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Addition is the form of an expression set equal to zero as the additive identity which is common practice in several areas of mathematics.
This section is referring to wiki page-1 of zone section-1 that is inherited from the zone section-1 by prime spin-1 and span- with the partitions as below.
/lexer
By the Euler's identity this addition should form as one (1) unit of an object originated by the 18s structure. For further on let's call this unit as the base unit.
Below is the list of primes spin along with their position, the polarity of the number, and the prime hexagon's overall rotation within 1000 numbers.
The Prime Hexagon is a mathematical structure developed by mathematician Tad Gallion. A Prime Hexagon is formed when integers are sequentially added to a field of tessellating equilateral triangles, where the path of the integers is changed whenever a prime number is encountered (GitHub: kaustubhcs/prime-hexagon).
5, 2, 1, 0
+7, 3, 1, 0
+11, 4, 1, 0
+13, 5, 1, 0
+17, 0, 1, 1
+19, 1, 1, 1
+23, 2, 1, 1
+29, 2, -1, 1
+31, 1, -1, 1
+37, 1, 1, 1
+41, 2, 1, 1
+43, 3, 1, 1
+47, 4, 1, 1
+53, 4, -1, 1
+59, 4, 1, 1
+61, 5, 1, 1
+67, 5, -1, 1
+71, 4, -1, 1
+73, 3, -1, 1
+79, 3, 1, 1
+83, 4, 1, 1
+89, 4, -1, 1
+97, 3, -1, 1
+101, 2, -1, 1
+103, 1, -1, 1
+107, 0, -1, 1
+109, 5, -1, 0
+113, 4, -1, 0
+127, 3, -1, 0
+131, 2, -1, 0
+137, 2, 1, 0
+139, 3, 1, 0
+149, 4, 1, 0
+151, 5, 1, 0
+157, 5, -1, 0
+163, 5, 1, 0
+167, 0, 1, 1
+173, 0, -1, 1
+179, 0, 1, 1
+181, 1, 1, 1
+191, 2, 1, 1
+193, 3, 1, 1
+197, 4, 1, 1
+199, 5, 1, 1
+211, 5, -1, 1
+223, 5, 1, 1
+227, 0, 1, 2
+229, 1, 1, 2
+233, 2, 1, 2
+239, 2, -1, 2
+241, 1, -1, 2
+251, 0, -1, 2
+257, 0, 1, 2
+263, 0, -1, 2
+269, 0, 1, 2
+271, 1, 1, 2
+277, 1, -1, 2
+281, 0, -1, 2
+283, 5, -1, 1
+293, 4, -1, 1
+307, 3, -1, 1
+311, 2, -1, 1
+313, 1, -1, 1
+317, 0, -1, 1
+331, 5, -1, 0
+337, 5, 1, 0
+347, 0, 1, 1
+349, 1, 1, 1
+353, 2, 1, 1
+359, 2, -1, 1
+367, 1, -1, 1
+373, 1, 1, 1
+379, 1, -1, 1
+383, 0, -1, 1
+389, 0, 1, 1
+397, 1, 1, 1
+401, 2, 1, 1
+409, 3, 1, 1
+419, 4, 1, 1
+421, 5, 1, 1
+431, 0, 1, 2
+433, 1, 1, 2
+439, 1, -1, 2
+443, 0, -1, 2
+449, 0, 1, 2
+457, 1, 1, 2
+461, 2, 1, 2
+463, 3, 1, 2
+467, 4, 1, 2
+479, 4, -1, 2
+487, 3, -1, 2
+491, 2, -1, 2
+499, 1, -1, 2
+503, 0, -1, 2
+509, 0, 1, 2
+521, 0, -1, 2
+523, 5, -1, 1
+541, 5, 1, 1
+547, 5, -1, 1
+557, 4, -1, 1
+563, 4, 1, 1
+569, 4, -1, 1
+571, 3, -1, 1
+577, 3, 1, 1
+587, 4, 1, 1
+593, 4, -1, 1
+599, 4, 1, 1
+601, 5, 1, 1
+607, 5, -1, 1
+613, 5, 1, 1
+617, 0, 1, 2
+619, 1, 1, 2
+631, 1, -1, 2
+641, 0, -1, 2
+643, 5, -1, 1
+647, 4, -1, 1
+653, 4, 1, 1
+659, 4, -1, 1
+661, 3, -1, 1
+673, 3, 1, 1
+677, 4, 1, 1
+683, 4, -1, 1
+691, 3, -1, 1
+701, 2, -1, 1
+709, 1, -1, 1
+719, 0, -1, 1
+727, 5, -1, 0
+733, 5, 1, 0
+739, 5, -1, 0
+743, 4, -1, 0
+751, 3, -1, 0
+757, 3, 1, 0
+761, 4, 1, 0
+769, 5, 1, 0
+773, 0, 1, 1
+787, 1, 1, 1
+797, 2, 1, 1
+809, 2, -1, 1
+811, 1, -1, 1
+821, 0, -1, 1
+823, 5, -1, 0
+827, 4, -1, 0
+829, 3, -1, 0
+839, 2, -1, 0
+853, 1, -1, 0
+857, 0, -1, 0
+859, 5, -1, -1
+863, 4, -1, -1
+877, 3, -1, -1
+881, 2, -1, -1
+883, 1, -1, -1
+887, 0, -1, -1
+907, 5, -1, -2
+911, 4, -1, -2
+919, 3, -1, -2
+929, 2, -1, -2
+937, 1, -1, -2
+941, 0, -1, -2
+947, 0, 1, -2
+953, 0, -1, -2
+967, 5, -1, -3
+971, 4, -1, -3
+977, 4, 1, -3
+983, 4, -1, -3
+991, 3, -1, -3
+997, 3, 1, -3
+
Including the 1st (2) and 2nd prime (3) all together will have a total of 168 primes. The number of 168 it self is in between 39th (167) and 40th prime (173).
The number of primes less than or equal to a thousand (π(1000) = 168) equals the number of hours in a week (7 * 24 = 168).
The most obvious interesting feature of proceeding this prime hexagon, the number line begins to coil upon itself, is it confines all numbers of primes spin!
Each time a prime number is encountered, the spin or ‘wall preference’ is switched. So, from the first cell, exit from 2’s left side. This sets the spin to left and the next cell is 3, a prime, so switches to right. 4 is not prime and continues right. 5 is prime, so switch to left and so on. (HexSpin)
As the number line winds about toward infinity, bending around prime numbers, it never exits the 24 cells. And it is the fact that 168 divided by 24 is exactly seven (7).
Surprisingly, the 24-cell hexagon confines all natural numbers. The reason: no prime numbers occupy a cell with a right or left wall on the t-hexagon’s outer boundary, other than 2 and 3, the initial primes that forced the number line into this complex coil. Without a prime number in the outer set of triangles, the number line does not change to an outward course and remains forever contained in the 24 cells. (HexSpin)
You may notice that there are twists and turns until 19 abuts 2 therefore this addition zone takes only the seven (7) primes out of the 18's structure of True Prime Pairs.
$True Prime Pairs:
+(5,7), (11,13), (17,19)
+
+layer | node | sub | i | f
+------+------+-----+----------
+ | | | 1 | --------------------------
+ | | 1 +-----+ |
+ | 1 | | 2 | (5) |
+ | |-----+-----+ |
+ | | | 3 | |
+ 1 +------+ 2 +-----+---- |
+ | | | 4 | |
+ | +-----+-----+ |
+ | 2 | | 5 | (7) |
+ | | 3 +-----+ |
+ | | | 6 | 11s
+------+------+-----+-----+------ } (36) |
+ | | | 7 | |
+ | | 4 +-----+ |
+ | 3 | | 8 | (11) |
+ | +-----+-----+ |
+ | | | 9 | |
+ 2 +------| 5 +-----+----- |
+ | | | 10 | |
+ | |-----+-----+ |
+ | 4 | | 11 | (13) ---------------------
+ | | 6 +-----+
+ | | | 12 |---------------------------
+------+------+-----+-----+------------ |
+ | | | 13 | |
+ | | 7 +-----+ |
+ | 5 | | 14 | (17) |
+ | |-----+-----+ |
+ | | | 15 | 7s √
+ 3 +------+ 8 +-----+----- } (36) |
+ | | | 16 | |
+ | |-----+-----+ |
+ | 6 | | 17 | (19) |
+ | | 9 +-----+ |
+ | | | 18 | --------------------------
+------|------|-----+-----+------
+
The tessellating field of equilateral triangles fills with numbers, with spin orientation flipping with each prime number encountered, creating 3 minor hexagons.
Prime numbers are numbers that have only 2 factors: 1 and themselves.
In conclusion, the number 1 is neither prime nor composite.
π(6+11) = π(17) = 7
So there should be a tight connection between 168 primes within 1000 with the 24-cell hexagon. Indeed it is also correlated with 1000 prime numbers.
When we continue the spin within the discussed prime hexagon with the higher numbers there are the six (6) internal hexagons within the Prime Hexagon.
Cell types are interesting, but they simply reflect a modulo 6 view of numbers. More interesting are the six internal hexagons within the Prime Hexagon. Like the Prime Hexagon, they are newly discovered. The minor hexagons form solely from the order, and type, of primes along the number line (HexSpin).
So the most important thing that need to be investigated is why the prime spinned by module six (6). What is the special thing about this number six (6) in primes behaviour?
Similarly, I have a six colored dice in the form of the hexagon. If I take a known, logical sequence of numbers, say 10, 100, 1000, 10000, and look at their spins in the hexagon, the resulting colors associated with each number should appear random – unless the sequence I’m investigating is linked to the nature of the prime numbers.
Moreover there are view statements mentioned by the provider which also bring us in to an attention like the modulo 6 above. We put some of them below.
That is, if the powers of 10 all returned with blue spin, or as a series of rainbows, or evenly alternating colors or other non-random results, then I’d say prime numbers appear to have a linkage to 10. I may not know what the the linkage is, just that it appears to exist (HexSpin).
Another is that phi and its members have a pisano period if the resulting fractional numbers are truncated.
I wondered if that property might hold for the incremental powers of phi as well. For this reason I chose to see numbers in the hexagon as quantum, and truncate off the decimal values to determine which integer cell they land in. That is what I found. Phi and its members have a pisano period if the resulting fractional numbers are truncated. (HexSpin).
It would mean that there should be undiscovered things hidden within the residual of this decimal values. In fact it is the case that happen with 3-forms in 7D.
Let's consider a prime spin theory of compactifying the 7-dimensional manifold on the 3-sphere of a fixed radius and study its dimensional reduction to 4D.
Proceeding, the number line begins to coil upon itself; 20 lands on 2’s cell, 21 on 3’s cell. Prime number 23 sends the number line left to form the fourth (4th) hexagon, purple. As it is not a twin, the clockwise progression (rotation) reverses itself. Twin primes 29 and 31 define the fifth (5th) hexagon, cyan. Finally, 37, again not a twin, reverses the rotation of the system, so 47 can define the yellow hexagon (HexSpin).
Taking 19 as a certain parameter we can see that the left handed cycles are happen on 5th-spin (forms 4th hexagon, purple) and 6th-spin (forms 5th hexagon, cyan). Both have different rotation with other spin below 9th spin (forms 6th hexagon, yellow).
All perfect squares within our domain (numbers not divisible by 2, 3 or 5) possess a digital root of 1, 4 or 7 and are congruent to either {1} or {19} modulo 30.
There’s another hidden dimension of our domain worth noting involving multiples of 360, i.e., when framed as n ≌ {1, 7, 11, 13, 17, 19, 23, 29, 31, 37, 41, 43, 47, 49, 53 59, 61, 67, 71, 73, 77, 79, 83, 89} modulo 90, and taking ‘bipolar’ differentials of perfect squares (PrimesDemystified)
16 × 6 = 96
Also note, the digital roots of the Prime Root Set as well as the digital roots of Fibonnaci numbers and indexed to it all sum to 432 (48x9) in 360° cycles.
Each of the digital root multiplication matrices produced by the six channels consists of what are known in mathematics as ‘Orthogonal Latin Squares’ (defined in Wikipedia as “an n x n array filled with n different symbols, each occurring exactly once in each row and exactly once in each column” … in our case every row and column of the repeating 6x6 matrices possesses the six elements: 1, 2, 4, 5, 7, 8 in some order). Also, the sum of the multiplicative digital roots = 108 x 24 = 2592 = 432 x 6.
We can generate triangles and magic squares by tiering the Fibonacci digital root sequence with two pairs of terms that are + 3 or + 6 from the initial terms {1,1}. The values of the 2nd and 3rd tiers, or rows, must differ, or symmetry is lost. In other words, the first two columns should read either {1,4,7 + 1,7,4, or vice versa} but not {1,4,7 + 1,4,7, or 1,7,4, + 1,7,4}. (PrimesDemystified)
The above seven (7) primes will act then as extended branes. This is what we mean by addition zones and it happens whenever a cycle is restarted.
When these 9 squares are combined and segregated to create a 6 x 6 (36 element) square, and this square is compared to the Vedic Square minus its 3’s, 6’s and 9’s (the result dubbed “Imaginary Square”), you’ll discover that they share identical vertical and horizontal secquences, though in a different order (alternating +2 and -2 from each other), and that these can be easily made to match exactly by applying a simple function multiplier, as described and illustrated later below. (PrimesDemystified)
They are the source of triangular coordinates when translated into vertices of a modulo 9 circle which by definition has 9 equidistant points each separated by 40°.
When we additively sum the three period-24 digital root cycles these dyads produce, then tier them, we create six 3 x 3 matrices (each containing values 1 thru 9) separated by repetitive number tiers in the following order: {1,1,1} {5,5,5} {7,7,7} {8,8,8} {4,4,4} {2,2,2}.
Remarkably, this periodic palindrome, with additive sum of 108, sequences the 6 possible permutations of values {3,6,9}. Interesting to consider a geometric object with a hidden palindromic dimension. But that’s not all: When the six triadic permutations forming the palindrome are labeled A, B, C, D, E, F in the order generated, ACE and BDF form 3 x 3 Latin squares. In both cases all rows, columns and principal diagonals sum to 18:
It’s remarkable that objects consisting of star polygons, spiraling irregular pentagons, and possessing nonagon perimeters and centers, can be constructed from only 27 coordinates pointing to 9 triangles in 3 variations. Each period-24 cycle produces two ‘palindromagons’. (PrimesDemystified)
In our approach a 3-form is not an object that exist in addition to the metric, it is the only object that exist and in particular the 4D metric, is defined by the 3-form.
Also, in the supergravity context a 7D manifold with a G2 structure is used for compactifying the 11D supergravity down to 4D. In contrast, we compactify from 7D to 4D. (General relativity from three-forms in seven dimensions - pdf)
The the main reason of assigning two (2) profiles instead of only one (1) is that we have to accommodate the major type of primes numbers called twin primes.
This is a necessary but not sufficient condition for N to be a prime as noted, for example, by N= 6(4)+1= 25, which is clearly composite. We note that each turn of the spiral equals an increase of six units. This means that we have a mod(6) situation allowing us to write: N mod(6)=6n+1 or N mod(6)=6n-1 (equivalent to 6n+5). (HexSpiral-Pdf)
Focusing on just the twin prime distribution channels, we see the relationships shown below [and, directly above, we show that two of the channels (B & C) transform bi-directionally by rotating 180° around one of their principal (lower-left to upper-right) diagonal axes]:
7th spin - 4th spin = (168 - 102)s = 66s = 6 x 11s = 30s + 36s
By the Δ(19 vs 18) Scenario those three are exactly landed in the 0's cell out of Δ18. See that the sum of 30 and 36 is 66 while the difference between 36 and 102 is also 66.
You likely noticed I began with 2 rather than 1 or 0 when I first constructed the hexagon. Why? Because they do not fit inside — they stick off the hexagon like a tail. Perhaps that’s where they belong. However, if one makes a significant and interesting assumption, then 1 and 0 fall in their logical locations – in the 1 and 0 cells, respectively. _(HexSpin)
0 + 30 + 36 + 102 = 168 = π(1000)
Because the value 30 is the first (common) product of the first 3 primes. And this 30th order repeats itself to infinity. Even in the first 30s system, therefore, the positions are fixed in which the number information positions itself to infinity. We call it the first member of the MEC 30.
From our consideration we can conclude that the distribution of prime numbers must have a static base structure, which is also confirmed logically in the further course. This static structure is altered by the products of the primes themselves, since these products must fall into the prime positions since they are not divisible by 2, 3 and 5. (Google Patent DE102011101032A9)
Speaking of iterative digital division–a powerful tool for exposing structure–we get this astonishing equation: iteratively dividing the digital roots of the first 12 Fibonacci numbers times the divisively iterated 1000th prime, 7919, times 3604 gives us 1000. Keep in mind that the first two and last two digits of the Fibo sequence below, 11 and 89, sum to 100; that 89 is the 11th Fibo number; that there are 1000 primes between 1 and 892; and that 89 has the Fibonacci sequence embedded in its decimal expansion
The four faces of our pyramid additively cascade 32 four-times triangular numbers (oeis.org/A046092: a(n) = 2(n+1) …).
The table below shows the telescopic progressions of triangular, 4-times triangular numbers and cascade of perfect squares that populate the pyramid’s faces.
The equality between the product on the 1st-line and the formulas in the 3rd- and 4th-lines is Euler's pentagonal number where p(33) = 10143
landed exactly by n - 7
.
Using Euler’s method to find p(40): A ruler with plus and minus signs (grey box) is slid downwards, the relevant terms added or subtracted. The positions of the signs are given by differences of alternating natural (blue) and odd (orange) numbers. In the SVG file, hover over the image to move the ruler (Wikipedia).
π(π(π(1000th prime))) + 1 = 40
As explicitly indicated by n - 7
within identition zones this p(33)
behave reversal to the exponentiation zones so it would stand as π(π(π(1000th prime)))+1
.
p(33) = p(40-7) = loop (100000) = 4 + 25 + 139 + 1091 + 8884 = 10143
So there would be the empty spaces for 18 - 7 = 11
numbers. By our project these spaces will be unified by all of the eleven (11) members of identition zones.
(11x7) + (29+11) + (25+6) + (11+7) + (4+1) = 77+40+31+18+5 = 171
So by simple words this 11 dimensions brings us back to the root functions. The only difference is the base unit. It is now carrying the above p(33) = 10143
.
This is the partial of the mapping scheme of our eQuantum Project. Our mapping is simulating a recombination of the three (3) layers of these prime pairs.
This section is referring to wiki page-2 of zone section-2 that is inherited from the zone section-2 by prime spin-2 and span- with the partitions as below.
/lexer
An Independent claim is also included for the localization and determination, or their material structures, by graphical representation of base sequences on various media, based on the new assignments and the derived vibrations and amplitudes.
In short this project is mapping the quantum way within a huge of prime objects (5 to 19) by lexering (11) the ungrammared feed (7) and parsering (13) across syntax (17).
5, 2, 1, 0
+7, 3, 1, 0
+11, 4, 1, 0
+13, 5, 1, 0
+17, 0, 1, 1
+19, 1, 1, 1
+
The 5+7+11+13 is the smallest square number expressible as the sum of four consecutive primes which are also two couples of prime twins!
$True Prime Pairs:
+ (5,7), (11,13), (17,19)
+
+ layer| i | f
+ -----+-----+---------
+ | 1 | 5
+ 1 +-----+
+ | 2 | 7
+ -----+-----+--- } 36 » 6®
+ | 3 | 11
+ 2 +-----+
+ | 4 | 13
+ -----+-----+---------
+ | 5 | 17
+ 3 +-----+ } 36 » 6®
+ | 6 | 19
+ -----+-----+---------
+
$True Prime Pairs:
+(5,7), (11,13), (17,19)
+
+layer | node | sub | i | f
+------+------+-----+----------
+ | | | 1 |
+ | | 1 +-----+
+ | 1 | | 2 | (5)
+ | |-----+-----+
+ | | | 3 |
+ 1 +------+ 2 +-----+----
+ | | | 4 |
+ | +-----+-----+
+ | 2 | | 5 | (7)
+ | | 3 +-----+
+ | | | 6 |
+------+------+-----+-----+------ } (36)
+ | | | 7 |
+ | | 4 +-----+
+ | 3 | | 8 | (11)
+ | +-----+-----+
+ | | | 9 |
+ 2 +------| 5 +-----+-----
+ | | | 10 |
+ | |-----+-----+
+ | 4 | | 11 | (13)
+ | | 6 +-----+
+ | | | 12 |
+------+------+-----+-----+------------------
+ | | | 13 |
+ | | 7 +-----+
+ | 5 | | 14 | (17)
+ | |-----+-----+
+ | | | 15 |
+ 3 +------+ 8 +-----+----- } (36)
+ | | | 16 |
+ | |-----+-----+
+ | 6 | | 17 | (19)
+ | | 9 +-----+
+ | | | 18 |
+------|------|-----+-----+------
+
$True Prime Pairs:
+(5,7), (11,13), (17,19)
+
+layer | node | sub | i | f
+------+------+-----+----------
+ | | | 1 | --------------------------
+ | | 1 +-----+ |
+ | 1 | | 2 | (5) |
+ | |-----+-----+ |
+ | | | 3 | |
+ 1 +------+ 2 +-----+---- |
+ | | | 4 | |
+ | +-----+-----+ |
+ | 2 | | 5 | (7) |
+ | | 3 +-----+ |
+ | | | 6 | 11s
+------+------+-----+-----+------ } (36) |
+ | | | 7 | |
+ | | 4 +-----+ |
+ | 3 | | 8 | (11) |
+ | +-----+-----+ |
+ | | | 9 | |
+ 2 +------| 5 +-----+----- |
+ | | | 10 | |
+ | |-----+-----+ |
+ | 4 | | 11 | (13) ---------------------
+ | | 6 +-----+ <----------------- strip √
+ | | | 12 |---------------------------
+------+------+-----+-----+------------ |
+ | | | 13 | |
+ | | 7 +-----+ |
+ | 5 | | 14 | (17) |
+ | |-----+-----+ |
+ | | | 15 | 7s = f(1000)
+ 3 +------+ 8 +-----+----- } (36) |
+ | | | 16 | |
+ | |-----+-----+ |
+ | 6 | | 17 | (19) |
+ | | 9 +-----+ |
+ | | | 18 | --------------------------
+------|------|-----+-----+------#
+
We consider a certain theory of 3-forms in 7 dimensions, and study its dimensional reduction to 4D, compactifying the 7-dimensional manifold on the 3-sphere of a fixed radius.
In our approach a 3-form is not an object that exist in addition to the metric, it is the only object that exist. The metric, and in particular the 4D metric, is defined by the 3-form. (General relativity from three-forms in seven dimensions - pdf)
In this article we will support this conjecture and develop a new approach to quantum gravity called smooth quantum gravity by using smooth 4-manifolds with an exotic smoothness structure.
The scaling behavior of this action is analyzed to obtain the classical theory of General Relativity (GRT) for large scales. (Smooth quantum gravity - pdf)
The holonomy tells you how to propagate MEC30. A spin network state assigns an amplitude to a set of spin half particles tracing out a path in space, merging and splitting.
This kind of approach has some obvious properties: there are non-linear gravitons, a connection to lattice gauge field theory and a dimensional reduction from 4D to 2D.
$True Prime Pairs:
+(5,7), (11,13), (17,19)
+
+layer | node | sub | i | f
+------+------+-----+---------- <----------------- Mobius strip √
+ | | | 1 | --------------------------
+ | | 1 +-----+ |
+ | 1 | | 2 | (5) |
+ | |-----+-----+ |
+ | | | 3 | |
+ 1 +------+ 2 +-----+---- |
+ | | | 4 | |
+ | +-----+-----+ |
+ | 2 | | 5 | (7) |
+ | | 3 +-----+ |
+ | | | 6 | 11s
+------+------+-----+-----+------ } (36) |
+ | | | 7 | |
+ | | 4 +-----+ |
+ | 3 | | 8 | (11) |
+ | +-----+-----+ |
+ | | | 9 | |
+ 2 +------| 5 +-----+----- |
+ | | | 10 | |
+ | |-----+-----+ |
+ | 4 | | 11 | (13) ---------------------
+ | | 6 +-----+ <----------------- Mobius strip
+ | | | 12 |---------------------------
+------+------+-----+-----+------------ |
+ | | | 13 | |
+ | | 7 +-----+ |
+ | 5 | | 14 | (17) |
+ | |-----+-----+ |
+ | | | 15 | 7s = f(1000)
+ 3 +------+ 8 +-----+----- } (36) |
+ | | | 16 | |
+ | |-----+-----+ |
+ | 6 | | 17 | (19) |
+ | | 9 +-----+ |
+ | | | 18 | --------------------------
+------|------|-----+-----+------ <----------------- Möbius strip √
+
The funny looking Möbius strip, which was also independently discovered in 1858 by the unlucky Listing whose name left the history of mathematics untouched.
Being the first example of a surface without orientation it did not shake the grounds of mathematics as much as the other discoveries of this list did, yet it provided a lot of practical applications, such as a resistant belt, and inspired mathematicians to come up with unorientable surfaces, like the Klein bottle.
Mathematical fields were created, we got the Turing Machine, fancy looking surfaces and, most importantly, the ability to re-examine our perceptions and adapt our tools accordingly. (freeCodeCamp)
These items are elementary parts possessing familiar properties but they never exist as free particles. Instead they join together by the strong force into bound states.
f(18) = f(7) + f(11) = (1+7+29) + 11th prime = 37 + 31 = 36 + 32 = 68
Eigennvalue curves (right) showing a triple eigenvalue at zero for τ = 1 and double eigenvalues at 1 ± √2i for τ = √43. On the left the graph of 1/|Q(λ)| with the same eigenvalue curves plotted in the ground plane. Green stars indicate the eigenvalues of A, blue stars the roots of puv(λ) and triangles the zeroes of Q0(λ)
10 + 10th prime + 10th prime = 10 + 29 + 29 = 68
$True Prime Pairs:
+(5,7), (11,13), (17,19)
+
+layer | node | sub | i | f
+------+------+-----+---------- <----------------- Mobius strip
+ | | | 1 | --------------------------
+ | | 1 +-----+ |
+ | 1 | | 2 | (5) |
+ | |-----+-----+ |
+ | | | 3 | |
+ 1 +------+ 2 +-----+---- |
+ | | | 4 | |
+ | +-----+-----+ |
+ | 2 | | 5 | (7) |
+ | | 3 +-----+ |
+ | | | 6 | 11s ‹-- (71) √
+------+------+-----+-----+------ } (36) |
+ | | | 7 | |
+ | | 4 +-----+ |
+ | 3 | | 8 | (11) |
+ | +-----+-----+ |
+ | | | 9 | |
+ 2 +------| 5 +-----+----- |
+ | | | 10 | |
+ | |-----+-----+ |
+ | 4 | | 11 | (13) ---------------------
+ | | 6 +-----+ <----------------- Mobius strip
+ | | | 12 |---------------------------
+------+------+-----+-----+------------ |
+ | | | 13 | |
+ | | 7 +-----+ |
+ | 5 | | 14 | (17) |
+ | |-----+-----+ |
+ | | | 15 | 7s ‹-- (43) √
+ 3 +------+ 8 +-----+----- } (36) |
+ | | | 16 | |
+ | |-----+-----+ |
+ | 6 | | 17 | (19) |
+ | | 9 +-----+ |
+ | | | 18 | --------------------------
+------|------|-----+-----+------ <----------------- Möbius strip
+
This pattern is raised up per six (6) cycles on the 19, 43 and 71. Since the members are limited to the sum of 43+71=114.
So here the bilateral way of 19 that originated by the (Δ1) is clearly the one that controls the scheme.
In the matrix pictured below, we list the first 24 elements of our domain, take their squares, calculate the modulo 90 congruence and digital roots of each square, and display the digital root factorization dyad for each square (and map their collective bilateral 9 sum symmetry). (PrimesDemystified)
7 x π(89) = 7 x 24 = 168 = π(1000)
$True Prime Pairs:
+(5,7), (11,13), (17,19)
+
+layer | node | sub | i | f. MEC 30 / 2
+------+------+-----+-----+------ ‹------------------------------ 0 {-1/2}
+ | | | 1 | --------------------------
+ | | 1 +-----+ |
+ | 1 | | 2 | (5) |
+ | |-----+-----+ |
+ | | | 3 | |
+ 1 +------+ 2 +-----+---- |
+ | | | 4 | |
+ | +-----+-----+ |
+ | 2 | | 5 | (7) |
+ | | 3 +-----+ |
+ | | | 6 | 11s ‹-- ∆28 = (71-43) √
+------+------+-----+-----+------ } (36) |
+ | | | 7 | |
+ | | 4 +-----+ |
+ | 3 | | 8 | (11) |
+ | +-----+-----+ |
+ | | | 9 |‹-- ∆9 = (89-71) / 2 √ |
+ 2 +------| 5* +-----+----- |
+ | | | 10 | |
+ | |-----+-----+ |
+ | 4 | | 11 | (13) ---------------------
+ | | 6 +-----+ ‹------------------------------ 15 {0}
+ | | | 12 |---------------------------
+------+------+-----+-----+------------ |
+ | | | 13 | |
+ | | 7 +-----+ |
+ | 5 | | 14 | (17) |
+ | |-----+-----+ |
+ | | | 15 | 7s ‹-- ∆24 = (43-19) √
+ 3* +------+ 8 +-----+----- } (36) |
+ | | | 16 | |
+ | |-----+-----+ |
+ | 6 | | 17 | (19) |
+ | | 9 +-----+ |
+ | | | 18 | --------------------------
+------|------|-----+-----+----- ‹----------------------------------- 30 {+1/2}
+
Given our domain is limited to numbers ≌ {1,7,11,13,17,19,23,29} modulo 30, only ϕ(m)/m = 8/30 or 26.66% of natural numbers N = {0, 1, 2, 3, …} need be sieved.
1+29=30; 7+23=30; 11+19=30; and 13+17=30.
What is critical to understand, is that the invisible hand of 2, 3 and 5, and their factorial 30, create the structure within which the balance of the prime numbers, i.e., all those greater than 5, are arrayed algorithmically–as we shall demonstrate. Primes 2, 3 and 5 play out in modulo 30-60-90 cycles (decomposing to {3,6,9} sequencing at the digital root level). Once the role of 2, 3 and 5 is properly understood, all else falls beautifully into place. (PrimesDemystified)
This section is referring to wiki page-3 of zone section-3 that is inherited from the zone section-3 by prime spin-3 and span- with the partitions as below.
/lexer
Prime hexagon is a mathematical structure developed by mathematician T. Gallion that is formed when integers are sequentially added to a field of tessellating equilateral triangles, where the path of the integers is changed whenever a prime is encountered.
This is not easy as they are linked to the nature of prime numbers, and nothing is easy about the nature of prime numbers. But I begin with this assumption: if the hexagons participate in the Universe in any way other than haphazardly, they must be demonstrably congruent to something organized (T. Gallion).
s p i n
+0 0 0 0
+1 0 0 0
+2 0 1 0 ◄--- 1st prime
+3 1 1 0 ◄--- 2nd prime
+--------
+5 2 1 0 ◄--- 3rd prime
+7 3 1 0
+11 4 1 0
+13 5 1 0
+17 0 1 1 ◄--- 7th prime
+19 1 1 1 ◄--- 8th prime
+
17 = 7th prime = (18 - 11) th prime
p r i m e s
+1 0 0 0 0
+2 1 0 0 0
+3 2 0 1 0 2 ◄--- 1st prime
+4 3 1 1 0 3 ◄--- 2nd prime
+5 5 2 1 0 5 ◄--- 3rd prime
+6 7 3 1 0
+7 11 4 1 0
+8 13 5 1 0
+9 17 0 1 1 17 ◄--- 7th prime
+10 19 1 1 1 19 ◄--- 8th prime
+-----
+11 23 2 1 1 23 ◄--- 9th prime √
+
You may learn that sets of algebraic objects has a multilinear relationship related to a vector space called tensor. Tensors may map between different objects such as vectors, scalars, and even other tensors.
p r i m e s
+1 0 0 0 0
+2 1 0 0 0
+3 2 0 1 0 2 ◄--- 1st prime
+4 3 1 1 0 3 ◄--- 2nd prime
+5 5 2 1 0 5 ◄--- 3rd prime
+6 7 3 1 0
+7 11 4 1 0
+8 13 5 1 0
+9 17 0 1 1 17 ◄--- 7th prime
+10 19 1 1 1 ∆1 ◄--- 8th prime ◄--- Terminating Digit
+-----
+11 23 2 1 1 √
+
(17+13) + (11+19) = (7+11) + (19+23) = 60
p r i m e s
+1 0 0 0 0 0
+2 1 0 0 0 1
+3 2 0 1 0 2
+4 3 1 1 0 3
+5 5 2 1 0 5
+6 7 3 1 0 7
+7 11 4 1 0 11
+8 13 5 1 0 13
+9 17 0 1 1 17 ◄--- 7th prime
+10 19 1 1 1 ∆1 ◄--- 0th ∆prime ◄--- Terminating Digit #0 √
+-----
+11 23 2 1 1 ∆2 ◄--- 1st ∆prime ◄--- Terminating Digit #1 √
++29 rows √
+-----
+41 √
+
In order to maintain the 36 symmetry (whether it is an addition zone or not), with this prime number 19 was found at least seven (7) pairs of truncated patterns.
The tessellating field of equilateral triangles fills with numbers, with spin orientation flipping with each prime number encountered, creating 3 minor hexagons.
π(6+11) = π(17) = 7
This polarity is happened per six (6) cycles by the polar of six (6) to one (1) and six (6) to seven (7) that leads to the prime number 61 and 67.
The above characteristics of primes in the hexagon suggests 0 family numbers split more than twin primes. I speculate these numbers split all primes. That is, all primes have a partner (of the opposite family) equidistant from such a number. For instance, 0 family member 18 splits twin primes 17 and 19, but is also 5 more than 13 and 5 less than 23, and it is also 11 more the 7, and 11 less than 29, etc. (Hexspin)
By which we finally found if this behaviour is cascaded bilaterally within the correlation between 61 as the 18th prime and 67 as the 19th prime.
The solution is not only to prove Re(z)= 1/2 but also to calculate ways for the imaginary part of the complex root of ζ(z)=0 and also to solve the Functional equations of Riemann
18 + 19 = π(61) + π(67) = 37
p r i m e s
+1 0 0 0 0 0
+2 1 0 0 0 1
+3 2 0 1 0 2
+4 3 1 1 0 3
+5 5 2 1 0 5
+6 7 3 1 0 7
+7 11 4 1 0 11
+8 13 5 1 0 13
+9 17 0 1 1 17 ◄--- 7th prime
+10 19 1 1 1 ∆1 ◄--- 0th ∆prime ◄--- Terminating Digit #0 (spin 18) √
+-----
+11 23 2 1 1 ∆2 ◄--- 1st ∆prime ◄--- Terminating Digit #1 (spin 19) √
++29 rows
+-----
+41
+
The Prime Spiral Sieve possesses remarkable structural and numeric symmetries. For starters, the intervals between the prime roots (and every subsequent row or rotation of the sieve) are perfectly balanced, with a period eight (8) difference sequence of: {6, 4, 2, 4, 2, 4, 6, 2} (Primesdemystified).
p r i m e s
+1 0 0 0 0 0
+2 1 0 0 0 1
+3 2 0 1 0 2
+4 3 1 1 0 3
+5 5 2 1 0 5
+6 7 3 1 0 7
+7 11 4 1 0 11
+8 13 5 1 0 13
+9 17 0 1 1 17 ◄--- 7th prime
+10 19 1 1 1 ∆1 ◄--- 0th ∆prime ◄--- Terminating Digit #0 (spin 18)
+-----
+11 23 2 1 1 ∆2 ◄--- 1st ∆prime ◄--- Terminating Digit #1 (spin 19)
++29 rows
+-----
+41
++59 rows √
+
Speaking of the Fibonacci number sequence, there is symmetry mirroring the above in the relationship between the terminating digits of Fibonacci numbers and their index numbers equating to members of the array populating the Prime Spiral Sieve.
Fibonacci level-1 (29) x Fibonacci level-2 (59) = 10x10 = 💯
p r i m e s
+1 0 0 0 0 0
+2 1 0 0 0 1
+3 2 0 1 0 2
+4 3 1 1 0 3
+5 5 2 1 0 5
+6 7 3 1 0 7
+7 11 4 1 0 11
+8 13 5 1 0 13
+9 17 0 1 1 17 ◄--- 7th prime
+10 19 1 1 1 ∆1 ◄--- 0th ∆prime ◄--- Terminating Digit #0 ◄- Fibonacci Index #18 √
+-----
+11 23 2 1 1 ∆2 ◄--- 1st ∆prime ◄--- Terminating Digit #1 ◄- Fibonacci Index #19 √
+..
+..
+40 163 5 1 0 ∆31 ◄- 11th ∆prime ◄- Terminating Digit #11 ◄- Fibonacci Index #29 √
+-----
+41
++59 rows ◄--- total 41+59 = 💯 rows = 10x10 rows √
+
(59² − 31²) = 360 x 7
p r i m e s
+1 0 0 0 0 0
+2 1 0 0 0 1
+3 2 0 1 0 2
+4 3 1 1 0 3
+5 5 2 1 0 5
+6 7 3 1 0 7
+7 11 4 1 0 11
+8 13 5 1 0 13
+9 17 0 1 1 17 ◄--- 7th prime
+10 19 1 1 1 ∆1 ◄--- 0th ∆prime ◄--- Fibonacci Index #18
+-----
+11 23 2 1 1 ∆2 ◄--- 1st ∆prime ◄--- Fibonacci Index #19
+..
+..
+40 163 5 1 0 ∆31 ◄- 11th ∆prime ◄-- Fibonacci Index #29
+-----
+41 167 0 1 1 ∆0
+42 173 0 -1 1 ∆1
+43 179 0 1 1 ∆2 ◄--- ∆∆1
+44 181 1 1 1 ∆3 ◄--- ∆∆2 ◄--- 1st ∆∆prime ◄--- Fibonacci Index #30 ✔️
+..
+..
+100 521 0 -1 2 ∆59 ◄--- ∆∆17 ◄--- 7th ∆∆prime ◄--- Fibonacci Index #36 ✔️
+-----
+
p r i m e s
+1 0 0 0 0 0
+2 1 0 0 0 1
+3 2 0 1 0 2
+4 3 1 1 0 3
+5 5 2 1 0 5
+6 7 3 1 0 7
+7 11 4 1 0 11
+8 13 5 1 0 13
+9 17 0 1 1 17 ◄--- 7th prime 👉 7s ✔️
+10 19 1 1 1 ∆1 ◄--- 0th ∆prime ◄--- Fibonacci Index #18
+-----
+11 23 2 1 1 ∆2 ◄--- 1st ∆prime ◄--- Fibonacci Index #19
+..
+..
+40 163 5 1 0 ∆31 ◄- 11th ∆prime ◄-- Fibonacci Index #29 👉 11s ✔️
+-----
+41 167 0 1 1 ∆0
+42 173 0 -1 1 ∆1
+43 179 0 1 1 ∆2 ◄--- ∆∆1
+44 181 1 1 1 ∆3 ◄--- ∆∆2 ◄--- 1st ∆∆prime ◄--- Fibonacci Index #30
+..
+..
+100 521 0 -1 2 ∆59 ◄--- ∆∆17 ◄--- 7th ∆∆prime ◄--- Fibonacci Index #36 👉 7s ✔️
+-----
+
These positions: 1 7 11 13 17 19 23 29. We refer to this basic system as MEC 30 - “Mathematical Elementary Cell 30”.
This static structure is altered by the products of the primes themselves, since these products must fall into the prime positions since they are not divisible by 2, 3 and 5.
The numbers not divisible by 2, 3 or 5 are highlighted. We call them prime positions, hence 1, 7, 11, 13, 17, 19, 23, 29. Important for our work is that in the following the term prime refers only to prime numbers that are in the prime positions. So primes 2, 3 and 5 are always excluded.
p r i m e s
+1 0 0 0 0 0
+2 1 0 0 0 1 ◄--- #29 ✔️
+3 2 0 1 0 2
+4 3 1 1 0 3
+5 5 2 1 0 5
+6 7 3 1 0 7 ◄--- #23 ✔️
+7 11 4 1 0 11 ◄--- #19 ✔️
+8 13 5 1 0 13 ◄--- # 17 ✔️
+9 17 0 1 1 17 ◄--- 7th prime 👉 7s
+10 19 1 1 1 ∆1 ◄--- 0th ∆prime ◄--- Fibonacci Index #18
+-----
+11 23 2 1 1 ∆2 ◄--- 1st ∆prime ◄--- Fibonacci Index #19
+..
+..
+40 163 5 1 0 ∆31 ◄- 11th ∆prime ◄-- Fibonacci Index #29 👉 11
+-----
+41 167 0 1 1 ∆0
+42 173 0 -1 1 ∆1
+43 179 0 1 1 ∆2 ◄--- ∆∆1
+44 181 1 1 1 ∆3 ◄--- ∆∆2 ◄--- 1st ∆∆prime ◄--- Fibonacci Index #30
+..
+..
+100 521 0 -1 2 ∆59 ◄--- ∆∆17 ◄--- 7th ∆∆prime ◄--- Fibonacci Index #36 👉 7s
+-----
+
In this one system, reproduced as an icon, we can show the distribution profile of the primes as well as their products over a checkerboard-like model in the 4.
p r i m e s
+1 0 0 0 0 0
+2 1 0 0 0 1 ◄--- #29 ◄--- #61 ✔️
+3 2 0 1 0 2
+4 3 1 1 0 3
+5 5 2 1 0 5
+6 7 3 1 0 7 ◄--- #23
+7 11 4 1 0 11 ◄--- #19
+8 13 5 1 0 13 ◄--- # 17 ◄--- #49 ✔️
+9 17 0 1 1 17 ◄--- 7th prime 👉 7s
+10 19 1 1 1 ∆1 ◄--- 0th ∆prime ◄--- Fibonacci Index #18
+-----
+11 23 2 1 1 ∆2 ◄--- 1st ∆prime ◄--- Fibonacci Index #19 ◄--- #43 ✔️
+..
+..
+40 163 5 1 0 ∆31 ◄- 11th ∆prime ◄-- Fibonacci Index #29 👉 11
+-----
+41 167 0 1 1 ∆0
+42 173 0 -1 1 ∆1
+43 179 0 1 1 ∆2 ◄--- ∆∆1
+44 181 1 1 1 ∆3 ◄--- ∆∆2 ◄--- 1st ∆∆prime ◄--- Fibonacci Index #30
+..
+..
+100 521 0 -1 2 ∆59 ◄--- ∆∆17 ◄--- 7th ∆∆prime ◄--- Fibonacci Index #36 👉 7s
+-----
+
In the matrix pictured below, we list the first 24 elements of our domain, take their squares, calculate the modulo 90 congruence and digital roots of each square, and display the digital root factorization dyad for each square (and map their collective bilateral 9 sum symmetry). (PrimesDemystified)
7 x π(89) = 7 x 24 = 168 = π(1000)
p r i m e s
+1 0 0 0 0 0
+2 1 0 0 0 1 ◄--- #29 ◄--- #61
+3 2 0 1 0 2 👉 2 ✔️
+4 3 1 1 0 3 👉 61 - 1 = 60 ✔️
+5 5 2 1 0 5
+6 7 3 1 0 7 ◄--- #23
+7 11 4 1 0 11 ◄--- #19
+8 13 5 1 0 13 ◄--- # 17 ◄--- #49
+9 17 0 1 1 17 ◄--- 7th prime 👉 7s
+10 19 1 1 1 ∆1 ◄--- 0th ∆prime ◄--- Fibonacci Index #18
+-----
+11 23 2 1 1 ∆2 ◄--- 1st ∆prime ◄--- Fibonacci Index #19 ◄--- #43
+..
+..
+40 163 5 1 0 ∆31 ◄- 11th ∆prime ◄-- Fibonacci Index #29 👉 11
+-----
+41 167 0 1 1 ∆0
+42 173 0 -1 1 ∆1
+43 179 0 1 1 ∆2 ◄--- ∆∆1
+44 181 1 1 1 ∆3 ◄--- ∆∆2 ◄--- 1st ∆∆prime ◄--- Fibonacci Index #30
+..
+..
+100 521 0 -1 2 ∆59 ◄--- ∆∆17 ◄--- 7th ∆∆prime ◄--- Fibonacci Index #36 👉 7s
+-----
+
The color spin addresses for numbers are generally straightforward – a composite number takes the spin of the prior prime. 4 spins blue because 3 spins blue. 8 is red because 7 is red. However, twin primes, and the 0 type numbers between them, are open to some interpretation.
(43 - 19)the prime = 24th prime = 89
$True Prime Pairs:
+(5,7), (11,13), (17,19)
+
+layer | node | sub | i | f. MEC 30 / 2
+------+------+-----+-----+------ ‹------------------------------ 0 {-1/2}
+ | | | 1 | --------------------------
+ | | 1 +-----+ |
+ | 1 | | 2 | (5) |
+ | |-----+-----+ |
+ | | | 3 | |
+ 1 +------+ 2 +-----+---- |
+ | | | 4 | |
+ | +-----+-----+ |
+ | 2 | | 5 | (7) |
+ | | 3 +-----+ |
+ | | | 6 | 11s ‹-- ∆28 = (71-43) √
+------+------+-----+-----+------ } (36) |
+ | | | 7 | |
+ | | 4 +-----+ |
+ | 3 | | 8 | (11) |
+ | +-----+-----+ |
+ | | | 9 |‹-- ∆9 = (89-71) / 2 √ |
+ 2 +------| 5 +-----+----- |
+ | | | 10 | |
+ | |-----+-----+ |
+ | 4 | | 11 | (13) ---------------------
+ | | 6 +-----+ ‹------------------------------ 15 {0}
+ | | | 12 |---------------------------
+------+------+-----+-----+------------ |
+ | | | 13 | |
+ | | 7 +-----+ |
+ | 5 | | 14 | (17) |
+ | |-----+-----+ |
+ | | | 15 | 7s ‹-- ∆24 = (43-19) √
+ 3 +------+ 8 +-----+----- } (36) |
+ | | | 16 | |
+ | |-----+-----+ |
+ | 6 | | 17 | (19) |
+ | | 9 +-----+ |
+ | | | 18 | --------------------------
+------|------|-----+-----+----- ‹----------------------------------- 30 {+1/2}
+
The number 120 has 32 prime positions minus 5 prime number products = 27 prime numbers. The information of the prime number products translates our theory into a checkerboard-like pattern using the finite 8 prime positions from the MEC 30, we call it Ikon. 8 × 8 primary positions = 64 primary positions of the checkerboard icon.
We apply the same principle as above for the determination of the prime position. Only with the difference that we move in the even positions of the MEC 30.
7 x π(89) = 7 x 24 = 168 = π(1000)
This section is referring to wiki page-4 of zone section-4 that is inherited from the zone section-7 by prime spin-5 and span- with the partitions as below.
/lexer
(10 - 2) th prime = 8th prime = 19
The subclasses of partitions systemically develops characters similar to the distribution of prime numbers.
tps://gist.github.com/eq19/e9832026b5b78f694e4ad22c3eb6c3ef#partition-function) represents the number of possible partitions of a non-negative integer n.
f(8 twins) = 60 - 23 = 37 inner partitions
p r i m e s
+1 0 0 0 0 0
+2 1 0 0 0 1 ◄--- #29 ◄--- #61
+3 2 0 1 0 2 👉 2
+4 3 1 1 0 3 👉 89 -29 = 61 - 1 = 60 ✔️
+5 5 2 1 0 5 👉 f(37) = f(8 twins) ✔️
+6 7 3 1 0 7 ◄--- #23
+7 11 4 1 0 11 ◄--- #19
+8 13 5 1 0 13 ◄--- # 17 ◄--- #49
+9 17 0 1 1 17 ◄--- 7th prime 👉 7s
+10 19 1 1 1 ∆1 ◄--- 0th ∆prime ◄--- Fibonacci Index #18
+-----
+11 23 2 1 1 ∆2 ◄--- 1st ∆prime ◄--- Fibonacci Index #19 ◄--- #43
+..
+..
+40 163 5 1 0 ∆31 ◄- 11th ∆prime ◄-- Fibonacci Index #29 👉 11
+-----
+41 167 0 1 1 ∆0
+42 173 0 -1 1 ∆1
+43 179 0 1 1 ∆2 ◄--- ∆∆1
+44 181 1 1 1 ∆3 ◄--- ∆∆2 ◄--- 1st ∆∆prime ◄--- Fibonacci Index #30
+..
+..
+100 521 0 -1 2 ∆59 ◄--- ∆∆17 ◄--- 7th ∆∆prime ◄--- Fibonacci Index #36 👉 7s
+-----
+
7 + 13 + 19 + 25 = 64 = 8 × 8 = 8²
Let weighted points be given in the plane . For each point a radius is given which is the expected ideal distance from this point to a new facility. We want to find the location of a new facility such that the sum of the weighted errors between the existing points and this new facility is minimized. This is in fact a nonconvex optimization problem. We show that the optimal solution lies in an extended rectangular hull of the existing points. Based on this finding then an efficient big square small square (BSSS) procedure is proposed.
Integers can be considered either in themselves or as solutions to equations (Diophantine geometry).
Young diagrams associated to the partitions of the positive integers 1 through 8. They are arranged so that images under the reflection about the main diagonal of the square are conjugate partitions (Wikipedia).
f(8🪟8) = 1 + 7 + 29 = 37 inner partitions
p r i m e s
+1 0 0 0 0 0
+2 1 0 0 0 1 ◄--- #29 ◄--- #61
+3 2 0 1 0 2 👉 2
+4 3 1 1 0 3 👉 89 -29 = 61 - 1 = 60
+5 5 2 1 0 5 👉 f(37) = f(8🪟8) ✔️
+6 7 3 1 0 7 ◄--- #23
+7 11 4 1 0 11 ◄--- #19
+8 13 5 1 0 13 ◄--- # 17 ◄--- #49
+9 17 0 1 1 17 ◄--- 7th prime 👉 7s
+10 19 1 1 1 ∆1 ◄--- 0th ∆prime ◄--- Fibonacci Index #18
+-----
+11 23 2 1 1 ∆2 ◄--- 1st ∆prime ◄--- Fibonacci Index #19 ◄--- #43
+..
+..
+40 163 5 1 0 ∆31 ◄- 11th ∆prime ◄-- Fibonacci Index #29 👉 11
+-----
+41 167 0 1 1 ∆0
+42 173 0 -1 1 ∆1
+43 179 0 1 1 ∆2 ◄--- ∆∆1
+44 181 1 1 1 ∆3 ◄--- ∆∆2 ◄--- 1st ∆∆prime ◄--- Fibonacci Index #30
+..
+..
+100 521 0 -1 2 ∆59 ◄--- ∆∆17 ◄--- 7th ∆∆prime ◄--- Fibonacci Index #36 👉 7s
+-----
+
When these subclasses of partitions are flatten out into a matrix, you want to take the Jacobian of each of a stack of targets with respect to a stack of sources, where the Jacobians for each target-source pair are independent .
It’s possible to build a Hessian matrix for a Newton’s method step using the Jacobian method. You would first flatten out its axes into a matrix, and flatten out the gradient into a vector (Tensorflow).
In summary, it has been shown that partitions into an even number of distinct parts and an odd number of distinct parts exactly cancel each other, producing null terms 0x^n, except if n is a generalized pentagonal number n=g_{k}=k(3k-1)/2}, in which case there is exactly one Ferrers diagram left over, producing a term (−1)kxn. But this is precisely what the right side of the identity says should happen, so we are finished. (Wikipedia)
p r i m e s
+1 0 0 0 0 0
+2 1 0 0 0 1 ◄--- #29 ◄--- #61
+3 2 0 1 0 2 👉 2
+4 3 1 1 0 3 👉 89 -29 = 61 - 1 = 60
+5 5 2 1 0 5 👉 f(37) = f(29🪟23) ✔️
+6 7 3 1 0 7 ◄--- #23
+7 11 4 1 0 11 ◄--- #19
+8 13 5 1 0 13 ◄--- # 17 ◄--- #49
+9 17 0 1 1 17 ◄--- 7th prime 👉 7s
+10 19 1 1 1 ∆1 ◄--- 0th ∆prime ◄--- Fibonacci Index #18
+-----
+11 23 2 1 1 ∆2 ◄--- 1st ∆prime ◄--- Fibonacci Index #19 ◄--- #43
+..
+..
+40 163 5 1 0 ∆31 ◄- 11th ∆prime ◄-- Fibonacci Index #29 👉 11
+-----
+41 167 0 1 1 ∆0
+42 173 0 -1 1 ∆1
+43 179 0 1 1 ∆2 ◄--- ∆∆1
+44 181 1 1 1 ∆3 ◄--- ∆∆2 ◄--- 1st ∆∆prime ◄--- Fibonacci Index #30
+..
+..
+100 521 0 -1 2 ∆59 ◄--- ∆∆17 ◄--- 7th ∆∆prime ◄--- Fibonacci Index #36 👉 7s
+-----
+
The code is interspersed with python, shell, perl, also demonstrates how multiple languages can be integrated seamlessly.
These include generating variants of their abundance profile, assigning taxonomy and finally generating a rooted phylogenetic tree.
p r i m e s
+1 0 0 0 0 0
+2 1 0 0 0 1 ◄--- #29 ◄--- #61
+3 2 0 1 0 2 👉 2
+4 3 1 1 0 3 👉 89 - 29 = 61 - 1 = 60
+5 5 2 1 0 5 👉 f(37) = ❓ 👈 Composite ✔️
+6 7 3 1 0 7 ◄--- #23
+7 11 4 1 0 11 ◄--- #19
+8 13 5 1 0 13 ◄--- # 17 ◄--- #49
+9 17 0 1 1 17 ◄--- 7th prime 👉 7s 👈 Composite ✔️
+10 19 1 1 1 ∆1 ◄--- 0th ∆prime ◄--- Fibonacci Index #18
+-----
+11 23 2 1 1 ∆2 ◄--- 1st ∆prime ◄--- Fibonacci Index #19 ◄--- #43
+..
+..
+40 163 5 1 0 ∆31 ◄- 11th ∆prime ◄-- Fibonacci Index #29 👉 11
+-----
+41 167 0 1 1 ∆0
+42 173 0 -1 1 ∆1
+43 179 0 1 1 ∆2 ◄--- ∆∆1
+44 181 1 1 1 ∆3 ◄--- ∆∆2 ◄--- 1st ∆∆prime ◄--- Fibonacci Index #30
+..
+..
+100 521 0 -1 2 ∆59 ◄--- ∆∆17 ◄--- 7th ∆∆prime ◄--- Fibonacci Index #36 👉 7s
+-----
+
This behaviour in a fundamental causal relation to the primes when the products are entered into the partitions system.
The subclasses of partitions systemically develops characters similar to the distribution of prime numbers. It would mean that there should be some undiscovered things hidden within the residual of the decimal values.
168 + 2 = 170 = (10+30)+60+70 = 40+60+70 = 40 + 60 + ∆(2~71)
p r i m e s
+1 0 0 0 0 0
+2 1 0 0 0 1 ◄--- #29 ◄--- #61
+3 2 0 1 0 2 👉 2
+4 3 1 1 0 3 👉 89 - 29 = 61 - 1 = 60
+5 5 2 1 0 5 👉 f(37) ✔️
+ 6 👉 11s Composite Partition ✔️
+6 7 3 1 0 7 ◄--- #23
+7 11 4 1 0 11 ◄--- #19
+8 13 5 1 0 13 ◄--- # 17 ◄--- #49
+9 17 0 1 1 17 ◄--- 7th prime
+ 18 👉 7s Composite Partition ✔️
+10 19 1 1 1 ∆1 ◄--- 0th ∆prime ◄--- Fibonacci Index #18
+-----
+11 23 2 1 1 ∆2 ◄--- 1st ∆prime ◄--- Fibonacci Index #19 ◄--- #43
+..
+..
+40 163 5 1 0 ∆31 ◄- 11th ∆prime ◄-- Fibonacci Index #29 👉 11
+-----
+41 167 0 1 1 ∆0
+42 173 0 -1 1 ∆1
+43 179 0 1 1 ∆2 ◄--- ∆∆1
+44 181 1 1 1 ∆3 ◄--- ∆∆2 ◄--- 1st ∆∆prime ◄--- Fibonacci Index #30
+..
+..
+100 521 0 -1 2 ∆59 ◄--- ∆∆17 ◄--- 7th ∆∆prime ◄--- Fibonacci Index #36 👉 7s
+-----
+
The initial concept of this work was the Partitioned Matrix of an even number w≥ 4:
To analyze the adequacy of the proposed formulas, probabilistically calculated reference values were adopted. (Partitions of even numbers - pdf)
p r i m e s
+1 0 0 0 0 0
+2 1 0 0 0 1 ◄--- #29 ◄--- #61
+3 2 0 1 0 2 👉 2
+4 3 1 1 0 3 👉 89 - 29 = 61 - 1 = 60
+5 5 2 1 0 5 👉 11 + 29 = 37 + 3 = 40 ✔️
+ 6 👉 11s Composite Partition ◄--- 2+60+40 = 102 ✔️
+6 7 3 1 0 7 ◄--- #23
+7 11 4 1 0 11 ◄--- #19
+8 13 5 1 0 13 ◄--- # 17 ◄--- #49
+9 17 0 1 1 17 ◄--- 7th prime
+ 18 👉 7s Composite Partition
+10 19 1 1 1 ∆1 ◄--- 0th ∆prime ◄--- Fibonacci Index #18
+-----
+11 23 2 1 1 ∆2 ◄--- 1st ∆prime ◄--- Fibonacci Index #19 ◄--- #43
+..
+..
+40 163 5 1 0 ∆31 ◄- 11th ∆prime ◄-- Fibonacci Index #29 👉 11
+-----
+41 167 0 1 1 ∆0
+42 173 0 -1 1 ∆1
+43 179 0 1 1 ∆2 ◄--- ∆∆1
+44 181 1 1 1 ∆3 ◄--- ∆∆2 ◄--- 1st ∆∆prime ◄--- Fibonacci Index #30
+..
+..
+100 521 0 -1 2 ∆59 ◄--- ∆∆17 ◄--- 7th ∆∆prime ◄--- Fibonacci Index #36 👉 7s
+-----
+
(11x7) + (29+11) + (25+6) + (11+7) + 4 = 77+40+31+18+4 = 170
This section is referring to wiki page-5 of gist section-1 that is inherited from the gist section-13 by prime spin-7 and span- with the partitions as below.
/lexer
The number 120 = MEC30 x 4 has 32 prime positions minus 5 prime number products = 27 prime numbers. The information of the prime number products translates our theory into a checkerboard-like pattern using the finite 8 prime positions from the MEC 30, we call it Ikon. 8 × 8 primary positions = 64 primary positions of the checkerboard icon.
Note that the hexagon in the middle has 37 circles and the total figure, a star of David has 73. For this one you go around one point of the pattern in a circle until you go past a letter that you have already covered. For instance in B-R-A-Sh you will have to switch the position for the Sh because it moves more than through the alphabet. S-I-T does the same with the T.
The above seven (7) primes will act then as extended branes. This is what we mean by addition zones and it happens whenever a cycle is restarted.
$True Prime Pairs:
+(5,7), (11,13), (17,19)
+
+layer | node | sub | i | f. MEC 30 / 2
+------+------+-----+-----+------ ‹------------------------------ 0 {-1/2}
+ | | | 1 | --------------------------
+ | | 1 +-----+ |
+ | 1 | | 2 | (5) |
+ | |-----+-----+ |
+ | | | 3 | |
+ 1 +------+ 2 +-----+---- |
+ | | | 4 | |
+ | +-----+-----+ |
+ | 2 | | 5 | (7) |
+ | | 3 +-----+ |
+ | | | 6 | 11s ‹-- ∆28 = (71-43)
+------+------+-----+-----+------ } (36) |
+ | | | 7 | |
+ | | 4 +-----+ |
+ | 3 | | 8 | (11) |
+ | +-----+-----+ |
+ | | | 9 |‹-- ∆9 = (89-71) / 2 |
+ 2 +------| 5* +-----+----- |
+ | | | 10 | |
+ | |-----+-----+ |
+ | 4 | | 11 | (13) ---------------------
+ | | 6 +-----+ ‹------------------------------ 15 {0}
+ | | | 12 |---------------------------
+------+------+-----+-----+------------ |
+ | | | 13 | |
+ | | 7 +-----+ |
+ | 5 | | 14 | (17) |
+ | |-----+-----+ |
+ | | | 15 | 7 x 24 = 168 ✔️
+ 3* +------+ 8 +-----+----- } (36) |
+ | | | 16 | |
+ | |-----+-----+ |
+ | 6 | | 17 | (19) |
+ | | 9 +-----+ |
+ | | | 18 | --------------------------
+------|------|-----+-----+----- ‹----------------------------------- 30 {+1/2}
+
This scheme goes to the unification of 11s with 7s to 18s meanwhile the 11th it self behave as residual by the 5th minor hexagon between the 30 to 36' cells.
1 | 2 | 3 | 4 | 5 | 6 | 7 | 8 | 9 | 10 | 11 | 12 | 13 | 14 | 15 | 16 | 17 | 18
+---+---+---+---+---+---+---+---+---+----+----+----+----+----+----+----+----+----
+ 19| 20| 21| 22| 23| 24| 25|
+---+---+---+---+---+---+---+
+ - | - | - | 28| 29|
+
By The Δ(19 vs 18) Scenario those three are exactly landed in the 0's cell out of Δ18. See that the sum of 30 and 36 is 66 while the difference between 36 and 102 is also 66.
You likely noticed I began with 2 rather than 1 or 0 when I first constructed the hexagon. Why? Because they do not fit inside — they stick off the hexagon like a tail. Perhaps that’s where they belong. However, if one makes a significant and interesting assumption, then 1 and 0 fall in their logical locations – in the 1 and 0 cells, respectively. _(HexSpin)
0 + 30 + 36 + 102 = 168 = π(1000)
0 | 1 | 2 | 3 | 4 | 5 | 6 | 7 | 8 | 9 | 10 | 11 | 12 | 13 | 14 | 15 | 16 | 17
+---+---+---+---+---+---+---+---+---+---+----+----+----+----+----+----+----+----
+ - | - | 20| 21| 22| 23| 24| 25|
+---+---+---+---+---+---+---+
+ - | - | - | - | 28| 29|
+---+---+---+---+---+---+
+ 30| 31|
+---+---+
+ 36|
+
This behaviour finaly brings us to a suggestion that the dimension in string theory are linked with the prime distribution level as indicated by the self repetition on MEC30.
7th spin - 4th spin = (168 - 102)s = 66s = 6 x 11s = 30s + 36s
p r i m e s
+1 0 0 0 0 0
+2 1 0 0 0 1 ◄--- #29 ◄--- #61 👈 1st spin ✔️
+3 2 0 1 0 2 👉 2
+4 3 1 1 0 3 👉 89 - 29 = 61 - 1 = 60
+5 5 2 1 0 5 👉 11 + 29 = 37 + 3 = 40
+ 6 👉 11s Composite Partition ◄--- 102 👈 4th spin ✔️
+6 7 3 1 0 7 ◄--- #23
+7 11 4 1 0 11 ◄--- #19
+8 13 5 1 0 13 ◄--- # 17 ◄--- #49
+9 17 0 1 1 17 ◄--- 7th prime
+ 18 👉 7s Composite Partition ◄--- 168 👈 7th spin ✔️
+10 19 1 1 1 ∆1 ◄--- 0th ∆prime ◄--- Fibonacci Index #18
+-----
+11 23 2 1 1 ∆2 ◄--- 1st ∆prime ◄--- Fibonacci Index #19 ◄--- #43
+..
+..
+40 163 5 1 0 ∆31 ◄- 11th ∆prime ◄-- Fibonacci Index #29 👉 11
+-----
+41 167 0 1 1 ∆0
+42 173 0 -1 1 ∆1
+43 179 0 1 1 ∆2 ◄--- ∆∆1
+44 181 1 1 1 ∆3 ◄--- ∆∆2 ◄--- 1st ∆∆prime ◄--- Fibonacci Index #30
+..
+..
+100 521 0 -1 2 ∆59 ◄--- ∆∆17 ◄--- 7th ∆∆prime ◄--- Fibonacci Index #36 👉 7s
+-----
+
It will be forced back to Δ19 making a cycle that bring back the 12 to → 13 of 9 collumns and replicate The Scheme 13:9 through (i=9,k=13)=9x3=27 with entry form of (100/50=2,60,40) as below:
The 10 ranks will coordinate with the 18 to raise up the symmetrical behaviour of 12+24=36 which is prime pair 17+19=36 and let the 2 and 3 out of 2,3,5,7 to begin a new cycle while the 5,7 will pair the 11,13 and 17,19 as True Prime Pairs.
I like that 0 can occupy a center point. Incidentally, this circular shape minus all my numbers and colors s has been called Seed of Life / Flower of Life by certain New Age groups who claim it has a sacred geometry. Please don’t see this as an endorsement of any spiritual group or religion. (Prime Hexagon - Circulat Form)
This section is referring to wiki page-6 of gist section-2 that is inherited from the gist section-29 by prime spin-11 and span- with the partitions as below.
/lexer
There are some mathematical shape of this residual objects. Torus is basically a donut shape, which has the property of of having variable Gaussian curvature.
The blue parts of the torus above have positive curvature, the red parts negative and the top grey band has zero curvature. If our 3 dimensional space was like the surface areas of a 4 dimensional torus, the parts would have different angle sums.
Some parts of the surface has positive curvature, others zero, others negative.
If you start anywhere on its surface and follow the curvature round you will eventually return to the same place having travelled on every part of the surface.
Mobius strip only has one side, there are two more bizarre shapes with strange properties.
The Klein bottleis in someways a 3D version of the Mobius strip and even though it exists in 3 dimensions, to make a true one you need to "fold through" the 4th dimension.
In mathematics, the Klein bottle (/ˈklaɪn/) is an example of a non-orientable surface; that is, informally, a one-sided surface which, if traveled upon, could be followed back to the point of origin while flipping the traveler upside down.
While a Möbius strip is a surface with a boundary, a Klein bottle has no boundary. For comparison, a sphere is an orientable surface with no boundary.
A sign inversion visualized as a vector pointing along the Möbius band when the circle is continuously rotated through a full turn of 360°.
A spinor associated to the conformal group of the circle, exhibiting a sign inversion on a full rotation of the circle through an angle of 2π.
(17+13) + (11+19) = (7+11) + (19+23) = 60
Eigennvalue curves (right) showing a triple eigenvalue at zero for τ = 1 and double eigenvalues at 1 ± √2i for τ = √43. On the left the graph of 1/|Q(λ)| with the same eigenvalue curves plotted in the ground plane. Green stars indicate the eigenvalues of A, blue stars the roots of puv(λ) and triangles the zeroes of Q0(λ)
7 + 11 + 13 = 31 1 + (26+6) + (27+6) = 66
0 | 1 | 2 | 3 | 4 | 5 | 6 | 7 | 8 | 9 | 10 | 11 | 12 | 13 | 14 | 15 | 16 | 17
+---+---+---+---+---+---+---+---+---+---+----+----+----+----+----+----+----+----
+ - | - | 20| 21| 22| 23| 24| 25|
+---+---+---+---+---+---+---+---+
+ - | - | - | - | 28| 29| ◄--- missing 26 & 27 ✔️
+---+---+---+---+---+---+
+ 30| 31| - | - | ◄--- missing 32 & 33 ✔️
+---+---+---+---+
+ 36|
+
This behaviour finaly brings us to a suggestion that the dimension in string theory are linked with the prime distribution level as indicated by the self repetition on MEC30.
7th spin - 4th spin = (168 - 102)s = 66s = 6 x 11s = 30s + 36s
$True Prime Pairs:
+(5,7), (11,13), (17,19)
+
+layer | node | sub | i | f. MEC 30 / 2
+------+------+-----+-----+------ ‹------------------------------ 0 {-1/2}
+ | | | 1 | --------------------------
+ | | 1 +-----+ |
+ | 1 | | 2 | (5) |
+ | |-----+-----+ |
+ | | | 3 | |
+ 1 +------+ 2 +-----+---- |
+ | | | 4 | |
+ | +-----+-----+ |
+ | 2 | | 5 | (7) |
+ | | 3 +-----+ |
+ | | | 6 | 11s ‹-- ∆28 = (71-43) √
+------+------+-----+-----+------ } (36) |
+ | | | 7 | |
+ | | 4 +-----+ |
+ | 3 | | 8 | (11) |
+ | +-----+-----+ |
+ | | | 9 |‹-- ∆9 = (89-71) / 2 √ |
+ 2 +------| 5* +-----+----- |
+ | | | 10 | |
+ | |-----+-----+ |
+ | 4 | | 11 | (13) ---------------------
+ | | 6 +-----+ ‹------------------------------ 15 {0}
+ | | | 12 |---------------------------
+------+------+-----+-----+------------ |
+ | | | 13 | |
+ | | 7 +-----+ |
+ | 5 | | 14 | (17) |
+ | |-----+-----+ |
+ | | | 15 | 7 x 24 = 168 √
+ 3* +------+ 8 +-----+----- } (36) |
+ | | | 16 | |
+ | |-----+-----+ |
+ | 6 | | 17 | (19) |
+ | | 9 +-----+ |
+ | | | 18 | --------------------------
+------|------|-----+-----+----- ‹----------------------------------- 30 {+1/2}
+
This model may explains the newly discovered prime number theorem in relatively simple layman's terms for anyone with a slight background in theoretical physics.
The property gives an in depth analysis of the not so random distribution of primes by showing how it has solved Goldbach’s conjecture and the Ulam spiral.
The model suggests a possible origin for both charge and half-integer spin and also reconciles the apparently contradictory criteria discussed above.
Arbitrary sequence of three (3) consecutive nucleotides along a helical path whose metric distances satisfy the relationship dn,n+3dn,n+2dn,n+1.
Optimally overlapping bps are indicated by the presence of the ovals (m) measures the overlapping resonance correlation length. (π − π orbital resonance in twisting duplex DNA)
Under certain conditions, energy could not take on any indiscriminate value, the energy must be some multiple of a very small quantity (later to be known as a quantum).
Twisted strip model for one wavelength of a photon with circular polarisation in at space. A similar photon in a closed path in curved space with periodic boundary conditions of length C.
The magnetic moment ~, angular momentum L~, and direction of propagation with velocity c are also indicated. (Is the electron a photon with toroidal topology? - pdf)
A deeper understanding requires a uni cation of the aspects discussed above in terms of an underlying principle.
This section is referring to wiki page-7 of gist section-3 that is inherited from the gist section-37 by prime spin-13 and span- with the partitions as below.
/lexer
36 + 36 - 6 partitions = 72 - 6 = 66 = 30+36 = 6x11
$True Prime Pairs:
+ (5,7), (11,13), (17,19)
+
+ layer| i | f
+ -----+-----+---------
+ | 1 | 5
+ 1 +-----+
+ | 2 | 7
+ -----+-----+--- } 36 » 6®
+ | 3 | 11
+ 2 +-----+
+ | 4 | 13
+ -----+-----+---------
+ | 5 | 17
+ 3 +-----+ } 36 » 6®
+ | 6 | 19
+ -----+-----+---------
+
#!/usr/bin/env python
+
+import numpy as np
+from scipy import linalg
+
+class SU3(np.matrix):
+ GELLMANN_MATRICES = np.array([
+ np.matrix([ #lambda_1
+ [0, 1, 0],
+ [1, 0, 0],
+ [0, 0, 0],
+ ], dtype=np.complex),
+ np.matrix([ #lambda_2
+ [0,-1j,0],
+ [1j,0, 0],
+ [0, 0, 0],
+ ], dtype=np.complex),
+ np.matrix([ #lambda_3
+ [1, 0, 0],
+ [0,-1, 0],
+ [0, 0, 0],
+ ], dtype=np.complex),
+ np.matrix([ #lambda_4
+ [0, 0, 1],
+ [0, 0, 0],
+ [1, 0, 0],
+ ], dtype=np.complex),
+ np.matrix([ #lambda_5
+ [0, 0,-1j],
+ [0, 0, 0 ],
+ [1j,0, 0 ],
+ ], dtype=np.complex),
+ np.matrix([ #lambda_6
+ [0, 0, 0],
+ [0, 0, 1],
+ [0, 1, 0],
+ ], dtype=np.complex),
+ np.matrix([ #lambda_7
+ [0, 0, 0 ],
+ [0, 0, -1j],
+ [0, 1j, 0 ],
+ ], dtype=np.complex),
+ np.matrix([ #lambda_8
+ [1, 0, 0],
+ [0, 1, 0],
+ [0, 0,-2],
+ ], dtype=np.complex) / np.sqrt(3),
+ ])
+
+
+ def computeLocalAction(self):
+ pass
+
+ @classmethod
+ def getMeasure(self):
+ pass
+
Now the following results: Due to the convolution and starting from the desired value of the prime position pairs, the product templates and prime numbers templates of the prime number 7 lie in the numerical Double strand parallel opposite.
In number theory, the partition functionp(n) represents the number of possible partitions of a non-negative integer n.
Integers can be considered either in themselves or as solutions to equations (Diophantine geometry).
Young diagrams associated to the partitions of the positive integers 1 through 8. They are arranged so that images under the reflection about the main diagonal of the square are conjugate partitions (Wikipedia).
By parsering π(1000)=168 primes of the 1000 id’s across π(π(10000))-1=200 of this syntax then the (Δ1) would be initiated. Based on Assigning Sitemap priority values You may see them are set 0.75 – 1.0 on the sitemap’s index:
Priority Page Name
+1 Homepage
+0.9 Main landing pages
+0.85 Other landing pages
+0.8 Main links on navigation bar
+0.75 Other pages on site
+0.8 Top articles/blog posts
+0.75 Blog tag/category pages
+0.4 – 0.7 Articles, blog posts, FAQs, etc.
+0.0 – 0.3 Outdated information or old news that has become less relevant
+
By this object orientation then the reinjected primes from the π(π(10000))-1=200 will be (168-114)+(160-114)=54+46=100. Here are our layout that is provided using Jekyll/Liquid to facilitate the cycle:
100 + 68 + 32 = 200
$True Prime Pairs:
+(5,7), (11,13), (17,19)
+
+layer | node | sub | i | f. MEC 30 / 2
+------+------+-----+-----+------ ‹--------------------------- 30 {+1/2} √
+ | | | 1 | --------------------------
+ | | 1 +-----+ |
+ | 1 | | 2 | (5) |
+ | |-----+-----+ |
+ | | | 3 | |
+ 1 +------+ 2 +-----+---- |
+ | | | 4 | |
+ | +-----+-----+ |
+ | 2 | | 5 | (7) |
+ | | 3 +-----+ |
+ | | | 6 | 11s
+------+------+-----+-----+------ } (36) |
+ | | | 7 | |
+ | | 4 +-----+ |
+ | 3 | | 8 | (11) |
+ | +-----+-----+ |
+ | | | 9 |‹-- |
+ 2 +------| 5* +-----+----- |
+ | | | 10 | |
+ | |-----+-----+ |
+ | 4 | | 11 | (13) --------------------- 32 √
+ | | 6 +-----+ ‹------------------------------ 15 {0} √
+ | | | 12 |---------------------------
+------+------+-----+-----+------------ |
+ | | | 13 | |
+ | | 7 +-----+ |
+ | 5 | | 14 | (17) |
+ | |-----+-----+ |
+ | | | 15 | 7s = f(1000)
+ 3* +------+ 8 +-----+----- } (36) |
+ | | | 16 | |
+ | |-----+-----+ |
+ | 6 | | 17 | (19) |
+ | | 9 +-----+ |
+ | | | 18 | -------------------------- 68 √
+------|------|-----+-----+----- ‹------ 0 {-1/2} √
+
p r i m e s
+1 0 0 0 0 0
+2 1 0 0 0 1 ◄--- #29 ◄--- #61 👈 1st spin
+3 2 0 1 0 2 👉 2
+4 3 1 1 0 3 👉 89 - 29 = 61 - 1 = 60
+5 5 2 1 0 5 👉 11 + 29 = 37 + 3 = 40
+ 6 👉 11s Composite Partition ◄--- 102 👈 4th spin
+6 7 3 1 0 7 ◄--- #23 👈 7+23 = 30 ✔️
+7 11 4 1 0 11 ◄--- #19 👈 11+19 = 30 ✔️
+8 13 5 1 0 13 ◄--- #17 ◄--- #49 👈 13+17 = 30 ✔️
+9 17 0 1 1 17 ◄--- 7th prime👈 17+7 != 30❓
+ 18 👉 7s Composite Partition ◄--- 168 👈 7th spin
+10 19 1 1 1 ∆1 ◄--- 0th ∆prime ◄--- Fibonacci Index #18
+-----
+11 23 2 1 1 ∆2 ◄--- 1st ∆prime ◄--- Fibonacci Index #19 ◄--- #43
+..
+..
+40 163 5 1 0 ∆31 ◄- 11th ∆prime ◄-- Fibonacci Index #29 👉 11
+-----
+41 167 0 1 1 ∆0
+42 173 0 -1 1 ∆1
+43 179 0 1 1 ∆2 ◄--- ∆∆1
+44 181 1 1 1 ∆3 ◄--- ∆∆2 ◄--- 1st ∆∆prime ◄--- Fibonacci Index #30
+..
+..
+100 521 0 -1 2 ∆59 ◄--- ∆∆17 ◄--- 7th ∆∆prime ◄--- Fibonacci Index #36 👉 7s
+-----
+
By taking a distinc function between f(π) as P vs f(i) as NP where eiπ + 1 = 0 then theoretically they shall be correlated to get an expression of the prime platform similar to the Mathematical Elementary Cell 30 (MEC30).
∆17 + ∆49 = ∆66
p r i m e s
+1 0 0 0 0 0
+2 1 0 0 0 1 ◄--- #29 ◄--- #61 👈 1st spin
+3 2 0 1 0 2 👉 2
+4 3 1 1 0 3 👉 89 - 29 = 61 - 1 = 60
+5 5 2 1 0 5 👉 11 + 29 = 37 + 3 = 40
+ 6 👉 11s Composite Partition ◄--- 102 👈 4th spin
+6 7 3 1 0 7 ◄--- #23 👈 part of MEC30 ✔️
+7 11 4 1 0 11 ◄--- #19 👈 part of MEC30 ✔️
+8 13 5 1 0 13 ◄--- #17 ◄--- #49 👈 part of MEC30 ✔️
+9 17 0 1 1 17 ◄--- 7th prime👈 not part of MEC30 ❓
+ 18 👉 7s Composite Partition ◄--- 168 👈 7th spin
+10 19 1 1 1 ∆1 ◄--- 0th ∆prime ◄--- Fibonacci Index #18
+-----
+11 23 2 1 1 ∆2 ◄--- 1st ∆prime ◄--- Fibonacci Index #19 ◄--- #43
+..
+..
+40 163 5 1 0 ∆31 ◄- 11th ∆prime ◄-- Fibonacci Index #29 👉 11
+-----
+41 167 0 1 1 ∆0
+42 173 0 -1 1 ∆1
+43 179 0 1 1 ∆2 ◄--- ∆∆1
+44 181 1 1 1 ∆3 ◄--- ∆∆2 ◄--- 1st ∆∆prime ◄--- Fibonacci Index #30
+..
+..
+100 521 0 -1 2 ∆59 ◄--- ∆∆17 ◄--- 7th ∆∆prime ◄--- Fibonacci Index #36 👉 7s
+-----
+
∆102 - ∆2 - ∆60 = ∆40
p r i m e s
+1 0 0 0 0 0
+2 1 0 0 0 1 ◄--- #29 ◄--- #61 👈 1st spin
+3 2 0 1 0 2 👉 2
+4 3 1 1 0 3 👉 89 - 29 = 61 - 1 = 60
+5 5 2 1 0 5 👉 11 + 29 = 37 + 3 = 40
+ 6 👉 11s Composite Partition ◄--- 102 👈 4th spin
+6 7 3 1 0 7 ◄--- #23 👈 30 ◄--- break MEC30 symmetry ✔️
+7 11 4 1 0 11 ◄--- #19 👈 30 ✔️
+8 13 5 1 0 13 ◄--- #17 ◄--- #49 👈 30 ✔️
+9 17 0 1 1 17 ◄--- 7th prime👈 not part of MEC30 ❓
+ 18 👉 7s Composite Partition ◄--- 168 👈 7th spin
+10 19 1 1 1 ∆1 ◄--- 0th ∆prime ◄--- Fibonacci Index #18
+-----
+11 23 2 1 1 ∆2 ◄--- 1st ∆prime ◄--- Fibonacci Index #19 ◄--- #43
+..
+..
+40 163 5 1 0 ∆31 ◄- 11th ∆prime ◄-- Fibonacci Index #29 👉 11
+-----
+41 167 0 1 1 ∆0
+42 173 0 -1 1 ∆1
+43 179 0 1 1 ∆2 ◄--- ∆∆1
+44 181 1 1 1 ∆3 ◄--- ∆∆2 ◄--- 1st ∆∆prime ◄--- Fibonacci Index #30
+..
+..
+100 521 0 -1 2 ∆59 ◄--- ∆∆17 ◄--- 7th ∆∆prime ◄--- Fibonacci Index #36 👉 7s
+-----
+
The partitions of odd composite numbers (Cw) are as important as the partitions of prime numbers or Goldbach partitions (Gw). The number of partitions Cw is fundamental for defining the available lines (Lwd) in a Partitioned Matrix that explain the existence of partitions Gw or Goldbach partitions. (Partitions of even numbers - pdf)
30s + 36s (addition) = 6 x 11s (multiplication) = 66s
p r i m e s
+1 0 0 0 0 0
+2 1 0 0 0 1 ◄--- #29 ◄--- #61 👈 1st spin
+3 2 0 1 0 2 👉 2
+4 3 1 1 0 3 👉 89 - 29 = 61 - 1 = 60
+5 5 2 1 0 5 👉 11 + 29 = 37 + 3 = 40
+ 6 👉 11s Composite Partition ◄--- 102 👈 4th spin
+6 7 3 1 0 7 ◄--- #23 👈 f(#30) ◄--- break MEC30 symmetry
+7 11 4 1 0 11 ◄--- #19 👈 30
+8 13 5 1 0 13 ◄--- #17 ◄--- #49 👈 30
+9 17 0 1 1 17 ◄--- 7th prime 👈 f(#36) ◄--- antisymmetric state ✔️
+ 18 👉 7s Composite Partition ◄--- 168 👈 7th spin
+10 19 1 1 1 ∆1 ◄--- 0th ∆prime ◄--- Fibonacci Index #18
+-----
+11 23 2 1 1 ∆2 ◄--- 1st ∆prime ◄--- Fibonacci Index #19 ◄--- #43
+..
+..
+40 163 5 1 0 ∆31 ◄- 11th ∆prime ◄-- Fibonacci Index #29 👉 11
+-----
+41 167 0 1 1 ∆0
+42 173 0 -1 1 ∆1
+43 179 0 1 1 ∆2 ◄--- ∆∆1
+44 181 1 1 1 ∆3 ◄--- ∆∆2 ◄--- 1st ∆∆prime ◄--- Fibonacci Index #30
+..
+..
+100 521 0 -1 2 ∆59 ◄--- ∆∆17 ◄--- 7th ∆∆prime ◄--- Fibonacci Index #36 👉 7s
+-----
+
By this chapter we are going to learn whether the spin discussed in prime hexagon has something to do with the nature so we begin with the spin in physic
This section is referring to wiki page-8 of gist section-4 that is inherited from the gist section-53 by prime spin-17 and span- with the partitions as below.
/lexer
Spin is an intrinsic form of angular momentum carried by elementary particles, and thus by composite particles such as hadrons, atomic nuclei, and atoms.
There are two (2) types force carriers and three (3) type of generations. The origin of multiple generations of the particular count of 3, is an unsolved problem of physics.
In particle physics, a generation or family is a division of the elementary particles.
The basic features of quark–lepton generation or families, such as their masses and mixings etc., can be described by some of the proposed family symmetries.
A lepton is a particle of half-integer spin (spin 1⁄2) while a boson has integer spin: scalar boson (spin = 0), vector bosons (spin = 1) and tensor boson (spin = 2).
Those particles with half-integer spins, are known as fermions, while those particles with integer spins, such as 0, 1, 2, are known as bosons.
For example, a helium-4 atom in the ground state has spin 0 and behaves like a boson, even though the quarks and electrons which make it up are all fermions. (Wikipedia)
Quantum field theory is any theory that describes a quantized field.
This theory describes all the known fields and all the known interactions other than gravity. (Quora)
Experimental observation of the SM particles was completed by the discoveries of top quark (1995), direct interaction of tau neutrino (2000), and Higgs boson (2013).
Feynman diagram of the fusion of two (2) electroweak vector bosons to the scalar Higgs boson, which is a prominent process of the generation of Higgs bosons at particle accelerators. (The symbol q means a quark particle, W and Z are the vector bosons of the electroweak interaction. H° is the Higgs boson.) (Wikipedia)
There are three (3) generations of quarks (up/down, strange/charm, and top/bottom), along with three (3) generations of leptons (electron, muon, and tau). All of these particles have been observed experimentally, and we don’t seem to have seen anything new along these lines. A priori, this doesn’t eliminate the possibility of a fourth generation, but the physicists I’ve spoken to do not think additional generations are likely. (StackExchange)
The construction 🏗️ of Standard Model took a long time to build. Physicist J.J. Thomson discovered the electron in 1897, and scientists at the Large Hadron Collider found the final piece of the puzzle, the Higgs boson, in 2012.
In particle physics, a vector boson is a boson whose spin equals one. Vector bosons that are also elementary particles are gauge bosons, the force carriers of fundamental interactions. Some composite particles are vector bosons, for instance any vector meson (quark and antiquark).
In the SM interactions are determined by a gauge quantum field theory containing the internal symmetries of the unitary group product SU(3)C × SU(2)L × U(1)Y [?].
In the Standard Model, the Higgs boson is a massive scalar boson whose mass must be found experimentally. It is the only particle that remains massive even at high energies.
The Higgs boson field (often referred to as the God particle) is a scalar field with two neutral and two electrically charged components that form a complex doublet of the weak isospin SU(2) symmetry.
Also, physicists understand that about 95 percent of the universe is not made of ordinary matter as we know it. Instead, much of the universe consists of dark matter and dark energy that do not fit into the Standard Model.
It has zero spin, even (positive) parity, no electric charge, and no colour charge, and it couples to (interacts with) mass.
So now I will attempt to show the minor hexagons are significant. This is not easy as they are linked to the nature of prime numbers, and nothing is easy about the nature of prime numbers. But I begin with this assumption: if the hexagons participate in the Universe in any way other than haphazardly, they must be demonstrably congruent to something organized. That is, if I can show they are organized (not random) in relation to some other thing, then primes and the thing are linked. (Hexspin)
7th spin - 4th spin = (168 - 102)s = 66s = 6 x 11s = 30s + 36s
In particle physics, an elementary particle or fundamental particle is a subatomic particle that is not composed of other particles.
The Standard Model presently recognizes seventeen distinct particles (twelve fermions and five bosons). As a consequence of flavor and color combinations and antimatter, the fermions and bosons are known to have 48 and 13 variations, respectively. Among the 61 elementary particles embraced by the Standard Model number electrons and other leptons, quarks, and the fundamental bosons. (Wikipedia)
Subatomic particles such as protons or neutrons, which contain two or more elementary particles, are known as composite particles.
The Standard Model of Particle Physics, describes for us all know fundamental interaction in nature till date, with the exception of Gravity (work on this front is going on). Here is a summary of the fundamental content of the standard model
They interact, they transfer energy and momentum and angular momentum; excitations are created and destroyed. Every excitation that’s possible has a reverse excitation. (Quora)
The SM was basically developed in 1970-s. It describes the electromagnetic, weak and strong fundamental interactions.
The Standard Model explains three of the four fundamental forces that govern the universe: electromagnetism, the strong force, and the weak force.
The fourth fundamental force is gravity, which is not adequately explained by the Standard Model.
By our project the 18’s on the gist will cover five (5) unique functions that behave as one (1) central plus four (4) zones. This scheme will be implemented to all of the 168 repositories as bilateral way (in-out) depend on their postion on the system. So along with the gist it self then there shall be 1 + 168 = 169
units of 1685 root functions.
5 + 2 x 5 x 168 = 5 + 1680 = 1685 root functions
It is supposed that elementary particles participate in gravitational interactions as well, though there is no sufficient quantum gravity theory.
Elementary particles are classified according to their spin. Fermions are one of the two fundamental classes of particles, the other being bosons. Fermions have half-integer spin while bosons have integer spin.
According to the Standard Model there are five (5) elementary bosons:
These four are the gauge bosons:
A second order tensor boson (spin = 2) called the graviton (G) has been hypothesised as the force carrier for gravity, but so far all attempts to incorporate gravity into the Standard Model have failed.
The diagram shows the elementary particles of the Standard Model (the Higgs boson, the three generations of quarks and leptons, and the gauge bosons), including their names, masses, spins, charges, chiralities, and interactions with the strong, weak and electromagnetic forces. It also depicts the crucial role of the Higgs boson in Electroweak Symmetry Breaking, and shows how the properties of the various particles differ in the (high-energy) symmetric phase (top) and the (low-energy) broken-symmetry phase (bottom). (Wikipedia)
Theories that lie beyond the Standard Model include various extensions of the standard model through supersymmetry, such as the Minimal Supersymmetric Standard Model (MSSM) and Next-to-Minimal Supersymmetric Standard Model (NMSSM), and entirely novel explanations, such as string theory, M-theory, and extra dimensions. As these theories tend to reproduce the entirety of current phenomena, the question of which theory is the right one, or at least the “best step” towards a Theory of Everything, can only be settled via experiments, and is one of the most active areas of research in both theoretical and experimental physics.
By next chapter we will discuss the mechanism of symmetry breaking where the neutral Higgs field interacts with other particles to give them mass.
>1)+f+t+w+C.slice(T);break;default:t=C+f+t+w}return s(t)}return y=void 0===y?6:/[gprs]/.test(m)?Math.max(1,Math.min(21,y)):Math.max(0,Math.min(20,y)),w.toString=function(){return t+""},w}return{format:h,formatPrefix:function(t,e){var n=h(((t=Vs(t)).type="f",t)),r=3*Math.max(-8,Math.min(8,Math.floor($s(e)/3))),i=Math.pow(10,-r),a=ec[8+r/3];return function(t){return n(i*t)+a}}}};function rc(t){return qs=nc(t),Xs=qs.format,Zs=qs.formatPrefix,qs}rc({decimal:".",thousands:",",grouping:[3],currency:["$",""],minus:"-"});var ic=function(t){return Math.max(0,-$s(Math.abs(t)))},ac=function(t,e){return Math.max(0,3*Math.max(-8,Math.min(8,Math.floor($s(e)/3)))-$s(Math.abs(t)))},oc=function(t,e){return t=Math.abs(t),e=Math.abs(e)-t,Math.max(0,$s(e)-$s(t))+1},sc=function(){return new cc};function cc(){this.reset()}cc.prototype={constructor:cc,reset:function(){this.s=this.t=0},add:function(t){lc(uc,t,this.t),lc(this,uc.s,this.s),this.s?this.t+=uc.t:this.s=uc.t},valueOf:function(){return this.s}};var uc=new cc;function lc(t,e,n){var r=t.s=e+n,i=r-e,a=r-i;t.t=e-a+(n-i)}var hc=Math.PI,fc=hc/2,dc=hc/4,pc=2*hc,gc=180/hc,yc=hc/180,vc=Math.abs,mc=Math.atan,bc=Math.atan2,xc=Math.cos,_c=Math.ceil,kc=Math.exp,wc=(Math.floor,Math.log),Ec=Math.pow,Tc=Math.sin,Cc=Math.sign||function(t){return t>0?1:t<0?-1:0},Sc=Math.sqrt,Ac=Math.tan;function Mc(t){return t>1?0:t<-1?hc:Math.acos(t)}function Oc(t){return t>1?fc:t<-1?-fc:Math.asin(t)}function Dc(t){return(t=Tc(t/2))*t}function Nc(){}function Bc(t,e){t&&Fc.hasOwnProperty(t.type)&&Fc[t.type](t,e)}var Lc={Feature:function(t,e){Bc(t.geometry,e)},FeatureCollection:function(t,e){for(var n=t.features,r=-1,i=n.length;++r=0?1:-1,i=r*n,a=xc(e=(e*=yc)/2+dc),o=Tc(e),s=Uc*o,c=zc*a+s*xc(i),u=s*r*Tc(i);Wc.add(bc(u,c)),Yc=t,zc=a,Uc=o}var Jc=function(t){return Vc.reset(),$c(t,Hc),2*Vc};function Qc(t){return[bc(t[1],t[0]),Oc(t[2])]}function Kc(t){var e=t[0],n=t[1],r=xc(n);return[r*xc(e),r*Tc(e),Tc(n)]}function tu(t,e){return t[0]*e[0]+t[1]*e[1]+t[2]*e[2]}function eu(t,e){return[t[1]*e[2]-t[2]*e[1],t[2]*e[0]-t[0]*e[2],t[0]*e[1]-t[1]*e[0]]}function nu(t,e){t[0]+=e[0],t[1]+=e[1],t[2]+=e[2]}function ru(t,e){return[t[0]*e,t[1]*e,t[2]*e]}function iu(t){var e=Sc(t[0]*t[0]+t[1]*t[1]+t[2]*t[2]);t[0]/=e,t[1]/=e,t[2]/=e}var au,ou,su,cu,uu,lu,hu,fu,du,pu,gu=sc(),yu={point:vu,lineStart:bu,lineEnd:xu,polygonStart:function(){yu.point=_u,yu.lineStart=ku,yu.lineEnd=wu,gu.reset(),Hc.polygonStart()},polygonEnd:function(){Hc.polygonEnd(),yu.point=vu,yu.lineStart=bu,yu.lineEnd=xu,Wc<0?(au=-(su=180),ou=-(cu=90)):gu>1e-6?cu=90:gu<-1e-6&&(ou=-90),pu[0]=au,pu[1]=su},sphere:function(){au=-(su=180),ou=-(cu=90)}};function vu(t,e){du.push(pu=[au=t,su=t]),e >>1;u[g] Exponentiation is an operation involving two numbers, the Exponentiation is an operation involving two numbers, the base and the exponent or power. Exponentiation is written as bn, where b is the base and n is the power. This section is referring to wiki page-21 of gist section-17 that is inherited from the gist section-109 by prime spin-30 and span- with the partitions as below. /lexer Exponentiation zones allows multiplication zones on representing recursive residues by virtualizing addition zones on top of the original. The first appearance of e in a printed publication was in Euler's Mechanica (1736). It is unknown why Euler chose the letter e. Leonhard Euler started to use the letter e for the constant in 1727 or 1728, in an unpublished paper on explosive forces in cannons, and in a letter to Christian Goldbach on 25 November 1731. (Wikipedia) This exponentiation takes important roles since by the multiplication zones the MEC30 forms a matrix of We present a method to increase the dynamical range of a Residue Number System (RNS) by adding virtual RNS layers on top of the original RNS, where the required modular arithmetic for a modulus on any non-bottom layer is implemented by means of an RNS Montgomery multiplication algorithm that uses the RNS on the layer. We further observed that in order to change the RSA modulus, only some constants for computing on the top layer with moduli on the middle layer need to be updated. This update need not be computed in a secure manner and hence can be done quickly. (Recursive Residues - pdf) π(π(30+37)) = π(π(67)) = π(19) = 8 These representations are a curious finding. They relate particles to antiparticles by using only the complex conjugate i → −i, they fill these as of Euler's Identity. Euler’s identity is a special case of Euler’s formula e^ix = cos x + i sin x when evaluated for x = π, In addition, it is directly used in a proof that π is transcendental, which implies the impossibility of squaring the circle. (Wikipedia) Euler angles specify the rotation of the X, Y, and Z rotation axes. The Euler angle is the culprit of the singularities in matrix algebra. In this work we present a matrix generalization of the Euler identity about exponential representation of a complex number. The concept of matrix exponential is used in a fundamental way. We define a notion of matrix imaginary unit which generalizes the usual complex imaginary unit. The Euler-like identity so obtained is compatible with the classical one. Also, we derive some exponential representation for matrix real and imaginary unit, and for the first Pauli matrix Euler identity present a matrix generalization of the about exponential representation for matrix real and imaginary unit which compatible with the Pauli matrix Gell–Mann matrices are to SU(3) what the Pauli matrices are to SU(2). Gell–Mann -matrices are a complete set of Hermitian 3 ⊗ 3 noncommuting trace-orthogonal matrices. They are at the heart of Quantum Chromodynamics (QCD), an integral part of the Standard Model. They are also used in quantum information theory to represent qutrits. (Wolfram) This imaginary unit is particularly important in both mathematics and physics. For example, those matrices (and their generalizations) are important in Lie Theory. As usual, the images on the left are snapshots of the particles at different times. Those times correspond to the grey slices in the space-time diagram on the right. You can see the specific interaction points in the space-time diagram, where the blue particle is emitted and then absorbed by the red particles. (Slimy.com) So it will need a gap between each identities to proceed the thing. Let's discuss how it goes by the seven (7) hidden dimensions. Our scenario of prime identity is layering three (3) prime pairs out of the symmetrical behaviour of 36 as the smallest number (greater than 1) which is not a prime. By our project this prime layering is called The True Prime Pairs and to be intrepeted as: Mapping the quantum way within a huge of primes objects (5 to 19) by lexering (11) the ungrammared feed (7) and parsering (13) across syntax (17). The (3) layers represents generation in the Standard Model of flavor that counts six (6) flavours of quarks and six (6) flavours of leptons. Leptons may be assigned the six flavour quantum numbers: electron number, muon number, tau number, and corresponding numbers for the neutrinos. The strength of such mixings is specified by a matrix called the Pontecorvo–Maki–Nakagawa–Sakata matrix (PMNS matrix). (Wikipedia) While there are nine (9) possible combinations of color/anti-color pairs, due to symmetry considerations one of these combinations is eliminated. A gluon can effectively carry one of eight (8) possible color/anti-color combinations. These matrices are particularly important in both mathematics and physics. For example, these matrices (and their generalizations) are important in Lie theory. Gell-mann matrices are a complete set of Hermitian noncommuting trace-orthogonal matrices. In addition, they also play an important role in physics where they can be thought to model the eight gluons that mediate the strong force quantum chromodynamics, an analogue of the Pauli matrices well-adapted to applications in the realm of quantum mechanics. (Wolfram) This quark model underlies flavor SU(3), or Eightfold Way, the successful classification scheme organizing the large number of lighter hadrons The pseudoscalar meson nonet. Members of the original meson “octet (8)” are shown in green, the singlet in magenta. Figure below shows the application of this decomposition to the mesons. (Wikipedia) The symmetrical states can couple to a pair of pseudoscalar mesons in a wave, and hence their widths and masses are strongly influenced by these couplings. In order to be four-spinors like the electron and other lepton components, there must be one quark component for every combination of flavour and colour, bringing the total to 24 (3 for charged leptons, 3 for neutrinos, and 2·3·3 = 18 for quarks). Each of these is a four (4) component bispinor, for a total of 96 complex-valued components for the fermion field. (Wikipedia) Eightfold Way = 8 × (6®+6®) = 96® In fact this particular count of three (3) as the Eightfold Way Generation of 6 by 6 flavors is the major case of every theories in physics to get in to the TOE. The origin of multiple generations of fermions, and the particular count of 3, is an unsolved problem of physics. In standard quantum field theory, under certain assumptions, a single fermion field can give rise to multiple fermion poles with mass ratios of around eπ≈23 and e2π≈535 potentially explaining the large ratios of fermion masses between successive generations and their origin. (Wikipedia) 6 x 114 - 30 - 30 - 5 = 619 = 6 x 19 = 114th prime The quark model for baryons has been very successful in describing them as qqq states, including those with nonzero internal orbital angular momentum. However, final meson-baryon states (and thus states of qq¯+qqq) play an important role as well. Why do we see certain types of strongly interacting elementary particles and not others? This question was posed over 50 years ago in the context of the quark model. The present article describes recent progress in our understanding of such “exotic” mesons and baryons. (Multiquark States - pdf) There are higher dimensional numbers besides complex numbers. The classical octet meson is now nonet. Thus consequently it would go higher than E8. These are called hypercomplex numbers, such as, quaternions (4D), octonions (8D), sedenions (16D), pathions (32D), chingons (64D), routons (128D), and voudons (256D). These names were coined by Robert P.C. de Marrais and Tony Smith. It is an alternate naming system providing relief from the difficult Latin names, such as: trigintaduonions (32D), sexagintaquattuornions (64D), centumduodetrigintanions (128D), and ducentiquinquagintasexions (256D). (Wordpress.com) The three (3) layers as explained above is in the 1st-term of our discussed structure. So the next step is the 2nd-term which goes to the four (4) dimensional space-time. 4D-dimensional space-time is much more complex due to the extra degree of freedom. Almost all of the rest of unsolved problems in physics are correlated with. The set of points in Euclidean 4-space having the same distance R from a fixed point P0 forms a hypersurface known as a 3-sphere where R is substituted by function R(t) with t meaning the cosmological age of the universe. Growing or shrinking R with time means expanding or collapsing universe, depending on the mass density inside (Wikipedia). The main reason is that the general relativity not consistent with quantum mechanics. It is even a sign that Einstein's equations are somehow incomplete. Throughout his life, Einstein published hundreds of books and articles. He published more than 300 scientific papers and 150 non-scientific ones. On 5 December 2014, universities and archives announced the release of Einstein’s papers, comprising more than 30,000 unique documents (Wikipedia). Comparatively, four-dimensional space has an extra coordinate axis, orthogonal to the other three, which is usually labeled w to describe the two additional cardinal directions of up toward and down from, respectively. On the other hand, one does not yet have a mathematically complete example of a quantum gauge theory in 4D Space vs Time, nor even a precise definition of quantum gauge theory in four dimensions. Will this change in the 21st century? We hope so! (Clay Institute’s - Yang Mills Official problem description). The Lorentz group consists, unsurprisingly, of the Lorentz transformations, which are the linear transformations preserving the Minkowski dot product. Equivalently, they are the linear transformations fixing that hyperboloid of two sheets. If we discard one of the sheets, we obtain the orthochronous (time-preserving) subgroup. And when n = 24, we get a very beautiful discrete subgroup, namely the automorphism group of the II(25,1) lattice intimately related to the Leech lattice. (Complex Projective 4-Space) This diagram is representing groupings (leptons, quarks, weak-force bosons) with 6 quarks in a way that parallels the 6 leptons. There are 8 different types of tiny particles, or ‘states’, that we can find in a special kind of space that has 6 dimensions and involves both real and imaginary numbers. These particles include: In a diagram at the top left, this 6-dimensional space is shown to be curved. In another diagram at the bottom right, we see two waves that are perpendicular to each other, representing the motion of a particle in a ‘Dirac harmonic oscillator’ – a concept in quantum mechanics. (Physics In History) In this paper, you may find a way to apply the Gell-Mann transformations made by the λi matrices using Geometric Algebra Cl3,0. The action of C⊗O on itself can be seen to generate a 64-complex-dimensional algebra, wherein we are able to identify two sets of generators for SU(3)c. We apply these generators to the rest of the space, and find that it breaks down into the SU(3)c representations of exactly three generations of quarks and leptons. They are at the heart of Quantum Chromodynamics (QCD), an integral part of the Standard Model. They are also used in quantum information theory to represent qutrits. Gell–Mann matrices are to SU(3) what the Pauli matrices are to SU(2). (Wolfram) These unifying principles of both mathematics and physics might come in the form of grand unified theories, supersymmetry, string theory, or perhaps something else. Standard heuristic mathematical models of population dynamics are often constructed using ordinary differential equations (ODEs). These deterministic models yield pre-dictable results which allow researchers to make informed recommendations on public policy. A common immigration, natural death, and fission ODE model is derived from a quantum mechanics view. (A Quantum Mechanics Approach.pdf) Although, at the moment evidence do not have a complete model. However, it becomes a little more clear that this unlikely algebra is not going away. While the Dirac CP-violating phase δℓ can be determined in the future, how to probe or constrain the Majorana CP-violating phases ρ and σ is still an open question Four of the dimensions are the usual four of spacetime. The six (or perhaps seven) extra dimensions are rolled up to be almost unobservable. We don’t see 6 (or 7) of these extra dimensions because - we assume - they are rolled up a la Kaluza–Klein theory into a 6 dimensional Calabi–Yau space The most promising candidate is SO(10) but it does not contain any exotic fermions (i.e. additional fermions besides the Standard Model and the right-handed neutrino), and it unifies each generation into a single irreducible representation. In particle physics, SO(10) refers to a grand unified theory (GUT) based on the spin group Spin(10). The shortened name SO(10) is conventional[1] among physicists, and derives from the Lie algebra or less precisely the Lie group of SO(10), which is a special orthogonal group that is double covered by Spin(10). SO(10) subsumes the Georgi–Glashow and Pati–Salam models, and unifies all fermions in a generation into a single field. This requires 12 new gauge bosons, in addition to the 12 of SU(5) and 9 of SU(4)×SU(2)×SU(2). It has been long known that the SO(10) model is free from all perturbative local anomalies, computable by Feynman diagrams. However, it only became clear in 2018 that the SO(10) model is also free from all nonperturbative global anomalies on non-spin manifolds — an important rule for confirming the consistency of SO(10) grand unified theory, with a Spin(10) gauge group and chiral fermions in the 16-dimensional spinor representations, defined on non-spin manifolds. (Wikipedia) In the spin-foam formalism, the Barrett–Crane model, which was for a while the most promising state-sum model of 4D Lorentzian quantum gravity It was based on representations of the noncompact groups SO(3,1) or SL(2,C), so the spin foam faces (and hence the spin network edges) were labelled by positive real numbers as opposed to the half-integer labels of SU(2) spin networks. (Wikipedia) The field content of this theory is the massless N = 8 supergravity which comprises the graviton, 8 gravitinos, 28 vector fields. In four spacetime dimensions, N = 8 supergravity, speculated by Stephen Hawking, is the most symmetric quantum field theory which involves gravity and a finite number of fields. It has eight (8) supersymmetries, which is the most any gravitational theory can have, since there are eight half-steps between spin 2 and spin −2. (The spin 2 graviton is the particle with the highest spin in this theory.) There has been renewed interest in the 21st century, with the possibility that string theory may be finite. (Wikipedia) One remarkable property of both string and M-theory is that seven (7) extra dimensions are required for the theory's consistency, on top of the four dimensions in our universe. There exist scenarios in which there could actually be more than 4D of spacetime. String theories require extra dimensions of spacetime for their mathematical consistency. These are situations where theories in two or three spacetime dimensions are no more useful. In string theory, spacetime is 26-dimensional, while in superstring theory it is 10-dimensional, and in M-theory it is 11-dimensional. This classification theorem identifies several infinite families of groups as well as 26 additional groups which do not fit into any family. (Wikipedia) So the last "Superstring revolution" was impressive but it was close to 30 years ago now - and we still don't seem to be adopting it as "The Truth". M Theory and/or Loop Quantum Gravity hold the promise of resolving the conflict between general relativity and quantum mechanics but lack experimental connections to predictability in physics. The prediction of particle mass and lifetimes is a good indicator for its validity. (TOE - pdf) We suspect that using that Lorentz, all four have the same complexified Lie algebra. In loop quantum gravity it makes matters even more confusing. There is a proof that it is impossible to embed all the three generations in E8 without the presence of additional particles that do not exist in the physical world. This is a somewhat arbitrary choice, selected for leaving W3 and color invariant. Once the first generation of fermions, with correct charges and spins, are assigned to elements of e8, this T rotates them to the second and third generations. There is such an assignment known to the author that gives the correct hypercharges for all three generations, but it is not a triality rotation and it produces unusual spins. A correct description of the relationship between triality and generations, if it exists, awaits a better understanding. (An Exceptionally Simple Theory of Everything - pdf) The matter representations come in three copies (generations) of the 16 representation. The Yukawa coupling is 10H 16f 16f. *This includes a right-handed neutrino”. One may either include three copies of singlet representations φ and a Yukawa coupling (the “double seesaw mechanism”); or else, add the Yukawa interaction or add the nonrenormalizable coupling. (Wikipedia) Beyond leading approx. we define mGUT as the mass of the heavy 24 gauge bosons, while mT = mHT is the mass of the triplet Higgs. The cleanest signature for a Higgs sector with triplet fields would be the discovery of doubly charged Higgs Bosons. Like Pauli’s bold prediction of the neutrino and GIM’s bold prediction of the charm quark, the equally bold speculation of Kobayashi and Maskawa was proved absolutely correct, when the fermions of the third generation began to be discovered one by one. First came the tau lepton in 1975, closely followed by the bottom quark in 1977. There followed a 17-year hiatus till the 1994 discovery of the top quark, and another 6 years wait till the existence of the tau neutrino νwas confirmed in 2000. Is the fermion red? green? blue? Does the fermion have isospin up? down? These five questions can be represented by an exterior algebra of 2⁵ or 32-complex dimensional. This thesis constitutes a first attempt to derive aspects of standard model particle physics from little more than an algebra. Furthermore, we show that these three-generation results can be extended, so as to include all 48 fermionic U(1)em charges. (Standard Model from an algebra - pdf) Subatomic particles such as protons or neutrons, which contain two or more elementary particles, are known as composite particles. The Standard Model of Particle Physics, describes for us all know fundamental interaction in nature till date, with the exception of Gravity (work on this front is going on). Here is a summary of the fundamental content of the standard model They interact, they transfer energy and momentum and angular momentum; excitations are created and destroyed. Every excitation that’s possible has a reverse excitation. (Quora) It is hypothesized that gravitational interactions are mediated by an as yet undiscovered elementary particle, dubbed the graviton. Elementary particles and their interactions are considered by a theoretical framework called the Standard Model (SM) of Particle Physics. The Standard Model presently recognizes seventeen distinct particles (twelve fermions and five bosons). As a consequence of flavor and color combinations and antimatter, the fermions and bosons are known to have 48 and 13 variations, respectively. Among the 61 elementary particles embraced by the Standard Model number electrons and other leptons, quarks, and the fundamental bosons. (Wikipedia) 17 distinct particles = 12 fermions + 5 bosons = 48 + 13 = 61 variations In order to be four-spinors like the electron and other lepton components, there must be one quark component for every combination of flavour and colour, bringing the total to 24 (3 for charged leptons, 3 for neutrinos, and 2·3·3 = 18 for quarks). Each of these is a four (4) component bispinor, for a total of 96 complex-valued components for the fermion field. (Wikipedia) It is stated that each of the 24 components is a four component bispinor. A bispinor is constructed out 2 simpler component spinor so there are eight (8) spinors in total. Bispinors are so called because they are constructed out of two (2) simpler component spinors, the Weyl spinors. Each of the two (2) component spinors transform differently under the two (2) distinct complex-conjugate spin-1/2 representations of the Lorentz group. This pairing is of fundamental importance, as it allows the represented particle to have a mass, carry a charge, and represent the flow of charge as a current, and perhaps most importantly, to carry angular momentum. (Wikipedia) ((3+3) + 2x(3x3)) x 4 = (3 + 3 + 18) x 4 = 24 x 4 = 96 components Thus fermion is constructed out of eight (8) spinors that brings the total of 96 components consist of 12 charged leptons, 12 neutrinos and 72 quarks. The physical evolution of neutrino parameters with respect to energy scale may help elucidate the mechanism for their mass generation. The most general Lagrangian with massless neutrinos, one finds that the dynamics depend on 19 parameters, whose numerical values are established by experiment. The renormalization scale may be identified with the Planck scale or fine-tuned to match the observed cosmological constant. However, both options are problematic. (Wikipedia) The Standard Model with massive neutrinos need 7 more parameters (3 masses and 4 PMNS matrix parameters) for a total of 26 parameters. In principle, there is one further parameter in the Standard Model; the Lagrangianof QCD can contain a phase that would lead to CP violation in the strong interac-tion. Likewise, the coupling constants of the three gauge interactions are of a similar order of magnitude, hinting that they might be different low-energy manifestations of a Grand Unified Theory (GUT) of the forces. These patterns provide hints for, as yet unknown, physics beyond the Standard Model. (Modern Particle Physics - pdf) (24-5) + (24-17) = 19 + 7 = 26 The first diagram corresponds to the first term at right hand side of equality, while the other two diagrams with back-moving lines combine to produce the second term. We study the anomalous scale symmetry breaking effects on the proton mass in QCD due to quantum fluctuations at ultraviolet scales. Dynamical response of the scalar Hamiltonian HS in the presence of the fermion , generating a contribution to the fermion mass (Scale symmetry breaking - pdf) The dotted line represents the dynamical Higgs particles h and the crossed circle denotes the scalar Hamiltonian linear in h. Now we show the interplay of the finite system of prime positions with the 15 finite even positions in the cyclic convolution. Consequently, we only need to fold a 30’s cycle as so that we can identify the opposite prime positions that form their specific pairs in a specific convolution. 13+17 = 11+19 = 30 The coupling g between the Higgs field and the fermion is proportional to fermion mass. Let's consider a prime spin theory of compactifying the 7-dimensional manifold on the 3-sphere of a fixed radius and study its dimensional reduction to 4D. We now place integers sequentially into the lattice with a simple rule: Each time a prime number is encountered, the spin or ‘wall preference’ is switched. So, from the first cell, exit from 2’s left side. This sets the spin to left and the next cell is 3, a prime, so switches to right. 4 is not prime and continues right. 5 is prime, so switch to left and so on. There are twists and turns until 19 abuts 2. (HexSpin) In our approach a 3-form is not an object that exist in addition to the metric, it is the only object that exist and in particular the 4D metric, is defined by the 3-form. We would like to say that our present use of G2 structures (3-forms in 7D) is different from whatone can find in the literature on Kaluza–Klein compactifications of supergravity. Also, in the supergravity context a 7D manifold with a G2 structure is used for compactifying the 11D supergravity down to 4D. In contrast, we compactify from 7D to 4D. (General relativity from three-forms in seven dimensions - pdf) The complete theory was obtained by dimensional reduction of the 11D supergravity on a seven (7) torus and realizing the exceptional symmetry group E7(7) In particular, these theories include the compactification of eleven-dimensional supergravity on the seven-sphere S7, which gives rise to a four-dimensional theory with compact non-abelian gauge group SO(8) (11D Supergravity and Hidden Symmetries - pdf) The most general Lagrangian with massless neutrinos, one finds that the dynamics depend on 19 parameters, whose numerical values are established by experiment. Straightforward extensions of the Standard Model with massive neutrinos need 7 more parameters (3 masses and 4 PMNS matrix parameters) for a total of 26 parameters. The neutrino parameter values are still uncertain. The 19 certain parameters are summarized here: As these theories tend to reproduce the entirety of current phenomena, the question of which theory is the right one, or at least the “best step” towards a Theory of Everything, can only be settled via experiments (Wikipedia) Please note that we are not talking about the number 19 which is the 8th-prime. Here we are talking about 19th as sequence follow backward position of the 18th. The same number of 7 vs 11 dimensions as we have discussed are hold by 7 primes vs 11 natural numbers in every first term of the prime spin. Consider the following: The further terms will only have their specific meaning when they are formed in the favor of True Prime Pairs which we called as Δ(19 vs 18) Scenario Symmetry breaking in Quantum Field Theory (QFT) applies to the scalar field, at first so that it can have an impact and give mass to gauge bosons and fermions. In QFT this is currently done by manually adding an extra term to the field’s self-interaction, creating the famous Mexican Hat potential well. This (otherwise) plain and featureless “absorbtion” of the Goldstone modes in the EW field could be a reason why a complex, synergy-creating quality of the scalar field is largely unnoticed in QFT. Obviously this has the potential to become a new research challenge in physics. (TGMResearch) The greatest problem in theoretical physics is combining the general relativity with quantum mechanics. Actually it is related to a non-standard renormalization. A lot number of positive color-charges move from the positive charged particle toward the negative charged particles, and negative color-charges move from negative charged particle toward the positive charged particle and they combine in each other. Due to the fact that everything is made up of sub quantum energy, the classical concept of acceleration and relativistic Newton’s second law needs to be reviewed. (Gravity in Time space - pdf) Renormalization was first developed in quantum electrodynamics (QED) to make sense of infinite integrals in perturbation theory. Renormalization is a collection of techniques in quantum field theory, statistical field theory, and the theory of self-similar geometric structures, that are used to treat infinities arising in calculated quantities by altering values of these quantities to compensate for effects of their self-interactions. (Wikipedia) The problem is raised when the non-standard renormalization hides the scheme and scale-independent quantum anomalous energy (QAE) contribution in the mass. In this paper we have studied the renormalization of the QCD trace anomaly separately for the quark and gluon parts of the energy momentum tensor. We have also found that C¯q,g(µ) does not go to zero as µ → ∞ even in the chiral limit, contrary to what one would naively expect from the one-loop calculation (3.16). (Quark and gluon contributions to the QCD trace anomaly - pdf) (24-5) + (24-17) = 19 + 7 = 26 In order to explain the generation process of gravitational energy between two identical sign charged particles, it is necessary to explain the process of the generated electromagnetic energy by the interaction of their electrical repulsion. In quantum mechanics, the graviton is a hypothetical elementary particle that mediates the force of gravitation in the framework of quantum field theory. If it exists, the graviton must be massless and must have a spin of 2. This is because the source of gravitation is the stress-energy tensor, a second-rank tensor. This definition of graviton is not able to describe gravitational phenomena, so we need a new definition of graviton. (What is CPH Theory - pdf) The physical evolution of neutrino parameters with respect to energy scale may help elucidate the mechanism for their mass generation. We study the anomalous scale symmetry breaking effects on the proton mass in QCD due to quantum fluctuations at ultraviolet scales. Dynamical response of the scalar Hamiltonian HS in the presence of the fermion , generating a contributionto the fermion mass The dotted line represents the dynamical Higgs particles h and the crossed circle denotes the scalar Hamiltonian linear in h. The coupling g between the Higgs field and the fermion is proportional to fermion mass. (Scale symmetry breaking - pdf) The first diagram corresponds to the first term at right hand side of equality, while the other two diagrams with back-moving lines combine to produce the second term. By True Prime Pars we shall take 36 nodes to conjugate partitions. So the most possible way is taking the 3rd layer which hold the sum 36 of prime pair 19 and 17. A chiral phenomenon is one that is not identical to its mirror image (see the article on mathematical chirality). The spin of a particle may be used to define a handedness, or helicity, for that particle, which, in the case of a massless particle, is the same as chirality. A symmetry transformation between the two is called parity transformation. Invariance under parity transformation by a Dirac fermion is called chiral symmetry. The discovery of neutrino oscillation implies that neutrinos have mass, so the photon is the only confirmed massless particle; gluons are expected to also be massless, although this has not been conclusively tested.[b] Hence, these are the only two particles now known for which helicity could be identical to chirality, and only the photon has been confirmed by measurement. All other observed particles. The first term will directly be identified as a forward moving diagram for external mψψ¯ insertion, while the second term corresponds to the combination of two backward moving diagrams using the relation in energy denominators. The helicity of a particle is positive (“right-handed”) if the direction of its spin is the same as the direction of its motion. It is negative (“left-handed”) if the directions of spin and motion are opposite. So a standard clock, with its spin vector defined by the rotation of its hands, has left-handed helicity if tossed with its face directed forwards. By Chiral symmetry the Vector gauge theories with massless Dirac fermion fields ψ exhibit chiral symmetry, i.e., rotating the left-handed and the right-handed components independently makes no difference to the theory. We can write this as the action of rotation on the fields: The Standard Model with massive neutrinos need 7 more parameters (3 CKM and 4 PMNS matrix parameters) for a total of 26 parameters. By our concept these 7 parameters correspond to π(17) = 7 prime identities of additional zones. Massive fermions do not exhibit chiral symmetry, as the mass term in the Lagrangian, mψψ, breaks chiral symmetry explicitly. The general principle is often referred to by the name chiral symmetry. The rule is absolutely valid in the classical mechanics of Newton and Einstein, but results from quantum mechanical experiments show a difference in the behavior of left-chiral versus right-chiral subatomic particles. (Wikipedia) 1 + 77 = 78 = 3 copies of 26-dimensions The first term forms the photonic contribution while the second term is the fermionic contribution (two backward). The first backward is correspond to the three (3) known neutrino flavors: the electron-, muon- and tau-neutrino which are left-handed. Summary of various critical points in the context of superpotential observed in this paper first : Gauge symmetry, supersymmetry, vacuum expectation value of field, superpotential and cosmological constants. We expect that the nontrivial r-dependence of vevs makes Einstein-Maxwell equations consistent not only at the critical points but also along the supersymmetric RG flow connecting two critical points. (N = 8 Supergravity: Part I - pdf) Taking 19 as a certain parameter we can see that the left handed cycles are happen on 5th-spin (forms 4th hexagon, purple) and 6th-spin (forms 5th hexagon, cyan). Both have different rotation with other spin below 9th spin (forms 6th hexagon, yellow). Proceeding, the number line begins to coil upon itself; 20 lands on 2’s cell, 21 on 3’s cell. Prime number 23 sends the number line left to form the fourth (4th) hexagon, purple. As it is not a twin, the clockwise progression (rotation) reverses itself. Twin primes 29 and 31 define the fifth (5th) hexagon, cyan. Finally, 37, again not a twin, reverses the rotation of the system, so 47 can define the yellow hexagon (HexSpin). 7th spin - 4th spin = (168 - 102)s = 66s = 6 x 11s = 30s + 36s Thus it appears that the cosmological models] derived from compactification of 11d supergravity on a manifold with G2 holonomy have some hidden E7 symmetry. There are By the Δ(19 vs 18) Scenario those three are exactly landed in the 0's cell out of Δ18. See that the sum of 30 and 36 is 66 while the difference between 36 and 102 is also 66. You likely noticed I began with 2 rather than 1 or 0 when I first constructed the hexagon. Why? Because they do not fit inside — they stick off the hexagon like a tail. Perhaps that’s where they belong. However, if one makes a significant and interesting assumption, then 1 and 0 fall in their logical locations – in the 1 and 0 cells, respectively. _(HexSpin) 0 + 30 + 36 + 102 = 168 = π(1000) By defining the pattern on each individual numbers against homogeneous sorting. Using this method then out of bilateral way the ∆(19 vs 18) Scenario we could get in to Scheme-33. The electroweak force is believed to have separated into the electromagnetic and weak forces during the quark epoch of the early universe. The quark epoch ended when the universe was about 10−⁶ seconds old, when the average energy of particle interactions had fallen below the binding energy of hadrons. The following period, when quarks became confined within hadrons, is known as the hadron epoch. (Wikipedia) In terms of Feynman diagrams it has shown that the expansion of N = 8 supergravity is in some ways a product of two N = 4 super Yang–Mills theories. The number 28, aside from being triangular wave of perfect pyramid, is the sum of the first 5 primes and the sum of the first 7 natural numbers. The intervention of the Golden Ratio can be seen as a way to enter the quantum world, the world of subtle vibrations, in which we observe increasing energy levels as we move to smaller and smaller scales. El Nachie has proposed a way of calculating the fractal dimension of quantum space-time. The resulting value (Figure 7) suggests that the quantum world is composed of an infinite number or scaled copies of our ordinary 4-dimensional space-time. Setting k=0 one obtains the classical dimensions of heterotic superstring theory, namely 26, 16, 10, 6 and 4, as well as the constant of super-symmetric (αgs=26) and non super-symmetric (αg=42) unification of all fundamental forces. As we have seen in section 2, the above is a Fibonacci-like sequence with a very concise geometrical interpetation related to numbers 5, 11 and φ. (Phi in Particle Physics) d(43,71,114) = d(7,8,6) » 786 We can use simplexes to triangulate a surface and compute the Euler characteristic and other topological properties in this fashion. Several aspects of torsion in string-inspired cosmologies are reviewed. In particular, its connection with fundamental, string-model independent, axion fields associated with the massless gravitational multiplet of the string are discussed. Finally, the current-era phenomenology of this model is briefly described with emphasis placed on the possibility of alleviating tensions observed in the current-era cosmological data. A brief phenomenological comparison with other cosmological models in contorted geometries is also made. (Torsion in String Cosmologies - pdf) 114 = 102 + 66 - 29 - 25 = 6 + (6x6) + 6 x (6+6) = 6 x (6+6) + 6 + (6x6) = 25 + 89 The value of the vacuum energy (or more precisely, the renormalization scale used to calculate this energy) may also be treated as an additional free parameter. In Fuller’s synergetic geometry, symmetry breaking is modeled as 4 sub-tetra’s, of which 3 form a tetrahelix and the 4th. “gets lost”. The latter solves into a Goldstone oscillation and a vacuum expectation value (VEV), among other unique properties. The scalar field’s self-interaction is a Golden Ratio scale-invariant group effect, such as geometrically registered by the icosa-dodeca matrix. (TGMResearch) The second backward of second term will return to the right handed. Since this second term is the fermionic contribution then it will correspond to the right handed neutrinos. If right-handed neutrinos exist but do not have a Majorana mass, the neutrinos would instead behave as three (3) Dirac fermions and their antiparticles with masses coming directly from the Higgs interaction, like the other Standard Model fermions. Majorana fermions cannot possess intrinsic electric or magnetic moments, only toroidal moments.[7][8][9] Such minimal interaction with electromagnetic fields makes them potential candidates for cold dark matter. (Wikipedia) In other words, the synchronized path integral represents a deterministic approach to scalar field's self-excitation, and thus to the confined state in quentum physics Beside the operator proof, here we also provide a diagrammatic argument of the above derivation, using the QED in background field in Sec. 5 as an example. Finally, the mass derivative of the external wave function uN is more complicated, which is shown the remaining diagrams where the mψψ¯ are inserted at external legs. (Scale symmetry breaking - pdf) Let us make some concluding remarks with the help of the Fritzsch-Xing "pizza" plot. It offers a summary of 28 free parameters associated with the SM itself and neutrino masses, lepton flavor mixing angles and CP-violating phases. The reduction of pure gravity from eleven dimensions down to D = 4 dimensions yields a gravitational theory with seven (7) abelian vector fields Aµn, Those results, compared with those for the nucleon, indicate quite different pattern, revealed as a new aspect by exploiting the quark/gluon decomposition of the QCD trace anomaly. The matrix elements of this quark/gluon decomposition of the QCD trace anomaly allow us to derive the QCD constraints on the hadron’s gravitational form factors, in particular, on the twist-four gravitational form factor, Cq,g. We find quite different pattern in the obtained results between the nucleon and the pion. (Twist-four gravitational - pdf) 2+7 = 3×3 lepton vs quarks This fact may also provide a possible explanation for why almost all of the particle interactions we see are describable by renormalizable theories. The Standard Model of particle physics contains only renormalizable operators, but the interactions of general relativity become nonrenormalizable operators if one attempts to construct a field theory of quantum gravity in the most straightforward manner (treating the metric in the Einstein–Hilbert Lagrangian as a perturbation about the Minkowski metric), suggesting that perturbation theory is not satisfactory in application to quantum gravity. It may be that any others that may exist at the GUT or Planck scale simply become too weak to detect in the realm we can observe, with one exception: gravity, whose exceedingly weak interaction is magnified by the presence of the enormous masses of stars and planets. (Wikipedia) For the renormalization mixing at twist four, the Feynman diagram calculation of ZF and ZC is available to the two-loop order. Moreover, it is shown that the constraints imposed by the RG invariance of (1.1) allow to determine the power series in αs for ZF as well as ZC in the MS-like schemes, completely from the perturbative expansions of β(g) and γm(g), which are now known to five-loop order [43–48] in the literature. Thus, all the renormalization constants in (2.3)–(2.6) are determined up to the three-loop accuracy. (Twist-four gravitational - pdf) A gauge colour rotation is a spacetime-dependent SU(3) group element. They span the Lie algebra of the SU(3) group in the defining representation. The Gell-Mann matrices, developed by Murray Gell-Mann, are a set of eight linearly independent 3×3 traceless Hermitian matrices used in the study of the strong interaction in particle physics. They span the Lie algebra of the SU(3) group in the defining representation. Indeed, a particularly well-chosen cellular automaton on II(9,1) or II(25,1) would be a discretised version of 10- or 26-dimensional string theory. The Lie algebra E6 of the D4-D5-E6-E7-E8 VoDou Physics model can be represented in terms of 3 copies of the 26-dimensional traceless subalgebra J3(O)o of the 27-dimensional Jordan algebra J3(O) by using the fibration E6 / F4 of 78-dimensional E6 over 52-dimensional F4 and the structure of F4 as doubled J3(O)o based on the 26-dimensional representation of F4. (Tony’s Home) The fact that quarks of the same electric charge possess a mass hierarchy is a big puzzle. It must be highly correlated with the hierarchy of quark flavor mixing. This chapter is intended to provide a brief description of some important issues regarding quark masses, flavor mixing and CP-violation. A comparison between the salient features of quark and lepton flavor mixing structures is also made. Here our focus is on the five (5) parameters of strong and weak CP violation. In the quark sector, the strong CP-violating phase θ remains unknown, but the weak CP-violating phase δq has been determined to a good degree of accuracy. In the lepton sector, however, none of the CP-violating phases has been measured. (Quark Mass Hierarchy and Flavor Mixing Puzzles - pdf) The 3x3 lepton vs quark mixing matrices appearing in the weak charged-current interactions are referred to, respectively, as the PMNS matrix U, and the CKM matrix V, which all the fermion fields are the mass eigenstates. Muons are about 200 times heavier than the electron. The larger mass makes them unstable. Muons exist for only about two microseconds—or two-millionths of a second—before they decay. Electrons live forever. The tau; elementary subatomic particle is similar to the electron but 3,477 times heavier. Like the electron and the muon, the tau is an electrically charged member of the lepton family of subatomic particles; the tau is negatively charged, while its antiparticle is positively charged. (ResearchGate) Bound state corrections to the semileptonic width and measured by a number moments analyses have permitted the extraction to a level of a few %. In principle, there is one further parameter in the Standard Model; the Lagrangian of QCD can contain a phase that would lead to CP violation in the strong interaction. Likewise, the coupling constants of the three gauge interactions are of a similar order of magnitude, hinting that they might be different low-energy manifestations of a Grand Unified Theory (GUT) of the forces. These patterns provide hints for, as yet unknown, physics beyond the Standard Model. (Modern Particle Physics P.500 - pdf) Below is a model of E11 (shown by 11 dimensions). Its absolute dimensions represent all related key knowledges of modern physics. Moreover this model represents Quark-Gluon Plasma, with all of the fundamental forces in the early stage after Big Bang. (Youtube) Classically, we have only one 11-dimensional supergravity theory: 7D hyperspace + 4 common dimensions. The four (4) faces of our pyramid additively cascade 32 four-times triangular numbers Note that The above 11 stands as the central point which is correlated to 77 sequencial processes of sun vs moon orbits starting with the symmetri breaking that involving 9 and 7. Back in 1982, a very nice paper by Kugo and Townsend, Supersymmetry and the Division Algebras, explained some of this, ending up with some comments on the relation of octonions to d=10 super Yang-Mills and d=11 super-gravity. The headline argument is that octonions are important and interesting because they’re The Strangest Numbers in String Theory, even though they play only a minor role in the subject. (math.columbia.edu) A number of other GUT models are based upon subgroups of SO(10). They are the minimal left-right model, SU(5), flipped SU(5) and the Pati–Salam model. SU(5) fermions of standard model in 5+10 representations. The sterile neutrino singlet’s 1 representation is omitted. Neutral bosons are omitted, but would occupy diagonal entries in complex superpositions. X and Y bosons as shown are the opposite of the conventional definition The simplest theory describing the above is the SU(3) one with the gluons as the basis states of the Lie algebra. That is, gluons transform in the adjoint representation of SU(3), which is 8-dimensional. The Cartan–Weyl basis of the Lie algebra of SU(3) is obtained by another change of basis, where one defines The Root System for SU(3). The Lie group structure of the Lorentz group is explored. Its generators and its Lie algebra are exhibited, via the study of infinitesimal Lorentz transformations. The Lie algebras of these two groups are shown to be identical (up to some isomorphism). 19 + i(13+5) = 19 + i18 A bispinor is more or less "the same thing" as a Dirac spinor. The convention used here is that the article on the Dirac spinor presents plane-wave solutions to the Dirac equation. The four pairwise disjoint and non-compact connected components of the Lorentzgroup L = O(1, 3) and corresponding subgroups: Of course, the sets L↓−, L↑− and L↓+ do not represent groups due to the missing identity element. (The-four-pairwise-disjoint) 19 + 7 = 26 Fermion particles are described by Fermi–Dirac statistics and have quantum numbers described by the Pauli exclusion principle. They include the quarks and leptons, as well as any composite particles consisting of an odd number of these, such as all baryons and many atoms and nuclei. Fermions have half-integer spin; for all known elementary fermions this is 1⁄2. In the Standard Model, there are 12 types of elementary fermions: six quarks and six leptons. All known fermions except neutrinos, are also Dirac fermions; that is, each known fermion has its own distinct antiparticle. It is not known whether the neutrino is a Dirac fermion or a Majorana fermion.[4] Fermions are the basic building blocks of all matter. They are classified according to whether they interact via the strong interaction or not. In physics, a subatomic particle is a particle smaller than an atom.[1] Experiments show that light could behave like a stream of particles (called photons) as well as exhibiting wave-like properties. This led to the concept of wave–particle duality to reflect that quantum-scale particles behave both like particles and like waves; they are sometimes called wavicles to reflect this. (Wikipedia) This scheme goes to the unification of 11s with 7s to 18s meanwhile the 11th it self behave as residual by the 5th minor hexagon between the 30 to 36' cells. The interaction of any pair of fermions in perturbation theory can be modelled as: Two fermions go in → interaction by boson exchange → Two changed fermions go out. The exchange of bosons always carries energy and momentum between the fermions, thereby changing their speed and direction. The exchange may also transport a charge between the fermions, changing the charges of the fermions in the process (e.g., turn them from one type of fermion to another). Since bosons carry one unit of angular momentum, the fermion’s spin direction will flip from +1⁄2 to −1⁄2 (or vice versa) during such an exchange (in units of the reduced Planck’s constant). (Wikipedia) 36th prime - 30th prime = 151 - 113 = 1 + 37 The boson, photon and gravity forces are assigned to 30, 31 and 32. Gluon force and exchange are assigned to 33 and 34 which are then standing as the lexer and parser. Below we will demonstrate how factorization algorithms and twin prime dyad cycling at the digital root level rotate the vertices of equilateral triangles within {9/3} star polygons like the one pictured above. These rotations are encoded in 3 x 3 matrices generated by period-24 digital root dyad tri-level cycling. We will also reveal the Latin Square reflecting {3,6,9} hidden in plain sight betwixt and between the twin prime distribution channels; all of its rows, columns and principal diagonals summing to 18. PrimesDemystified 19 + 18 + 102 = 37 + 102 = 139 = 34th prime = (40 - 6)the prime This lead to a consequence of SU(5) grand unification (assigned to 35) showing a complex scalar Higgs boson of 24 gauge groups observe mass of W boson (assigned to 36). An overview of the various families of elementary and composite particles, and their interactions. Fermions are on the left, and Bosons are on the right. According to the Standard Model there are five (5) elementary bosons with thirteen (13) variations. These 5 and 13 will be assigned to the “5xid’s of 31~35 (sequenced)” and “13xid’s of 36~68 (unsequenced)”, respectively (see the sidebar menu). So the 36 should behave as a central. Therefore the total files that inherited from this scheme will be 109 = 29th prime = (10th prime)th prime This behaviour finaly brings us to a suggestion that the dimension in string theory are linked with the prime distribution level as indicated by the self repetition on MEC30. There are 7 hidden dimensions in 11-d Supergravity, which is the low energy approximation to M theory, which also has 7 hidden dimensions. (Prime Curios!) π(1000) - loop(1,30) - loop(31,36) = 168 - 29 - 25 = 114 By the identition zones we are going to discuss in detail how this reversal behaviour of 8-dimensions is converting the 11 dimensions to Ploting 40th prime scheme of the three (3) layers with all the features of 3rd prime identity as explained above then they would form their recycing through the three (3) times bilateral 9 sums as shown below. 89^2 - 1 = 7920 = 22 x 360 = 66 x 120 = (168 - 102) x 120 Going deeper there are many things raised up as questions. So in this project we are going to analyze it using a javascript library called Chevrotain. The spin states for the powers of pi. The Prime Hexagon is an integer environment, so pi powers are truncated. I believe these data suggest prime numbers are linked in some way to pi. (HexSpin) Since the modulo 6 is occured all over the spin then we have defined that this 4 zones should stand as default configuration as you can see on the left sidebar. In order to maintain the 18’s structure between each of repositories to correlate with the above density then we could use a hierarchical database that stores low-level settings for the operating system such as windows registry. Using the javascript library from Chevotrain and data parser from Jekyll/Liquid finally we found the correlation between the lexer and parser trough the powers of pi. In this example, the content from a Markdown document It is going to setup CI/CD for up to 1000 public repositories out of millions that available on GitHub. You may visit our mapping scheme for more detail. The 619 is the 114th prime. By the True Prime Pairs it is laid on the last index of 6 with prime 19 where as 6x19 is also 114. Let's put 19 hexagons within the 3 layers. 168+618 - 19x6x6 = 786 - 684 = 102 When recombination is occur then the prime 13 is forced to → 12 where the impact (Δ1) goes to 18+13+12=43 on the last 7th row. This sequence is simulated by a flowchart having 12 arrows flowing on 10 (ten) shapes of prime 31 up to 71 (40 nodes). Mapping the quantum way within a huge of primes objects (5 to 19) by lexering (11) the ungrammared feed (7) and parsering (13) across syntax (17) (₠Quantum). 6+6 + 6/\6 = 6+6 + 15 = 27-day month By this project the above would be deployed as default layout. It is set to be avalaible throughout the whole platform via a single page within a parser repository which is acting as prime 13. Their interface will be in json and xml format. Here is for the sample: Using a kind of interface such as docker then it could be developed cross platform. Evenso. Let assume that all alpabethic letter in the sequence is representing a local disk so you may build your own pattern in your PC such as shown below: This also introduces a lower bound of Mod 90 originated from the 4th coupling of MEC30 which is holded by five (5) cells between 13 and 17. The Minimal Supersymmetric Standard Model (MSSM) contains two Higgs doublets, leading to five (5) physical Higgs bosons: At tree-level, the masses are governed by two parameters, often taken to be mA and tan β [3]. When tan β >> 1, A is nearly degenerated with one of the CP-even states (denoted ϕ). (ScienceDirect) By The GitHub Runner you can connect to the Google COS Instance. For self-hosted runners defined at the organization level, configure runs-on.group in your workflow file to target a runner groups or combine groups and labels. Why collaborating with physicists? You can find a great and fairly complete overview of ML papers in HEP. (Pata Slides) π(10) = 2,3,5,7 This way will also be our approach to Euler's identity. 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=c?u:u*("desc"==n[i]?-1:1)}return t.index-e.index}},function(t,e,n){var r=n(42);t.exports=function(t,e){if(t!==e){var n=void 0!==t,i=null===t,a=t==t,o=r(t),s=void 0!==e,c=null===e,u=e==e,l=r(e);if(!c&&!l&&!o&&t>e||o&&s&&u&&!c&&!l||i&&s&&u||!n&&u||!a)return 1;if(!i&&!o&&!l&&t0}t.exports=function(t,e,r,i){var a,o,s,c,u,l,h,f,d,p,g,y,v;if(a=e.y-t.y,s=t.x-e.x,u=e.x*t.y-t.x*e.y,d=a*r.x+s*r.y+u,p=a*i.x+s*i.y+u,0!==d&&0!==p&&n(d,p))return;if(o=i.y-r.y,c=r.x-i.x,l=i.x*r.y-r.x*i.y,h=o*t.x+c*t.y+l,f=o*e.x+c*e.y+l,0!==h&&0!==f&&n(h,f))return;if(0===(g=a*c-o*s))return;return y=Math.abs(g/2),{x:(v=s*l-c*u)<0?(v-y)/g:(v+y)/g,y:(v=o*u-a*l)<0?(v-y)/g:(v+y)/g}}},function(t,e,n){var r=n(43),i=n(31),a=n(153).layout;t.exports=function(){var t=n(371),e=n(374),i=n(375),u=n(376),l=n(377),h=n(378),f=n(379),d=n(380),p=n(381),g=function(n,g){!function(t){t.nodes().forEach((function(e){var n=t.node(e);r.has(n,"label")||t.children(e).length||(n.label=e),r.has(n,"paddingX")&&r.defaults(n,{paddingLeft:n.paddingX,paddingRight:n.paddingX}),r.has(n,"paddingY")&&r.defaults(n,{paddingTop:n.paddingY,paddingBottom:n.paddingY}),r.has(n,"padding")&&r.defaults(n,{paddingLeft:n.padding,paddingRight:n.padding,paddingTop:n.padding,paddingBottom:n.padding}),r.defaults(n,o),r.each(["paddingLeft","paddingRight","paddingTop","paddingBottom"],(function(t){n[t]=Number(n[t])})),r.has(n,"width")&&(n._prevWidth=n.width),r.has(n,"height")&&(n._prevHeight=n.height)})),t.edges().forEach((function(e){var n=t.edge(e);r.has(n,"label")||(n.label=""),r.defaults(n,s)}))}(g);var y=c(n,"output"),v=c(y,"clusters"),m=c(y,"edgePaths"),b=i(c(y,"edgeLabels"),g),x=t(c(y,"nodes"),g,d);a(g),l(x,g),h(b,g),u(m,g,p);var _=e(v,g);f(_,g),function(t){r.each(t.nodes(),(function(e){var n=t.node(e);r.has(n,"_prevWidth")?n.width=n._prevWidth:delete n.width,r.has(n,"_prevHeight")?n.height=n._prevHeight:delete n.height,delete n._prevWidth,delete n._prevHeight}))}(g)};return g.createNodes=function(e){return arguments.length?(t=e,g):t},g.createClusters=function(t){return arguments.length?(e=t,g):e},g.createEdgeLabels=function(t){return arguments.length?(i=t,g):i},g.createEdgePaths=function(t){return arguments.length?(u=t,g):u},g.shapes=function(t){return arguments.length?(d=t,g):d},g.arrows=function(t){return arguments.length?(p=t,g):p},g};var o={paddingLeft:10,paddingRight:10,paddingTop:10,paddingBottom:10,rx:0,ry:0,shape:"rect"},s={arrowhead:"normal",curve:i.curveLinear};function c(t,e){var n=t.select("g."+e);return n.empty()&&(n=t.append("g").attr("class",e)),n}},function(t,e,n){"use strict";var r=n(43),i=n(97),a=n(12),o=n(31);t.exports=function(t,e,n){var s,c=e.nodes().filter((function(t){return!a.isSubgraph(e,t)})),u=t.selectAll("g.node").data(c,(function(t){return t})).classed("update",!0);u.exit().remove(),u.enter().append("g").attr("class","node").style("opacity",0),(u=t.selectAll("g.node")).each((function(t){var s=e.node(t),c=o.select(this);a.applyClass(c,s.class,(c.classed("update")?"update ":"")+"node"),c.select("g.label").remove();var u=c.append("g").attr("class","label"),l=i(u,s),h=n[s.shape],f=r.pick(l.node().getBBox(),"width","height");s.elem=this,s.id&&c.attr("id",s.id),s.labelId&&u.attr("id",s.labelId),r.has(s,"width")&&(f.width=s.width),r.has(s,"height")&&(f.height=s.height),f.width+=s.paddingLeft+s.paddingRight,f.height+=s.paddingTop+s.paddingBottom,u.attr("transform","translate("+(s.paddingLeft-s.paddingRight)/2+","+(s.paddingTop-s.paddingBottom)/2+")");var d=o.select(this);d.select(".label-container").remove();var p=h(d,f,s).classed("label-container",!0);a.applyStyle(p,s.style);var g=p.node().getBBox();s.width=g.width,s.height=g.height})),s=u.exit?u.exit():u.selectAll(null);return a.applyTransition(s,e).style("opacity",0).remove(),u}},function(t,e,n){var r=n(12);t.exports=function(t,e){for(var n=t.append("text"),i=function(t){for(var e,n="",r=!1,i=0;i
Exponentiation Zones (30-36)
The Root System
8 x 8 = 64 = 8²
where the power of 2 stands as exponent
#!/usr/bin/env bash
+
+edit_file () {
+
+ NUM=$(($2 + 0))
+
+ while IFS=' ' read -ra SPIN; do
+ T+=("${SPIN[0]}")
+ R+=("${SPIN[1]}")
+ A+=("${SPIN[2]}")
+ C+=("${SPIN[3]}")
+ K+=("${SPIN[4]}")
+ I+=("${SPIN[5]}")
+ N+=("${SPIN[6]}")
+ G+=("${SPIN[7]}")
+ done < /tmp/spin.txt
+
+ FRONT="---\n"
+ FRONT+="sort: ${K[$NUM]}\n"
+ FRONT+="span: ${I[$NUM]}\n"
+ FRONT+="spin: ${N[$NUM]}\n"
+ FRONT+="suit: ${G[$NUM]}\n"
+ FRONT+="---\n"
+
+ IFS=$'\n' read -d '' -r -a LINE < _Sidebar.md
+ TEXT="${LINE[$NUM]}" && TITLE=${TEXT%|*}
+ FRONT+="# $TITLE\n\n"
+
+ [[ $NUM -le 9 ]] && sed -i "1s|^|$FRONT|" $1
+ if [[ $NUM -lt 2 || $NUM == 9 ]]; then
+ mv -f $1 ${1%/*}/README.md
+ sed '1,6!d' ${1%/*}/README.md
+ fi
+}
+
+FILE=${1##*/} && SORT=${FILE%.*}
+[[ $SORT =~ ^-?[0-9]+$ ]] && edit_file $1 $SORT
+
Three (3) Layers
$True Prime Pairs:
+ (5,7), (11,13), (17,19)
+
+ layer| i | f
+ -----+-----+---------
+ | 1 | 5
+ 1 +-----+
+ | 2 | 7
+ -----+-----+--- } 36 » 6®
+ | 3 | 11
+ 2 +-----+
+ | 4 | 13
+ -----+-----+---------
+ | 5 | 17
+ 3 +-----+ } 36 » 6®
+ | 6 | 19
+ -----+-----+---------
+
$True Prime Pairs:
+(5,7), (11,13), (17,19)
+
+layer | node | sub | i | f
+------+------+-----+----------
+ | | | 1 |
+ | | 1 +-----+
+ | 1 | | 2 | (5)
+ | |-----+-----+
+ | | | 3 |
+ 1 +------+ 2 +-----+----
+ | | | 4 |
+ | +-----+-----+
+ | 2 | | 5 | (7)
+ | | 3 +-----+
+ | | | 6 |
+------+------+-----+-----+------ } (36) » 6®
+ | | | 7 |
+ | | 4 +-----+
+ | 3 | | 8 | (11)
+ | +-----+-----+
+ | | | 9 |
+ 2 +------| 5 +-----+-----
+ | | | 10 |
+ | |-----+-----+
+ | 4 | | 11 | (13)
+ | | 6 +-----+
+ | | | 12 |
+------+------+-----+-----+------------------
+ | | | 13 |
+ | | 7 +-----+
+ | 5 | | 14 | (17)
+ | |-----+-----+
+ | | | 15 |
+ 3 +------+ 8 +-----+----- } (36) » 6®
+ | | | 16 |
+ | |-----+-----+
+ | 6 | | 17 | (19)
+ | | 9 +-----+
+ | | | 18 |
+------|------|-----+-----+------
+
#!/usr/bin/env python
+
+import numpy as np
+from scipy import linalg
+
+class SU3(np.matrix):
+ GELLMANN_MATRICES = np.array([
+ np.matrix([ #lambda_1
+ [0, 1, 0],
+ [1, 0, 0],
+ [0, 0, 0],
+ ], dtype=np.complex),
+ np.matrix([ #lambda_2
+ [0,-1j,0],
+ [1j,0, 0],
+ [0, 0, 0],
+ ], dtype=np.complex),
+ np.matrix([ #lambda_3
+ [1, 0, 0],
+ [0,-1, 0],
+ [0, 0, 0],
+ ], dtype=np.complex),
+ np.matrix([ #lambda_4
+ [0, 0, 1],
+ [0, 0, 0],
+ [1, 0, 0],
+ ], dtype=np.complex),
+ np.matrix([ #lambda_5
+ [0, 0,-1j],
+ [0, 0, 0 ],
+ [1j,0, 0 ],
+ ], dtype=np.complex),
+ np.matrix([ #lambda_6
+ [0, 0, 0],
+ [0, 0, 1],
+ [0, 1, 0],
+ ], dtype=np.complex),
+ np.matrix([ #lambda_7
+ [0, 0, 0 ],
+ [0, 0, -1j],
+ [0, 1j, 0 ],
+ ], dtype=np.complex),
+ np.matrix([ #lambda_8
+ [1, 0, 0],
+ [0, 1, 0],
+ [0, 0,-2],
+ ], dtype=np.complex) / np.sqrt(3),
+ ])
+
+
+ def computeLocalAction(self):
+ pass
+
+ @classmethod
+ def getMeasure(self):
+ pass
+
$True Prime Pairs:
+(5,7), (11,13), (17,19)
+
+layer | node | sub | i | f
+------+------+-----+----------
+ | | | 1 |
+ | | 1 +-----+
+ | 1 | | 2 | (5)
+ | |-----+-----+
+ | | | 3 |
+ 1 +------+ 2 +-----+----
+ | | | 4 |
+ | +-----+-----+
+ | 2 | | 5 | (7)
+ | | 3 +-----+
+ | | | 6 |
+------+------+-----+-----+------ } (36) » 6® -------------
+ | | | 7 | |
+ | | 4 +-----+ |
+ | 3 | | 8 | (11) |
+ | +-----+-----+ |
+ | | | 9 | <-------- Eightfold Way = 8 × (6®+6®) = 96®
+ 2 +------| 5 +-----+----- |
+ | | | 10 | |
+ | |-----+-----+ |
+ | 4 | | 11 | (13) |
+ | | 6 +-----+ |
+ | | | 12 | |
+------+------+-----+-----+------------------ |
+ | | | 13 | |
+ | | 7 +-----+ |
+ | 5 | | 14 | (17) |
+ | |-----+-----+ |
+ | | | 15 | |
+ 3 +------+ 8 +-----+----- } (36) » 6® -----------------
+ | | | 16 |
+ | |-----+-----+
+ | 6 | | 17 | (19)
+ | | 9 +-----+
+ | | | 18 |
+------|------|-----+-----+------
+
The Four (4) Dimensions
$True Prime Pairs:
+(5,7), (11,13), (17,19)
+
+layer | node | sub | i | f
+------+------+-----+----------
+ | | | 1 |
+ | | 1 +-----+
+ | 1 | | 2 | (5)
+ | |-----+-----+
+ | | | 3 |
+ 1 +------+ 2 +-----+----
+ | | | 4 |
+ | +-----+-----+
+ | 2 | | 5 | (7)
+ | | 3 +-----+
+ | | | 6 |
+------+------+-----+-----+------ } (36) » 6® 👈 up toward ✔️
+ | | | 7 |
+ | | 4 +-----+
+ | 3 | | 8 | (11)
+ | +-----+-----+
+ | | | 9 |
+ 2 +------| 5 +-----+-----
+ | | | 10 |
+ | |-----+-----+
+ | 4 | | 11 | (13)
+ | | 6 +-----+
+ | | | 12 |
+------+------+-----+-----+------------------
+ | | | 13 |
+ | | 7 +-----+
+ | 5 | | 14 | (17)
+ | |-----+-----+
+ | | | 15 |
+ 3 +------+ 8 +-----+----- } (36) » 6® 👈 down from ✔️
+ | | | 16 |
+ | |-----+-----+
+ | 6 | | 17 | (19)
+ | | 9 +-----+
+ | | | 18 |
+------|------|-----+-----+------
+
Extra Dimensions
Syntax Description Last
Standard Model
How many quarks?
Answer-1: 3 generation x 3 color x 2 types x 2 each = 36 quarks
+
Answer-2: 6 flavour x 3 colors x 2 types = 36 quarks
+
Answer-3: 6 flavour x 3 colour x 4 bispinor = 72 quarks
+
There are 72 quarks
Fermion | spinors | charged | neutrinos | quark | components
+ Field | (s) | (c) | (n) | (q=s.c.n) | Σ(c+n+q)
+===========+=========+=========+===========+===========+============
+bispinor-1 | 2 | 3 | 3 | 18 | 24
+-----------+---------+---------+-----------+-----------+------------ } 48
+bispinor-2 | 2 | 3 | 3 | 18 | 24
+===========+=========+=========+===========+===========+===========
+bispinor-3 | 2 | 3 | 3 | 18 | 24
+-----------+---------+---------+-----------+-----------+------------ } 48
+bispinor-4 | 2 | 3 | 3 | 18 | 24
+===========+=========+=========+===========+===========+============
+ Total | 8 | 12 | 12 | 72 | 96
+
Free Parameters
$True Prime Pairs:
+(5,7), (11,13), (17,19)
+
+layer | node | sub | i | f. MEC 30 / 2
+------+------+-----+-----+------ ‹------------------------------ 0 {-1/2}
+ | | | 1 | --------------------------
+ | | 1 +-----+ |
+ | 1 | | 2 | (5) |
+ | |-----+-----+ |
+ | | | 3 | |
+ 1 +------+ 2 +-----+---- |
+ | | | 4 | |
+ | +-----+-----+ |
+ | 2 | | 5 | (7) |
+ | | 3 +-----+ |
+ | | | 6 | 11s ‹-- ∆28 = (71-43)
+------+------+-----+-----+------ } (36) |
+ | | | 7 | |
+ | | 4 +-----+ |
+ | 3 | | 8 | (11) |
+ | +-----+-----+ |
+ | | | 9 |‹-- ∆9 + ∆18 = ∆27 |
+ 2 +------| 5* +-----+----- |
+ | | | 10 | |
+ | |-----+-----+ |
+ | 4 | | 11 | (13) --------------------- ∆32
+ | | 6 +-----+ ‹------------------------------ 15 {0}
+ | | | 12 |---------------------------
+------+------+-----+-----+------------ |
+ | | | 13 | |
+ | | 7 +-----+ |
+ | 5 | | 14 | (17) |
+ | |-----+-----+ |
+ | | | 15 | 7s ‹-- ∆24 = (43-19)
+ 3* +------+ 8 +-----+----- } (36) |
+ | | | 16 | |
+ | |-----+-----+ |
+ | 6 | | 17 | (19) ‹-- parameters ✔️ |
+ | | 9 +-----+ |
+ | | | 18 | -------------------------- ∆68 - ∆18 = ∆50
+------|------|-----+-----+----- ‹----------------------------------- 30 {+1/2}
+
Fermion | spinors | charged | neutrinos | quark | components | parameter
+ Field | (s) | (c) | (n) | (q=s.c.n) | Σ(c+n+q | (complex)
+===========+=========+=========+===========+===========+============+===========
+bispinor-1 | 2 | 3 | 3 | 18 | 24 | 19+i5 ✔️
+-----------+---------+---------+-----------+-----------+------------+-----------
+bispinor-2 | 2 | 3 | 3 | 18 | 24 | 17+i7 ✔️
+===========+=========+=========+===========+===========+============+===========
+bispinor-3 | 2 | 3 | 3 | 18 | 24 | ❓
+-----------+---------+---------+-----------+-----------+------------+-----------
+bispinor-4 | 2 | 3 | 3 | 18 | 24 | ❓
+===========+=========+=========+===========+===========+============+===========
+ Total | 8 | 12 | 12 | 72 | 96 | ❓
+
Fermion | spinors | charged | neutrinos | quark | components | parameter
+ Field | (s) | (c) | (n) | (q=s.c.n) | Σ(c+n+q | (complex)
+===========+=========+=========+===========+===========+============+===========
+bispinor-1 | 2 | 3 | 3 | 18 | 24 | 19+i5
+-----------+---------+---------+-----------+-----------+------------+-----------
+bispinor-2 | 2 | 3 | 3 | 18 | 24 | 17+i7
+===========+=========+=========+===========+===========+============+===========
+bispinor-3 | 2 | 3 | 3 | 18 | 24 | 11+i13 ✔️
+-----------+---------+---------+-----------+-----------+------------+-----------
+bispinor-4 | 2 | 3 | 3 | 18 | 24 | ❓
+===========+=========+=========+===========+===========+============+===========
+ Total | 8 | 12 | 12 | 72 | 96 | ❓
+
The Seven (7) Groups
$True Prime Pairs:
+(5,7), (11,13), (17,19)
+
+layer | node | sub | i | f
+------+------+-----+---------
+ | | | 1 | --------------------------
+ | | 1 +-----+ |
+ | 1 | | 2 | (5) |
+ | |-----+-----+ |
+ | | | 3 | |
+ 1 +------+ 2 +-----+---- |
+ | | | 4 | |
+ | +-----+-----+ |
+ | 2 | | 5 | (7) |
+ | | 3 +-----+ |
+ | | | 6 | 11s ✔️
+------+------+-----+-----+------ } (36) |
+ | | | 7 | |
+ | | 4 +-----+ |
+ | 3 | | 8 | (11) |
+ | +-----+-----+ |
+ | | | 9 | |
+ 2 +------| 5 +-----+----- |
+ | | | 10 | |
+ | |-----+-----+ |
+ | 4 | | 11 | (13) ---------------------
+ | | 6 +-----+ <---------------- strip
+ | | | 12 |---------------------------
+------+------+-----+-----+------------ |
+ | | | 13 | |
+ | | 7 +-----+ |
+ | 5 | | 14 | (17) |
+ | |-----+-----+ |
+ | | | 15 | 7s ✔️
+ 3 +------+ 8 +-----+----- } (36) |
+ | | | 16 | |
+ | |-----+-----+ |
+ | 6 | | 17 | (19) |
+ | | 9 +-----+ |
+ | | | 18 | --------------------------
+------|------|-----+-----+------
+
$True Prime Pairs:
+(5,7), (11,13), (17,19)
+
+layer | node | sub | i | f
+------+------+-----+----------
+ | | | 1 | --------------------------
+ | | 1 +-----+ |
+ | 1 | | 2 | (5) |
+ | |-----+-----+ |
+ | | | 3 | |
+ 1 +------+ 2 +-----+---- |
+ | | | 4 | |
+ | +-----+-----+ |
+ | 2 | | 5 | (7) |
+ | | 3 +-----+ |
+ | | | 6 | 11s
+------+------+-----+-----+------ } (36) |
+ | | | 7 | |
+ | | 4 +-----+ |
+ | 3 | | 8 | (11) |
+ | +-----+-----+ |
+ | | | 9 | |
+ 2 +------| 5 +-----+----- |
+ | | | 10 | |
+ | |-----+-----+ |
+ | 4 | | 11 | (13) ---------------------
+ | | 6 +-----+ <---------------- strip
+ | | | 12 |---------------------------
+------+------+-----+-----+------------ |
+ | | | 13 | |
+ | | 7 +-----+ |
+ | 5 | | 14 | (17) |
+ | |-----+-----+ | extra
+ | | | 15 | 7s <-- parameters ✔️
+ 3 +------+ 8 +-----+----- } (36) |
+ | | | 16 | |
+ | |-----+-----+ certain |
+ | 6 | | 17 | (19) <-- parameters ✔️ |
+ | | 9 +-----+ |
+ | | | 18 | --------------------------
+------|------|-----+-----+------
+
The True Prime Pairs:
+(5,7), (11,13), (17,19)
+
+|--------------- 7¤ ---------------|👈
+|-------------- {89} --------------|
++----+----+----+----+----+----+----+----+----+----+----+----+----+----+
+| 5 | 7 | 11 |{13}| 17 | 19 | 17 |{12}| 11 | 19 |{18}| 18 | 12 |{13}|
++----+----+----+----+----+----+----+----+----+----+----+----+----+----+
+ |---- {48} ----|---- {48} ----|---- {43} ----|
+ |----- 3¤ -----|----- 3¤ -----|----- 3¤ -----|
+ |-------------------- 9¤ --------------------|👈
+
+ Fermion | spinors | charged | neutrinos | quark | components | parameter
+ Field | (s) | (c) | (n) | (q=s.c.n) | Σ(c+n+q | (complex)
+===========+=========+=========+===========+===========+============+===========
+bispinor-1 | 2 | 3 | 3 | 18 | 24 | 19+i5
+-----------+---------+---------+-----------+-----------+------------+-----------
+bispinor-2 | 2 | 3 | 3 | 18 | 24 | 👉17+i7
+===========+=========+=========+===========+===========+============+===========
+bispinor-3 | 2 | 3 | 3 | 18 | 24 | 11+i13👈
+-----------+---------+---------+-----------+-----------+------------+-----------
+bispinor-4 | 2 | 3 | 3 | 18 | 24 | 19+i5
+===========+=========+=========+===========+===========+============+===========
+ Total | 8 | 12 | 12 | 72 | 96 | 66+i30
+
The Quantum Gravity
$True Prime Pairs:
+(5,7), (11,13), (17,19)
+
++----+----+----+----+----+-👇-+
+| 5 | 7 | 11 |{13}| 17 | 19 |
++----+----+----+----+----+----+
+|------------ {72} -----------|
+|------------- 6¤ ------------|
+
+The Fermion Fields
+(19,17,i12), (11,19,i18), (18,12,i13)
+
++-👇-+----+----+----+----+----+----+----+----+
+| 19 | 17 |{12}| 11 | 19 |{18}| 18 | 12 |{13}|
++----+----+----+----+----+----+----+----+----+
+|---- {48} ----|---- {48} ----|---- {43} ----|
+|------------ {96} -----------|----- 3¤ -----|
+
+Spontaneous Symmetry Breaking:
+(5,7), (11,13,17) , (19,17,12), (11,19,18), (18,12,13)
+
+|--------------- 7¤ ---------------|
+|-------------- {89} --------------|
++----+----+----+----+----+-👇-+-👇-+----+----+----+----+----+----+----+
+| 5 | 7 | 11 |{13}| 17 | 19 | 17 |{12}| 11 | 19 |{18}| 18 | 12 |{13}|
++----+----+----+----+----+----+----+----+----+----+----+----+----+----+
+ |-- {36} -|------ {60} -------|---- {43} ----|
+ |--- 2¤ --|------- 4¤ --------|----- 3¤ -----|
+ |-------------------- 9¤ --------------------|
+
$True Prime Pairs:
+(5,7), (11,13), (17,19)
+
++----+----+----+----+----+-👇-+
+| 5 | 7 | 11 |{13}| 17 | 19 |
++----+----+----+----+----+----+
+|------------ {72} -----------|
+|------------- 6¤ ------------|
+
+Spontaneous Symmetry Breaking:
+(5,7), (11,13,17) , (19,17,12), (11,19,18), (18,12,13)
+
+|--------------- 7¤ ---------------|
+|-------------- {89} --------------|
++----+----+----+----+----+-👇-+-👇-+----+----+----+----+----+----+----+
+| 5 | 7 | 11 |{13}| 17 | 19 | 17 |{12}| 11 | 19 |{18}| 18 | 12 |{13}|
++----+----+----+----+----+----+----+----+----+----+----+----+----+----+
+ |-- {36} -|------ {60} -------|---- {43} ----|
+ |--- 2¤ --|------- 4¤ --------|----- 3¤ -----|
+ |-------------------- 9¤ --------------------|
+
+|--------------- 7¤ ---------------|
+|-------------- {89} --------------|
++----+----+----+----+----+-💢-+----+----+----+----+----+----+----+----+
+| 5 | 7 | 11 |{13}| 17 | 19 | 17 |{12}| 11 | 19 |{18}| 18 | 12 |{13}|
++----+----+----+----+----+----+----+----+-👇-+----+----+----+----+----+
+ |-👇-|--------- {77} ---------|---- {43} ----|✔️
+ |-1¤ |---------- 5¤ ----------|----- 3¤ -----|
+ |-------------------- 9¤ --------------------|
+
14 + 7 × 16 = 126
integral octonions. It was shown that the set of transformations which preserve the octonion algebra of the root system of E7 is the adjoint Chevalley group G2(2). It is possible to decompose these 126 imaginary octonions into eighteen (18) sets of seven (7) imaginary octonionic units that can be transformed to each other by the finite subgroup of matrices. These lead to 18 sets of 7, which we see in figures figure-77 and figure-88. (M-theory, Black Holes and Cosmology - pdf) Fermion | spinors | charged | neutrinos | quark | components | parameter
+ Field | (s) | (c) | (n) | (q=s.c.n) | Σ(c+n+q | (complex)
+===========+=========+=========+===========+===========+============+===========
+bispinor-1 | 2 | 3 | 3 | 18 | 24 | 19
+-----------+---------+---------+-----------+-----------+------------+-- 17💢36
+bispinor-2 | 2 | 3 | 3 | 18 | 24 | i12 ✔️
+===========+=========+=========+===========+===========+============+===========
+bispinor-3 | 2 | 3 | 3 | 18 | 24 | 11
+-----------+---------+---------+-----------+-----------+------------+-- 19💢30
+bispinor-4 | 2 | 3 | 3 | 18 | 24 | i18 ✔️
+===========+=========+=========+===========+===========+============+===========
+ SubTotal | 8 | 12 | 12 | 72 | 96 | 66+i30
+===========+=========+=========+===========+===========+============+===========
+
$True Prime Pairs:
+(5,7), (11,13), (17,19)
+
+Prime Loops:
+π(10) = 4 (node)
+π(100) = 25 (partition)
+π(1000) - 29 = 139 (section)
+π(10000) - 29th - 29 = 1091 (segment)
+π(100000) - 109th - 109 = 8884 (texture)
+Sum: 4 + 25 + 139 + 1091 + 8884 = 10143 (object)
+
+ | 168 | 618 |
+-----+-👇--+-👇--+-----+-----+ ---
+ 19¨ | 3¨ | 4¨ | 6¨ | 6¨ | 4¤ -----> assigned to "id:30" |
+-----+-----+-----+-----+-----+ |
+ 17¨ | {5¨}| {3¨}| 2¨ | 7¨👈 4¤ -----> assigned to "id:31" |
+ +-----+-----+-----+-----+ |
+{12¨}| 6¨ | 6¨ | 2¤ (M & F) -----> assigned to "id:32" |
+ +-----+-----+-----+ 96¨
+ 11¨ | 3¨ | {3¨}| {5¨}| 3¤ -----> assigned to "id:33" |
+-----+-----+-----+-----+-----+ |
+ 19¨ | 4¨ | 4¨ | 5¨ | 6¨ | 4¤ -----> assigned to "id:34" |
+ +-----+-----+-----+-----+ |
+{18¨}| 5¨ | 5¨ | 8¨ | 3¤ -----> assigned to "id:35" |
+ +-----+-----+-----+-----+-----+-----+-----+-----+-----+ ---
+ 43¨ | {3¨}| {5¨}| 5¨ | {5¨}| {3¨}| 7¨ | {5¨}| {3¨}| 7¨ | 9¤ (C1 & C2) 43¨
+-----+-----+-----+-----+-----+-----+-----+-----+-----+-----+ ---
+139¨ |----- 13¨ -----|------ 15¨ ------|------ 15¨ ------|
+ | 1 2 3 | 4 5 6 | 7 8 9 |
+ Δ Δ Δ
+ Mod 30 Mod 60 Mod 90
+
$True Prime Pairs:
+(5,7), (11,13), (17,19)
+
+layer | node | sub | i | f
+------+------+-----+-----+------
+ | | | 1 | --------------------------
+ | | 1 +-----+ |
+ | 1 | | 2 | (5) |
+ | |-----+-----+ |
+ | | | 3 | |
+ 1 +------+ 2 +-----+---- |
+ | | | 4 | |
+ | +-----+-----+ |
+ | 2 | | 5 | (7) |
+ | | 3 +-----+ |
+ | | | 6 | 11s ‹-- ∆28 = (71-43) ✔️
+------+------+-----+-----+------ } (36) |
+ | | | 7 | |
+ | | 4 +-----+ |
+ | 3 | | 8 | (11) |
+ | +-----+-----+ |
+ | | | 9 | |
+ 2 +------| 5* +-----+----- |
+ | | | 10 | |
+ | |-----+-----+ |
+ | 4 | | 11 | (13) ---------------------
+ | | 6 +-----+ <-------------- strip of the id: 37 (TOE)
+ | | | 12 |---------------------------
+------+------+-----+-----+------------ |
+ | | | 13 | |
+ | | 7 +-----+ |
+ | 5 | | 14 | (17) |
+ | |-----+-----+ |
+ | | | 15 | 7s ‹-- ∆24 = (43-19) ✔️
+ 3* +------+ 8 +-----+----- } (36) |
+ | | | 16 | |
+ | |-----+-----+ |
+ | 6 | | 17 | (19) |
+ | | 9 +-----+ |
+ | | | 18 | --------------------------
+------|------|-----+-----+-----
+
$True Prime Pairs:
+(5,7$True Prime Pairs:
+(5,7), (11,13), (17,19)
+
+layer | node | sub | i | f
+------+------+-----+-----+------
+ | | | 1 | --------------------------
+ | | 1 +-----+ |
+ | 1 | | 2 | (5) |
+ | |-----+-----+ |
+ | | | 3 | |
+ 1 +------+ 2 +-----+---- |
+ | | | 4 | |
+ | +-----+-----+ |
+ | 2 | | 5 | (7) |
+ | | 3 +-----+ |
+ | | | 6 | 11s ‹-- ∆28 = (71-43)
+------+------+-----+-----+------ } (36) |
+ | | | 7 | |
+ | | 4 +-----+ |
+ | 3 | | 8 | (11) |
+ | +-----+-----+ |
+ | | | 9 | |
+ 2 +------| 5* +-----+----- |
+ | | | 10 | |
+ | |-----+-----+ |
+ | 4 | | 11 | (13) ---------------------
+ | | 6 +-----+ <-----vacuum energy <--- ∆60 = (131-71) ✔️
+ | | | 12 |---------------------------
+------+------+-----+-----+------------ |
+ | | | 13 | |
+ | | 7 +-----+ |
+ | 5 | | 14 | (17) |
+ | |-----+-----+ |
+ | | | 15 | 7s ‹-- ∆24 = (43-19)
+ 3* +------+ 8 +-----+----- } (36) |
+ | | | 16 | |
+ | |-----+-----+ |
+ | 6 | | 17 | (19) |
+ | | 9 +-----+ |
+ | | | 18 | --------------------------
+------|------|-----+-----+-----
+
$True Prime Pairs:
+(5,7), (11,13), (17,19)
+
+Prime Loops:
+π(10) = 4 (node)
+π(100) = 25 (partition)
+π(1000) - 29 = 139 (section)
+π(10000) - 29th - 29 = 1091 (segment)
+π(100000) - 109th - 109 = 8884 (texture)
+Sum: 4 + 25 + 139 + 1091 + 8884 = 10143 (object)
+
+ | 168 | 618 |
+-----+-----+-----+-----+-----+ ---
+ 19¨ | 3¨ | 4¨ | 6¨ | 6¨ | 4¤ -----> assigned to "id:30" 19¨
+-----+-👇--+-👇--+-----+-----+ ---
+ 17¨ | {5¨}| {3¨}| 2¨ | 7¨ | 4¤ -----> assigned to "id:31" |
+ +-----+-----+-----+-----+ |
+{12¨}| 6¨ | 6¨ | 2¤ (M & F) -----> assigned to "id:32" |
+ +-----+-----+-----+ |
+ 11¨ | 3¨ | {3¨}| {5¨}| 3¤ ---> Np(33) assigned to "id:33" -----> 77¨
+-----+-----+-----+-----+-----+ |
+ 19¨ | 4¨ | 4¨ | 5¨ | 6¨ | 4¤ -----> assigned to "id:34" |
+ +-----+-----+-----+-----+ |
+{18¨}| 5¨ | 5¨ | 8¨ | 3¤ -----> assigned to "id:35" |
+ +-----+-----+-----+-👇--+-👇--+-----+-👇--+-👇--+-----+ ---
+ 43¨ | {3¨}| {5¨}| 5¨ | {5¨}| {3¨}| 7¨ | {5¨}| {3¨}| 7¨ | 9¤ (C1 & C2) 43¨
+-----+-----+-----+-----+-----+-----+-----+-----+-----+-----+ ---
+139¨ |----- 13¨ -----|------ 15¨ ------|------ 15¨ ------|
+ | 1 2 3 | 4 5 6 | 7 8 9 |
+ Δ Δ Δ
+ Mod 30 Mod 60 Mod 90
+
n = 1,...,7
, and 1+27=28
scalar fields, parametrizing the coset space GL(7)/SO(7). The dimensional reduction of the antisymmetric 3-form to D = 4 dimensions gives rise to one 3-form field, seven 2-form fields. (11D Supergravity and Hidden Symmetries - pdf)
$True Prime Pairs:
+(5,7), (11,13), (17,19)
+
+Prime Loops:
+π(10) = 4 (node)
+π(100) = 25 (partition)
+π(1000) - 29 = 139 (section)
+π(10000) - 29th - 29 = 1091 (segment)
+π(100000) - 109th - 109 = 8884 (texture)
+Sum: 4 + 25 + 139 + 1091 + 8884 = 10143 (object)
+
+ | 168 | 618 |
+-----+-----+-----+-----+-----+ ---
+ 19¨ | 3¨ | 4¨ | 6¨ | 6¨ | 4¤ -----> assigned to "id:30" 19¨
+-----+-----+-----+-👇--+-👇--+ ---
+ 17¨ | {5¨}| {3¨}| 2¨ | 7¨ | 4¤ -----> assigned to "id:31" |
+ +-----+-----+-----+-----+ |
+{12¨}| 6¨ | 6¨ | 2¤ (M & F) -----> assigned to "id:32" |
+ +-👇--+-👇--+-----+ |
+ 11¨ | 3¨ | {3¨}| {5¨}| 3¤ ---> Np(33) assigned to "id:33" -----> 77¨
+-----+-----+-----+-----+-----+ |
+ 19¨ | 4¨ | 4¨ | 5¨ | 6¨ | 4¤ -----> assigned to "id:34" |
+ +-----+-----+-----+-----+ |
+{18¨}| 5¨ | 5¨ | 8¨ | 3¤ -----> assigned to "id:35" |
+ +-----+-----+-----+-----+-----+-----+-----+-----+-----+ ---
+ 43¨ | {3¨}| {5¨}| 5¨ | {5¨}| {3¨}| 7¨ | {5¨}| {3¨}| 7¨ | 9¤ (C1 & C2) 43¨
+-----+-----+-----+-----+-----+-----+-----+-----+-----+-----+ ---
+139¨ |----- 13¨ -----|------ 15¨ ------|------ 15¨ ------|
+ | 1 2 3 | 4 5 6 | 7 8 9 |
+ Δ Δ Δ
+ Mod 30 Mod 60 Mod 90
+
$True Prime Pairs:
+(5,7), (11,13), (17,19)
+
+Prime Loops:
+π(10) = 4 (node)
+π(100) = 25 (partition)
+π(1000) - 29 = 139 (section)
+π(10000) - 29th - 29 = 1091 (segment)
+π(100000) - 109th - 109 = 8884 (texture)
+Sum: 4 + 25 + 139 + 1091 + 8884 = 10143 (object)
+
+ | 168 | 618 |
+-----+-----+-----+-----+-----+ ---
+ 19¨ | 3¨ | 4¨ | 6¨ | 6¨ | 4¤ -----> assigned to "id:30" 19¨
+-----+-----+-----+-----+-----+ ---
+ 17¨ | {5¨}| {3¨}| 2¨ | 7¨ | 4¤ -----> assigned to "id:31" |
+ +-----+-----+-----+-----+ |
+{12¨}| 6¨ | 6¨ | 2¤ (M & F) -----> assigned to "id:32" |
+ +-👇--+-👇--+-----+ |
+ 11¨ | 3¨ | {3¨}| {5¨}| 3¤ ---> Np(33) assigned to "id:33" -----> 77¨
+-----+-----+-----+-----+-----+ |
+ 19¨ | 4¨ | 4¨ | 5¨ | 6¨ | 4¤ -----> assigned to "id:34" |
+ +-----+-----+-----+-----+ |
+{18¨}| 5¨ | 5¨ | 8¨ | 3¤ -----> assigned to "id:35" |
+ +-----+-----+-----+-----+-----+-----+-----+-----+-----+ ---
+ 43¨ | {3¨}| {5¨}| 5¨ | {5¨}| {3¨}| 7¨ | {5¨}| {3¨}| 7¨ | 9¤ (C1 & C2) 43¨
+-----+-----+-----+-----+-----+-----+-----+-----+-----+-----+ ---
+139¨ |----- 13¨ -----|------ 15¨ ------|------ 15¨ ------|
+ | 1 2 3 | 4 5 6 | 7 8 9 |
+ Δ Δ Δ
+ Mod 30 Mod 60 Mod 90
+
12+3+2+8+1=26
free parameters.The 11 Dimensions
T7 = 28; 28 x 4 = 112
),T32 = 528; 528 x 4 = 2112
),4 x 32 = 128
is the perimeter of the square base which has an area of 32^2 = 1024 = 2^10
). (PrimesDemystified)
8§8 |------- 5® --------|------------ 7® --------------|
+ |QED|------------------- QCD ----------------------|👈
+ | 1 |-------------- 77 = 4² + 5² + 6² -------------|
+------+---|---+---+---+---+---+---+---+---+----+----+----+
+ repo |{1}|{2}| 3 | 4 | 5 | 6 | 7 | 8 | 9 | 10 | 11 |{12}| 1,77
+------+---|---+---+---+---+---+---+---+---+----+----+----+
+ user | 7 | - | - | - | - | 7 | 8 | - | - | 8 | 8 | 3 |
+------+---|👇-+👇-+---+---+---+---+---+---+----+----+----+ 7,78
+ main | - | 9 | 7 | 9 | 6 | - | - | 8 | 5 | - | - | - |
+------+---|---+---+---+---+---+---+---+---+----+----+----+
+ Δ | Δ | Δ | Δ
+ Φ17|Φ29 | 96-99| 100 - 123 ({24})
+ |--- A,T,G,C ---| | └── 100 - 103 (4x) » 100
+ Δ 2x2 = 4x |------- 2x3 = 6x -------| └── 104 - 109 (6x) » 30
+ {98} | └── 110 - 123 (14x)» 70
+
The pairwise disjoint
Fermion | spinors | charged | neutrinos | quark | components | parameter
+ Field | (s) | (c) | (n) | (q=s.c.n) | Σ(c+n+q | (complex)
+===========+=========+=========+===========+===========+============+===========
+bispinor-1 | 2 | 3 | 3 | 18 | 24 | 19+i5
+-----------+---------+---------+-----------+-----------+------------+-----------
+bispinor-2 | 2 | 3 | 3 | 18 | 24 | 17+i7
+===========+=========+=========+===========+===========+============+===========
+bispinor-3 | 2 | 3 | 3 | 18 | 24 | 11+i13
+-----------+---------+---------+-----------+-----------+------------+-----------
+bispinor-4 | 2 | 3 | 3 | 18 | 24 | 19+i5
+===========+=========+=========+===========+===========+============+===========
+ Total | 8 | 12 | 12 | 72 | 96 | 66+i30 ✔️
+
Bispinors | spinors | charged | neutrinos | quark | components | parameter
+ Field | (s) | (c) | (n) | (q=s.c.n) | Σ(c+n+q | (complex)
+===========+=========+=========+===========+===========+============+===========
+bispinor-1 | 2 | 3 | 3 | 18 | 24 | 19
+-----------+---------+---------+-----------+-----------+------------+-- 17
+bispinor-2 | 2 | 3 | 3 | 18 | 24 | i5+i7 ✔️
+===========+=========+=========+===========+===========+============+===========
+bispinor-3 | 2 | 3 | 3 | 18 | 24 | 11
+-----------+---------+---------+-----------+-----------+------------+-- 19
+bispinor-4 | 2 | 3 | 3 | 18 | 24 | i13+i5 ✔️
+===========+=========+=========+===========+===========+============+===========
+ Total | 8 | 12 | 12 | 72 | 96 | 66+i30
+
Parsering Structure
1 + 7 + 29 = 37
including one (1) main page.7 x 11 = 77
partitions.Grand Unification
$True Prime Pairs:
+(5,$True Prime Pairs:
+ (5,7), (11,13), (17,19)
+
+ layer| i | f
+ -----+-----+---------
+ | 1 | 5
+ 1 +-----+
+ | 2 | 7
+ -----+-----+--- } 36 » 6®
+ | 3 | 11
+ 2 +-----+
+ | 4 | 13
+ -----+-----+---------
+ | 5 | 17
+ 3 +-----+ } 36 » 6®
+ | 6 | 19
+ -----+-----+---------
+
+layer | node | sub | i | f
+------+------+-----+----------
+ | | | 1 | -------------------- _site --- 71 = 72-1
+ | | 1 +-----+ |
+ | 1 | | 2 | (5) _saas
+ | |-----+-----+ |
+ | | | 3 | --------- _data
+ 1 +------+ 2 +-----+---- | |
+ | | | 4 | 5x --- _posts
+ | +-----+-----+ | | |
+ | 2 | | 5 | (7) ----- | _drafts
+ | | 3 +-----+ | |
+289+11=300 | | 6 | | _plugins
+------+------+-----+-----+----- 72 x 6 7x ------------ 11x = 77 (rational)◄--
+ | | | 7 | | _includes |
+ | | 4 +-----+ | | |
+ | 3 | | 8 | (11) --- | _layouts |
+ | +-----+-----+ | | | |
+ | | | 9 | 2x --- assets (69 = 72-3) |
+ 2 +------| 5 +-----+----- | | |
+ | | | 10 | --------- _saas |
+ | |-----+-----+ | |
+ | 4 | | 11 | (13) ----------------_site -- 71 = 72-1 |
+ | | 6 +-----+ |
+329+71=400 | | 12 |------------------------------ 70 = 72-2 |
+------+------+-----+-----+ 11x
+ | | | 13 | |
+ | | 7 +-----+ |
+ | 5 | | 14 | (17) ◄------------------------------------------- (17)
+ | |-----+-----+ |
+ | | | 15 | ◄-- 42 x 6 partitions of 13 (irrational) |
+ 3 +------+ 8 +-----+----- +
+ | | | 16 | |
+ | |-----+-----+ |
+ | 6 | | 17 | (19) ◄------------------------------------------- (19)
+ | | 9 +-----+ |
+168+32=200 | | | 18 |------------------------------ 68 = 72-4 |
+------|------|--|--+-----+ |
+ 900 ----- |
+ |
+
document.md
that specifies layout: docs
gets pushed into the {{ content }}
tag of the layout file docs.html
. Because the docs layout itself specifies layout: page
, the content from docs.html
gets pushed into the {{ content }}
tag in the layout file page.html
. Finally because the page layout specifies layout: default
, the content from page.html
gets pushed into the {{ content }}
tag of the layout file default.html
. (JekyllRb)Default Configuration
{
+ "title":"Mapping System",
+ "content":"<p>Hello, <strong>world</strong>.\nI am here.</p>\n",
+ "links": [
+ {"title":"Introduction","url":"https://www.eq19.com/intro/"},
+ {"title":"Go tour on Mapping System ","url":"https://www.eq19.com/maps/"},
+ {"title":"A backed pretty display for markdown","url":"https://www.eq19.com/gistio/"},
+ {"title":"Gist.io for programmers","url":"https://gist.io/@eq19/d2336e28e79702acf38edd182003d5e0"}
+ ]
+}
+