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which should not be confused with the physical observation of a recti- linear trajectory that applies only to a given scale. In fact, this tangential propagation takes place on a horizon smaller than the observation scale. The internal horizons, which he called “temporal openings,” are defined 1 aod soa by stroboscopic observations. Due to our perceptive inability, each non-observation interval is in itself a stroboscopic series of observations/non-observations. My next figure is inspired by J. P. Garnier Malet’s theory. The particles are defined by their speed of motion in a given horizon. They seem to be at rest while they go through a “temporal opening,” whereas the par- ticles are really part of a horizon where time flows more quickly. Nev- ertheless, the arguments proposed by this physicist fit in with a strictly dynamic vision of bodies. He did not mention the states of res- onance or intricateness. However, he did point out that the fundamen- tal doubling motion applies to both quantum mechanics and relativist mechanics in cosmology. I think the following sibylline sentence is essential: the propagation of a particle is just an appearance in a given horizon. It is important to understand that all mechanics is due for an overhaul. Just like Lehto, one of the very first who brought up the doubling principle, Garnier Malet specified that the durations of the temporal openings are connected to the periodicity of a particle. He even went one step further by presenting the notion of a spinback, which consists in a triple rotation of the particle or of horizon Q). A spinback can be radial or tangential, the first being an anticipation of the other. Ladvise experts to visit this physicist’s website” for a detailed study of the formalism used and to learn more about his description of the a4 seven juxtaposed horizons. In his theorem of the three horizons of doubling, he argued that a doubling transformation requires three particles (internal, intermedi- ate, external) embedded into seven stroboscopic times. Iam sure the following crucial element will pique your interest. Gar- nier Malet defined the maximum radial velocity of the horizon/internal particle Q, during doubling as follows: “During time Tt of 4x54 = 216 spinbacks (mp) of particle Q,, the motion of this particle accelerates from 1 to 10°, whereas horizon Q, accelerates from | to 10°.... The application of the doubling theory to the solar system has thus enabled the theoret- ical ‘calculation’ of the following velocity in kilometers/second: C = (216mp/t) 10* = 54n”? (nR,/4t) 10° = 299 796 km./sec.