novelty-meter.md
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The novelty meter
- 2026-09-21 [Proved] Backward, elementarily:
S_fvanishes fory > 2, soF(s) zeta(s-1)/zeta(s) = (6/pi^2) F(2) 2^(s-2)/(s-2) + int_0^2 E_f(y) y^(s-3) dy, andE_f = O(y^(3/2 - eps))continues the right side toRe s > 1/2 + eps; a zerorhothere needsF(rho) zeta(rho - 1) = 0, impossible sincezeta(rho - 1) != 0forRe(rho - 1)in(-1/2, 0)andF(rho + k) != 0for somek, elsef(u) u^(rho - 1)is orthogonal to every polynomial on[1, 2]andf = 0by Weierstrass, withu^k f(u)again a bump; so the smoothed novelty rate for all bumps implies RH, and the meter is an equivalence as hard as RH, not a route. Witness: stack.md, The novelty meter. - 2026-09-21 [Proved] The indicator's
1/2is a sharp-cutoff artefact:sum_(n <= x) phi(n) - 3x^2/pi^2isO(x log x)by the Mobius routesum_d mu(d) T(floor(x/d))andOmega(x)because it jumps byphi(p) = p - 1at every prime, so the indicator meter sits at exponent1iny,1/2inq, unconditionally and sharply, above they^(3/2)of the zeros, and says nothing about zeros; the jump between consecutive integers readsphi(p) - 3(2p - 1)/pi^2,392073.4atp = 1000003and3920735.7atp = 10000019. Witness: lab/py/smoothed-noveltymain, SHARP CUTOFF. - 2026-09-21 [Refuted] The smoothed novelty meter as a route to RH on this tree: on any finite range the smoothed error is a rendering of the first zeros, the bump's Mellin transform killing high zeros faster than any power, so a zero off the line at any height where RH is already checked is invisible here; the meter can neither certify nor refute the hypothesis. Witness: lab/py/smoothed-novelty
main, the 138-zero agreement at2.0e-06. - 2026-09-21 [Verified] Read at source, Verjovsky, Kodai Math. J. 17 (1994) 596-608: with
m_q(f) = q sum_n phi(n) f(q^(1/2) n)andm_0(f) = (6/pi^2) int_0^infty u f(u) du, Theorem A givesm_q(f) = m_0(f) + O(q^(1/2) log q)for continuous compactly supportedfon(0, infinity); Theorem B part 1, RH iffm_q(f) = m_0(f) + o(q^(3/4 - eps))for everyf in C_c^r,2 <= r <= infinity, and everyeps > 0; part 2, foralpha in (1/2, 3/4)the erroro(q^(alpha - eps))for allf in C_c^2iffzetahas no zero inRe s > 2(1 - alpha); part 3, for the characteristic function of an intervallimsup q^-alpha abs(m_q(f) - m_0(f)) = infinityfor everyalpha > 1/2; arXiv:1711.03593 Theorem 5.1 restates the smooth case iny = q^(1/2)aso(y)ando(y^(3/2 - eps))and refers its proof to the Kodai article. Witness: doi:10.2996/kmj/1138040054 p. 597 and arXiv:1711.03593 Appendix B. - 2026-09-21 [Proved] The Mellin identity
sum_n phi(n) f(ny) = (1/(2 pi i)) int_(Re s = c) F(s) zeta(s-1)/zeta(s) y^-s dsforc > 2andfa bump on[1, 2], with main term(6/pi^2) F(2) y^-2from the pole ofzeta(s-1)ats = 2; under RH and with1/zeta(s) << abs(t)^deltauniformly onRe s >= 1/2 + eps, the input the Gaussian Franel study reads at source atK = Q, the errorE_f(y) = y^2 S_f(y) - (6/pi^2) F(2)isO(y^(3/2 - eps))forf in C^2. Witness: stack.md, The novelty meter, assembled from the Mellin transform; lab/py/smoothed-noveltymellin_c2printsF(2) = 24/35beside the closed form. - 2026-09-21 [Verified] On
y = 2^-j,jfrom 8 to 23.5 in steps of1/16,phisieved to3 * 10^7, the slope inq = y^2of the per-octave root mean square ofE_freads0.5023for the indicator of[1, 2](lower and upper eight octaves0.5296and0.4883),0.7498for theC^2bump64 (u-1)^3 (2-u)^3(windows0.7553and0.7487),0.7471for theC^infinitybumpexp(4 - 1/((u-1)(2-u)))(windows0.7474and0.7460), window residuals0.065to0.169and full-range residuals0.179,0.092,0.115, no window pair differing by more than0.05; the sieve agrees with brute-force gcd counts to 2000 and with the Mobius route atx = 10^6, and the summation noise atj = 23.5is5.6e-17againstabs(E_f) = 5.4e-12. Witness: lab/py/smoothed-noveltyslopes,totients,totient_sum_mobius. - 2026-09-21 [Proved] Under RH, for smooth
f,E_f(y) = sum_rho F(rho) (zeta(rho - 1)/zeta'(rho)) y^(2 - rho) + O(y^(3/2 + delta)), the sum over nontrivial zeros as residues through the cited heights, written for simple zeros; each term has modulusabs(c_rho) y^(2 - Re rho), so the exponent inqis1 - beta/2at a zero of real partbeta,3/4on the line and smaller at the zero of a pair that sits right of it. Witness: stack.md, The novelty meter, by the contour shift toRe s = 1/2 - delta. - 2026-09-21 [Verified] The residue sum over the first 138 zeros (height 300,
zeta(rho - 1)andzeta'(rho)from PARI) reproduces the measuredE_fof theC^infinitybump over the whole grid to a relative2.0e-06(one zero0.50, ten2.7e-02, thirty2.0e-03), coefficients1.879e-01at the first zero to1.475e-07at the 138th; for theC^2bump the coefficients fall likegamma^-3.22on the 138, itsFbeingO(abs(s)^-4),1.386e-01to6.541e-06, and the truncation stops at2.3e-04;abs(E_f)/y^(3/2)lies in[1.3e-04, 0.558]for theC^infinitybump against2 sum abs(c_rho) = 0.755over the same 138 zeros. Witness: lab/py/smoothed-noveltymain,zeros_from_pari,mellin_cinf. - 2026-09-21 [Verified] Cross-reference to the slopes row: the per-octave method reads "the samples with
jin[k, k+1), 16 of them except the 9 of the last octave[23, 23.5], placed atj = k + 1/2"; the printed slopes are unchanged. Witness: lab/py/smoothed-noveltyslopes,octave_rms. - 2026-09-21 [Verified] Cross-reference to the 138-zero row:
gamma^-3.22is now printed by the generator as the least-squares power ofabs(c_rho)againstgammaon the 138 zeros,-3.22for theC^2bump. Witness: lab/py/smoothed-noveltymain, EXPLICIT FORMULA.