Alternative Kahler Conditions

Let us initially consider one given arbitrary orbifold eigenset, that is moving in a reverberation -- via a relatively rectangular Lagrangian-based path, that moves at its corners towards the relative left -- as the said respective orbifold eigenset will work here to keep iterating in this case scenario, as a holonomic substrate that acts in a manner that is cyclical as a Hamiltonian operator that behaves in a permutative tense, per each succeeding individually taken cycle of such a so-eluded-to reverberation.  Let us as well, consider that -- at an external reference frame -- the self-same orbifold eigenset  is to reverberate from going into the relative "up" directorial-based direction towards then going into the relative "down" directorial-based direction, as a tensor that is behaving as such a so-eluded-to metrical-gauge-based Hamiltonian operator, over the course of the same group-metric in which such a said eigenset is to be moving via an iterative entity of reverberation, that cycles to the relative left at each succeeding corner of its Fourier-based flow, at what would here be more of an internal-based reference frame.  As eluded-to before in earlier posts, that group-attractor that is most Yukawa to the course of action that is here to be utilized, in so as to work to allow for the just mentioned "up-and-down" tensoric reverberation, acts in a chiral-based manner -- in so as to help in working to allow for the said "upward" motion of the so-stated orbifold eigenset, whereas, that self-same group-attractor that is most Yukawa to the course of action that is here to be utilized, in so as to work to allow for the just mentioned "up-and-down" tensoric reverberation, acts in an antichiral-based manner -- in so as to help in working to allow for the said "downward" motion of the said orbifold eigenset.  Again as eluded-to before, the so-stated relative chiral tendency will tend to work to form torsional eigenindices, that bear  singularities that are of Real Reimmanian roots, while the so-stated relative antichiral tendency will tend to work to form torsional eigenindices, that bear  complex roots.  This alteration of the so-stated orbifold eigenset, from first going into the relative norm-to-forward-holomorphic direction, while then going into the relative norm-to-reverse-holomorphic direction -- will tend to work to form an antiholomorphic Kahler condition, that is proximal localized to certain superstrings that are Yukawa to that Ward-Caucy-based environment -- that is just external to the immediate internal reference frame of the left-tending reverberative flow of the said orbifold eigenset of this given arbitrary respective case.
I will continue with the suspense later!  To Be Continued!  Samuel David Roach.

Isomorphisms Among Adjacent Orbifolds

If a given arbitrary orbifold is shaped in a manner that is neither Minkowski (flat) shaped nor parabollic shaped nor elliptical shaped, then an adjacent orbifold that is of the same universe is not necessarily trivially isomorphic to the initially eluded to orbifold that is shaped in a respectively unique manner.  Depending upon the shape that an orbifold has, an adjacent orbifold that is of the same universe as the initially eluded to orbifold may be shaped in one of many different manners of potential permutation -- depending upon the respective shape of the initially said given arbitrary orbifold.  The more permutations from an orbifold as being either flat, parabollic or elliptical in shape, the more of a chance that a given arbitrary adjacent orbifold that is of the same universe is not necessarily trivially isomormphic to the first given arbitrary said orbifold -- in terms of the corresponding differential geometry.  This is when one is comparing a relationship of the initially eluded to remapping of the topological contour of the first respective orbifold with the topological contour of the second respective orbifold. Again, two adjacent orbifolds that are of the same universe are comprised of Planck-like phenomena that bear an orphoganal differential arrangement -- when relative to one or more of the Planck-like phenomena of the other said orbifold that is here to be of the same universe.  Also, two orbifolds that are of the same universe bear Planck-like phenomena, to where each of the said phenomena bear an intrinsic vibration that is norm to one or more of the Planck-like phenomena that work to comprise the other orbifold that is here of the same universe  -- with a codeterminable wobble that is at a differential sway of ~1.104735878*10^(-81)I degrees.  This angle is equal to the span of arc that 96 spatial dimensions is capable of -- 96piI degrees-- divided by 273*10^(81)I degrees.  This angle is also equal to the span of arc that 32 spatial dimensions is capable of -- 32piI degrees -- divided by 91*^(81)I degrees.  As I have mentioned before, between superstrings that are adjacent -- there is a capability of up to 10^(81) formats of angling.  I will not say what the rest of the derivation as to the number of parallel universes that there are both in overall spatiality and also are just in our set of universes, since this is a touchy subject.  Sometimes, I would rather have people underestimate me than to overestimate me.  Yet, this is no fudging of anything at all.  I will continue with the suspense later!  Sincerely, Sam Roach.