Generalized complete-intersection conjecture for Jordan-type loci

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Let QQ be a stable partition of length ℓ\ell, let JQJ_Q be a Jordan matrix of type QQ, and let NJQ\mathcal N_{J_Q} be the variety of nilpotent matrices commuting with JQJ_Q. For a partition PP with D(P)=Q\mathfrak D(P)=Q, let WPQW^Q_P denote the corresponding Jordan-type locus. Generalized Jordan-type-locus conjecture. The closure of WPQW^Q_P in NJQ\mathcal N_{J_Q} is an irreducible complete intersection of codimension ℓ(P)−ℓ\ell(P)-\ell, with defining equations of degree at most ℓ\ell. The source presents this as a proposed generalization of an earlier theorem, and gives no resolution here.

References

Primary source

Mats Boij, Anthony Iarrobino and Leila Khatami, “Jordan Type stratification of spaces of commuting nilpotent matrices”, arXiv:2409.13553 (2025).

Progress summary

Refreshed
Claimed progress

The conjecture remains unproved in three or more blocks; only the one- and two-block cases are established, while a newly submitted proof is unverified.

The conjecture asserts that each Jordan-type stratum closure is an irreducible complete intersection of codimension ℓ(P)−ℓ\ell(P)-\ell, cut out by equations of degree at most ℓ\ell. The September 2024 paper presents this as open for ℓ≥3\ell\ge 3, despite one catalogue label calling the source “solved.”

Known results

  • The case ℓ=1\ell=1 is described as straightforward.
  • Theorem 1.3 proves the conjecture for ℓ=2\ell=2 (September 2024).
  • A November 2024 note verifies the corresponding equations in the two-part stable case, without extending the result to ℓ≥3\ell\ge 3.
  • A June 2026 survey continues to describe the broader stratification problem as open.

Community submission (unverified), August 24, 2026

A submitted proof argues the full conjecture using multiplier coordinates on the centralizer, nilpotence conditions, and proposed equations indexed by box data. The available submission is unverified and does not establish a settled result.

Current status (as of August 2026): The cases ℓ=1\ell=1 and ℓ=2\ell=2 are recorded as proved, while the generalized conjecture for ℓ≥3\ell\ge 3 remains open; the August 2026 submitted proof is unverified.

Sources

Solutions 1

ProofThis solution needs a summarySee full solutionHide full solution

The generalized complete-intersection conjecture for Jordan type

1. The theorem

Let k\mathsf k be an infinite field. For a partition RR, write ℓ(R)\ell(R) for its number of parts and D(R)\mathfrak D(R) for the Jordan type of the dense orbit in the nilpotent commutator of a nilpotent matrix of type RR. Let

Q=(q1>⋯>qℓ),qa−qa+1≥2,Q=(q_1>\cdots>q_\ell),\qquad q_a-q_{a+1}\ge2,

be stable, fix a Jordan matrix JQJ_Q, and put

NJQ={B∈Mn(k):Bn=0, BJQ=JQB}.\mathcal N_{J_Q}=\{B\in M_n(\mathsf k):B^n=0,\ BJ_Q=J_QB\}.

For every partition PP satisfying D(P)=Q\mathfrak D(P)=Q, put

WPQ={B∈NJQ:PB=P}.W_P^Q=\{B\in\mathcal N_{J_Q}:P_B=P\}.

We prove that WPQ‾\overline{W_P^Q} is an irreducible complete intersection of codimension ℓ(P)−ℓ\ell(P)-\ell, and that its defining ideal is generated by polynomials of degree at most ℓ\ell.

We use the Box Theorem of Irving--Kosir--Mastnak: on putting da=qa−qa+1d_a=q_a-q_{a+1}, the partitions in D−1(Q)\mathfrak D^{-1}(Q) are indexed bijectively by

I=(i1,…,iℓ),1≤ia≤da−1 (a<ℓ),1≤iℓ≤qℓ,(1.1)I=(i_1,\ldots,i_\ell),\qquad 1\le i_a\le d_a-1\ (a<\ell),\qquad 1\le i_\ell\le q_\ell, \tag{1.1}

and the corresponding partition PIQP_I^Q has ℓ(PIQ)=∣I∣:=∑aia\ell(P_I^Q)=|I|:=\sum_ai_a.

2. Multiplier coordinates and the proposed equations

Put O=k[[t]]O=\mathsf k[[t]] and identify the underlying k[t]\mathsf k[t]-module with

VQ=⨁a=1ℓO/(tqa),V_Q=\bigoplus_{a=1}^{\ell}O/(t^{q_a}),

where JQJ_Q is multiplication by tt. In row-vector convention a commuting endomorphism is represented by a multiplier matrix M=(mab(t))M=(m_{ab}(t)), with

ord⁡mab≥(qb−qa)+.\operatorname {ord}m_{ab}\ge(q_b-q_a)_+.

Each entry is represented by its unique polynomial in the appropriate truncation. Because the qaq_a are distinct, the semisimple quotient of the centralizer is kℓ\mathsf k^\ell. Thus MM is nilpotent exactly when the constant term of every maam_{aa} is zero. These remaining coefficients are affine coordinates on NJQ\mathcal N_{J_Q}.

Fix a box index II and set

zr=dr−1−ir−1(2≤r≤ℓ).z_r=d_{r-1}-i_{r-1}\quad(2\le r\le\ell).

For every 1≤j≤ℓ1\le j\le\ell and 2≤h≤ij2\le h\le i_j define one polynomial fj,hf_{j,h}. For j=1j=1, set

f1,h=[th−1]m11.f_{1,h}=[t^{h-1}]m_{11}.

For j>1j>1, put Ta(j,h)=∑r=aj−1ir+hT_a(j,h)=\sum_{r=a}^{j-1}i_r+h for 1≤a≤j1\le a\le j, and, for 2≤a≤j2\le a\le j, put

Wa(j)=∑r=ajzr.(2.1)W_a(j)=\sum_{r=a}^{j}z_r. \tag{2.1}

Choose the largest a∈{2,…,j}a\in\{2,\ldots,j\} for which Wa(j)≥Ta(j,h)W_a(j)\ge T_a(j,h), if such an aa exists, and otherwise put a=1a=1. (When h≤zjh\le z_j, this chooses a=ja=j.) Define

fj,h=[tTa(j,h)−1]det⁡M[a,j],[a,j].(2.2)f_{j,h}=[t^{T_a(j,h)-1}]\det M_{[a,j],[a,j]}. \tag{2.2}

For a=ja=j, (2.2) is just [th−1]mjj[t^{h-1}]m_{jj}. Let

CI=(fj,h:1≤j≤ℓ, 2≤h≤ij),YI=V(CI).C_I=(f_{j,h}:1\le j\le\ell,\ 2\le h\le i_j),\qquad Y_I=V(C_I).

There are

m=∑j(ij−1)=∣I∣−ℓ(2.3)m=\sum_j(i_j-1)=|I|-\ell \tag{2.3}

generators, and (2.2) has degree j−a+1≤ℓj-a+1\le\ell.

3. Connected permutation blocks and weighted carries

For consecutive indices write

Drj(t)=det⁡M[r,j],[r,j],Dr,r−1=1.D_{rj}(t)=\det M_{[r,j],[r,j]},\qquad D_{r,r-1}=1.

For b≤cb\le c, let KbcK_{bc} be the signed sum of the permutation monomials in DbcD_{bc} whose permutation has no break before cc; a break at u<cu<c means π([b,u])=[b,u]\pi([b,u])=[b,u]. Put Kbb=mbbK_{bb}=m_{bb}.

Every permutation has a unique decomposition into consecutive indecomposable blocks. Splitting that decomposition at the cut a−1∣aa-1\mid a gives the identity over Z\mathbb Z

Drj=Dr,a−1Daj+∑b=ra−1∑c=ajDr,b−1KbcDc+1,j.(3.1)D_{rj}=D_{r,a-1}D_{aj}+ \sum_{b=r}^{a-1}\sum_{c=a}^{j} D_{r,b-1}K_{bc}D_{c+1,j}. \tag{3.1}

If b<cb<c, every indecomposable permutation crosses each cut u∣u+1u\mid u+1, b≤u<cb\le u<c, downward at least once. A downward entry crossing that cut contains tdut^{d_u}. Consequently

ord⁡Kbc≥qb−qc=∑u=bc−1du.(3.2)\operatorname {ord}K_{bc}\ge q_b-q_c =\sum_{u=b}^{c-1}d_u. \tag{3.2}

This bound is termwise and is therefore valid in every characteristic.

Lemma 3.1 (interval carry lemma)

If all equations in CIC_I vanish at MM, then, for every 1≤r≤j≤ℓ1\le r\le j\le\ell,

ord⁡Drj≥νrjI,(3.3)\operatorname {ord}D_{rj}\ge\nu^I_{rj}, \tag{3.3}

where

ν1jI=∑u=1jiu,(3.4)\nu^I_{1j}=\sum_{u=1}^{j}i_u, \tag{3.4}

and, for r≥2r\ge2,

νrjI=min⁡p=r−1,…,j(∑u=rpzu+∑u=p+1jiu).(3.5)\nu^I_{rj}= \min_{p=r-1,\ldots,j} \left(\sum_{u=r}^{p}z_u+\sum_{u=p+1}^{j}i_u\right). \tag{3.5}

For p=r−1p=r-1 the first sum is empty; for p=jp=j the second is empty.

Proof

We prove a slightly sharper induction. While the equations at vertex jj have been processed only through hh, replace the last iji_j in (3.4)--(3.5) by hh; denote the resulting number by νrj(h)\nu_{rj}(h). Thus, for r≥2r\ge2,

νrj(h)=Tr(j,h)+min⁡(0,ϵr,ϵr+ϵr+1,…,∑u=rjϵu),(3.6)\nu_{rj}(h)=T_r(j,h)+ \min\left(0,\epsilon_r,\epsilon_r+\epsilon_{r+1},\ldots, \sum_{u=r}^{j}\epsilon_u\right), \tag{3.6}

where ϵu=zu−iu\epsilon_u=z_u-i_u for u<ju<j and ϵj=zj−h\epsilon_j=z_j-h.

Let aa be the endpoint selected in (2.1). Write Sx=∑u=xjϵu=Wx(j)−Tx(j,h)S_x=\sum_{u=x}^{j}\epsilon_u=W_x(j)-T_x(j,h). By maximality of aa, Sa≥0S_a\ge0 when a>1a>1, whereas Sx<0S_x<0 for every x>ax>a. For x>ax>a, every proper prefix in (3.6) is Sx−Sp+1>SxS_x-S_{p+1}>S_x; hence the terminal sum is the minimum. For x=ax=a, every proper prefix is nonnegative, so zero is the minimum. For x<ax<a, the minimum occurs before aa. It follows that

\begin{aligned} &\nu_{rj}(h)=\nu_{rj}(h-1)+1 &&\Longleftrightarrow r\le a,\tag{3.7}\\ &\nu_{aj}(h)=T_a(j,h) &&(a>1), \tag{3.8}\\ &\nu_{rj}(h)=W_r(j)=\nu_{rj}(h-1) &&(r>a), \tag{3.9}\\ &\nu_{rj}(h)=\nu^I_{r,a-1}+T_a(j,h) &&(r<a). \tag{3.10} \end{aligned}

We now use outer induction on jj and inner induction on hh. The case j=1j=1 is immediate from the diagonal equations. At h=1h=1 for j>1j>1, zj≥1z_j\ge1, so a=ja=j. Use (3.1) at the cut j−1∣jj-1\mid j:

Drj=Dr,j−1mjj+∑b=rj−1Dr,b−1Kb,j.D_{rj}=D_{r,j-1}m_{jj}+ \sum_{b=r}^{j-1}D_{r,b-1}K_{b,j}.

The first term has order at least νr,j−1I+1=νrj(1)\nu^I_{r,j-1}+1=\nu_{rj}(1). In a crossing term, successively use νr,bI≤νr,b−1I+db\nu^I_{r,b}\le\nu^I_{r,b-1}+d_b; the remaining last cost is dj−1=ij−1+zj≥ij−1+1d_{j-1}=i_{j-1}+z_j\ge i_{j-1}+1. Hence every crossing term has the same lower bound. This proves the inner base. For h≥2h\ge2, inner induction and (3.7)--(3.8) give

ord⁡Daj≥Ta(j,h)−1.\operatorname {ord}D_{aj}\ge T_a(j,h)-1.

Equation (2.2) raises this order to Ta(j,h)T_a(j,h). Intervals starting to the right of aa require no increase by (3.9). If r<ar<a, apply (3.1). Its noncrossing term has order at least the right side of (3.10). A crossing term has order at least

Xb,c=νr,b−1I+∑u=bc−1du+νc+1,j(h−1).(3.11)X_{b,c}=\nu^I_{r,b-1}+\sum_{u=b}^{c-1}d_u+\nu_{c+1,j}(h-1). \tag{3.11}

Here and below the ν\nu-value of an empty interval is zero.

The elementary choices in (3.5) give

νr,bI≤νr,b−1I+ib≤νr,b−1I+db\nu^I_{r,b}\le\nu^I_{r,b-1}+i_b\le\nu^I_{r,b-1}+d_b

and

νc,j(h−1)≤zc+νc+1,j(h−1)≤dc−1+νc+1,j(h−1).\nu_{c,j}(h-1)\le z_c+\nu_{c+1,j}(h-1) \le d_{c-1}+\nu_{c+1,j}(h-1).

Absorbing the outer summands in (3.11) with these inequalities reduces its minimum to b=a−1,c=ab=a-1,c=a. Using (3.9),

Xb,c≥νr,a−2I+da−1+Wa+1(j)=νr,a−2I+ia−1+Wa(j)≥νr,a−1I+Ta(j,h)=νrj(h).(3.12)\begin{aligned} X_{b,c} &\ge \nu^I_{r,a-2}+d_{a-1}+W_{a+1}(j)\\ &=\nu^I_{r,a-2}+i_{a-1}+W_a(j)\\ &\ge\nu^I_{r,a-1}+T_a(j,h) =\nu_{rj}(h). \end{aligned} \tag{3.12}

Set Wj+1(j)=0W_{j+1}(j)=0, and give every empty interval determinant and its ν\nu-value order zero. If a=1a=1, there is no propagation: (2.2) itself is the required full-prefix coefficient. This proves the induction. Taking h=ijh=i_j proves (3.3). □\square

In particular,

CI(M)=0⟹ord⁡Δj≥sj:=∑u=1jiu,Δj=D1j.(3.13)C_I(M)=0\quad\Longrightarrow\quad \operatorname {ord}\Delta_j\ge s_j:=\sum_{u=1}^{j}i_u, \qquad \Delta_j=D_{1j}. \tag{3.13}

Lemma 3.2 (Fitting consequence)

If (3.13) holds, then dim⁡kker⁡B≥∣I∣\dim_{\mathsf k}\ker B\ge |I|.

Proof

First, if AA is any set of pp rows, then

ord⁡det⁡MA,[1,p]≥sp.(3.14)\operatorname {ord}\det M_{A,[1,p]}\ge s_p. \tag{3.14}

If A=[1,p]A=[1,p], this is exactly (3.13). Otherwise p<ℓp<\ell. Group the determinant terms by the last break vv for which the first vv columns are matched to the first vv rows. The part before the break is Δv\Delta_v. The remaining matching has no later internal break, and the nonprefix row set contains a row bigger than pp. It therefore crosses every cut (v+1)∣(v+2),…,p∣(p+1)(v+1)\mid(v+2),\ldots,p\mid(p+1) downward and costs at least ∑r=v+1pdr≥∑r=v+1pir\sum_{r=v+1}^{p}d_r\ge\sum_{r=v+1}^{p}i_r. This proves (3.14). If ∣A∣=∣E∣|A|=|E| and EE contains [1,p][1,p], Laplace expansion in those columns similarly gives

ord⁡det⁡MA,E≥sp.(3.15)\operatorname {ord}\det M_{A,E}\ge s_p. \tag{3.15}

In row convention, coker⁡B\operatorname {coker}B is presented over OO by the rows of

[MD],D=diag⁡(tq1,…,tqℓ).(3.16)\begin{bmatrix}M\\D\end{bmatrix}, \qquad D=\operatorname {diag}(t^{q_1},\ldots,t^{q_\ell}). \tag{3.16}

A maximal minor of (3.16) is, up to sign,

t∑r∈Cqrdet⁡MA,E,E=[1,ℓ]∖C.(3.17)t^{\sum_{r\in C}q_r}\det M_{A,E}, \qquad E=[1,\ell]\setminus C. \tag{3.17}

If C=∅C=\varnothing, (3.17) is Δℓ\Delta_\ell. Otherwise put p=min⁡C−1p=\min C-1. Then E⊇[1,p]E\supseteq[1,p], and (3.15), together with

∑r=p+1ℓir≤∑r=p+1ℓ−1(dr−1)+qℓ≤qp+1,(3.18)\sum_{r=p+1}^{\ell}i_r \le\sum_{r=p+1}^{\ell-1}(d_r-1)+q_\ell \le q_{p+1}, \tag{3.18}

shows that (3.17) is divisible by t∣I∣t^{|I|}. The valuation of the zeroth Fitting ideal of a finite-length OO-module is its length. Hence length⁡Ocoker⁡B≥∣I∣\operatorname {length}_O\operatorname {coker}B\ge|I|, which equals dim⁡kker⁡B\dim_{\mathsf k}\ker B. □\square

4. Gaussian chambers and separation

For a box index II, put eb=qb−ibe_b=q_b-i_b. Start with the following Gaussian parameters. The matrix LL is lower unitriangular, UU is upper triangular, and

ord⁡Uaa=ia(ia<qa),Uℓℓ=0(iℓ=qℓ),ord⁡Lab≥qb−qa−ib(a>b).(4.1)\operatorname {ord}U_{aa}=i_a\quad(i_a<q_a),\qquad U_{\ell\ell}=0\quad(i_\ell=q_\ell),\qquad \operatorname {ord}L_{ab}\ge q_b-q_a-i_b\quad(a>b). \tag{4.1}

More explicitly, Uab∈O/(tqb)U_{ab}\in O/(t^{q_b}) for a<ba<b, Ubb∈tibO/(tqb)U_{bb}\in t^{i_b}O/(t^{q_b}) with nonzero leading coefficient, and Lab∈teb−qaO/(teb)L_{ab}\in t^{e_b-q_a}O/(t^{e_b}) for a>ba>b. In the terminal possibility iℓ=qℓi_\ell=q_\ell, set Uℓℓ=0U_{\ell\ell}=0; the condition on a nonzero leading coefficient is imposed only when ib<qbi_b<q_b.

Form the ordinary power-series matrix M^=LU\widehat M=LU, and let MM be its canonical multiplier matrix: reduce column bb modulo tqbt^{q_b}. Let KI\mathcal K_I be the image of this parameter space. Before and after reduction the product is tiled. Indeed, in a lower entry (a,b)(a,b), the term through bb has order at least qb−qaq_b-q_a, while a term through c<bc<b has the additional positive amount qc−qb−icq_c-q_b-i_c; diagonal cross terms have positive order. Thus KI⊆NJQ\mathcal K_I\subseteq\mathcal N_{J_Q}.

The truncated parameter map is injective. This follows directly from Doolittle recursion. Assuming the preceding rows of UU and columns of LL have been recovered, row bb recovers every UbcU_{bc}, c≥bc\ge b, from

Mbc−∑s<bLbsUsc(modtqc).M_{bc}-\sum_{s<b}L_{bs}U_{sc}\pmod {t^{q_c}}.

These products are independent of the representatives already recovered: for s<cs<c, an ambiguity divisible by test^{e_s} vanishes modulo tqct^{q_c}, since es≥qs+1+1>qce_s\ge q_{s+1}+1>q_c. Then column bb recovers every LabL_{ab}, a>ba>b, from

Mab−∑s<bLasUsb=LabUbb(modtqb).M_{ab}-\sum_{s<b}L_{as}U_{sb} =L_{ab}U_{bb}\pmod {t^{q_b}}.

Multiplication by Ubb=tibU_{bb}=t^{i_b} times a unit is injective on the displayed quotient teb−qaO/(teb)t^{e_b-q_a}O/(t^{e_b}). If the last pivot is zero, it is prescribed and there are no parameters below it; the final residual entry is forced. Thus the recursion also covers the terminal case. The lower parameters contribute qaq_a coefficients for every a>ba>b, the strictly upper parameters contribute qbq_b coefficients for every a<ba<b, and the diagonal parameters contribute qb−ibq_b-i_b. The ambient multiplier space has the same off-diagonal counts and qb−1q_b-1 diagonal coefficients. Multiplication is injective by the recursion above. Hence

KI is irreducible,dim⁡KI=dim⁡NJQ−m.(4.2)\mathcal K_I\text{ is irreducible},\qquad \dim\mathcal K_I=\dim\mathcal N_{J_Q}-m. \tag{4.2}

We next account explicitly for the column truncations. Put DQ=diag⁡(tq1,…,tqℓ)D_Q=\operatorname {diag}(t^{q_1},\ldots,t^{q_\ell}). There is a power-series matrix HH such that

M^=M+HDQ.(4.3a)\widehat M=M+HD_Q. \tag{4.3a}

We first need a shifted flag estimate for the unreduced product. If r≤pr\le p and A⊆{r,…,ℓ}A\subseteq\{r,\ldots,\ell\} has ∣A∣=p−r+1|A|=p-r+1, then

ord⁡det⁡M^A,[r,p]≥νr,pI.(4.3b)\operatorname {ord}\det\widehat M_{A,[r,p]} \ge\nu^I_{r,p}. \tag{4.3b}

Indeed, apply ordinary Cauchy--Binet to LULU. A middle set SS is contained in [1,p][1,p]. Let uu be its largest omitted element of [r,p][r,p], with u=r−1u=r-1 when none is omitted. Upper triangularity forces the pivots u+1,…,pu+1,\ldots,p, at cost iu+1+⋯+ipi_{u+1}+\cdots+i_p. For r≤x≤ur\le x\le u,

#(S∩[1,x−1])=(x−r)+#(([r,p]∖S)∩[x,p])>x−r≥#(A∩[1,x−1]).\#(S\cap[1,x-1]) =(x-r)+\#\bigl(([r,p]\setminus S)\cap[x,p]\bigr) >x-r\ge\#(A\cap[1,x-1]).

Thus every nonzero matching in the lower minor crosses downward each cut r−1∣r,…,u−1∣ur-1\mid r,\ldots,u-1\mid u. Moreover, for a>sa>s,

ord⁡Las≥qs−is−qa≥∑x=s+1azx.\operatorname {ord}L_{as}\ge q_s-i_s-q_a \ge\sum_{x=s+1}^{a}z_x.

The lower cost is therefore at least zr+⋯+zuz_r+\cdots+z_u. Together with the forced pivots this is the uu-alternative in (3.5). When r=1r=1, necessarily S=[1,p]S=[1,p], and its principal upper pivots instead give ν1pI=∑x=1pix\nu^I_{1p}=\sum_{x=1}^p i_x directly. This proves (4.3b).

Expand a canonical interval determinant multilinearly using (4.3a). In a term using a nonempty set C⊆[r,j]C\subseteq[r,j] of remainder columns, let c=min⁡Cc=\min C. It contains the factor t∑b∈Cqbt^{\sum_{b\in C}q_b}. Laplace expansion first in the HH-columns and then in the untouched prefix [r,c−1][r,c-1], followed by (4.3b), gives order at least qc+νr,c−1Iq_c+\nu^I_{r,c-1}. Here an empty prefix has order zero. The definitions (3.4)--(3.5) and the box bounds give

νrjI≤νr,c−1I+∑u=cjiu,∑u=cjiu≤qc.(4.3c)\nu^I_{rj}\le\nu^I_{r,c-1}+\sum_{u=c}^ji_u,\qquad \sum_{u=c}^ji_u\le q_c. \tag{4.3c}

The last inequality is strict when j<ℓj<\ell, by ∑u=cjiu≤∑u=cj(du−1)<qc\sum_{u=c}^j i_u\le\sum_{u=c}^j(d_u-1)<q_c. When j=ℓj=\ell but iℓ<qℓi_\ell<q_\ell, it follows instead from

∑u=cℓiu≤qc−qℓ−(ℓ−c)+iℓ<qc.\sum_{u=c}^{\ell}i_u \le q_c-q_\ell-(\ell-c)+i_\ell<q_c.

Thus every remainder term has order at least νrjI\nu^I_{rj}, and the term with no remainder columns has the same bound by (4.3b). For the canonical multiplier matrix we have proved

ord⁡Drj≥νrjI.(4.3)\operatorname {ord}D_{rj}\ge\nu^I_{rj}. \tag{4.3}

The endpoint rule (2.1) says precisely that the right side is at least the target in (2.2), so KI⊆YI\mathcal K_I\subseteq Y_I.

At the generic point of KI\mathcal K_I, equality holds in (4.3) whenever j<ℓj<\ell or ij<qji_j<q_j; this is the only form needed below. In these cases the second inequality in (4.3c) is strict, so every nonempty remainder term has order strictly greater than νrjI\nu^I_{rj}. For the raw product, the case r=1r=1 is witnessed by the principal middle set and the monomial ∏u=1jUuu\prod_{u=1}^jU_{uu}. For r≥2r\ge2, besides the principal Cauchy--Binet term, each alternative indexed by p=r,…,jp=r,\ldots,j in (3.5) is witnessed by the middle set

{r−1,r,…,p−1,p+1,…,j}.\{r-1,r,\ldots,p-1,p+1,\ldots,j\}.

Match the lower rows u=r,…,pu=r,\ldots,p to u−1u-1, then the upper rows u−1u-1 to columns uu; match the remaining rows diagonally. Its order is ∑u=rpzu+∑u=p+1jiu\sum_{u=r}^{p}z_u+\sum_{u=p+1}^{j}i_u, and the product of its independent leading Gaussian coefficients is a unique monomial with coefficient ±1\pm1. Thus it cannot cancel in any characteristic.

There is also a direct kernel calculation which does not treat LL as an endomorphism of VQV_Q. For x∈VQx\in V_Q, define the surjection

Φ:VQ⟶⨁bO/(teb),Φ(x)=((xL)b mod teb)b.\Phi:V_Q\longrightarrow\bigoplus_b O/(t^{e_b}), \qquad \Phi(x)=((xL)_b\bmod t^{e_b})_b.

Condition (4.1) makes this well-defined, and triangular back-substitution makes it surjective. Since M^−M=HDQ\widehat M-M=HD_Q, the two matrices induce the same endomorphism of VQV_Q. If y=xLy=xL, solve the equations yU=0yU=0 in increasing output column. Once ya∈teay_a\in t^{e_a} for a<ba<b, its contribution to column bb vanishes because

ea=qa−ia≥qa+1+1>qb.e_a=q_a-i_a\ge q_{a+1}+1>q_b.

The bb-th equation is therefore equivalent to yb∈teby_b\in t^{e_b}. Consequently xM=0xM=0 if and only if Φ(x)=0\Phi(x)=0, and hence

dim⁡ker⁡B=dim⁡ker⁡Φ=∑b(qb−eb)=∑bib=∣I∣.(4.4)\dim\ker B=\dim\ker\Phi =\sum_b(q_b-e_b)=\sum_b i_b=|I|. \tag{4.4}

We will need the following separation fact.

Lemma 4.1 (chamber separation)

If ∣I∣=∣J∣|I|=|J| and all equations in CIC_I vanish identically on KJ\mathcal K_J, then I=JI=J.

Proof

We first prove Jj≥IjJ_j\ge I_j by induction on jj. If J1<I1J_1<I_1, the generic order of m11m_{11} on KJ\mathcal K_J is J1J_1, contradicting Lemma 3.1 and (3.4); hence the case j=1j=1 holds. Suppose it is known before jj, but Jj=Ij−δJ_j=I_j-\delta with δ>0\delta>0. In particular Jj<qjJ_j<q_j, so the generic-order equality is valid for every interval ending at this jj. Lemma 3.1, applied because CIC_I vanishes on KJ\mathcal K_J, therefore gives

νrjJ≥νrjI(1≤r≤j).(4.5)\nu^J_{rj}\ge\nu^I_{rj}\qquad(1\le r\le j). \tag{4.5}

For r≥2r\ge2, (3.5) has the recursion

νrjX=min⁡{ArjX, zrX+νr+1,jX},ArjX=∑u=rjXu,zrX=dr−1−Xr−1.(4.6)\nu^X_{rj}=\min\left\{A^X_{rj},\ z_r^X+\nu^X_{r+1,j}\right\}, \qquad A^X_{rj}=\sum_{u=r}^{j}X_u,\quad z_r^X=d_{r-1}-X_{r-1}. \tag{4.6}

Use the elementary fact that, if A′<AA'<A, Z′≤ZZ'\le Z, and min⁡(A′,Z′)≥min⁡(A,Z)\min(A',Z')\ge\min(A,Z), then Z′=Z=min⁡(A,Z)Z'=Z=\min(A,Z). At r=jr=j, outer induction gives zjJ≤zjIz_j^J\le z_j^I, while AjjJ=AjjI−δA^J_{jj}=A^I_{jj}-\delta. Equations (4.5)--(4.6) therefore force zjJ=zjIz_j^J=z_j^I, hence Jj−1=Ij−1J_{j-1}=I_{j-1}, and also νjjJ=νjjI\nu^J_{jj}=\nu^I_{jj}. Descending in rr, the same argument successively forces Jr−1=Ir−1J_{r-1}=I_{r-1} and νrjJ=νrjI\nu^J_{rj}=\nu^I_{rj}. At r=1r=1, however,

ν1jJ=∑u≤jJu=∑u≤jIu−δ<ν1jI,\nu^J_{1j}=\sum_{u\le j}J_u =\sum_{u\le j}I_u-\delta<\nu^I_{1j},

contradicting (4.5). Thus J≥IJ\ge I coordinatewise. Equal total sums give J=IJ=I. □\square

5. Incidence geometry

We record the dimension and irreducibility facts used below. Work first over an algebraic closure. For R=(dmd)dR=(d^{m_d})_d, let AR=CMn(JR)A_R=C_{M_n}(J_R). There is a surjection

AR⟶∏dMmdA_R\longrightarrow\prod_dM_{m_d}

with kernel rad⁡AR\operatorname {rad}A_R, and an element of ARA_R is nilpotent exactly when every component of its semisimple image is nilpotent. Thus NJR\mathcal N_{J_R} is the inverse image of a product of ordinary nilpotent cones. Consequently

NJR is geometrically irreducible,dim⁡NJR=dim⁡AR−ℓ(R).(5.1)\mathcal N_{J_R}\text{ is geometrically irreducible},\qquad \dim\mathcal N_{J_R}=\dim A_R-\ell(R). \tag{5.1}

If D(P)=Q\mathfrak D(P)=Q, the commuting-pair incidence variety

CP,Q={(B,A)∈OP×OQ:AB=BA}≅GLn×GPWQP\mathcal C_{P,Q} =\{(B,A)\in\mathcal O_P\times\mathcal O_Q:AB=BA\} \cong GL_n\times^{G_P}W_Q^P

is irreducible, because WQPW_Q^P is the dense open type locus in the irreducible variety NJP\mathcal N_{J_P}. By (5.1),

dim⁡CP,Q=n2−ℓ(P).\dim\mathcal C_{P,Q}=n^2-\ell(P).

Projection to OQ\mathcal O_Q gives

dim⁡WPQ=dim⁡AQ−ℓ(P),codim⁡NJQWPQ=ℓ(P)−ℓ.(5.2)\dim W_P^Q=\dim A_Q-\ell(P),\qquad \operatorname {codim}_{\mathcal N_{J_Q}}W_P^Q=\ell(P)-\ell. \tag{5.2}

Also CP,Q=GLn×GQWPQ\mathcal C_{P,Q}=GL_n\times^{G_Q}W_P^Q. The group GQ=AQ×G_Q=A_Q^\times is connected: it is an extension of ∏dGLmd\prod_dGL_{m_d} by 1+rad⁡AQ1+\operatorname {rad}A_Q. It therefore fixes each irreducible component of the fiber; more than one such component would make the associated bundle reducible. Hence WPQW_P^Q and its closure are geometrically irreducible.

For an arbitrary RR with WRQ≠∅W_R^Q\ne\varnothing, the same incidence calculation gives

codim⁡NJQWRQ≥ℓ(R)−ℓ,(5.3)\operatorname {codim}_{\mathcal N_{J_Q}}W_R^Q \ge\ell(R)-\ell, \tag{5.3}

and the inequality is strict if D(R)≠Q\mathfrak D(R)\ne Q: in that case the type-QQ locus is not dense in the irreducible NJR\mathcal N_{J_R}.

6. Identification of the equation locus

For every box index II, let RIR_I be the generic Jordan type on KI\mathcal K_I. From (4.4), ℓ(RI)=∣I∣\ell(R_I)=|I|. The generic-type open subset of KI\mathcal K_I lies in WRIQW_{R_I}^Q, so (4.2) gives codim⁡WRIQ≤m\operatorname {codim}W_{R_I}^Q\le m. On the other hand (5.3) gives codim⁡WRIQ≥ℓ(RI)−ℓ=m\operatorname {codim}W_{R_I}^Q\ge\ell(R_I)-\ell=m. Equality holds, and the strict clause of (5.3) gives

D(RI)=Q,KI‾=WRIQ‾.(6.1)\mathfrak D(R_I)=Q,\qquad \overline{\mathcal K_I}=\overline{W_{R_I}^Q}. \tag{6.1}

Indeed, both irreducible varieties in (6.1) have codimension mm.

The assignment ρ:I↦RI\rho:I\mapsto R_I maps the finite Box index set into D−1(Q)\mathfrak D^{-1}(Q). It is injective. Indeed, if RI=RJR_I=R_J, then ∣I∣=ℓ(RI)=ℓ(RJ)=∣J∣|I|=\ell(R_I)=\ell(R_J)=|J|, and (6.1) gives KI‾=KJ‾\overline{\mathcal K_I}=\overline{\mathcal K_J}. Since CIC_I vanishes on KI\mathcal K_I, it therefore vanishes on KJ\mathcal K_J, and Lemma 4.1 gives I=JI=J. By the Box Theorem, the domain and codomain of ρ\rho have the same finite cardinality. Thus ρ\rho is a bijection. In particular, every partition PP with D(P)=Q\mathfrak D(P)=Q is RIR_I for a unique II, and

KI‾=WRIQ‾⊆YI.(6.2)\overline{\mathcal K_I}=\overline{W_{R_I}^Q}\subseteq Y_I. \tag{6.2}

Now let ZZ be any irreducible component of YIY_I, and let RZR_Z be its generic Jordan type. Since CIC_I has mm generators, Krull's height theorem gives codim⁡Z≤m\operatorname {codim}Z\le m. The generic-type open part of ZZ lies in WRZQW_{R_Z}^Q. Lemmas 3.1--3.2 give ℓ(RZ)≥∣I∣\ell(R_Z)\ge|I|, while (5.3) gives

codim⁡Z≥codim⁡WRZQ≥ℓ(RZ)−ℓ≥∣I∣−ℓ=m.(6.3)\operatorname {codim}Z \ge\operatorname {codim}W_{R_Z}^Q \ge\ell(R_Z)-\ell \ge|I|-\ell=m. \tag{6.3}

Every inequality is equality. Thus D(RZ)=Q\mathfrak D(R_Z)=Q and ℓ(RZ)=∣I∣\ell(R_Z)=|I|. By the bijection ρ\rho, write RZ=RJR_Z=R_J; then ∣J∣=ℓ(RJ)=∣I∣|J|=\ell(R_J)=|I|. By (6.1), the irreducible closure WRJQ‾\overline{W_{R_J}^Q} is KJ‾\overline{\mathcal K_J}. It has the same dimension as ZZ, hence equals ZZ. Therefore every polynomial in CIC_I vanishes on KJ\mathcal K_J. Lemma 4.1 gives J=IJ=I. Thus YIY_I has a unique irreducible component and

(YI)red=WRIQ‾.(6.4)(Y_I)_{\mathrm{red}}=\overline{W_{R_I}^Q}. \tag{6.4}

It remains only to check the scheme structure. Let M0M_0 be the diagonal point with maa=tiam_{aa}=t^{i_a}, using zero if a=ℓ,iℓ=qℓa=\ell,i_\ell=q_\ell. It belongs to YIY_I, because every coefficient selected in (2.2) is strictly below the order of the corresponding diagonal product. Order the equations by increasing (j,h)(j,h), and use the distinct ambient coordinates yj,h=[th−1]mjjy_{j,h}=[t^{h-1}]m_{jj}. If a=a(j,h)a=a(j,h) is the endpoint in (2.2), multilinearity gives

∂fj,h∂yj,h(M0)=[t∑r=aj−1ir]Da,j−1(M0)=1.(6.5)\frac{\partial f_{j,h}}{\partial y_{j,h}}(M_0) =[t^{\sum_{r=a}^{j-1}i_r}]D_{a,j-1}(M_0)=1. \tag{6.5}

An equation at an earlier vertex does not involve mjjm_{jj}. At the same vertex, if h′<hh'<h, differentiating fj,h′f_{j,h'} with respect to yj,hy_{j,h} selects a coefficient of the corresponding Da′,j−1(M0)D_{a',j-1}(M_0) strictly below its diagonal order, and hence gives zero. Thus this m×mm\times m Jacobian minor is triangular with diagonal one. The scheme YIY_I is smooth of codimension mm at M0M_0.

The ideal CIC_I has mm generators and height mm, so it is a complete intersection in the polynomial coordinate ring of NJQ\mathcal N_{J_Q}. The quotient is Cohen--Macaulay and has no embedded associated primes. By (6.4) there is only one minimal prime. Equation (6.5) gives a nonempty smooth open subset of its irreducible support, so that open contains the generic point and the generic localization is reduced. A Cohen--Macaulay ring is S1S_1; together with generic reducedness this implies reducedness. Thus CIC_I is prime and is the defining ideal of WRIQ‾\overline{W_{R_I}^Q}.

Given the original PP, choose the unique II with P=RIP=R_I. By (2.3), the codimension is ∣I∣−ℓ=ℓ(P)−ℓ|I|-\ell=\ell(P)-\ell, and every generator has degree at most ℓ\ell. This proves the theorem.

7. Ground field and references used

All equations and determinant identities above are integral, and all unique leading monomials have coefficient ±1\pm1. The proof over an algebraic closure therefore gives geometric primeness and geometric irreducibility in every characteristic. Faithfully flat descent gives the assertion over the original infinite field k\mathsf k.

The statement is Conjecture 4.2 of M. Boij, A. Iarrobino, and L. Khatami, Jordan type stratification of spaces of commuting nilpotent matrices, Linear Algebra Appl. 710 (2025), 183--202 (https://arxiv.org/abs/2409.13553). The Box Theorem used above is in J. Irving, T. Kosir, and M. Mastnak, A Proof of the Box Conjecture for Commuting Pairs of Matrices (https://arxiv.org/abs/2403.18574).