Monday, April 9, 2012

Session One Of Course Ten On The Light-Cone-Gauge and Gravity

How do the units of spin, orbit, and transversal momentum of a light-cone-gauge eigenstate fit into the workings of the said light-cone-guage eigenstate?  Each light-cone-gauge quanta is divided into 44 discrete transversal "pieces."  Each of the mentioned light-cone-gauge quanta is divided into 84 discrete segments in terms of orbital momentum.  Each light-cone-gauge quanta is divided into 128 discrete segments in terms of spin-based momentum.  In light-cone-gauge eigenstates that are connected directly to one-dimensional superstrings of discrete energy permittivity, the transversal discrete segments have three times the momentum of the other discrete segments.  With light-cone-gauge eigenstates that are attached to two-dimensional superstrings of discrete energy permittivity that correspond to the norm-to-forward-holomorphic end of the binding that exists between a superstring of discrete energy permittivity and its corresponding Fadeev-Popov-Trace -- these loci that appertain more directly with the norm-to-forward-holomorphic related general section of the Royal Arc -- the spin-related discrete units appertaining to 2-d strings have 1.03125 times the momentum of the spin-related discrete units of light-cone-gauge eigenstates that respectively correspond to those that appertain to one-dimensional superstrings that exist as discrete units of energy permittivity.  During the same arbitrary duration in which BRST happens, the orbit-related discrete units that correspond to a light-cone-gauge eigenstate that is directly affiliated with a two-dimensional superstring have 1.5228095 times the momentum of the orbit-related units that respecitively correspond to a covariant light-cone-gauge eigenstate that is directly affiliated with a one-dimensional superstring.  During the same arbitrary metric that involves a single period of BRST, the transversal discrete units that are associated with the light-cone-gauge eigenstate that is related to a two-dimensional superstring of discrete energy permittivity has 1.909090... times the momentum of the prior mentioned respectively related basis of 44 that I had recently mentioned that involves two-d superstrings in terms of its light-cone-gauge eigenstate, and, the larger of the two Hamiltonian-Based momentums that I have mentioned  earlier in this sentence has only .636363... times the momentum of the transversal discrete units of light-cone-gauge quanta that is attached to respective related one-dimensional superstrings that are simultaneoulsy covariant via a conipoint that is central between the two described arbitrary given superstrings.  With light-cone-gauge quanta that are attacherd to 2-d superstring of the relatively "lower" half of the Royal Arc, the orbit-based discrete units have ~ 1.5714285 times the orbit-related momentum of light-cone-gauge quanta that are attached to a corresponding one-d superstring that is undergoing the same simultaneous parity of Hamiltonian Operation within a shared general region.  The spin-related momentum of these respective quanta is base 128, or, as in the case of 1-d superstrings that are related in terms of their light-cone-gauge eigenstates --  the transversal momentum of these quanta is .636363... times what the said momentum has in the corelative light-cone-gauge eigenstates that are related to the same said respective two-dimensional superstrings.  Sam.  If I made a few mistakes, I am sorry.  I gotta run!  Sincerely, Sam.                    

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