Let us initially consider two different covariant mass-bearing cohesive sets of discrete energy quanta, of which are here to be in the process of being conveyed, by the kinetic transfer of a correlative Legendre (co)homology, via a unitary Lagrangian; to where these inferred mass-bearing sets of discrete energy quanta, are here to both be exhibiting the same relativistic scalar amplitude of a Majorana-Weyl-Invariant-Mode. That mass-bearing cohesive set of discrete energy quanta of the two, that is here to be working to exhibit a stronger holomorphic hermitian wave-tug, as it is here to be in the process of being conveyed through the workings of a De Rham cohomology, over a discrete duration of time (via a directly corresponding Fourier Transformation), will tend to bear a greater probability, of working to bear a greater scalar amplitude of a fractal modulus, than the other of the two mentioned mass-bearing cohesive sets of discrete energy quanta. To Be Continued! Sincerely, SAMUEL DAVID ROACH. (1989).
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