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CSM_RH Paper 28 — Bounded-Primitive Sieve Neutrality and the Residual PESC Self-Energy Lock

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CSM_RH Paper 28

Bounded-Primitive Sieve Neutrality and the Residual PESC Self-Energy Lock

Project: CSM_RH
Paper: 28
Version: v0.1
Date: 2026-09-07
Parent state: CSM_RH v1.18 / Paper 27
Campaign: 27 — DIRECT_PESC_ATTACK_II
Status: direct bilinear sieve-model audit / fixed-exponent equivalence theorem; not a proof or disproof of RH


0. Trust boundary

This paper does not prove or disprove the Riemann Hypothesis.

RH_PROVED = FALSE
RH_DISPROVED = FALSE
GLOBAL_RH_CERTIFICATE = FALSE
CSM_RH_ROOT_STATUS = OPEN

Campaign 27 returns from positive fourth-moment surrogates to the signed bilinear PESC root.

The first direct attack is to subtract the modern sieve approximant Λ\Lambda^\sharp inside the bilinear energy.

The result is a closure theorem:

because the centered sieve model has a subpolynomially bounded primitive, subtracting it is fixed-exponent neutral. The residual self-correlation is PESC-equivalent at every first-strip exponent.

Thus the modern local sieve model captures congruence structure but does not absorb a polynomial smooth prime-error drift.

No live GLM-5.3-Flash run is claimed.


1. Lambda-side PESC analogue

Work first with the centered von Mangoldt sequence

an=Λ(n)1.\boxed{ a_n=\Lambda(n)-1. }

Define its primitive

A(j)=njan=ψ(j)j.\boxed{ A(j)=\sum_{n\le j}a_n = \psi(j)-j. }

For the dyadic endpoint interval

Nj2N1,N\le j\le2N-1,

define the endpoint multiplicity

wN(n)=#{j[N,2N1]:nj}.\boxed{ w_N(n) = \#\{ j\in[N,2N-1]: n\le j \}. }

Thus

wN(n)={N,nN,2Nn,N<n<2N,0,n2N.w_N(n) = \begin{cases} N,&n\le N,\\ 2N-n,&N<n<2N,\\ 0,&n\ge2N. \end{cases}

Define

Ja(N)=j=N2N1A(j)2,J_a(N) = \sum_{j=N}^{2N-1}A(j)^2, Da(N)=n<2NwN(n)an2,D_a(N) = \sum_{n<2N}w_N(n)a_n^2,

and

Ca(N)=n<2NwN(n)anA(n1).\boxed{ \mathcal C_a(N) = \sum_{n<2N} w_N(n)a_nA(n-1). }

The exact energy identity is

Ja=Da+2Ca.\boxed{ J_a = D_a + 2\mathcal C_a. }

For first fixed-strip exponents 0<κ<1/20<\kappa<1/2, Paper 10's prime-power stripping transfers this Lambda-side mean-square / self-correlation branch back to the canonical prime-only PESC branch.


2. Modern sieve approximant

The 2026 higher-uniformity framework uses

Λ(n)=Qφ(Q)1(n,Q)=1,\boxed{ \Lambda^\sharp(n) = \frac{Q}{\varphi(Q)} 1_{(n,Q)=1}, }

where

Q=P(R)=p<RpQ=P(R) = \prod_{p<R}p

and

R=exp((logX)1/10).\boxed{ R = \exp \left( (\log X)^{1/10} \right). }

Define the centered model

bn=Λ(n)1.\boxed{ b_n = \Lambda^\sharp(n)-1. }

Define the true residual

fn=Λ(n)Λ(n).\boxed{ f_n = \Lambda(n)-\Lambda^\sharp(n). }

Then

an=bn+fn.\boxed{ a_n=b_n+f_n. }

Let

B(j)=njbn,B(j)=\sum_{n\le j}b_n,

and

F(j)=njfn.F(j)=\sum_{n\le j}f_n.

Then

A(j)=B(j)+F(j).\boxed{ A(j)=B(j)+F(j). }

3. Exact zero mean of the model over one period

The function Λ\Lambda^\sharp is periodic modulo QQ.

Over a complete residue period,

n=1QΛ(n)=Qφ(Q)φ(Q)=Q.\sum_{n=1}^{Q} \Lambda^\sharp(n) = \frac{Q}{\varphi(Q)} \varphi(Q) = Q.

Therefore:

Theorem 3.1 — Exact Period Mean

n=1Qbn=0.\boxed{ \sum_{n=1}^{Q}b_n = 0. }

Thus the centered model has zero primitive drift over every complete period.


4. Subpolynomial primitive bound

Because bnb_n is QQ -periodic with zero period mean,

supjB(j)Q(1+Qφ(Q)).\boxed{ \sup_j|B(j)| \ll Q \left( 1+ \frac{Q}{\varphi(Q)} \right). }

Mertens' product estimate gives

Qφ(Q)logR.\frac{Q}{\varphi(Q)} \ll \log R.

Chebyshev's estimate for the first Chebyshev function gives

logQ=p<Rlogp=O(R).\log Q = \sum_{p<R}\log p = O(R).

But

R=exp((logX)1/10)=o(logX).R = \exp \left( (\log X)^{1/10} \right) = o(\log X).

Hence

Q=Xo(1)\boxed{ Q = X^{o(1)} }

and therefore

Theorem 4.1 — Bounded Primitive of the Sieve Model

supjB(j)=Xo(1).\boxed{ \sup_j|B(j)| = X^{o(1)}. }

This is the decisive low-frequency property of Λ\Lambda^\sharp.


5. Mean-square equivalence after sieve subtraction

Define the residual mean-square

Jf(N)=j=N2N1F(j)2.\boxed{ J_f(N) = \sum_{j=N}^{2N-1}F(j)^2. }

Since

A=F+B,A=F+B,

we have

JaJf=2j=N2N1F(j)B(j)+j=N2N1B(j)2.J_a-J_f = 2\sum_{j=N}^{2N-1}F(j)B(j) + \sum_{j=N}^{2N-1}B(j)^2.

Chebyshev's bound gives

ψ(x)x.\psi(x)\ll x.

The periodic model has total summatory function

nxΛ(n)=x+Xo(1).\sum_{n\le x}\Lambda^\sharp(n) = x+X^{o(1)}.

Hence

F(j)=O(N)F(j)=O(N)

uniformly for j2Nj\le2N.

Combining with Theorem 4.1:

Theorem 5.1 — Fixed-Exponent Mean-Square Neutrality

Ja(N)=Jf(N)+O(N2Xo(1)).\boxed{ J_a(N) = J_f(N) + O \left( N^2X^{o(1)} \right). }

Therefore, for every fixed

0<κ<1,0<\kappa<1, Ja(N)N3κ+o(1)    Jf(N)N3κ+o(1).\boxed{ J_a(N) \ll N^{3-\kappa+o(1)} \iff J_f(N) \ll N^{3-\kappa+o(1)}. }

For the canonical first-strip branch we later restrict to κ<1/2\kappa<1/2 because of prime-power stripping.


6. Diagonal equivalence

Define

Df(N)=n<2NwN(n)fn2.D_f(N) = \sum_{n<2N} w_N(n)f_n^2.

Since

an=fn+bn,a_n=f_n+b_n, DaDf=n<2NwN(n)[2fnbn+bn2].D_a-D_f = \sum_{n<2N} w_N(n) [ 2f_nb_n+b_n^2 ].

On the relevant range,

fn+bn=Xo(1).|f_n|+|b_n| = X^{o(1)}.

Also,

0wN(n)N0\le w_N(n)\le N

and there are O(N)O(N) contributing nn.

Therefore:

Theorem 6.1 — Diagonal Neutrality

Da(N)=Df(N)+O(N2Xo(1)).\boxed{ D_a(N) = D_f(N) + O \left( N^2X^{o(1)} \right). }

7. Residual PESC equivalence

Define

Cf(N)=n<2NwN(n)fnF(n1).\boxed{ \mathcal C_f(N) = \sum_{n<2N} w_N(n)f_nF(n-1). }

The residual energy identity is

Jf=Df+2Cf.J_f = D_f + 2\mathcal C_f.

Subtracting from the original energy identity and using Theorems 5.1 and 6.1 gives:

Theorem 7.1 — Sieve-Residual PESC Equivalence

Ca(N)=Cf(N)+O(N2Xo(1)).\boxed{ \mathcal C_a(N) = \mathcal C_f(N) + O \left( N^2X^{o(1)} \right). }

Hence for every fixed

0<κ<1,0<\kappa<1, Ca(N)N3κ+o(1)    Cf(N)N3κ+o(1).\boxed{ \mathcal C_a(N) \ll N^{3-\kappa+o(1)} \iff \mathcal C_f(N) \ll N^{3-\kappa+o(1)}. }

Combining with the already certified prime-power bridge:

Corollary 7.2 — Canonical First-Strip Residual Equivalence

For every fixed

0<κ<12,0<\kappa<\frac12,

the canonical prime-only PESC fixed-power bound is exponent-equivalent to the Lambda-sharp residual self-correlation bound

Cf(N)N3κ+o(1).\boxed{ \mathcal C_f(N) \ll N^{3-\kappa+o(1)}. }

Create:

B-RH-004
SIEVE_RESIDUAL_PESC_EQUIVALENCE
status:
  CERTIFIED

8. Direct cross-term identity

The equivalence can also be seen directly.

Since

a=f+ba=f+b

and

A=F+B,A=F+B,

the two mixed PESC terms are

nwN(n)bnF(n1)+nwN(n)fnB(n1).\sum_nw_N(n)b_nF(n-1) + \sum_nw_N(n)f_nB(n-1).

Using

Δ(BF)n=bnF(n1)+fnB(n1)+bnfn,\Delta(BF)_n = b_nF(n-1) + f_nB(n-1) + b_nf_n,

the mixed sum becomes

nwN(n)Δ(BF)nnwN(n)bnfn.\boxed{ \sum_nw_N(n)\Delta(BF)_n - \sum_nw_N(n)b_nf_n. }

By the definition of wNw_N,

nwN(n)Δ(BF)n=j=N2N1B(j)F(j).\sum_nw_N(n)\Delta(BF)_n = \sum_{j=N}^{2N-1}B(j)F(j).

Both terms are

O(N2Xo(1)).O(N^2X^{o(1)}).

Thus the model-residual cross terms are exponent-neutral.

The critical term is the residual self-correlation Cf\mathcal C_f.


9. Bounded-primitive approximant neutrality

The argument above does not fundamentally depend on the exact sieve formula.

It reveals a general principle:

an approximant whose centered primitive is subpolynomial cannot absorb a polynomial-scale cumulative drift, and subtracting it cannot lower the first fixed-power mean-square/PESC strength.

Create:

O-RH-060
BOUNDED_PRIMITIVE_APPROXIMANT_NEUTRALITY
status:
  CERTIFIED FOR THE LAMBDA-SHARP MODEL

The statement is certified here for the specific modern Λ\Lambda^\sharp approximant.

A general abstract version would require explicit hypotheses on pointwise size and primitive growth.


10. What Lambda-sharp captures

The model Λ\Lambda^\sharp captures the deterministic obstruction from small prime divisibility.

Its periodic primitive is tiny at polynomial scale.

Therefore it can encode:

small-prime congruence structure;
local sieve density;
structured local model terms.

But it cannot encode:

a cumulative component x^beta with fixed beta>0;
a persistent polynomial smooth drift;
the long low-frequency mode responsible for fixed-strip strength.

The latter remains almost completely inside

F=AB.F=A-B.

11. Current local residual theorem is compatible with a fixed drift

The 2026 theorem gives for almost all polynomial short intervals

F(x+H)F(x)HlogAX\boxed{ F(x+H)-F(x) \ll H\log^{-A}X }

for every fixed A>0A>0 in the stated range.

Now consider a hypothetical smooth component

Fβ(x)=xβ,0<β<1.F_{\beta}(x)=x^\beta, \qquad 0<\beta<1.

For

H=o(X),H=o(X), Fβ(x+H)Fβ(x)=βHXβ1+O(H2Xβ2).F_\beta(x+H)-F_\beta(x) = \beta H X^{\beta-1} + O \left( H^2X^{\beta-2} \right).

But for every fixed AA,

Xβ1logAX.\boxed{ X^{\beta-1} \ll \log^{-A}X. }

Therefore the current log-accurate short-interval residual theorem is fully compatible with every fixed power drift xβx^\beta with β<1\beta<1.

Create:

O-RH-061
LOG_LOCAL_RESIDUAL_BLIND_TO_FIXED_POWER_DRIFT
status:
  CERTIFIED AS STRENGTH AUDIT

12. Why the bilinear route is drift-sensitive

Although a local residual increment theorem does not detect xβx^\beta, the residual PESC does.

For a smooth cumulative mode

F(x)xβ,F(x)\asymp x^\beta,

its increment is

fnβnβ1,f_n \asymp \beta n^{\beta-1},

and the bilinear product has scale

fnF(n)n2β1.f_nF(n) \asymp n^{2\beta-1}.

After the endpoint weight contributes one factor NN and the nn -sum another scale factor, the residual self-correlation has natural exponent

N2β+1.\boxed{ N^{2\beta+1}. }

Thus a PESC bound

N3κN^{3-\kappa}

is incompatible at exponent scale with

β>1κ2.\beta > 1-\frac{\kappa}{2}.

This matches the certified Mellin-pole strip law.

The bilinear root target is therefore genuinely sensitive to the smooth drift that current local residual uniformity ignores.


13. Campaign 27 track audit

P2-1 — signed prime sampling with drift subtraction

status:
  LAMBDA-SHARP DRIFT SUBTRACTION TOO SMALL

reason:
  model primitive X^{o(1)}

P2-2 — PESC after sieve-model subtraction

status:
  EXACT FIXED-EXPONENT EQUIVALENCE

result:
  B-RH-004

P2-3 — bilinear residual/model cross term

status:
  HARMLESS O(N^2 X^{o(1)})

critical term:
  residual self-correlation

P2-4 — scale-coupled signed recurrence

status:
  NO NEW FIXED-GAP RECURRENCE FOUND

existing cumulative-contraction criterion remains

P2-5 — direct arithmetic drift exclusion

status:
  CURRENT LOCAL RESIDUAL THEOREMS BLIND TO FIXED DRIFT

new bilinear arithmetic theorem:
  still needed

14. Direct PESC branch verdict

The sieve-model subtraction does not create a weaker target.

Instead it clarifies the root obstruction:

PESCis essentially the self-energy off=ΛΛ\boxed{ \text{PESC} \quad\text{is essentially the self-energy of} \quad f=\Lambda-\Lambda^\sharp }

because the structured model has negligible primitive at polynomial scale.

Therefore:

model terms:
  harmless

model/residual cross terms:
  harmless

residual self-energy:
  PESC-equivalent

This is the shortest bilinear closure obtained so far.


15. No new frontier

Campaign 27 does not create another canonical frontier.

The canonical target remains:

F-RH-010
PESC

The direct theorem candidate remains:

F-RH-016
MLEPG

The residual formulation is a certified equivalent first-strip representation, not a new target.


16. Campaign 28

The next campaign is:

CSM_RH Campaign 28
ENDOGENOUS_DRIFT_COERCIVITY_ATTACK

The problem is now intentionally narrow:

find a genuinely prime-arithmetic bilinear theorem which prevents the residual primitive F=(ΛΛ)F=\sum(\Lambda-\Lambda^\sharp) from carrying a persistent polynomial smooth drift.


17. Campaign 28 tracks

E1 — residual prime-sampling coercivity

Use the fact that f=ΛΛf=\Lambda-\Lambda^\sharp is not an arbitrary derivative.

Test whether

nwN(n)fnF(n1)\sum_n w_N(n)f_nF(n-1)

has a sign/coercivity property after subtracting explicit sieve-model terms.

E2 — Selberg symmetry on the residual primitive

Insert

Λ=Λ+f\Lambda=\Lambda^\sharp+f

into the prime-only Selberg symmetry formula.

Keep the periodic model exact and isolate a bilinear identity involving FF.

Reject the route if the resulting forcing remains only O(X)O(X) and is compatible with every fixed power drift.

E3 — multiplicative sampling of a smooth residual drift

Assume

F(x)cxβF(x)\approx cx^\beta

on one dyadic scale and compute how the prime/multiplicative sampling identities respond.

Seek a contradiction requiring less than a full fixed-power PNT theorem.

E4 — two-scale signed residual energy

Relate residual PESC at NN and 2N2N directly.

A valid candidate must generate fixed contraction mass without passing through a positive variance frontier.

E5 — canonical drift projection with arithmetic remainder

Define a canonical low-frequency projection of FF and prove that the residual prime arithmetic contracts the projected coefficient.

The projection may depend on scale but must not use the unknown zero set or assume the desired PNT bound.


18. Campaign 28 rejection filters

Reject a candidate if:

R1. The model primitive is subpolynomial and the argument merely subtracts it again.

R2. The new statement is residual PESC under another name.

R3. It uses only the current local bound HlogAXH\log^{-A}X.

R4. It assumes a fixed zero-free strip.

R5. It uses a generic smoothness principle valid for arbitrary sequences.

R6. It creates a positive higher-moment surrogate.


19. External calibration

The modern approximant used here is

Λ(n)=P(R)φ(P(R))1(n,P(R))=1,R=exp((logX)1/10),\Lambda^\sharp(n) = \frac{P(R)}{\varphi(P(R))} 1_{(n,P(R))=1}, \qquad R=\exp((\log X)^{1/10}),

and current almost-all short-interval residual bounds are of arbitrary logarithmic accuracy in the prime case.

These are the correct contemporary inputs for the present sieve-subtraction audit.


20. State transition

CSM_RH v1.18
  ->
CSM_RH v1.19

with:

Campaign 27
  CLOSED_AS_DIRECT_SIEVE_MODEL_PESC_AUDIT

B-RH-004
  SIEVE_RESIDUAL_PESC_EQUIVALENCE
  CREATED / CERTIFIED

O-RH-060
  BOUNDED_PRIMITIVE_APPROXIMANT_NEUTRALITY
  CREATED / CERTIFIED FOR LAMBDA-SHARP

O-RH-061
  LOG_LOCAL_RESIDUAL_BLIND_TO_FIXED_POWER_DRIFT
  CREATED / CERTIFIED AS STRENGTH AUDIT

F-RH-010
  PESC
  REMAINS OPEN / ROOT TARGET

F-RH-016
  MLEPG
  REMAINS OPEN

Campaign 28
  ENDOGENOUS_DRIFT_COERCIVITY_ATTACK
  READY

21. Final status

RH = OPEN

PESC = OPEN

MLEPG = OPEN

LAMBDA-SHARP SUBTRACTION = FIXED-EXPONENT NEUTRAL

MODEL PRIMITIVE = X^{o(1)}

RESIDUAL PRIMITIVE = CARRIES THE PESC-HARD DRIFT

CURRENT LOCAL RESIDUAL THEOREM = LOG-ACCURATE BUT DRIFT-BLIND

RESIDUAL SELF-CORRELATION = PESC-EQUIVALENT

NEXT CAMPAIGN = 28

The decisive identity is

Ca(N)=Cf(N)+O(N2Xo(1)).\boxed{ \mathcal C_a(N) = \mathcal C_f(N) + O(N^2X^{o(1)}). }

For first-strip exponents, the modern sieve model changes the local structure but not the global fixed-power difficulty.