2.1 Superspace

As in the introduction, the superspace ring $\Omega _n = {\mathbb {C}}[{\mathbf {x}}_n] \otimes \wedge \{ \mathbf {\theta }_n \}$ is the tensor product of a symmetric algebra of rank n and an exterior algebra of rank n, both over ${\mathbb {C}}$ . A monomial in $\Omega _n$ is a nonzero product of the generators ${\mathbf {x}}_n = (x_1, \dots , x_n)$ and $\mathbf {\theta }_n = (\theta _1, \dots , \theta _n)$ . A bosonic monomial is a monomial that only involves the generators ${\mathbf {x}}_n$ , whereas a fermionic monomial is a monomial that only involves the generators $\mathbf {\theta }_n$ . For any subset $J \subseteq [n]$ , we let $\theta _J$ be the product of the fermionic generators $\theta _j$ indexed by $j \in J$ in increasing order; we have a direct sum decomposition

(2.1) $$ \begin{align} \Omega_n = \bigoplus_{J \subseteq [n]} {\mathbb {C}}[{\mathbf {x}}_n] \cdot \theta_J. \end{align} $$

The Gale order $\leq _{\mathrm {Gale}}$ on subsets $J \subseteq [n]$ of the same cardinality will be used heavily. This partial order is defined by

(2.2) $$ \begin{align} \{ a_1 < \cdots < a_r \} \leq_{\mathrm {Gale}} \{ b_1 < \cdots < b_r \}\ \text{if}\ a_i \leq b_i\ \text{for all}\ i. \end{align} $$

This order will be used to compare fermionic monomials $\theta _J$ in the superspace ring $\Omega _n$ .

The ring $\Omega _n$ may be identified with polynomial valued differential forms on ${\mathbb {C}}^n$ ; as such, it carries a plethora of derivative operators. For $1 \leq i \leq n$ , let $\partial _i: {\mathbb {C}}[{\mathbf {x}}_n] \rightarrow {\mathbb {C}}[{\mathbf {x}}_n]$ be the usual partial differentiation with respect to $x_i$ . By acting on the first tensor factor of $\Omega _n = {\mathbb {C}}[{\mathbf {x}}_n] \otimes \wedge \{ \mathbf {\theta }_n \}$ , this extends to an action $\partial _i: \Omega _n \rightarrow \Omega _n$ . For $1 \leq i \leq n$ , let $\partial ^{\theta }_i: \wedge \{ \mathbf {\theta }_n \} \rightarrow \wedge \{ \mathbf {\theta }_n \}$ be the contraction operator defined on fermionic monomials by

(2.3) $$ \begin{align} \partial^\theta_i: \theta_{j_1} \cdots \theta_{j_r} = \begin{cases} (-1)^{s-1} \theta_{j_1} \cdots \widehat{\theta_{j_s}} \cdots \theta_{j_r} & \text{if}\ j_s = i\ \text{for some}\ s, \\ 0 & \text{otherwise} \end{cases} \end{align} $$

for any distinct indices $1 \leq j_1, \dots , j_r \leq n$ where $\widehat {\cdot }$ denotes omission. By acting on the second tensor factor of $\Omega _n = {\mathbb {C}}[{\mathbf {x}}_n] \otimes \wedge \{ \mathbf {\theta }_n \}$ , we have a fermionic derivative operator $\partial ^{\theta }_i: \Omega _n \rightarrow \Omega _n$ .

We let $d: \Omega _n \rightarrow \Omega _n$ be the Euler operator of differential geometry defined by

(2.4) $$ \begin{align} d: f \mapsto \sum_{i = 1}^n \partial_i f \cdot \theta_i \end{align} $$

for all $f \in \Omega _n$ . This operator lowers bosonic degree by 1 while raising fermionic degree by 1. We will need ‘higher’ versions $d_j: \Omega _n \rightarrow \Omega _n$ $(j \geq 1)$ of these operators given by

(2.5) $$ \begin{align} d_j: f \mapsto \sum_{i = 1}^n \partial_i^j f \cdot \theta_i. \end{align} $$

The operator $d_j$ decreases bosonic degree by j while raising fermionic degree by 1. We have $d_1 = d$ . If $J = \{ j_1 < j_2 < \cdots \}$ is a set of positive integers, we write

(2.6) $$ \begin{align} d_J := d_{j_1} d_{j_2} \cdots \end{align} $$

for the corresponding product of higher Euler operators.

Considering bosonic and fermionic degree separately, superspace $\Omega _n$ admits a bigrading

(2.7) $$ \begin{align} \Omega_n = \bigoplus_{i \geq 0} \bigoplus_{j = 0}^n (\Omega_n)_{i,j} \quad \text{ where } \quad (\Omega_n)_{i,j} = {\mathbb {C}}[{\mathbf {x}}_n]_i \otimes \wedge^j \{ \mathbf{\theta}_n \}. \end{align} $$

The diagonal action of the symmetric group ${\mathfrak {S}}_n$ on $\Omega _n$ preserves this bigrading. As in the introduction, we let $(\Omega _n)^{{\mathfrak {S}}_n}$ be the fixed subalgebra for this action.

Let $I \subseteq \Omega _n$ be a bihomogeneous ideal in superspace (such as $SI_n$ ). Analysis of the quotient ring $\Omega _n/I$ is often complicated by the fact that its elements $f + I$ are cosets rather than superspace elements $f \in \Omega _n$ . The theory of (superspace) harmonics is a powerful technique for replacing cosets with honest elements of superspace. We turn to a description of this method.

The partial derivative operators $\partial _i, \partial ^\theta _i: \Omega _n \rightarrow \Omega _n$ satisfy the relations

(2.8) $$ \begin{align} \partial_i \partial_j = \partial_j \partial_i \quad \quad \partial_i \partial^{\theta}_j = \partial^{\theta}_j \partial_i \quad \quad \partial^{\theta}_i \partial^{\theta}_j = - \partial^{\theta}_j \partial^{\theta}_i \end{align} $$

for all $1 \leq i, j \leq n$ . Since these are the defining relations of $\Omega _n$ , for any superspace element $f = f(x_1, \dots , x_n, \theta _1, \dots , \theta _n) \in \Omega _n$ , we get an operator

(2.9) $$ \begin{align} \partial f = f(\partial_1, \dots, \partial_n, \partial^{\theta}_1, \dots, \partial^{\theta}_n): \Omega_n \rightarrow \Omega_n \end{align} $$

by replacing each $x_i$ in f with the bosonic derivative $\partial _i$ and each $\theta _i$ in f with the fermionic derivative $\partial ^{\theta }_i$ . This leads to an action of superspace on itself given by

(2.10) $$ \begin{align} \odot: \Omega_n \times \Omega_n \rightarrow \Omega_n \quad \quad f \odot g := (\partial f)(g). \end{align} $$

The $\odot $ -action gives $\Omega _n$ -module structure on $\Omega _n$ .

We use the $\odot $ -action to construct an inner product on $\Omega _n$ as follows. Let $\overline {\cdot }: \Omega _n \rightarrow \Omega _n$ be the conjugate-linear involution that fixes all bosonic monomials, satisfies $\overline { \theta _{i_1} \cdots \theta _{i_r} } = \theta _{i_r} \cdots \theta _{i_1}$ for all fermionic monomials $\theta _{i_1} \cdots \theta _{i_r}$ , and sends any scalar $c \in {\mathbb {C}}$ to its complex conjugate $\overline {c}$ . The pairing

(2.11) $$ \begin{align} \langle -, - \rangle: \Omega_n \times \Omega_n \rightarrow \Omega_n \quad \quad \langle f, g \rangle := \text{constant term of}\ f \odot \overline{g} \end{align} $$

is easily seen to be an inner product, with the monomials $\{ x_1^{a_1} \cdots x_n^{a_n} \cdot \theta _I \}$ forming an orthogonal (but not orthonormal) basis.

Now suppose $I \subseteq \Omega _n$ is a bihomogeneous ideal defined over ${\mathbb {R}}$ (such as $SI_n$ ). We have the equality

(2.12) $$ \begin{align} I^{\perp} = \{ g \in \Omega_n \,:\, f \odot g = 0 \text{ for all}\ f \in I \} \end{align} $$

of subspaces of $\Omega _n$ , where $I^{\perp }$ is calculated with respect to the above inner product. The subspace $I^{\perp } \subseteq \Omega _n$ is the harmonic space attached to I. We have a direct sum decomposition $\Omega _n = I \oplus I^{\perp }$ and an isomorphism of bigraded vector spaces $\Omega _n/I \cong I^{\perp }$ . If I is ${\mathfrak {S}}_n$ -stable, the isomorphism $\Omega _n/I \cong I^{\perp }$ is also an isomorphism of bigraded ${\mathfrak {S}}_n$ -modules. The harmonic model $I^{\perp }$ of $\Omega _n/I$ is useful because its members are honest superspace elements rather than cosets.

We close this subsection with a combinatorial identity due to Sagan and Swanson that will be useful in our analysis of $SR_n$ . For a subset $J \subseteq [n]$ , we define the J-staircase to be the sequence ${\mathrm {st}}(J) = ({\mathrm {st}}(J)_1, \dots , {\mathrm {st}}(J)_n)$ , where

(2.13) $$ \begin{align} {\mathrm{st}}(J)_1 := \begin{cases} 0 & 1 \in J \\ 1 & 1 \notin J \end{cases} \end{align} $$

and

(2.14) $$ \begin{align} {\mathrm{st}}(J)_{i+1} := \begin{cases} {\mathrm{st}}(J)_i & i+1 \in J \\ {\mathrm{st}}(J)_i + 1 & i+1 \notin J. \end{cases} \end{align} $$

For example, if $n = 7$ and $J = \{ 3,5,6\}$ , we have ${\mathrm {st}}(J) = ({\mathrm {st}}(J)_1, \dots , {\mathrm {st}}(J)_7) = (1,2,2,3,3,3,4)$ . Observe that ${\mathrm {st}}(\varnothing ) = (1, 2, \dots , n)$ is the usual staircase.

Lemma 2.1. (Sagan-Swanson [Reference Sagan and Swanson33])

We have the polynomial identity

(2.15) $$ \begin{align} \sum_{J \subseteq [n]} \left( \prod_{i = 1}^n [{\mathrm{st}}(J)_i]_q \right) \cdot z^{|J|} = \sum_{k = 1}^n z^{n-k} \cdot [k]!_q \cdot {\mathrm {Stir}}_q(n,k). \end{align} $$

2.2 Commutative algebra

Our overarching strategy for analyzing $SR_n$ is to transfer problems involving the superspace ring $\Omega _n$ to problems involving the better-understood polynomial ring ${\mathbb {C}}[{\mathbf {x}}_n]$ . We review the relevant notions from commutative algebra.

A commutative graded ${\mathbb {C}}$ -algebra $A = \bigoplus _{i \geq 0} A_i$ is Artinian if A is a finite-dimensional ${\mathbb {C}}$ -vector space. The Hilbert series of A is

(2.16) $$ \begin{align} {\mathrm {Hilb}}(A;q) := \sum_{i \geq 0} \dim_{\mathbb {C}}(A_i) \cdot q^i, \end{align} $$

assuming each graded piece $A_i$ is finite-dimensional.

A sequence $f_1, \dots , f_n$ of n polynomials in ${\mathbb {C}}[{\mathbf {x}}_n]$ of homogeneous positive degrees is a regular sequence if, for each $0 \leq i \leq n-1$ , we have a short exact sequence

(2.17) $$ \begin{align} 0 \rightarrow {\mathbb {C}}[{\mathbf {x}}_n]/(f_1, \dots, f_i) \xrightarrow{\, \, \times f_{i+1} \, \, } {\mathbb {C}}[{\mathbf {x}}_n]/(f_1, \dots, f_i) \xrightarrow{ \, \, \mathrm{can.} \, \,} {\mathbb {C}}[{\mathbf {x}}_n]/(f_1, \dots ,f_i, f_{i+1}) \rightarrow 0, \end{align} $$

where the first map is induced by multiplication by $f_{i+1}$ and the second map is the canonical projection. If the regular sequence $f_1, \dots , f_n$ consists of homogeneous polynomials, the quotient ring ${\mathbb {C}}[{\mathbf {x}}_n]/(f_1, \dots , f_n)$ is a finite-dimensional graded vector space with Hilbert series

(2.18) $$ \begin{align} {\mathrm {Hilb}}({\mathbb {C}}[{\mathbf {x}}_n]/(f_1, \dots, f_n); q) = [\deg f_1]_q \cdots [\deg f_n]_q. \end{align} $$

An Artinian graded quotient ${\mathbb {C}}[{\mathbf {x}}_n]/{\mathfrak {a}}$ of ${\mathbb {C}}[{\mathbf {x}}_n]$ is a complete intersection if ${\mathfrak {a}} = (f_1, \dots , f_n)$ for some length n regular sequence $f_1, \dots , f_n \in {\mathbb {C}}[{\mathbf {x}}_n]$ of homogeneous polynomials.

The regularity of a sequence $f_1, \dots , f_n \in {\mathbb {C}}[{\mathbf {x}}_n]$ of polynomials of homogeneous positive degree can be interpreted in terms of the variety cut out by $f_1, \dots , f_n$ . Given any set $S \subseteq {\mathbb {C}}[{\mathbf {x}}_n]$ of polynomials, write

(2.19) $$ \begin{align} {\mathbf {V}}(S) := \{ {\mathbf {z}} \in {\mathbb {C}}^n \,:\, f({\mathbf {z}}) = 0 \text{ for all}\ f \in S \} \end{align} $$

for the locus of points in ${\mathbb {C}}^n$ on which the polynomials in S vanish.

Let ${\mathfrak {a}} \subseteq {\mathbb {C}}[{\mathbf {x}}_n]$ be an ideal and let $f \in {\mathbb {C}}[{\mathbf {x}}_n]$ be a polynomial. The colon ideal (or ideal quotient) is

(2.20) $$ \begin{align} ({\mathfrak {a}} : f) := \{ g \in {\mathbb {C}}[{\mathbf {x}}_n] \,:\, f \cdot g \in {\mathfrak {a}} \} \subseteq {\mathbb {C}}[{\mathbf {x}}_n]. \end{align} $$

It is not difficult to check that $({\mathfrak {a}} : f)$ is an ideal in ${\mathbb {C}}[{\mathbf {x}}_n]$ which contains ${\mathfrak {a}}$ , and that $({\mathfrak {a}} : f) = {\mathbb {C}}[{\mathbf {x}}_n]$ if and only if $f \in {\mathfrak {a}}$ .

Colon ideals will play a crucial role in our work, and we will need a criterion for determining a generating set for them. Let $A = \bigoplus _{i = 0}^d A_i$ be a finite-dimensional graded ${\mathbb {C}}$ -algebra with $A_d \neq 0$ . The algebra A is a Poincaré duality algebra if

• • its top component $A_d \cong {\mathbb {C}}$ is a 1-dimensional complex vector spaces, and

• • for any $0 \leq i \leq d$ , the multiplication map $A_i \otimes A_{d-i} \longrightarrow A_d \cong {\mathbb {C}}$ is a perfect pairing.

If $A = \bigoplus _{i = 0}^d A_d$ is a Poincaré duality algebra with $d \neq 0$ , the maximal degree d is called the socle degree of A. The following commutative algebra lemma will be remarkably useful to us.

We remark that [Reference Abe, Horiguchi, Masuda, Murai and Sato2, Lem. 2.4] was stated over the field ${\mathbb {R}}$ of real numbers, but its proof goes through without change for arbitrary fields.

The polynomial ring ${\mathbb {C}}[{\mathbf {x}}_n]$ inherits a theory of harmonics from the superspace ring $\Omega _n$ . Partial differentiation yields an action $\odot : {\mathbb {C}}[{\mathbf {x}}_n] \times {\mathbb {C}}[{\mathbf {x}}_n] \rightarrow {\mathbb {C}}[{\mathbf {x}}_n]$ of the polynomial ring ${\mathbb {C}}[{\mathbf {x}}_n]$ on itself, which gives rise to an inner product

(2.21) $$ \begin{align} \langle -, - \rangle: {\mathbb {C}}[{\mathbf {x}}_n] \times {\mathbb {C}}[{\mathbf {x}}_n] \rightarrow {\mathbb {C}} \quad \quad \langle f, g \rangle = \text{ constant term of } f \odot \overline{g}. \end{align} $$

If $I \subseteq {\mathbb {C}}[{\mathbf {x}}_n]$ is a homogeneous ideal, we have a direct sum decomposition ${\mathbb {C}}[{\mathbf {x}}_n] = I \oplus I^{\perp }$ and an identification

(2.22) $$ \begin{align} I^{\perp} = \{ g \in {\mathbb {C}}[{\mathbf {x}}_n] \,:\, f \odot g = 0 \text{ for all}\ f \in I \} \end{align} $$

of the harmonic space $I^{\perp }$ as a subspace of ${\mathbb {C}}[{\mathbf {x}}_n]$ .

The harmonic theory of the classical coinvariant ideal $I_n \subseteq {\mathbb {C}}[{\mathbf {x}}_n]$ is given as follows. Let $\delta _n \in {\mathbb {C}}[{\mathbf {x}}_n]$ be the Vandermonde determinant

(2.23) $$ \begin{align} \delta_n := \prod_{i < j} (x_j - x_i) \in {\mathbb {C}}[{\mathbf {x}}_n]. \end{align} $$

Then $I_n^{\perp }$ is a cyclic ${\mathbb {C}}[{\mathbf {x}}_n]$ -module under the $\odot $ -action generated by $\delta _n$ . In symbols, we have

(2.24) $$ \begin{align} I_n^{\perp} = {\mathbb {C}}[{\mathbf {x}}_n] \odot \delta_n. \end{align} $$

We write $H_n$ for the subspace $I_n^{\perp } = {\mathbb {C}}[{\mathbf {x}}_n] \odot \delta _n \subseteq {\mathbb {C}}[{\mathbf {x}}_n]$ ; we have an isomorphism $R_n \cong H_n$ of graded ${\mathfrak {S}}_n$ -modules. The annihilator of $\delta _n$ under the $\odot $ -action is precisely the coinvariant ideal $I_n$ :

(2.25) $$ \begin{align} {\mathrm {ann}}_{{\mathbb {C}}[{\mathbf {x}}_n]}(\delta_n) = \{ f \in {\mathbb {C}}[{\mathbf {x}}_n] \,:\, f \odot \delta_n = 0 \} = I_n. \end{align} $$

3.1 A regular sequence in ${\mathbb {C}}[{\mathbf {x}}_n]$

Our first lemma gives a general technique for constructing interesting elements of the supercoinvariant ideal $SI_n$ .

Proof. The operator d commutes with the action of ${\mathfrak {S}}_n$ on $\Omega _n$ , so the result follows from the Leibniz formula

(3.1) $$ \begin{align} d(fg) = df \cdot g \pm f \cdot dg, \quad \quad \end{align} $$

which holds for any bihomogeneous $f, g \in \Omega _n$ (the sign is $+$ if f has even fermionic degree and $-$ otherwise) and the relation $d \circ d = 0$ .

Ideals in $\Omega _n$ that are closed under the action of d are called differential ideals. To the knowledge of the authors, the supercoinvariant ideal $SI_n$ is the first differential ideal that has received significant attention in algebraic combinatorics.

The most important elements of $SI_n$ arising from Lemma 3.1 are as follows. Let $h_r, e_r \in {\mathbb {C}}[{\mathbf {x}}_n]$ be the complete homogeneous and elementary symmetric polynomials

(3.2) $$ \begin{align} h_r := \sum_{1 \leq i_1 \leq \cdots \leq i_r \leq n} x_{i_1} \cdots x_{i_r} \quad \quad e_r := \sum_{1 \leq i_1 < \cdots < i_r \leq n} x_{i_1} \cdots x_{i_r}. \end{align} $$

Here and throughout, if $S \subseteq [n]$ is an index set, we use $h_r(S)$ and $e_r(S)$ to denote the complete homogeneous and elementary symmetric polynomials of degree r in the variables indexed by S. For example, we have

$$ \begin{align*} h_2(134) = x_1^2 + x_1 x_3 + x_1 x_4 + x_3^2 + x_3 x_4 + x_4^2 \quad \text{and} \quad e_2(134) = x_1 x_3 + x_1 x_4 + x_3 x_4. \end{align*} $$

For any subset $S \subseteq [n]$ , it is well-known that

(3.3) $$ \begin{align} h_r(S) \in I_n \quad \text{whenever}\ r> n - |S|. \end{align} $$

Indeed, (3.3) follows inductively from the identity $h_r(S \cup i) = x_i h_{r-1}(S \cup i) + h_r(S)$ , which holds whenever $i \notin S$ . By Lemma 3.1, we have

(3.4) $$ \begin{align} dh_r(S) \in SI_n \quad \text{whenever}\ r> n - |S|. \end{align} $$

Elements of $SI_n$ of the form (3.3) and (3.4) are the only ones we will need.

For any subset $J \subseteq [n]$ , we construct a sequence $(q_{J,1}, q_{J,2}, \dots , q_{J,n})$ of superspace elements as follows. Given $J \subseteq [n]$ , the sequence $(q_{J,1}, q_{J,2}, \dots , q_{J,n})$ in $\Omega _n$ is defined by

(3.5) $$ \begin{align} q_{J,i} := \begin{cases} h_i(\{i, i+1, \dots, n\}) \cdot \theta_J & i < \min(J) \\ dh_r(J \cup \{i+1, \dots, n\}) \cdot \theta_{J - \max(J \cap \{1, \dots, i\})} & i \geq \min(J), \end{cases} \end{align} $$

where in the second branch $r = n - |J \cup \{i+1, \dots , n\}| + 1$ .

The superspace elements $q_{J,i}$ may be visualized (and remembered) as follows. Consider a linear array of n boxes labeled $1, \dots , n$ from left to right, where the boxes in positions $j \in J$ are decorated with a $\theta $ . We consider moving a pointer from left to right along this array. When $n = 7$ and $J = \{3,5,6\}$ , the picture is shown in Figure 1.

• • When the pointer is at a position i which is strictly to the left of all of the $\theta $ decorations, the corresponding superspace element is $q_{J,i} = h_i(\{i, i+1, \dots , n\}) \cdot \theta _J$ .

• • When the pointer is at a position i which is weakly to the right of at least one $\theta $ decoration, the corresponding superspace element is $q_{J,i} = dh_r(J \cup \{i+1, \dots , n \}) \cdot \theta _{\overline {J}}$ , where $\overline {J}$ consists of all elements of J except for the closest element $j \in J$ weakly to the right of the pointer and $r = n - |J \cup \{i+1, \dots , n\}| + 1$ is the minimal degree such that $h_r(J \cup \{i+1, \dots , n\}) \in I_n$ lies in the classical coinvariant ideal.

In our example, we have

$$ \begin{align*} q_{J,1} = h_1(1234567) \cdot \theta_{356} \quad q_{J,2} = h_2(234567) \cdot \theta_{356} \quad q_{J,3} = d h_3(34567) \cdot \theta_{56} \quad q_{J,4} = d h_4(3567) \cdot \theta_{56} \end{align*} $$

$$ \begin{align*} q_{J,5} = d h_4(3567) \cdot \theta_{36} \quad q_{J,6} = d h_4(3567) \cdot \theta_{35} \quad q_{J,7} = d h_5(356) \cdot \theta_{35}. \end{align*} $$

We record some basic observations about the polynomials $q_{J,i}$ .

Proof. The memberships (3.3) and (3.4) and the construction of $q_{J,i}$ imply (1). Moving the pointer from $i-1$ to i does not change the bosonic degree of $q_{J,i}$ when the box i is decorated with a $\theta $ , and increases the bosonic degree of $q_{J,i}$ by 1 otherwise, so (2) also holds by construction. To see why (3) is true, observe that the only surviving fermionic monomials $\theta _K$ in the expression

(3.6) $$ \begin{align} dh_r(J \cup \{i+1, \dots, n\}) \cdot &\theta_{J - \max(J \cap \{1, \dots, i\})} = \nonumber\\ & \sum_{k \in J \cup \{i+1, \dots, n \}} \partial_k h_r(J \cup \{i+1, \dots, n\}) \cdot \theta_k \cdot \theta_{J - \max(J \cap \{1, \dots, i\})} \end{align} $$

satisfy $J \leq _{\mathrm {Gale}} K$ .

Figure 1

The pointer construction for the superspace elements $q_{J,i} \in \Omega _n$ and the polynomials $p_{J,i} \in {\mathbb {C}}[{\mathbf {x}}_n]$ . Here, $n = 7$ and $J = \{3,5,6\}$ . Boxes whose positions in J are indicated with a $\theta $ . Shaded boxes indicate the set of bosonic variables involved at each stage; boxes with a $\theta $ are always shaded. The degree of the h-polynomial in $q_{J,i}$ and $p_{J,i}$ is the number of unshaded boxes, plus one. Once the pointer crosses the red line (i.e., reaches the minimum element of J), the definition of $q_{J,i}$ and $p_{J,i}$ involves derivatives. The pointer points to shaded boxes to the left of the right line, and an unshaded box or $\theta $ box to the right of the red line. The $\theta $ decoration with an $\times $ corresponds to an unused $\theta $ -variable $\theta _s$ in the case of $q_{J,i}$ , or a partial derivative $\partial _s$ in the case of $p_{J,i}$ . The $\times $ appears on the closest $\theta $ which is weakly to the left of the pointer.

We will be interested in the projections of the $q_{J,i}$ to ${\mathbb {C}}[{\mathbf {x}}_n] \cdot \theta _J$ . To this end, define polynomials $(p_{J,1}, p_{J,2}, \dots , p_{J,n}) \in {\mathbb {C}}[{\mathbf {x}}_n]$ by the rule

(3.7) $$ \begin{align} p_{J,i} = \begin{cases} h_i(i, i+1, \dots, n\}) & i < \min(J) \\ \partial_s( h_r(J \cup \{i+1, \dots, n\})) & s = \max(J \cap \{1, \dots, i\}), \end{cases} \end{align} $$

where (as in the definition of $q_{J,i}$ ) in the second branch $r := n - |J \cup \{i+1, \dots , n\}| + 1$ . As with the superspace elements $q_{J,i}$ , the polynomials $p_{J,i}$ are easily visualized using the pointer construction. The index s on the partial derivative operator $\partial _s$ is the maximal element of j weakly to the left of the pointer. As the pointer moves from left to right, the degree of the h-polynomial increases and its number of arguments decreases. When $n = 7$ and $J = \{3,5,6\}$ , Figure 1 yields

$$ \begin{align*} p_{J,1} = h_1(1234567) \quad p_{J,2} = h_2(234567) \quad p_{J,3} = \partial_3 h_3(34567) \quad p_{J,4} = \partial_3 h_4(3567) \end{align*} $$

$$ \begin{align*} p_{J,5} = \partial_5 h_4(3567) \quad p_{J,6} = \partial_6 h_4(3567) \quad p_{J,7} = \partial_6 h_5(356). \end{align*} $$

By Lemma 3.2 (3), we have

(3.8) $$ \begin{align} q_{J,i} \equiv \pm p_{J,i} \cdot \theta_J \quad\mod \bigoplus_{J <_{\mathrm {Gale}} K} {\mathbb {C}}[{\mathbf {x}}_n] \cdot \theta_K \end{align} $$

for all subsets $J \subseteq [n]$ and $1 \leq i \leq n$ . The polynomials $p_{J,i} \in {\mathbb {C}}[{\mathbf {x}}_n]$ are the ‘Gale-leading terms’ of the $q_{J,i} \in \Omega _n$ and will give us access to the tools of classical commutative algebra in ${\mathbb {C}}[{\mathbf {x}}_n]$ . In particular, we will prove that $p_{J,1}, \dots , p_{J,n}$ is a regular sequence in ${\mathbb {C}}[{\mathbf {x}}_n]$ as long as $1 \notin J$ . Our first step in doing so is an identity involving partial derivatives of homogeneous symmetric polynomials in partial variable sets.

Lemma 3.3. If $S \subseteq [n]$ is any subset with $a,b \in S$ and $c \notin S$ , then

(3.9) $$ \begin{align} \partial_a h_r(S) = \partial_b h_r(S) + (x_c - x_b) \cdot \partial_b h_{r-1}(S \cup c) - (x_c - x_a) \cdot \partial_a h_{r-1}(S \cup c) \end{align} $$

for all $r> 1$ .

In Lemma 3.3, we allow the possibility $a = b$ , in which case the claimed equation is trivial.

Proof. The RHS of Equation (3.9) may be expanded and regrouped to give

(3.10) $$ \begin{align} &\partial_b h_r(S) + (x_c - x_b) \partial_b h_{r-1}(S \cup c) - (x_c - x_a) \partial_a h_{r-1}(S \cup c) = \nonumber\\ &\quad \left[ \partial_b (h_r(S) + x_c h_{r-1}(S \cup c)) - \partial_a(x_c h_{r-1}(S \cup c)) \right] - [x_b \partial_b h_{r-1}(S \cup c)] + [x_a \partial_a h_{r-1}(S \cup c)]. \end{align} $$

Since $h_r(S) + x_c h_{r-1}(S \cup c) = h_r(S \cup c)$ , the expression in the first set of brackets $[ \, \cdots ]$ on the RHS of Equation (3.10) equals $[\partial _b h_r(S \cup c) - \partial _a h_r(S \cup c) + \partial _a h_r(S)]$ , the expression in the second set of brackets equals $[ \partial _b (x_b h_{r-1}(S \cup c)) - h_{r-1}(S \cup c) ]$ , and the expression in the third set of brackets equals $ [ \partial _a (x_a h_{r-1}(S \cup c)) - h_{r-1}(S \cup c)]$ . Plugging all this in yields

(3.11)

with the indicated cancellations. After performing these cancellations, the RHS of Equation (3.11) may be regrouped as

(3.12) $$ \begin{align} [\partial_b h_r(S \cup c) - \partial_a h_r(S \cup c) + \partial_a h_r(S)] - [ \partial_b (x_b h_{r-1}(S \cup c))] + [ \partial_a (x_a h_{r-1}(S \cup c))] \nonumber\\ = \partial_a h_r(S) + \left\{ \partial_b (h_r(S \cup c) - x_b h_{r-1}(S \cup c)) \right\} - \left\{ \partial_a(h_r(S \cup c) - x_a h_{r-1}(S \cup c)) \right\}. \end{align} $$

Since the expression $h_r(S \cup c) - x_b h_{r-1}(S \cup c) = h_r( (S \cup c) - b )$ is independent of $x_b$ , the partial derivative $\partial _b$ in the first set of curly braces $\{ \, \cdots \}$ on the RHS of Equation (3.12) vanishes; the expression in the second set of curly braces vanishes for similar reasons. This completes the proof of Equation (3.9).

The polynomial identity in Lemma 3.3 is, to the authors, somewhat miraculous; it would be nice to have a conceptual understanding of ‘why’ it should be true. We use this identity to show that the ideal ${\mathcal {I}}_J$ generated by the polynomials $p_{J,1}, \dots , p_{J,n} \in {\mathbb {C}}[{\mathbf {x}}_n]$ contains certain strategic partial derivatives.

Proof. We prove the following claim, which is stronger than the lemma and amenable to induction.

Claim: The polynomials in question lie in the ideal

(3.13) $$ \begin{align} {\mathcal{I}}^{\prime}_J := (p_{J,j_0}, p_{J,j_0 + 1}, \dots, p_{J,n}) \subseteq {\mathbb {C}}[x_{j_0}, x_{j_0 + 1}, \dots, x_n], \end{align} $$

where $j_0 = \min (J)$ is the smallest element of J.

The pointer construction makes it clear that the generators of ${\mathcal {I}}^{\prime }_J$ do not involve the variables $x_1, x_2, \dots , x_{j_0 - 1}$ and so lie in the polynomial ring ${\mathbb {C}}[x_{j_0}, x_{j_0 + 1}, \dots , x_n]$ generated by the remaining variables. We prove the Claim by induction on the number $n - j_0 + 1$ of variables in the ambient ring of  ${\mathcal {I}}^{\prime }_J$ .

If $J = \{n-r+1, \dots , n-1, n\}$ is a terminal subset of $[n]$ , the polynomials in the Claim are generators of the ideal ${\mathcal {I}}^{\prime }_J$ . Furthermore, for any subset $J \subseteq [n]$ , if $j = \max (J)$ is the largest element of J, then $\partial _j h_{n-|J|+1}(J) = p_{J,n}$ is also a generator of ${\mathcal {I}}^{\prime }_J$ .

By the above paragraph, we may assume that $j_0 = \min (J) \neq \max (J)$ and that there exists an element $c \in [n] - J$ with $c> j_0$ . Let $c_0 := \min \{ j_0 < c \leq n \,:\, c \notin J \}$ be the smallest such c and define $S \subseteq [n]$ by

(3.14) $$ \begin{align} S := \{ j_0, j_0 + 1, \dots , n-1, n \} - \{ c_0 \}. \end{align} $$

Observe that the elements $j_0, j_0 + 1, \dots , c_0 - 2, c_0 - 1$ of S lie in J. Let $r := n - |S| + 1$ . We apply Lemma 3.3 iteratively as follows.

• • Since $\partial _{c_0 - 1} h_r(S), \partial _{c_0 - 1} h_{r-1}(S \cup c_0), \partial _{c_0 - 2}(S \cup c_0) \in {\mathcal {I}}^{\prime }_J$ , Lemma 3.3 with $a = c_0 - 2, b = c_0 - 1$ , and $c = c_0$ implies $\partial _{c_0 - 2} h_r(S) \in {\mathcal {I}}^{\prime }_J$ .

• • Since $\partial _{c_0 - 2} h_r(S), \partial _{c_0 - 2} h_{r-1}(S \cup c_0), \partial _{c_0 - 3}(S \cup c_0) \in {\mathcal {I}}^{\prime }_J$ , Lemma 3.3 with $a = c_0 - 3, b = c_0 - 2,$ and $c = c_0$ implies $\partial _{c_0 - 3} h_r(S) \in {\mathcal {I}}^{\prime }_J$ .

• • Since $\partial _{c_0 - 3} h_r(S), \partial _{c_0 - 3} h_{r-1}(S \cup c_0), \partial _{c_0 - 4}(S \cup c_0) \in {\mathcal {I}}^{\prime }_J$ , Lemma 3.3 with $a = c_0 - 3, b = c_0 - 2,$ and $c = c_0$ implies $\partial _{c_0 - 4} h_r(S) \in {\mathcal {I}}^{\prime }_J$ , and so on.

We see that the polynomials

(3.15) $$ \begin{align} p^{\prime}_{J,j_0} := \partial_{j_0} h_r(S) \quad p^{\prime}_{J,j_0 + 1} := \partial_{j_0 + 1} h_r(S) \quad \dots \quad p^{\prime}_{J,c_0 - 1} := \partial_{c_0 - 1} h_r(S) \end{align} $$

lie in ${\mathcal {I}}^{\prime }_J$ so that

(3.16) $$ \begin{align} (p^{\prime}_{J,j_0}, p^{\prime}_{J,j_0 + 1}, \dots, p^{\prime}_{J,c_0 - 1}, p_{J,c_0 + 1}, p_{J, c_0 + 2}, \dots, p_{J, n}) \subseteq {\mathcal{I}}^{\prime}_J \end{align} $$

as ideals in ${\mathbb {C}}[x_{j_0}, x_{j_0 + 1}, \dots , x_n]$ . But the generators on the ideal on the LHS of (3.16) do not involve the variable $x_{c_0}$ . In fact, if we consider the variable set

(3.17) $$ \begin{align} {\mathbf {x}} := (x_{j_0}, x_{j_0 + 1}, \dots, x_{c_0 - 1}, x_{c_0 + 1}, \dots, x_{n-1}, x_n) \end{align} $$

obtained from our old variable set $(x_{j_0}, x_{j_0 + 1}, \dots , x_n)$ by removing $x_{c_0}$ , then

(3.18) $$ \begin{align} (p^{\prime}_{J,j_0}, p^{\prime}_{J,j_0 + 1}, \dots, p^{\prime}_{J,c_0 - 1}, p_{J,c_0 + 1}, p_{J, c_0 + 2}, \dots, p_{J, n}) = {\mathcal{I}}^{\prime}_{J'} \end{align} $$

as ideals in ${\mathbb {C}}[{\mathbf {x}}]$ where $J' = (J - j_0) \cup c_0$ is the corresponding cyclic rotation of the set J. Since the variable set ${\mathbf {x}}$ contains fewer variables than the original set $\{ x_{j_0}, x_{j_0 + 1}, \dots , x_n \}$ , we are done by induction.

An example may help clarify Lemma 3.4 and its proof. Suppose $n = 7$ and $J = \{3,5,6\}$ . We have ${\mathcal {I}}_J = (p_{J,1}, \dots , p_{J,7})$ , where

$$ \begin{align*} p_{J,1} = h_1(1234567) \quad p_{J,2} = h_2(234567) \quad p_{J,3} = \partial_3 h_3(34567) \quad p_{J,4} = \partial_3 h_4(3567) \end{align*} $$

$$ \begin{align*} p_{J,5} = \partial_5 h_4(3567) \quad p_{J,6} = \partial_6 h_4(3567) \quad p_{J,7} = \partial_6 h_5(356). \end{align*} $$

Our aim is to show that the ideal ${\mathcal {I}}_J$ contains the elements

$$ \begin{align*} \partial_3 h_5(356), \quad \partial_5 h_5(356), \quad \partial_6 h_5(356). \end{align*} $$

To this end, we reason as follows.

• • The element $\partial _6 h_5(356) = p_{J,7}$ is a generator of ${\mathcal {I}}_J$ . This was one of the desired memberships.

• • Since $\partial _3 h_3(34567) = p_{J,3}, \partial _3 h_4(3567) = p_{J,4},$ and $\partial _5 h_4(3567) = p_{J,5}$ are elements of ${\mathcal {I}}_J$ , Lemma 3.3 with $S = \{3,5,6,7\}, a = 3, b = 5$ and $c = 4$ implies $\partial _3 h_4(3567) \in {\mathcal {I}}_J$ .

• • Since $\partial _3 h_4(3567), \partial _6 h_4(3567) = p_{J,6},$ and $\partial _6 h_5(356)$ are elements of ${\mathcal {I}}_J$ , Lemma 3.3 with ${S = \{3,5,6\}, a = 3, b = 6}$ and $c = 7$ implies $\partial _3 h_5(356) \in {\mathcal {I}}_J$ . This was one of the desired memberships.

• • Since $\partial _5 h_4(3567) = p_{J,5}, \partial _6 h_4(3567) = p_{J,6}, \partial _6 h_5(356) \in {\mathcal {I}}_J$ , Lemma 3.3 with $S = \{3,5,6\}, a = 5, b = 6$ and $c = 7$ implies $\partial _5 h_5(356) \in {\mathcal {I}}_J$ . This was the remaining desired membership.

Observe that we did not use the generators $p_{J,1}, p_{J,2} \in {\mathcal {I}}_J$ to derive these memberships, so that in fact we showed membership in the smaller ideal

$$ \begin{align*} {\mathcal{I}}^{\prime}_J = (p_{J,3}, p_{J,4}, p_{J,5}, p_{J,6}, p_{J,7}) \subseteq {\mathbb {C}}[x_3,x_4,x_5,x_6,x_7]. \end{align*} $$

If $1 \in J$ , then $p_{J,1} = \partial _1 h_1(x_1, \dots , x_n) = \partial _1 (x_1 + \cdots + x_n) = 1$ is a unit in ${\mathbb {C}}[{\mathbf {x}}_n]$ . Correspondingly, we have ${\mathrm {st}}(J)_1 = 0$ . Since members of regular sequences are required to be of positive homogeneous degree, we must exclude this case from Lemma 3.5.

Proof. Since $1 \notin J$ , the sequence ${\mathrm {st}}(J)$ has positive entries. The assertion on degrees is Lemma 3.2 (2). As in Lemma 3.4, let ${\mathcal {I}}_J = ( p_{J,1}, \dots , p_{J,n} ) \subseteq {\mathbb {C}}[{\mathbf {x}}_n]$ . By Lemma 2.2, it is enough to show that the variety ${\mathbf {V}}({\mathcal {I}}) \subseteq {\mathbb {C}}^n$ cut out by ${\mathcal {I}}$ consists of $\{ 0 \}$ alone. We use elimination to focus on coordinates in ${\mathbb {C}}^n$ indexed by J.

Swanson and Wallach proved [Reference Swanson and Wallach37, Lem. 6.2] that that the polynomials $\partial _j h_{n-|J|+1}(J)$ for $j \in J$ have no common zero in ${\mathbb {C}}^J$ . By Lemma 3.4, for any locus point $a = (a_1, \dots , a_n) \in {\mathbf {V}}({\mathcal {I}}_J)$ , we must have $a_j = 0$ for any $j \in J$ . Setting the variables $\{x_j \,:\, j \in J \}$ to zero in the remaining polynomials

(3.19) $$ \begin{align} p_{J,i} \mid_{x_j \rightarrow 0 \text{ for } j \in J} \quad \quad (i \notin J) \end{align} $$

gives a sequence of positive degree homogeneous polynomials in ${\mathbb {C}}[x_i \,:\, i \notin J]$ which are easily seen to be triangular. We conclude that $a_i = 0$ for $i \notin J$ , so that $a = 0$ as required.

Lemma 3.5 implies that the quotient ring ${\mathbb {C}}[{\mathbf {x}}_n]/(p_{J,1}, \dots , p_{J,n})$ has Hilbert series

(3.20) $$ \begin{align} {\mathrm {Hilb}}( {\mathbb {C}}[{\mathbf {x}}_n]/(p_{J,1}, \dots, p_{J,n}); q) = [{\mathrm{st}}(J)_1]_q \cdots [{\mathrm{st}}(J)_n]_q. \end{align} $$

This formula remains true when $1 \in J$ , for then $p_{J,1} = 1$ and ${\mathbb {C}}[{\mathbf {x}}_n]/(p_{J,1}, \dots , p_{J,n}) = 0$ . In particular, there exists a set ${\mathcal {B}}_n(J) \subseteq {\mathbb {C}}[{\mathbf {x}}_n]$ of homogeneous polynomials with degree generating function $[{\mathrm {st}}(J)_1]_q \cdots [{\mathrm {st}}(J)_n]_q$ such that ${\mathcal {B}}_n(J)$ descends to a vector space basis of ${\mathbb {C}}[{\mathbf {x}}_n]/(p_{J,1}, \dots , p_{J,n})$ .

3.2 An abstract straightening lemma

The proof of Lemma 3.5 relied on a a tricky induction in Lemma 3.4 and miraculous polynomial identity in Lemma 3.3. Our next result should persuade the reader that Lemma 3.5 was worth the effort.

Lemma 3.6. (Straightening)

Let $J \subseteq [n]$ with ${\mathrm {st}}(J) = ({\mathrm {st}}(J)_1, \dots , {\mathrm {st}}(J)_n)$ . There exists a finite set ${\mathcal {B}}_n(J) \subseteq {\mathbb {C}}[{\mathbf {x}}_n]$ of nonzero homogeneous polynomials with degree generating function

(3.21) $$ \begin{align} \sum_{m \in {\mathcal{B}}_n(J)} q^{\deg(m)} = [{\mathrm{st}}(J)_1]_q [{\mathrm{st}}(J)_2]_q \cdots [{\mathrm{st}}(J)_n]_q \end{align} $$

such that for any polynomial $f \in {\mathbb {C}}[{\mathbf {x}}_n]$ , we have an expression of the form

(3.22) $$ \begin{align} f \cdot \theta_J = \left(\sum_{m\in {\mathcal{B}}_n(J)} c_{f,m} \cdot m \cdot \theta_J \right) + g + \Sigma, \end{align} $$

where

• • the $c_{f,m} \in {\mathbb {C}}$ are constants which depend on f and m,

• • the element $g \in SI_n$ lies in the supercoinvariant ideal, and

• • the ‘error term’ $\Sigma $ lies in $\bigoplus _{J <_{{\mathrm {Gale}}} K} {\mathbb {C}}[{\mathbf {x}}_n] \cdot \theta _K$ .

Proof. As explained after Lemma 3.5, there exists a set ${\mathcal {B}}_n(J) \subseteq {\mathbb {C}}[{\mathbf {x}}_n]$ of homogeneous polynomials with the given degree generating function which descends to a vector space basis of ${\mathbb {C}}[{\mathbf {x}}_n]/(p_{J,1}, \dots , p_{J,n})$ . We prove that ${\mathcal {B}}_n(J)$ satisfies the conditions of the lemma.

The given polynomial $f \in {\mathbb {C}}[{\mathbf {x}}_n]$ may be written as

(3.23) $$ \begin{align} f = \left( \sum_{m \in {\mathcal{B}}_n(J)} c_{f,m} \cdot m \right) + \sum_{j = 1}^n A_j \cdot p_{J,j} \end{align} $$

for some scalars $c_{f,m} \in {\mathbb {C}}$ and polynomials $A_j \in {\mathbb {C}}[{\mathbf {x}}_n]$ . Multiplying both sides of Equation (3.23) by $\theta _J$ yields

(3.24) $$ \begin{align} f \cdot \theta_J = \left( \sum_{m \in {\mathcal{B}}_n(J)} c_{f,m} \cdot m \cdot \theta_J \right) + \sum_{j = 1}^n A_j \cdot p_{I,j} \cdot \theta_J. \end{align} $$

Equation (3.8) gives the relation

(3.25) $$ \begin{align} f \cdot \theta_J \equiv \left( \sum_{m \in {\mathcal{B}}_n(J)} c_{f,m} \cdot m \cdot \theta_J \right) + \sum_{j = 1}^n \pm A_j \cdot q_{J,j} \quad\mod \bigoplus_{J <_{\mathrm {Gale}} K} {\mathbb {C}}[{\mathbf {x}}_n] \cdot \theta_K \end{align} $$

modulo the linear subspace $\bigoplus _{J <_{\mathrm {Gale}} K} {\mathbb {C}}[{\mathbf {x}}_n] \cdot \theta _K$ of $\Omega _n$ . Finally, Lemma 3.2 (1) implies the membership $g := \sum _{j = 1}^n \pm A_j \cdot q_{J,j} \in SI_n$ , which completes the proof.

Lemma 3.6 implies that the set ${\mathcal {B}}_n \subseteq \Omega _n$ of superspace elements given by

(3.26) $$ \begin{align} {\mathcal{B}}_n := \bigsqcup_{J \subseteq [n]} {\mathcal{B}}_n(J) \cdot \theta_J \end{align} $$

descends to a spanning set in $SR_n$ . Indeed, if this were not the case, let $J \subseteq [n]$ be a Gale-maximal subset such that $f \cdot \theta _J \in \Omega _n$ does not lie in the span of ${\mathcal {B}}_n$ modulo $SI_n$ for some $f \in {\mathbb {C}}[{\mathbf {x}}_n]$ . Lemma 3.6 implies that

(3.27) $$ \begin{align} f \cdot \theta_J \equiv \left(\sum_{m\in {\mathcal{B}}_n(J)} c_{f,m} \cdot m \cdot \theta_J \right) + \Sigma \qquad \mod SI_n \end{align} $$

for some constants $c_{f,m} \in {\mathbb {C}}$ where $\Sigma \in \bigoplus _{J <_{{\mathrm {Gale}}} K} {\mathbb {C}}[{\mathbf {x}}_n] \cdot \theta _K$ . The term in the parentheses certainly lies in the span of ${\mathcal {B}}_n$ . The Gale-maximality of J implies that $\Sigma $ lies in the span of ${\mathcal {B}}_n$ , as well, giving a contradiction.

The straightening result of Lemma 3.6 is rather abstract in that it does not give a formula for the polynomials in ${\mathcal {B}}_n(J)$ . While any generic set of polynomials of the appropriate degrees will do, the authors are unaware of an explicit formula for the set ${\mathcal {B}}_n(J)$ . In general, objects related to $SR_n$ have resisted analysis by Gröbner-theoretic techniques, which is reflected in the abstract statement of Lemma 3.6.

Lemma 3.6 implies an upper bound for the bigraded Hilbert series of $SR_n$ . Given two polynomials $f(q,z), g(q,z)$ in variables $q, z$ , we write $f \leq g$ to mean that $g - f$ is a polynomial in $q,z$ with nonnegative coefficients.

Proposition 3.7. The bigraded Hilbert series ${\mathrm {Hilb}}(SR_n;q,z)$ is bounded above by

(3.28) $$ \begin{align} {\mathrm {Hilb}}(SR_n;q,z) \leq \sum_{J \subseteq [n]} z^{|J|} \sum_{f \in {\mathcal{B}}_n(J)} q^{\deg(f)} = \sum_{k = 1}^n z^{n-k} \cdot [k]!_q \cdot {\mathrm {Stir}}_q(n,k). \end{align} $$

4.1 The differential operators ${\mathfrak {D}}_J$

Let ${\mathcal {H}}$ be the $n \times n$ matrix of complete homogeneous symmetric polynomials whose row i, column j entry is given by

(4.1) $$ \begin{align} {\mathcal{H}} := \left( h_{i-j}(x_i, x_{i+1}, \dots, x_n) \right)_{\substack{1 \leq i \leq n \\ 1 \leq j \leq n}}. \end{align} $$

We have $h_0 = 1$ and interpret $h_{j-i} = 0$ whenever $i> j$ , so the matrix ${\mathcal {H}}$ is lower triangular with 1’s on the diagonal. We use the matrix ${\mathcal {H}}$ to define a family of differential operators as follows. Given a subset $K \subseteq [n]$ , we introduce the ‘reversal’ notation

(4.2) $$ \begin{align} K^* := \{ n-k+1 \,:\, k \in K \}. \end{align} $$

Definition 4.1. For any subset $J \subseteq [n]$ , define a differential operator ${\mathfrak {D}}_J$ acting on $\Omega _n$ by

(4.3) $$ \begin{align} {\mathfrak{D}}_J(f) := \sum_{|I| = |J|} (-1)^{\sum I} \Delta_{[n] - J, ([n] - I)^*}({\mathcal{H}}) \odot d_I (f), \end{align} $$

where $\Delta _{[n] - J, ([n] - I)^*}({\mathcal {H}}) \in {\mathbb {C}}[{\mathbf {x}}_n]$ is the minor of ${\mathcal {H}}$ with row set $[n] - J$ and column set $([n] - I)^*$ .

Since the matrix ${\mathcal {H}}$ is lower triangular, the coefficient of $d_I$ in ${\mathfrak {D}}_J$ is zero unless we have $I^* \leq _{\mathrm {Gale}} J$ in Gale order. As an example, when $n = 3$ , the matrix ${\mathcal {H}}$ is given by

$$ \begin{align*} {\mathcal{H}} = \begin{pmatrix} 1 & 0 & 0 \\ x_2 + x_3 & 1 & 0 \\ x_3^2 & x_3 & 1 \end{pmatrix} \end{align*} $$

and we have the differential operators

acting on superspace elements $f \in \Omega _3$ where the indicated minors of ${\mathcal {H}}$ vanish for support reasons. Applying the formula $d_i(f) = ( x_1^i \odot f ) \theta _1 + (x_2^i \odot f) \theta _2 + (x_3^i \odot f) \theta _3$ , these operators may be expressed in the more illuminating form

$$ \begin{align*} {\mathfrak{D}}_{12}(f) &= ( x_1 (x_1 - x_2) (x_1 - x_3) x_2 (x_2 - x_3) ) \odot f \cdot \theta_1 \theta_2 \\ {\mathfrak{D}}_{13}(f) &= ( x_1^2 x_2^2 + x_1^2 x_2 x_3 - x_1 x_2^2 x_3 - x_1^3 x_3 ) \odot f \cdot \theta_1 \theta_2 - (x_1 (x_1 - x_2) (x_1 - x_3) x_3) \odot f \cdot \theta_1 \theta_3 \\ {\mathfrak{D}}_{23}(f) &= (x_1^2 x_2 - x_1 x_2^2) \odot f \cdot \theta_1 \theta_2 + (x_1^2 x_3 - x_1 x_3^2) \odot f \cdot \theta_1 \theta_3 + (x_2 (x_2 - x_3) x_3) \odot f \cdot \theta_2 \theta_3, \end{align*} $$

which reveals a triangularity property with respect to the fermionic monomials $\theta _1 \theta _2, \theta _1 \theta _3$ and $\theta _2 \theta _3$ . Furthermore, the ‘leading coefficient’ $\theta _J$ involved in ${\mathfrak {D}}_J$ has the form $f_J \odot (-)$ up to a sign where the polynomials $f_J$ were defined in the introduction. We will show that this is a general phenomenon. Our first lemma in this direction is a simple result on the application of the $d_I$ operator to polynomials in ${\mathbb {C}}[{\mathbf {x}}_n]$ ; its proof is left to the reader.

Lemma 4.2. Let $f \in {\mathbb {C}}[{\mathbf {x}}_n]$ be a polynomial and let $I = \{ i_1 < \cdots < i_r \}$ and $K = \{k_1 < \cdots < k_r \}$ be two subsets of $[n]$ of the same size. The coefficient of $\theta _K$ in $d_I(f) \in \Omega _n$ is the determinant of partial derivatives

(4.4) $$ \begin{align} \begin{vmatrix} \partial_{k_1}^{i_1} f & & \cdots & & \partial_{k_1}^{i_r} f \\ & & & & \\ \vdots & & & & \vdots \\ & & & & \\ \partial_{k_r}^{i_1} f & & \cdots & & \partial_{k_r}^{i_r} f \\ \end{vmatrix}. \end{align} $$

Definition 4.1 and Lemma 4.2 motivate the following family of polynomials ${\mathfrak {F}}_{J,K} \in {\mathbb {C}}[{\mathbf {x}}_n]$ indexed by pairs of subsets $J, K \subseteq [n]$ . The definition of the ${\mathfrak {F}}_{J,K}$ also involves the matrix ${\mathcal {H}}$ .

Definition 4.3. Let J and K be two subsets of $[n]$ of the same size. Define a polynomial ${\mathfrak {F}}_{J,K} \in {\mathbb {C}}[{\mathbf {x}}_n]$ by

(4.5) $$ \begin{align} {\mathfrak{F}}_{J,K} := \sum_{|I| = |J| = |K|} (-1)^{\sum I} \Delta_{[n] - J, ([n] - I)^*}({\mathcal{H}}) \cdot \left| x_k^i \right|{}_{k \in K, i \in I}, \end{align} $$

where the row and column indices in the determinant $\left | x_k^i \right |{}_{k \in K, i \in I}$ are written in increasing order.

The differential operators ${\mathfrak {D}}_J$ and the polynomials ${\mathfrak {F}}_{J,K}$ are related by

(4.6) $$ \begin{align} {\mathfrak{D}}_J(f) = \sum_{|K| = |J|} \left( {\mathfrak{F}}_{J,K} \odot f \right) \times \theta_K \end{align} $$

for all $f \in {\mathbb {C}}[{\mathbf {x}}_n]$ .

We aim to show that the ${\mathfrak {F}}_{J,K}$ are triangular with respect to Gale order. As a first step, we express ${\mathfrak {F}}_{J,K}$ as a single $n \times n$ determinant.

Lemma 4.5. Let $J = \{ j_1 < \cdots < j_r \}$ and $K = \{ k_1 < \cdots < k_r \}$ be two subsets of $[n]$ of the same size. Write $b(J) = (b(J)_1 < b(J)_2 < \cdots )$ for the entries in the complement $[n] - J$ of the set J, written in increasing order. Define an $n \times n$ matrix $A_{J,K}$ in block form

(4.7) $$ \begin{align} A_{J,K} = \begin{pmatrix} B_{J,K} \\ C_{J,K} \end{pmatrix}, \end{align} $$

where the top block $B_{J,K}$ has size $r \times n$ and entries

(4.8) $$ \begin{align} B_{J,K} = \begin{pmatrix} x_{k_1}^n & & \cdots & & x_{k_1}^1 \\ \vdots & & & & \vdots \\ x_{k_r}^n & & \cdots & & x_{k_r}^1 \\ \end{pmatrix} \end{align} $$

and the bottom block $C_{J,K}$ has size $(n-r) \times n$ and entries

(4.9) $$ \begin{align} C_{J,K} = ( h_{b(J)_i - j}(x_{b(J)_i}, x_{b(J)_i + 1}, \dots, x_n) )_{1 \leq i \leq n-r, \, \, 1 \leq j \leq n}. \end{align} $$

We have ${\mathfrak {F}}_{J,K} = \pm \det (A_{J,K})$ .

Proof. The determinant $\det (A_{J,K})$ may be evaluated using the rule

(4.10) $$ \begin{align} \det(A_{J,K}) = \sum_{\substack{I \subseteq [n] \\ |I| = r}} (-1)^{\sum I - {r +1 \choose 2}} \cdot \Delta_I(B_{J,K}) \cdot \Delta_{[n]-I}(C_{J,K}), \end{align} $$

where $\Delta _I(B_{J,K})$ is the maximal minor of $B_{J,K}$ with column set I and $\Delta _{[n]-I}(C_{J,K})$ is the maximal minor of $C_{J,K}$ with complementary column set $[n] - I$ . Now compare with the definition of ${\mathfrak {F}}_{J,K}$ .

To illustrate Lemma 4.5, we let $n = 5$ , $J = \{1,3\}$ , and write $K = \{a,b\}$ for $1 \leq a < b \leq 5$ . Lemma (4.5) expresses ${\mathfrak {F}}_{J,K} = {\mathfrak {F}}_{13,ab}$ as the following $5 \times 5$ determinant:

$$ \begin{align*} {\mathfrak{F}}_{13,ab} = \pm \begin{vmatrix} x_a^5 & x_a^4 & x_a^3 & x_a^2 & x_a^1 \\[2pt] x_b^5 & x_b^4 & x_b^3 & x_b^2 & x_b^1 \\[2pt] h_1(2345) & 1 & 0 & 0 & 0 \\[2pt] h_3(45) & h_2(45) & h_1(45) & 1 & 0 \\[2pt] h_4(5) & h_3(5) & h_2(5) & h_1(5) & 1 \end{vmatrix}. \end{align*} $$

The determinant in Lemma 4.5 may be evaluated to give the desired triangularity relation for the polynomials ${\mathfrak {F}}_{J,K}$ . Lemma 4.5 will also imply that the ${\mathfrak {F}}_{J,J}$ are given the polynomials $f_J \in {\mathbb {C}}[{\mathbf {x}}_n]$ appearing in the introduction. We reiterate their definition below.

Definition 4.6. For any subset $J \subseteq [n]$ , let $f_J \in {\mathbb {C}}[{\mathbf {x}}_n]$ be the polynomial

(4.11) $$ \begin{align} f_J := \prod_{j \in J} x_j \left( \prod_{i = j+1}^n (x_j - x_i) \right). \end{align} $$

Observe that the f-polynomial corresponding to a set J factors $f_J = \prod _{j \in J} f_{\{j\}}$ into f-polynomials corresponding to singletons contained in J. The polynomials $f_J \in {\mathbb {C}}[{\mathbf {x}}_n]$ will have deep ties to the supercoinvariant ring $SR_n$ . For later use, we record a criterion for when $f_J$ lies in the classical coinvariant ideal $I_n \subseteq {\mathbb {C}}[{\mathbf {x}}_n]$ .

Proof. Suppose $1 \in J$ , so that $f_{\{1\}} \mid f_J$ . We claim $f_{\{1\}} = x_1 (x_1 - x_2) ( x_1 - x_3) \cdots (x_1 - x_n) \in I_n$ . Indeed, if t is a new variable, then modulo $I_n$ we have

(4.12) $$ \begin{align} 1 \equiv \frac{1}{(1 - t x_1) (1 - t x_2 ) \cdots (1 - t x_n)} \quad\mod I_n \end{align} $$

so that

(4.13) $$ \begin{align} (1 - t x_2) \cdots (1 - t x_n) \equiv \frac{1}{1 -t x_1} \quad\mod I_n, \end{align} $$

and taking the coefficient of $t^d$ yields

(4.14) $$ \begin{align} (-1)^d e_d(x_2, \dots, x_n) \equiv x_1^d \quad\mod I_n. \end{align} $$

We conclude that

(4.15) $$ \begin{align} f_{\{1\}} = \sum_{d = 0}^{n-1} (-1)^d e_d(x_2, \dots, x_n) \cdot x_1^{n-d} \equiv n \cdot x_1^n \equiv 0 \quad\mod I_n, \end{align} $$

where we used the fact that $x_1^n \in I_n$ .

Now suppose $1 \notin J$ . Recall that ${\mathrm {ann}}_{{\mathbb {C}}[{\mathbf {x}}_n]}(\delta _n) = I_n$ under the $\odot $ -action of ${\mathbb {C}}[{\mathbf {x}}_n]$ on itself. Therefore, to show that $f_J \notin I_n$ , it is enough to show that $f_J \odot \delta _n \neq 0$ . Since $f_J = \prod _{j \in J} f_{\{j\}}$ , it suffices to show that $f_J \odot \delta _n \neq 0$ when $J = J_0 := \{2, 3, \dots , n \}$ is the maximal subset of $[n]$ not containing $1$ . By definition, we have

(4.16) $$ \begin{align} f_{J_0} = (x_2 x_3 \cdots x_n) \times \prod_{2 \leq r < s \leq n} (x_r - x_s) \end{align} $$

so that the terms of $f_{J_0}$ are (up to a global sign) the terms of $\delta _n$ in which $x_1$ does not appear. If we use $\doteq $ to denote equality up to a nonzero scalar, we therefore have

(4.17) $$ \begin{align} f_{J_0} \odot \delta_n \doteq f_{J_0} \odot f_{J_0}> 0, \end{align} $$

where we used the fact that both $f_{J_0}$ and $\delta _n$ are homogeneous of degree ${n \choose 2}$ and the fact that $f \odot f> 0$ for any homogeneous nonzero polynomial f.

The determinant in Lemma 4.5 may be evaluated to give the desired triangularity relation for the polynomials ${\mathfrak {F}}_{J,K}$ . Lemma 4.5 will also imply that ${\mathfrak {F}}_{J,J} = \pm f_J$ .

Lemma 4.8. We have ${\mathfrak {F}}_{J,K} = 0$ unless $J \geq _{{\mathrm {Gale}}} K$ in Gale order. Furthermore, we have

(4.18) $$ \begin{align} {\mathfrak{F}}_{J,J} = \pm f_J. \end{align} $$

Proof. We factor $\prod _{k \in K} x_k$ out of the upper block $B_{J,K}$ of the determinant $\det (A_{J,K}) = \pm {\mathfrak {F}}_{J,K}$ in Lemma 4.5. Next, we apply column operations to eliminate the $h_d(S)$ ’s in the bottom portion $C_{J,K}$ of this determinant.

Specifically, we focus on each pivot 1 in $C_{J,K}$ from bottom to top. Working to the left from a given pivot 1, in row i of $C_{J,K}$ , we subtract $x_c$ times column j of $A_{J,K}$ from column $j-1$ , where $x_c$ is a variable belonging to $\{x_{b(J)_i}, \dots , x_n \} - \{ x_{b(J)_{i+1}}, \dots , x_n \}$ . Since $h_d(S) = x_c h_{d-1}(S) + h_d(S - c)$ whenever $c \in S$ , this eliminates the $h_d(S)$ ’s from the bottom portion $C_{J,K}$ of our determinant. After performing these operations, the determinant $\det (A_{J,K})$ is reduced to a single maximal minor of its (new) upper portion $B_{J,K}$ , from which the result follows.

To see how this works in our example $J = \{1,3\}$ and $K = \{a, b\}$ , we factor out $x_a x_b$ from the top two rows of our determinant to get

$$ \begin{align*} \begin{vmatrix} x_a^5 & x_a^4 & x_a^3 & x_a^2 & x_a^1 \\[2pt] x_b^5 & x_b^4 & x_b^3 & x_b^2 & x_b^1 \\[2pt] h_1(2345) & 1 & 0 & 0 & 0 \\[2pt] h_3(45) & h_2(45) & h_1(45) & 1 & 0 \\[2pt] h_4(5) & h_3(5) & h_2(5) & h_1(5) & 1 \end{vmatrix} = x_a x_b \begin{vmatrix} x_a^4 & x_a^3 & x_a^2 & x_a^1 & 1 \\[2pt] x_b^4 & x_b^3 & x_b^2 & x_b^1 & 1 \\[2pt] h_1(2345) & 1 & 0 & 0 & 0 \\[2pt] h_3(45) & h_2(45) & h_1(45) & 1 & 0 \\[2pt] h_4(5) & h_3(5) & h_2(5) & h_1(5) & 1 \end{vmatrix}. \end{align*} $$

Our focus shifts to the bottom three rows. Since the bottom pivot 1 is in column 5, we subtract $x_5$ times each column from the previous column, resulting in

$$ \begin{align*} x_a x_b \begin{vmatrix} x_a^4 & x_a^3 & x_a^2 & x_a^1 & 1 \\[2pt] x_b^4 & x_b^3 & x_b^2 & x_b^1 & 1 \\[2pt] h_1(2345) & 1 & 0 & 0 & 0 \\[2pt] h_3(45) & h_2(45) & h_1(45) & 1 & 0 \\[2pt] h_4(5) & h_3(5) & h_2(5) & h_1(5) & 1 \end{vmatrix} = x_a x_b \begin{vmatrix} x_a^4 - x_a^3 x_5 & x_a^3 - x_a^2 x_5 & x_a^2 - x_a x_5 & x_a^1 - x_5 & 1 \\[2pt] x_b^4 - x_b^3 x_5 & x_b^3 - x_b^2 x_5 & x_b^2 - x_b x_5 & x_b^1 - x_5 & 1 \\[2pt] h_1(234) & 1 & 0 & 0 & 0 \\[2pt] h_3(4) & h_2(4) & h_1(4) & 1 & 0 \\[2pt] 0 & 0 & 0 & 0 & 1 \end{vmatrix}. \end{align*} $$

This has the effect of eliminating the argument $x_5$ from the h’s. To eliminate the $x_4$ ’s from the arguments of the h’s, we focus on the pivot 1 in row 4, column 4. For each column before column 2, we subtract $x_4$ times the subsequent column. The result is

$$ \begin{align*} x_a x_b \begin{vmatrix} x_a^4 - x_a^3 x_5 - x_a^3 x_4 + x_a^2 x_4 x_5 & x_a^3 - x_a^2 x_5 - x_a^2 x_4 + x_a x_4 x_5 & x_a^2 - x_a x_5 - x_a x_4 + x_4 x_5 & x_a^1 - x_5 & 1 \\[2pt] x_b^4 - x_b^3 x_5 - x_b^3 x_4 + x_b^2 x_4 x_5 & x_b^3 - x_b^2 x_5 - x_b^2 x_4 + x_b x_4 x_5 & x_b^2 - x_b x_5 - x_b x_4 + x_4 x_5 & x_b^1 - x_5 & 1 \\[2pt] h_1(23) & 1 & 0 & 0 & 0 \\[2pt] 0 & 0 & 0 & 1 & 0 \\[2pt] 0 & 0 & 0 & 0 & 1 \end{vmatrix}. \end{align*} $$

The entries of this matrix are better written using elementary symmetric polynomials, viz.

$$ \begin{align*} x_a x_b \begin{vmatrix} x_a^4 - x_a^3 e_1(45) + x_a^2 e_2(45) & x_a^3 - x_a^2 e_1(45) + x_a e_2(45) & x_a^2 - x_a e_1(45) + e_2(45) & x_a - e_1(5) & 1 \\[2pt] x_b^4 - x_b^3 e_1(45) + x_b^2 e_2(45) & x_b^3 - x_b^2 e_1(45) + x_b e_2(45) & x_b^2 - x_b e_1(45) + e_2(45) & x_b - e_1(5) & 1 \\[2pt] h_1(23) & 1 & 0 & 0 & 0 \\[2pt] 0 & 0 & 0 & 1 & 0 \\[2pt] 0 & 0 & 0 & 0 & 1 \end{vmatrix}. \end{align*} $$

Continuing to pivot 1 in row 3, column 2, we multiply the second column by $- x_2 - x_3$ and add it to the first column. The result is

$$ \begin{align*} x_a x_b \begin{vmatrix} x_a^4 - x_a^3 e_1(2345) + x_a^2 e_2(2345) - x_a e_3(2345) + e_4(2345) & x_a^3 - x_a^2 e_1(45) + x_a e_2(45) & x_a^2 - x_a e_1(45) + e_2(45) & x_a - e_1(5) & 1 \\[2pt] x_b^4 - x_b^3 e_1(2345) + x_b^2 e_2(2345) - x_b e_3(2345) + e_4(2345) & x_b^3 - x_b^2 e_1(45) + x_b e_2(45) & x_b^2 - x_b e_1(45) + e_2(45) & x_b - e_1(5) & 1 \\[2pt]0 & 1 & 0 & 0 & 0 \\[2pt] 0 & 0 & 0 & 1 & 0 \\[2pt] 0 & 0 & 0 & 0 & 1 \end{vmatrix}. \end{align*} $$

which may be expressed as the smaller $2 \times 2$ determinant

$$ \begin{align*} x_a x_b \begin{vmatrix} x_a^4 - x_a^3 e_1(2345) + x_a^2 e_2(2345) - x_a e_3(2345) + e_4(2345) & x_a - e_1(5) \\[2pt] x_b^4 - x_b^3 e_1(2345) + x_b^2 e_2(2345) - x_b e_3(2345) + e_4(2345) & x_b - e_1(5) \end{vmatrix}. \end{align*} $$

The entries in this smaller determinant factor as

$$ \begin{align*} x_a x_b \begin{vmatrix} (x_a - x_2)(x_a - x_3)(x_a - x_4)(x_a - x_5) & (x_a - x_5) \\[2pt] (x_b - x_2)(x_b - x_3)(x_b - x_4)(x_b - x_5) & (x_b - x_5) \\ \end{vmatrix}. \end{align*} $$

For general $J = \{j_1 < \cdots < j_r \}$ and $K = \{k_1 < \cdots < k_r \}$ , this procedure yields the formula

(4.19) $$ \begin{align} {\mathfrak{F}}_{J,K} = \pm \prod_{k \in K} x_k \cdot \begin{vmatrix} \prod_{i> j_q} (x_{k_p} - x_i) \end{vmatrix}_{1 \leq p, q \leq r}, \end{align} $$

expressing ${\mathfrak {F}}_{J,K}$ as an $r \times r$ determinant times the variables indexed by K. If $k_p> j_q$ , the $(p,q)$ -entry of the determinant in Equation (4.19) vanishes. If $J \not \leq _{\mathrm {Gale}} K$ , this determinant has the block form $\begin {vmatrix} * & * \\ \mathbf {0} & * \end {vmatrix}$ where the southwest block of zeros intersects the main diagonal, so that ${\mathfrak {F}}_{J,K} = 0$ . If $J = K$ , the determinant in Equation (4.19) is upper triangular, and the product of diagonal entries is as described in the statement of the lemma.

4.2 The colon ideal $(I_n : f_J)$ in ${\mathbb {C}}[{\mathbf {x}}_n]$

Thanks to Lemma 4.8, the differential operators ${\mathfrak {D}}_J$ exhibit useful triangularity with respect to the Gale order on fermionic monomials. In order to consider their fermionic leading term $\theta _J$ , we will study the colon ideals

(4.20) $$ \begin{align} (I_n : f_J) := \{ g \in {\mathbb {C}}[{\mathbf {x}}_n] \,:\, g \cdot f_J \in I_n \} \subseteq {\mathbb {C}}[{\mathbf {x}}_n], \end{align} $$

where $I_n \subseteq {\mathbb {C}}[{\mathbf {x}}_n]$ is the classical coinvariant ideal.

It will turn out (Theorem 4.12) that the ideal $(I_n : f_J)$ has two other equivalent definitions. As a first step to proving this, we introduce the following bigraded subspace of $\Omega _n$ .

Swanson and Wallach showed [Reference Swanson and Wallach37] that $SH^{\prime }_n$ is annihilated by the supercoinvariant ideal $SI_n \subseteq \Omega _n$ under the $\odot $ -action, so that $SH^{\prime }_n \subseteq SH_n$ is a subset of the superharmonic space. We will show (Theorem 5.1) that in fact $SH^{\prime }_n = SH_n$ . For now, we can use $SH^{\prime }_n$ and our triangularity results (Lemmas 3.2 and 4.8) to show that the polynomials $p_{J,1}, \dots , p_{J,n}$ from Section 3 lie in $(I_n : f_J)$ .

Proof. Let $q_{J,i} \in SI_n$ be the supercoinvariant ideal element associated to $p_{J,i}$ . By Lemma 3.2 (3), we have

(4.21) $$ \begin{align} q_{J,i} = p_{J,i} \cdot \theta_J + \sum_{J <_{\mathrm {Gale}} L} A_L \cdot \theta_L \end{align} $$

for some polynomials $A_L \in {\mathbb {C}}[{\mathbf {x}}_n]$ . However, Lemma 4.8 implies that

(4.22) $$ \begin{align} {\mathfrak{D}}_J(\delta_n) \doteq (f_J \odot \delta_n) \cdot \theta_J + \sum_{K <_{\mathrm {Gale}} J} B_K \cdot \theta_K \end{align} $$

for some $B_K \in {\mathbb {C}}[{\mathbf {x}}_n]$ , where $\doteq $ denotes equality up to a nonzero scalar. Since ${\mathfrak {D}}_J$ is a linear combination of $d_I$ operators with coefficients in $\partial _1, \dots , \partial _n$ , we have

(4.23) $$ \begin{align} {\mathfrak{D}}_J(\delta_n) \in SH^{\prime}_n \subseteq SH_n, \end{align} $$

where the $\subseteq $ is justified by the work of Swanson and Wallach [Reference Swanson and Wallach37]. Since $SI_n$ annihilates $SH_n$ under the $\odot $ -action and $q_{J,i} \in SI_n$ , we have

(4.24) $$ \begin{align} q_{J,i} \odot {\mathfrak{D}}_J(\delta_n) = 0. \end{align} $$

The triangularity relations (4.21) and (4.22) force

(4.25) $$ \begin{align} (p_{J,i} \cdot f_J) \odot \delta_n = p_{J,i} \odot (f_J \odot \delta_n) = 0. \end{align} $$

Since ${\mathrm {ann}}_{{\mathbb {C}}[{\mathbf {x}}_n]}(\delta _n) = I_n$ , this implies that $p_{J,i} \cdot f_J \in I_n$ , or equivalently, $p_{J,i} \in (I_n : f_J)$ .

The colon ideals $(I_n : f_J)$ are connected to a class of permutations in ${\mathfrak {S}}_n$ . If $1 \leq j \leq n$ , a permutation $w \in {\mathfrak {S}}_n$ is called j-resentful if $w(j) = n$ , or the value $w(j)+1$ appears among ${w(j+1), w(j+2), \dots , w(n)}$ .Footnote ⁴ The permutation w is j-Nietzschean if it is not j-resentful.Footnote ⁵

If $J \subseteq [n]$ is a subset, a permutation $w \in {\mathfrak {S}}_n$ is J-Nietzschean if it is j-Nietzschean for all $j \in J$ . We write

(4.26) $$ \begin{align} {\mathfrak{N}}_J := \{ w \in {\mathfrak{S}}_n \,:\, w \text{ is}\ J\text{-Nietzschean} \} \end{align} $$

for the set of all J-Nietszschean permutations in ${\mathfrak {S}}_n$ . Nietzschean permutations are counted by a simple product formula.

Proposition 4.11. Let $J \subseteq [n]$ . The number of J-Nietzschean permutations in ${\mathfrak {S}}_n$ is given by

(4.27) $$ \begin{align} |{\mathfrak{N}}_J| = \prod_{i = 1}^n {\mathrm{st}}(J)_i, \end{align} $$

where ${\mathrm {st}}(J) = ({\mathrm {st}}(J)_1, \dots , {\mathrm {st}}(J)_n)$ is the J-staircase.

Proof. We consider decomposing the one-line notation of permutations $w = [w(1), \dots , w(n)] \in {\mathfrak {S}}_n$ to the permutation $[1] \in {\mathfrak {S}}_1$ by iteratively removing the last letter $w(n)$ and ‘standardizing’ to the unique order-isomorphic permutation in ${\mathfrak {S}}_{n-1}$ . For example, the permutation $[6,3,5,1,4,7,2] \in {\mathfrak {S}}_7$ decomposes as follows:

Reversing this process, we can build up from $[1] \in {\mathfrak {S}}_1$ to a permutation in ${\mathfrak {S}}_n$ by appending a new letter to the end at each stage. In order for the resulting permutation $w = [w(1), \dots , w(n)] \in {\mathfrak {S}}_n$ to be J-Nietzschean, suppose we have a permutation $[v(1), \dots , v(k-1)] \in {\mathfrak {S}}_{k-1}$ at some intermediate stage and we want to build a permutation in ${\mathfrak {S}}_{k}$ . We may append any of the numbers in $\{1, \dots , k\}$ to $[v(1), \dots , v(k-1)]$ , except the following.

• • If $k \in J$ is a Nietzschean position, we cannot append k, since this would ultimately force $w(k) = n$ or force an entry 1 larger than $w(k)$ to appear among $w(k+1), \dots , w(n)$ , so that w would be k-resentful.

• • Whether or not k is a Nietzschean position, we cannot append a value $v(j) + 1$ for any Nietzschean position $j \in J$ satisfying $j < k$ , since this would ultimately force $w(j) + 1$ to appear among $w(j+1), \dots , w(n)$ , so that w would be j-resentful. The value $v(j)$ at a Nietzschean position $j < k$ inductively satisfies $v(j) < k-1$ .

In general, the conditions above imply that the number of choices to append to $[v(1), \dots , v(k-1)]$ is

(4.28) $$ \begin{align} k+1 - | \{ j \in J \,:\, j \leq k \}|, \end{align} $$

which yields the claimed product formula.

We will see that $|{\mathfrak {N}}_J| = \dim {\mathbb {C}}[{\mathbf {x}}_n]/(I_n:f_J)$ , so J-Nietzschean permutations enumerate bases of ${\mathbb {C}}[{\mathbf {x}}_n] / (I_n : f_J)$ . However, the connection between Nietzschean permutations and colon ideals goes deeper than this. To explain, we recall the powerful theory of orbit harmonics.

For any subset $Z \subseteq {\mathbb {C}}^n$ , let ${\mathbf {I}}(Z) \subseteq {\mathbb {C}}[{\mathbf {x}}_n]$ be the ideal of polynomials which vanish on Z:

(4.29) $$ \begin{align} {\mathbf {I}}(Z) := \{ f \in {\mathbb {C}}[{\mathbf {x}}_n] \,:\, f({\mathbf {z}}) = 0 \text{ for all}\ {\mathbf {z}} \in Z \}. \end{align} $$

The quotient ring ${\mathbb {C}}[Z] := {\mathbb {C}}[{\mathbf {x}}_n]/{\mathbf {I}}(Z)$ is the coordinate ring of Z and has a natural identification with the family of polynomial functions $Z \longrightarrow {\mathbb {C}}$ . If we assume the locus $Z \subseteq {\mathbb {C}}^n$ is finite (as we will from here on), by Lagrange interpolation any function $Z \longrightarrow {\mathbb {C}}$ is the restriction of a polynomial in ${\mathbb {C}}[{\mathbf {x}}_n]$ , so we may identify ${\mathbb {C}}[Z]$ with the vector space formal ${\mathbb {C}}$ -linear combinations of elements of Z.

The quotient ring ${\mathbb {C}}[Z] = {\mathbb {C}}[{\mathbf {x}}_n]/{\mathbf {I}}(Z)$ is almost never graded, but there is a way to produce a graded quotient of ${\mathbb {C}}[{\mathbf {x}}_n]$ from ${\mathbf {I}}(Z)$ . For any nonzero polynomial $f \in {\mathbb {C}}[{\mathbf {x}}_n]$ , let $\tau (f)$ be the highest degree homogeneous component of f. That is, if $f = f_d + \cdots + f_1 + f_0$ where $f_i$ is homogeneous of degree i and $f_d \neq 0$ , we have $\tau (f) = f_d$ . We define a new ideal ${\mathrm {gr}} \, {\mathbf {I}}(Z) \subseteq {\mathbb {C}}[{\mathbf {x}}_n]$ by

(4.30) $$ \begin{align} {\mathrm {gr}} \, {\mathbf {I}}(Z) := ( \tau(f) \,:\, f \in {\mathbf {I}}(Z), \, f \neq 0 ) \subseteq {\mathbb {C}}[{\mathbf {x}}_n]. \end{align} $$

The ideal ${\mathrm {gr}} \, {\mathbf {I}}(Z)$ is homogeneous by construction. We have an isomorphism of vector spaces

(4.31) $$ \begin{align} {\mathbb {C}}[Z] = {\mathbb {C}}[{\mathbf {x}}_n]/{\mathbf {I}}(Z) \cong {\mathbb {C}}[{\mathbf {x}}_n]/ {\mathrm {gr}} \, {\mathbf {I}}(Z), \end{align} $$

where the latter quotient ${\mathbb {C}}[{\mathbf {x}}_n]/ {\mathrm {gr}} \, {\mathbf {I}}(Z)$ is a graded vector space. The Hilbert series of ${\mathbb {C}}[{\mathbf {x}}_n]/ {\mathrm {gr}} \, {\mathbf {I}}(Z)$ may be regarded as a q-enumerator of Z which depends in a subtle way on the embedding of Z inside ${\mathbb {C}}^n$ .

As an example, if $Z = {\mathfrak {S}}_n$ is the set of points in ${\mathbb {C}}^n$ of the form $[w(1), \dots , w(n)]$ for $w \in {\mathfrak {S}}_n$ , then ${\mathrm {gr}} \, {\mathbf {I}}({\mathfrak {S}}_n) = I_n$ is the classical coinvariant ideal and the coinvariant ring $R_n = {\mathbb {C}}[{\mathbf {x}}_n]/I_n$ is obtained in this way. The following result states that the colon ideals $(I_n : f_J)$ also arise via orbit harmonics.

Theorem 4.12. For any subset $J \subseteq [n]$ , the following three ideals in ${\mathbb {C}}[{\mathbf {x}}_n]$ are equal.

1. 1. The colon ideal $(I_n : f_J)$ .

2. 2. The ideal $(p_{J,1}, \dots , p_{J,n})$ generated by the homogeneous polynomials $p_{J,1}, \dots , p_{J,n} \in {\mathbb {C}}[{\mathbf {x}}_n]$ .

3. 3. The homogeneous ideal ${\mathrm {gr}} \, {\mathbf {I}}({\mathfrak {N}}_J)$ attached to the locus ${\mathfrak {N}}_J \subseteq {\mathbb {C}}^n$ of J-Nietzschean permutations in ${\mathfrak {S}}_n$ . Here we consider ${\mathfrak {S}}_n \subseteq {\mathbb {C}}^n$ as the set of rearrangements of the specific point $(1, 2, \dots , n) \in {\mathbb {C}}^n$ .

If ${\mathcal {I}}_J \subseteq {\mathbb {C}}[{\mathbf {x}}_n]$ denotes this common ideal, the Hilbert series of ${\mathbb {C}}[{\mathbf {x}}_n] / {\mathcal {I}}_J$ is given by

(4.32) $$ \begin{align} {\mathrm {Hilb}} \left( {\mathbb {C}}[{\mathbf {x}}_n] / {\mathcal{I}}_J; q \right) = \prod_{i = 1}^n [{\mathrm{st}}(J)_i]_q, \end{align} $$

where ${\mathrm {st}}(J) = ({\mathrm {st}}(J)_1, \dots , {\mathrm {st}}(J)_n)$ is the J-staircase.

Proof. Suppose $1 \in J$ . Lemma 4.7 states that $f_J \in I_n$ , so that $(I_n : f_J) = {\mathbb {C}}[{\mathbf {x}}_n]$ . Furthermore, we have $p_{J,1} = \partial _1 h_1(x_1, \dots , x_n) = 1$ , so that $(p_{J,1}, \dots , p_{J,n}) = {\mathbb {C}}[{\mathbf {x}}_n]$ . Finally, since every permutation $w \in {\mathfrak {S}}_n$ is 1-resentful, we have ${\mathfrak {N}}_J = \varnothing $ so that ${\mathrm {gr}} \, {\mathbf {I}}({\mathfrak {N}}_J) = {\mathbb {C}}[{\mathbf {x}}_n]$ . Since ${\mathrm {st}}(J)_1 = 0$ , we are done in this case and assume that $1 \notin J$ going forward.

Lemma 4.10 yields the containment of ideals

(4.33) $$ \begin{align} (p_{J,1}, \dots, p_{J,n}) \subseteq (I_n : f_J) \end{align} $$

so that $(2) \subseteq (1)$ . We apply Lemma 2.3 with ${\mathfrak {a}} = I_n, {\mathfrak {a}}' = (p_{J,1}, \dots , p_{J,n}),$ and $f = f_J$ . We check the conditions of this lemma.

• • The ideal $I_n$ is generated by the regular sequence $e_1, \dots , e_n \in {\mathbb {C}}[{\mathbf {x}}_n]$ . The Artinian quotient ${\mathbb {C}}[{\mathbf {x}}_n]/(e_1, \dots , e_n)$ is a complete intersection, and hence Gorenstein. Artinian Gorenstein graded quotients of ${\mathbb {C}}[{\mathbf {x}}_n]$ are Poincaré duality algebras; see, for example, [Reference Maeno and Watanabe24, Prop. 2.1]. The socle degree of $I_n$ is ${n \choose 2}$ .Footnote ⁶

• • Since $1 \notin J$ , Lemma 3.5 implies that $p_{J,1}, \dots , p_{J,n}$ is a regular sequence, so that the quotient ${\mathbb {C}}[{\mathbf {x}}_n] / (p_{J,1}, \dots , p_{J,n})$ is also a Poincaré duality algebra. The socle degree of this algebra is $\deg p_{J,1} + \cdots + \deg p_{J,n} - n = {\mathrm {st}}(J)_1 + \cdots + {\mathrm {st}}(J)_n - n$ .

• • Since $1 \notin J$ , Lemma 4.7 implies $f_J \notin I_n$ . Furthermore, the polynomial $f_J$ has degree $\deg f_J = \sum _{i = 1}^n (i - {\mathrm {st}}(J)_i)$ .

Since we have

(4.34) $$ \begin{align} {\mathrm{st}}(J)_1 + \cdots + {\mathrm{st}}(J)_n - n + \sum_{i = 1}^n (i - {\mathrm{st}}(J)_i) = {n \choose 2}, \end{align} $$

we may apply Lemma 2.3 to conclude

(4.35) $$ \begin{align} (p_{J,1}, \dots, p_{J,n}) = (I_n : f_J) \end{align} $$

so that (1) = (2). This also implies that the claimed Hilbert series formula holds for ${\mathcal {I}}_J = (1)$ or $(2)$ .

For any radical ideals ${\mathcal {I}}, {\mathcal {J}} \subseteq {\mathbb {C}}[{\mathbf {x}}_n]$ , the colon ideal $({\mathcal {I}}:{\mathcal {J}}) = \{ f \in {\mathbb {C}}[{\mathbf {x}}_n] \,:\, f \cdot {\mathcal {J}} \subseteq {\mathcal {I}} \}$ has the interpretation

(4.36) $$ \begin{align} {\mathbf {V}}({\mathcal{I}}:{\mathcal{J}}) = \overline{ {\mathbf {V}}({\mathcal{I}}) - {\mathbf {V}}({\mathcal{J}})} \end{align} $$

in terms of varieties in ${\mathbb {C}}^n$ , where the bar stands for Zariski closure. If ${\mathbf {V}}({\mathcal {I}})$ is a finite locus of points, the bar can be removed.

Write ${\mathfrak {R}}_J := {\mathfrak {S}}_n - {\mathfrak {N}}_J$ for the resentful complement of the J-Nietzschean permutations in ${\mathfrak {S}}_n$ . Recall that we take the specific embedding of ${\mathfrak {S}}_n \subset {\mathbb {C}}^n$ by taking all rearrangements of the coordinates of $(1, 2, \dots , n) \in {\mathbb {C}}^n$ . This also embeds ${\mathfrak {R}}_J$ and ${\mathfrak {N}}_J$ inside ${\mathbb {C}}^n$ .

The (inhomogeneous) polynomial

(4.37) $$ \begin{align} \tilde{f}_J := \prod_{j \in J} (x_j - n) \prod_{i> j} (x_j - x_i + 1) \end{align} $$

vanishes on ${\mathfrak {R}}_J$ . In fact, we have

(4.38) $$ \begin{align} {\mathfrak{N}}_J = {\mathfrak{S}}_n - {\mathbf {V}}(\tilde{f}_J) = {\mathbf {V}}(\tilde{I}_n) - {\mathbf {V}}(\tilde{f}_J), \end{align} $$

where $\tilde {I}_n$ is the ‘deformed version’ of the classical coinvariant ideal

(4.39) $$ \begin{align} \tilde{I}_n := \langle e_d(x_1, \dots, x_n) - e_d(1, \dots, n) \,:\, 1 \leq d \leq n \rangle. \end{align} $$

Since $\tilde {I}_n$ is radical and $\tilde {f}_J$ has no repeated factors, the Nullstellensatz implies

(4.40) $$ \begin{align} {\mathbf {I}}({\mathfrak{N}}_J) = {\mathbf {I}} ( {\mathbf {V}}(\tilde{I}_n) - {\mathbf {V}}(\tilde{f}_J) ) = {\mathbf {I}}({\mathbf {V}}(\tilde{I}_n : \tilde{f}_J)) = \sqrt{ (\tilde{I}_n : \tilde{f}_J) } = (\tilde{I}_n : \tilde{f}_J), \end{align} $$

where $\sqrt {\cdot }$ stands for the radical of an ideal. Taking associated graded ideals gives

(4.41) $$ \begin{align} {\mathrm {gr}} \, {\mathbf {I}}({\mathfrak{N}}_J) = {\mathrm {gr}} \, (\tilde{I}_n : \tilde{f}_J) \subseteq ( {\mathrm {gr}} \, \tilde{I}_n : f_J ) = (I_n : f_J), \end{align} $$

where the containment $\subseteq $ is justified by considering the leading term of a polynomial $\tilde {g} \in {\mathbb {C}}[{\mathbf {x}}_n]$ such that $\tilde {g} \cdot \tilde {f}_J \in \tilde {I}_n$ .

For arbitrary ideals ${\mathcal {I}}$ and polynomials f, the containment ${\mathrm {gr}} \, ({\mathcal {I}} : f ) \subseteq ({\mathrm {gr}} \, {\mathcal {I}} : \tau (f) )$ can certainly be strict. However, in our setting, Proposition 4.11 and the fact that

(4.42) $$ \begin{align} \dim {\mathbb {C}}[{\mathbf {x}}_n] / (I_n : f_J) = \prod_{i = 1}^n {\mathrm{st}}(J)_i = |{\mathfrak{N}}_J| \end{align} $$

imply

(4.43) $$ \begin{align} |{\mathfrak{N}}_J| = \dim {\mathbb {C}}[{\mathbf {x}}_n] / {\mathrm {gr}} \, {\mathbf {I}}({\mathfrak{N}}_J) \leq \dim {\mathbb {C}}[{\mathbf {x}}_n]/(I_n:f_J) = |{\mathfrak{N}}_J|, \end{align} $$

which forces ${\mathrm {gr}} \, {\mathbf {I}}({\mathfrak {N}}_J) = (I_n : f_J)$ so that (1) = (3) and the theorem is proved.

5.1 Operator theorem

We are ready to give our characterization of the harmonic space $SH_n = SI_n^{\perp } \subseteq \Omega _n$ . The following result was conjectured by Swanson and Wallach [Reference Swanson and Wallach37], and was previously conjectured by N. Bergeron, Li, Machacek, Sulzgruber and Zabrocki (unpublished).

Theorem 5.1. (Operator Theorem)

The superharmonic space $SH_n \subseteq \Omega _n$ is generated as a ${\mathbb {C}}[{\mathbf {x}}_n]$ -module under the $\odot $ -action by $d_I(\delta _n)$ for subsets $I \subseteq [n-1]$ . In symbols, we have

(5.1) $$ \begin{align} SH_n = \sum_{I \subseteq [n-1]} {\mathbb {C}}[{\mathbf {x}}_n] \odot d_I(\delta_n). \end{align} $$

The sum appearing in Theorem 5.1 is not direct. Since $d_i(\delta _n) = 0$ whenever $i> n$ and we have $d_i d_j = - d_j d_i$ , Theorem 5.1 may be rephrased as follows.

Proof. Observe that the sum on the RHS of Equation (5.1) is the space $SH^{\prime }_n$ of Definition 4.9. As explained after Definition 4.9, Swanson and Wallach proved [Reference Swanson and Wallach37] that $SH^{\prime }_n \subseteq SH_n$ . Since $SR_n \cong SH_n$ , Corollary 3.7 gives an upper bound on the dimension of $SH_n$ . In order to show that this containment is an equality, we use the ${\mathfrak {D}}_J$ operators and the colon ideals $(I_n : f_J)$ to show that the dimension of $SH^{\prime }_n$ is sufficiently large.

Let $J \subseteq [n]$ . Applying the differential operator ${\mathfrak {D}}_J$ to $\delta _n$ yields an element ${\mathfrak {D}}_J(\delta _n) \in SH^{\prime }_n$ . We use our lemmata to derive the following facts about the superspace element ${\mathfrak {D}}_J(\delta _n)$ .

• • By Lemma 4.2 and the vanishing assertion of Lemma 4.8, the coefficient of $\theta _K$ in ${\mathfrak {D}}_J(\delta _n)$ is zero unless $K \leq _{{\mathrm {Gale}}} J$ .

• • By Lemma 4.2 and the product formula in Lemma 4.8, the coefficient of $\theta _J$ in ${\mathfrak {D}}_J(\delta _n)$ is $\pm \, f_J \odot \delta _n $ .

For any element $f \in \Omega _n$ , the annihilator

(5.2) $$ \begin{align} {\mathrm {ann}}_{{\mathbb {C}}[{\mathbf {x}}_n]} f = \{ g \in {\mathbb {C}}[{\mathbf {x}}_n] \,:\, g \odot f = 0 \} \subseteq {\mathbb {C}}[{\mathbf {x}}_n] \end{align} $$

is an ideal in the polynomial ring ${\mathbb {C}}[{\mathbf {x}}_n]$ . For any subset $J \subseteq [n]$ , we calculate

(5.3) $$ \begin{align} {\mathrm {ann}}_{{\mathbb {C}}[{\mathbf {x}}_n]}( f_J \odot \delta_n) = ( {\mathrm {ann}}_{{\mathbb {C}}[{\mathbf {x}}_n]} \delta_n : f_J) = (I_n : f_J), \end{align} $$

where we used the fact that the annihilator of the Vandermonde $\delta _n$ is the classical coinvariant ideal $I_n$ . We claim that there exists a set ${\mathcal {B}}_n(J) \subseteq {\mathbb {C}}[{\mathbf {x}}_n]$ of homogeneous polynomials such that

• • the set ${\mathcal {B}}_n(J)$ has degree generating function $\sum _{g \in {\mathcal {B}}(J)} q^{\deg (g)} = \prod _{i = 1}^n [{\mathrm {st}}(J)_i]_q$ and

• • the set $\{ g \odot (f_J \odot \delta _n) \,:\, g \in {\mathcal {B}}_n(J) \}$ of polynomials in ${\mathbb {C}}[{\mathbf {x}}_n]$ is linearly independent.

Indeed, Theorem 4.12 implies that there exists a set ${\mathcal {B}}_n(J) \subseteq {\mathbb {C}}[{\mathbf {x}}_n]$ of homogeneous polynomials with the given degree generating function which descends to a linearly independent subset of ${\mathbb {C}}[{\mathbf {x}}_n] / (I_n : f_J )$ . Since ${\mathrm {ann}}_{{\mathbb {C}}[{\mathbf {x}}_n]}(\delta _n) = I_n$ , for any such ${\mathcal {B}}_n(J)$ , the set of polynomials $\{ g \odot (f_J \odot \delta _n) \,:\, g \in {\mathcal {B}}_n(J) \}$ will be linearly independent in ${\mathbb {C}}[{\mathbf {x}}_n]$ .

We combine our observations to prove the theorem. Suppose that some linear combination

(5.4) $$ \begin{align} \sum_{J \subseteq [n]} \sum_{g_J \in {\mathcal{B}}_n(J)} c_{J,g_J} (g_J \cdot \theta_J) \in \Omega_n \end{align} $$

(where the $c_{J,g_J} \in {\mathbb {C}}$ are scalars) annihilates the space $SH^{\prime }_n$ as a differential operator:

(5.5) $$ \begin{align} \left(\sum_{J \subseteq [n]} \sum_{g_J \in {\mathcal{B}}_n(J)} c_{J,g_J} (g_J \cdot \theta_J) \right) \odot SH^{\prime}_n = 0. \end{align} $$

By fermionic homogeneity, we may as well assume that

$(\star )$ for all $J \subseteq [n]$ such that there is some $c_{J,g_J} \neq 0$ , the set J has a fixed size.

In particular, for any $K \subseteq [n]$ , we have

(5.6) $$ \begin{align} \left(\sum_{J \subseteq [n]} \sum_{g_J \in {\mathcal{B}}_n(J)} c_{J,g_J} (g_J \cdot \theta_J) \right) \odot {\mathfrak{D}}_K(\delta_n) = 0. \end{align} $$

Working toward a contradiction, assume that at least one of the scalars $c_{J,g_J} \in {\mathbb {C}}$ is nonzero. Choose $J_0 \subseteq [n]$ minimal under the Gale order such that at least one $c_{J_0, g_{J_0}}$ is nonzero. Letting $K = J_0$ , we have

(5.7) $$ \begin{align} \!0 &= \left(\sum_{J \subseteq [n]} \sum_{g_J \in {\mathcal{B}}_n(J)} c_{J,g_J} ( g_J \cdot \theta_J) \right) \odot {\mathfrak{D}}_{J_0}(\delta_n)\qquad \qquad\qquad \end{align} $$

(5.8) $$ \begin{align} &\doteq \left( \sum_{g_{J_0} \in {\mathcal{B}}_n(J_0)} c_{J_0,g_{J_0}} \cdot g_{J_0} \right) \odot \text{(coefficient of}\ \theta_{J_0}\ \text{in}\ {\mathfrak{D}}_{J_0}(\delta_n)) \end{align} $$

(5.9) $$ \begin{align} &\ = \sum_{g_{J_0} \in {\mathcal{B}}_n(J_0)} c_{J_0,g_{J_0}} \cdot g_{J_0} \odot \left[ \pm f_{J_0} \odot \delta_n \right],\qquad\qquad\qquad\qquad \end{align} $$

where the second equality follows from the homogeneity assumption $(\star )$ and our Gale minimality assumption and $\doteq $ denotes equality up to a nonzero scalar. The linear independence of the set $\{ g_{J_0} \odot ( f_{J_0} \odot \delta _n ) \,:\, g_{J_0} \in {\mathcal {B}}_n(J_0) \}$ forces $c_{J_0,g_{J_0}} = 0$ for all $g_{J_0} \in {\mathcal {B}}_n(J_0)$ , which is a contradiction.

We have the chain of inequalities

(5.10) $$ \begin{align} \sum_J |{\mathcal{B}}_n(J) | \leq \dim SH^{\prime}_n \leq \dim SH_n = \dim SR_n \leq \sum_J |{\mathcal{B}}_n(J)|, \end{align} $$

where the first inequality comes from the last paragraph, the second inequality follows because ${SH^{\prime }_n \subseteq SH_n}$ , the equality holds because $SH_n$ is the harmonic space to the quotient $SR_n$ , and the last inequality holds because of Corollary 3.7. These are all equalities, forcing $SH_n = SH^{\prime }_n$ .

5.2 Hilbert series

Our goal in this subsection is to calculate the Hilbert series of $SR_n$ and describe a method for producing bases of $SR_n$ . The key to our approach is the following general linear independence criterion.

Lemma 5.2. Suppose that for each $J \subseteq [n]$ , we have a set ${\mathcal {C}}_n(J) \subseteq {\mathbb {C}}[{\mathbf {x}}_n]$ of homogeneous polynomials such that ${\mathcal {C}}_n(J)$ descends to a linearly independent subset of ${\mathbb {C}}[{\mathbf {x}}_n] / (I_n : f_J)$ . Then the set ${\mathcal {C}}_n \subseteq \Omega _n$ given by

(5.11) $$ \begin{align} {\mathcal{C}}_n := \bigsqcup_{J \subseteq [n]} {\mathcal{C}}_n(J) \cdot \theta_J \end{align} $$

descends to a linearly independent subset of $SR_n$ .

The proof of Lemma 5.2 is quite similar to the proof of Theorem 5.1.

Proof. If not, we could find scalars $c_{J, g_J} \in {\mathbb {C}}$ not all zero so that

(5.12) $$ \begin{align} \sum_{J \subseteq [n]} \sum_{g_J \in {\mathcal{C}}_n(J)} c_{J, g_J} (g_J \cdot \theta_J) = 0 \quad \text{in}\ SR_n \end{align} $$

or equivalently,

(5.13) $$ \begin{align} \left( \sum_{J \subseteq [n]} \sum_{g_J \in {\mathcal{C}}_n(J)} c_{J, g_J} (g_J \cdot \theta_J) \right) \odot SH_n = 0. \end{align} $$

If we choose $J_0 \subseteq [n]$ to be Gale-minimal such that $c_{J_0, g_{J_0}} \neq 0$ for some $g_{J_0} \in {\mathcal {C}}_n(J_0)$ , the relation

(5.14) $$ \begin{align} \left( \sum_{J \subseteq [n]} \sum_{g_J \in {\mathcal{C}}_n(J)} c_{J, g_J} (g_J \cdot \theta_J) \right) \odot {\mathfrak{D}}_{J_0} (\delta_n) = 0 \end{align} $$

implies (just as in the proof of Theorem 5.1) that

(5.15) $$ \begin{align} \sum_{g_{J_0} \in {\mathcal{C}}_n(J_0)} c_{J_0, g_{J_0}} \cdot g_{J_0} \odot (f_{J_0} \odot \delta_n) = 0, \end{align} $$

which contradicts the linear independence of ${\mathcal {C}}_n(J_0)$ in ${\mathbb {C}}[{\mathbf {x}}_n] / (I_n : f_{J_0})$ .

We have all the tools necessary to calculate the Hilbert series of $SR_n$ . This proves a conjecture [Reference Sagan and Swanson33, Conj. 6.5] of Sagan and Swanson.

Theorem 5.3. The bigraded Hilbert series of $SR_n$ is

(5.16) $$ \begin{align} {\mathrm {Hilb}}(SR_n;q,z) = \sum_{k = 1}^n z^{n-k} \cdot [k]!_q \cdot {\mathrm {Stir}}_q(n,k). \end{align} $$

Proof. For all subsets $J \subseteq [n]$ , let $B_n(J) \subseteq {\mathbb {C}}[{\mathbf {x}}_n]$ be a family of homogeneous polynomials which descends to a basis of ${\mathbb {C}}[{\mathbf {x}}_n]/(I_n : f_J)$ . By Theorem 4.12, the degree generating function for polynomials in ${\mathcal {B}}_n(J)$ is

(5.17) $$ \begin{align} \sum_{g_J \in {\mathcal{B}}_n(J)} q^{\deg(g_J)} = [{\mathrm{st}}(J)_1]_q \cdots [{\mathrm{st}}(J)_n]_q. \end{align} $$

Lemma 5.2 guarantees that ${\mathcal {B}}_n := \bigsqcup _{J \subseteq [n]} {\mathcal {B}}_n(J) \cdot \theta _J$ descends to a linearly independent subset of $SR_n$ . However, Lemma 2.1 shows that

(5.18) $$ \begin{align} &{\mathrm {Hilb}}(SR_n;q,z) \geq \sum_{J \subseteq [n]} \left( \sum_{g_J \in {\mathcal{B}}_n(J)} q^{\deg(g_J)} \right) \cdot z^{|J|} \nonumber\\ &\qquad\qquad\qquad\qquad\qquad\qquad\qquad\qquad= \sum_{k = 1}^n z^{n-k} \cdot [k]!_q \cdot {\mathrm {Stir}}_q(n,k) \geq {\mathrm {Hilb}}(SR_n;q,z), \end{align} $$

where the inequality is a consequence of Proposition 3.7. This forces the linearly independent subset ${\mathcal {B}}_n \subseteq SR_n$ to be a basis and the inequalities to be equalities.

We present a recipe for building bases of $SR_n$ from bases of the various commutative quotients ${\mathbb {C}}[{\mathbf {x}}_n] / (I_n : f_J)$ . We also show how bases of the quotients ${\mathbb {C}}[{\mathbf {x}}_n] / (I_n : f_J)$ induce bases of the superharmonic space $SH_n$ . Since $\Omega _n = SH_n \oplus SI_n$ , bases of $SH_n$ automatically descend to bases of $SR_n = \Omega _n / SI_n$ . Working in $SH_n$ can be useful for machine computations since we do not need to consider cosets $f + SI_n \in SR_n$ .

Theorem 5.4. Suppose that, for every subset $J \subseteq [n]$ , we have a set ${\mathcal {B}}_n(J) \subseteq {\mathbb {C}}[{\mathbf {x}}_n]$ of polynomials. Let

(5.19) $$ \begin{align} {\mathcal{B}}_n := \bigsqcup_{J \subseteq [n]} {\mathcal{B}}_n(J) \cdot \theta_J. \end{align} $$

The following are equivalent.

1. 1. For all $J \subseteq [n]$ , the set ${\mathcal {B}}_n(J)$ descends to a basis of the quotient ring ${\mathbb {C}}[{\mathbf {x}}_n] / (I_n : f_J)$ .

2. 2. We have a basis of the superharmonic space $SH_n$ given by

   (5.20) $$ \begin{align} \bigsqcup_{J \subseteq [n]} \left\{ (b_J \cdot \theta_J \odot {\mathfrak{D}}_J(\delta_n)) \odot {\mathfrak{D}}_J(\delta_n) \,:\, b_J \in {\mathcal{B}}_n(J) \right\}. \end{align} $$

Either of (1) or (2) implies the following.

1. 1. The set ${\mathcal {B}}_n$ descends to a basis of $SR_n$ .

Proof. The proof of Theorem 5.3 shows that (1) implies (3), so it is enough to verify that (1) and (2) are equivalent.

We define a map $\Psi $ of vector spaces

(5.21) $$ \begin{align} \Psi: \bigoplus_{J \subseteq [n]} {\mathbb {C}}[{\mathbf {x}}_n] / (I_n : f_J) \longrightarrow SH_n \end{align} $$

by the formula

(5.22) $$ \begin{align} \Psi: \left( h_J \right)_{J \subseteq [n]} \longmapsto \sum_{J \subseteq [n]} ( h_J \cdot \theta_J \odot {\mathfrak{D}}_J(\delta_n) ) \odot {\mathfrak{D}}_J(\delta_n). \end{align} $$

Since the coefficient of $\theta _J$ in ${\mathfrak {D}}_J(\delta _n)$ is $\pm (f_J \odot \delta _n)$ , we have

(5.23) $$ \begin{align} \left [ (I_n : f_J) \cdot \theta_J \right] \odot {\mathfrak{D}}_J(\delta_n) = 0 \end{align} $$

so that $\Psi $ is well-defined.

We claim that $\Psi $ is a bijection. Theorems 4.12 and 5.3 imply that the domain and codomain of $\Psi $ have the same dimension, so it is enough to show that $\Psi $ is a surjection. Indeed, Lemma 4.8 implies ${\mathfrak {D}}_J(\delta _n) = (f_J \odot \delta _n) \cdot \theta _J + \Sigma $ , where $\Sigma \in \bigoplus _{K <_{\mathrm {Gale}} J} {\mathbb {C}}[{\mathbf {x}}_n] \cdot \theta _K$ . As a consequence, we have

(5.24) $$ \begin{align} ({\mathbb {C}}[{\mathbf {x}}_n] \cdot \theta_J) \odot {\mathfrak{D}}_J(\delta_n) = {\mathbb {C}}[{\mathbf {x}}_n] \odot (f_J \odot \delta_n) \end{align} $$

for each $J \subseteq [n]$ . However, Theorem 4.12 implies that ${\mathbb {C}}[{\mathbf {x}}_n] / (I_n : f_J)$ is Artinian Gorenstein with socle spanned by $f_J \odot \delta _n$ . It follows that

(5.25) $$ \begin{align} {\mathbb {C}}[{\mathbf {x}}_n] \odot (f_J \odot \delta_n) = (I_n : f_J)^\perp \end{align} $$

as ideals in ${\mathbb {C}}[{\mathbf {x}}_n]$ . Working modulo the subspace $\bigoplus _{K <_{\mathrm {Gale}} J} {\mathbb {C}}[{\mathbf {x}}_n] \cdot \theta _K$ , we have

(5.26) $$ \begin{align} &\left[({\mathbb {C}}[{\mathbf {x}}_n] \cdot \theta_J) \odot {\mathfrak{D}}_J(\delta_n) \right] \odot {\mathfrak{D}}_J(\delta_n) = (I_n : f_J)^\perp \odot {\mathfrak{D}}_J(\delta_n) \nonumber\\[5pt] &\qquad\qquad\qquad\qquad\qquad\qquad\qquad\qquad\qquad\equiv {\mathbb {C}}[{\mathbf {x}}_n] \odot {\mathfrak{D}}_J(\delta_n) \quad\mod \bigoplus_{K <_{\mathrm {Gale}} J} {\mathbb {C}}[{\mathbf {x}}_n] \cdot \theta_K. \end{align} $$

The surjectivity of $\Psi $ follows from induction on Gale order and Theorem 5.1.

5.3 Superspace Artin monomials

Theorem 5.4 gives a recipe for finding bases ${\mathcal {B}}_n$ of $SR_n$ from bases ${\mathcal {B}}_n(J)$ of the commutative quotients ${\mathbb {C}}[{\mathbf {x}}_n] / (I_n : f_J)$ . Although a generic set ${\mathcal {B}}_n(J) \subseteq {\mathbb {C}}[{\mathbf {x}}_n]$ of polynomials of the appropriate degrees will descend to a basis of ${\mathbb {C}}[{\mathbf {x}}_n] / (I_n : f_J)$ , the complexity of the ideals $(I_n : f_J) \subseteq {\mathbb {C}}[{\mathbf {x}}_n]$ has so far obstructed progress on finding non-generic bases ${\mathcal {B}}_n(J)$ of ${\mathbb {C}}[{\mathbf {x}}_n] / (I_n : f_J)$ . We present a conjecture in this direction.

Define the set of J-Artin monomials by

(5.27) $$ \begin{align} {\mathcal{A}}_n(J) := \left\{ x_1^{a_1} \cdots x_n^{a_n} \,:\, a_i < {\mathrm{st}}(J)_i \right\}. \end{align} $$

That is, the set ${\mathcal {A}}_n(J)$ consists of monomials in ${\mathbb {C}}[{\mathbf {x}}_n]$ whose exponent sequences fit below the J-staircase. We have ${\mathcal {A}}_n(J) = \varnothing $ whenever $1 \in J$ . If $J = \varnothing $ , then ${\mathcal {A}}_n(\varnothing ) = \{ x_1^{a_1} \cdots x_n^{a_n} \,:\, a_i < i \}$ was proven by E. Artin [Reference Artin4] to descend to a basis of $R_n$ .

Artin’s result [Reference Artin4] proves Conjecture 5.5 when $J = \varnothing $ . By Theorem 5.4, if Conjecture 5.5 is true, then

(5.28) $$ \begin{align} {\mathcal{A}}_n = \bigsqcup_{J \subseteq [n]} {\mathcal{A}}_n(J) \cdot \theta_J \end{align} $$

would descend to a basis for $SR_n$ . This would prove a conjecture [Reference Sagan and Swanson33, Conj. 6.7] of Sagan and Swanson.Footnote ⁷ Thanks to Theorem 4.12, for any given J it would suffice to prove that ${\mathcal {A}}_n(J)$ is linearly independent in or spans ${\mathbb {C}}[{\mathbf {x}}_n] / (I_n : f_J)$ .

We will give evidence for Conjecture 5.5 by showing that it holds when $J = \{r+1, \dots , n-1, n\}$ is Gale-maximal. This requires a preparatory lemma on certain ideals ${\mathcal {J}}_{r,p,n} \subseteq {\mathbb {C}}[{\mathbf {x}}_n]$ generated by partial derivatives of h-polynomials.

Lemma 5.6. Let $r \geq 1$ , let $1 \leq p \leq n+1$ , and consider the ideal

(5.29) $$ \begin{align} {\mathcal{J}}_{r,p,n} := \left( \partial_1 h_r, \partial_2 h_r, \dots, \partial_{p-1} h_r, \partial_{p} h_{r+1}, \dots, \partial_{n-1} h_{r+1}, \partial_n h_{r+1} \right) \subseteq {\mathbb {C}}[{\mathbf {x}}_n] \end{align} $$

generated by n partial derivatives of homogeneous symmetric polynomials in the full variable set ${\mathbf {x}}_n$ . The set of monomials

(5.30) $$ \begin{align} {\mathcal{M}}_{r,p,n} := \left\{ x_1^{b_1} \cdots x_n^{b_n} \,:\, b_i < r-1 \text{ for}\ i < p\ \text{and } b_i < r \text{ for}\ i \geq p \right\} \end{align} $$

descends to a basis for ${\mathcal {J}}_{r,p,n}$ .

Lemma 5.6 says that ${\mathbb {C}}[{\mathbf {x}}_n]/{\mathcal {J}}_{r,p,n}$ shares the same monomial basis as the quotient by variable powers ${\mathbb {C}}[{\mathbf {x}}_n]/(x_1^{r-1} ,\dots , x_{p-1}^{r-1}, x_p^r, \dots , x_n^r)$ . Since ${\mathcal {J}}_{r,p,n}$ has inscrutable Gröbner theory, our proof of Lemma 5.6 relies on exact sequences. Harada, Horiguchi, Murai, Precup and Tymoczko used a similar style of argument to prove an analogous result [Reference Harada, Horiguchi, Murai, Precup and Tymoczko19, Thm. 7.1] on an Artin-like basis for the cohomology rings of regular nilpotent Hessenberg varieties.

Proof. If $r = 1$ and $p> 1$ , then $\partial _1 h_1 = \partial _1 (x_1 + \cdots + x_n) = 1 \in {\mathcal {J}}_{r,p,n}$ so that ${\mathcal {J}}_{r,p,n} = {\mathbb {C}}[{\mathbf {x}}_n]$ is the unit ideal. Since ${\mathcal {M}}_{1,p,n} = \varnothing $ , the result is true in this case. We assume that $r> 1$ or $r = 1$ and $p = 1$ going forward.

We leave it to the reader to verify the formula

(5.31) $$ \begin{align} x_1 \partial_1 h_r + \cdots + x_{p-1} \partial_{p-1} h_r + \partial_{p} h_{r+1} + \cdots + \partial_n h_{r+1} = C \cdot h_r, \end{align} $$

where $C = r + n - p + 1$ . Since $1 \leq p \leq n+1$ and $r \geq 1$ , we have $C> 0$ , and Equation (5.31) implies that

(5.32) $$ \begin{align} h_r \in {\mathcal{J}}_{r,p,n}. \end{align} $$

In particular, if we let $S = [n] - \{p\}$ , we have

(5.33) $$ \begin{align} \partial_p h_{r+1} = \partial_p \left( x_p h_r + h_{r+1}(S) \right) = h_r + x_p \cdot \partial_p h_r \in {\mathcal{J}}_{r,p,n} \end{align} $$

so that ${\mathcal {J}}_{r,p+1,n} \subseteq {\mathcal {J}}_{r,p,n}$ and ${\mathbf {V}}({\mathcal {J}}_{r,p,n}) \subseteq {\mathbf {V}}({\mathcal {J}}_{r,p+1,n})$ . Swanson and Wallach [Reference Swanson and Wallach37, Lem. 6.2] showed that ${\mathbf {V}}({\mathcal {J}}_{r,n+1,n}) = \{0\}$ , so that ${\mathbf {V}}({\mathcal {J}}_{r,p,n}) = \{0 \}$ (our assumptions on r and p guarantee that the generators of ${\mathcal {J}}_{r,p,n}$ have positive degree). Lemma 2.2 shows that the generating set of ${\mathcal {J}}_{r,p,n}$ is a regular sequence, so that

(5.34) $$ \begin{align} {\mathrm {Hilb}} \left( {\mathbb {C}}[{\mathbf {x}}_n] / {\mathcal{J}}_{r,p,n}; q \right) = [ r-1 ]_q^{p-1} \cdot [r]_q^{n-p+1}. \end{align} $$

The memberships (5.32) and (5.33) imply that $x_p \cdot \partial _p h_r \in {\mathcal {J}}_{r,p,n}$ , so that $x_p \cdot {\mathcal {J}}_{r,p+1,n} \subseteq {\mathcal {J}}_{r,p,n}$ . We therefore have an exact sequence

(5.35) $$ \begin{align} \frac{{\mathbb {C}}[{\mathbf {x}}_n]}{{\mathcal{J}}_{r,p+1,n}} \xrightarrow{ \, \, \times \, x_p \, \,} \frac{{\mathbb {C}}[{\mathbf {x}}_n]}{{\mathcal{J}}_{r,p,n}} \xrightarrow{ \, \, \mathrm{can.} \, \, } \frac{{\mathbb {C}}[{\mathbf {x}}_n]}{{\mathcal{J}}_{r,p,n} + (x_p)} \rightarrow 0, \end{align} $$

where the first map is induced by multiplication by $x_p$ and the second map is the canonical projection. The next step is to identify the target of the second map in this sequence in terms of a smaller variable set.

Let $\bar {{\mathbf {x}}}_{n-1} = (x_1, \dots , x_{p-1}, x_{p+1}, \dots , x_n)$ be the variable set ${\mathbf {x}}_n$ with $x_p$ removed. Let

(5.36) $$ \begin{align} \pi: {\mathbb {C}}[{\mathbf {x}}_n] \twoheadrightarrow {\mathbb {C}}[\bar{{\mathbf {x}}}_{n-1}] \end{align} $$

be the surjection defined by $\pi (x_i) = x_i$ for $i \neq p$ and $\pi (x_p) = 0$ . Let $\bar {{\mathcal {J}}}_{r,p,n-1} \subseteq {\mathbb {C}}[\bar {{\mathbf {x}}}_{n-1}]$ be the ideal with the same generating set as ${\mathcal {J}}_{r,p,n-1}$ , but in the variable set $\bar {{\mathbf {x}}}_{n-1}$ . Writing $S = [n] - \{p\}$ , for any $d> 0$ and any $i \neq p$ , we have the evaluation

(5.37) $$ \begin{align} &\pi: \partial_i h_d \mapsto \left[ \partial_i h_d \right]_{x_p \, \rightarrow \, 0} = \left[ \partial_i (x_p \cdot h_{d-1} + h_d(S)) \right]_{x_p \, \rightarrow \, 0} \nonumber \\ &\qquad\qquad\qquad\qquad\qquad\qquad\qquad\qquad\qquad= \left[ x_p \cdot \partial_i ( h_{d-1} + h_d(S)) \right]_{x_p \, \rightarrow \, 0} = \partial_i h_d(S). \end{align} $$

Furthermore, we have

(5.38) $$ \begin{align} \pi: \partial_p h_d \mapsto \left[ \partial_p h_d \right]_{x_p \, \rightarrow \, 0} = \left[ \partial_p (x_p \cdot h_{d-1} + h_d(S)) \right]_{x_p \, \rightarrow \, 0} = h_{d-1}(S). \end{align} $$

Comparing the generators of ${\mathcal {J}}_{r,p,n}$ with those of $\bar {{\mathcal {J}}}_{r,p,n-1}$ and using $h_r(S) \in \bar {{\mathcal {J}}}_{r,p,n-1}$ , we conclude that

(5.39) $$ \begin{align} \pi \left( {\mathcal{J}}_{r,p,n} + (x_p) \right) = \bar{{\mathcal{J}}}_{r,p,n-1} \end{align} $$

so that the exact sequence (5.35) induces a new exact sequence

(5.40) $$ \begin{align} \frac{{\mathbb {C}}[{\mathbf {x}}_n]}{{\mathcal{J}}_{r,p+1,n}} \xrightarrow{ \, \, \times \, x_p \, \,} \frac{{\mathbb {C}}[{\mathbf {x}}_n]}{{\mathcal{J}}_{r,p,n}} \xrightarrow{ \, \, \psi \, \, } \frac{{\mathbb {C}}[\bar{{\mathbf {x}}}_{n-1}]}{\bar{{\mathcal{J}}}_{r,p,n-1}} \rightarrow 0, \end{align} $$

where the surjection $\psi $ is induced by $\pi $ . The Hilbert series formula (5.34) implies that the dimensions of the vector spaces on either side of (5.40) add to the dimension of the vector space in the middle, so the first map in (5.40) is injective, and we have a short exact sequence

(5.41) $$ \begin{align} 0 \rightarrow \frac{{\mathbb {C}}[{\mathbf {x}}_n]}{{\mathcal{J}}_{r,p+1,n}} \xrightarrow{ \, \, \times \, x_p \, \,} \frac{{\mathbb {C}}[{\mathbf {x}}_n]}{{\mathcal{J}}_{r,p,n}} \xrightarrow{ \, \, \psi \, \, } \frac{{\mathbb {C}}[\bar{{\mathbf {x}}}_{n-1}]}{\bar{{\mathcal{J}}}_{r,p,n-1}} \rightarrow 0. \end{align} $$

By induction, we may assume that ${\mathcal {M}}_{r,p+1,n}$ descends to a basis of ${\mathbb {C}}[{\mathbf {x}}_n]/{\mathcal {J}}_{r,p+1,n}$ and that

(5.42) $$ \begin{align} \bar{{\mathcal{M}}}_{r,p,n-1} := \left\{ x_1^{b_1} \cdots x_{p-1}^{b_{p-1}} x_{p+1}^{b_{p+1}} \cdots x_n^{b_n} \,:\, b_i < r-1 \text{ for}\ i < p\ \text{and }\ b_i < r \text{ for}\ i> p \right\} \end{align} $$

descends to a basis of ${\mathbb {C}}[\bar {{\mathbf {x}}}_{n-1}]/\bar {{\mathcal {J}}}_{r,p,n-1}$ . The exactness of (5.41) and the observation

(5.43) $$ \begin{align} {\mathcal{M}}_{r,p,n} = x_p \cdot {\mathcal{M}}_{r,p+1,n} \sqcup \bar{{\mathcal{M}}}_{r,p,n-1} \end{align} $$

guarantee that ${\mathcal {M}}_{r,p,n}$ descends to a basis for ${\mathbb {C}}[{\mathbf {x}}_n]/{\mathcal {J}}_{r,p,n}$ , which completes the proof.

Proof. By Theorem 4.12, the generators of $(I_n : f_J) \subseteq {\mathbb {C}}[{\mathbf {x}}_n]$ are

(5.44) $$ \begin{align} &h_1(x_1, \dots, x_n), \, \, h_2(x_1, \dots, x_n), \quad \dots \quad h_r(x_r, \dots, x_n), \nonumber\\ &\qquad\qquad\qquad\partial_{r+1} h_{r+1}(x_{r+1}, \dots, x_n), \, \, \partial_{r+2} h_{r+1}(x_{r+1}, \dots, x_n), \quad \dots \quad \partial_n h_{r+1}(x_{r+1}, \dots, x_n). \end{align} $$

Since $h_d(x_d, \dots , x_n) = x_d^d + \Sigma $ , where $\Sigma $ is a linear combination of terms which are $> x_d^d$ in lexicographial order, we see that ${\mathbb {C}}[{\mathbf {x}}_n] / (I_n : f_J)$ is spanned by monomials of the form $x_1^{b_1} \cdots x_n^{b_n}$ where $b_i < i$ for $i \leq r$ . The generators $\partial _i h_{r+1}(x_{r+1}, \dots , x_n)$ of $(I_n : f_J)$ and Lemma 5.6 (applied over the set $\{x_{r+1}, \dots , x_n \}$ of variables indexed by J) imply that ${\mathcal {A}}_n(J)$ descends to a spanning set of ${\mathbb {C}}[{\mathbf {x}}_n] / (I_n : f_J)$ . This spanning set must be a basis by Theorem 4.12.

Given Proposition 5.7, a natural strategy for proving Conjecture 5.5 would be to induct on the position of J in Gale order. The base case of J Gale-maximal is handled by Proposition 5.7. If $i \notin J$ and $i+1 \in J$ , we have $s_i \cdot J <_{\mathrm {Gale}} J$ , where $s_i = (i,i+1)$ is the adjacent transposition in ${\mathfrak {S}}_n$ . Furthermore, the property $({\mathfrak {a}} : f g) = ( ({\mathfrak {a}} : f) : g)$ of colon ideals gives rise to a natural injection