Reading the opening post of a software question

https://www.researchgate.net/post/Hasnt_software_engineering_been_relying_on_an_untested_hypothesis_of_computer_science_by_mistakenly_assuming_the_hypothesis_to_be_a_fact

encouraged me to publish the following about Quantism.

FOUR EXAMPLES OF ENTANGLEMENT

1.- SPATIUM ENTANGLEMENT

Consider the standard elementary geometrization of "absolute" three dimensional physical space. In this context instead of "point in physical space" we will say "spatium state".

For a given space coordinate system with XYZ axis, spatium state S corresponds with a point P in geometric XYZ space, that is, S corresponds with a triple of numbers in \R^3. Point P projects over coordinate points Px, Py, Pz, each belonging one of the coordinate axis, hence

P = Px + Py + Pz

If furthermore Px=\alpha Ux, Py=\beta Uy, Pz=\gamma Uz with Ux, Uy, Uz unit vectors we have that P is the following linear combination

P=\alpha Ux + \beta Uy + \gamma Uz

But each of the normalized vectors Ux, Uy, Uz corresponds with some spatium state, say Sx, Sy, Sz. Therefore the Cartesian, traditional, high school decomposition according to coordinate axis becomes the following postmodern phrase:

** Spatium state S is a spatium entanglement of Sx, Sy, Sz **

The spatium physical state S is therefore the spatium physical superposition of the normalized spatium physical states Sx, Sy, Sz.

Can I pretend this is a new, mysterious physical property of space?

2.- SPATIUM-TEMPUS ENTANGLEMENT

Add now a clock and a numerical time dimension T. Consider a space-time physical event S and call it a "spatium-tempus state" with corresponding space-time four-vector P decomposable as

Px=\alpha Ux, Py=\beta Uy, Pz=\gamma Uz, Pt=\delta Ut

where Ux, Uy, Uz, Ut have been normalized. These correspond with spatium-tempus states Sx, Sy, Sz, St. We can now say

** Spatium-tempus physical state S is the spatium-tempus physical entanglement of spatium-tempus physical states Sx, Sy, Sz, St **

Does someone disagrees that this is deep Physics?

3.- MULTIPLEX ENTANGLEMENT

Suppose a physical system consists of physical states S described by means of points of an n-dimensional differentiable manifold M^n. This means that each S corresponds with a P of M^n. In this situation instead of "physical state" we will say "multiplex state". I did check the dictionary. Latin translation of "manifold" is "multiplex".

Let the open subset V of M^n be such that it contains point P corresponding to physical multiplex state S, and assume additionally that V is the domain of a coordinate chart

f:V\to \R^n

By hypothesis, there is a point p in \R^n such that f(P)=p. Let e_1, ... , e_n be the canonical basis of \R^n. Things will now advance towards esoteric virtuality since, generally speaking, f(V) need not be all of \R^n.

Being a vector in \R^n element p can be written as

p=p_1 e_1 + ... + p_n e_n

If there are multiplex physical states S_1, ... , S_n such that f(S_j)=e_j it will be said that e_j determines the "real" multiplex physical state S_j. Otherwise e_j determines a "virtual" multiplex physical state that need not be specified. Never mind what these virtual physical states could really be. They are often invoked by reputable writers. Whether states are real or virtual, it can now be said that

** Multiplex physical state S is the multiplex entanglement of S_1, ... , S_n **

It should be possible to refine this example to include Lagrangian and Hamiltonian systems.

How much physical insight does this provides?

4.- QUANTUM ENTANGLEMENT

Consider quantum states S corresponding with normalized wave functions. Let \psi be a normalized finite linear combination of normalized quantum eigenfunction \psi_j of some self-adjoint qunatum mechanical operator H

\psi = \mu_1 \psi_1 + ... + \mu_n \psi_n

If S_j are the quantum physical states corresponding to the the eigenfunctions \psi_j we can say that

** Quantum state S is an entanglement of quantum stationary states S_1, ... , S_n **

It must be remarked that in practice the operator H does not have to be explicitly given, nor its eigenvalues and eigenfunctions have to be calculated.

Quantum entanglement does not seem much more than the entanglements above.

5.- CONCLUSION

Examples 1, 2, 3 are entanglements formulated in the context of classical Physics. Example 4 is quantum entanglement.

Is "quantum entanglement" a substantial physical concept? Or is just traditional "linear combination"?

Cordially,

Daniel Crespin

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