From Accelerating Via A Euclidean-Related Path Into Accelerating Via A Clifford-Related Path

When any one given arbitrary Noether-based orbifold eigenset, that is here to work to maintain its general tense of spatial dimensionality, is to initially go from being spatially transferred into a tense of a smooth transversally accelerating pattern of motion, via a mappable cohomology that may be traced in a Laplacian-based euclidean-related path, Into then subsequently altering in the general genus of its Lagrangian-based path, -- by being smoothly delineated via a mappable cohomology-related path, that is instead here to be of a Clifford-related manner, in spite of working to bear what would otherwise be the same consistent general pattern of being spatially transferred, via a tense of what would otherwise be the same general type of a smooth transversally accelerating manner of motion, over an evenly-gauged Hamiltonian eigenmetric, that is here to be of the same duration as the initially inferred general tense of motion; then, at the point in time and space at which such a said orbifold eigenset is here to be altering from being spatially transferred as a Hamiltonian Operator, that is here to initially be working to form a euclidean mappable cohomology-related path, via the operational translation of its Lagrangian, over a discrete quantum of time, Into subsequently being spatially transferred as a Hamiltonian operator, that is here to work to form a hyperbolic mappable cohomology-related path, via the operational translation of its Lagrangian, over a discrete quantum of time, -- this general type of an occurrence will consequently tend to work to cause, at the proscribed point of such an alteration in the general genus of a mappable-tracing, a set of one or more Lagrangian-based Chern-Simons singularities; -- although to where such a respective general genus of a scenario, will Often not tend to work to form metric-related Chern-Simons singularities, on account of the stated condition here proscribed of such an orbifold eigenset of such a respective given arbitrary case, to be a case in which one is here to be considering a Hamiltonian Operator, that is to be maintaining its condition of a smoothly-accelerating transversal-based pattern of motion, through time and space. Samuel Roach.