The boundary double-layer probability measure on a circle #
For a positively oriented circle and a base point xi on that circle, the
scalar boundary double-layer density is 1 / (2 pi) away from the unique
parameter value representing xi and is zero at that parameter by the
inverse-at-zero convention. The exceptional singleton has measure zero, so
the density is nonnegative and has total mass one.
This completely discharges the geometric probability-measure interface in the disk model and recovers the sharp boundary-phase invariant for every polynomial through the general boundary-measure theorem.
Main declarations #
crouzeixBoundaryDoubleLayerDensity_ball_eq_inv_two_pi_of_ne-- the pointwise density away from the base point;integral_crouzeixBoundaryDoubleLayerDensity_ball-- its total mass is one;crouzeixBoundaryDoubleLayerDensity_ball_nonneg-- its pointwise sign;crouzeixBoundaryPhaseContractive_ball_of_boundaryDoubleLayerDensity-- sharp phase contractivity on every positive-radius disk.
Away from its boundary base point, the double-layer density of a
positive circle is the constant 1 / (2 pi).
The boundary double-layer density of a positive circle has total mass one at every boundary base point.
The boundary double-layer density of a positive circle is everywhere nonnegative, including its inverse-at-zero value at the base point.
Every polynomial satisfies the sharp boundary-phase invariant on a positive-radius disk, obtained from the explicit circle probability density.