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Source. Theorem 2, p. 650, of K. J. Swanepoel, Independence Numbers of Planar Contact Graphs, Discrete Comput. Geom. 28 (2002), no. 4, 649-670, doi:10.1007/s00454-002-2897-y; labels and pages as printed in that journal edition, the one named on the source card.

Read depth. Claims checked: the statement and the definitions it uses were read clause by clause on the printed pages; the proof (Sections 3 and 5, pp. 654-661 and 665-670) was read for structure only. Nothing here is independently reviewed.

Statement

Setting (p. 650). A convex disc is a compact convex body in the plane R2\mathbb R^2. Two translates of CC touch when they share boundary points but no interior points, and a finite collection of translates is a packing when no two share interior points; its contact graph has the translates as vertices and the touching pairs as edges. FC(n)F_C(n) is the smallest independence number of the contact graph of a packing of nn translates of CC. The disc CC is a paralleloid when it has two parallel supporting lines meeting CC in segments abab and cdcd whose lengths sum to strictly more than the length of the intersection of CC with any line parallel to them (p. 650, Fig. 1).

Theorem 2 (p. 650, quoted). "If CC is not a paralleloid, then there exists a constant c>14c > \frac{1}{4} depending on CC, such that FC(n)≥cnF_C(n) \geq cn."

The paper's context for the statement (p. 650): if CC is a parallelogram then FC(n)=⌈n/4⌉F_C(n)=\lceil n/4\rceil, and if CC is not a parallelogram the contact graphs are planar and FC(n)≥n/4F_C(n)\ge n/4; the class of non-paralleloids includes every strictly convex disc (abstract, p. 649), in particular the circle. The theorem gives no explicit value of cc. The paper also remarks that the 516n\frac{5}{16}n upper bound of Pach and Tóth for the circle easily generalizes to any CC; that remark is not proved there.

Proof pointer

Contact graphs of translates of CC are the minimum distance graphs of the normed plane whose unit ball is the difference body C−CC-C, and CC is a paralleloid exactly when C−CC-C is (pp. 650-651). Section 3 (pp. 654-661) shows, for an integer m≥5m\ge5 and c=m/(4m−1)c=m/(4m-1), that a smallest counterexample to FC(n)≥cnF_C(n)\ge cn contains the broken-lattice configuration of Theorem 4 (p. 661); Proposition 3 (p. 652, cited from Brass) supplies the proper Brass measure that a non-paralleloid unit ball admits. Section 5 (pp. 665-670) excludes that configuration for mm large enough in terms of the norm: local estimates in Lemma 11 (p. 665) and Lemma 14 (pp. 666-669) feed Lemma 15 (p. 669), whose proof (p. 670) takes m>4+2/δ+41/δεm>4+2/\delta+41/\delta\varepsilon and derives that the unit circle would have circumference greater than 88. The paper omits the proofs of Lemmas 12 and 13 (p. 666), which the proof of Lemma 14 uses repeatedly.

Dependencies

Propositions 1-5, Lemmas 1-9 and 11-15, and Theorem 4 of the same paper; Proposition 3 is cited from Brass, and the circumference bound for a normed unit circle from Thompson's Minkowski Geometry.

Bears on

  • Problem 1066: the problem's graphs are the contact graphs of packings of translates of a circle, which is not a paralleloid, so the theorem gives g(n)≥cng(n)\ge cn for some unspecified c>14c>\frac14. For the circle Theorem 1 gives the explicit c=831c=\frac{8}{31}.