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Hypergraphic Poset: Polyhedral & Lattice Theory

Updated 9 July 2026
  • Hypergraphic posets are defined as partial orders on acyclic orientations derived from hypergraphic polytopes constructed via Minkowski sums.
  • They encompass classical models such as the weak Bruhat order and Tamari lattice by interpreting hypergraph intervals and cyclic arrangements.
  • Lattice criteria based on sourcing and intersection properties guide when these posets become distributive, semidistributive, or full lattices.

A hypergraphic poset is the partial order PHP_{\mathbb H} attached to a hypergraph H\mathbb H on [n]={1,2,,n}[n]=\{1,2,\dots,n\} by orienting the $1$-skeleton of its hypergraphic polytope ΔH=HHΔH\Delta_{\mathbb H}=\sum_{H\in\mathbb H}\Delta_H, where ΔH=conv{eh:hH}\Delta_H=\operatorname{conv}\{e_h:h\in H\}, with a generic linear functional ω\omega. Its elements can be described as acyclic orientations, or source assignments, on the hyperedges, and its order is generated by ω\omega-increasing flips. The construction subsumes several classical posets: the weak Bruhat order on the permutahedron, the Tamari lattice on the associahedron, and, in the cyclic-interval setting, the cyclohedron poset of maximal tubings on the cycle (Bergeron et al., 2024, Gélinas et al., 5 May 2026).

1. Polyhedral definition

Fix a hypergraph H2[n]\mathcal H\subseteq 2^{[n]}, usually with all singletons {i}H\{i\}\in\mathcal H. For each hyperedge H\mathbb H0, the simplex

H\mathbb H1

is the standard simplex on the corresponding coordinate basis vectors, and the hypergraphic polytope is the Minkowski sum

H\mathbb H2

This polytope is a deformed permutahedron, and singletons affect only translation, not the combinatorics (Gélinas, 21 Aug 2025).

A standard choice of linear functional is

H\mathbb H3

although the construction is formulated for a generic H\mathbb H4. Every edge of the H\mathbb H5-skeleton of H\mathbb H6 is oriented in the direction of increasing H\mathbb H7-value, producing an acyclic digraph on the vertices of H\mathbb H8. The hypergraphic poset H\mathbb H9 is then the transitive closure of this oriented [n]={1,2,,n}[n]=\{1,2,\dots,n\}0-skeleton; equivalently, its Hasse diagram is the transitive reduction of the same orientation (Gélinas, 21 Aug 2025).

This polyhedral definition is fundamental because it places order-theoretic questions inside the geometry of generalized permutahedra. In particular, the central structural problem is not whether the orientation exists—it always does for generic [n]={1,2,,n}[n]=\{1,2,\dots,n\}1—but when the resulting acyclic digraph defines a lattice.

2. Acyclic orientations, sourcings, and coordinate order

An orientation of a hypergraph [n]={1,2,,n}[n]=\{1,2,\dots,n\}2 is a choice of a source in each hyperedge,

[n]={1,2,,n}[n]=\{1,2,\dots,n\}3

Equivalently, for every [n]={1,2,,n}[n]=\{1,2,\dots,n\}4, one draws an arrow [n]={1,2,,n}[n]=\{1,2,\dots,n\}5. The orientation is acyclic if the resulting directed graph on [n]={1,2,,n}[n]=\{1,2,\dots,n\}6 has no directed cycle. Vertices of [n]={1,2,,n}[n]=\{1,2,\dots,n\}7 are indexed by these acyclic orientations, and [n]={1,2,,n}[n]=\{1,2,\dots,n\}8-increasing edges in the polytope correspond to increasing flips, in which the source of a collection of covering hyperedges changes from [n]={1,2,,n}[n]=\{1,2,\dots,n\}9 to $1$0 with $1$1 while preserving acyclicity (Gélinas, 21 Aug 2025).

The same structure can be phrased as a sourcing problem. A sourcing $1$2 of a hypergraph chooses $1$3 for each hyperedge $1$4, and the set of all sourcings is ordered componentwise: $1$5 All sourcings therefore form the product of chains $1$6. The acyclic sourcing poset $1$7 is the induced subposet on acyclic sourcings; in general, $1$8 need not be a lattice (Abram et al., 3 Aug 2025).

A major structural result is the source characterization for arbitrary hypergraphs: for any two acyclic orientations $1$9 of ΔH=HHΔH\Delta_{\mathbb H}=\sum_{H\in\mathbb H}\Delta_H0,

ΔH=HHΔH\Delta_{\mathbb H}=\sum_{H\in\mathbb H}\Delta_H1

Thus ΔH=HHΔH\Delta_{\mathbb H}=\sum_{H\in\mathbb H}\Delta_H2 is the coordinatewise order on the set of acyclic source-sequences, not merely a reachability order defined abstractly by flips (Gélinas, 21 Aug 2025). A plausible implication is that many lattice-theoretic questions about ΔH=HHΔH\Delta_{\mathbb H}=\sum_{H\in\mathbb H}\Delta_H3 reduce to asking when the set of acyclic source-sequences forms a sublattice of the ambient product of chains.

3. Classical models and standard examples

The hypergraphic-poset framework recovers several canonical combinatorial orders. These examples are central because they show that hypergraphic posets are not a niche generalization, but a common language for familiar polyhedral orders (Bergeron et al., 2024, Gélinas et al., 5 May 2026).

Hypergraph ΔH=HHΔH\Delta_{\mathbb H}=\sum_{H\in\mathbb H}\Delta_H4 Polytope ΔH=HHΔH\Delta_{\mathbb H}=\sum_{H\in\mathbb H}\Delta_H5 Poset ΔH=HHΔH\Delta_{\mathbb H}=\sum_{H\in\mathbb H}\Delta_H6
All ΔH=HHΔH\Delta_{\mathbb H}=\sum_{H\in\mathbb H}\Delta_H7-subsets ΔH=HHΔH\Delta_{\mathbb H}=\sum_{H\in\mathbb H}\Delta_H8 Permutahedron Weak Bruhat order
All intervals ΔH=HHΔH\Delta_{\mathbb H}=\sum_{H\in\mathbb H}\Delta_H9 Stasheff associahedron / Loday’s associahedron Tamari lattice
All regular and cyclic intervals Bott–Taubes cyclohedron Cyclo-lattice of maximal tubing on the cycle

For the complete-graph hypergraph ΔH=conv{eh:hH}\Delta_H=\operatorname{conv}\{e_h:h\in H\}0, the vertices of ΔH=conv{eh:hH}\Delta_H=\operatorname{conv}\{e_h:h\in H\}1 are permutations of ΔH=conv{eh:hH}\Delta_H=\operatorname{conv}\{e_h:h\in H\}2, the flips are adjacent transpositions that increase inversion number, and ΔH=conv{eh:hH}\Delta_H=\operatorname{conv}\{e_h:h\in H\}3 is the weak Bruhat order on ΔH=conv{eh:hH}\Delta_H=\operatorname{conv}\{e_h:h\in H\}4. In source-sequence terms, each edge ΔH=conv{eh:hH}\Delta_H=\operatorname{conv}\{e_h:h\in H\}5 is sent to ΔH=conv{eh:hH}\Delta_H=\operatorname{conv}\{e_h:h\in H\}6, which recovers the usual inversion-set description of weak order (Bergeron et al., 2024, Gélinas et al., 5 May 2026).

For the interval hypergraph ΔH=conv{eh:hH}\Delta_H=\operatorname{conv}\{e_h:h\in H\}7, ΔH=conv{eh:hH}\Delta_H=\operatorname{conv}\{e_h:h\in H\}8 is the associahedron, and acyclic orientations are in bijection with binary trees with ΔH=conv{eh:hH}\Delta_H=\operatorname{conv}\{e_h:h\in H\}9 leaves, or triangulations of an ω\omega0-gon. The resulting poset is the Tamari lattice. Concretely, each interval-edge ω\omega1 is oriented according to which among ω\omega2 or ω\omega3 appears first in the bracketed tree-walk around the polygon (Bergeron et al., 2024, Gélinas et al., 5 May 2026).

For the complete cyclic-interval hypergraph, containing all regular and cyclic intervals, ω\omega4 is the Bott–Taubes cyclohedron and ω\omega5 is the cyclo-lattice of maximal tubing on the cycle (Gélinas et al., 5 May 2026).

4. Lattice criteria in the interval and cyclic-interval regimes

The basic misconception to avoid is that a hypergraphic poset is automatically a lattice. Even in highly structured families, latticehood is a classification problem rather than a formal consequence of the definition.

For interval hypergraphs ω\omega6, Bergeron and Pilaud give a complete lattice-theoretic classification. The fundamental criterion is: ω\omega7 They further characterize when ω\omega8 is distributive, semidistributive, and a lattice quotient of weak order. In particular, distributivity requires an additional “initial/final” condition on overlaps; join-semidistributivity requires intersection closure together with a four-interval “diamond” condition; and the natural surjection ω\omega9 is a full lattice quotient exactly when ω\omega0 is closed under all subintervals, in which case ω\omega1 factors as a Cartesian product of Tamari lattices (Bergeron et al., 2024).

The cyclic-interval case extends this picture. An edge ω\omega2 is regular if ω\omega3 with ω\omega4 and ω\omega5, and cyclic if ω\omega6 for some ω\omega7. A cyclic-interval hypergraph is one whose hyperedges are all regular or cyclic, with all singletons included. For such a hypergraph ω\omega8, define for every interval ω\omega9

H2[n]\mathcal H\subseteq 2^{[n]}0

Then H2[n]\mathcal H\subseteq 2^{[n]}1 is a lattice if and only if, for every interval H2[n]\mathcal H\subseteq 2^{[n]}2, two conditions hold: first, the collection of regular edges in H2[n]\mathcal H\subseteq 2^{[n]}3 is closed under intersection; second, every hugging quadruple in H2[n]\mathcal H\subseteq 2^{[n]}4 admits a fix. Here a hugging quadruple consists of H2[n]\mathcal H\subseteq 2^{[n]}5 with H2[n]\mathcal H\subseteq 2^{[n]}6 containing H2[n]\mathcal H\subseteq 2^{[n]}7, H2[n]\mathcal H\subseteq 2^{[n]}8 containing H2[n]\mathcal H\subseteq 2^{[n]}9, and with {i}H\{i\}\in\mathcal H0 regular while {i}H\{i\}\in\mathcal H1 are cyclic, or vice versa. A fix is an edge {i}H\{i\}\in\mathcal H2 such that

{i}H\{i\}\in\mathcal H3

This gives a complete lattice characterization for cyclic-interval hypergraphs and extends both the interval result of Bergeron–Pilaud and the complete cyclic-interval result of Adenbaum et al. (Gélinas et al., 5 May 2026, Adenbaum et al., 10 Oct 2025).

The proof strategy in the cyclic-interval case is itself structurally informative. Necessity comes from restricting to {i}H\{i\}\in\mathcal H4 and analyzing minimal failures of join-existence inside hugging quadruples. Sufficiency is established by constructing, for any two acyclic orientations {i}H\{i\}\in\mathcal H5, a pseudo-join {i}H\{i\}\in\mathcal H6 by a regulated path of local “max-moves” on sources of edges, then proving that {i}H\{i\}\in\mathcal H7 is acyclic, dominates both {i}H\{i\}\in\mathcal H8 and {i}H\{i\}\in\mathcal H9, and is minimal with that property; meets are obtained symmetrically (Gélinas et al., 5 May 2026).

A distinct but closely related development studies hypergraphic posets through path hypergraphs of directed graphs. For a directed graph H\mathbb H00 on H\mathbb H01, the path hypergraph H\mathbb H02 has as hyperedges the vertex-sets of all directed paths in H\mathbb H03. When H\mathbb H04 is acyclic and increasing, these hyperedges are intervals in the partial order induced by H\mathbb H05 (Abram et al., 3 Aug 2025).

This perspective brings in two additional posets. The acyclic reorientation poset H\mathbb H06 is defined for a directed acyclic graph H\mathbb H07 by reversing or not reversing each arc, subject to acyclicity. The ornamentation poset H\mathbb H08 consists of compatible choices of ornaments H\mathbb H09, where an ornament at H\mathbb H10 is a subset H\mathbb H11 such that, in the induced subgraph on H\mathbb H12, every H\mathbb H13 has a directed path to H\mathbb H14. Ornamentations are ordered componentwise by inclusion and form a lattice. The paper exhibits commutative squares of order-preserving surjections linking weak order on H\mathbb H15, H\mathbb H16, H\mathbb H17, and H\mathbb H18 (Abram et al., 3 Aug 2025).

For rooted, or more generally unstarred increasing trees, the acyclic sourcing poset of the path hypergraph is isomorphic to the ornamentation lattice: H\mathbb H19 and this lattice is a lattice quotient of H\mathbb H20. For any increasing tree, the ornamentation lattice is the MacNeille completion of H\mathbb H21 (Abram et al., 3 Aug 2025). This gives polytopal realizations of ornamentation lattices and answers an open question of C. Defant and A. Sack.

The same work characterizes which subhypergraphs H\mathbb H22 of a path hypergraph of an increasing tree H\mathbb H23 again yield lattices. Such hypergraphs are called intreeval hypergraphs. The criterion is: H\mathbb H24 This recovers the interval-hypergraph criterion on a path as a special case (Abram et al., 3 Aug 2025).

6. Structural significance and directions

The modern view of hypergraphic posets combines polyhedral realization, source-sequence combinatorics, and lattice theory. On the polyhedral side, hypergraphic polytopes realize acyclic sourcing posets through linear orientation, and graphical zonotopes realize the analogous reorientation posets (Abram et al., 3 Aug 2025). On the order-theoretic side, the coordinatewise source characterization shows that the difficulty lies not in defining the order, but in understanding the structure of the acyclic region inside the ambient product of chains (Gélinas, 21 Aug 2025).

This viewpoint clarifies why classical lattices recur. Many familiar lattices appear as H\mathbb H25 when H\mathbb H26 ranges over building-sets, nestohedra, graphical zonotopes, and hyperplane arrangement galleries (Gélinas et al., 5 May 2026). It also explains negative examples. The acyclic sourcing poset need not be a lattice in general; the freehedron hypergraph fails even to be a lattice in the interval setting, and a small starred tree produces ornamentations while the corresponding acyclic sourcing poset has a diamond and is not a lattice (Bergeron et al., 2024, Abram et al., 3 Aug 2025).

Several open directions are explicitly identified. Beyond the interval case, one may ask for a full classification of hypergraphs H\mathbb H27 for which H\mathbb H28 is semidistributive, congruence-uniform, or distributive. A second question is which hypergraphic posets arise as lattice quotients of weak order outside the interval case. A third concerns the geometry of H\mathbb H29: characterizing those hypergraphic polytopes that are “nice” generalized permutahedra with lattice H\mathbb H30-skeletons (Bergeron et al., 2024).

Taken together, these results place the hypergraphic poset at the intersection of generalized permutahedra, acyclic orientation theory, weak-order quotients, and lattice completions. The interval and cyclic-interval classifications provide precise test cases, while the source characterization for arbitrary hypergraphs suggests that the general theory is governed by the combinatorics of allowable source-sequences rather than by the geometry alone (Gélinas, 21 Aug 2025, Gélinas et al., 5 May 2026).

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