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This page checks the sign change behind Theorem 1.4 of Li and Zhuang's draft (the version of 11 October 2026 recorded on their claim page): the argument by which the weighted-dilation manuscript proves its Theorem 1.2, the count of primes pp with P+(p−1)≤xδP^+(p-1)\le x^\delta, is rerun for primes Nu=2u−1N_u=2u-1 in place of Nu=2u+1N_u=2u+1. The observation and the outline of the change are Li and Zhuang's; the check below is Plasma AI's, author-recorded and unreviewed. It is a check of every step at which the sign enters, read in the library's transcription of Sections 2–7 of the manuscript. The steps that do not involve the sign are used as the manuscript writes them; they, and Sections 3–5, are premises of this sign audit. The complete conditional derivation writes out the Type II and sieve arguments and separately examines the analytic core at author standing. Its uniform premises (P) and (E) remain unrefereed inputs.

The claimed conclusion

Conditional count. Assume that the manuscript's argument for its Theorem 1.2 is correct in every step that does not involve the form 2u+12u+1: the results of its Section 2, Theorem 5.1 (with Sections 3 and 4 behind it), Proposition 7.1, Lemmas 7.3 and 7.4, and the sign-free steps of the proofs of Theorem 6.1 and of Section 7. Then for every fixed 0<δ<1/40<\delta<1/4, as x→∞x\to\infty through real values,

#{p prime: 2x−1≤p≤4x−1, P+(p+1)≤xδ}≥x1−o(1).(1)\#\{p\text{ prime}:\ 2x-1\le p\le4x-1,\ P^+(p+1)\le x^\delta\} \ge x^{1-o(1)}. \tag{1}

In particular Hypothesis A+\mathrm A^+ holds: for 0<δ<1/40<\delta<1/4 and η>0\eta>0, (1) at x=yx=y gives at least y1−o(1)≥y1−ηy^{1-o(1)}\ge y^{1-\eta} primes p≤5yp\le5y with P+(p+1)≤yδP^+(p+1)\le y^\delta for all large real yy. The range in (1) lies inside the range 2x−2<p≤5x2x-2<p\le5x of Li and Zhuang's Theorem 1.4.

The manuscript fixes the notation used below: L=log⁡xL=\log x, W=exp⁡(L)W=\exp(\sqrt L), the weight A(u)=aQ(u∗)Wℓ(u)A(u)=a_Q(u_*)W_\ell(u) on integers uu (its (6.3) and the Section 7 choices q=1/2q=1/2, ℓ=1\ell=1), whose definition involves only uu, the smooth cutoff Ψ(u/x)\Psi(u/x) with Ψ\Psi supported in a fixed compact subinterval of (0,∞)(0,\infty) (in Section 7, inside [1,2][1,2]), and the mass XA=∑uA(u)Ψ(u/x)X_A=\sum_uA(u)\Psi(u/x). The sign enters only through NuN_u.

The Type II estimate

The changed statement is Theorem 6.1 with mn=2u−1mn=2u-1 in place of mn=2u+1mn=2u+1 in its display (6.5), with the same hypotheses and constants. Its proof changes at the following places and nowhere else.

Large group-prime factor. The bound exp⁡(O(L))\exp(O(\sqrt L)) for the number of divisors mm of NuN_u all of whose prime factors exceed WW uses only Nu≪xN_u\ll x, which holds on the support of Ψ(u/x)\Psi(u/x): such an integer has O(L/log⁡W)=O(L)O(L/\log W)=O(\sqrt L) prime factors above WW, counted with multiplicity. It holds for 2u−12u-1.

Absolute control. The bound (6.10) becomes ∑u≍xτ(u)τ(2u−1)≪xLO(1)\sum_{u\asymp x}\tau(u)\tau(2u-1)\ll xL^{O(1)}, by Cauchy's inequality and the fixed divisor moments of the manuscript's Lemma 2.5 applied to uu and to the odd integers 2u−1≪x2u-1\ll x.

The diagonal. For m=m′m=m' the two equations mn=2eh−1=2eh′−1mn=2eh-1=2eh'-1 force h=h′h=h'. For fixed m,nm,n the admissible ee divide (mn+1)/2(mn+1)/2, and

∑e∣(mn+1)/2τ(mn+12e)2≤τ(mn+1)3,\sum_{e\mid(mn+1)/2}\tau\Bigl(\frac{mn+1}{2e}\Bigr)^2\le\tau(mn+1)^3,

since each term is at most τ(mn+1)2\tau(mn+1)^2 and there are at most τ(mn+1)\tau(mn+1) terms. Collecting by v=mnv=mn gives

Ndiag≪LO(1)∑v≍xτ(v)τ(v+1)3≪xLC5,\mathcal N_{\rm diag}\ll L^{O(1)}\sum_{v\asymp x}\tau(v)\tau(v+1)^3 \ll xL^{C_5},

again by Cauchy's inequality and Lemma 2.5. The exponent is independent of the splitting parameter K0K_0, as in the manuscript.

The determinant identity. Take an off-diagonal pair

mn=2eh−1,m′n=2eh′−1,m≠m′.(2)mn=2eh-1,\qquad m'n=2eh'-1,\qquad m\ne m'. \tag{2}

The first equation gives mn≡−1(mod2e)mn\equiv-1\pmod{2e}, so nn is a unit modulo 2e2e. Subtracting, (m′−m)n=2e(h′−h)(m'-m)n=2e(h'-h), hence 2e∣m′−m2e\mid m'-m. Write m′−m=−2ekm'-m=-2ek with an integer k≠0k\ne0. Then h′−h=−knh'-h=-kn, and

mh′−m′h=m(h−kn)−(m−2ek)h=−k(mn−2eh)=k.mh'-m'h=m(h-kn)-(m-2ek)h=-k(mn-2eh)=k.

So the cross products are again z=m′hz=m'h and z+k=mh′z+k=mh', with the shift kk of the opposite sign to the manuscript's choice; Theorem 5.1 allows every integral 0<∣k∣≤LC0<|k|\le L^C. The size bound 0<∣k∣≪LK0+Cs0<|k|\ll L^{K_0+C_s} of (6.17) follows from ∣m′−m∣≪U|m'-m|\ll U and e≫EL−Cs=UL−K0−Cse\gg EL^{-C_s}=UL^{-K_0-C_s}.

The converse. Fix an integer k≠0k\ne0, positive integers m,m′,h,h′m,m',h,h' with P−(m),P−(m′)>WP^-(m),P^-(m')>W, m′h=zm'h=z and mh′=z+kmh'=z+k, and suppose $m'\equiv m\pmod{2|k|}$ and e=(m−m′)/(2k)>0e=(m-m')/(2k)>0. Then ee is an integer, and

m(h′−h)=k+(m′−m)h=k−2ekh=−k(2eh−1).m(h'-h)=k+(m'-m)h=k-2ekh=-k(2eh-1).

Every prime factor of mm exceeds WW, while ∣k∣≤LO(1)<W|k|\le L^{O(1)}<W for large xx, so (m,k)=1(m,k)=1 and m∣2eh−1m\mid2eh-1. Put n=(2eh−1)/mn=(2eh-1)/m, a positive integer. Then h′−h=−knh'-h=-kn and m′n=mn−2ekn=2eh−1+2e(h′−h)=2eh′−1m'n=mn-2ekn=2eh-1+2e(h'-h)=2eh'-1, which recovers (2). The forward and converse maps are inverse to each other, as in the manuscript. Both mm and m′m' are odd and coprime to kk, hence units modulo 2∣k∣2|k|, so the congruence is imposed by the same character expansion (6.19).

The cutoff arguments. In place of (6.20) the smooth (e,n)(e,n) cutoffs are evaluated at

e=m−m′2k,n=2eh−1m=(m−m′)zkmm′−1m,e=\frac{m-m'}{2k},\qquad n=\frac{2eh-1}m=\frac{(m-m')z}{kmm'}-\frac1m,

which differ from the manuscript's expressions only by the sign of kk and of the last term. Their derivatives in log⁡(m/U)\log(m/U), log⁡(m′/U)\log(m'/U) and log⁡(z/Z)\log(z/Z) obey the bounds stated after (6.20), so the Fourier separation has the same total variation.

The endpoints. Since m,m′m,m' are free of group primes, z∗=m′h∗z_*=m'h_*, (z+k)∗=mh∗′(z+k)_*=mh'_*, Wℓ(z)=Wℓ(h)W_\ell(z)=W_\ell(h) and Wℓ(z+k)=Wℓ(h′)W_\ell(z+k)=W_\ell(h'), exactly as before. The endpoint functions (6.22) and (6.23) and the separated summand are unchanged, with character modulus 2∣k∣2|k|, and the discrepancy hypothesis is still carried by the original sequence α\alpha. Theorem 5.1 bounds each separated correlation, and the remaining steps, including the order of precisions in Remark 6.2, are unchanged.

The extraction of primes

Candidate mass. Proposition 7.1 concerns A(u)A(u), XAX_A and the prime factors of uu only, and is used as stated.

Type I distribution. For odd squarefree dd, the congruence 2u−1≡0(modd)2u-1\equiv0\pmod d holds exactly when u≡2ˉ(modd)u\equiv\bar2\pmod d, where 2ˉ\bar2 is the inverse of 22 modulo dd, which is a unit class. The proof of Proposition 7.2 uses only that the congruence fixes one unit class of uu: character orthogonality on that class, the cost of the noncoprime moduli, and the large sieve and Siegel–Walfisz bounds for the twisted sums are all taken in absolute value. The remainder bound (7.8) therefore holds for Nu=2u−1N_u=2u-1, and it excludes dd with (d,u)>1(d,u)>1 automatically.

Preliminary sieve. For an odd prime pp the Type I main term gives density 1/(p−1)1/(p-1) for p∣Nup\mid N_u, as before, so the sieve bound (7.11) and its singular series S\mathfrak S are unchanged. Every NuN_u is odd, so the prime 22 never divides it.

Composites away from balance. Theorem 6.1 for 2u−12u-1, Lemmas 7.3 and 7.4 and the sieve with moduli pdpd through the Type I bound give (7.21) and (7.22) unchanged. Lemma 7.4's bound (7.17) uses only mn=Numn=N_u with Nu≍xN_u\asymp x.

Balanced composites. The two applications of Theorem 6.1 now concern mn=2u−1mn=2u-1. In the two-variable sieve, D1D_1 contains the complete micro-band lists, including the exceptional rough integer, and one marked prime per P-group. Its pure prime entries are at least L20L^{20}, and every prime factor of the exceptional integer exceeds WW, so D1D_1 is odd. Hence D1∣uD_1\mid u and mn=2u−1mn=2u-1 give

mn≡−1(modD1)mn\equiv-1\pmod{D_1}

in place of mn≡1mn\equiv1. For each unit residue of mm modulo D1D_1 exactly one residue of nn satisfies this, including when D1D_1 has prime-power factors, so there are again exactly φ(D1)\varphi(D_1) residue pairs. For an odd prime l∤D1l\nmid D_1 the bad events are mn≡0(modl)mn\equiv0\pmod l for l≤Wl\le W, with 2l−12l-1 residue pairs, and, for a banned prime, l∣ul\mid u, which now reads mn≡−1(modl)mn\equiv-1\pmod l, with l−1l-1 residue pairs. The two sets are disjoint, so ν(l)\nu(l), the densities g(l)g(l), the Chinese-remainder counts, the lattice errors (7.28) and the Euler product (7.29) are unchanged, and so is the dyadic bound (7.30) and the balanced bound (7.31), with the same constant CbalC_{\rm bal}.

Counting the primes. The parameter choices are made in the manuscript's order. Subtracting (7.31) from (7.22) leaves ∑2u−1 primeA(u)Ψ(u/x)≫XA/L\sum_{2u-1\text{ prime}}A(u)\Psi(u/x)\gg X_A/L. Each summand is at most exp⁡(O(L))\exp(O(\sqrt L)) by Proposition 7.1, XA≫xL−CAX_A\gg xL^{-C_A}, and u↦2u−1u\mapsto2u-1 is injective, so at least x1−o(1)x^{1-o(1)} distinct primes p=2u−1p=2u-1 occur. Since Ψ(u/x)≠0\Psi(u/x)\ne0 forces x≤u≤2xx\le u\le2x, they satisfy 2x−1≤p≤4x−12x-1\le p\le4x-1, and

P+(p+1)=P+(2u)=max⁡(2,P+(u))≤xδP^+(p+1)=P^+(2u)=\max\bigl(2,P^+(u)\bigr)\le x^\delta

for large xx, because every prime factor of a supported uu lies in [L20,xδ][L^{20},x^\delta]. This is (1).

Quantifiers, errors and the order of choices

The transfer retains the manuscript's quantifiers, not an effective numerical threshold. Fix δ∈(0,1/4)\delta\in(0,1/4) and the candidate geometry, including Ψ\Psi, r0r_0, the Q/P bands, the finite lower-bound prefix, and j′,θj',\theta of (7.24). Its estimates give constants CA,Cw,cA>0C_A,C_w,c_A>0 with XA≥cAxL−CAX_A\ge c_AxL^{-C_A} and each prime summand at most exp⁡(CwL)\exp(C_w\sqrt L) once xx exceeds a threshold depending on the fixed parameters. None of these bounds depends on the sign.

The balanced error is exactly of the form

Cbal(κ+L−1)XAL+o(XA/L),C_{\rm bal}(\kappa+L^{-1})\frac{X_A}{L}+o(X_A/L),

where the source asserts that CbalC_{\rm bal} is independent of κ,b1,j∗∗\kappa,b_1,j_{**} and the later discrepancy precision SS. The residue calculation above preserves that independence. Choose κ∈(0,1/50)\kappa\in(0,1/50) with Cbalκ<S/4C_{\rm bal}\kappa<\mathfrak S/4, then b1b_1 small enough for (7.11), (7.19) and (7.22), and set b∗=b1/3b_*=b_1/3. Choose j∗∗j_{**} so that η∗<b∗/4\eta_*<b_*/4, as required by Theorem 6.1 and (7.10), and fix the finite exponent mesh. Type I is used at the source's level x1/2−κ/2x^{1/2-\kappa/2}; changing a unit class does not enlarge that level.

Next choose the Type II saving D∗D_* so large that its error xL−D∗xL^{-D_*}, including the fixed powers of LL from all dyadic sums and separations, is o(XA/L)o(X_A/L). For example, if those losses are at most LClossL^{C_{\rm loss}}, it is enough to take D∗>CA+1+ClossD_*>C_A+1+C_{\rm loss}. Those coefficient exponents are fixed independently of SS. Theorem 6.1 then fixes its required discrepancy exponent BB; only afterwards is SS chosen large enough for Lemma 7.3 to supply it. The source's sign-free assertions of these bounds and their uniformity remain explicit premises of this argument.

With every parameter fixed in that order, subtraction leaves cXA/LcX_A/L on primes for a fixed c>0c>0 and all sufficiently large real xx. Consequently the retained lower bound is

c′xL−CA−1exp⁡(−CwL).c' xL^{-C_A-1}\exp(-C_w\sqrt L).

For each fixed η>0\eta>0, its ratio to x1−ηx^{1-\eta} tends to infinity, because ηL−(CA+1)log⁡L−CwL+log⁡c′→∞\eta L-(C_A+1)\log L-C_w\sqrt L+\log c'\to\infty. Taking the maximum of the earlier thresholds and this last threshold gives x0(δ,η)x_0(\delta,\eta) valid for every real x≥x0x\ge x_0. No uniformity as δ↓0\delta\downarrow0, and no computable value of x0x_0, is claimed. This is exactly the fixed-δ\delta quantification needed by A+\mathrm A^+.

Places checked and not checked

Read in full here, in the transcription, for every use of the sign: the statements of Theorem 1.2, Theorem 5.1 with its endpoint form (5.1)–(5.4), and Theorem 6.1; the results of Section 2 that Sections 6 and 7 use (Theorems 2.2 and 2.3, Corollary 2.4, Lemmas 2.5–2.9 and Corollary 2.10), none of which involves the sign; the whole proof of Theorem 6.1; and the whole of Section 7, including the proofs of Propositions 7.1 and 7.2 and Lemmas 7.3 and 7.4. Sections 1–5 and 8 were searched for the form 2u+12u+1, which occurs there only in the description of the method in the introduction. Every use of the sign in those proofs is listed above, each with the identity, bound or count that replaces it. The sign-free steps were read for their role, not checked line by line.

Outside this sign audit: Sections 3–5, the transference theorem, the ideal kernels and the lifted shift cancellation, which carry the new analytic method and on which Theorem 5.1 rests; the sign-free steps of Sections 6 and 7; and the cited external results. The [[research/smooth_successor_primes/shift_sign_analytic_core|separate analytic-core examination]] records proof-depth author reading of Sections 3–5 and the precise uniform assertion still needed; it grants no independent standing. Li and Zhuang record that Lean statements for the manuscript required the hypothesis ℓ≥1\ell\ge1 in its definition of prime groups; Section 7 takes ℓ=1\ell=1, so this does not affect the count.