Functional equation conjecture for well-aligned pairs

From papers

Let WAn\operatorname{WA}_{n} denote the set of well-aligned pairs for a nonnegative integer nn, and let W(x)\mathcal{W}(x) be its exponential generating function:

W(x)=n0WAnxnn!=1+1x11!+3x22!+17x33!+147x44!+1729x55!+25827x66!+468593x77!+.\mathcal{W}(x)=\sum_{n\geq 0}|\operatorname{WA}_{n}|\frac{x^{n}}{n!}=1+1\frac{x^1}{1!}+3\frac{x^2}{2!}+17\frac{x^3}{3!}+147\frac{x^4}{4!}+1729\frac{x^5}{5!}+25827\frac{x^6}{6!}+468593\frac{x^7}{7!}+\cdots.

Functional equation conjecture. The exponential generating function satisfies

W(x)=W(x)22W(x).\mathcal{W}'(x)=\frac{\mathcal{W}(x)^2}{2-\mathcal{W}(x)}.

This conjecture predicts a recursive description of the numbers of well-aligned pairs and provides quantitative information about the family of pairs used to compute Schubert structure coefficients. The source offers it as a numerological observation, and no resolution is given.

Progress summary

Open

The proposed counting rule has only been checked numerically, and no proof or counterexample has been found.

The conjecture asserts that the exponential generating function for well-aligned pairs satisfies W(x)=W(x)22W(x)\mathcal{W}'(x)=\frac{\mathcal{W}(x)^2}{2-\mathcal{W}(x)}. The available source presents this as a numerological observation rather than a proved theorem.

Current status (as of August 2026): The functional equation remains an open conjecture; its initial coefficients are consistent with it, but no verified proof or counterexample is recorded.

Sources
Sources & referencesView supporting material

Primary source

Hunter Spink and Vasu Tewari, “Richardson tableaux and Schubert positivity”, arXiv:2510.12391 (2026).

Additional references

3 papers in this index state this conjecture (2010–2025). The statement above is taken from the most recent of them; the others are arXiv:2005.04829, arXiv:1002.0554.

Solutions 1

Proof

A complete proof of the functional equation for well-aligned pairs

Problem. MathDB #382424, “Functional equation conjecture for well-aligned pairs.”

Primary source. Hunter Spink and Vasu Tewari, Richardson tableaux and Schubert positivity, arXiv:2510.12391v2, revised July 29, 2026, Definition 2.1 and Conjecture 6.1. The source verifies the proposed identity through permutation size seven. OEIS A234289 specifies the conjectured sequence and its differential equation but does not identify or enumerate well-aligned pairs.

Theorem

Let Wn\mathcal W_n denote the set of well-aligned ordered pairs of permutations in SnS_n, including the unique empty pair in W0\mathcal W_0. Then the exponential generating function

W(t)=n0Wntnn!W(t)=\sum_{n\geq 0}|\mathcal W_n|\frac{t^n}{n!}

satisfies the exact formal differential equation

W(t)=W(t)22W(t),W(0)=1.\boxed{\displaystyle W'(t)=\frac{W(t)^2}{2-W(t)},\qquad W(0)=1.}

Consequently, the conjecture holds in every permutation size. More strongly, the complete ascent-run refinement of the enumeration satisfies an explicitly solvable formal transport equation.

1. The source definition and insertion of the minimum

For a permutation vSnv\in S_n, write δ(v)Sn1\delta(v)\in S_{n-1} for the permutation obtained by deleting its entry 11 and decreasing all remaining entries by one. The source calls (v,w)(v,w) aligned when, writing

i=v1(1),j=w1(1),i=v^{-1}(1),\qquad j=w^{-1}(1),

one has

ijandv(i)<v(i+1)<<v(j).(1)i\leq j \quad\text{and}\quad v(i)<v(i+1)<\cdots<v(j). \tag{1}

The pair is well-aligned if it is aligned and (δ(v),δ(w))(\delta(v),\delta(w)) is well-aligned. The empty pair is the initial object.

Fix an existing pair (v,w)Wn(v,w)\in\mathcal W_n. Increase every entry of both permutations by one. To construct an element of Wn+1\mathcal W_{n+1}, insert the new entry 11 independently into the two resulting words. Every well-aligned extension arises uniquely in this manner: deleting the new minimum recovers the old pair, and the only additional condition is (1).

Decompose vv into its maximal consecutive increasing runs. Suppose one such run has length 1\ell\geq 1, and insert the new minimum immediately before its (p+1)(p+1)-st entry, where

0p1.0\leq p\leq \ell-1.

The insertion splits this run into a prefix of length pp, omitted when p=0p=0, and an increasing run of length

q=p+12(2)q=\ell-p+1\geq 2 \tag{2}

beginning with the new minimum. If the minimum is in position ii of the new first permutation, the permitted positions jj in the second permutation are precisely

j=i,i+1,,i+q1.(3)j=i,i+1,\ldots,i+q-1. \tag{3}

Indeed, these and only these positions satisfy (1), because the increasing run beginning at position ii has exactly qq entries. Crucially, the number qq of permitted insertion positions is independent of ww.

Every insertion gap except the final gap is uniquely the gap immediately before an entry in some increasing run. The remaining final gap appends the minimum to vv; in this case condition (1) forces it to be appended to ww as well. This creates one new singleton run and gives exactly one extension.

2. The ascent-run derivation

Introduce commuting variables u1,u2,u_1,u_2,\ldots, put u0=1u_0=1, and assign weight deguj=j\deg u_j=j. For a permutation vv whose increasing runs have lengths 1,,r\ell_1,\ldots,\ell_r, let

run(v)=a=1rua.\operatorname{run}(v)=\prod_{a=1}^{r}u_{\ell_a}.

Define the weighted counting polynomial

Fn(u)=(v,w)Wnrun(v),F0=1.(4)F_n(\boldsymbol u) =\sum_{(v,w)\in\mathcal W_n}\operatorname{run}(v), \qquad F_0=1. \tag{4}

On the polynomial ring Q[u1,u2,]\mathbb Q[u_1,u_2,\ldots], define the derivation DD by D(u0)=0D(u_0)=0, the Leibniz rule, and

D(u)=p=01(p+1)upup+1=p0, q2\p+q=+1qupuq.(5)D(u_\ell) =\sum_{p=0}^{\ell-1}(\ell-p+1)u_pu_{\ell-p+1} =\sum_{\substack{p\geq 0,\ q\geq 2\p+q=\ell+1}} q\,u_pu_q. \tag{5}

The term indexed by (p,q)(p,q) replaces an increasing run of length \ell by the runs of lengths pp and qq described in (2), and its coefficient qq is exactly the number of second-permutation insertion positions in (3). The Leibniz rule selects which existing run is changed. The final-gap insertion contributes multiplication by u1u_1. Therefore the preceding insertion bijection proves, with no omission or overcount,

Fn+1=(D+u1)Fn.(6)F_{n+1}=(D+u_1)F_n. \tag{6}

In particular, for the refined exponential generating function

F(t;u)=n0Fn(u)tnn!,F(t;\boldsymbol u) =\sum_{n\geq0}F_n(\boldsymbol u)\frac{t^n}{n!},

we obtain

Ft=DF+u1F,F(0;u)=1.(7)\frac{\partial F}{\partial t}=DF+u_1F, \qquad F(0;\boldsymbol u)=1. \tag{7}

Every polynomial FnF_n is homogeneous of weight nn; hence all formal operations below are well-defined coefficientwise in the weight-completed polynomial ring.

3. Integrating the derivation

Let

a(t)=etDu1,J(t)=0ta(s)ds.a(t)=e^{tD}u_1, \qquad J(t)=\int_0^t a(s)\,ds.

Because DD commutes with its exponential,

DJ(t)=0tDesDu1ds=0ts(esDu1)ds=a(t)u1.(8)DJ(t) =\int_0^t D e^{sD}u_1\,ds =\int_0^t\frac{\partial}{\partial s} \bigl(e^{sD}u_1\bigr)\,ds =a(t)-u_1. \tag{8}

Consequently eJ(t)e^{J(t)} satisfies (7):

teJ(t)=a(t)eJ(t),DeJ(t)+u1eJ(t)=(DJ(t)+u1)eJ(t)=a(t)eJ(t).\begin{aligned} \frac{\partial}{\partial t}e^{J(t)} &=a(t)e^{J(t)},\\ De^{J(t)}+u_1e^{J(t)} &=\bigl(DJ(t)+u_1\bigr)e^{J(t)} =a(t)e^{J(t)}. \end{aligned}

The formal initial-value problem (7) has a unique solution, so

F(t;u)=exp(0tesDu1ds).(9)F(t;\boldsymbol u) =\exp\left(\int_0^t e^{sD}u_1\,ds\right). \tag{9}

To determine the integrand, introduce the auxiliary series

X(t,z)=0(etDu)z.(10)X(t,z)=\sum_{\ell\geq0}\bigl(e^{tD}u_\ell\bigr)z^\ell. \tag{10}

Equation (5) gives the exact generating-series identity

D(0uz)=p0q2qupuqzp+q1=(p0upzp)(q2quqzq1).\begin{aligned} D\left(\sum_{\ell\geq0}u_\ell z^\ell\right) &=\sum_{p\geq0}\sum_{q\geq2} q\,u_pu_qz^{p+q-1}\\ &=\left(\sum_{p\geq0}u_pz^p\right) \left(\sum_{q\geq2}q\,u_qz^{q-1}\right). \end{aligned}

Since the exponential of a derivation preserves products,

Xt=X(Xza(t)),a(t)=[z]X(t,z).(11)\boxed{\displaystyle \frac{\partial X}{\partial t} =X\left(\frac{\partial X}{\partial z}-a(t)\right), \qquad a(t)=[z]X(t,z). } \tag{11}

The constant term of XX is always etDu0=1e^{tD}u_0=1.

4. Specialization and the formal Burgers equation

Now specialize every run variable to one. Write X(t,z)X(t,z) and a(t)a(t) again for their specialized series, and set

W(t)=F(t;1,1,).W(t)=F(t;1,1,\ldots).

By (9),

W(t)=a(t)W(t),W(0)=1.(12)W'(t)=a(t)W(t), \qquad W(0)=1. \tag{12}

Since u=1u_\ell=1 for every 0\ell\geq0, equation (10) has initial data

X(0,z)=0z=11z.(13)X(0,z)=\sum_{\ell\geq0}z^\ell=\frac{1}{1-z}. \tag{13}

Introduce

Y(t,z)=W(t)X(t,z),τ(t)=0tdsW(s).(14)Y(t,z)=W(t)X(t,z), \qquad \tau(t)=\int_0^t\frac{ds}{W(s)}. \tag{14}

Equations (11) and (12) imply

Yt=WX+WXt=aWX+WX(Xza)=YWYz.(15)\begin{aligned} \frac{\partial Y}{\partial t} &=W'X+W\frac{\partial X}{\partial t}\\ &=aWX+WX\left(\frac{\partial X}{\partial z}-a\right)\\ &=\frac{Y}{W}\frac{\partial Y}{\partial z}. \end{aligned} \tag{15}

Because τ(0)=1\tau'(0)=1, the series τ(t)\tau(t) has a compositional inverse. Regarding YY as a function of (τ,z)(\tau,z), (15) becomes the formal inviscid Burgers equation

Yτ=YYz,Y(0,z)=11z.(16)\frac{\partial Y}{\partial\tau} =Y\frac{\partial Y}{\partial z}, \qquad Y(0,z)=\frac{1}{1-z}. \tag{16}

Its unique formal solution is characterized by

Y(τ,z)=11zτY(τ,z).(17)Y(\tau,z)=\frac{1}{1-z-\tau Y(\tau,z)}. \tag{17}

Indeed, the right-hand side determines coefficients recursively in τ\tau, has the required initial condition, and implicit differentiation gives Yτ=YYzY_\tau=Y Y_z. Equivalently,

Y(τ,z)=1z(1z)24τ2τ.(18)Y(\tau,z) =\frac{1-z-\sqrt{(1-z)^2-4\tau}}{2\tau}. \tag{18}

5. Recovering the conjectured differential equation

The constant term of X(t,z)X(t,z) is one; therefore

Y(t,0)=W(t).(19)Y(t,0)=W(t). \tag{19}

Substituting z=0z=0 into (17) yields

W(t)=11τ(t)W(t),W(t)=\frac{1}{1-\tau(t)W(t)},

or equivalently

τ(t)=W(t)1W(t)2.(20)\tau(t)=\frac{W(t)-1}{W(t)^2}. \tag{20}

Differentiate (20) and use τ(t)=1/W(t)\tau'(t)=1/W(t):

1W(t)=2W(t)W(t)3W(t).\frac{1}{W(t)} =\frac{2-W(t)}{W(t)^3}W'(t).

Since W(0)=1W(0)=1, both W(t)W(t) and 2W(t)2-W(t) are formally invertible. We obtain

W(t)=W(t)22W(t).\boxed{\displaystyle W'(t)=\frac{W(t)^2}{2-W(t)}. }

This is exactly Conjecture 6.1 for all n0n\geq0.

For completeness, integration also gives the implicit closed form

t=22W(t)logW(t),(21)t=2-\frac{2}{W(t)}-\log W(t), \tag{21}

so that, writing U(t)=W(t)1U(t)=W(t)-1,

t=2U(t)1+U(t)log(1+U(t)).(22)t=\frac{2U(t)}{1+U(t)}-\log\bigl(1+U(t)\bigr). \tag{22}

The initial exact counts are

Wn=1,1,3,17,147,1729,25827,468593,10012083,246287521,6856204803,.\bigl|\mathcal W_n\bigr| =1,1,3,17,147,1729,25827,468593,10012083, 246287521,6856204803,\ldots.

The source checked only the terms through n=7n=7; the derivation above establishes the entire infinite sequence and its stronger ascent-run-refined transport equation.

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