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The finite lexicographic lift tie-break is coherent
Statement
Fix one finite universe of uniquely indexed dyadic sites and weights and a dimension . For an ordered tuple of distinct sites whose first sites are affinely independent, the lexicographic lift procedure in Stable-id lexicographic lift perturbation for cocircular and power ties is the determinant sign of one common formal lifted configuration. Every exact nonzero power determinant retains its original sign, every exact zero has a nonzero polynomial tie determinant, and all tuples therefore receive mutually coherent signs. No numeric perturbation parameter is selected or assumed.
Facts & Assumptions
Given: A finite indexed site universe , an ordered tuple of sites from with distinct identifiers, and an affinely independent first sites.
Finite indexed geometric site sets and duplicate handling: identifiers are unique in the input universe, coordinates and weights are dyadic, and the universe is finite.
Dyadic orientation and lifted sphere determinants: the exact determinant is the finite signed Leibniz sum in the displayed row and column order, and the base orientation determinant uses rows .
Stable-id lexicographic lift perturbation for cocircular and power ties: each site uses its one fixed universe rank, and its lifted height is perturbed by the monomial ; the returned sign is the coefficient sign at the least exponent with nonzero coefficient.
The first sites are affinely independent, so their orientation determinant is nonzero.
Proof
Expand the determinant polynomial in [F3] along its lifted-height column. It has constant coefficient equal to the original determinant and one perturbation term for each row; the coefficient of the query row's perturbation is its cofactor, which is up to sign. By [A1] this coefficient is nonzero, so the polynomial is not identically zero.
The exponents are distinct because the ranks in [F3] are distinct across the fixed universe [F1]. Thus no two perturbation terms have the same exponent and their nonzero coefficients cannot cancel. The sign selected by the procedure is exactly the sign of the first nonzero coefficient in this one polynomial, so it is a well-defined sign of one common lifted tuple, not a separate choice for each predicate.
If the original determinant is nonzero, its constant coefficient is the unique term of exponent , while all perturbation exponents are positive; therefore the first nonzero coefficient is the original determinant and its sign is unchanged. If the original determinant is zero, step 1.1 shows a nonzero tie polynomial and step 2.1 gives its unique first coefficient. The finite set supplies one fixed rank assignment for every tuple, so the signs are coherent and the procedure uses no arbitrary epsilon choice.
Depends on
Used by
- Finite exact 3D Delaunay and regular lower-hull cavity repair Algorithm
- A cocircular four-site tie selects the stable-id diagonal Example
- An illegal planar Delaunay flip strictly decreases lifted interpolation volume Lemma
- Generic lower lifted facets project to a triangulation of the convex hull Lemma
- Exact 3D lower-hull insertion covers the hull and terminates Theorem
- Exact planar insertion terminates with a weak empty-circle triangulation Theorem
- Three-dimensional Delaunay and regular output size is quadratic Theorem
Cited to discharge well-definedness by Stable-id lexicographic lift perturbation for cocircular and power ties.
Dependency tree · two levels
7 results within two dependency steps of this one, each drawn at its shortest distance from it. An arrow runs from a result to what uses it, so the chart reads left to right and ends at this result, which carries a heavier outline. Every node is a link to that result. Click elsewhere on the chart to enlarge it.
Sources
- Don Sheehy, Computational Geometry, Fall 2014, Lecture 22: Weighted Delaunay Triangulations (standard reference, not scraped)
- CGAL 6.3 User Manual, 3D Triangulations, Regular Triangulation (standard reference, not scraped)