rho(D_{2})\neq 0.

To finish the proof of Theorem 1.2 we need to show that the ideal generated by the first module contains the other modules. But this is clear by the definition of maps ρ(D)\rho(D) and by the last part of the proof of Proposition 5.2 as the other numbering schemes all contain the first.

Note that Vω7D7V_{\omega_{7}}^{D_{7}} decomposes to Vω6D6 ⊕ Vω5D6V_{\omega_{6}}^{D_{6}}{\mathord{\,\oplus}\,}V_{\omega_{5}}^{D_{6}} as a D6D_{6} module, and this splitting gives rise to the the bundles ξ\xi and η\eta over Q12Q^{12}. Thus they are both irreducible and dual to one another. In this case it is straightforward to calculate Hj(Λj+1ξ)H^{j}(\Lambda^{j+1}\xi) if one knows the decomposition of Λj+1Vω6D6\Lambda^{j+1}V_{\omega_{6}}^{D_{6}}. In fact we calculated the entire minimal free resolution which is available at http://www.math.neu.edu/∼\simweyman/mathindex.html for the interested reader. In particular the only generator of the ideal is the module Vω4V_{\omega_{4}} as stated in the theorem.

All spaces discussed in this section are to be considered as linear subspaces of (A ⊗ B) ⊗ 3=A ⊗ 3 ⊗ B ⊗ 3(A{\mathord{\,\otimes}\,}B)^{{\mathord{\,\otimes}\,}3}=A^{{\mathord{\,\otimes}\,}3}{\mathord{\,\otimes}\,}B^{{\mathord{\,\otimes}\,}3} and all evaluations are as multi-linear forms. In particular, the symmetrization map

realizes S3(A ⊗ B)⊂(A ⊗ B) ⊗ 3S^{3}(A{\mathord{\,\otimes}\,}B)\subset(A{\mathord{\,\otimes}\,}B)^{{\mathord{\,\otimes}\,}3} as πS((A ⊗ B) ⊗ 3)\pi_{S}((A{\mathord{\,\otimes}\,}B)^{{\mathord{\,\otimes}\,}3}). Similarly we regard S2A ⊗ A⊂A ⊗ 3S^{2}A{\mathord{\,\otimes}\,}A\subset A^{{\mathord{\,\otimes}\,}3} as the image of the symmetrization map x ⊗ y ⊗ z↦12(x ⊗ y ⊗ z+y ⊗ z ⊗ z)x{\mathord{\,\otimes}\,}y{\mathord{\,\otimes}\,}z\mapsto\frac{1}{2}(x{\mathord{\,\otimes}\,}y{\mathord{\,\otimes}\,}z+y{\mathord{\,\otimes}\,}z{\mathord{\,\otimes}\,}z) and likewise for S2B ⊗ B⊂B ⊗ 3S^{2}B{\mathord{\,\otimes}\,}B\subset B^{{\mathord{\,\otimes}\,}3}.

where KS(A)K_{S}(A) is the kernel of the map S2A ⊗ A  →  S3AS^{2}A{\mathord{\,\otimes}\,}A{\mathord{\;\rightarrow\;}}S^{3}A, which is a GL(A)GL(A)-module isomorphic to S21AS_{21}A. In particular, if R∈KS(A)R\in K_{S}(A), we have R(u,v,w)=R(v,u,w)R(u,v,w)=R(v,u,w) for all u,v,w∈A∗u,v,w\in A^{*} and

which holds because R(u,v,w)+R(u,w,v)+R(v,w,u)+R(v,w,u)+R(w,u,v)+R(w,v,u)=0R(u,v,w)+R(u,w,v)+R(v,w,u)+R(v,w,u)+R(w,u,v)+R(w,v,u)=0, and setting w=uw=u gives 2R(u,v,u)+2R(u,u,v)+2R(v,u,u)=4R(u,v,u)+2R(u,u,v)=02R(u,v,u)+2R(u,u,v)+2R(v,u,u)=4R(u,v,u)+2R(u,u,v)=0.

By definition S1(Y)={T∈I2(Y) ⊗ A∣πS,A(T)=0}S_{1}(Y)=\{T\in I_{2}(Y){\mathord{\,\otimes}\,}A\mid\pi_{S,A}(T)=0\}, where

Elements of S1(Y)⊂KS(A)S_{1}(Y)\subset K_{S}(A) have the property that as tri-linear forms they vanish on any triple of the form (v,v,w)(v,v,w) with [v]∈Y[v]\in Y and ww arbitrary.

Any element of KS(A) ⊗ KS(B)⊂(A ⊗ B) ⊗ 3K_{S}(A){\mathord{\,\otimes}\,}K_{S}(B)\subset(A{\mathord{\,\otimes}\,}B)^{{\mathord{\,\otimes}\,}3} may be written as a sum ∑Ri ⊗ Ti\sum R_{i}{\mathord{\,\otimes}\,}T_{i} with Ri∈KS(A)R_{i}\in K_{S}(A) and Ti∈KS(B)T_{i}\in K_{S}(B), thus any element of πS(KS(A) ⊗ KS(B))\pi_{S}(K_{S}(A){\mathord{\,\otimes}\,}K_{S}(B)) is of the form P=πS(∑Ri ⊗ Ti)P=\pi_{S}(\sum R_{i}{\mathord{\,\otimes}\,}T_{i}) with Ri∈KS(A)R_{i}\in K_{S}(A) and Ti∈KS(B)T_{i}\in K_{S}(B). We compute

The first equality holds because of the six permutations in S3{\mathfrak{S}}_{3}, only three yield different elements, the second because Ri∈S2A ⊗ AR_{i}\in S^{2}A{\mathord{\,\otimes}\,}A and Ti∈S2B ⊗ BT_{i}\in S^{2}B{\mathord{\,\otimes}\,}B, and the third by (2).

which is zero because Ri,α∈I2(Y)R_{i,\alpha}\in I_{2}(Y) for all i,αi,\alpha. Similarly πS(KS(A) ⊗ S1(Z))⊂I3(σ(Seg(Y×Z))\pi_{S}(K_{S}(A){\mathord{\,\otimes}\,}S_{1}(Z))\subset I_{3}(\sigma(Seg(Y\times Z)).

Now say P=πS(∑Ri ⊗ Ti)∈(KS(A) ⊗ KS(B))∩I3(σ(Seg(Y×Z))P=\pi_{S}(\sum R_{i}{\mathord{\,\otimes}\,}T_{i})\in(K_{S}(A){\mathord{\,\otimes}\,}K_{S}(B))\cap I_{3}(\sigma(Seg(Y\times Z)). Without loss of generality we assume the RiR_{i} are linearly independent modulo S1(Y)S_{1}(Y) and the TiT_{i} are linearly independent modulo S1(Z)S_{1}(Z). Fix (y,z)∈U(y,z)\in U, we obtain a linear equation

where ci,y,z=Ti(y,y,z)c_{i,y,z}=T_{i}(y,y,z) and if y,zy,z are chosen generically all the coefficients are nonzero because we are working mod S1(Z)S_{1}(Z). Note that the index range for ii is at most from 11 to  min {dim KS(A),dim KS(B)}\text{ min }\{\text{dim}\,K_{S}(A),\text{dim}\,K_{S}(B)\}. We will show each Ri(v,v,w)R_{i}(v,v,w) must be zero for all v,w∈Y^v,w\in\hat{Y}. Since Y^\hat{Y} spans AA and the expression is linear in ww, we can have this hold for all v∈Y^v\in\hat{Y} and w∈Aw\in A, but this in turn implies that each Ri∈S1(Y)R_{i}\in S_{1}(Y).

To obtain the desired vanishing, fix v,wv,w and consider the Ri(v,v,w)=riR_{i}(v,v,w)=r_{i} as constants. We have an equation

As remarked above, since ZZ is linearly non-degenerate, we may choose dim B\text{dim}\,B elements zs∈Z^z_{s}\in\hat{Z} that give a basis of B∗B^{*}. Similarly, we may choose (dim B+12)−dim I2(Z)\binom{\text{dim}\,B+1}{2}-\text{dim}\,I_{2}(Z) elements yt∈Z^y_{t}\in\hat{Z} such that the vectors yt2y_{t}^{2} span I2(Z)⊥⊂S2B∗I_{2}(Z){}^{\perp}\subset S^{2}B^{*}. Thus the vectors yt2 ⊗ zsy_{t}^{2}{\mathord{\,\otimes}\,}z_{s} give a basis of I2(Z)⊥ ⊗ B∗I_{2}(Z){}^{\perp}{\mathord{\,\otimes}\,}B^{*}. Thus the pairing with elements of KS(B)/S1(Z)K_{S}(B)/S_{1}(Z) is perfect, which implies that the matrix given by pairing the yt2 ⊗ zsy_{t}^{2}{\mathord{\,\otimes}\,}z_{s} with the TiT_{i} has a one-sided inverse, so we have enough independent equations to force all the rir_{i} to vanish.

The argument for the S3A ⊗ S3BS^{3}A{\mathord{\,\otimes}\,}S^{3}B factor is similar, but easier, as there is no need to symmetrize. Write P=∑Ri ⊗ TiP=\sum R_{i}{\mathord{\,\otimes}\,}T_{i} with Ri∈S3AR_{i}\in S^{3}A and Ti∈S3BT_{i}\in S^{3}B.

Now Ri∈I3(σ(Y))R_{i}\in I_{3}(\sigma(Y)) iff Ri(v,v,w)=0R_{i}(v,v,w)=0 for all v,w∈Y^v,w\in\hat{Y} and one concludes as above. ∎

We now show there are no new generators in degrees greater than three.

1. Case Y=G​(2,B)𝑌𝐺2𝐵Y=G(2,B)

We need to study the exactness of the middle step of

Here by ∣∣π∣≤4\mid_{|\pi|\leq 4}, we mean the components of Sa,b(Λ2B)S_{a,b}(\Lambda^{2}B) that occur in the decomposition of Sp(A ⊗ Λ2B)=⊕a+b=pSa,bA ⊗ Sa,b(S1,1B)S^{p}(A{\mathord{\,\otimes}\,}\Lambda^{2}B)=\oplus_{a+b=p}S_{a,b}A{\mathord{\,\otimes}\,}S_{a,b}(S_{1,1}B) that as partitions SπBS_{\pi}B have length at most four.

Let BB have dimension nn and consider the rank variety

Over B:=A∗ ⊗ G(n−1,B∗){\mathcal{B}}:=A^{*}{\mathord{\,\otimes}\,}G(n-1,B^{*}) we have the bundle with fiber A∗ ⊗ Λ2SA^{*}{\mathord{\,\otimes}\,}\Lambda^{2}{\mathcal{S}} which provides a desingularization of Rn−1(A∗ ⊗ Λ2B∗)R_{n-1}(A^{*}{\mathord{\,\otimes}\,}\Lambda^{2}B^{*}). Our corresponding bundles are η=A ⊗ Λ2S∗\eta=A{\mathord{\,\otimes}\,}\Lambda^{2}{\mathcal{S}}^{*} and ξ=A ⊗ (Λ2B/Λ2S)=A ⊗ S∗ ⊗ Q∗\xi=A{\mathord{\,\otimes}\,}(\Lambda^{2}B/\Lambda^{2}{\mathcal{S}})=A{\mathord{\,\otimes}\,}{\mathcal{S}}^{*}{\mathord{\,\otimes}\,}{\mathcal{Q}}^{*}. Note that rank ξ=2(n−1)\text{rank}\,\xi=2(n-1).

where π′\pi^{\prime} denotes the conjugate partition to π\pi, so if π=(a,b)\pi=(a,b), then π′=(2a,1b)\pi^{\prime}=(2^{a},1^{b}).

We apply the Bott algorithm (see e.g. , §4.1.5) to the weight μ=ωa+ωa+b−(2a+b)ωn\mu=\omega_{a}+\omega_{a+b}-(2a+b)\omega_{n} The only potential way to have non-zero cohomology is at step (n−1)−(a+b)(n-1)-(a+b), or at step (n−1)−a(n-1)-a or step n−1n-1.

To obtain nonzero H(n−1)−(a+b)(B,Λn−(a+b)ξ)H^{(n-1)-(a+b)}({\mathcal{B}},\Lambda^{n-(a+b)}\xi), −(2a+b)+(n−1−(a+b))-(2a+b)+(n-1-(a+b)) must be negative and −(2a+b)+(n−1−(a+b))+2-(2a+b)+(n-1-(a+b))+2 must be non-negative, so we must have 3a+2b=n−13a+2b=n-1. Write i=2a+bi=2a+b, so Hi(B,Λi+1ξ)=Sn−i,2i−nA ⊗ S22i−n,12n−2iBH^{i}({\mathcal{B}},\Lambda^{i+1}\xi)=S_{n-i,2i-n}A{\mathord{\,\otimes}\,}S_{2^{2i-n},1^{2n-2i}}B.

To obtain nonzero H(n−1)−a(B,Λn−aξ)H^{(n-1)-a}({\mathcal{B}},\Lambda^{n-a}\xi), −(2a+b)+(n−1−a)-(2a+b)+(n-1-a) must be negative and −(2a+b)+(n−1−a)+2-(2a+b)+(n-1-a)+2 must be non-negative, implying 3a+b=n+13a+b=n+1, contradicting a+b≤n−1a+b\leq n-1.

To obtain nonzero Hn−1(B,Λnξ)H^{n-1}({\mathcal{B}},\Lambda^{n}\xi), we would have to have −(2a+b)+(n−1)<−1-(2a+b)+(n-1)<-1 and −(2a+b)+(n−1)+2-(2a+b)+(n-1)+2 non-negative, implying 2a+b=n+22a+b=n+2 contradicting a+b≤n−1a+b\leq n-1.

Let B,AB,A be vector spaces respectively of dimensions n,2n,2 and consider the rank variety

Then the ideal of Rn−1R_{n-1} is generated in degrees ⌈n2⌉≤d≤⌊2n3⌋\lceil\frac{n}{2}\rceil\leq d\leq\lfloor\frac{2n}{3}\rfloor by the modules

Write B=G/Pi0{\mathcal{B}}=G/P_{i_{0}}. Following the conventions of , i0=4,6i_{0}=4,6 respectively. We write the Levi factor of p{\mathfrak{p}} as g0=f+⟨Zi0⟩{\mathfrak{g}}_{0}={\mathfrak{f}}+\langle Z_{i_{0}}\rangle, where f{\mathfrak{f}} is semi-simple (respectively a3+a1\mathfrak{a}_{3}+\mathfrak{a}_{1} and d5\mathfrak{d}_{5}) and ⟨Zi0⟩\langle Z_{i_{0}}\rangle is the center of g0{\mathfrak{g}}_{0}.

We will obtain the result by computing Hi(B,Λi+1ξ)H^{i}({\mathcal{B}},\Lambda^{i+1}\xi) via Hi(B,Λi+1gr(ξ))H^{i}({\mathcal{B}},\Lambda^{i+1}gr(\xi)) and applying a result of Ottaviani and Rubei.

where EλE_{\lambda} denotes the irreducible bundle corresponding to the g0{\mathfrak{g}}_{0}-module of highest weight λ\lambda.

We first compute the decomposition of the exterior powers of the g0{\mathfrak{g}}_{0}-module giving rise to gr(ξ)gr(\xi) as an f{\mathfrak{f}} module and then compute the action of Zi0Z_{i_{0}} to determine the coefficient on ωi0\omega_{i_{0}} for each irreducible f{\mathfrak{f}}-module appearing.

The f{\mathfrak{f}}-module decomposition is straightforward with the aid of LiE , keeping in mind that dim A=2\text{dim}\,A=2:

One then uses LiE to decompose these GL(U)-modules as f{\mathfrak{f}}-modules. Next to determine the weight on the marked node (i.e., the coefficient of ωi0\omega_{i_{0}}), one uses the grading element Zi0∈tZ_{i_{0}}\in{\mathfrak{t}} which has the property that Zi0(αj)=δi0,jZ_{i_{0}}(\alpha_{j})=\delta_{i_{0},j}. Thus if λ=∑i≠i0λiωi\lambda=\sum_{i\neq i_{0}}\lambda^{i}\omega_{i} is an irreducible f{\mathfrak{f}}-module appearing in Wμ ⊗ kW_{\mu}^{{\mathord{\,\otimes}\,}k}, where the ωi\omega_{i} are fundamental weights of g{\mathfrak{g}}, to find the coefficient of ωi0\omega_{i_{0}} of the g0{\mathfrak{g}}_{0}-module, one calculates

where (c−1)(c{}^{-1}) denotes the inverse of the Cartan matrix. In both our cases Zi0(μ)=−13Z_{i_{0}}(\mu)=-\frac{1}{3}.

Now one calculates Hj(B,Λpgr(ξ))H^{j}({\mathcal{B}},\Lambda^{p}gr(\xi)). In practice we first calculated Hp−1(B,Λpgr(ξ))H^{p-1}({\mathcal{B}},\Lambda^{p}gr(\xi)), and only if this was nonzero did we calculate the other Hj(B,Λpgr(ξ))H^{j}({\mathcal{B}},\Lambda^{p}gr(\xi)).

The coordinate ring of σ​(X)𝜎𝑋\sigma(X)

The following proposition is due to F. Zak (, p. 51):

We work with the affine variety σ^(X)⊂V\hat{\sigma}(X)\subset V.

Notations as above. Let H=Stab(vλ+vμ)H=Stab(v_{\lambda}+v_{\mu}). Then

In particular, the irreducible GG-module VλV_{\lambda} occurs in K[G]HK[G]^{H} with multiplicity equal to the number of HH-fixed points in Vλ∗V_{\lambda}^{*}.

Since G/H⊆σ^(X)G/H\subseteq\hat{\sigma}(X) we obtain an inclusion K[σ^(X)]⊆K[G/H]K[\hat{\sigma}(X)]\subseteq K[G/H] by restricting functions on σ^(X)\hat{\sigma}(X). By , Theorem 3, Chapter II, section 3, the coordinate ring of GG has a left-right decomposition (as a (G−G)(G-G)-bimodule)

X=G(k,W)X=G(k,W), with k>2k>2. Here without loss of generality we may take dim W≥2k\text{dim}\,W\geq 2k. Indeed, if dimW<2kdimW<2k, we may pass to the dual Grassmannian G(dim W−k,W∗)G(\text{dim}\,W-k,W^{*}). If dim(W)>2kdim(W)>2k, σ^(X)\hat{\sigma}(X) is contained in the subspace variety R2k(ΛkW)R_{2k}(\Lambda^{k}W) of tensors that can be written using ≤2k\leq 2k basis vectors. Let W′⊂WW^{\prime}\subset W be a 2k2k dimensional subspace. Consider the subgroup H′⊂HH^{\prime}\subset H,

The quotient SLK(W)/H′SL_{K}(W)/H^{\prime} can be identified with the variety HomKinj(W′,W)Hom_{K}^{inj}(W^{\prime},W) of injective linear maps from W′W^{\prime} to WW. Since the complement of HomKinj(W′,W)Hom_{K}^{inj}(W^{\prime},W) in HomK(W′,W)Hom_{K}(W^{\prime},W) has codimension ≥2\geq 2 every regular function on HomKinj(W′,W)Hom_{K}^{inj}(W^{\prime},W) extends to HomK(W′,W)Hom_{K}(W^{\prime},W). This means that we have the equalities

Here in the last equality we may view λ\lambda as a partition. Note that the last equality states that the module (SλW)∗(S_{\lambda}W)^{*} appears with multiplicity dim SλW′\text{dim}\,S_{\lambda}W^{\prime}.

This reduces the calculation of (SλW)H(S_{\lambda}W)^{H} to the case W=W′W=W^{\prime}. Assuming now that dim(W)=2kdim(W)=2k, with basis e1,...,e2ke_{1},...,e_{2k}, we may take vλ+vμ=e1∧⋯∧ek+ek+1∧⋯∧e2kv_{\lambda}+v_{\mu}=e_{1}\wedge\cdots\wedge e_{k}+e_{k+1}\wedge\cdots\wedge e_{2k}. Then

Considering G(k,W)=SL(W)/PkG(k,W)=SL(W)/P_{k}, it is clear that no fundamental representation other than Wωk=ΛkWW_{\omega_{k}}=\Lambda^{k}W has an HH-fixed vector and in WωkW_{\omega_{k}} there is a 22-dimensional subspace of such spanned by e1∧⋯∧eke_{1}\wedge\cdots\wedge e_{k} and ek+1∧⋯∧e2ke_{k+1}\wedge\cdots\wedge e_{2k}. The corresponding two copies of ΛkW\Lambda^{k}W generate the ring of invariants in the following sense. We claim:

Two generating fundamental representations are in bidegrees (1,0)(1,0) and (0,1)(0,1). If we work instead with GL(W)GL(W), since HH acts trivially on the determinant, we get

To see this, write E=⟨e1,...,ek⟩,F=⟨ek+1,...,e2k⟩E=\langle e_{1},...,e_{k}\rangle,F=\langle e_{k+1},...,e_{2k}\rangle, we want to see how many instances of the trivial representation of SL(E)×SL(F)SL(E)\times SL(F) occurs in the irreducible SL(W)SL(W) module SλWS_{\lambda}W. Now, since W=E ⊕ FW=E{\mathord{\,\oplus}\,}F

This means this ring is the homomorphic image of the symmetric algebra on two copies of ΛkW\Lambda^{k}W corresponding to components in bidegrees (1,0)(1,0) and (0,1)(0,1) which is our claim.

so we need i1+b1=i2+b2=⋯=ik+bki_{1}+b_{1}=i_{2}+b_{2}=\cdots=i_{k}+b_{k} and a1−b1−i1=a2−b2−i2=⋯=ak−bk−ika_{1}-b_{1}-i_{1}=a_{2}-b_{2}-i_{2}=\cdots=a_{k}-b_{k}-i_{k}. This means the vectors ejij+bjfjaj−ije_{j}^{i_{j}+b_{j}}f_{j}^{a_{j}-i_{j}} have to be all of the same weight, for j=1,…,kj=1,\ldots,k.

the dimension of the subspace of HH-invariant vectors is min aj−max bj+1{\rm min}\ a_{j}-{\rm max}\ b_{j}+1.

References