Abstract: What is the smallest size of a family of subsets of [n] such that it does not contain an induced copy of Q2​ as a poset (known as the \textit{diamond}), but adding a new set creates such a copy? It is easy to see that a maximal chain has this property, and thus the answer is at most n+1. Despite the simplicity of the diamond structure, the lower bound stagnated at n​ for quite some time, until recently the authors obtained a linear lower bound. In this paper, we fully solve this question showing that such a family must have size at least n+1.
The paper proves the main result that every induced-diamond-saturated family in the Boolean lattice has at least n+1 sets, matching the maximal-chain construction and establishing sat*(n,Dâ‚‚)=n+1.
The authors combine minimal and maximal decompositions, a peeling process, trace arguments, and disjointness lemmas to convert local diamond witnesses into a global linear lower bound.
The result confirms a strong case of the bounded-versus-linear saturation dichotomy, while leaving the classification of all extremal families and exact values for higher Boolean lattices open.
Overview
This paper by Ivan and Jaffe determines the induced saturation number of the diamond poset D2​ (the two-dimensional Boolean lattice) exactly: for every n, sat∗(n,D2​)=n+1 (2604.06521). The upper bound is elementary—a maximal chain of subsets of [n] contains no induced diamond, yet adding any missing set creates one. The substance of the paper is the matching lower bound, which closes a gap that had persisted at n​ for years before the authors' recent linear bound of (n+1)/5 [diamondlinear]. The result also confirms a strong instance of the prevailing dichotomy conjecture in poset saturation, which predicts that every finite poset has either bounded or linearly growing saturation number [keszegh2021induced].
Background and context
A family F⊆P([n]) is P-saturated if it avoids an induced copy of P but any outside set completes one; sat∗(n,P) is the minimum size of such a family. The notion was introduced by Ferrara et al. [ferrara2017saturation], and the general theory exhibits a coarse dichotomy: the saturation number is either bounded or at least n0 [freschi2023induced], while always polynomially bounded [polynomial]. Linearity had previously been established only for a short list of posets—the butterfly, the antichain, non-chain complete multipartite posets, the n1 poset, and the diamond—and among these the diamond resisted exact analysis longest.
The paper's structural contribution goes beyond the specific value. The authors note that even identifying which features make a poset's saturation number unbounded remains open; their earlier work showed that adding at most three "special" points to any poset yields a poset with linear saturation number [gluing], and that linear sums propagate unboundedness under certain conditions [sums].
Framework
The proof assumes n2 is diamond-saturated with n3 (otherwise a lemma of Ferrara et al. already gives n4). Under this assumption there exist a minimal and a maximal element that are incomparable. The authors then define two symmetric decompositions:
Minimal side: n5 (minimal elements), n6 (sets that are minimal elements of diamonds whose other three members lie in n7), n8 (maximal elements of n9 not contained in any member of sat∗(n,D2​)=n+10), and sat∗(n,D2​)=n+11, the sets in sat∗(n,D2​)=n+12 serving as middle elements of diamonds generated by members of sat∗(n,D2​)=n+13.
Maximal side: the dual objects sat∗(n,D2​)=n+14 obtained by passing to complements.
Two facts anchor the argument. First, sat∗(n,D2​)=n+15 is sat∗(n,D2​)=n+16-saturated, so every subset of sat∗(n,D2​)=n+17 either contains a member of sat∗(n,D2​)=n+18, is contained in one, or is contained in a member of sat∗(n,D2​)=n+19. Second, [n]0 and [n]1 are disjoint, as are [n]2 and [n]3. Supporting lemmas supply local structure: for each [n]4 with [n]5 minimal, some pair [n]6 lies in [n]7 above [n]8; each [n]9 forces at least n​0 members of n​1 of size at least n​2; and each n​3 admits, for each n​4, a member of n​5 inside n​6 containing n​7.
Lower bounding n​8
The central device is a peeling process on n​9. Writing (n+1)/50 for the subfamily of (n+1)/51 containing (n+1)/52, the authors iteratively select an element (n+1)/53 whose trace family (n+1)/54 is inclusion-minimal among traces on the current support, remove it, and continue until exhaustion. This produces disjoint blocks (n+1)/55 partitioning (n+1)/56, where (n+1)/57 is the set of ground elements appearing in no minimal set, together with (n+1)/58 distinct members (n+1)/59 satisfying F⊆P([n])0.
Under the assumption F⊆P([n])1 (where F⊆P([n])2), an inductive argument shows that each F⊆P([n])3 yields a distinct pair of sets in F⊆P([n])4: one meeting F⊆P([n])5 in exactly F⊆P([n])6 and another incomparable companion. The construction augments a maximal trace set F⊆P([n])7 with a carefully chosen filler F⊆P([n])8 from F⊆P([n])9—chosen via a covering-counting lemma guaranteeing avoidance of all minimal sets—so that the resulting set must be covered by some P0, whose generating diamond then supplies the two desired middle elements. Distinctness across all P1 follows from the intersection pattern with the blocks.
Combining the pieces gives P2, and, when P3, the stronger bound P4 with all contributing P5-sets containing P6. By complement symmetry, analogous bounds hold for P7.
Disjointness and the final contradiction
To combine the two sides additively, the paper establishes that when P8, the families P9 and P0 are disjoint. Three propositions deliver this:
P1 when P2: a set that is simultaneously minimal and maximal forces, for each of its elements P3, three distinct members of P4 differing from it exactly by P5, giving P6.
P7 (and dually): immediate, since membership would contradict minimality.
P8 when P9: a double-counting argument using Lemma sizeB constructs sat∗(n,P)0 forced members of sat∗(n,P)1 around a hypothetical common element sat∗(n,P)2; since sat∗(n,P)3 and sat∗(n,P)4, at least two coincide, pinning down the overlap exactly as sat∗(n,P)5 of total size sat∗(n,P)6—but the top element sat∗(n,P)7 of the second diamond escapes this collection, forcing sat∗(n,P)8.
With disjointness in hand, the main theorem follows by contradiction from sat∗(n,P)9 in two cases. If n00, the additive bounds give n01, and a size-separation argument (via Lemma sizeA) shows n02, yielding n03. If n04 (say), the strengthened bound plus Lemma nicelemmame produces a forest of pairs n05 over n06; accounting for overlaps between this forest, n07, and n08 gives n09, and any maximal element n10 lies outside all three collections, pushing the count to n11—a contradiction. Hence n12.
Limitations and open questions
The proof is specific to the diamond; the authors state plainly that it reveals little about the structure of extremal diamond-saturated families. Beyond maximal chains, n13 together with all singletons, and n14 together with all co-singletons, no diamond-saturated family of size exactly n15 is known, and they conjecture these are the only ones—with the sharper conditional claim that any such family avoiding both n16 and n17 has size at least n18 for a universal constant n19. Whether a size-n20 example avoiding n21 and n22 exists is left open. For higher Boolean lattices, they exhibit a construction showing n23 and conjecture generally that n24 for n25; neither the n26 case nor the general form is settled here. The method also relies on the assumption n27 to obtain disjointness of the two sides, so the argument does not directly transfer to settings where that hypothesis fails.
Conclusion
The paper settles the induced saturation number of the diamond at exactly n28, upgrading the known linear lower bound to the precise optimum and providing the first exact value for a poset whose analysis had proven resistant. Technically, the contribution rests on a nested-trace decomposition of the minimal elements, a filling scheme that converts coverage by n29 into distinct witnesses in n30, and disjointness results that allow the minimal and maximal sides to be summed. The classification of extremal families and the extension to general hypercubes n31 remain open.
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