Orientations Between Orbifolds and Orbifold eigensets

An orbifold is a set of one or more superstrings that work together in such a manner in so as to operate as a specific function.  An orbifold eigenset is a set of one or more orbifolds that work together in such a manner in so as to operate as a specific function.  Each orbifold of an orbifold eigenset that is comprised of more than one orbifold has a slightly different part to play in the overall operation of the here stated given arbitrary orbifold eigenset.  Let us here consider two different orbifold eigensets that would represent two different spaces that functioned in so as to perform two different operations.  The first of such orbifold eigensets in this given arbitrary case will here consist of one orbifold only.  The second of such orbifold eigensets in the same said case scenario will here consist of many orbifold eigensets.  Both of the mentioned orbifold eigensets is formatted in such a manner in so as to be Real Reimmanian in terms of their Gaussian characteristics.  So, both of the said two orbifold eigensets can then be solved into a Gaussian format that is not complex in terms of their determinant genus.  The first respective orbifold eigenset will here contain fewer superstrings than the second mentioned respective orbifold eigenset.  So, the translation of the differential geometry of the spatial inter-relation of the first said orbifold eigenset would tend to here be easier to format into Gaussian form than the translation of the differential geometry of the spatial inter-relation of the second said orbifold eigenset.  In order to compare the Hamiltonian operations of the two mentioned given arbitrary orbifold eigensets, one must take a Jacobian eigenbasis that will here translate the patterning of the first mentioned orbifold eigenset to the second mentioned orbifold eigenset.  Now, take the two orbifolds over time.  Both of the said orbifold eigensets here will be moved through a Lagrangian that will here involve a majorization of codifferentiable, codeterminable, and covariant special re-delineation through time as the two mentioned different physically-based spaces kinematically move through a binary Hilbert-based spatial operand that is here fixed when one is considering the hermitian and non-spurious nature of the trajectory of the projection of the two correlatively moving physically moving spaces that move at a steady-state-based Hamiltonian-based pulse that is Yau-Exact -- while yet constant in terms of the genus of the directoral-based flow of the said kinematic flow of the two eluded to orbifold eigensets.  Let us now say, in this case, that the two spaces form two binary paths that move away from each other over time in a hyperbolic manner that is smooth in trajectoral path per iteration of group instanton.  Then, the longer that the motion of the two said eigensets continues to be performed over time, the less direct influence that these two orbifolds have upon each other.  Such a non-Chern-Simmons-based flow that is constant in acceleration over time is an example of a Dirac operational index that bears a certain degree of Clifford Expansion that is maintained until it is perturbated by an outside force.
I will continue with the suspense later!  Sincerely, Samuel David Roach.