Wave Interference and Constructive Resonance in Mersenne Number Distribution: A High-Precision Heuristic for Prime Exponent Localization.

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Authors: José Manuel Briceño Mendoza
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Abstract

I. The Resonance Core (The Transcendental Phase) At the heart of the algorithm lies the argument of the sine function. We calculate a transcendental phase ($\theta$) defined by: $$\theta = (n \ln(n+1)) \cdot (e^2\pi)$$ • $n \ln(n+1)$: This expression correlates with the Prime Number Theorem, which states that the density of primes near $n$ is approximately $1/\ln n$. By scaling $n$ by its natural logarithm, we adjust the value according to its "natural position" within the prime hierarchy. • $e^2\pi$: This serves as the Coupling Constant. By utilizing $e$ and $\pi$, we hypothesize that Mersenne Primes oscillate at a universal harmonic frequency. The product $e^2\pi$ represents the bridge between exponential growth ($e$) and geometric circularity ($\pi$). II. The Correction Factor $\beta$ (Euler’s Gyroscope) A dynamic correction is applied to filter the "noise" from false candidates: $$\beta = \text{frac}\left(\frac{n \gamma}{\ln(n+1)}\right)$$ Where $\gamma \approx 0.577215...$ is the Euler-Mascheroni Constant. • Logic: $\gamma$ represents the accumulated error between the harmonic series and the natural logarithm. In the distribution of primes, there is a persistent "drift." • Fractional Shift: By taking only the decimal part ($\beta \pmod 1$), we apply a "micro-tuning" to the phase. Real Mersenne exponents "resist" this shift due to the rigid mathematical structure of $2^n-1$, while common primes are pulled out of resonance. III. The Purity Threshold ($\Psi_{adjusted}$) The final state is projected onto a sinusoidal wave: $$\Psi(n) = \sin(\theta + \beta)$$ The algorithm identifies exponents where $|\Psi| > 0.999995$. • Physical Significance: We are searching for Constructive Interference Nodes. At these points, the logarithmic density, transcendental constants, and Euler’s drift align perfectly. • The Candidate Paradox: While "Elite Candidates" reach near-perfect resonance ($|\Psi| \to 1.0000$), real Mersenne Primes often exhibit a slight "imperfection." This suggests that a real Mersenne prime requires a specific amount of Primal Entropy to exist as a prime number rather than collapsing into divisibility (numerical crystallization). IV. Mathematical Formalization The total phase $\Phi(n)$ is defined as the sum of the Logarithmic Momentum and the Euler Drift Factor: $$\Phi(n) = \left[ \underbrace{n \ln(n+1)}_{\text{Primordial Mass}} + \underbrace{\text{frac}\left(\frac{n \gamma}{\ln(n+1)}\right)}_{\text{Euler Correction}} \right] \cdot \underbrace{e^2 \pi}_{\text{Transcendental Scale}}$$ The resonance value is extracted via: $$\Psi(n) = \sin(\Phi(n))$$ V. Analysis of "Mersenne Entropy" For the OSF registry, we document the following observations: 1. Pure Resonance Nodes ($|\Psi| \to 1$): These represent perfect harmonic solutions in the transcendental field, often resulting in "False Elites" (harmonic ghosts). 2. Mersenne Quasi-Resonance ($0.998 < |\Psi| < 0.9999$): Real Mersenne Primes inhabit the "penumbra" of the node. This suggests that Mersenne primality requires a critical phase shift to maintain its unique status in the numerical field.

Fields of Study & Subjects

Analytic Number Theory Research Advanced Mathematical Theories and Applications Mathematical and Computational Methods

Publication details

Publication date
1 January 2026
Document type
Preprint