Corection

A norm-state is actually a set of first-ordered-point particles that has one, or relatively few, first-ordered point particles that are supplementally norm to a Minkowski surface of first-ordered point particles. Again, positive-norm states travel holomorphically, while negative-norm-states travel antiholomorphically. In the Klein bottle, the norm-states consist of one first-ordered point particle that is norm to a Minkowski surface of first-ordered point particles that form a 3X3 point particle square. The "top" point particle is just above the "bottom" square by 10^(-43) meters, from the center of the central first-ordered point particle of the associated square to the center of the "top" first-ordered point particle. The "top" first-ordered point particle of each norm-state is angled as previously described from the "top" first-ordered point particle of each reverse holomorphically oriented point particle. Here, negative-norm-states start at the top surface of the Klein bottle with positive-norm-states angled relatively just within this this, yet intertial-wise positioned. The negative-norm-states of the Klein bottle within the positive-norm-states of the Klein bottle then angle as described upward to reach from the central "top" of a positive-norm-state to the central "top" of a negative-norm-state. This structure continues across and down the Klein bottle to form the Neumman conditions of the norm conditions that exist within the Klein bottle when its interior is not perturbated, not mentioning the back-and-forth rebounding of the norm-states given their associated holomorphisms. The entry of a superstring and its corresponding Planck phenomena related phenomenon shakes the given superstring, while keeping the superstring in tact by its associated Planck phenomena related phenomenon equally gaining in impedance due to a Dirac relationship in the metric-gauge sub-quantum that exists between a superstring and its correlative Planck phenomena related phenomenon. A Planck phenomena related phenomenon is the field trajectory of a superstring. The fabric itself of a Fadeev-Popov-Trace is 10^(-129) meters thick, while being 10^(-43) meters long. So, the shaking of a superstring in a Kaeler metric stirs up metric-gauge in the given superstring, while equally settling the impedance of its corresponding Fadeev-Popov-Trace. The light-cone-gauge eigenstate between these reverses the metric-gauge absorption factor that is related to these aspects discrete quantum energy. This is due to the hermitian Ward conditions of light-cone-gauge eigenstates. In so long as a superstring has the opposite abelian geometry in its neighborhood abelian nature of the light-cone-gauge. This is known as a gauge transformation.