Quantum Noise Floor, Quantified

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Matinga’s Quantum Dependency - Noise Floor Function

All events and systems in physics and in any form of communication must contain some a priori - earlier information shared between communicating portions of the system. This means any detection (absorbing/reading) of any signal or energy transfer is only possible if the fundamental, unscaled or unamplified energy element is in both emitting/writing portions.

This means the quantum randomness must be re-designated the term quantum pseudo randomness or pseudo-noise. It must be a complex set of relations or active identities in the form of individual, discrete oscillations or standing waves which add up to a noisy standing wave with an extended period - yet a fixed period regardless. This indicates there is almost certainly quantum structure, rather than random 'noise' - or lack of information.

If you plot two sine waves, summed in Desmos.com, Graphing Calculator, you find that the irregular wave has a resting shape or pattern. Use waves which are only harmonics of each other and you will witness it sooner with less 'squinting' and uncertainty.

The principle multiplies out to every wave if you add them arithmetically and if you multiply that set of waves by a scalar or harmonic. The set of waves form one ‘prohibitively difficult’ to ‘decipher’ waveform without the original variables.

They add up to one singular function regardless. By definition, any function capable of being reduced to one mathematical function is an example of similarity to material, Bose-Einstein condensate. It is the exclusive, Matinga Quantum Dependency.

The greatest number of discrete wavelengths which I have read in articles on the worldwide web has been 4,294,967,296. This number is also consistent with 32 bit or 2^32. The number of wavelengths , less 1, is consistent with the Maximum number of wavelengths in analogue electronics.

An algorithm is shown below to synthesise the current understanding of quantum noise floor:

To constrain noise floor variables to within a pre-allotted array limit, use the Limiting Function method. Substitute the limit as c, and the noise floor variables, collectively as x.

Quantum Noise Floor

A [ 1 ] = Sin ( 2 rad * Pi rad * x / n ) - ( ( ( Sin ( 2 rad * Pi rad * x / n ) + x ) -x ) x ), ++ x

A = Sin^2 ( Pi * x ), 1st harmonic of Sin ^ ( Pi * x [ i ] )

A = Sin ^ 2 ( Pi * A [ 1 ] )

The algorithm will produce a series of discrete oscillations between 0 and 1 which will repeat until they reach an amplification of 2^32. To make use of noise floor, amplify, in natural number amplification increments, past amplification of 'a = 1'.

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