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Sidon Sets: Uniqueness and Applications

Updated 8 July 2026
  • Sidon sets are subsets of groups defined by the uniqueness condition (a+b=c+d implies {a,b} = {c,d}), ensuring distinct additive or multiplicative representations.
  • Their study spans additive combinatorics, finite-field geometry, coding theory, and harmonic analysis, leading to optimal constructions and bounds in various settings.
  • Modern variants, including q-analogues and operator-space formulations, extend Sidon phenomena to cryptographic functions and network coding applications.

Sidon denotes a cluster of uniqueness and interpolation phenomena that originated with additive B2B_2 sequences and now span additive combinatorics, finite-field geometry, coding theory, harmonic analysis, and operator spaces. In its classical form, a Sidon set is a subset AA of an abelian group such that a+b=c+da+b=c+d implies {a,b}={c,d}\{a,b\}=\{c,d\}; modern variants include multiplicative Sidon sets in N\mathbb N, Sidon subsets of F2t\mathbb F_2^t, Sidon sets in dual groups of compact abelian groups, completely Sidon sets in discrete groups, and the qq-analogues called Sidon spaces (Cilleruelo et al., 2018, Doorn et al., 3 May 2026, Lewko, 4 Jun 2026, Pisier, 2017, Castello et al., 2023).

1. Core meanings and definitions

The unifying theme is uniqueness of representation under a binary or multilinear operation. In additive combinatorics, a Sidon set AA in an abelian group satisfies

a+b=c+d{a,b}={c,d}.a+b=c+d \Rightarrow \{a,b\}=\{c,d\}.

In F2t\mathbb F_2^t, the characteristic-AA0 formulation is equivalent to requiring that the sum of any four distinct elements is never AA1. In multiplicative number theory, a multiplicative Sidon set AA2 satisfies

AA3

In harmonic analysis on a compact abelian group AA4 with dual group AA5, a set AA6 is Sidon if there exists AA7 such that

AA8

for every finite AA9. In the a+b=c+da+b=c+d0-analogue, an a+b=c+da+b=c+d1-subspace a+b=c+da+b=c+d2 is a Sidon space if for nonzero a+b=c+da+b=c+d3,

a+b=c+da+b=c+d4

(Cilleruelo et al., 2018, Czerwinski et al., 2024, Lewko, 4 Jun 2026, Doorn et al., 3 May 2026, Castello et al., 2023).

Setting Defining uniqueness property Typical reformulation
Additive groups a+b=c+da+b=c+d5 pairwise sums are distinct
a+b=c+da+b=c+d6 no four distinct elements sum to a+b=c+da+b=c+d7 a+b=c+da+b=c+d8
Multiplicative subsets of a+b=c+da+b=c+d9 {a,b}={c,d}\{a,b\}=\{c,d\}0 unordered products are distinct
Dual groups {a,b}={c,d}\{a,b\}=\{c,d\}1 {a,b}={c,d}\{a,b\}=\{c,d\}2-{a,b}={c,d}\{a,b\}=\{c,d\}3 comparability on {a,b}={c,d}\{a,b\}=\{c,d\}4 bounded interpolation on {a,b}={c,d}\{a,b\}=\{c,d\}5
Sidon spaces {a,b}={c,d}\{a,b\}=\{c,d\}6 {a,b}={c,d}\{a,b\}=\{c,d\}7

A further abstraction replaces pair sums by a fixed linear form {a,b}={c,d}\{a,b\}=\{c,d\}8. A set {a,b}={c,d}\{a,b\}=\{c,d\}9 is then N\mathbb N0-Sidon if N\mathbb N1 is injective on N\mathbb N2. In an infinite vector space, infinite N\mathbb N3-Sidon sets exist if and only if the coefficient set N\mathbb N4 has distinct subset sums, and the integer growth bounds become N\mathbb N5 in general and N\mathbb N6 for explicit constructions (Nathanson, 2021).

2. Additive combinatorics in integers and finite groups

Classical Sidon theory is organized by the near-square-root bound. For a finite abelian group N\mathbb N7 of order N\mathbb N8, a Sidon set N\mathbb N9 of size F2t\mathbb F_2^t0 satisfies F2t\mathbb F_2^t1, so dense Sidon means F2t\mathbb F_2^t2. A geometric synthesis asserts that all known dense Sidon subsets of abelian groups arise from projective planes through a common construction, and the desarguesian classification recovers the Singer, Bose, Spence, and Hughes–Cilleruelo families; the same framework also yields many examples from nondesarguesian planes and motivates the conjecture that all dense Sidon sets arise in this way (Eberhard et al., 2021).

Several extremal variants are now well developed. For Sidon systems of F2t\mathbb F_2^t3-subsets of F2t\mathbb F_2^t4, the maximum size F2t\mathbb F_2^t5 satisfies

F2t\mathbb F_2^t6

with F2t\mathbb F_2^t7, F2t\mathbb F_2^t8, and F2t\mathbb F_2^t9; in the random model qq0, the threshold for being Sidon is qq1 (Cilleruelo et al., 2018). For arbitrary qq2-element subsets of qq3, if qq4 denotes the minimum possible size of the largest Sidon subset, then

qq5

and the same lower bound holds uniformly for qq6-point subsets of qq7 (Bailleul et al., 4 May 2026).

The basis problem is a separate line of inquiry. Erdős asked for an infinite Sidon sequence that is an asymptotic basis of order qq8. Modularly, for all sufficiently large qq9, there exists a Sidon set in AA0 that is a basis of order AA1; in the integers, there exists an infinite AA2 sequence that is an asymptotic basis of order AA3, and for every AA4 there exists a Sidon sequence that is an asymptotic basis of order AA5 in the sense that every sufficiently large integer is a sum of four elements of the sequence, one of them at most AA6 (Cilleruelo, 2013). A complementary density result shows that there exists a Sidon set AA7 with

AA8

so the triple sumset of a genuine Sidon sequence can already have positive lower density even though the order-AA9 basis question remains open (Kiss et al., 2021).

3. Sidon sets in a+b=c+d{a,b}={c,d}.a+b=c+d \Rightarrow \{a,b\}=\{c,d\}.0, coding theory, and APN constructions

Over a+b=c+d{a,b}={c,d}.a+b=c+d \Rightarrow \{a,b\}=\{c,d\}.1, Sidon sets are tightly linked to binary linear codes. If a+b=c+d{a,b}={c,d}.a+b=c+d \Rightarrow \{a,b\}=\{c,d\}.2 is represented as the column set of a parity-check matrix a+b=c+d{a,b}={c,d}.a+b=c+d \Rightarrow \{a,b\}=\{c,d\}.3, then the associated code a+b=c+d{a,b}={c,d}.a+b=c+d \Rightarrow \{a,b\}=\{c,d\}.4 satisfies: a+b=c+d{a,b}={c,d}.a+b=c+d \Rightarrow \{a,b\}=\{c,d\}.5 is sum-free iff a+b=c+d{a,b}={c,d}.a+b=c+d \Rightarrow \{a,b\}=\{c,d\}.6, and a+b=c+d{a,b}={c,d}.a+b=c+d \Rightarrow \{a,b\}=\{c,d\}.7 is sum-free Sidon iff a+b=c+d{a,b}={c,d}.a+b=c+d \Rightarrow \{a,b\}=\{c,d\}.8. Consequently, the nonexistence of a binary a+b=c+d{a,b}={c,d}.a+b=c+d \Rightarrow \{a,b\}=\{c,d\}.9 code is equivalent to the upper bound F2t\mathbb F_2^t0 for Sidon sets in F2t\mathbb F_2^t1. The trivial estimate

F2t\mathbb F_2^t2

is sharpened to F2t\mathbb F_2^t3 for odd F2t\mathbb F_2^t4, and to an explicit even-F2t\mathbb F_2^t5 bound of the form

F2t\mathbb F_2^t6

for F2t\mathbb F_2^t7. The same paper classifies maximal Sidon sets up to affine equivalence for F2t\mathbb F_2^t8, proves that every maximal Sidon set in F2t\mathbb F_2^t9 has size AA00, and shows that the possible sizes in AA01 are AA02 (Czerwinski et al., 2023).

A second major theme identifies Sidon sets with graphs of cryptographically strong functions. For AA03, the graph

AA04

is Sidon if and only if AA05 is APN. Intersecting AA06 with a hyperplane corresponding to a maximizing Walsh coefficient produces a Sidon set in AA07 of size

AA08

Using 8-bit APN functions of linearity AA09, this yields Sidon sets of size AA10 in AA11, improving the previous best-known size AA12, and it produces a binary AA13 code. The same analysis proves the general APN bound AA14 (Czerwinski et al., 2024).

The cryptographic analogy has recently been pushed further. For Sidon sets AA15, minimal linearity is characterized exactly by the AA16-cover property: every AA17 has exactly AA18 representations as AA19 with AA20. This classification is recast through the Cayley graph of the Boolean function AA21, yielding strongly regular graphs; in particular, the unique rank-AA22 strongly regular graph with parameters AA23 is realized as such a Cayley graph, and the best-known lower bound for the largest Sidon set in AA24 is improved by AA25 for all AA26 (Thornburgh, 19 Jan 2025). Related work on polynomial graphs in AA27 shows that planar polynomials make AA28 a maximum Sidon set, while various monomial and cubic candidates over AA29 are excluded by exact multiplicity criteria (Afifurrahman et al., 2021).

4. Harmonic-analytic, probabilistic, and operator-space formulations

In harmonic analysis, Sidon sets are interpolation sets for Fourier coefficients. For a compact abelian group AA30 with dual AA31, a subset AA32 is Sidon precisely when bounded data on AA33 extend to Fourier transforms of bounded continuous functions or bounded measures with uniform control. In dual groups of bounded torsion, this interpolation property is equivalent to a purely combinatorial decomposition statement: AA34 The final missing prime-power case is proved by combining Pisier’s proportional quasi-independence theorem, Bourgain’s projection theorem, a local dimension bound for reduced signed relations, and a Rado–Horn support-partition argument; in prime-power groups, the number of quasi-independent pieces is bounded by

AA35

(Lewko, 4 Jun 2026).

For torsion-free dual groups, Sidon sets admit an even sharper proportional structure. A Sidon set is proportionally AA36-degree independent for every AA37, and for every AA38 one can extract proportionally large subsets with Sidon constant at most AA39, the minimum possible value. The argument combines Pisier’s proportional characterization, higher-order independence, and Riesz-product interpolation; in torsion groups such uniform small constants can fail (Hare et al., 2018).

The same vocabulary extends beyond characters. Any uniformly bounded AA40-orthonormal system is AA41-fold tensor Sidon, improving Bourgain–Lewko’s AA42-fold result, and a bounded system is randomly Sidon if and only if it is AA43-fold tensor Sidon, equivalently AA44-fold tensor Sidon for some or all AA45. Pisier’s proof uses Talagrand’s majorizing measure theorem, Gaussian domination, and a tensor decomposition

AA46

(Pisier, 2016).

A noncommutative version replaces classical Banach-space Sidonicity by operator-space structure. A subset AA47 of a discrete group AA48 is completely Sidon if its span in AA49 is completely isomorphic to AA50 with maximal operator space structure. Completely Sidon sets are stable under finite unions, bounded Hermitian functions on symmetric completely Sidon sets extend to positive definite functions, and AA51 is completely Sidon if and only if the dual operator space AA52 is exact (Pisier, 2017).

5. Sidon spaces and AA53-analogues

Sidon spaces are the AA54-analogues of Sidon sets. An AA55-subspace AA56 is Sidon exactly when

AA57

for nonzero AA58, or equivalently when

AA59

Roth, Raviv, and Tamo showed that this is equivalent to saying that the cyclic orbit AA60 has full size AA61 and minimum subspace distance AA62, making Sidon spaces precisely the optimal one-orbit cyclic subspace codes of that type (Castello et al., 2023).

A large class of constructions lives inside sums of two multiplicative cosets of a fixed subfield. Writing AA63, one considers

AA64

or, in graph form,

AA65

for a linearized polynomial AA66. The paper “Constructions and equivalence of Sidon spaces” characterizes when AA67 is Sidon through an intrinsic “Sidon space property” for AA68, proves that scattered polynomials yield Sidon space polynomials, establishes a sharp monomial criterion in degree-AA69 extensions, gives a direct-sum construction, and formulates semilinear equivalence in terms of AA70-actions and AA71-orbits (Castello et al., 2023).

The generalized theory replaces pairwise multiplicative uniqueness by AA72-fold multiplicative uniqueness. An AA73-Sidon space is a subspace AA74 such that equality of two AA75-fold products of nonzero elements forces equality of the multisets of one-dimensional AA76-subspaces. If AA77 denotes the AA78-span, then

AA79

and equality implies that AA80 is AA81-Sidon. The same framework gives lower bounds on AA82, prime-degree strengthenings, constructions from AA83-sets and irreducible polynomials, and a scattered-polynomial construction

AA84

which is AA85-Sidon whenever AA86 is scattered and AA87 generates an extension of degree at least AA88 (Castello, 2023). These spaces are motivated not only by combinatorics but also by random linear network coding, because one-orbit cyclic subspace codes derived from Sidon spaces achieve large size together with minimum distance AA89 (Castello, 2023).

6. Multiplicative, geometric, and current developments

The multiplicative analogue asks for subsets of AA90 with unique unordered products. If AA91 denotes the least AA92 such that some multiplicative Sidon set AA93 meets every interval AA94, then primes show that multiplicative Sidon sets can be large, while Erdős proved that the maximum size is

AA95

Recent work answers Sárközy’s square-root question by proving

AA96

via the explicit congruence class construction AA97 with AA98, and then improves this asymptotically to

AA99

using primes in short intervals, a private-prime Sidon criterion, and a weighted Hall matching argument. A notable auxiliary feature is that the square-root proof was autonomously discovered and formally verified in Lean by Aristotle, and the power-saving argument was formalized in Lean under its analytic inputs (Doorn et al., 3 May 2026).

A subsequent refinement lowers the exponent dramatically: a+b=c+da+b=c+d00 The proof introduces a Lovász Local Lemma selection principle for choosing one element from each of many large local sets while preserving multiplicative Sidonicity, then combines it with exceptional-set bounds for primes in short intervals. Under Lindelöf- or RH-type estimates one further gets the conditional bound a+b=c+da+b=c+d01 (Doorn et al., 5 Jun 2026). This suggests that the exact order of a+b=c+da+b=c+d02, currently bracketed between logarithmic lower bounds and subpower upper bounds, remains one of the central open problems in the multiplicative theory.

Sidon sequences also admit a geometric incarnation in CAT(0) geometry. Given a finite Sidon sequence a+b=c+da+b=c+d03, Barré and Pichot construct link graphs a+b=c+da+b=c+d04 such that

a+b=c+da+b=c+d05

With equilateral triangles, this is exactly the nonpositive-curvature link condition. The same paper shows that the number of representations of an integer as an alternating triple sum a+b=c+da+b=c+d06 determines the local ring data governing embedded Euclidean flats in the associated CAT(0) complex (Barré et al., 2023).

Taken together, these developments show that Sidon phenomena are not a single theorem but a recurrent structural principle. Depending on the ambient category, Sidon means unique additive representation, unique multiplicative representation, bounded Fourier interpolation, operator-space a+b=c+da+b=c+d07-structure, or uniqueness of multiplicative factorizations in subspace codes. A plausible implication is that progress in one setting—Walsh-spectral methods over a+b=c+da+b=c+d08, projection and quasi-independence in harmonic analysis, or prime-distribution estimates in multiplicative problems—often exports nontrivially to the others (Thornburgh, 19 Jan 2025, Lewko, 4 Jun 2026, Doorn et al., 5 Jun 2026).

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