The Third Part of Session Seven of Course 19 -- The Klein Bottle and Orbifold Differentiation

When one is to spatially majorize a basic planar surface that acts as a Hamiltonian-based operand in time and space, that is of a simple flat-space-like configuration,  when this is in terms of what the tendency of what you will physically get in the process -- one will tend to have a three-dimensional physical field that works here to bear an added tensoric-based genus, that will here tend to be related predominantly to the physical existence of a spin-orbital-based coniaxioin -- to where this said spin-orbital-based coniaxion will here tend to curve in so as is the relatively local general curvature of the directly related space-time-fabric would then have a tendency to curve as such.  When one is to then here work to extrapolate a majorization of the directly previously mentioned three-dimensional spatial field -- that would here have an added spin-orbital coniaxion that is incorporated as had been eluded-to into the Hamiltonian operand of that particular eigenstate of space that is to bear any of certain given arbitrary Hamiltonian operators, that would here be functional from within the just-eluded-to general region, one will then get a set of two additional tensorsic-based operators "on top of that"-- that will here tend to be related predominantly to the physical existence of both a transversal-based coniaxion and a radial-based coniaxion -- this said set of both a transversal-based coniaxion and a radial-based coniaxion of which will here tend to curve, in so as is the here relatively local general curvature of the directly related space-time-fabric would then have a tendency to curve as such.