According to the classic harmonic approach, an orientation density function (odf)
f is expanded into its corresponding Fourier orthogonal series with respect to generalized spherical harmonics, and a pole density function (pdf)
into its corresponding Fourier orthogonal series with respect to spherical harmonics. While pdfs are even (antipodally symmetric) functions, odfs are generally not. Therefore, the part
of the odf which cannot be determined from normal diffraction pdfs can be mathematically represented as the odd portion of its series expansion. If the odf
f is given, the even part
can be mathematically represented explicitly in terms of
f itself. Thus, it is possible to render maps of
harmonic orientation ghosts, and to evaluate
variants of mathematical standard odfs resulting in identical pdfs independent of pdf data. However, if only normal diffraction pdfs are known, the data-dependent
variation width of feasible odfs remained unaccessible, and within the harmonic approach a measure of confidence in a solution of the pdf-to-odf inversion problem does not exist.According to any discrete approach, an odf
f defined on some set
G of orientations is expanded into its corresponding Fourier orthogonal series with respect to indicator functions of the elements of a partition of
G, and a pdf
defined on the upper (lower) unit hemisphere
S
+
3
3 into its corresponding Fourier orthogonal series with respect to indicator functions of the elements of a partition of
S
+
3
. The ambiguity of the pdf-to-odf inversion problem is discussed in terms of column-rank deficiency of the augmented projection matrix. The implication of the harmonic approach to split an odf into a
uniquely determined and an
undetermined part does no longer seem to be reasonable. However, it is possible to numerically determine data-dependent confidence intervals for the Fourier coefficients with respect to the indicator functions which can be immediately interpreted as mean orientation densities within the elements of the partition of
G. Doing so for all Fourier coefficients in the finite series expansion, i.e. for all elements of the partition of the set
G, eventually results in the data-dependent variation width of odfs feasible with respect to given pdf data, and to the partitions of
G and
S
+
3
.Thus it is confirmed that the appearance of orientation ghosts, in particular correlations of
true and
ghost orientation components, depends on the representation of an odf. It may be questioned whether in practical applications the implicit assumption of the harmonic method that the even part
can be determined uniquely and free of error is generally a reasonable initial condition to develop ghost correction procedures.
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