Some Stough That may Explain Better Gauge-Bosons

Gauge-Bosons are E(6)XE(6) strings.  These are examples of heterotic strings.  Gauge-Bosons exist in the substringular neighborhood adjacent to the light-cone-gauge eigenstates of superstrings that comprise discrete energy permittivity.  A gauge-boson -- such as all heterotic superstrings -- is a closed superstring.  Gauge-Bosons pluck the light-cone-gauge eigenstates of superstrings that comprise discrete energy permittivity -- like a harp is plucked -- so that vibrations known of as Schwinger-Indices may form in such a manner so that the Rarita Structure may oscillate in order for the Ricci Scalar to take effect & so that the Wick Action may form (the latter is indirectly caused by the activity of Schwinger-Indices).  In the process of gauge-bosons plucking light-cone-gauge eigenstates, here, in a given arbitrary example, a gauge-boson initially touches a second-ordered light-cone-gauge eigenstate in a Gliossi manner at an arbitrary covariant codeterminable manner.  As the said gauge-boson begins to "pluck" the mentioned second-ordered light-cone-gauge eigenstate, the directly corresponding gauge-boson forms a torsion with the said light-cone-gauge eigenstate that pulls here in four different formats of holomorphic directoralization.  The gauge-boson pulls, and, in any order that the here said gauge-boson is directed to do so, in the norm-to-norm-to-holomorphic general direction, the norm-to-reverse-norm-to-holomorphic general direction, the holomorphic general direction, and, in the reverse holomorphic general direction.  All for wave-tugs just mentioned-- or wave-pulls -- these happen in four different sub-metrics over BRST.  A closed superstring that directly comprises discrete energy permittivity is generally thought of as a two-dimensional superstring that directly bears a three-dimensional field.  Since a gauge-boson -- appearing at first notice SEEMS to initially be such a closed string, yet, having the gauge-metrical activity of pulling in four different general holomorphic-based directoralizaitons over the course of BRST, then, such a mentioned boson -- a gauge-boson -- actually exists in a tense of twelve spatial dimensions plus time.  This is in part also due to the condition that the mentioned Gliossi-based torsioning that happen at a Poincaire-based cohomological coniaxial tends to happen in equal scalar amplitude of displacement in terms of the distance that the related Lagrangian of the corresponding pull is extended for all four holomorphic-based general directoralizations that I had mentioned.  When one then considers that a closed superstring tends to have a field of three spatial dimensions plus time, and that four holomophic spatial general directoralizations that codifferentiate via a wave-tug that is displaced via an equal Lagrangian-based displacement during the same iteration of BRST during instanton happens in this case, then, in a very real manner, an E(6)XE(6) superstring acts as a twelve-dimensional superstring that bears a ghost field over an integration of a successive series of instantons that mirrors the condition of a Gliossi-Sherk-Olive-based field that is here thirteen-dimensional.  (The residue due to the activity of the release of the corresponding Gliossi-based cohomological torsioning that happens when the related Poincaire-based coniaxial is pulled apart via the an equal and opposite wave-tug  that happens in the opposite directoralization pulse that "bounces" the related gauge-bosons off of the corresponding light-cone-gauge eigenstates is what works to form the appearance of such a field.)  I will continue with the suspense later!  Sam Roach.