Resonant Vibration Of A Quantum Of Discrete Energy Impedance

 When all of the second-order light-cone-gauge eigenstates, of which are here to work to comprise the workings, of one given arbitrary respective individually taken first-order light-cone-gauge eigenstate, are here to bear a homeomorphic harmonization of their vibrational oscillation, this general genus of a kinematic process, will often tend to help, in working to allow, for such an inferred quantum of discrete energy impedance, to consequently have a heightened capacity, of resulting in working to form, a tense of resonant vibration. I WILL CONTINUE WITH THE SUSPENSE LATER1 O BE CONTINUED! SINCERELY, SAMUEL DAVID ROACH. 

Pulsation, Velocity, And Acceleration

 When a first-order torsional metric-pulse, is to be inversely coupled, by a first-order torsional heuristic-pulse, this will often tend to work, to form the general tense, of a transversal-based velocity. Furthermore; When a first-order torsional metric-pulse, is to be inversely coupled, by a second-order torsional heuristic-pulse, this will often tend to work, to form the general tense, of a transversal-based acceleration. I WILL CONTINUE WITH THE SUSPENSE LATER!  TO BE CONTINUED! SAM. 

Inverted Torsional Metric-Pulse

 When one is to have a given arbitrary case scenario, of which is here to work to involve a first-order inverted torsional metric-pulse, acting as a given arbitrary example of a particular genus of a Chern-Simons Invariant gauge-action, this may often work to involve a directly corroborative loosening, of a state or condition of a proximal local wave-tug, as acting to work to exhibit the Fourier-Related display, of the workings of a directly associated p-Adic cohomology. TO BE CONTINUED! SAMUEL ROACH. (1989).

Symmetrically Duplicated Tense Of Gauge-Invariance

 The more symmetrically duplicated of a tense of gauge-invariance, that the individually taken first-order light-cone-gauge eigenstates are here to bear interdependently amongst themselves, in a respectively covariant manner, to where such stated first-order light-cone-gauge eigenstates, are here to mutually come together, in so as to work to comprise the net light-cone-gauge eigenstate, that is of a correlative respective mass-bearing cohesive set of discrete energy quanta, it consequently follows, that the more likely that such an eluded-to "team" of mass-bearing discrete energy quanta, will consequently result, in working to bear a respective tense of isotropic stability. (This is to where, such a just stated "team" of mass-bearing energy, will thereby often tend to work to bear a correlative tense of a homomorphic nature.) I WILL CONTINUE WITH THE SUSPENSE LATER! SINCERELY, SAMUEL DAVID ROACH. (1989).