A Little Bit As To Why Certain Spaces Interact

When two different unique orbifolds that are of the same universe interact with each other over a given arbitrary Fourier Transformation in a viable manner, these given arbitrary orbifolds that work to here describe two different unique spaces of physical phenomena bear adjacent Planck-related phenomena -- that work to help comprise the physical composition of the said respective orbifolds -- that are orphoganal when relative to one another when one is to map the individual distributions of the said Fadeev-Popov-Traces at their delineations over a successive series of group instantons.  This orphoganal relative placement of covariant codeterminiable codifferentiable delineation works to allow for the vibratorial oscillations that are emitted from the said Traces to be orphoganal with a relativistic wobble of ~1.104735878*10(-81)I degrees.  Since all touch is related to a 90 degree correlation, spaces that are Real relative to one another always tend to have adjacent Planck-related phenomena that are norm when such corresponding Traces are mapped-out relative to one another in order for such spaces to codifferentiate with one another in any viable manner that bears a direct correspondence of the one space or orbifold when relative to the other respective space or orbifold.  So, the condition of relative norm-conditions is what works to draw in and to draw away physical spaces that are Real when in correlation to one another, in order that the conditions and the activities of Gaussian Transformations are o be able to act as an operation that allows for the continual kinematic redelineation of the substringular to be both spontaneous and perpetual.  This is why it takes Real Reimmanian Hamiltonian-based operators, operations, and operands in order to allow for the direct interplay of superstringular phenomena to codifferentiate when the corresponding spaces -- that act as orbifold-based phenomena -- are bearing delineatory orphoganation that works to allow such covariant spaces to be of the same universe.  Thus, it takes Njenhuis Hamiltonian-based operators, operations, and operands in order to allow for the direct interplay of superstringular phenomena to codifferntiate when the corresponding spaces -- that act as orbifold-based phenomenea -- are bearing delineatory orphoganation that works to allow such covariant spaces to be of different universes that here imbue a relatively rare correspondence.  So, if two spaces that were initially of different universes become assimilated in a directly viable manner in which there is a significant Yakawa Coupling Hamiltonian basis of codeterminable functionability, then, such spaces or orbifolds will then more than likely be at least temporarily of the same universe over the course of at least a transient Fourier Transform.