Thursday, October 13, 2016

Part 5 Of Session 2 Of Course 20 -- Calabi Interactions And Calabi Manifolds

Let us initially consider the general tendency, as to the general differential geometry of the relative conglomeration of one discrete quantum of energy, to where there are here to be:  one respective given arbitrary correlative Fadeev-Popov-Trace eigenstate, its correlative superstring of discrete energy permittivity, as is to here be at a positioning that is just to the relative forward-holomorphic of a Laplacian-based distribution at the very start of BRST, and, the here correlative counterstring, as is to here be at a positioning that is just to the relative forward-holomorphic of a Laplacian-based distribution, as well, at the very start of BRST.  It is the correlative light-cone-gauge eigenstate, of the so-eluded-to discrete quantum of energy -- that acts in so as to work to inter-connect the so-stated Fadeev-Popov-Trace eigenstate with its directly correlative superstring of discrete energy permittivity.  And, it is a correlative proximal localized set of mini-stringular segmentation -- that acts in so as to work to inter-connect the so-stated superstring of discrete energy permittivity with its directly corresponding counterstring.  The most inert tendency of a given arbitrary holomorphic flow, is to here, be going in a Fourier-based manner, in a relatively "straight" manner -- from the initial relative Laplacian-based distribution of the here correlative Fadeev-Popov-Trace eigenstate, towards the initial relative Laplacian-based distribution of the here correlative counterstring, -- over a successive series of group-related instantons.  Quite often, in reality (the theorertical versus the actual), when there is any general genus of a torsioning, that is to here happen to the holonomic substrate of any of one individually taken discrete quantum of energy, it will then tend to cause a Fourier-based differentiation of a kinematic-based Hamiltonian operation, to where the interconnections, that may have here been of an initial state of linearity -- will then work to, instead, bear a tendency towards an oscillitory-based bending of the torsional-based eigenindices -- that are to here be interconnecting the proximal localized partially integrated genre, of such a said discrete quantum of energy.  Such a resultant oscillation of the kinematic-based eigenindices, that work to bind the partially integrated genus of one respective given arbitrary quantum of energy -- will work to help in the here resultant alteration of the directoral-based Hamiltonian operation, that is to here be correlative to a continued change in the here respective holomorphic direction of the said discrete quantum of energy.
To Be Continued!  Sincerely, Samuel David Roach.

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