Showing posts with label coholomology. Show all posts
Showing posts with label coholomology. Show all posts

Wednesday, December 28, 2016

More As To Rham And Doubolt Cohomologies

Let us initially consider an orbifold eigenset, that is moving through a discrete unitary Lagrangian -- over a sequential series of group-related instantons.  Let us next say that the said orbifold eigenset, is to be moving toward a phenomenology that works to bear a much higher gravitational-based index -- to where the topological substrate that is being moved towards, works to bear a much higher mass than the initially so-stated orbifold eigenset does, in this given arbitrary respective case scenario.  The initially said orbifold eigenset, is to be initially moving via a cohomological mappable-tracing -- that works to bear here a Rham-based cohomology.  Space-time-fabric tends to bend, and not be of a perfectly "straight" nature.  The Fourier-based activity of gravity, is the main general course of force -- that tends to work at bending space-time-fabric.  Since the topological substrate that is being moved towards, works to bear a higher gravitational index, the Fourier-based activity of the first so-stated orbifold eigenset, that is moving towards the second said topological substrate -- will tend to form more of a bending of space-time-fabric per time -- as the said orbifold eigenset is to here be moving closer and closer to the so-eluded-to holonomic substrate, that is of a higher mass-based index.  This will then tend to mean, that as the initially so-stated orbifold eigenset is to be moving towards the so-eluded-to mass that is of a higher genus of Hodge-based index, the more that the initially said Rham-based cohomology will then tend to convert into a Doubolt-based cohomology.  This will then mean, that the closer that the holonomic substrate that is of a lower genus of mass moves towards the holonomic substrate that is of a higher genus of mass -- there is more of a likely-hood of the Hamiltonian operand that is of its initially hermitian-based nature, will then tend to form both at least one Lagrangian-based Chern-Simons singularity and/or one metrical-based Chern-Simons singularity.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.