Course 3 on Lorentz-Four-Contractions, Session 14, Part 1

The appearance of stringular contraction is in the globally distinguishable. You may wonder, "What does he mean by detecting a string within a neighborhood as it is iterating and reiterating several times?" Since a string is a small phenomenon that is of itself a vibration of several point particles that comprise its make-up, then, as a string defines its position as what it is for just a moment, it is iterated. Change is constant. The strings existence as a string in a specific position as being exactly what it was during the metric of pointal organization that allows it to be that is basically no longer than the instantaneous organizational moment that it takes for the points to become "exact" and "linear" when considering the basis of a 1-D string or a vibrating strand, form an instanton-quaternionic-field-impulse range right before this iteration, and then dissociate after this iteration. So stringular organization is only a transient thing when considering ultimon flow. Yet, if you detected a "string" at any spot, it would show a sense of stability in terms of empirical reality, even though it would indicate a condition of vibration. How? When a string in the globally distinguishable appears to be basically vibrating as a still phenomenon, then the substringular action indicates motion of the string that keeps coming back to basically the same spot if in a state of superconformal invariance. Since the string keeps approximating the same position here after it keeps returning after circling the Continuum each time, it appears to be basically changeless in terms of Cartesian displacement as a unit. The condition in the lateral displacement of the string as a unit is the condition of a phenomenon that does not differentiate kinematically as a unit in the globally distinguishable. I will appease the suspense of my readers by providing more knowledge of this session later.

Notes for FTAAN

A swivel configuration appertaining to a one-dimensional superstring may be supplementally norm to the norm to holomorphic direction, or a swivel configuration appertaining to a one-dimensional superstring may be in the holomorphic direction.

A swivel configuration appertaining to a two-dimensional superstring may be supplementally norm to the norm to holomorphic direction in the general directoralization of the associated superstring's topology, or a swivel configuration appertaining to a two-dimensional superstring may be in the holomorphic direction.

Swivel configurations of a vibrating strand ( one-dimensional superstring, or of a vibrating hoop (two-dimensional superstring) do not necessarily intrinsically take away metric-gauge from a superstring in and of themself. Metric-Gauge is taken away as a decrement in a superstring's extra supply of potential permittivity by the Fourier successive utilization of the given superstring over a sequential series of iterations that define a group metric.

The difference between a swivel configuration as I have described, and a mini-loop that is a form of metric-gauge is that a mini-loop is tightly knit in a manner that makes the whole given superstring completely hermitian unless the said superstring is perturbated by a swivel configuration that has one or more Chern Simmons cusps. Such Chern Simmons cusps bear a non-discrete limit covariance relative to the topology that exists Wardwise on either sides of the cusps described.