A Description Of Ghosts of Klein Bottle Eigenstates

A Klein Bottle eigenstate in one discrete unit of the Klein Bottle.
The Klein Bottle is a general term for a type of physical pheonmenon that exists all over the place in physicality.
A Klein Bottle eigenstate is built based on the Ward conditions of something known as a Schotky Construction.
A Schotky Construction is comprised of four orientifolds that exist as two parallel Klein Bottle associated sides that are perpindicular to two flushly oriented parallel Klein Bottle sides that in and of themselves also happen to be parallel to each other. An orientifold is one of two parallel sides of a Schotky Construction that act as relatively loose mini-string that bear a semipermeable allowance of what is to enter them while also what is to not enter them. These adjacent "house-shade"-like mini-string that comprise the described two sets of orientafolds are used to help draw in the proper norm-states while yet dejecting inappropriate norm-states that should not enter the Schotky Construction of a Klein Bottle eigenstate. The norm to antiholomorphic side of a Klein Bottle eigenstate is comprised of relatively compactified mini-string that are interconnected, while the norm to holomorphic side of a Klein Bottle eigenstate is open to stringular and Planck phenomenon related phenomena that has a need of entering the described Schotky Construction in order that discrete energy permittivity and discrete energy impedance may be rejuvinated so that energy may be able to persisty. A Klein Bottle eigenstate is four Planck Lengths long, two Planck Lengths wide, and one Planck Length thick. As a Schotky Construction as a Klein Bottle eigenstate is redistributed over a Fourier Transformation, the norm-states and/or the scattered Fock Space that is redistributed by the described motion form a physical memory of where and how the associated Klein Bottle eigenstate kinematically differentiated over time. One of such a physical memory of one Klein Bottle eigenstate is considered to be a discrete ghost anomaly of one Klein Bottle eigenstate. As the phenomena within the region of such a described ghost anomaly is moved upon by phenomena once the ghost has already formed, the said ghost anomaly is scattered in order to form residue that may have alterior purposes -- such as forming dilatons and dilatinos in order that gravitational particles may be able to be formed. Remember, ghosts that exist in the neighborhood of a given Real Reimmanian Plane often bear spontaneous interchange with ghosts that are off of the neighborhood of a given Real Reimmanian Plane. Besides these essential functions of transient ghost anomalies, ghost anomalies also are used to share with other point particles what is necessary for the recycling of norm-states, scattered Fock Space, as well as helping with the recycling of superstrings after a relatively long group metric.