When Chern-Simons Invariants are to be embedded upon the holonomic substrate of the force of pressurized vacuum, -- this tends to work to form force-fields.
When Chern-Simons Invariants are to be embedded upon the holonomic substrate of the point- commutative force, -- this tends to work at helping to form the i*PI(del) Action.
When Chern-Simons Invariants are to be embedded upon the holonomic substrate of the strong force, -- this tends to work to help at forming the multiplicit Majorana-Weyl-Invariant-Mode.
When Chern-Simons Invariants are to be embedded upon the holonomic substrate of the electromotive force, -- this tends to work to help form, what may be generally thought of as being charge.
When Chern-Simons Invariants are to be embedded upon the holonomic substrate of the weak force (spontaneous radioactive decay), -- this tends to help at working to form entropy as a whole.
To Be Continued! Sincerely, Samuel David Roach.
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