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CSM_RH Paper 30 — Fixed-Order Selberg Exponent Invariance and the Growing-Order Complexity Threshold

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CSM_RH Paper 30

Fixed-Order Selberg Exponent Invariance and the Growing-Order Complexity Threshold

Project: CSM_RH
Paper: 30
Version: v0.1
Date: 2026-09-07
Parent state: CSM_RH v1.20 / Paper 29
Campaign: 29 — HIGHER_ORDER_SELBERG_AMPLIFIER_ATTACK
Status: generalized-von-Mangoldt amplifier audit; 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

Paper 29 showed that the classical fixed-order Selberg feedback is forcing-critical for every fixed Mellin mode xρx^\rho with ρ<1\Re\rho<1.

Campaign 29 tests whether generalized von Mangoldt functions

Λk=μlogk\Lambda_k = \mu*\log^k

can amplify this feedback into a fixed polynomial drift gap.

The result is:

fixed k:
  exponent-neutral

finite fixed-order combinations:
  no certified remainder cancellation

slowly growing k:
  can amplify logarithmic/subpower precision

fixed-power critical order:
  k ~ log X / log log X

at that order:
  pointwise/combinatorial complexity becomes polynomial in X

current fixed-k theorems:
  not uniform enough to cross the critical order

Higher-order Selberg methods are genuine amplifiers, but the audited theory supplies a subpower amplifier rather than a certified fixed-power amplifier.


1. Generalized von Mangoldt functions

For an integer

k1,k\ge1,

define

Λk(n)=dnμ(d)(lognd)k.\boxed{ \Lambda_k(n) = \sum_{d\mid n} \mu(d) \left( \log\frac nd \right)^k. }

Equivalently,

Λk=μlogk.\boxed{ \Lambda_k = \mu*\log^k. }

The Dirichlet series is

n1Λk(n)ns=(1)kζ(k)(s)ζ(s),s>1.\boxed{ \sum_{n\ge1} \frac{\Lambda_k(n)}{n^s} = (-1)^k \frac{\zeta^{(k)}(s)}{\zeta(s)}, \qquad \Re s>1. }

Also,

Λk+1=Λklog+ΛΛk.\boxed{ \Lambda_{k+1} = \Lambda_k\log + \Lambda*\Lambda_k. }

The function is nonnegative and supported on integers with at most kk distinct prime factors.

At a prime,

Λk(p)=(logp)k.\boxed{ \Lambda_k(p) = (\log p)^k. }

2. Fixed-k summatory polynomial

For each fixed

k1,k\ge1,

there exists a polynomial RkR_k of degree k1k-1 with leading term

ktk1k t^{k-1}

such that

Theorem 2.1 — Fixed-Order Generalized Selberg Summatory Formula

nxΛk(n)=xRk(logx)+Ok(x).\boxed{ \sum_{n\le x}\Lambda_k(n) = xR_k(\log x) + O_k(x). }

Equivalently, retaining only the leading term,

nxΛk(n)=kx(logx)k1+Ok(x(logx)k2).\boxed{ \sum_{n\le x}\Lambda_k(n) = kx(\log x)^{k-1} + O_k \left( x(\log x)^{k-2} \right). }

For k=2k=2, this contains the classical Selberg symmetry formula.

For k2k\ge2, the almost-prime observable is much smoother than the prime observable itself.


3. Complete polynomial subtraction

Define

Ek(x)=nxΛk(n)xRk(logx).\boxed{ E_k(x) = \sum_{n\le x}\Lambda_k(n) - xR_k(\log x). }

Theorem 2.1 gives

Ek(x)=Ok(x).\boxed{ E_k(x) = O_k(x). }

Normalize by the natural leading scale:

E~k(x)=Ek(x)x(logx)k1.\widetilde E_k(x) = \frac{ E_k(x) }{ x(\log x)^{k-1} }.

Then for fixed kk,

E~k(x)=Ok((logx)(k1)).\boxed{ \widetilde E_k(x) = O_k \left( (\log x)^{-(k-1)} \right). }

Thus increasing a fixed order can manufacture arbitrarily high fixed logarithmic precision.

It does not yet manufacture a power of xx.


4. Fixed-zero response of Lambda-k

Let ρ\rho be a simple nontrivial zero of ζ\zeta.

Near

s=ρ,s=\rho,

write

ζ(s)=ζ(ρ)(sρ)+O((sρ)2).\zeta(s) = \zeta'(\rho)(s-\rho) + O \left( (s-\rho)^2 \right).

Then

(1)kζ(k)(s)ζ(s)(-1)^k \frac{\zeta^{(k)}(s)}{\zeta(s)}

either:

  1. has a simple pole at ρ\rho, with residue(1)kζ(k)(ρ)ζ(ρ),\boxed{ (-1)^k \frac{ \zeta^{(k)}(\rho) }{ \zeta'(\rho) }, } if ζ(k)(ρ)0\zeta^{(k)}(\rho)\ne0 ;

or

  1. has the pole cancelled because the numerator also vanishes there.

Therefore:

Theorem 4.1 — Fixed-Order Zero-Exponent Invariance

Whenever the generalized detector sees the zero ρ\rho, its explicit-formula contribution has exponent

xρ.\boxed{ x^\rho. }

Changing fixed kk changes the coefficient, not the real exponent.

If the numerator cancels the pole, the detector becomes less sensitive to that particular zero rather than more coercive.

Create:

O-RH-064
FIXED_ORDER_GENERALIZED_SELBERG_ZERO_EXPONENT_INVARIANCE
status:
  CERTIFIED AS STRENGTH AUDIT

5. Fixed-k forcing versus fixed Mellin mode

For a fixed zero or hypothetical Mellin drift with

ρ=β<1,\Re\rho=\beta<1,

the generalized detector has mode scale

Ok,ρ(xβ)O_{k,\rho}(x^\beta)

whenever the pole survives.

The unconditional complete-model remainder is

Ok(x).O_k(x).

Hence

xβ=o(x).\boxed{ x^\beta = o(x). }

After normalization by x(logx)k1x(\log x)^{k-1}:

forcing

Ok((logx)(k1))\boxed{ O_k \left( (\log x)^{-(k-1)} \right) }

zero/drift mode

Ok,ρ(xβ1(logx)(k1)).\boxed{ O_{k,\rho} \left( x^{\beta-1} (\log x)^{-(k-1)} \right). }

Their ratio is

xβ1.\boxed{ x^{\beta-1}. }

It is independent of kk at exponent level.

Thus fixed-order amplification sharpens the logarithmic normalization while leaving the fixed Mellin mode buried inside the Ok(x)O_k(x) forcing.


6. Finite fixed-order linear combinations

Let KK be fixed and consider

LK(s)=k=1Kck(1)kζ(k)(s)ζ(s).\boxed{ \mathcal L_K(s) = \frac{ \sum_{k=1}^{K} c_k(-1)^k\zeta^{(k)}(s) }{ \zeta(s) }. }

At a simple zero ρ\rho, if

k=1Kck(1)kζ(k)(ρ)0,\sum_{k=1}^{K} c_k(-1)^k \zeta^{(k)}(\rho) \ne0,

then LK\mathcal L_K still has a simple pole at ρ\rho.

Hence the associated zero contribution still has exponent xρx^\rho.

If the numerator vanishes, the filter misses that zero.

Therefore a fixed-order differential filter cannot move a surviving zero mode to a better exponent.

It can only alter or remove its residue.


7. Main-term cancellation does not cancel unknown remainders

For fixed KK, known polynomial main terms

xRk(logx)xR_k(\log x)

can be combined exactly.

But the current unconditional statements provide separate errors

Ek(x)=Ok(x).E_k(x)=O_k(x).

A finite linear combination gives only

kKckEk(x)=OK(xkKck)\boxed{ \sum_{k\le K}c_kE_k(x) = O_K \left( x\sum_{k\le K}|c_k| \right) }

without additional joint information.

One cannot use cancellation among independent big- OO errors as theorem authority.

Create:

O-RH-065
FIXED_ORDER_REMAINDER_NONCOHERENCE
status:
  CERTIFIED AS CURRENT-THEOREM AUDIT

This does not say that the true remainders never cancel.

It says that current fixed-order summatory formulae do not certify such cancellation.


8. Historical calibration: higher weight really does amplify

Higher-weight Selberg/Bombieri/Wirsing methods are not useless.

Historically, elementary methods were strengthened from the original PNT to error terms of the form

ψ(x)x=OA(x(logx)A)\boxed{ \psi(x)-x = O_A \left( x(\log x)^{-A} \right) }

for every fixed A>0A>0.

Later Diamond–Steinig-type methods obtained stretched-exponential subpower remainders of the form

xexp(c(logx)θ)\boxed{ x \exp \left( -c(\log x)^\theta \right) }

for fixed θ>0\theta>0 in the known elementary range.

Thus higher weighting and recursion can increase cumulative amplification beyond every fixed logarithmic power.

But these estimates remain

x1o(1),\boxed{ x^{1-o(1)}, }

not x1δx^{1-\delta}.

This is consistent with the CSM_RH subpower / fixed-power distinction.


9. Critical growing order

Suppose one tries to turn a formal logarithmic factor

(logX)k(\log X)^{-k}

into a fixed power

Xδ.X^{-\delta}.

The balance equation is

kloglogXδlogX.k\log\log X \sim \delta\log X.

Therefore the critical order is

Theorem 9.1 — Fixed-Power Order Scale

kcritδlogXloglogX.\boxed{ k_{\mathrm{crit}} \asymp \delta \frac{ \log X }{ \log\log X }. }

Any order satisfying

k=o(logXloglogX)k = o \left( \frac{\log X}{\log\log X} \right)

can generate at most a subpower factor from powers of logX\log X.


10. Pointwise weight complexity at the critical order

At a prime,

Λk(p)=(logp)k.\Lambda_k(p) = (\log p)^k.

At

k=clogXloglogX,k = c \frac{\log X}{\log\log X},

we have

(logX)k=Xc+o(1).\boxed{ (\log X)^k = X^{c+o(1)}. }

Thus the generalized detector itself acquires polynomial-size spikes exactly when the formal logarithmic amplifier enters fixed-power territory.

The pointwise bound

0Λk(n)(logn)k0\le\Lambda_k(n)\le(\log n)^k

therefore ceases to be exponent-neutral.


11. Factorial proof-complexity scale

The elementary fixed- kk summatory argument expands powers of logarithms and integrates expressions of the form

logky.\log^k y.

The natural coefficient scale includes factorial-size quantities.

Stirling gives

log(k!)=klogkk+O(logk).\boxed{ \log(k!) = k\log k-k+O(\log k). }

At the critical order

k=clogXloglogX,k = c \frac{\log X}{\log\log X},

one gets

k!=Xc+o(1).\boxed{ k! = X^{c+o(1)}. }

Therefore any factorial-type dependence hidden inside the fixed- kk constant Ok(1)O_k(1) becomes polynomial in XX at exactly the order required for fixed-power amplification.

The existing theorem

Ek(x)=Ok(x)E_k(x)=O_k(x)

is stated for fixed kk and provides no uniform control capable of excluding this exponent cost.

Create:

O-RH-066
GROWING_ORDER_FACTORIAL_COMPLEXITY_THRESHOLD
status:
  CERTIFIED AS CURRENT-METHOD UNIFORMITY BARRIER

The statement is not that every possible proof must lose k!k!.

It is that the current fixed- kk theorem contains no uniformity strong enough to cross the critical order, and factorial-scale dependence is already exponent-critical there.


12. Support complexity at large order

The generalized function Λk\Lambda_k is supported on integers with at most kk distinct prime factors.

For fixed kk, this is a strong smoothing from primes to bounded-order almost primes.

At

klogXloglogX,k \asymp \frac{\log X}{\log\log X},

the allowed number of distinct prime factors is far larger than the typical order loglogX\log\log X.

Thus the support restriction becomes weak for typical integers.

This is a qualitative warning:

small fixed k:
  strong almost-prime smoothing

critical growing k:
  broad support, large weights

The very mechanism that smooths the prime problem at fixed order becomes less selective when the order approaches fixed-power scale.


13. Growing-order verdict

There are three regimes.

Regime I — fixed k

k=O(1).k=O(1).

Result:

arbitrary fixed log powers possible;
fixed zero exponent unchanged;
fixed-power coercivity absent.

Regime II — subcritical growing k

k=o(logXloglogX).k = o \left( \frac{\log X}{\log\log X} \right).

Formal log amplification remains

Xo(1).X^{-o(1)}.

This is compatible with stretched-exponential/subpower error improvements.

Regime III — critical order

klogXloglogX.k \asymp \frac{\log X}{\log\log X}.

Formal amplification can become a fixed power.

But:

pointwise weights:
  polynomial in X

factorial-type constants:
  polynomial in X

fixed-k summatory theorem:
  no authorized uniformity

almost-prime support:
  substantially less selective

No certified net fixed power is obtained.


14. Campaign 29 track audit

H1 — fixed-k generalized Selberg response

status:
  CLOSED

zero exponent:
  invariant

forcing:
  O_k(x)

H2 — finite linear-combination forcing cancellation

status:
  NO CERTIFIED CANCELLATION OF O_k(x) REMAINDERS

fixed-zero exponent:
  unchanged if pole survives

H3 — growing-k amplification

status:
  SUBCRITICAL -> SUBPOWER

critical order:
  complexity/uniformity barrier

H4 — generalized almost-prime to PESC transfer

status:
  NO LOWER-STRENGTH FIXED-POWER TRANSFER FOUND

H5 — spectral polynomial in Selberg operator

status:
  FIXED ORDER CHANGES RESIDUES, NOT ZERO EXPONENTS

no coercive filter found

15. Campaign 29 verdict

No fixed-power theorem is proved.

The higher-order Selberg route is classified as:

real amplifier:
  YES

arbitrary fixed log-power:
  YES

subpower / stretched-log potential:
  YES

certified fixed-power:
  NO

fixed-order route:
  CLOSED AS EXPONENT-NEUTRAL

growing-order route:
  OPEN IN PRINCIPLE BUT CURRENTLY UNAUTHORIZED AT CRITICAL ORDER

The root target remains PESC.


16. New certified obstruction package

Create:

O-RH-064
FIXED_ORDER_GENERALIZED_SELBERG_ZERO_EXPONENT_INVARIANCE
CERTIFIED

O-RH-065
FIXED_ORDER_REMAINDER_NONCOHERENCE
CERTIFIED AS CURRENT-THEOREM AUDIT

O-RH-066
GROWING_ORDER_FACTORIAL_COMPLEXITY_THRESHOLD
CERTIFIED AS CURRENT-METHOD UNIFORMITY BARRIER

No new frontier is created.


17. Return to the arithmetic root

The generalized Selberg shell has now been audited at:

order 2;
fixed higher order;
finite fixed-order combinations;
subcritical growing order;
critical growing-order exponent budget.

No lower-strength fixed-power bridge is found.

Therefore CSM_RH returns again to:

F-RH-010
PESC

with no additional surrogate.


18. Campaign 30

The next campaign is:

CSM_RH Campaign 30
PARITY_SENSITIVE_PESC_ATTACK

The goal is not to introduce another almost-prime smoothing layer.

It is to identify arithmetic information that distinguishes the true prime residual from the family of generalized almost-prime models.


19. Campaign 30 tracks

Q1 — PESC parity decomposition

Decompose the residual prime detector according to Liouville/Möbius parity information while preserving the signed endogenous primitive.

The target must remain bilinear.

Q2 — asymptotic-sieve scalar defect

Use the Bombieri asymptotic-sieve perspective: higher generalized von Mangoldt information leaves a parity-sensitive scalar undetermined.

Identify the analogue of that undetermined scalar inside PESC.

Q3 — parity-breaking bilinear input

Revisit Friedlander–Iwaniec-type parity-breaking hypotheses, but require a direct bilinear bridge to PESC rather than EMBF/PACPSA surrogate proliferation.

Q4 — prime-versus-almost-prime drift comparator

Construct an observable whose value on Λ\Lambda differs at fixed exponent from every bounded-order generalized almost-prime model.

Q5 — direct residual sign structure

Search for a prime-specific signed identity involving f=ΛΛf=\Lambda-\Lambda^\sharp that is not shared by Λk\Lambda_k for k2k\ge2.


20. Campaign 30 rejection filters

Reject a candidate if:

R1. It only introduces another Λk\Lambda_k or almost-prime average.

R2. It reproduces EMBF/EMDQO without a direct PESC bridge.

R3. It uses parity-breaking as a slogan without an exponent ledger.

R4. It obtains only logarithmic/subpower precision.

R5. It assumes a fixed zero strip.

R6. It creates another positive higher-moment target.


21. External calibration

Current/classical calibration:

  1. For fixed kk, $$ \sum_{n\le x}\Lambda_k(n)

    xR_k(\log x)+O_k(x), $$ with RkR_k of degree k1k-1 and leading term k(logx)k1k(\log x)^{k-1}.

  2. The generalized von Mangoldt functions satisfy $$ \Lambda_{k+1}

    \Lambda_k\log

    \Lambda*\Lambda_k. $$

  3. Higher-weight elementary methods historically improve the PNT remainder through arbitrary logarithmic powers and stretched-exponential subpower scales.

  4. Bombieri's asymptotic-sieve perspective shows that very rich higher-almost-prime information can still leave the prime/parity component undetermined.

These facts motivate the next parity-sensitive return to PESC.


22. State transition

CSM_RH v1.20
  ->
CSM_RH v1.21

with:

Campaign 29
  CLOSED_AS_HIGHER_ORDER_SELBERG_AMPLIFIER_AUDIT

O-RH-064
  CREATED / CERTIFIED

O-RH-065
  CREATED / CERTIFIED AS CURRENT-THEOREM AUDIT

O-RH-066
  CREATED / CERTIFIED AS CURRENT-METHOD UNIFORMITY BARRIER

F-RH-010
  PESC
  REMAINS OPEN / ROOT TARGET

F-RH-016
  MLEPG
  REMAINS OPEN

Campaign 30
  PARITY_SENSITIVE_PESC_ATTACK
  READY

23. Final status

RH = OPEN

PESC = OPEN

MLEPG = OPEN

FIXED-ORDER HIGHER SELBERG = EXPONENT-NEUTRAL

FINITE FIXED-ORDER FILTER = NO CERTIFIED REMAINDER CANCELLATION

SUBCRITICAL GROWING ORDER = SUBPOWER

FIXED-POWER CRITICAL ORDER = log X / log log X

CURRENT UNIFORMITY AT CRITICAL ORDER = INSUFFICIENT

HIGHER SELBERG = REAL SUBPOWER AMPLIFIER, NOT CERTIFIED FIXED-POWER AMPLIFIER

NEXT CAMPAIGN = 30

The central scale law is

(logX)k=XδkδlogXloglogX.\boxed{ (\log X)^{-k} = X^{-\delta} \quad\Longleftrightarrow\quad k \sim \delta \frac{\log X}{\log\log X}. }

At precisely this order,

(logX)k=Xδ+o(1)\boxed{ (\log X)^k = X^{\delta+o(1)} }

and factorial-type kk -dependence also enters polynomial exponent scale.

The current fixed- kk generalized Selberg theory does not provide a certified net fixed power across this threshold.