docs(p28): post-submission lint polish (chktex W2/W24) on the audited release line

Whitespace-only polish of solution.tex: 46 chktex warnings fixed
- W2 (43x): 'word \eqref{...}' -> 'word~\eqref{...}' and continuation-line
  joins so references stay glued to their prose
- W24 (3x): \label glued to the \begin{...} line
- W8 kept (5x, all in the DOI identifier 10.1090/S0025-5718-1965-0194620-7:
  single hyphens are correct there, not prose dashes)

Verified: chktex W2+W24 = 0 (total 128, all W3/W25 brace suggestions + W8
DOI false positives); pdflatex 3-pass clean build (0 errors, 0 warnings,
0 overfull, 17 pages, 0 '??'); token-level PDF text diff vs the shipped
e85d7bf9 PDF shows only glyph-extraction/wrap artifacts (content identical,
whitespace-only tex diff).

NOTE: this is the parallel audited line (492c8ab provenance), NOT the
authority manuscript (completed-submissions 1cbb5982, hand-maintained,
must not be regenerated).
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allaun 2026-08-08 03:34:11 -05:00
parent cd4ae757d9
commit 2f4fd8d9ee
2 changed files with 37 additions and 58 deletions

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@ -323,14 +323,10 @@ The constant and generic coefficient equations are
\frac{(A(j-1)+B(j-1))\chi_{j-1}}{\psi_{j-1}}\right]=1 \frac{(A(j-1)+B(j-1))\chi_{j-1}}{\psi_{j-1}}\right]=1
\quad(j\ge1). \quad(j\ge1).
\end{equation} \end{equation}
Clearing the displayed nonzero factors turns Clearing the displayed nonzero factors turns~\eqref{eq:ore0}--\eqref{eq:tail-coefficients} into polynomial
\eqref{eq:ore0}--\eqref{eq:tail-coefficients} into polynomial
equalities with every coefficient zero. The independent script equalities with every coefficient zero. The independent script
\texttt{p28\_standalone\_equations.py} expands precisely these equalities \texttt{p28\_standalone\_equations.py} expands precisely these equalities
using only rational addition and multiplication. Equation using only rational addition and multiplication. Equation~\eqref{eq:tail-coefficients} gives the first row of~\eqref{eq:tail-contiguity}; applying~\eqref{eq:ore0}--\eqref{eq:ore3} successively gives the other three
\eqref{eq:tail-coefficients} gives the first row of
\eqref{eq:tail-contiguity}; applying
\eqref{eq:ore0}--\eqref{eq:ore3} successively gives the other three
Euler-jet rows. Euler-jet rows.
\end{proof} \end{proof}
@ -377,9 +373,8 @@ z(\theta+\tfrac16)(\theta+\tfrac12)(\theta+\tfrac56)\right]y=0.
\] \]
Substituting \(z=-x/(1-x)\), using Substituting \(z=-x/(1-x)\), using
\(\theta=(1-x)x\partial_x\), and multiplying by \(72(1-x)\) \(\theta=(1-x)x\partial_x\), and multiplying by \(72(1-x)\)
expands to \eqref{eq:transformed-ode}. expands to~\eqref{eq:transformed-ode}.
Using the displayed decomposition of \(C\), equations Using the displayed decomposition of \(C\), equations~\eqref{eq:ascension}--\eqref{eq:transformed-ode} give
\eqref{eq:ascension}--\eqref{eq:transformed-ode} give
\[ \[
Ck_0=-\frac54. Ck_0=-\frac54.
\] \]
@ -417,8 +412,7 @@ direct substitution in the authoritative matrix gives
\end{equation} \end{equation}
Thus \(J_N(0)\) has rank one. Thus \(J_N(0)\) has rank one.
The first nonconstant coefficient of the \(\F43\) in The first nonconstant coefficient of the \(\F43\) in~\eqref{eq:tail} equals
\eqref{eq:tail} equals
\[ \[
c_N=\frac{u(3u-2)(3u+2)}{144(u-1)^2}=a_N^{-1}. c_N=\frac{u(3u-2)(3u+2)}{144(u-1)^2}=a_N^{-1}.
\] \]
@ -430,8 +424,8 @@ Since \(z=-x+O(x^2)\),
+O(x) +O(x)
\right],\qquad \eta_N\ne0. \right],\qquad \eta_N\ne0.
\end{equation} \end{equation}
The leading vector in \eqref{eq:tail-direction} is precisely the image The leading vector in~\eqref{eq:tail-direction} is precisely the image
direction in \eqref{eq:rank-one}. direction in~\eqref{eq:rank-one}.
The other expansion required below is equally direct. Since The other expansion required below is equally direct. Since
\[ \[
F_{N+1}=\kappa_{N+1}z^{N+2}(1+O(z)),\qquad F_{N+1}=\kappa_{N+1}z^{N+2}(1+O(z)),\qquad
@ -443,13 +437,12 @@ k_{N+1}=x^{N+2}\widetilde\eta_N
\left(\e_1+xs_N+O(x^2)\right), \left(\e_1+xs_N+O(x^2)\right),
\qquad\widetilde\eta_N\ne0. \qquad\widetilde\eta_N\ne0.
\end{equation} \end{equation}
Moreover, \eqref{eq:rank-one} gives Moreover,~\eqref{eq:rank-one} gives
\[ \[
J_N(0)\e_1=u^3(a_N,-1,-1,-1)^T\ne0. J_N(0)\e_1=u^3(a_N,-1,-1,-1)^T\ne0.
\] \]
\begin{lemma}[DVR step, including the extra first-column zero] \begin{lemma}[DVR step, including the extra first-column zero]\label{lem:dvr}
\label{lem:dvr}
Let \(R_0=\Q[[x]]\), \(H=\diag(x,1,1,1)\), and suppose Let \(R_0=\Q[[x]]\), \(H=\diag(x,1,1,1)\), and suppose
\[ \[
E=x^NLH,\qquad L\in\operatorname{Mat}_4(R_0),\qquad Ek=0. E=x^NLH,\qquad L\in\operatorname{Mat}_4(R_0),\qquad Ek=0.
@ -514,12 +507,9 @@ Consequently the constant term in the first column of \(fC\) is
\(-5/4\), cancelling the first component of every row of \(-5/4\), cancelling the first component of every row of
\((5/4)\mathcal P\). Hence \(\mathcal E_0=L_0H\). \((5/4)\mathcal P\). Hence \(\mathcal E_0=L_0H\).
Apply Lemma~\ref{lem:dvr} inductively, using Apply Lemma~\ref{lem:dvr} inductively, using~\eqref{eq:annihilation},~\eqref{eq:rank-one},~\eqref{eq:tail-direction},~\eqref{eq:next-tail-direction}, the displayed
\eqref{eq:annihilation}, \eqref{eq:rank-one},
\eqref{eq:tail-direction}, \eqref{eq:next-tail-direction}, the displayed
nonzero first column of \(J_N(0)\), and \(M_Nk_{N+1}=k_N\). nonzero first column of \(J_N(0)\), and \(M_Nk_{N+1}=k_N\).
The stronger last-row assertion follows from The stronger last-row assertion follows from~\eqref{eq:row-relation}.
\eqref{eq:row-relation}.
\end{proof} \end{proof}
\section{The terminating denominator} \section{The terminating denominator}
@ -536,8 +526,7 @@ and define
Since \(x=-z/(1-z)\), this is also the first component of Since \(x=-z/(1-z)\), this is also the first component of
\((-z)^nCG_N\). \((-z)^nCG_N\).
\begin{proposition}[Exact terminating denominator] \begin{proposition}[Exact terminating denominator]\label{prop:terminating}
\label{prop:terminating}
For every \(N\ge0\), For every \(N\ge0\),
\begin{equation}\label{eq:qhat} \begin{equation}\label{eq:qhat}
\frac{\widehat Q_N(z)}{\alpha_n} \frac{\widehat Q_N(z)}{\alpha_n}
@ -619,8 +608,7 @@ integer \(n\) are nonzero for \(n\ge1\); no value is obtained by dividing
at \(z=0\), because the verifier cross-multiplies first and the reconstructed at \(z=0\), because the verifier cross-multiplies first and the reconstructed
base functions have removable limits there. The mandatory base functions have removable limits there. The mandatory
sparse-polynomial verifier checks every sparse-polynomial verifier checks every
reconstruction equation, the closing factorization, and reconstruction equation, the closing factorization, and~\eqref{eq:full-gauge}--\eqref{eq:matrix-scalar-bridge} by cross
\eqref{eq:full-gauge}--\eqref{eq:matrix-scalar-bridge} by cross
multiplication. For any reconstructed horizontal row these identities give multiplication. For any reconstructed horizontal row these identities give
\begin{equation}\label{eq:terminating-step} \begin{equation}\label{eq:terminating-step}
p_{n+1} p_{n+1}
@ -642,7 +630,7 @@ P(n,t)={}&-5n-76n^2+1404n^3+4360n^4+4320n^5+1440n^6\\
&+(-51+659n+3086n^2+4500n^3+2232n^4)t^2\\ &+(-51+659n+3086n^2+4500n^3+2232n^4)t^2\\
&+(-72-432n-864n^2-576n^3)t^3. &+(-72-432n-864n^2-576n^3)t^3.
\end{align*} \end{align*}
Thus \eqref{eq:terminating-step} is the scalar form of the displayed Thus~\eqref{eq:terminating-step} is the scalar form of the displayed
matrix recurrence; no differential-equation uniqueness is used below. matrix recurrence; no differential-equation uniqueness is used below.
Let Let
@ -698,13 +686,11 @@ Moreover,
\[ \[
\deg((d_0(\theta)+zd_1(\theta))p_n)\le n+1. \deg((d_0(\theta)+zd_1(\theta))p_n)\le n+1.
\] \]
Equations \eqref{eq:term-constant}--\eqref{eq:term-top} therefore prove, Equations~\eqref{eq:term-constant}--\eqref{eq:term-top} therefore prove,
coefficient by coefficient, that the right side of coefficient by coefficient, that the right side of~\eqref{eq:terminating-step} is
\eqref{eq:terminating-step} is
\(\alpha_{n+1}\sum_{k=0}^{n+1}h_{n+1,k}z^k\). \(\alpha_{n+1}\sum_{k=0}^{n+1}h_{n+1,k}z^k\).
Starting from \eqref{eq:base-horizontal-row}, Starting from~\eqref{eq:base-horizontal-row},~\eqref{eq:full-gauge} propagates the horizontal form at every step.
\eqref{eq:full-gauge} propagates the horizontal form at every step. This proves~\eqref{eq:qhat} and~\eqref{eq:normalization} for the actual
This proves \eqref{eq:qhat} and \eqref{eq:normalization} for the actual
row \(CG_N\), not merely for a scalar surrogate. row \(CG_N\), not merely for a scalar surrogate.
The mandatory standalone checker independently expands the cleared The mandatory standalone checker independently expands the cleared
identities and rejects any nonzero coefficient. identities and rejects any nonzero coefficient.
@ -722,15 +708,14 @@ Moreover,
\end{corollary} \end{corollary}
\begin{proof} \begin{proof}
For \(0\le k\le n\), the coefficient of \(z^k\) in For \(0\le k\le n\), the coefficient of \(z^k\) in~\eqref{eq:qhat} has sign \((-1)^k\). Since \(z_0<0\), every summand is
\eqref{eq:qhat} has sign \((-1)^k\). Since \(z_0<0\), every summand is
nonnegative. Also nonnegative. Also
\[ \[
\frac{576n^2(2n+1)^2}{(6n+1)(6n+5)}-29n^2 \frac{576n^2(2n+1)^2}{(6n+1)(6n+5)}-29n^2
=\frac{n^2(1260n^2+1260n+431)} =\frac{n^2(1260n^2+1260n+431)}
{(6n+1)(6n+5)}>0. {(6n+1)(6n+5)}>0.
\] \]
Iterating \eqref{eq:normalization} proves the lower bound. Iterating~\eqref{eq:normalization} proves the lower bound.
\end{proof} \end{proof}
\section{From formal contact to convergence at \section{From formal contact to convergence at
@ -802,7 +787,7 @@ We now verify the analytic hypothesis behind the next step. On
so the series defining \(y\) and its first three Euler derivatives are so the series defining \(y\) and its first three Euler derivatives are
holomorphic on a neighborhood of the closed disk. Because \(f=O(x)\), holomorphic on a neighborhood of the closed disk. Because \(f=O(x)\),
the simple pole of \(C\) cancels in \(fC\), so \(\mathcal E_0\) is the simple pole of \(C\) cancels in \(fC\), so \(\mathcal E_0\) is
holomorphic there. Inspection of \eqref{eq:deformed-matrix} shows that holomorphic there. Inspection of~\eqref{eq:deformed-matrix} shows that
each \(M_m\) is holomorphic off \(x=0\) in this disk and has at most a each \(M_m\) is holomorphic off \(x=0\) in this disk and has at most a
simple pole at \(0\). Hence simple pole at \(0\). Hence
\(\mathcal R_{N,r}=x^n(\mathcal E_N)_{r,1}\), with \(n=N+1\), is \(\mathcal R_{N,r}=x^n(\mathcal E_N)_{r,1}\), with \(n=N+1\), is
@ -828,7 +813,7 @@ Corollary~\ref{cor:positivity} yields
Q_N(x_0)\ge Q_N(x_0)\ge
18\cdot29^N(N!)^2(1-x_0)^n. 18\cdot29^N(N!)^2(1-x_0)^n.
\] \]
Combining this with \eqref{eq:cauchy}, we obtain Combining this with~\eqref{eq:cauchy}, we obtain
\begin{equation}\label{eq:geometric-error} \begin{equation}\label{eq:geometric-error}
\left|\frac{E_{N,r}(x_0)}{q_N(x_0)}\right| \left|\frac{E_{N,r}(x_0)}{q_N(x_0)}\right|
=\left|\frac{\mathcal R_{N,r}(x_0)}{Q_N(x_0)}\right| =\left|\frac{\mathcal R_{N,r}(x_0)}{Q_N(x_0)}\right|
@ -850,20 +835,19 @@ Therefore
\section{Identification of the first-column limit} \section{Identification of the first-column limit}
By \eqref{eq:seed-identities} and the definition of \(\Phi\), By~\eqref{eq:seed-identities} and the definition of \(\Phi\),
\[ \[
A_0-\Phi A_1 A_0-\Phi A_1
=-A(\mathcal E_0)_{0,*}-B(\mathcal E_0)_{1,*}. =-A(\mathcal E_0)_{0,*}-B(\mathcal E_0)_{1,*}.
\] \]
Multiplying by \(G_N\e_1\), dividing by Multiplying by \(G_N\e_1\), dividing by
\(A_1G_N\e_1=S q_N\), and using \(A_1G_N\e_1=S q_N\), and using~\eqref{eq:error-vanish}, we get
\eqref{eq:error-vanish}, we get
\[ \[
\lim_{N\to\infty} \lim_{N\to\infty}
\frac{A_0G_N\e_1}{A_1G_N\e_1} \frac{A_0G_N\e_1}{A_1G_N\e_1}
=\Phi(x_0). =\Phi(x_0).
\] \]
Equation \eqref{eq:CM-value} therefore proves Equation~\eqref{eq:CM-value} therefore proves
\begin{equation}\label{eq:first-column} \begin{equation}\label{eq:first-column}
\boxed{ \boxed{
\lim_{N\to\infty}\frac{P_{N,1}}{Q_{N,1}} \lim_{N\to\infty}\frac{P_{N,1}}{Q_{N,1}}
@ -927,8 +911,7 @@ Q_R(1)=-(64R^3-105R^2+274R-233)<0,\qquad
Consequently the unique exterior zero is a simple real number Consequently the unique exterior zero is a simple real number
\(\rho>1\). \(\rho>1\).
\begin{lemma}[Explicit dominant-product dichotomy] \begin{lemma}[Explicit dominant-product dichotomy]\label{lem:dominant-product}
\label{lem:dominant-product}
Fix \(\tau\) with Fix \(\tau\) with
\[ \[
\max_{\lambda\ne\rho}|\lambda|<\tau<1, \max_{\lambda\ne\rho}|\lambda|<\tau<1,
@ -997,7 +980,7 @@ For stable columns \(\|h\|\le1\), set
\[ \[
\Psi_m(h)=\frac{E_mh-c_m}{a_m-b_mh}. \Psi_m(h)=\frac{E_mh-c_m}{a_m-b_mh}.
\] \]
Equations \eqref{eq:block-bounds}--\eqref{eq:block-separation} give Equations~\eqref{eq:block-bounds}--\eqref{eq:block-separation} give
\[ \[
\|\Psi_m(h)\| \|\Psi_m(h)\|
\le\frac{d_*+\epsilon}{a_*-\epsilon}<1. \le\frac{d_*+\epsilon}{a_*-\epsilon}<1.
@ -1009,7 +992,7 @@ For two such columns,
+\frac{(E_mk-c_m)b_m(h-k)} +\frac{(E_mk-c_m)b_m(h-k)}
{(a_m-b_mh)(a_m-b_mk)}, {(a_m-b_mh)(a_m-b_mk)},
\] \]
so \eqref{eq:graph-contraction-constant} gives so~\eqref{eq:graph-contraction-constant} gives
\[ \[
\|\Psi_m(h)-\Psi_m(k)\|\le q\|h-k\|. \|\Psi_m(h)-\Psi_m(k)\|\le q\|h-k\|.
\] \]
@ -1042,7 +1025,7 @@ U_m(a)=Z_m(a)P=(\alpha_m,\beta_m),\qquad
\xi_m=\alpha_m-\beta_mh_m,\qquad \xi_m=\alpha_m-\beta_mh_m,\qquad
d_m=a_m-b_mh_{m+1}. d_m=a_m-b_mh_{m+1}.
\] \]
Using \eqref{eq:graph-invariance} in Using~\eqref{eq:graph-invariance} in
\(U_{m+1}=U_mT_m\) gives the exact scalar equation \(U_{m+1}=U_mT_m\) gives the exact scalar equation
\[ \[
\xi_{m+1}=d_m\xi_m. \xi_{m+1}=d_m\xi_m.
@ -1053,8 +1036,7 @@ Define the composed seed functional and product
L_m=\prod_{\ell=m_0}^{m-1}d_\ell. L_m=\prod_{\ell=m_0}^{m-1}d_\ell.
\] \]
Both are now explicit, \(\Lambda\) is linear, and Both are now explicit, \(\Lambda\) is linear, and
\(\xi_m=\Lambda(a)L_m\). Equations \(\xi_m=\Lambda(a)L_m\). Equations~\eqref{eq:block-bounds}--\eqref{eq:block-separation} ensure
\eqref{eq:block-bounds}--\eqref{eq:block-separation} ensure
\(d_m\ne0\). \(d_m\ne0\).
If \(\Lambda(a)=0\), then \(\alpha_m=\beta_mh_m\) and If \(\Lambda(a)=0\), then \(\alpha_m=\beta_mh_m\) and
@ -1063,7 +1045,7 @@ If \(\Lambda(a)=0\), then \(\alpha_m=\beta_mh_m\) and
\|\beta_{m+1}\|<(d_*+\epsilon)\|\beta_m\| \|\beta_{m+1}\|<(d_*+\epsilon)\|\beta_m\|
<\tau\|\beta_m\|, <\tau\|\beta_m\|,
\] \]
which proves \eqref{eq:exceptional-decay}. which proves~\eqref{eq:exceptional-decay}.
If \(\Lambda(a)\ne0\), put \(r_m=\beta_m/\xi_m\). Exact substitution If \(\Lambda(a)\ne0\), put \(r_m=\beta_m/\xi_m\). Exact substitution
gives gives
@ -1089,8 +1071,7 @@ Since \(\alpha_m/\xi_m=1+r_mh_m\to1\),
\[ \[
U_m(a)=\Lambda(a)L_m\bigl((1,0)+o_a(1)\bigr). U_m(a)=\Lambda(a)L_m\bigl((1,0)+o_a(1)\bigr).
\] \]
Multiplying by \(P^{-1}\) proves Multiplying by \(P^{-1}\) proves~\eqref{eq:dominant-asymptotic} with
\eqref{eq:dominant-asymptotic} with
\[ \[
w=(1,0)P^{-1},\qquad w\mathcal S=\rho w. w=(1,0)P^{-1},\qquad w\mathcal S=\rho w.
\] \]
@ -1119,7 +1100,7 @@ inverse rescaling absorbed into \(L_m\). Since \(R>7\) and \(\rho>1\),
every displayed grouping is positive. Thus \(w_j(\rho)>0\) for every displayed grouping is positive. Thus \(w_j(\rho)>0\) for
\(j=1,2,3,4\); below we abbreviate \(w_j=w_j(\rho)\). \(j=1,2,3,4\); below we abbreviate \(w_j=w_j(\rho)\).
Undoing the balancing in \eqref{eq:dominant-asymptotic} gives, whenever Undoing the balancing in~\eqref{eq:dominant-asymptotic} gives, whenever
\(\Lambda(a)\ne0\), \(\Lambda(a)\ne0\),
\begin{equation}\label{eq:all-column-asymptotic} \begin{equation}\label{eq:all-column-asymptotic}
aG_m\e_j=(m!)^2m^{-(j-1)} aG_m\e_j=(m!)^2m^{-(j-1)}
@ -1131,19 +1112,17 @@ The positivity estimate and \(Q_m=x_0^{m+1}q_m\) give
\frac{q_m(x_0)}{(m!)^2} \frac{q_m(x_0)}{(m!)^2}
\ge18(R-1)\,[29(R-1)]^m. \ge18(R-1)\,[29(R-1)]^m.
\end{equation} \end{equation}
If \(\Lambda(C)=0\), the first coordinate of If \(\Lambda(C)=0\), the first coordinate of~\eqref{eq:exceptional-decay} would contradict~\eqref{eq:q-lower}.
\eqref{eq:exceptional-decay} would contradict \eqref{eq:q-lower}.
Therefore Therefore
\[ \[
\Lambda(A_1)=S\Lambda(C)\ne0. \Lambda(A_1)=S\Lambda(C)\ne0.
\] \]
If \(\Lambda(A_0)=0\), then If \(\Lambda(A_0)=0\), then~\eqref{eq:exceptional-decay},~\eqref{eq:dominant-asymptotic}, and
\eqref{eq:exceptional-decay}, \eqref{eq:dominant-asymptotic}, and
\(|d_m|>1\) for large \(m\) would make the first-column quotient tend \(|d_m|>1\) for large \(m\) would make the first-column quotient tend
to zero, contradicting \eqref{eq:first-column}. Hence to zero, contradicting~\eqref{eq:first-column}. Hence
\(\Lambda(A_0)\ne0\) as well. \(\Lambda(A_0)\ne0\) as well.
Because \(w_j>0\), equation \eqref{eq:all-column-asymptotic} first proves Because \(w_j>0\), equation~\eqref{eq:all-column-asymptotic} first proves
that every \(Q_{m,j}\) is nonzero for all sufficiently large \(m\), and that every \(Q_{m,j}\) is nonzero for all sufficiently large \(m\), and
only then permits division: only then permits division:
\[ \[