A Description Of Fadeev-Popov Ghosts

Every superstring that is not heterotic bears a certain type of field trajectory that is known as a Fadeev-Popov Trace. The field trajectory of a heterotic superstring is either a light-cone-gauge eigenstate (for E(6)XE(6) superstrings) or a discrete Schwinger Index vibration that is on the periphery of an orbifold or an orbifold eigenset (for E(8)XE(8) superstrings). A Fadeev-Popov Trace is based on the shape of a Chis shape that has a figure-eight shape inscribed within it with a common center. An ideal Fadeev-Popov Trace is one of one-trillion of such related phenomena. Such phenomena are also known of as Plank phenomenon related phenomena. Such phenomena comprise discrete impedance of discrete energy. During each instanton, Fadeev-Popov Trace eigenstates iterate at the reverse holomorphic side of their respective non-heterotic superstrings. After a sequential series of instantons, a Fadeev-Popov eigenstate leaves a physical memory of where the described Trace was located and how it was kinematically differentiating in the transiently prior set of Laplacian states that existed right before the then existing instanton as shown through the said sequential series of instantons that define Fourier Transformation which here describes the directly prior motion of the described trajectory of the associated superstring. This timeless integrated into time wise redistribution of point particles that describes the physical memory of where and how the field trajectory of superstrings has moved after a transient group metric that is covariant and/or conformally invariant is the ghost field of such a Fadeev-Popov Trace. Such a physical memory of one Fadeev-Popov Trace is called a Fadeev-Popov ghost.