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Poset of Regions in Hyperplane Arrangements

Updated 6 July 2026
  • Poset of Regions is a partial order defined on the chambers of a hyperplane arrangement by comparing the hyperplanes that separate them from a fixed base region.
  • It structures arrangement theory by yielding graded orders, establishing canonical links to acyclic orientations and embedding into complete ortholattices via Dedekind–MacNeille completions.
  • Applications extend to graphic, Shi, and toric arrangements, providing concrete models that connect combinatorial properties with geometric and lattice-theoretic frameworks.

Searching arXiv for papers on posets of regions, hyperplane arrangements, and related completions. The poset of regions is the partial order obtained from a hyperplane arrangement after choosing a base region and comparing regions by inclusion of the hyperplanes that separate them from that base. In arrangement theory this construction organizes chambers of real arrangements, yields canonical graded orders such as the weak order for the braid arrangement, and, for central arrangements, admits a Dedekind–MacNeille completion described by lattices of regular closed sets. Related work also uses specialized posets to encode regions of Shi arrangements inside fixed Coxeter cones, and develops toric analogues in which regions correspond not to single acyclic orientations but to source-to-sink flip classes (Develin et al., 2012, Santocanale et al., 2013, Meszaros, 2011).

1. Base-region order in ordinary hyperplane arrangements

For a finite hyperplane arrangement H⊂Rn\mathcal{H}\subset \mathbb{R}^n, a region is a connected component of

Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.

If a base region R0R_0 is fixed, the separation set Sep(R,R0)\mathrm{Sep}(R,R_0) consists of the hyperplanes of H\mathcal{H} that separate RR from R0R_0. The poset of regions PR(A,R0)PR(\mathcal{A},R_0) is then defined by

R≤R′ifSep(R,R0)⊆Sep(R′,R0),R\le R' \quad \text{if} \quad \mathrm{Sep}(R,R_0)\subseteq \mathrm{Sep}(R',R_0),

with cover relations R⋅ ⁣ ⁣ ⁣<R′R\mathbin{\cdot\!\!\!<}R' when Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.0 and Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.1 are adjacent and Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.2 for a single hyperplane Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.3. This order is graded by

Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.4

In the central case considered for arrangements Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.5 in Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.6, one writes Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.7 for the set of regions and, after choosing a base region Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.8, defines

Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.9

and

R0R_00

The resulting ordered set is denoted R0R_01 (Develin et al., 2012, Santocanale et al., 2013).

For graphic arrangements this order has a standard combinatorial model. If R0R_02 is a finite simple graph, the graphic hyperplane arrangement is

R0R_03

A point R0R_04 in the complement determines an acyclic orientation R0R_05 by directing R0R_06 as R0R_07 if R0R_08. This gives a bijection between chambers and acyclic orientations, and Greene–Zaslavsky and Stanley showed that

R0R_09

where Sep(R,R0)\mathrm{Sep}(R,R_0)0 is the Tutte polynomial. For the complete graph Sep(R,R0)\mathrm{Sep}(R,R_0)1, Sep(R,R0)\mathrm{Sep}(R,R_0)2 is the braid arrangement; its regions are indexed by permutations Sep(R,R0)\mathrm{Sep}(R,R_0)3 via

Sep(R,R0)\mathrm{Sep}(R,R_0)4

and Sep(R,R0)\mathrm{Sep}(R,R_0)5 is isomorphic to the right weak order on Sep(R,R0)\mathrm{Sep}(R,R_0)6 (Develin et al., 2012).

2. Central arrangements and Dedekind–MacNeille completion

For a central hyperplane arrangement Sep(R,R0)\mathrm{Sep}(R,R_0)7 in Sep(R,R0)\mathrm{Sep}(R,R_0)8, the poset Sep(R,R0)\mathrm{Sep}(R,R_0)9 admits a completion described in terms of closure spaces. A closure operator on a set H\mathcal{H}0 is an extensive, idempotent, isotone map H\mathcal{H}1 with H\mathcal{H}2. Its associated kernel operator is

H\mathcal{H}3

A subset H\mathcal{H}4 is closed if H\mathcal{H}5, open if H\mathcal{H}6, regular closed if H\mathcal{H}7, regular open if H\mathcal{H}8, and clopen if it is simultaneously closed and open. The regular closed subsets form the complete lattice H\mathcal{H}9, and a subset is regular closed iff it is the closure of some open set. The orthogonal operation

RR0

defines an orthocomplementation of RR1, so RR2 is an ortholattice (Santocanale et al., 2013).

In the arrangement-theoretic application, one chooses, for each RR3, a vector RR4 on the same side of RR5 as the base region RR6, normalized by RR7 for a fixed RR8. With

RR9

and for a region R0R_00,

R0R_01

the assignment R0R_02 is an order-isomorphism from R0R_03 onto the set R0R_04 of strongly bi-convex subsets of R0R_05, namely those R0R_06 such that R0R_07. Here R0R_08 is the relative convex hull operator on R0R_09, and PR(A,R0)PR(\mathcal{A},R_0)0 is an atomistic convex geometry.

The decisive structural statement is Theorem 6.7: PR(A,R0)PR(\mathcal{A},R_0)1 is the Dedekind–MacNeille completion of PR(A,R0)PR(\mathcal{A},R_0)2 via the embedding PR(A,R0)PR(\mathcal{A},R_0)3. Because finite convex geometries yield pseudocomplemented lattices of regular closed sets, the Dedekind–MacNeille completion of PR(A,R0)PR(\mathcal{A},R_0)4 is pseudocomplemented. Thus the ordinary poset of regions of a central arrangement sits canonically inside a complete ortholattice with an explicitly defined orthocomplementation and with pseudocomplementation guaranteed by convex-geometric finiteness (Santocanale et al., 2013).

3. Shi arrangements and local posets encoding regions

In the study of Shi arrangements, the phrase “poset of regions” must be distinguished from a different construction that encodes regions inside a fixed Coxeter cone by antichains. For type PR(A,R0)PR(\mathcal{A},R_0)5, the Coxeter arrangement is

PR(A,R0)PR(\mathcal{A},R_0)6

with dominant cone

PR(A,R0)PR(\mathcal{A},R_0)7

and cones PR(A,R0)PR(\mathcal{A},R_0)8 indexed by permutations PR(A,R0)PR(\mathcal{A},R_0)9. The Shi arrangement used there is

R≤R′ifSep(R,R0)⊆Sep(R′,R0),R\le R' \quad \text{if} \quad \mathrm{Sep}(R,R_0)\subseteq \mathrm{Sep}(R',R_0),0

whose number of regions is

R≤R′ifSep(R,R0)⊆Sep(R′,R0),R\le R' \quad \text{if} \quad \mathrm{Sep}(R,R_0)\subseteq \mathrm{Sep}(R',R_0),1

For R≤R′ifSep(R,R0)⊆Sep(R′,R0),R\le R' \quad \text{if} \quad \mathrm{Sep}(R,R_0)\subseteq \mathrm{Sep}(R',R_0),2, the relevant poset is

R≤R′ifSep(R,R0)⊆Sep(R′,R0),R\le R' \quad \text{if} \quad \mathrm{Sep}(R,R_0)\subseteq \mathrm{Sep}(R',R_0),3

ordered by

R≤R′ifSep(R,R0)⊆Sep(R′,R0),R\le R' \quad \text{if} \quad \mathrm{Sep}(R,R_0)\subseteq \mathrm{Sep}(R',R_0),4

Antichains in R≤R′ifSep(R,R0)⊆Sep(R′,R0),R\le R' \quad \text{if} \quad \mathrm{Sep}(R,R_0)\subseteq \mathrm{Sep}(R',R_0),5 are exactly the sets of ceilings, equivalently floors, of regions of R≤R′ifSep(R,R0)⊆Sep(R′,R0),R\le R' \quad \text{if} \quad \mathrm{Sep}(R,R_0)\subseteq \mathrm{Sep}(R',R_0),6 contained in R≤R′ifSep(R,R0)⊆Sep(R′,R0),R\le R' \quad \text{if} \quad \mathrm{Sep}(R,R_0)\subseteq \mathrm{Sep}(R',R_0),7. Consequently,

R≤R′ifSep(R,R0)⊆Sep(R′,R0),R\le R' \quad \text{if} \quad \mathrm{Sep}(R,R_0)\subseteq \mathrm{Sep}(R',R_0),8

where R≤R′ifSep(R,R0)⊆Sep(R′,R0),R\le R' \quad \text{if} \quad \mathrm{Sep}(R,R_0)\subseteq \mathrm{Sep}(R',R_0),9 is the number of antichains of R⋅ ⁣ ⁣ ⁣<R′R\mathbin{\cdot\!\!\!<}R'0 (Meszaros, 2011).

The same pattern persists in type R⋅ ⁣ ⁣ ⁣<R′R\mathbin{\cdot\!\!\!<}R'1. The type R⋅ ⁣ ⁣ ⁣<R′R\mathbin{\cdot\!\!\!<}R'2 Shi arrangement is

R⋅ ⁣ ⁣ ⁣<R′R\mathbin{\cdot\!\!\!<}R'3

and its number of regions is

R⋅ ⁣ ⁣ ⁣<R′R\mathbin{\cdot\!\!\!<}R'4

For a signed permutation R⋅ ⁣ ⁣ ⁣<R′R\mathbin{\cdot\!\!\!<}R'5, one defines

R⋅ ⁣ ⁣ ⁣<R′R\mathbin{\cdot\!\!\!<}R'6

again with interval order

R⋅ ⁣ ⁣ ⁣<R′R\mathbin{\cdot\!\!\!<}R'7

The regions of R⋅ ⁣ ⁣ ⁣<R′R\mathbin{\cdot\!\!\!<}R'8 lying in R⋅ ⁣ ⁣ ⁣<R′R\mathbin{\cdot\!\!\!<}R'9 are in bijection with the antichains of Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.00, so

Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.01

These local posets support refined bijections. In type Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.02, regions of Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.03 correspond to parking functions; in type Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.04, regions of Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.05 correspond to sequences Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.06 with Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.07. The ceiling and floor statistics satisfy

Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.08

and

Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.09

A standard misconception is that the posets Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.10 and Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.11 are global posets of regions. They are not: they are specialized local encoding devices whose antichains recover the sets of ceilings or floors for regions inside a fixed Coxeter cone (Meszaros, 2011).

4. Graphic arrangements, chamber posets, and toric analogues

In the ordinary graphic setting, every chamber determines an acyclic orientation and hence an ordinary poset. For a chamber Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.12, the associated orientation Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.13 defines a poset Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.14 by taking the transitive closure of the relation “Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.15 precedes Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.16 along a directed path in Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.17.” Chains in Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.18 correspond to coordinate inequalities Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.19 valid on Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.20, the Hasse diagram is obtained by deleting redundant transitive edges, and linear extensions of Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.21 index braid chambers whose union closure equals the closure of Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.22. This is the standard combinatorial content carried by regions of graphic arrangements (Develin et al., 2012).

The toric theory modifies this picture by passing from Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.23 to the torus Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.24. For a graph Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.25, the toric graphic arrangement is

Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.26

A toric chamber is a connected component of the complement. Directing Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.27 by Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.28 when the fractional parts satisfy Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.29 defines a map to Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.30, but unlike the classical case, points in the same toric chamber need not determine the same orientation: moving one coordinate across Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.31 can turn a source into a sink without crossing a toric hyperplane.

This leads to flip equivalence. Two acyclic orientations are equivalent if they differ by a sequence of source-to-sink flips. The main correspondence theorem states that

Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.32

and therefore

Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.33

For Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.34, the toric chambers are indexed by cyclic classes Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.35 of permutations, called toric total orders, and their number is Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.36.

The toric framework develops analogues of chains, transitivity, Hasse diagrams, and total extensions. A toric chain is a subset Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.37 for which there exists a cyclic order Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.38 such that every Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.39 in the toric chamber has some cyclic shift Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.40 with

Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.41

Toric transitive closure adds edges implied by toric directed paths, and this closure operator is convex. The toric Hasse diagram is obtained by removing chord edges from toric directed cycles. The paper does not define a full toric poset-of-regions structure analogous to Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.42; instead it treats chambers, flip classes, toric transitivity, and toric Hasse diagrams as the appropriate toric replacement (Develin et al., 2012).

5. Regular closed lattices, clopen subposets, and extended permutohedra

The lattice-theoretic completion of a poset of regions belongs to a broader theory of closure spaces and regular closed sets. For any closure space Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.43, Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.44 is always a complete lattice. If Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.45 is a family of regular closed sets, then

Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.46

For any closure space Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.47 and any subset Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.48, Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.49 is the Dedekind–MacNeille completion of Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.50 iff every regular closed set is a join of members of Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.51; this occurs, in particular, if every regular open set is a union of members of Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.52 (Santocanale et al., 2013).

A particularly important class is that of closure spaces of semilattice type, where Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.53 is a poset and every minimal covering Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.54 of Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.55 satisfies Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.56. Such closure spaces are atomistic convex geometries. For well-founded closure spaces of semilattice type, Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.57 is tight in Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.58, meaning that the inclusion preserves all existing joins and meets. In the same context, Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.59 is a lattice iff Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.60. The paper also establishes a hierarchy of quasi-identities Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.61 weaker than both meet- and join-semidistributivity, gives a finite semilattice-type example where Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.62 is not semidistributive, and proves that for finite semilattice-type closure spaces,

Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.63

This framework includes two families closely connected with region posets. For a graph Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.64, if Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.65 is the set of all nonempty connected subsets of Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.66 and Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.67 closes under disjoint unions, then

Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.68

is the extended permutohedron on Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.69, while

Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.70

is the permutohedron on Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.71. For a join-semilattice Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.72, the canonical closure operator Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.73 yields Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.74 and Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.75. In the semilattice case, every open subset is a union of clopen sets, Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.76 is generated as a complete ortholattice by the ideals of Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.77, Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.78 is the Dedekind–MacNeille completion of Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.79, and every completely join-irreducible element of Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.80 is clopen. For finite join-semilattices, Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.81 is a bounded homomorphic image of a free lattice (Santocanale et al., 2013).

6. Special cases, failures, and conceptual boundaries

Several boundary phenomena clarify what the poset-of-regions perspective does and does not capture. In the graph setting, Theorem 14.1 gives an exact criterion: Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.82 More generally, if Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.83 is a finite graph and either a block graph or a cycle, then Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.84 is the Dedekind–MacNeille completion of Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.85. This need not hold in general: for Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.86, the extended permutohedron Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.87 is not the Dedekind–MacNeille completion of Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.88. The failure is tied to the existence of completely join-irreducible regular closed sets that are not clopen. The paper also exhibits a minimal regular open neighborhood Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.89 of Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.90 containing no clopen neighborhood of Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.91, showing that for complete graphs Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.92 with Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.93, not every regular open subset is a union of clopen sets (Santocanale et al., 2013).

The toric theory has a different limitation. Although one can formally mimic a base-region order by separation sets of toric hyper-subtori, the torus is not simply connected, orientations vary within a chamber by flips, and the resulting global order need not be graded or a lattice. The toric framework therefore shifts emphasis from a classical poset of regions to the correspondence

Rn∖⋃H∈HH.\mathbb{R}^n\setminus\bigcup_{H\in\mathcal{H}}H.94

together with toric chains, toric total extensions, toric transitive closure, and toric Hasse diagrams. In this sense toric partial orders are an analogue of region posets rather than a direct transplantation of the classical construction (Develin et al., 2012).

Taken together, these results place the poset of regions in a broader structural landscape. In ordinary real arrangements it is a base-region order on chambers; in central arrangements it embeds into a pseudocomplemented ortholattice of regular closed sets; in Shi arrangements it coexists with local interval-order encodings tailored to ceilings and floors; and in the toric setting it is replaced by a chamber theory organized by flip equivalence and cyclic order. This suggests that the enduring role of the poset of regions is not only to order chambers, but also to act as the interface between arrangement geometry and the combinatorics of lattices, orientations, antichains, and completion procedures (Santocanale et al., 2013, Meszaros, 2011).

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