Change In Tense Of Slater-Related Propagation

Let us consider an orbifold eigenset, that is here to be moving via a Lagrangian-based path, that is of a euclidean nature, -- to where the here inferred propagation of this said orbifold eigenset, is here to be of a Slater-related nature.  This implies, that the propagation of the said eigenset -- is here to be in the process of being translated through space, via a mean Lagrangian-related Hamiltonian operand, -- to where such a said eigenset, may consequently be depicted of as a set of a discrete quanta of energy, -- that are here to be in the process of being transferred in a relatively "straight" manner, through some sort of a tense of an identity function, (F(y) = F(x)).  Furthermore; let's now say, that the ensuing nature of the motion of such a said orbifold eigenset, via its correlative Lagrangian-based path, is here to alter from its initial euclidean-related nature, -- to where even though the said orbifold eigenset is still to be propagated in a Slater-related manner, it is to instead to be of a Clifford-related nature.  Consequently; the said orbifold eigenset, is now to work to bear a hyperbolic translational flow of its spatial eigenindices, in the process of its spatial transference over time, -- to where, instead of the said respective eigenset to thence to be moving in a manner that may be depicted of as being translated in a relatively "straight" way, via some sort of an identity function, it is instead to be moving in a manner that may be depicted of as being translated in a relatively concave-up way, such as with (F(y) = F(x)^(a constant)).  Sam Roach.