The Fourier-Related-Progression of a given arbitrary Hamiltonian Operator, may often tend to be perceived of, as being, the quotient that is here to exist, between the respective Fourier-Transformation of the said Hamiltonian Operator, as divided by the directly associated Lagrangian of that self-same inferred "team" of discrete energy quanta. (To where; Such a stated "team" of discrete energy quanta, may be thought of as being a means of working to describe, the herein mentioned "Hamiltonian Operator.") SINCERELY, SAMUEL DAVID ROACH. TO BE CONTINUED LATER!!!
No comments:
Post a Comment