The prime numbers are distinguished from the non-primes by their common coordinates at the intersection of the and curves. Intuitively, the factorial function as represents the means to check for even divisibility for a natural number . Taking the factorial, we can create an matrix array where each row/column entry equals
(1.7.372)
which is implemented using the following MATLAB code for a specified natural number
NumM= [];
n1=n;
for j=1:(n1-1)
vec= [];
for k=1:(n1-1)
iter=mod(j*k, n1);
vec= [vec, iter];
end
NumM= [NumM; vec];
end
We use this algorithm to evaluate the natural numbers from to , arranging these matrices in the array
(1.7.373)
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Table 1.7.4. – The natural number matricesarranged in an array form. The zeros in the matrices represent composite number even divisibility. Prime numbersare the zero-less matrices.
The matrices are displayed in Table 1.7.4, which are symmetric, and each equals its own matrix transpose. The interpretation of the position of the zeros in the composite numbers is the row/column numbers represent the specific evenly divisible product(s). For example, in the matrix, the zeros coincide with products generated by , recalling this is congruent modulo 9. In each of the matrices submatrices are highlighted in grey and light blue, with the orange crosses representing shared rows/columns in the submatrices for even-valued . We draw attention to the odd-valued matrices in particular and the diagonal and anti-diagonal of these submatrices, which we evaluate congruent modulo the product of the elements in
(1.7.374)
(1.7.375)
(1.7.376)
These congruent modulo diagonal/anti-diagonal element products yield values consistent with the primary generators oriented counterclockwise and clockwise from the identity for the prime numbers.
By the inherent complex geometry, primality testing can be achieved by ensuring each element transforms by a power to equal one of the two guaranteed generators. Using the exponents in the Geometric Numbers, a matrix array can be created as follows for
(1.7.377)
where each element in the matrix portion above represents each vertex element from the -gon raised to the powers through The guaranteed generators are and , which by powers, will form the entire group
(1.7.378)
The zeros in row and column represent the identity and are trivial in these positions for primality testing. We remove the outer ring of sequential numbers formed by , then highlight in red the values that equal the generators in the expression below
(1.7.379)
finding that a symmetric ring of generators forms in the matrix. The generator power hits ensure the four other non-identity elements in are also generators of the group, showing that To clearly see this, the non-identity vertices in exponential form when raised to sequential powers have the representation
(1.7.380)
Expressing the submatrix of powers in this form, we find
(1.7.381)
which simplifies after calculating the power products and performing modulo arithmetic to
(1.7.382)
where once again the generators are highlighted in red. The first power test for that lands on a generator is sufficient to show that is also a generator of
Theory (1.7.383) – Fora finite Geometric Number, the complex conjugate of any generatoris also a generator of the group
ProofThe complex conjugate for any non-identity vertex, with vertex numberoriented on the-gon, equals
By the symmetry of, both vertices are an equal distance in radians on the boundary of the complex unit disc from the identity atGiven thatis a generator, it lands on eitherandfor a given power. The equal radian distance thattravels then lands on the conjugate generator to that of, and is, therefore, a generator
From the previous matrix, the red vertex entries in the upper half (first two rows) are mirrored in the lower half by their complex conjugates, given that
(1.7.384)
(1.7.385)
The same conjugate relationship holds for the left and right two columns. This implies that for the , generator, testing is only required for the two vertices counterclockwise from , or the two vertices clockwise from In layperson's terms, checking the non-identity vertices in the top or bottom half is sufficient to test primality.
Wilson's theorem states that prime numbers obey the following
(1.7.386)
The theorem can be applied by returning to the power table, where color in blue the submatrices with values associated with the generator, and in green, the generator.
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(1.7.387)
We calculate the product of the elements located on the anti-diagonal modulo
(1.7.388)
which is consistent with the theorem, given that for , we find
(1.7.389)
and . In the Geometric Numbers the value represents the generator. By Fermat's little theorem
(1.7.390)
we only need to calculate the anti-diagonal from one green submatrix, given that , finding the same result
(1.7.391)
This case's values formed the anti-diagonal from the submatrices containing the generator. To contrast, we can perform the same calculation using the anti-diagonal from a blue submatrix, finding
(1.7.392)
which represents the other generator . For the reader, we include the matrix array representations for three larger natural numbers in the following tables, one non-prime , and the twin prime pair , which represent the Geometric Numbers and . Each array has color-coded submatrices that represent pairings of transpose symmetry in the array for each number.
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Table 1.7.5– The numeric power products of
As expected, the non-prime has a total of sixteen zeros in its matrix array representation, the even divisibility of its prime decomposition numbers Eight possible transpose sub-symmetries in , are seen by the matching color submatrix pairs. Taken as a whole, a global symmetry exists as two transpose symmetries, represented by the amalgam of all blue-shaded and green-shaded submatrices.
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Table 1.7.6– The numeric power-productsof
In Table 1.7.6 and Table 1.7.7, all entries in each array are non-zero, which is consistent with the non-divisibility of the prime numbers. There are only two transform symmetries for and , consistent with one global symmetry for their power products.
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Table 1.7.7– The numeric power-products of.
There is a profound beauty when the prime numbers are seen in the complex geometry instead of the natural numbers on the line. To reveal this beauty, we define the positive integers by the counterclockwise oriented guaranteed primary generators for each geometric -gon using the following parametric wave function
(1.7.393)
Specifically, the waveform intersects each -gon at the corresponding primary generator vertex . The waveform is plotted in Figure 1.7.36 for prime numbers in green, and non-prime numbers in blue. For , chords connect the positive and negative guaranteed primary generator vertices.
Figure 1.7.36 – The positive integer waveform function intersects each disc at the primary generator vertex , for the prime numbers in green and the non-prime numbers in blue.
The waveform can be rotated around the -axis to by the specific argument value , where represents the integer value of the natural numbers . We chose to rotate in the negative/clockwise orientation, manifested by the following parametric function
(1.7.394)
Figure 1.7.37 – The specific natural numbers waveform for . The
Geometric Primesare labelled for the first eight prime numbers and.
For the individual natural number representations of , the waveform will intersect the specific at the identity element, shown in Figure 1.7.37 for the first eight prime numbers. For each , the -gon representation is conveyed by the points on the unit circles for each of its vertices.
Figure 1.7.38 – The intersections occurring at the positive peaks of the waveforms along the -axis.
Evenly divisibility can be seen geometrically for by waveform intersects for these numbers by the waveforms that comprise the said numbers prime decomposition. For example, the waveform can be seen to intersection vertices of the blue unit circles at . The intersections with the identity element of each is seen in Figure 1.7.38 at the positive peaks along the -axis for each waveform.
Figure 1.7.39 – Plots of the positive integer waveform functions and
We define the positive integer function , as the waveform intersecting with each negative oriented guaranteed primary generator
(1.7.395)
which differs from by the sign for the imaginary portion of the parametric function. The and wave functions are plotted in Figure 1.7.39, in which, it is straightforward to see the waveforms intersect with the vertices of each -gon in a complex conjugate relationship to one another.