Disposition: PASS on the paper identities and the matched control margin; CORRECTION to review-status wording; OPEN on the original all-height sign.
Reviewed scientific baseline: d93aaf6b8dbe1fcbebf6fff4f6d1f71d993f4208
(PR75). Working HEAD when read: edc65638cc5e761a0290b38d54ff0b9bac140697.
I read AGENTS section 0, this audit’s brief and derivation (1)-(12), the
relevant ZERO-GEOMETRY register entry, PR75’s complete pair/boundary
derivation, PR74’s complete-moment control and its adversarial review.
The parent performed the full register review; I did not independently
replay every historical proof or certificate. No scan or computation was
run. Source applicability was checked directly against
Csordas, arXiv:1309.0055v2, Definition
1.2 and Section 2. This file is internal review working material.
Wall check: Same open gap. Closest: NS100/101 and PR74/75. The change repairs ordinary-transform domain accounting; no new original-arithmetic lower bound has been supplied. An existing matched control defeats only the stated generic primitive-positivity inference.
The argument assumes the inherited complete original phi is positive; it does not assume its Fourier transform has a Laguerre sign. This premise can also be checked directly: for u>=0, put w_n=pin^2exp(2u). Applying the displayed differential operator termwise to the convergent theta series gives
phi(u)=sum_(n>=1) exp(u/2-w_n)*w_n*(2*w_n-3) > 0.
Here w_n>=pi>3/2; reciprocity gives the negative half-line. Thus using positive phi in the Green representation does not import the desired transform sign. The Green multiplier is correct: at a=1/2, exp(-aabs(u))/(2a)=exp(-abs(u)/2), and the right side of the equation is 4phi. The difference of the two decaying solutions has the form c_plusexp(u/2)+c_minus*exp(-u/2); decay at both ends kills both coefficients. No extra homogeneous or point-mass term can be retained.
The strict upper envelope in (4) uses the strictly positive theta tail in (1), while its strict lower bound uses the Green representation. These are separate justifications, and both hold at u=0. Reflecting the exact smooth h is legitimate; reflecting a finite series here would not be the same argument.
The bounds in (6) have the correct constants. The product envelope is exp(-max(abs(s),T)), T=abs(t). Its central interval contributes 2Texp(-T) for A_0 and 2T^3exp(-T)/3 for A_2; the two exterior intervals contribute 2exp(-T) and 2(T^2+2T+2)exp(-T), respectively.
The u=s+t, v=s-t Jacobian is 1/2. Including s^2=(u+v)^2/4 gives the factor 1/8 for the second moment. Its square terms yield -2YY’’ and its cross terms yield +2*Y’^2, proving the factor 1/4 in (8). This relies on the stated even real f, not on arbitrary noneven kernels.
Independently expanding the product gives
L1[p*Y]=p^2*L1[Y]+(p'^2-p*p'')*Y^2,
p=r^2+1/4,
p'^2-p*p''=2*(r^2-1/4).
Thus (9) and (10) are correct. The positive correction required inside abs(r)<1/2 cannot be removed. The pair calculation neither estimates nor changes this obligation.
Exceptional real points cause no division problem:
The regularization changes the entire-transform class: the complex zeros of p are genuine poles of Y, not removable singularities. In particular X(+/-i/2)=1/4, so the residues of Y=4X/p are -i at i/2 and +i at -i/2. On either boundary of the convergence strip one spatial tail has a nondecaying oscillatory leading term. Its ordinary improper integral fails even away from the pole; analytic continuation at those other boundary points is a different operation. The draft distinguishes them.
Write k=m2/m0>0 and r_beta=pi/beta. For beta^2>=pi^2*k,
X(r_beta)>=m0/2,
L1[X](r_beta)/X(r_beta)^2<=6*k,
B_beta^2*L1[X_beta](r_beta)
=L1[X](r_beta)-2*beta^2*X(r_beta)^2.
The negative coefficient is important: from X^2>=m0^2/4 one gets the upper bound
L1[X_beta](r_beta)
<= -(beta^2-3*k)*m0^2/(2*B_beta^2)<0.
No inequality direction is reversed. Strictness follows from k>0 and pi^2>3. The additional beta>=2 restriction is inherited from the control family’s zero-strip discussion, not needed for this moment inequality. There is no claim here for the particular beta=2 member when its moment condition is not established.
More explicitly, define the exact corrected-target difference
D_beta(r)=L1[Y_beta](r)
-2*(1/4-r^2)*Y_beta(r)^2/p(r)^2.
Equation (9), applied to the complete control, gives the full margin
D_beta(r_beta)=16*L1[X_beta](r_beta)/p(r_beta)^2
<= -8*(beta^2-3*k)*m0^2
/(B_beta^2*p(r_beta)^2) < 0.
This is simply the existing control margin transferred through an exact identity. It is not a new estimate for original X. It works whichever side of abs(r)=1/2 contains r_beta.
The envelope is genuinely retained, rather than merely asymptotic: triangle inequalities give exp(u/2)*exp(-abs(u-beta)/2)<=exp(beta/2) for u>=0, and the other shift contributes exp(-beta/2). The weighted sum is bounded by precisely B_beta. For u>beta all three leading terms sum to B_beta, so the leading tail coefficient is exactly one after division. Positivity and evenness also survive. These facts do not require the original nonlinear IVP.
Constants in derivative and shifted-tail remainder bounds can depend on the chosen beta. This should be explicit if any summary uses the word “uniform”: the draft proves each fixed control shares the hypotheses, not a beta-uniform family of every derivative bound. There is no contradiction between positive L1 at r=0 for each fixed beta and its negative value at r=pi/beta as beta grows.
No fatal mathematical defect found in the bounded audit. No surviving independent original-arithmetic sign method is identified by this review. No scan, row, thaw, manuscript version or general route closure follows.