Noether Current And Velocity

When one is to have one given arbitrary combination of discrete quanta of energy, to be put together in one respective given arbitrary spatial arrangement -- with the proscribed Hodge-Indices as to the quantity of both the one-dimensional superstrings of discrete energy permittivity with their correlative substringular counterparts and the two-dimensional superstrings of discrete energy permittivity with their correlative substringular counterparts, that help to work to make-up the physical composition of one respective given arbitrary orbifold eigenset, as well as with the proscribed Hodge-Indices as to the quantity of both the respective and the correlative light-cone-gauge eigenstates and the respective and the correlative Fadeev-Popov-Trace eigenstates that work to form the discrete energy impedance that acts in so as to help make-up the physical composition of one respective given arbitrary orbifold eigenset -- then, one is to have the general format as to what the holonomic substrate of the phenomenology that you are looking for is. If such a substringular arrangement is in such a position, in so as to exhibit one specific given arbitrary tense of Majorana-Weyl-Covariance -- to where this is to work to form a specific effectual Noether Current that bears a resultant topological sway in one given arbitrary directoral-based translation, and if the tense of the vibration of the directly affiliated superstrins is to be of a Calabi-Yau-based nature, in so as to work at helping to form a Calabi-Yau manifold, then, this just described substringular arrangement will tend to form a respective given arbitrary mass, that will work to bear a velocity that will go in the direction of the directoral-based propagation that is of a state of optimum rest, -- for the so-eluded-to composite mass of the so-eluded-to substringular entity of such a case scenario.  To the extent of the lack of cohomological-based inhibition that the just described substringular entity is to have, on account of a respectively loosened tense of the correlative Majorana-Weyl-Covariance, --  the greater that the tendency will be, as to either the scalar amplitude and/or the scalar magnitude of the here directly pertinent Noether Current will be.  The greater that the Noether Current is, per the directly associated amount of substringular phenomenology that is to be transferred from one spot to another, the greater that the velocity of such a substringular phenomenology will then tend to be.  So if two different orbifold eigensets are to work to bear two different quanta of Hodge-based indices, yet are to still  bear the same eigenbase of Noether Current, in such a manner in so as to both be moving in the same Ward-Caucy-based directoralization of topological sway at the same time, via the vantage-point of a central conipoint -- then, that respective orbifold eigenset of such a case, that is to bear the smaller of the two so-eluded-to sets of Hodge-based indices, will then tend to travel at a faster velocity, over the directly associated group-metric that works to inter-bind the two said orbifold eiegnsets in both a codeterminable, a codifferentiable, and in a covariant manner, over time.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.