Perturbation Out Of Homotopy

 When the isomorphic symmetry of the holonomic metric, of an initially homotopic set of discrete energy, is brought into a perturbative state, this will often tend to incur the general physical condition, to where such a mentioned respective set of discrete energy quanta, is thence to often tend to ensue, in so as to spontaneously be brought out of such a general physical condition of homotopy. SAMUEL ROACH.

Perturbation Of Cohomology -- Often Associated With An Increased State Of Entropy

 When a given arbitrary Noether-Based Hamiltonian Operator, of which is here to be initially exhibiting the display of a De Rham cohomology, is to spontaneously alter, into exhibiting the display of a Dolbeault cohomology, this will often tend to be directly associated, with an increased state of entropy. SAM.

The Coupling Of Two Projected Etale Cohomology-Related Covariant Kinematic Structures, That Are Relatively Nijenhuis To One Another

 The Gliosis-Based coupling of two different initially projected Etale cohomology-related covariant kinematic structures of topological manifold, that are here to bear the initial state or condition, of working to exhibit the display, of a relatively Nijenhuis relationship with one another, may, at times, have the general tendency of consequentially resulting, once these are here to work to bear the ensuing inferred coupling interaction, in the spontaneous subsequent formation, of a set of one or more p-Adic cohomology-related covariant kinematic structures of topological manifold. TO BE CONTINUED! SINCERELY, SAMUEL ROACH.

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).

Lack Of Perturbation Of Motion In Relation To Light -- Gauge-Invariance

 Whenever an energy state is to LACK a tense of perturbative motion, in relation to light -- it will consequently tend to be gauge-invariant. TO BE CONTINUED! SINCERELY, SAMUEL ROACH. (1989).

The Main Difference Between Voltage AND The Main Influence Formed By The Force Of Pressurized Vacuum

 The Main difference between Voltage AND the Main Influence that is created by the Force of Pressurized Vacuum (this Main Influence, of which is a general tense of a metric-gauge-related field), is:

Voltage is kinetic energy per charge; Whereas, the Main Influence that is created by the force of pressurized vacuum -- is equivalent to energy in static equilibrium, of which tends to be in a state of super-conformal invariance at an internal reference-frame, per charge. I will continue with the suspense later! To Be Continued! Sincerely, SAM. (1989).

The Majorana-Weyl-Invariant-Mode, And The Rest State Of Mass-Bearing Sets Of Discrete Energy Quanta

 It is the multiplicity of the general exhibition of the Majorana-Weyl-Invariant-Mode, that works to be the primary type of an influence, -- that is here to work to help in allowing, for mass-bearing cohesive sets of discrete energy quanta, to have the general capacity, of being able to be brought into a "state of rest." SAMUEL DAVID ROACH.

Highly Magnetic Cohesive Set Of Discrete Energy Quanta

 A given arbitrary Noether-based mass-bearing cohesive set of discrete energy quanta, that is here to be of the nature of a specific given arbitrary Hodge-Index of a quantum energy state, -- is to tend to be of a highly magnetic nature; when it is both to work to bear an isotropically stable homeomorphic rotational spatial translation, over a proscribed duration of time, as well as when it is to work to bear an isotropically stable homeomorphic transversal spatial translation, over that same eluded-to proscribed duration of time. Sincerely, SAM ROACH. (1989).