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4th-Order Adjacency Tensor

Updated 16 February 2026
  • 4th-Order Adjacency Tensor is a symmetric representation that captures complex 4-adic interactions in hypergraphs and hb-graphs.
  • It utilizes null vertices and normalization techniques to standardize non-uniform edge sizes and incorporate vertex multiplicities.
  • The tensor underpins advanced spectral analysis and scalable algorithms using methods like tensor-times-same-vector for efficient computation.

A 4th-order adjacency tensor is a symmetric tensorial representation that encodes the multiway structure of 4-adic interactions in hypergraphs, non-uniform hypergraphs, and generalized objects such as hyperbag-graphs (hb-graphs, i.e., hypergraphs with multiset edges). The 4th-order adjacency tensor construction is central for advancing spectral theory and higher-order network analysis, supporting both theoretical and computational approaches for systems with complex multiway relationships.

1. Notions of Adjacency in Higher-Order Structures

Adjacency in classical graphs is a binary relationship, naturally represented by a 2nd-order matrix. For hypergraphs—where edges can join any subset of the vertex set—adjacency must generalize to higher-order relations:

  • k-adjacency: A tuple of kk (not necessarily distinct) vertices is k-adjacent if it is contained in a hyperedge of size at least kk.
  • e-adjacency: For each edge (hyperedge) ee, all vertices within ee are e-adjacent; this captures the simultaneous co-membership structure central to hypergraph data.

For non-uniform hypergraphs, where edge sizes vary, pairwise matrices fail to capture the intrinsic higher-order connectivity; an order-rr tensor, with rr being the maximal hyperedge cardinality, is required for a lossless representation (Ouvrard et al., 2017, Ouvrard et al., 2018).

2. Construction of the 4th-Order Adjacency Tensor

Explicit constructions vary according to the type of structure—simple hypergraph, non-uniform hypergraph, or hb-graph. The construction outlined below follows the most general approach based on (Ouvrard et al., 2018), with cross-references to (Aksoy et al., 2023, Ouvrard et al., 2017), and (Ouvrard et al., 2018).

a) General Definition for hb-graphs (Natural Multisets)

Let H=(V,E)H = (V, E) with V={v1,…,vn}V = \{v_1, \dots, v_n\} and each e∈Ee \in E a multiset, i.e., me:V→Nm_e : V \rightarrow \mathbb{N} records vertex multiplicities. Set kk0, the maximum multiset cardinality of any edge.

  • For each kk1 of size kk2, introduce a "null" vertex kk3 of multiplicity kk4.
  • The extended multiset kk5 consists of the elements of kk6, plus kk7 copies of kk8.
  • The tensor kk9 has dimension ee0, symmetrized in all indices:

ee1

where ee2, and ee3 is nonzero only when the indices match the extended multiset ee4:

ee5

b) Specialization to ee6 (Order 4)

Set ee7; introduce null vertices ee8, ee9, ee0. For ee1 of size ee2:

  • ee3
  • ee4
  • Nonzero values:

ee5

if the index multiset is given by the multiplicities ee6 for ee7 and ee8 entries equal to ee9 (location of rr0) (Ouvrard et al., 2018).

An entry is nonzero if and only if, for some rr1 of size rr2, rr3 of the indices equal rr4 for rr5 and rr6 of the indices equal rr7.

c) Uniform Hypergraphs

If the hypergraph is 4-uniform (every edge has size exactly 4), no null vertices are needed, and the tensor reduces to rr8:

rr9

with full permutation symmetry in all indices (Pearson et al., 2012).

3. Key Properties

  • Permutation symmetry: rr0 is invariant under any permutation of indices.
  • Degree normalization: The m-degree of vertex rr1, denoted rr2 (i.e., the sum of its multiplicities), is recovered by summing rr3 over the last three indices:

rr4

  • Handling duplicates: Multiplicities rr5 in multiset edges contribute factorial weights, such as rr6 in the numerator.
  • Edge encoding: The specific "null" vertex associated to edge size rr7 ensures that edges of different cardinalities are uniquely identified in the tensor structure (Ouvrard et al., 2018, Ouvrard et al., 2017, Ouvrard et al., 2018).

4. Concrete Examples

Given rr8 (rr9) and edges: H=(V,E)H = (V, E)0 (H=(V,E)H = (V, E)1), H=(V,E)H = (V, E)2 (H=(V,E)H = (V, E)3), H=(V,E)H = (V, E)4 (H=(V,E)H = (V, E)5). The tensor H=(V,E)H = (V, E)6 (of dimension 6) includes, for instance:

  • For H=(V,E)H = (V, E)7: H=(V,E)H = (V, E)8, H=(V,E)H = (V, E)9. Each of the 12 tuples matching two V={v1,…,vn}V = \{v_1, \dots, v_n\}0, one V={v1,…,vn}V = \{v_1, \dots, v_n\}1, and one V={v1,…,vn}V = \{v_1, \dots, v_n\}2 is assigned V={v1,…,vn}V = \{v_1, \dots, v_n\}3-value V={v1,…,vn}V = \{v_1, \dots, v_n\}4.
  • For V={v1,…,vn}V = \{v_1, \dots, v_n\}5 (V={v1,…,vn}V = \{v_1, \dots, v_n\}6): pattern V={v1,…,vn}V = \{v_1, \dots, v_n\}7, with each tuple receiving V={v1,…,vn}V = \{v_1, \dots, v_n\}8-value V={v1,…,vn}V = \{v_1, \dots, v_n\}9.

For e∈Ee \in E0 and e∈Ee \in E1: Each permutation of e∈Ee \in E2 indexes yields e∈Ee \in E3; all other entries vanish.

c) General Hypergraph via Polynomial Homogeneization

The construction via homogeneous polynomials or the hypergraph uniformisation process leads to a tensor of dimension e∈Ee \in E4 (for order 4), assigning e∈Ee \in E5 to each valid pattern obtained by augmenting an edge of size e∈Ee \in E6 with e∈Ee \in E7 auxiliary indices; all other entries are zero (Ouvrard et al., 2017, Ouvrard et al., 2018).

5. Spectral Theory

The spectral theory of the 4th-order adjacency tensor underpins higher-order generalizations of eigenvalues and centralities:

  • H-eigenvalues:

e∈Ee \in E8

The set of real H-eigenvalues is finite; if the hypergraph is connected, the spectral radius e∈Ee \in E9 is attained at a unique positive eigenvector (up to scaling) (Pearson et al., 2012).

  • Z-eigenvalues:

me:V→Nm_e : V \rightarrow \mathbb{N}0

The largest Z-eigenvalue me:V→Nm_e : V \rightarrow \mathbb{N}1 has an associated nonnegative unit-norm eigenvector; strict positivity is guaranteed under additional "nice" connectivity (Pearson et al., 2012).

  • E-eigenvalues:

me:V→Nm_e : V \rightarrow \mathbb{N}2

For 4-partite 4-graphs, the E-spectrum is symmetric about zero.

A Gershgorin-type bound applies for me:V→Nm_e : V \rightarrow \mathbb{N}3 symmetric and degree-normalized:

me:V→Nm_e : V \rightarrow \mathbb{N}4

where me:V→Nm_e : V \rightarrow \mathbb{N}5 is the maximum vertex m-degree, and me:V→Nm_e : V \rightarrow \mathbb{N}6 is the maximum m-degree over null indices (Ouvrard et al., 2018). In the 4-uniform case, this reduces to me:V→Nm_e : V \rightarrow \mathbb{N}7 (Ouvrard et al., 2017).

6. Computational and Algorithmic Aspects

Direct formation of the me:V→Nm_e : V \rightarrow \mathbb{N}8-size adjacency tensor is typically avoided in practice for large me:V→Nm_e : V \rightarrow \mathbb{N}9. Recent developments, e.g., tensor-times-same-vector (TTSV) methods, achieve efficient computation (kk00 time), central for centrality and clustering algorithms:

  • For vector kk01, kk02 is computed without explicit tensor storage (Aksoy et al., 2023).
  • The tensor is formally kk03-dimensional but only nonzero on patterns prescribed by the edge structure and the normalization scheme.

TTSV algorithms enable the use of 4th-order adjacency tensors in scalable hypergraph data analysis, extracting higher-order structure inaccessible to matrix-based approaches (Aksoy et al., 2023).

7. Connections and Generalizations

The 4th-order adjacency tensor is encapsulated by multiple frameworks:

  • Hypergraph uniformization and polynomial homogeneization (Ouvrard et al., 2017, Ouvrard et al., 2018): Orders non-uniform edges by introducing auxiliary vertices, producing a homogeneous symmetric tensor encoding all hyperedge layers in a single structure.
  • hb-graphs and multisets (Ouvrard et al., 2018): Accommodates multiedges with multiplicity, requiring careful normalization and null-vertex bookkeeping.
  • Stirling number–based weighting (Aksoy et al., 2023): Equidistributes edge-weight over all index patterns representing full coverage of edge vertices, crucial for algorithms exploiting multilinear spectral theory.

All approaches converge on the core requirement: a fully symmetric, degree-normalized, combinatorially faithful encoding of 4-adic adjacency, serving as a canonical representation for higher-order spectral, algebraic, and algorithmic analyses in hypergraph-based models.

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