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Delsarte Duals: Theory in Coding and Geometry

Updated 14 July 2026
  • Delsarte duals are dual constructions that associate primal extremal objects with complementary dual certificates across Euclidean, finite-field, and coding theory settings.
  • They enable the transfer of structural information by linking orthogonality, defect sequences, and linear programming duality to achieve sharp bounds and tiling properties.
  • Applications range from optimizing convex body packings and analyzing rank-metric code distributions to unifying diverse constructs in finite geometry and q-matroid theory.

Searching arXiv for the cited papers to ground the article in current literature. Delsarte duals are dual objects associated with Delsarte-type extremal problems and orthogonality constructions. In current usage, the term includes the dual tempered distributions Φ=δ0+ν\Phi=\delta_0+\nu for the Euclidean Delsarte problem, the trace-orthogonal complement UDU^{\perp_D} and the quotient-model dual UdU^d for Fq\mathbb F_q-subspaces of Fqm\mathbb F_{q^m}-vector spaces, the trace-orthogonal dual CC^\perp of Delsarte rank-metric codes, and dual feasible solutions for higher-order Delsarte linear programs for binary codes (Kolountzakis et al., 11 Oct 2025, Borello et al., 29 Sep 2025, Cruz et al., 2015, Coregliano et al., 8 Jan 2025). Across these settings, duality transfers structural information between primal objects and dual certificates, complements, or quotient constructions.

1. Principal meanings of the term

The literature does not use “Delsarte dual” for a single uniform construction. Instead, the name appears in several technically distinct frameworks.

Setting Primal object Dual object
Euclidean Delsarte problem admissible positive-definite ff on Rd\mathbb R^d tempered distribution Φ=δ0+ν\Phi=\delta_0+\nu
Fq\mathbb F_q-subspaces of UDU^{\perp_D}0 UDU^{\perp_D}1 UDU^{\perp_D}2 and quotient-model dual UDU^{\perp_D}3
Delsarte rank-metric codes UDU^{\perp_D}4 UDU^{\perp_D}5 under UDU^{\perp_D}6
Higher-order Delsarte LPs level-UDU^{\perp_D}7 primal feasible UDU^{\perp_D}8 dual feasible family UDU^{\perp_D}9

In the finite-field settings, duality is induced by nondegenerate bilinear forms and dimension-complement formulas. In the Euclidean and coding-theoretic LP settings, duality is linear-programming duality, where the dual object is a certificate for an extremal bound rather than an orthogonal complement. The recent literature treats these viewpoints in parallel rather than reducing them to a single formalism (Kolountzakis et al., 11 Oct 2025, Borello et al., 29 Sep 2025, Cruz et al., 2015, Coregliano et al., 8 Jan 2025).

2. Euclidean-space Delsarte duality

For an open set UdU^d0 of finite Lebesgue measure, symmetric with respect to the origin and containing UdU^d1, the Euclidean Delsarte primal problem seeks real-valued functions UdU^d2 on UdU^d3 such that UdU^d4, UdU^d5 is even, UdU^d6, UdU^d7 for all UdU^d8, and UdU^d9 for all Fq\mathbb F_q0. The Delsarte constant is

Fq\mathbb F_q1

The same exposition states the universal bound Fq\mathbb F_q2 (Kolountzakis et al., 11 Oct 2025).

The dual variable is a tempered distribution of the form

Fq\mathbb F_q3

where Fq\mathbb F_q4 is a positive Radon measure supported in Fq\mathbb F_q5. Its Fourier transform is again a positive measure,

Fq\mathbb F_q6

The dual Delsarte constant is

Fq\mathbb F_q7

A central point is that weak and strong duality must be proved in the continuous setting. Weak duality gives

Fq\mathbb F_q8

while strong duality sharpens this to

Fq\mathbb F_q9

The proof of strong duality proceeds by embedding the primal feasible region into a convex cone in

Fqm\mathbb F_{q^m}0

and applying a Hahn–Banach separation argument. The same work also proves existence of extremizers for both the primal and dual problems: the primal supremum is attained by a continuous admissible Fqm\mathbb F_{q^m}1, and the dual supremum is attained by some Fqm\mathbb F_{q^m}2.

When Fqm\mathbb F_{q^m}3 and Fqm\mathbb F_{q^m}4 are extremal, one obtains tiling-type complementarity relations. The support of Fqm\mathbb F_{q^m}5 lies in Fqm\mathbb F_{q^m}6, and the support of Fqm\mathbb F_{q^m}7 lies in Fqm\mathbb F_{q^m}8. Consequently,

Fqm\mathbb F_{q^m}9

and also

CC^\perp0

The paper describes this by saying that the primal extremal function and the dual extremal measure “tile” one another by convolution in space and in frequency.

The principal application in the same work concerns convex bodies and packings. For a bounded measurable set CC^\perp1 of positive measure, its essential difference set is

CC^\perp2

The classical Cohn–Elkies argument gives

CC^\perp3

The trivial volume bound CC^\perp4 is recovered by the admissible trial function CC^\perp5. If CC^\perp6 is a convex body that does not tile CC^\perp7 by translations, then

CC^\perp8

The proof uses extremal data for CC^\perp9 to obtain a measure ff0 with

ff1

so ff2 weakly tiles its complement; the argument then invokes the structure theorem of Kolountzakis–Lev–Matolcsi 2023 that a convex body which weakly tiles its complement must tile properly (Kolountzakis et al., 11 Oct 2025).

3. Subspace Delsarte duality, weight, and defect

Let ff3, viewed also as an ff4-space of dimension ff5. Write ff6 for the lattice of ff7-subspaces and ff8 for the lattice of all ff9-subspaces. Fix a nondegenerate Rd\mathbb R^d0-bilinear form Rd\mathbb R^d1, and let Rd\mathbb R^d2. For Rd\mathbb R^d3, the trace-orthogonal Delsarte dual is

Rd\mathbb R^d4

This satisfies

Rd\mathbb R^d5

so Rd\mathbb R^d6 is an order-reversing involution of Rd\mathbb R^d7 (Borello et al., 29 Sep 2025).

The same framework introduces weight and defect relative to a fixed Rd\mathbb R^d8 of Rd\mathbb R^d9-dimension Φ=δ0+ν\Phi=\delta_0+\nu0 with Φ=δ0+ν\Phi=\delta_0+\nu1. For any Φ=δ0+ν\Phi=\delta_0+\nu2,

Φ=δ0+ν\Phi=\delta_0+\nu3

For each Φ=δ0+ν\Phi=\delta_0+\nu4,

Φ=δ0+ν\Phi=\delta_0+\nu5

The sequence Φ=δ0+ν\Phi=\delta_0+\nu6 is nondecreasing, with Φ=δ0+ν\Phi=\delta_0+\nu7 and Φ=δ0+ν\Phi=\delta_0+\nu8. Its positive jumps determine the sequence of maximum nonzero defects

Φ=δ0+ν\Phi=\delta_0+\nu9

A second notion, denoted Fq\mathbb F_q0, is defined in a quotient model originating from the Lunardon–Polverino “translation ovoid” argument. Every Fq\mathbb F_q1 of dimension Fq\mathbb F_q2 with Fq\mathbb F_q3 can be realized as the projection of an Fq\mathbb F_q4-dimensional Fq\mathbb F_q5-subgeometry Fq\mathbb F_q6 onto Fq\mathbb F_q7, where Fq\mathbb F_q8 is an Fq\mathbb F_q9-space disjoint from UDU^{\perp_D}00. If UDU^{\perp_D}01 is the UDU^{\perp_D}02-orthogonal of UDU^{\perp_D}03, then

UDU^{\perp_D}04

This UDU^{\perp_D}05 is called a Delsarte dual of UDU^{\perp_D}06; provided UDU^{\perp_D}07, one has UDU^{\perp_D}08 and UDU^{\perp_D}09.

The quotient-model dual controls defect data exactly. If

UDU^{\perp_D}10

then

UDU^{\perp_D}11

Thus UDU^{\perp_D}12 has the same defect-sequence length UDU^{\perp_D}13, with positive defects occurring at complementary dimensions. The same paper also gives a bijection UDU^{\perp_D}14 between minimal subspaces of positive defect, reversing inclusion. This framework is used there to unify classes of subspaces studied in finite geometry and to give a new geometric interpretation of code duality (Borello et al., 29 Sep 2025).

4. Delsarte duals of rank-metric codes

For a prime power UDU^{\perp_D}15, let UDU^{\perp_D}16 be endowed with the nondegenerate symmetric bilinear form

UDU^{\perp_D}17

If UDU^{\perp_D}18 is an UDU^{\perp_D}19-linear rank-metric code, its Delsarte dual is

UDU^{\perp_D}20

Nondegeneracy gives

UDU^{\perp_D}21

The associated rank distribution is

UDU^{\perp_D}22

and if UDU^{\perp_D}23, the Delsarte analogue of the Singleton bound is

UDU^{\perp_D}24

The rank defect is

UDU^{\perp_D}25

with UDU^{\perp_D}26 (Cruz et al., 2015).

MacWilliams identities relate the rank distributions of UDU^{\perp_D}27 and UDU^{\perp_D}28. In the form quoted in the paper, for UDU^{\perp_D}29,

UDU^{\perp_D}30

Hence the full rank distribution of UDU^{\perp_D}31 determines that of UDU^{\perp_D}32, and conversely. If UDU^{\perp_D}33 is MRD or, more generally, dually-QMRD, then for each UDU^{\perp_D}34 with UDU^{\perp_D}35,

UDU^{\perp_D}36

so the entire distribution depends only on UDU^{\perp_D}37. In the general positive-defect case, the high-rank frequencies are determined by the parameters together with the “small-rank” numbers. When UDU^{\perp_D}38, UDU^{\perp_D}39, and UDU^{\perp_D}40, one has

UDU^{\perp_D}41

A complementary geometric description uses UDU^{\perp_D}42 rank-metric codes. If UDU^{\perp_D}43 is a generator matrix of a nondegenerate UDU^{\perp_D}44-linear code UDU^{\perp_D}45, and UDU^{\perp_D}46 is the UDU^{\perp_D}47-span of its column vectors in UDU^{\perp_D}48, then

UDU^{\perp_D}49

and the minimum rank distance is

UDU^{\perp_D}50

Moreover, UDU^{\perp_D}51 is, up to UDU^{\perp_D}52-equivalence, the Delsarte dual of UDU^{\perp_D}53, and the defect-sequence rule recovers the Wei-type duality

UDU^{\perp_D}54

Within this framework, MRD, near-MRD, quasi-MRD, and UDU^{\perp_D}55-MRD codes are analyzed via defect sequences, and several of these classes are shown to be closed under duality (Borello et al., 29 Sep 2025).

5. Dual formulations of higher-order Delsarte LPs

For binary codes of block length UDU^{\perp_D}56 and minimum distance UDU^{\perp_D}57, Delsarte’s original level-1 primal LP uses a function UDU^{\perp_D}58 supported on

UDU^{\perp_D}59

normalized by UDU^{\perp_D}60, with UDU^{\perp_D}61, UDU^{\perp_D}62, and UDU^{\perp_D}63. Its dual can be written in terms of a function UDU^{\perp_D}64 as

UDU^{\perp_D}65

subject to

UDU^{\perp_D}66

A feasible UDU^{\perp_D}67 certifies an upper bound on code size. Classically, choosing UDU^{\perp_D}68 in terms of Krawtchouk polynomials recovers the MRRW bound (Coregliano et al., 8 Jan 2025).

The higher-order hierarchy replaces single codewords by matrices UDU^{\perp_D}69 and defines UDU^{\perp_D}70 through the linear span of the rows of UDU^{\perp_D}71. The primal formulation imposes positivity of suitable partial Fourier transforms after applying elements of UDU^{\perp_D}72. The symmetrized dual uses functions

UDU^{\perp_D}73

with objective

UDU^{\perp_D}74

subject to a validity inequality on UDU^{\perp_D}75 and the positivity constraints UDU^{\perp_D}76. When UDU^{\perp_D}77, this reduces to the classical level-1 dual; at level UDU^{\perp_D}78, a feasible dual bounds UDU^{\perp_D}79.

A central structural result is the lifting theorem. If UDU^{\perp_D}80 and UDU^{\perp_D}81 is feasible for the level-UDU^{\perp_D}82 dual with objective value

UDU^{\perp_D}83

then one can explicitly construct a feasible level-UDU^{\perp_D}84 dual UDU^{\perp_D}85 with objective

UDU^{\perp_D}86

The paper interprets this as showing that any level-UDU^{\perp_D}87 dual bound automatically lifts to level UDU^{\perp_D}88 without loss in the natural exponent. It also gives a dual-based completeness proof: if UDU^{\perp_D}89 is closed under taking subspaces and

UDU^{\perp_D}90

then for every UDU^{\perp_D}91 the optimum of the subspace-symmetric dual is exactly

UDU^{\perp_D}92

The same work further states that the spectral construction via the polynomial UDU^{\perp_D}93 and combinatorial “cylinder” arguments is the first from-scratch dual at level UDU^{\perp_D}94, and that it recovers the MRRW rate

UDU^{\perp_D}95

up to lower-order terms for small relative distance UDU^{\perp_D}96 (Coregliano et al., 8 Jan 2025).

6. Applications, closure properties, and recurring distinctions

Delsarte duality has direct consequences beyond coding bounds. In the q-matroid setting, a q-matroid UDU^{\perp_D}97 on UDU^{\perp_D}98 is specified by a rank function UDU^{\perp_D}99 satisfying the axioms UdU^d00 UdU^d01, UdU^d02 monotonicity, and UdU^d03 submodularity. If UdU^d04 is a UdU^d05 matrix over UdU^d06 of rank UdU^d07, then

UdU^d08

defines an UdU^d09-representable q-matroid UdU^d10, depending only on the UdU^d11-system UdU^d12 spanned by the columns, and UdU^d13 is the dual q-matroid UdU^d14. For direct sums of uniform q-matroids, Delsarte duality yields the equivalence

UdU^d15

if and only if

UdU^d16

The same paper also defines the rank-generating function

UdU^d17

and states that when UdU^d18, the weight enumerator UdU^d19 is recovered from UdU^d20 by a simple substitution (Borello et al., 29 Sep 2025).

A recurring source of ambiguity is that the same expression refers to different dual mechanisms. In the subspace theory, UdU^d21 is the trace-orthogonal complement inside UdU^d22, whereas UdU^d23 is a quotient-model dual living in a different ambient dimension. In Euclidean extremal theory, the dual is a tempered distribution UdU^d24, not an orthogonal complement. In higher-order coding LPs, the dual consists of feasible certificates UdU^d25. Another common simplification is to regard weak and strong linear duality as automatic in every setting; the Euclidean theory explicitly notes that this is automatic in the finite group setting, but requires proof in the continuous setting (Kolountzakis et al., 11 Oct 2025). These distinctions are structural rather than terminological: each version of Delsarte duality is tailored to the ambient category in which the extremal problem is posed.

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