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Complementary Edge Ideal in Graph-Theoretic Algebra

Updated 8 July 2026
  • Complementary edge ideal is a squarefree monomial ideal associated with a graph, where each generator is the product of all variables except two corresponding to an edge.
  • It bridges graph theory and commutative algebra by linking duality principles with classifications such as Cohen–Macaulay, Gorenstein, and sequentially Cohen–Macaulay properties.
  • Studies of its powers, minimal resolutions, and Rees algebras reveal precise regularity patterns, linearity conditions, and persistence behaviors influenced by specific graph structures.

to=arxiv_search 大发快三开奖 天天中彩票不中返json {"query":"\"complementary edge ideal\" arXiv", "max_results": 10, "sort_by": "submittedDate"}ถวายสัตย์ฯ A complementary edge ideal is, in current graph-theoretic commutative algebra, the squarefree monomial ideal

Ic(G)  =  (x1x2xnxixj  :  {i,j}E(G))K[x1,,xn]I_c(G)\;=\;\Bigl(\,\frac{x_1x_2\cdots x_n}{x_i\,x_j}\;:\;\{i,j\}\in E(G)\Bigr)\subset K[x_1,\dots,x_n]

attached to a finite simple graph GG on [n][n]. Its generators all have degree n2n-2, and every squarefree monomial ideal generated in degree n2n-2 arises in this form for a suitable graph (Ficarra et al., 14 Aug 2025). A nearby, but distinct, usage appears for a $1$-dimensional flag simplicial complex Δ\Delta, where the Stanley–Reisner ideal

IΔ=(xixj:{i,j}Δ)=I((Δ)c)I_\Delta=(x_i x_j:\{i,j\}\notin \Delta)=I((\Delta)^c)

is described as the complementary edge ideal of Δ\Delta because it is the edge ideal of the graph-theoretic complement of Δ\Delta (Navarra et al., 1 Jul 2026). The modern literature develops both usages, with the GG0-generated ideal GG1 serving as the central object in a broad classification program.

1. Definition, realization, and duality

For a graph GG2 with vertex set GG3, the complementary edge ideal GG4 is generated by the squarefree monomials whose support is the complement of one edge of GG5. If GG6 has an isolated vertex GG7, then GG8 does not divide any generator, and one has

GG9

directly from the definition (Ficarra, 2 Mar 2026).

A fundamental realization theorem states that every squarefree monomial ideal generated in degree [n][n]0 is a complementary edge ideal. Concretely, if

[n][n]1

then each [n][n]2 has the form [n][n]3 for a unique pair [n][n]4, hence [n][n]5 for the graph whose edges are those pairs (Ficarra et al., 14 Aug 2025). This gives a graph-theoretic model for the entire class of squarefree degree-[n][n]6 ideals.

The construction is closely tied to Alexander duality. One formulation identifies [n][n]7 with the Alexander dual of the usual edge ideal of the complement graph [n][n]8, up to the obvious identification of variables (Ficarra, 2 Mar 2026). A more explicit description writes

[n][n]9

where n2n-20 is the clique complex of n2n-21 and n2n-22 is its pure n2n-23-skeleton (Hibi et al., 13 Aug 2025). This dual viewpoint underlies the Cohen–Macaulay, sequentially Cohen–Macaulay, and linearity criteria proved for n2n-24.

2. Basic structural classifications

The algebraic properties of n2n-25 are governed by explicit graph classes. When n2n-26 has no isolated vertices, the principal classifications are as follows.

Property of n2n-27 Graph-theoretic characterization
Sequentially Cohen–Macaulay n2n-28 is chordal
Cohen–Macaulay n2n-29 is a forest or a complete graph
Gorenstein n2n-20
Matroidal n2n-21 is a complete multipartite graph

These equivalences are established in the recent systematic treatment of complementary edge ideals (Ficarra et al., 14 Aug 2025). The matroidal criterion is also equivalent to n2n-22 being n2n-23-free, or equivalently a disjoint union of cliques (Ficarra et al., 14 Aug 2025).

A finer nearly Gorenstein classification is also available. Under the no-isolated-vertices hypothesis, n2n-24 is nearly Gorenstein exactly when

n2n-25

with the first two cases nearly Gorenstein but not Gorenstein, and the last four Gorenstein (Ficarra et al., 14 Aug 2025).

Linearity properties for the ideal itself admit a particularly sharp criterion. One treatment proves that n2n-26 has a linear resolution if and only if it has linear quotients if and only if it is linearly related if and only if n2n-27 is connected (Hibi et al., 13 Aug 2025). The same source shows that n2n-28 has a pure minimal free resolution if and only if n2n-29 is connected or a disjoint union of edges, and that $1$0 is level if and only if $1$1 is complete, or a tree, or a disjoint union of edges (Hibi et al., 13 Aug 2025).

The minimal-prime structure is also described combinatorially. One statement gives

$1$2

so the minimal primes are indexed by induced triangles or induced pairs of nonadjacent vertices (Hibi et al., 13 Aug 2025). Correspondingly, $1$3 is unmixed if and only if $1$4 is complete or triangle-free (Hibi et al., 13 Aug 2025).

For the minimal free resolution of $1$5 itself, the only nonzero graded Betti numbers occur in bidegrees

$1$6

and one has

$1$7

for the base ideal $1$8 (Hibi et al., 13 Aug 2025).

3. Powers, regularity, associated primes, and the $1$9-function

The powers of a complementary edge ideal exhibit a rigid piecewise-linear regularity pattern. If Δ\Delta0 denotes the number of connected components of Δ\Delta1 of size Δ\Delta2, then for every Δ\Delta3,

Δ\Delta4

Moreover, the depth function Δ\Delta5 is non-increasing (Ficarra et al., 14 Aug 2025). The same large-degree framework shows more generally that if a squarefree monomial ideal is generated in degrees Δ\Delta6, then its depth stabilizes by Δ\Delta7, and for complementary edge ideals the Betti numbers of Δ\Delta8 depend only on the combinatorics of Δ\Delta9 and not on the base field IΔ=(xixj:{i,j}Δ)=I((Δ)c)I_\Delta=(x_i x_j:\{i,j\}\notin \Delta)=I((\Delta)^c)0 (Ficarra, 2 Mar 2026).

The criterion for linear powers is exact. The following are equivalent: IΔ=(xixj:{i,j}Δ)=I((Δ)c)I_\Delta=(x_i x_j:\{i,j\}\notin \Delta)=I((\Delta)^c)1 has a linear resolution for some IΔ=(xixj:{i,j}Δ)=I((Δ)c)I_\Delta=(x_i x_j:\{i,j\}\notin \Delta)=I((\Delta)^c)2; IΔ=(xixj:{i,j}Δ)=I((Δ)c)I_\Delta=(x_i x_j:\{i,j\}\notin \Delta)=I((\Delta)^c)3 has linear quotients for some IΔ=(xixj:{i,j}Δ)=I((Δ)c)I_\Delta=(x_i x_j:\{i,j\}\notin \Delta)=I((\Delta)^c)4; and IΔ=(xixj:{i,j}Δ)=I((Δ)c)I_\Delta=(x_i x_j:\{i,j\}\notin \Delta)=I((\Delta)^c)5. Equivalently, the same holds for all IΔ=(xixj:{i,j}Δ)=I((Δ)c)I_\Delta=(x_i x_j:\{i,j\}\notin \Delta)=I((\Delta)^c)6 (Ficarra et al., 14 Aug 2025). Thus a connected graph of size at least IΔ=(xixj:{i,j}Δ)=I((Δ)c)I_\Delta=(x_i x_j:\{i,j\}\notin \Delta)=I((\Delta)^c)7 has linear quotients in every power, whereas disconnectedness among nontrivial components forces failure of linearity in higher powers.

The associated primes of all powers are explicitly determined. Writing

IΔ=(xixj:{i,j}Δ)=I((Δ)c)I_\Delta=(x_i x_j:\{i,j\}\notin \Delta)=I((\Delta)^c)8

one has for every IΔ=(xixj:{i,j}Δ)=I((Δ)c)I_\Delta=(x_i x_j:\{i,j\}\notin \Delta)=I((\Delta)^c)9,

Δ\Delta0

and each such Δ\Delta1 appears already for all powers Δ\Delta2 (Ficarra, 2 Mar 2026). In particular, complementary edge ideals satisfy the persistence property: Δ\Delta3 for Δ\Delta4 (Ficarra, 2 Mar 2026).

The Δ\Delta5-function is equally explicit. If Δ\Delta6, then for every Δ\Delta7,

Δ\Delta8

and in all cases

Δ\Delta9

If Δ\Delta0 has linear powers, then Δ\Delta1 for all Δ\Delta2 (Ficarra, 2 Mar 2026). The cycle Δ\Delta3 provides a concrete model: Δ\Delta4 for every Δ\Delta5, while

Δ\Delta6

(Ficarra, 2 Mar 2026).

4. Rees algebras, fiber cones, and depth stability

The Rees algebra

Δ\Delta7

admits a combinatorial description through the defining ideal Δ\Delta8, where Δ\Delta9 and GG00 for the complementary edge generators GG01. A structural theorem states that every primitive binomial in GG02 can be chosen so as to have GG03-degree at most GG04. Equivalently, GG05 has a Gröbner basis consisting of binomials

GG06

with GG07 of degree at most GG08 (Ficarra et al., 22 Sep 2025).

This immediately yields bounds on the GG09-regularity: GG10 while asymptotic regularity gives the lower bound

GG11

(Ficarra et al., 22 Sep 2025). The same paper proves large normality and Cohen–Macaulayness results: if GG12 is bipartite, or if GG13 is connected unicyclic, then GG14 is a normal Cohen–Macaulay domain (Ficarra et al., 22 Sep 2025).

Koszulness is known in two further cases. If GG15 is a tree, then GG16 has a quadratic Gröbner basis and GG17 is Koszul. The same holds for a connected unicyclic graph whose unique cycle has length GG18 or GG19 (Ficarra et al., 22 Sep 2025). The fiber cone GG20 is normal exactly when GG21 satisfies the odd-cycle condition (Ficarra et al., 22 Sep 2025).

Asymptotic depth is controlled by the number GG22 of bipartite connected components of GG23, with isolated vertices counted as bipartite components. The analytic spread is

GG24

and the limit depth formula is

GG25

(Ficarra et al., 22 Sep 2025). The index of depth stability satisfies

GG26

and equality holds for path graphs. More precisely, if GG27, then

GG28

so GG29 (Ficarra et al., 22 Sep 2025).

5. Licci behavior, random graphs, and homological shifts

The liaison-theoretic classification is especially rigid. Localizing at the homogeneous maximal ideal GG30, one has: GG31 (Lama, 17 Mar 2026). The proof combines the Cohen–Macaulay criterion GG32 Cohen–Macaulay GG33 GG34 is a forest or a complete graph with the Huneke–Ulrich numerical obstruction for licci ideals; among complete graphs, only GG35 survives (Lama, 17 Mar 2026).

This licci criterion ties directly to standard homological invariants. If GG36 is licci and GG37 is a connected forest, then GG38 and GG39. If GG40 is a disconnected forest, then GG41 and GG42 (Lama, 17 Mar 2026). The random-graph consequence is asymptotic: for the Erdős–Rényi graph GG43,

GG44

This follows from the equivalence between non-licci behavior and the presence of a cycle of length GG45 (Lama, 17 Mar 2026).

A separate homological line studies powers via homological shift ideals and algebras. For a monomial ideal GG46, the GG47-th homological shift ideal GG48 is generated by the multidegrees appearing in the GG49-th free module of a minimal multigraded free resolution. For complementary edge ideals of trees and cycles, this structure can be computed explicitly (Lu et al., 17 Nov 2025).

Projective dimension of powers is particularly transparent in several families. If GG50 is a connected bipartite graph on GG51 vertices, then

GG52

and thereafter GG53 (Lu et al., 17 Nov 2025). For a tree on GG54 vertices,

GG55

For an even cycle of length GG56,

GG57

while for an odd cycle of length GG58,

GG59

These formulas show that powers of GG60 can have large projective dimension even when the base ideal has GG61 (Lu et al., 17 Nov 2025).

For trees, the homological shift algebras are especially structured: GG62 is generated in degree GG63, and GG64, after dividing by a suitable monomial, is exactly a Veronese-type ideal. Conversely, every Veronese-type ideal arises in this way from a caterpillar tree (Lu et al., 17 Nov 2025).

6. The GG65-dimensional flag-complex usage and squarefree powers

In the simplicial-complex literature, a GG66-dimensional flag simplicial complex GG67 is exactly a graph with no triangles, and its Stanley–Reisner ideal is

GG68

In this setting GG69 is often called the complementary edge ideal of GG70 because it is the edge ideal of the complement graph of GG71 (Navarra et al., 1 Jul 2026). This usage differs from the GG72-generated ideal GG73, but it is algebraically adjacent: both are squarefree monomial ideals controlled by forbidden induced subgraphs.

For an arbitrary graph GG74, the GG75-th squarefree power

GG76

encodes matchings of size GG77. The central linearity theorem states that for GG78,

GG79

which is disconnected and satisfies GG80 (Navarra et al., 1 Jul 2026).

Transferred to a GG81-dimensional flag complex GG82, this becomes a forbidden-subgraph criterion: GG83 (Navarra et al., 1 Jul 2026). The Betti table then has a highly constrained form. There is always a linear strand in bidegrees GG84. If GG85 contains an induced even-bipartite GG86 with GG87 even, then

GG88

indeed

GG89

and no other nonzero extra Betti numbers occur (Navarra et al., 1 Jul 2026).

If GG90 contains no such even complete bipartite graph but does contain a crown graph GG91, then all first syzygies remain linear, GG92, but nonlinearity first appears at

GG93

(Navarra et al., 1 Jul 2026). Consequently,

GG94

nor any induced crown graph GG95 (Navarra et al., 1 Jul 2026).

The model examples isolate the two obstruction types. If GG96, then GG97 has GG98, coming from the unique induced GG99. If [n][n]00, then [n][n]01 is linearly related but not linearly resolved, with first failure at [n][n]02 (Navarra et al., 1 Jul 2026). These examples complete the combinatorial picture of the complementary-edge-ideal terminology in the triangle-free setting.

The two strands of the subject therefore share a common pattern: a squarefree monomial ideal attached to complementary graph data, with homological behavior governed by induced subgraphs, duality, and explicit graph classes. In the [n][n]03-generated theory this leads to classifications of Cohen–Macaulayness, Gorensteinness, licci behavior, Rees algebras, and asymptotic invariants; in the [n][n]04-dimensional flag-complex theory it leads to exact forbidden-subgraph criteria for linear relations and linear resolutions of squarefree powers.

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