Prime Potential Density Function

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Consider that primes are the dissonant instances within harmonic sets of those dissonant instances. That is, the nth prime begins a harmonic set across \({Z}\). Suppose:

When a harmonic set of \(p(n)\) encounters a number that is dissonant (not within that harmonic set), this number becomes the next element of \({P}\).

For example, starting at \(2\):

\( h(p(1)) = {h}(2)=\{ 2, 4, 6, 8, 10 \dots\} \)

and,

\( {h}(p(2)) = {h}(3) = \{3, 6, 9, 12, 15 \dots\} \)

So,

\(\vert {H}(n) \vert = \infty \frac{ 1 }{ p(n) }\), e.g. \(\vert {H}(1) \vert = \infty \frac{ 1 }{ 2 }\)

and,

\(\vert {Z} – {H}(n) \vert =\infty \frac{p(n) – 1}{p(n)}\), e.g. \(\vert {Z} – {H}(2) \vert = \infty \frac{ 2 }{ 3 }\)

We see that as we progress through the primes, harmonic sets progressively eliminate all subsequent factors of that prime as potential primes. Therefore, the potential of encountering a dissonant real (and consequently, a prime number) becomes less frequent as \(n \to \infty\). We will refer to this quality as Prime Potential Density (\(d\)). Thus, as \(n \to \infty, d \to 0\).

If we are looking for \(d(n)\) at the nth prime, then all primes prior must be factored into the prime potential density to ensure all harmonic sets are eliminated. So,

\(d(n) = \vert {Z} \vert \frac{p(n)-1}{p(n)} \frac{p(n-1)-1}{p(n-1)} \frac{p(n-2)-1}{p(n-2)} \dots\), e.g. \(d(3) = \infty \frac{ 5 – 1 }{ 5 } \frac{ 3 -1 }{ 3 } \frac{ 2 – 1 }{ 2 } \dots\)

Formally, the Prime Potential Density Function:

\(d(n) = \infty \prod\limits_{i=0}^{n} \frac{ p(n – i) – 1 }{ p(n – i) } \)
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