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Hyperbolic Bias and the Geometric Exclusion of Riemann Zeta Zeros
Chee Kian Yap
Posted: 24 April 2026
Various New Properties for Central Bell-Based Type 2 Bernoulli Polynomials of Order β
Ugur Duran
Posted: 24 April 2026
On k−Unitary Perfect Polynomials over F2
Wiam Zeid
,Haissam Chehade
,Issam Kaddoura
,Yahia Awad
Posted: 22 April 2026
The De Bruijn-Newman Constant Is Zero
Avi Gershon
Posted: 22 April 2026
Pólya-Ostrowski Groups and Unit Indices in Real Biquadratic Fields
Huda Naeem Hleeb Al-Jabbari
,Abbas Maarefparvar
Posted: 21 April 2026
Asymptotic Hyperbolicity of Jensen Polynomials and the Finite-Strip Obstruction for the Riemann Hypothesis
Michel Planat
We study the degree-d Jensen polynomials \( J_{d,n}(X) \) built from the moment sequence \( M_n=\int_0^\infty\Phi_1(u)u^{2n}\,du \) of the Riemann \( \Xi \)-function, which coincides with the classical Pólya–Jensen family. Using bridge coordinates, the staircase law, and Plancherel–Rotach asymptotics, we prove that \( J_{d,n}^\gamma \) is hyperbolic for all \( n\ge C_0^\infty d^4 \) (\( C_0^\infty\approx0.020 \); the analytic formula for \( C_0^\infty \) is rigorous but approximates the numerically observed value to within 2.6%); combined with the GORZ theorem for \( d\le8 \), this covers the entire asymptotic regime. We identify a phase-transition law \( n^*(d)=C_0^\infty d^4+\alpha d^3+\beta(-1)^d d^2+O(d) \) (Conjecture 3.5): the leading constant \( C_0^\infty\approx0.0195 \) is computed analytically and verified to within 2.6% of the empirical large-$d$ limit; the formula for \( \alpha \) is derived; its numerical value ≈ −0.2 to −0.3 is numerical evidence; the parity structure \( \beta(-1)^d d^2 \) is proved. For the finite strip \( 0\le n \) < \( C_0^\infty d^4 \) with \( d\ge9 \), the sole remaining gap, whose closure is equivalent to the Riemann Hypothesis under standard transversality, we establish four structural obstructions: ratio-barrier saturation (no usable margin, certified and numerical); frozen zero count (parity blocks any ladder, certified for \( d\le21 \)); interlacing-lift vacuity (proved); and a discriminant equivalence (proved under transversality), showing that all known local and inductive mechanisms fail simultaneously in this region. The problem reduces to: \( \operatorname{Disc}(J_{d,n}^\gamma)>0 \) for all \( d\ge9 \) and 0 ≤ n < \( C_0^\infty d^4 \); this requires moment data \( M_k \) for \( k\ge130 \), currently inaccessible.
We study the degree-d Jensen polynomials \( J_{d,n}(X) \) built from the moment sequence \( M_n=\int_0^\infty\Phi_1(u)u^{2n}\,du \) of the Riemann \( \Xi \)-function, which coincides with the classical Pólya–Jensen family. Using bridge coordinates, the staircase law, and Plancherel–Rotach asymptotics, we prove that \( J_{d,n}^\gamma \) is hyperbolic for all \( n\ge C_0^\infty d^4 \) (\( C_0^\infty\approx0.020 \); the analytic formula for \( C_0^\infty \) is rigorous but approximates the numerically observed value to within 2.6%); combined with the GORZ theorem for \( d\le8 \), this covers the entire asymptotic regime. We identify a phase-transition law \( n^*(d)=C_0^\infty d^4+\alpha d^3+\beta(-1)^d d^2+O(d) \) (Conjecture 3.5): the leading constant \( C_0^\infty\approx0.0195 \) is computed analytically and verified to within 2.6% of the empirical large-$d$ limit; the formula for \( \alpha \) is derived; its numerical value ≈ −0.2 to −0.3 is numerical evidence; the parity structure \( \beta(-1)^d d^2 \) is proved. For the finite strip \( 0\le n \) < \( C_0^\infty d^4 \) with \( d\ge9 \), the sole remaining gap, whose closure is equivalent to the Riemann Hypothesis under standard transversality, we establish four structural obstructions: ratio-barrier saturation (no usable margin, certified and numerical); frozen zero count (parity blocks any ladder, certified for \( d\le21 \)); interlacing-lift vacuity (proved); and a discriminant equivalence (proved under transversality), showing that all known local and inductive mechanisms fail simultaneously in this region. The problem reduces to: \( \operatorname{Disc}(J_{d,n}^\gamma)>0 \) for all \( d\ge9 \) and 0 ≤ n < \( C_0^\infty d^4 \); this requires moment data \( M_k \) for \( k\ge130 \), currently inaccessible.
Posted: 20 April 2026
From Chebyshev to Primorials: Establishing the Riemann Hypothesis
Frank Vega
Posted: 15 April 2026
Attack on the Riemann Hypothesis II
Huan Xiao
Posted: 15 April 2026
Geometric Insights into the Goldbach Conjecture
Frank Vega
Posted: 15 April 2026
On S-2 Prime Hyperideals of Commutative Hyperrings
Elif Tuysuz
,Gürsel Yeşilot
,Serkan Onar
,Sanem Yavuz
Posted: 15 April 2026
Attack on the Riemann Hypothesis
Huan Xiao
Posted: 15 April 2026
On Weakly S-Prime Hyperideals of Multiplicative Hyperrings
Elif Basak Turkoglu
,Gursel Yesilot
,Serkan Onar
,Sanem Yavuz
Posted: 14 April 2026
Wilf's Conjecture from the First Kunz Layer
Yaoran Yang
,Yutong Zhang
Posted: 08 April 2026
The Twin Prime Formula and the Infinitude of Twin Primes
Michael M. Anthony
Posted: 06 April 2026
The DNA of the Harmonized Sophie Germain and Twin Primes
Jan Feliksiak
,Monica U. Feliksiak
Posted: 06 April 2026
On the Log-Concavity of the Riemann Xi Kernel
Avi Gershon
Posted: 02 April 2026
On Series Involving Cubed Catalan Numbers
Kunle Adegoke
Posted: 02 April 2026
A Unified Proof of the Extended, Generalized, and Grand Riemann Hypothesis Based on the General Properties of L-Functions
Weicun Zhang
Posted: 01 April 2026
Finite Field Hudzik-Landes-Dragomir-Kato-Saito-Tamura Inequality
K. Mahesh Krishna
Posted: 01 April 2026
Finite Field Tarski-Maligranda Inequalities
K. Mahesh Krishna
Posted: 31 March 2026
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