A Description Of The Ghosts Of Hausendorf Projections

A ghost anomaly of a Hausendorf Projection is like a ghost of a Campbell Projection, except that a ghost of a Hausendorf Projection is comprised of interconnected Hausendorf norm-states instead of being comprised of interconnected Campbell norm-states.
A Hausendorf Projection involves less of a Laplacian-based abelian nature than that of a Campbell Projection and a Hausendorf Projection involves even less of a Laplacian-based abelian nature than that of a Campbell-Hausendorf Projection. What I mean here by a Laplacian-based abelian nature is the tautness of the differential geometry that exists between the integrative Hodge Index basis of the individual first-ordered point particles taken together as one whole.
As a Hausendorf Projection kinematically differentiates over the course of a Fourier Transformation, the wave-tug operational indices that are used to describe the Hamiltonian operation, the Hamiltonian operators, and the Hamiltonian operands that exist do to the motion of a Hausendorf Projection through the course of a successive series of instantons that describe a framework of time (as a covariant group metric) may involve a co-differentiating field networking that may be more non-abelian than expected theoretically. Yet, per individual instanton, the interlinking of the first-ordered point particles that comprise such a Hausendorf Projection will always bear a more non-abelian Laplacian differentiation than the interlinking of the first-ordered point particles that comprise a Campbell Projection over the same relativistic instanton of Laplacian differentiation. Such is true even when one compares such a Laplacian non-abelian nature of Hausendorf Projections verses those of a Campbell-Hausendorf Projection.
The scattered norm-states and/or the scattered non-linear and inexact Fock Space that is caused by the motion of a Hausendorf Projection -- that is kinematically re delineated from a relative Laplacian condition into the said scattered condition that happens over a Fourier Transformation -- will form a physical memory of where and how the previously described Hausendorf Projection kinematically differentiated over a local region of trajectory. Remember, ghost anomalies are always transient (they exist, yet over a relatively small covarian group metric).
Yet strangely enough, since the shape of Hausendorf Projections bears relative torsion, the ghosts of Hausendorf Projections tend to have more of an abelian nature than those of Campbell Projections. So, there is an inverse relation here which may be cited by the relative Dirac math which this involves.