Orbifold Couplings, A Little Start

When two orbifolds that are initially from two different universes are brought -- via an initial dual symmetrical Lagrangian of approach -- into a virtually Gliossi contact, then, these adjacent orbifolds that were initially from two different universes will often synchrounize their vibrations in so that these will then be of the same universe as each other.  This will, to an extent, depend upon both the binary dual directoral paths that are here to interact & the covariance of both the parity and chirality genus formats of the Hamiltonian operations of both orbifolds -- as these approach each other in a Yakawa manner that is here not Gliossi.  So, as such orbifolds come into an "apprehension" of each other, these slow down in a Reverse-Dirac-based manner as these become relatively near each other.  This given arbitrary tendency to slow is based, in part, upon the covariant, codeterminable, codifferentiable genus and amplitude of the respective Hamiltonian operation that works to describe the substringular momentum of the two approaching orbifolds & the Hodge Index of such an operation. The Njenhuis-based tensors of such  transversal and spin-orbital Hamiltonian dual operators that have just moved through the eluded to Hamiltonian dual operands will then, upon the synchrounization of their Gaussian Formats, become Real Reimmanian-based tensors.  Often, once such determined orbifolds have here become of Real-based spaces relative to one another, these will then enter a state of conformal invariance that tends to at least transiently be activated into a Noether-based mode.  To be continued.  Sam.