The Theory of Everything in one sentence, in matrix form, is based on the assumption of the existence of a square relaxation transition matrix Bnxn (n being the number of free nodes, not to be confused with the number of iterations or time steps N) for the time-dependent energy field U(x,y,z,t), in classical and quantum physics, such that:

U(x,y,z,t+dt)=B.U(x,y,z,t) + B^N . U(x,y,z,0) . . .(1)

We assert that no classical or quantum physics, or even any mathematics, can escape a derivation from Equation 1 or a subset of this equation.

Equation 1 leads to the existence of a transfer matrix D(N) such that:

U(x,y,z,t+ Ndt)=B.U(x,y,z,t) + B^N . U(x,y,z,0) . . .(2)

Which gives:

U(x,y,z,t)=D(N).(b+S) + B^N.IC . . . . . (3)

Where U(x,y,z,Ndt) is the classical and/or quantum energy density at the free point or node x,y,z and at time t = Ndt, where N is the time integer for the number of jumps or iterations woven in the Cartesian axes x,y,z and dt is the time interval or time jump.

Recall that we currently know of only two transition matrices: the well-known mathematical statistical Markov matrix and the proposed statistical transition matrix B.

Clearly, matrix B offers a significant improvement over the Markov matrix M because it takes into account the boundary condition vector b and the source term vector s, unlike the Markov matrix. b is the boundary condition vector, arranged in the appropriate order, and S is the appropriate source/sink term, in the appropriate units, placed at the main diagonal node Bii.

Clearly, D(N) is given by the finite sum of the matrix series, D(N)=B+B^2+B^3+ . . . . +B^N . . . . (4)

*It should be noted that equations 1, 2, 3, and 4 are not entirely new, but have been used effectively over the past four years to solve almost all types of scientific problems in closed volumes controlled by Dirichlet boundary conditions. These problems include:

i) the numerical solution of Laplace and Poisson PDEs;

ii) the numerical solution of the heat diffusion equation in the most general case;

iii) the numerical solution of time-dependent quantum mechanical problems in infinite free space under an arbitrary external potential

V, numerical differentiation and integration;

vi) the numerical derivation of stationary statistical distributions, such as Gaussian or normal distributions.

The five facts mentioned above lead to the following conclusion: Cairo intelligence techniques = natural intelligence = artificial intelligence in the strict sense = unified field theory.

The question arises:

if the Theory of Everything, or Unified Field Theory, known as the "Cairo Technique," works with exceptional success and has been known and published for over four years, why is it not generally accepted in the current scientific community?

The answer is simple and lies primarily in a flaw in the theory:

It reveals the fatal errors of Niels Bohr, E. Schrödinger, and A. Einstein, who dominated science for over a century.

This is why this theory does not appeal to the iron guardians of A. Einstein's relativity and the classical Schrödinger equation of 1927.

But who are the iron guardians of the classical Schrödinger equation as interpreted by Niels Bohr, Or more precisely, the iron guardians of Niels Bohr himself?

The phrase "iron guardians of the Schrödinger equation" refers to a group of physicists and mathematicians who ardently defend the equation and its classical interpretations, often resisting any attempt to modify or question it, sometimes going so far as to reject any perspective or alternative.

They are described as dogmatic in their adherence to the equation and its established interpretations, sometimes stimulating progress in quantum mechanics by rejecting new ideas or alternative approaches [Google search].

In other words, the iron guardians of the classical Schrödinger equation are those indoctrinated physicists and mathematicians who defend this incomplete and misleading equation until their last breath and who are, in reality, the iron guardians of the scientist Niels Bohr himself.

They know that sooner or later, Einstein's classical general relativity and that of Schrödinger, as interpreted by Bohr, will disappear and they will disappear with it.

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1-I. Abbas, Foundations of Quantum Mechanics and General Relativity -Theory and Practice

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