Complementary Tenses Of Light-Cone-Gauge-Based Helicity

Let us first consider here two different cites -- as to where there are two different second-order light-cone-gauge eigenstates that are each being plucked like a harp, by two different gauge-boson eigenstates -- over a covariant iteration of BRST.  Let us say that the helicity of the first respective given arbitrary Schwinger-Index -- that is formed by the plucking of its respective second-order light-cone-gauge eigenstate, is propagated at a complementary Ward-normalizable angle in retrospect to the helicity of the second respective given arbitrary Schwinger-Index -- that is formed by the plucking of its distinctly different respective second-order light-cone-gauge eigenstate -- in this given arbitrary case scenario.  Since the so-stated covariant-based Ward-normalizable angle, by which the two respective given tenses of helicity of the correlative individually taken vibrational oscillation of their respective second-order light-cone-gauge eigenstates, is of a complementary nature -- the pulsation of the vibrational effect of the one so-eluded-to tensor of Rarita Structure eigenstate will not tend to be of a Real Reimmanian nature to the other pulsation of the vibrational effect of the second so-eluded-to tensor of Rarita Structure eigenstate, of such a respective given arbitrary case.  This would then tend to make the viable gravitational effect of the first of such given arbitrary Rarita Structure eigenstates to be of a Li Algebra tensor, or, of a Njenhuis tense -- to the other of such given arbitrary Rarita Structure eigenstates.  I will continue with the suspense later!  To Be Continued!  Sincerely, Sam Roach.