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Strong ε-Net: Bounds & Constructions

Updated 27 June 2026
  • Strong ε-nets are subsets of a finite point set in ℝ^d ensuring any geometric range containing more than an ε fraction of points includes at least one point from the subset.
  • They differ from weak ε-nets by requiring the net’s points to belong to the original set, making them crucial for range families like axis-parallel rectangles, halfspaces, and disks.
  • Research in this field provides nearly tight upper and lower bounds using techniques such as slicing, grid partitioning, and Delaunay triangulation for effective net constructions.

A strong ϵ\epsilon-net is a combinatorial geometric object that provides a highly constrained representative subset of a finite point set in Rd\mathbb{R}^d with respect to a specified family of geometric ranges. For a given finite set PP of nn points and a family C\mathcal{C} of (typically convex) subsets of Rd\mathbb{R}^d, a strong ϵ\epsilon-net is a subset NPN \subseteq P such that every range CCC \in \mathcal{C} containing more than ϵn\epsilon n points of Rd\mathbb{R}^d0 also contains at least one point of Rd\mathbb{R}^d1. The defining property of a strong Rd\mathbb{R}^d2-net, in contrast with weak Rd\mathbb{R}^d3-nets, is that its constituent elements are required to be points of Rd\mathbb{R}^d4 itself rather than arbitrary points in the ambient space. The article "Small Strong Epsilon Nets" (Ashok et al., 2012) introduces and analyzes small strong Rd\mathbb{R}^d5-nets, providing exact and nearly tight upper and lower bounds on their minimal size and covering fraction for key geometric range families in the plane and higher dimensions.

1. Formal Definitions

Let Rd\mathbb{R}^d6 be a finite set of Rd\mathbb{R}^d7 points and Rd\mathbb{R}^d8 a family of geometric ranges. The central notions are:

  • Strong Rd\mathbb{R}^d9-net: A subset PP0 is a strong PP1-net for PP2 if for every PP3 with PP4, the intersection PP5 is nonempty.
  • Weak PP6-net: As above, but PP7 need only be a subset of PP8, not necessarily of PP9.
  • Centerpoint and Strong Centerpoint: A centerpoint nn0 of nn1 is a point lying in every convex set containing more than nn2 points of nn3; a strong centerpoint for nn4 is nn5 contained in every nn6 with nn7 for some constant nn8. In this language, a strong centerpoint is a one-point strong nn9-net.
  • Small strong C\mathcal{C}0-nets: For a family C\mathcal{C}1 of ranges, define C\mathcal{C}2 as the smallest C\mathcal{C}3 such that every C\mathcal{C}4-point set C\mathcal{C}5 admits a strong C\mathcal{C}6-net C\mathcal{C}7 of size C\mathcal{C}8, i.e., C\mathcal{C}9.

These definitions set the stage for the quantitative analysis of how well a finite subset of Rd\mathbb{R}^d0 can represent all large-range subsets defined by Rd\mathbb{R}^d1.

2. Main Results for Core Geometric Range Families

Three principal families are examined in the plane: axis-parallel rectangles (Rd\mathbb{R}^d2), halfspaces (Rd\mathbb{R}^d3), and disks (Rd\mathbb{R}^d4). The paper provides explicit finite-size bounds and asymptotic rates for Rd\mathbb{R}^d5 for each:

(I) Axis-parallel Rectangles Rd\mathbb{R}^d6

  • Strong Centerpoint: For axis-parallel boxes in Rd\mathbb{R}^d7, Rd\mathbb{R}^d8. In Rd\mathbb{R}^d9, this specializes to ϵ\epsilon0.
  • Small Nets in ϵ\epsilon1: For ϵ\epsilon2, explicit lower (LB) and upper (UB) bounds for ϵ\epsilon3 are as follows:
ϵ\epsilon4 1 2 3 4 5 6 7 8 9 10
LB ϵ\epsilon5 ϵ\epsilon6 ϵ\epsilon7 ϵ\epsilon8 ϵ\epsilon9 NPN \subseteq P0 NPN \subseteq P1 NPN \subseteq P2 NPN \subseteq P3 NPN \subseteq P4
UB NPN \subseteq P5 NPN \subseteq P6 NPN \subseteq P7 NPN \subseteq P8 NPN \subseteq P9 CCC \in \mathcal{C}0 CCC \in \mathcal{C}1 CCC \in \mathcal{C}2 CCC \in \mathcal{C}3 CCC \in \mathcal{C}4
  • Asymptotic Bounds: CCC \in \mathcal{C}5 for all CCC \in \mathcal{C}6; CCC \in \mathcal{C}7 by recursive grid and slicing constructions.

(II) Halfspaces CCC \in \mathcal{C}8 in CCC \in \mathcal{C}9

  • No Strong Centerpoint: ϵn\epsilon n0.
  • Upper Bounds: ϵn\epsilon n1 for all ϵn\epsilon n2.
  • Lower Bounds: For odd ϵn\epsilon n3, ϵn\epsilon n4 (tight); for even ϵn\epsilon n5, ϵn\epsilon n6. Notably, ϵn\epsilon n7, ϵn\epsilon n8.

(III) Disks ϵn\epsilon n9 in Rd\mathbb{R}^d00

  • No Strong Centerpoint: Rd\mathbb{R}^d01.
  • Upper Bound (for Rd\mathbb{R}^d02): Rd\mathbb{R}^d03.
  • Lower Bounds: For odd Rd\mathbb{R}^d04, Rd\mathbb{R}^d05; for even Rd\mathbb{R}^d06, Rd\mathbb{R}^d07. For Rd\mathbb{R}^d08, there is an explicit construction yielding Rd\mathbb{R}^d09.

3. Fundamental Proof Techniques

Several foundational methodologies underpin the analysis and construction of small strong Rd\mathbb{R}^d10-nets:

  • Slicing Arguments (Rectangles): Partition Rd\mathbb{R}^d11 using one or two coordinate-aligned slabs to localize high-density regions and recurse, yielding moderate-sized nets.
  • Grid Arguments (Theorem 3.1): Partition Rd\mathbb{R}^d12 into Rd\mathbb{R}^d13 horizontal and Rd\mathbb{R}^d14 vertical strips; select near-boundary neighbors to block empty rectangles, then apply recursion.
  • Convex Hull "Necklace" (Halfspaces): Traverse the convex hull of Rd\mathbb{R}^d15, selecting hull vertices so that each large exterior halfspace must contain a selected point.
  • Delaunay/Empty-Circle Argument (Disks): Use the Delaunay triangulation around a centerpoint and the crossing count of segments through triangle edges to force that large disks intersect certain key points.
  • Recursive Lower Bound: Construct two well-separated hard instances and combine, showing Rd\mathbb{R}^d16 for any convex family Rd\mathbb{R}^d17 and Rd\mathbb{R}^d18.

4. Explicit Constructions

Theoretical bounds are realized via concrete algorithmic constructions for small strong Rd\mathbb{R}^d19-nets:

  • Axis-parallel Rectangles: Starting from a strong centerpoint Rd\mathbb{R}^d20 (with covering ratio Rd\mathbb{R}^d21), draw vertical and horizontal lines through Rd\mathbb{R}^d22, partitioning Rd\mathbb{R}^d23 into four slabs. If any slab contains a large fraction, place a net there and its complement; if not, recursions on two slabs of half-size produce higher-order nets while optimizing the balance parameter Rd\mathbb{R}^d24.
  • Halfspaces: Maintain a set starting at a hull vertex, walk along the hull, and, upon encountering a halfspace that would avoid all previously selected points and contain too many points, add the current vertex. Ensure at most Rd\mathbb{R}^d25 points are selected.
  • Disks: Compute a centerpoint Rd\mathbb{R}^d26 and the Delaunay triangulation. The triangle containing Rd\mathbb{R}^d27 (say, Rd\mathbb{R}^d28) provides an edge (e.g., Rd\mathbb{R}^d29) heavily crossed by centerpoint-complement segments. The points Rd\mathbb{R}^d30 and Rd\mathbb{R}^d31 form the net, as any disk avoiding them can only capture a limited fraction of Rd\mathbb{R}^d32.

5. Tabulation of Bounds and Asymptotics

Key ranges and their small-Rd\mathbb{R}^d33 behaviors in the plane are summarized:

Rd\mathbb{R}^d34 Rd\mathbb{R}^d35 Rd\mathbb{R}^d36 Rd\mathbb{R}^d37
Rd\mathbb{R}^d38 Rd\mathbb{R}^d39 Rd\mathbb{R}^d40 Rd\mathbb{R}^d41
Rd\mathbb{R}^d42 Rd\mathbb{R}^d43 Rd\mathbb{R}^d44 Rd\mathbb{R}^d45
Rd\mathbb{R}^d46 Rd\mathbb{R}^d47 Rd\mathbb{R}^d48 Rd\mathbb{R}^d49
Asymptotics Rd\mathbb{R}^d50 Rd\mathbb{R}^d51 (odd Rd\mathbb{R}^d52), Rd\mathbb{R}^d53 even Rd\mathbb{R}^d54 Rd\mathbb{R}^d55, upper bounds similar to halfspaces (except Rd\mathbb{R}^d56)

These results yield the first nontrivial upper and lower bounds for constant-size strong Rd\mathbb{R}^d57-nets for the considered range families.

6. Open Problems and Research Directions

Several directions remain open for exploration:

  • Determining the exact values of Rd\mathbb{R}^d58 for Rd\mathbb{R}^d59, Rd\mathbb{R}^d60 for even Rd\mathbb{R}^d61, and Rd\mathbb{R}^d62 for Rd\mathbb{R}^d63.
  • Improving upper bounds for disks beyond Rd\mathbb{R}^d64 and closing the gap between bounds of type Rd\mathbb{R}^d65 (from halfspace-style constructions) and the currently known lower bounds.
  • Extending strong Rd\mathbb{R}^d66-net bounds to other low-VC-dimension families such as pseudo-disks or convex Rd\mathbb{R}^d67-gons (Ashok et al., 2012).

The study of small strong Rd\mathbb{R}^d68-nets delineates the precise interaction between geometric range families and discrete point set coverage, distinguishing itself from the theory of weak Rd\mathbb{R}^d69-nets by the requirement that covering points lie in Rd\mathbb{R}^d70. This work establishes existence results for strong centerpoints of axis-parallel boxes in arbitrary dimension and opens avenues for understanding combinatorial geometry through the lens of point set representativity and geometric range complexity.

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