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Deep Particular Partitions in Finite Vector Spaces

Updated 28 November 2025
  • Deep particular partitions are structured partitions of finite vector spaces that produce bent functions with constant Walsh transform magnitude.
  • They enable rigorous analysis of bent and vectorial bent functions by linking partition properties with Hadamard matrix criteria and balanced projections.
  • Key constructions include vectorial dual-bent and twisted Maiorana-McFarland forms, motivating ongoing research into non-WBP bent partitions.

A deep particular partition, commonly termed a "bent partition," is a structured partition of the finite vector space Vn(p)V_n^{(p)} (where nn is an even positive integer and pp is a prime) that underpins the construction of bent functions, vectorial bent functions, partial difference sets, and association schemes. Specifically, a partition Γ={A1,…,AK}\Gamma = \{A_1,\ldots,A_K\} of Vn(p)V_n^{(p)} is called bent if every pp-ary function f:Vn(p)→Fpf:V_n^{(p)} \to \mathbb{F}_p whose preimages match exactly K/pK/p blocks of Γ\Gamma is a bent function, characterized by Walsh transform values of constant magnitude pn/2p^{n/2} for all nn0 (Wang et al., 21 Sep 2025). Bent partitions systematically generalize classical bent and vectorial bent functions by allowing rigorous combinatorial and algebraic characterizations, including Hadamard matrix criteria in the binary case.

1. Definition and Fundamental Properties

Let nn1 denote an nn2-dimensional vector space over nn3 with nn4 even. A bent partition nn5 of nn6 consists of disjoint subsets nn7 covering the space; the depth nn8 refers to the cardinality of the partition. The requisite property is that any nn9-coloring of pp0 assigning each color exactly pp1 times yields a bent pp2-ary function pp3; thus, partition properties and bentness of all induced functions are tightly coupled.

Equivalently, for an index map pp4 (with pp5 and pp6 iff pp7), pp8 is bent if and only if pp9 is vectorial bent and all balanced projections (i.e., any permutation or balanced linear combination of its components) remain bent [(Wang et al., 21 Sep 2025), Theorem 1].

The seminal open problem, originally formulated by Anbar–Meidl (2022), asks whether every bent partition's depth Γ={A1,…,AK}\Gamma = \{A_1,\ldots,A_K\}0 must always be a power of Γ={A1,…,AK}\Gamma = \{A_1,\ldots,A_K\}1. To date, all known constructions satisfy Γ={A1,…,AK}\Gamma = \{A_1,\ldots,A_K\}2 for some integer Γ={A1,…,AK}\Gamma = \{A_1,\ldots,A_K\}3.

2. Regularity, Weak Regularity, and the Depth Problem

A Γ={A1,…,AK}\Gamma = \{A_1,\ldots,A_K\}4-ary bent function Γ={A1,…,AK}\Gamma = \{A_1,\ldots,A_K\}5 is called weakly regular if its Walsh transform has the form Γ={A1,…,AK}\Gamma = \{A_1,\ldots,A_K\}6 for each Γ={A1,…,AK}\Gamma = \{A_1,\ldots,A_K\}7, with Γ={A1,…,AK}\Gamma = \{A_1,\ldots,A_K\}8 and Γ={A1,…,AK}\Gamma = \{A_1,\ldots,A_K\}9 the dual. If Vn(p)V_n^{(p)}0, Vn(p)V_n^{(p)}1 is regular; otherwise, it is only weakly regular. A bent partition is said to be in class "WBP" (Editor's term: Weakly/Regular Bent Partition) if all bent functions generated by it are either all regular or all weakly regular, but not a mixture (Wang et al., 21 Sep 2025).

The depth–power–of–Vn(p)V_n^{(p)}2 theorem asserts that for any WBP-class partition Vn(p)V_n^{(p)}3 of Vn(p)V_n^{(p)}4, the depth Vn(p)V_n^{(p)}5 must be a power of Vn(p)V_n^{(p)}6 [(Wang et al., 21 Sep 2025), Theorem 3]. This result conclusively determines the depth for a large class of bent partitions, and in particular ensures that every Boolean (Vn(p)V_n^{(p)}7) bent partition has depth a power of Vn(p)V_n^{(p)}8.

3. Structure Theorems and Proof Outline

The proof of the depth–power–of–Vn(p)V_n^{(p)}9 result for WBP-class partitions relies on algebraic characterizations of weakly regular bent functions and the analysis of their duals. The dual pp0 of a pp1-ary bent function is constrained by the "c-form" functional identity:

pp2

This identity yields strong structural constraints on the algebraic form of pp3 and character sums pp4, where pp5 are the blocks of the partition determined by pp6 [(Wang et al., 21 Sep 2025), Theorem 2].

Specifically, for each pp7,

pp8

where pp9 and f:Vn(p)→Fpf:V_n^{(p)} \to \mathbb{F}_p0 are certain maps determined by f:Vn(p)→Fpf:V_n^{(p)} \to \mathbb{F}_p1 and its dual. Analyzing the range and integrality of these sums constrains f:Vn(p)→Fpf:V_n^{(p)} \to \mathbb{F}_p2 to divide f:Vn(p)→Fpf:V_n^{(p)} \to \mathbb{F}_p3, which, when true for all block unions, mandates f:Vn(p)→Fpf:V_n^{(p)} \to \mathbb{F}_p4 be a power of f:Vn(p)→Fpf:V_n^{(p)} \to \mathbb{F}_p5.

4. Constructions: Dual-Bent, Non-Dual-Bent, and Secondary Operations

Two principal construction paradigms for bent partitions are established: those arising from vectorial dual-bent functions and those not directly corresponding to dual-bent maps.

Vectorial Dual-Bent-Based Partitions

Suppose f:Vn(p)→Fpf:V_n^{(p)} \to \mathbb{F}_p6 is vectorial bent, with all scalar components f:Vn(p)→Fpf:V_n^{(p)} \to \mathbb{F}_p7 weakly regular and of the same duality sign f:Vn(p)→Fpf:V_n^{(p)} \to \mathbb{F}_p8. If one can find maps f:Vn(p)→Fpf:V_n^{(p)} \to \mathbb{F}_p9 and K/pK/p0 such that for K/pK/p1

K/pK/p2

then the preimage partition K/pK/p3 is bent of class WBP [(Wang et al., 21 Sep 2025), Theorem 4].

This property is fully expressible in terms of generalized Hadamard matrices K/pK/p4: all such matrices must be of weakly-regular type and the mixed products K/pK/p5 must be equal for all K/pK/p6.

Non-Dual-Bent Constructions and Twisted Maiorana-McFarland Forms

For certain vectorial bent K/pK/p7, if all K/pK/p8 are regular (or all weakly regular) and, for K/pK/p9, the functions Γ\Gamma0 are all equal to a nonzero Γ\Gamma1, then the blocks Γ\Gamma2(i) form a bent partition not arising from any dual-bent Γ\Gamma3 [(Wang et al., 21 Sep 2025), Corollary 1].

Infinite families can be constructed using "twisted Maiorana-McFarland" forms:

Γ\Gamma4

with compatible homogeneity and further conditions, yielding partitions beyond the dual-bent scope [(Wang et al., 21 Sep 2025), Proposition 3]. Additional secondary constructions combine smaller building blocks Γ\Gamma5 or pairs Γ\Gamma6 to form larger vectorial bent functions Γ\Gamma7 fulfilling the sufficient condition above.

Table: Construction Types and Core Properties

Construction Type Conditions Key Property
Vectorial dual-bent (⋆ holds, Γ\Gamma8) Γ\Gamma9 dual-bent, balanced pn/2p^{n/2}0 WBP, pn/2p^{n/2}1, Hadamard structure
Non-dual-bent, "twisted" pn/2p^{n/2}2 in (⋆), twisted forms WBP (not dual-bent), pn/2p^{n/2}3
Secondary constructions Gluing pn/2p^{n/2}4, pn/2p^{n/2}5; balanced bilinear pn/2p^{n/2}6 Combinatorial families, flexible depth

5. New Families of Vectorial Dual-Bent Functions

Whenever pn/2p^{n/2}7 in the duality condition, pn/2p^{n/2}8 is a vectorial dual-bent function. New families can be synthesized by combining two dual-bent functions pn/2p^{n/2}9 and nn00 using a balanced bilinear form nn01 on their ranges:

nn02

By carefully ensuring that the nn03 constants associated to nn04 and nn05 have opposite sign, their contributions to the dual vanish, guaranteeing the dual-bent structure of nn06 [(Wang et al., 21 Sep 2025), Theorem 6]. This operation recovers known Boolean vectorial bent forms and yields new exemplars through targeted substitutions for the building blocks.

6. Binary Case and Hadamard Matrix Characterization

For nn07, the bent partition criterion becomes purely combinatorial. Let nn08. Then nn09 is bent if and only if the nn10 matrices

nn11

are real Hadamard matrices and the triple products nn12 are identical for all nn13 [(Wang et al., 21 Sep 2025), Theorem 5]. This implies nn14 must be a power of nn15, aligning with the existence constraint for Hadamard matrices.

7. Open Problems and Future Directions

The depth–power–of–nn16 theorem settles the possible values of nn17 for WBP-class partitions, but the existence and classification of bent partitions outside WBP—those generating a mix of (non-)regular or non-weakly-regular bent functions—remains open. The sufficiency (and possible necessity) of the duality condition nn18 and the Hadamard-matrix criteria provide a practical and conceptual framework for constructing further examples [(Wang et al., 21 Sep 2025), Remark 2].

Secondary construction techniques, such as gluing smaller vectorial bent functions or using complete permutations, suggest broad avenues for systematically generating new families and a potential classification up to isomorphism. The identification and analysis of non-WBP bent partitions represent an active line of research.

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