Some More As To Substringular Fields

If a one-dimensional superstring of discrete energy permittivity is to move in a directoral-based manner that goes in the direction of its length -- either in the relative norm-to-holomorphic direction, or, in the relative norm-to-reverse-holomorphic direction -- then, the directly corresponding core-field-density of the correlative two-dimensional field that is thus formed, as may be extrapolated via the mappable tracing of the correlative ghost-based indices, will work to form a field that will bear a relatively conical-based topological swipe, over time.  This is true, whether the said one-dimensional superstring does or does not work to bear a definitive Real Reimmanian vibrational-based topological sway, in a radial manner, during the metric in which such a so-stated superstring of discrete energy permittivity is in the process of kinematically being displaced and re-delineated over the so-eluded-to Lagrangian -- in which the so-eluded-to phenomenology is being translated from one general spot to the next, in the so-stated either relative norm-to-holomorphic or relative reverse-norm-to-holomorphic directoral pattern, that I have here mentioned.  If the so-mentioned conical-based field, that is here a two-dimensional core-field-density that is formed by the said one-dimensional superstrings, bears no Njenhuis tensors in its Lagrangian-based topological sway, then, the so-stated conical field will be of a Minkowski nature -- that will here bear relatively few aberrations of cyclic permutations.  Yet, if the so-mentioned conical-based field is instead of such a nature that it bears one or more Njenhuis tensors in its Lagrangian-based topological sway, then, the so-stated conical field will be of more of a Hilbert nature.  A Minkowski field is of a flat space, and, a Hilbert field is of a volumed space.  So, if the just-eluded-to core field density of a Minkowski-based field, that is generated by the motion of a one-dimensional superstring over time, happens in a unitary Lagrangian that bears no Njenhuis tensors, then, the resultant cohomological-based ghost anomaly-related format of the correlative mappable tracing will be of a Rham nature -- if the vibrational aspects of the directly corresponding kinematic motion that is here eluded-to are harmonic in oscillation.  Yet, instead, if the so-eluded-to one-dimensional superstring either bears Lagrangian-based Njenhuis tensors, and/or if the so-eluded-to one-dimensional superstring bears metrical spikes in its vibrational oscillation -- over a given arbitrary metric in which it is moving over a successive series of instantons, then, the directly corresponding resultant cohomology will instead be of a Doubolt nature.  I will continue with the suspense later!
To Be Continued!  Sincerely, Sam Roach.