Quantum Gravity (feed)

Effective field theories have been a mainstay of theoretical physics since the 1930s but they haven't helped all that much with quantum gravity.

Tip

This section is referring to wiki page-23 of main section-1 that is from the spin section-127 by prime spin-32 and span- with the partitions as below.

/feed

  1. Addition Zones (0-18)
    1. True Prime Pairs
    2. Primes Platform
    3. Pairwise Scenario
    4. Power of Magnitude
    5. The Pairwise Disjoint
    6. The Prime Recycling ΞΆ(s)
    7. Implementation in Physics
  2. Multiplication Zones (18-30)
    1. Symmetrical Breaking (spin 8)
    2. The Angular Momentum (spin 9)
    3. Entrypoint of Momentum (spin 10)
    4. The Mapping of Spacetime (spin 11)
    5. Similar Order of Magnitude (spin 12)
    6. Searching for The Graviton (spin 13)
    7. Elementary Retracements (spin 14)
    8. Recycling of Momentum (spin 15)
    9. Exchange Entrypoint (spin 16)
    10. The Mapping Order (spin 17)
    11. Magnitude Order (spin 18)
  3. Exponentiation Zones (30-36)
    1. Electrodynamics (maps)
    2. Quantum Gravity (feed)
    3. Chromodynamics (lexer)
    4. Electroweak Theory (parser)
    5. Grand Unified Theory (syntax)
  4. Identition Zones (36-102)
    1. Theory of Everything (span 12)
    2. Everything is Connected (span 11)
    3. Truncated Perturbation (span 10)
    4. Quadratic Polynomials (span 9)
    5. Fundamental Forces (span 8)
    6. Elementary Particles (span 7)
    7. Basic Transformation (span 6)
    8. Hidden Dimensions (span 5)
    9. Parallel Universes (span 4)
    10. Vibrating Strings (span 3)
    11. Series Expansion (span 2)
    12. Wormhole Theory (span 1)

Here we decided to take a concept that gravity enter the event horizons of black holes and tunnel out again to deposit it into the background.

Event horizons

18

images (7)

19

images (6)

22

316503 image0

37

worm

22

quantum_anticentrifugal_force

Eternal Cyclic

We would expect that the quantum theory reduces to Einstein's theory of gravity. There is no way to put a black hole into the Hamiltonian.

searching graviton

Einstein's theory of General Relativity states that spacetime is curved by the presence of mass. This curvature influences the motion other objects with mass and gives rise to gravitation. Thus, gravity is a result of geometric features in spacetime.

.4dfbafd3f1e223eff196f2b8691bb992

21

main-qimg-b18921fc2fe38539d30c68227a3b41cc-pjlq

38

IMG_20240116_151732

fisica49_01

maxresdefault (1)

Gravitating Objects

Note

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 (Gravity in Time space - pdf)

A-lot-number-of-positive-color-charges-move-from-the-positive-charged-particle-toward-the

  Fermion  | spinors | charged | neutrinos |   quark   | components | parameter
   Field   |   (s)   |   (c)   |    (n)    | (q=s.c.n) |  Ξ£(c+n+q   | (complex)
===========+=========+=========+===========+===========+============+===========
bispinor-1 |    2    |    3    |     3     |    18     |     24     |   19
-----------+---------+---------+-----------+-----------+------------+-- 17
bispinor-2 |    2    |    3    |     3     |    18     |     24     |   i12 πŸ‘ˆ
===========+=========+=========+===========+===========+============+===========
bispinor-3 |    2    |    3    |     3     |    18     |     24     |   11
-----------+---------+---------+-----------+-----------+------------+-- 19
bispinor-4 |    2    |    3    |     3     |    18     |     24     |   i18
===========+=========+=========+===========+===========+============+===========
  SubTotal |    8    |   12    |    12     |    72     |     96     |   66+i30
Note

Think of it this way, all gravitating bodies in the universe would be surrounded at all times by a cloud of tunneling electrons. We cannot see these particles since they’re so small and since they permeate all of space. They would also tunnel to a different location about once every Planck time (about 10^-43 seconds) whenever they interact with another particle.

  • These interactions between particles amount to the exchanges of bosons between electrons and other electrons or other fermions. At each point where the electron absorbs another boson, we say that the wave function of the electron collapses, and it tunnels to a new location whereupon it interacts with yet another particle.
  • The cloud of electron surrounding gravitating objects would diminish in inverse proportion to the square of the distance; hence, if you recede from an objects’ surface, you’re less likely to find an electron tunneling from that object.
  • Electrons also make an excellent candidate for a particle of gravity since they absorb and emit photons readily, and we know from Einstein’s theory of general relativity that light interacts readily with gravitational fields, and that gravitational fields are thought to emit photons spontaneously.
  • This spontaneous emission of photons is what we refer to as the cosmological constant or dark energy, and in our current thinking on the topic we imagine that particles of antimatter are created and annihilate with particles of matter leading, occasionally, to the emission of a photon. I suspect that this is incorrect and that no such thing as antimatter really exists. I suspect that positrons are really tunneling W particles and that this Dirac Sea, or background of tunneling electrons, is really giving rise to this phenomenon of the cosmological constant, or vacuum energy, we observe inn nature.
  • As a consequence, we would need to adumbrate our standard model of particle physics by about half. This ought to be seen as a positive thing in physics. No longer do we have untestable assumptions (such as the creation and annihilation of particles) in our models, and we have a far easier means of now beginning to probe the quantum nature of gravity.

The other fascinating consequence of this way of thinking is that gravity would no longer be a fundamental force; instead it would be a secondary effect of electromagnetism. This should have been what we anticipated all along; and now, we might have a quantum theory focusing on only three forces and a theory of gravitation that is truly particle-based. (Medium - Article)

Cut the Standard Model

Note

We may gain a better understanding of black hole physics; wewe may gain the insight that tunneling electrons enter the event horizons of black holes, absorb a particle there, and tunnel out again to deposit it into the background. In this way, we could explain how black holes radiate away. (Medium - Article)

$True Prime Pairs:
(5,7), (11,13), (17,19)

     |    168    |    618    |
-----+-----+-----+-----+-----+                                             ---
 19Β¨ |  3Β¨ |  4Β¨ |  6Β¨ |  6Β¨ | 4Β€  ----->  assigned to "id:30"             19Β¨
-----+-----+-----+-----+-----+                                             ---
 17Β¨ | {5Β¨}| {3Β¨}|  2Β¨ |  7Β¨ | 4Β€  ----->  assigned to "id:31"              |
     +-----+-----+-----+-----+                                              |
{12Β¨}|  6Β¨ |  6Β¨ |  2Β€ (M & F)  βœ”οΈ ----->  assigned to "id:32"              |
     +-----+-----+-----+                                                    |
 11Β¨ |  .. |  .. |  .. | 3Β€ ---->  Np(33)  assigned to "id:33"  ----->  πŸ‘‰ 77Β¨
-----+-----+-----+-----+-----+                                              |
 19Β¨ |  .. |  .. |  .. |  .. | 4Β€  ----->  assigned to "id:34"              |
     +-----+-----+-----+-----+                                              |
{18Β¨}|  .. |  .. |  .. | 3Β€        ----->  assigned to "id:35"              |
     +-----+-----+-----+-----+-----+-----+-----+-----+-----+               ---
 43Β¨ |  .. |  .. |  .. |  .. |  .. |  .. |  .. |  .. |  .. | 9Β€ (C1 & C2)  43Β¨
-----+-----+-----+-----+-----+-----+-----+-----+-----+-----+               ---
139Β¨ |  1     2     3  |  4     5     6  |  7     8     9  |
                    Ξ”                 Ξ”                 Ξ”
Note

There are two groups of scientists (called collaborations) looking for evidence of gravitons in proton-proton collision experiments at the Large Hadron Collider at CERN. Once a graviton has been created, it’s expected to decay in one of a few possible ways - and it’s evidence of these decays that the collaborations are looking for. ATLAS search for evidence that the gravitons decays into two photons, and the CMS search for evidence that the graviton decays into two jets (bursts) of hadrons (a particular class of particle). (ThingsWeDontKnow.com)

fully-expanded-incl-matrices

Constructing the tableaux

Young_tableaux_1

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.

Screenshotgoogle

  Fermion  | spinors | charged | neutrinos |   quark   | components | parameter
   Field   |   (s)   |   (c)   |    (n)    | (q=s.c.n) |  Ξ£(c+n+q   | (complex)
===========+=========+=========+===========+===========+============+===========
bispinor-1 |    2    |    3    |     3     |    18     |     24     |   19
-----------+---------+---------+-----------+-----------+------------+-- 17
bispinor-2 |    2    |    3    |     3     |    18     |     24     |   i12 πŸ‘ˆ
===========+=========+=========+===========+===========+============+===========
bispinor-3 |    2    |    3    |     3     |    18     |     24     |   11
-----------+---------+---------+-----------+-----------+------------+-- 19
bispinor-4 |    2    |    3    |     3     |    18     |     24     |   i18
===========+=========+=========+===========+===========+============+===========
  SubTotal |    8    |   12    |    12     |    72     |     96     |   66+i30
===========+=========+=========+===========+===========+============+===========
majorana-1 |   2x2   |    -    |    18     |     -     |     18     |   18
-----------+---------+---------+-----------+-----------+------------+-----------
majorana-2 |   2x2   |    -    |    12     |     -     |     12     |   12 πŸ‘ˆ
-----------+---------+---------+-----------+-----------+------------+-----------
majorana-3 |   2x2   |    -    |    13     |     -     |     13     |   i13
===========+=========+=========+===========+===========+============+===========
  SubTotal |    12   |    -    |    43     |     -     |     43     |  30+i13
===========+=========+=========+===========+===========+============+===========
     Total |    20   |   12    |    55     |    72     |    139     |  96+i43 πŸ‘ˆ

PRI_196247467

Despite the popularity of dark matter and dark energy as an explanation of various empirical observations in physics, there remains no direct evidence of either.

Pairwise Scenario

The subclasses of partitions systemically develops characters similar to the distribution of prime numbers.

Tip

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.

Renormalization

This is managed within twelve (12) flows (A: to W:). Each flows is representing a certain period which is converting the three (3) layers of 19 cells with a cumulative sum of 1, 7 and 19 in sequence as explained before.

Quantum Chromodynamics

As we’ve already suggested, the number 30 figures large in our modulo 30 domain. The Prime Spiral Sieve is Archimedean in that the separation distance between turns equals 30, ad infinitum. The first two rotations increment as follows:

1-s2 0-S0550321321002340-gr008_lrg

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.

Subclasses of Partitions

image

(10 - 2) th prime = 8th prime = 19

default

The subclasses of partitions systemically develops characters similar to the distribution of prime Numbers represents the number of possible partitions of a non-negative integer n.

Rank of a partition

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 β—„--- #29 β—„--- #61
3 2 0 1 0 2 πŸ‘‰ 2
4 3 1 1 0 3 πŸ‘‰ 89 -29 = 61 - 1 = 60 βœ”οΈ
5 5 2 1 0 5 πŸ‘‰ f(37) = f(8 twins) βœ”οΈ
6 7 3 1 0 7 β—„--- #23
7 11 4 1 0 11 β—„--- #19
8 13 5 1 0 13 β—„--- # 17 β—„--- #49
9 17 0 1 1 17 β—„--- 7th prime πŸ‘‰ 7s
10 19 1 1 1 βˆ†1 β—„--- 0th βˆ†prime β—„--- Fibonacci Index #18
-----
11 23 2 1 1 βˆ†2 β—„--- 1st βˆ†prime β—„--- Fibonacci Index #19 β—„--- #43
..
..
40 163 5 1 0 βˆ†31 β—„- 11th βˆ†prime β—„-- Fibonacci Index #29 πŸ‘‰ 11
-----
41 167 0 1 1 βˆ†0
42 173 0 -1 1 βˆ†1
43 179 0 1 1 βˆ†2 β—„--- βˆ†βˆ†1
44 181 1 1 1 βˆ†3 β—„--- βˆ†βˆ†2 β—„--- 1st βˆ†βˆ†prime β—„--- Fibonacci Index #30
..
..
100 521 0 -1 2 βˆ†59 β—„--- βˆ†βˆ†17 β—„--- 7th βˆ†βˆ†prime β—„--- Fibonacci Index #36  πŸ‘‰ 7s
-----

7 + 13 + 19 + 25 = 64 = 8 Γ— 8 = 8Β²

Note

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.

A_BSSS_Algorithm_for_the_Location_Problem_with_Min.pdf

Integers can be considered either in themselves or as solutions to equations (Diophantine geometry).

Note

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(8πŸͺŸ8) = 1 + 7 + 29 = 37 inner partitions

p r i m e s
1 0 0 0 0 0
2 1 0 0 0 1 β—„--- #29 β—„--- #61
3 2 0 1 0 2 πŸ‘‰ 2
4 3 1 1 0 3 πŸ‘‰ 89 -29 = 61 - 1 = 60
5 5 2 1 0 5 πŸ‘‰ f(37) = f(8πŸͺŸ8) βœ”οΈ
6 7 3 1 0 7 β—„--- #23
7 11 4 1 0 11 β—„--- #19
8 13 5 1 0 13 β—„--- # 17 β—„--- #49
9 17 0 1 1 17 β—„--- 7th prime πŸ‘‰ 7s
10 19 1 1 1 βˆ†1 β—„--- 0th βˆ†prime β—„--- Fibonacci Index #18
-----
11 23 2 1 1 βˆ†2 β—„--- 1st βˆ†prime β—„--- Fibonacci Index #19 β—„--- #43
..
..
40 163 5 1 0 βˆ†31 β—„- 11th βˆ†prime β—„-- Fibonacci Index #29 πŸ‘‰ 11
-----
41 167 0 1 1 βˆ†0
42 173 0 -1 1 βˆ†1
43 179 0 1 1 βˆ†2 β—„--- βˆ†βˆ†1
44 181 1 1 1 βˆ†3 β—„--- βˆ†βˆ†2 β—„--- 1st βˆ†βˆ†prime β—„--- Fibonacci Index #30
..
..
100 521 0 -1 2 βˆ†59 β—„--- βˆ†βˆ†17 β—„--- 7th βˆ†βˆ†prime β—„--- Fibonacci Index #36  πŸ‘‰ 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 .

Note

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).

Partitioned-matrices-of-the-numbers-60-62-and-64-as-examples

Note

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 (βˆ’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 β—„--- #29 β—„--- #61
3 2 0 1 0 2 πŸ‘‰ 2
4 3 1 1 0 3 πŸ‘‰ 89 -29 = 61 - 1 = 60
5 5 2 1 0 5 πŸ‘‰ f(37) = f(29πŸͺŸ23) βœ”οΈ
6 7 3 1 0 7 β—„--- #23
7 11 4 1 0 11 β—„--- #19
8 13 5 1 0 13 β—„--- # 17 β—„--- #49
9 17 0 1 1 17 β—„--- 7th prime πŸ‘‰ 7s
10 19 1 1 1 βˆ†1 β—„--- 0th βˆ†prime β—„--- Fibonacci Index #18
-----
11 23 2 1 1 βˆ†2 β—„--- 1st βˆ†prime β—„--- Fibonacci Index #19 β—„--- #43
..
..
40 163 5 1 0 βˆ†31 β—„- 11th βˆ†prime β—„-- Fibonacci Index #29 πŸ‘‰ 11
-----
41 167 0 1 1 βˆ†0
42 173 0 -1 1 βˆ†1
43 179 0 1 1 βˆ†2 β—„--- βˆ†βˆ†1
44 181 1 1 1 βˆ†3 β—„--- βˆ†βˆ†2 β—„--- 1st βˆ†βˆ†prime β—„--- Fibonacci Index #30
..
..
100 521 0 -1 2 βˆ†59 β—„--- βˆ†βˆ†17 β—„--- 7th βˆ†βˆ†prime β—„--- Fibonacci Index #36  πŸ‘‰ 7s
-----

The code is interspersed with python, shell, perl, also demonstrates how multiple languages can be integrated seamlessly.

extended branes

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 β—„--- #29 β—„--- #61
3 2 0 1 0 2 πŸ‘‰ 2
4 3 1 1 0 3 πŸ‘‰ 89 - 29 = 61 - 1 = 60
5 5 2 1 0 5 πŸ‘‰ f(37) = ❓ πŸ‘ˆ Composite βœ”οΈ
6 7 3 1 0 7 β—„--- #23
7 11 4 1 0 11 β—„--- #19
8 13 5 1 0 13 β—„--- # 17 β—„--- #49
9 17 0 1 1 17 β—„--- 7th prime πŸ‘‰ 7s πŸ‘ˆ Composite βœ”οΈ
10 19 1 1 1 βˆ†1 β—„--- 0th βˆ†prime β—„--- Fibonacci Index #18
-----
11 23 2 1 1 βˆ†2 β—„--- 1st βˆ†prime β—„--- Fibonacci Index #19 β—„--- #43
..
..
40 163 5 1 0 βˆ†31 β—„- 11th βˆ†prime β—„-- Fibonacci Index #29 πŸ‘‰ 11
-----
41 167 0 1 1 βˆ†0
42 173 0 -1 1 βˆ†1
43 179 0 1 1 βˆ†2 β—„--- βˆ†βˆ†1
44 181 1 1 1 βˆ†3 β—„--- βˆ†βˆ†2 β—„--- 1st βˆ†βˆ†prime β—„--- Fibonacci Index #30
..
..
100 521 0 -1 2 βˆ†59 β—„--- βˆ†βˆ†17 β—„--- 7th βˆ†βˆ†prime β—„--- Fibonacci Index #36  πŸ‘‰ 7s
-----

This behaviour in a fundamental causal relation to the primes when the products are entered into the partitions system.

Composite behaviour

The-Standard-Model-of-particle-physics-with-Higgs-boson-at-the-center-includes-fractional ppm

It would mean that there should be some undiscovered things hidden within the residual of the decimal values.

integer partition

168 + 2 = 170 = (10+30)+60+70 = 40+60+70 = 40 + 60 + βˆ†(2~71)

p r i m e s
1 0 0 0 0 0
2 1 0 0 0 1 β—„--- #29 β—„--- #61
3 2 0 1 0 2 πŸ‘‰ 2
4 3 1 1 0 3 πŸ‘‰ 89 - 29 = 61 - 1 = 60
5 5 2 1 0 5 πŸ‘‰ f(37) βœ”οΈ
          6 πŸ‘‰ 11s Composite Partition βœ”οΈ
6 7 3 1 0 7 β—„--- #23
7 11 4 1 0 11 β—„--- #19
8 13 5 1 0 13 β—„--- # 17 β—„--- #49
9 17 0 1 1 17 β—„--- 7th prime
           18 πŸ‘‰ 7s Composite Partition βœ”οΈ
10 19 1 1 1 βˆ†1 β—„--- 0th βˆ†prime β—„--- Fibonacci Index #18
-----
11 23 2 1 1 βˆ†2 β—„--- 1st βˆ†prime β—„--- Fibonacci Index #19 β—„--- #43
..
..
40 163 5 1 0 βˆ†31 β—„- 11th βˆ†prime β—„-- Fibonacci Index #29 πŸ‘‰ 11
-----
41 167 0 1 1 βˆ†0
42 173 0 -1 1 βˆ†1
43 179 0 1 1 βˆ†2 β—„--- βˆ†βˆ†1
44 181 1 1 1 βˆ†3 β—„--- βˆ†βˆ†2 β—„--- 1st βˆ†βˆ†prime β—„--- Fibonacci Index #30
..
..
100 521 0 -1 2 βˆ†59 β—„--- βˆ†βˆ†17 β—„--- 7th βˆ†βˆ†prime β—„--- Fibonacci Index #36  πŸ‘‰ 7s
-----
Note

The initial concept of this work was the Partitioned Matrix of an even number wβ‰₯ 4:

  • It was shown that for every even number wβ‰₯ 4 it is possible to establish a corresponding Partitioned Matrix with a determined number of lines.
  • It was demonstrated that, fundamentally, the sum of the partitions is equal to the number of lines in the matrix: Lw = Cw + Gw + Mw.
  • It was also shown that for each and every Partitioned Matrix of an even number w β‰₯ 4 it is observed that Gw = Ο€(w) βˆ’ (Lw βˆ’ Cw), which means that the number of Goldbach partitions or partitions of prime numbers of an even number w β‰₯ 4 is given by the number of prime numbers up to w minus the number of available lines (Lwd) calculated as follows: Lwd = Lw βˆ’ Cw.

To analyze the adequacy of the proposed formulas, probabilistically calculated reference values were adopted. (Partitions of even numbers - pdf)

Batch Jacobian

p r i m e s
1 0 0 0 0 0
2 1 0 0 0 1 β—„--- #29 β—„--- #61
3 2 0 1 0 2 πŸ‘‰ 2
4 3 1 1 0 3 πŸ‘‰ 89 - 29 = 61 - 1 = 60
5 5 2 1 0 5 πŸ‘‰ 11 + 29 = 37 + 3 = 40 βœ”οΈ
          6 πŸ‘‰ 11s Composite Partition β—„--- 2+60+40 = 102 βœ”οΈ
6 7 3 1 0 7 β—„--- #23
7 11 4 1 0 11 β—„--- #19
8 13 5 1 0 13 β—„--- # 17 β—„--- #49
9 17 0 1 1 17 β—„--- 7th prime 
           18 πŸ‘‰ 7s Composite Partition 
10 19 1 1 1 βˆ†1 β—„--- 0th βˆ†prime β—„--- Fibonacci Index #18
-----
11 23 2 1 1 βˆ†2 β—„--- 1st βˆ†prime β—„--- Fibonacci Index #19 β—„--- #43
..
..
40 163 5 1 0 βˆ†31 β—„- 11th βˆ†prime β—„-- Fibonacci Index #29 πŸ‘‰ 11
-----
41 167 0 1 1 βˆ†0
42 173 0 -1 1 βˆ†1
43 179 0 1 1 βˆ†2 β—„--- βˆ†βˆ†1
44 181 1 1 1 βˆ†3 β—„--- βˆ†βˆ†2 β—„--- 1st βˆ†βˆ†prime β—„--- Fibonacci Index #30
..
..
100 521 0 -1 2 βˆ†59 β—„--- βˆ†βˆ†17 β—„--- 7th βˆ†βˆ†prime β—„--- Fibonacci Index #36  πŸ‘‰ 7s
-----

(11x7) + (29+11) + (25+6) + (11+7) + 4 = 77+40+31+18+4 = 170

16S rRNA amplicons study