Lorentz-Four-Contractions and Orbifolds

If a given arbitrary physical phenomenon moves through either a binary or a tritiary-based Lagrangian, in the process of traveling at such a velocity to where the said physical phenomena bears a Lorentz-Four-Contraction of two for either the two spatial dimensions that are appertaining to that eluded to motion that is going through a binary Lagrangian, or, for those three spatial dimensions that are appertaining to that eluded to motion that is going through a tritiary Lagrangian, then, these two or three respective given arbitrary spatial dimensions will be the ones, of the said physical phenomenon that has here been eluded to as moving as such, that will be contracted to the scalar amplitude of two in both respective given arbitrary cases.  This is given the conditions of this bilateral given arbitrary set of cases, in which the eluded to formats of physical scenario involve one or more additional spatial dimensions than those that are here moving, in each respective case, in such a manner in so that all of those spatial dimensions that are here directly involved with the directoral pull of each individual case of the kinematic flow of the two so-stated Lagrangian spatial delineations over time will thence be contracted to the same degree of scalar amplitude.  This is because the velocity of each of the spatial dimensions that are directly associated with each of the eluded to kinematic flow geni in both respective cases are moving at the same eluded to velocity -- to where the Lorentz-Four-Contractions of each of the just eluded to parametric-based spatial dimensions that are contracted are thus contracted to a scalar factor of two.  Such a general format of motion would then here involve a typically hermitian-based format of spatial curvature -- over that duration that would here involve the Hamiltonian operation of the eluded to physical phenomenon that is moving through either a binary or in a tritiary-based basis of Lagrangian-based space, in which the said genus of both individual respective Hamiltonian operands that are crossed during the process of the transversal motion of the said physical phenomenon over time is moving in a curvature that changes in either the same number of spatial derivatives or less than the number of dimensions that it is moving in in an operand-based tense over a sequential series of instanton, to where the then here present existence of Chern-Simmons singularities is minimal -- these just mentioned geni of singularities would only exist here if there is a metrical spur in the kinematic-based harmonics of the motion of the eluded to general format of physical phenomena.  To Be Continued!  Sam Roach.