For finite involutive non-degenerate set-theoretic solutions of the Yang–Baxter equation, the simple solutions are the indecomposable building blocks from which all others are assembled by extensions, within Drinfeld's 1992 program of classifying all such solutions. It is known that no simple solution can have composite square-free cardinality, while simple solutions exist for every prime cardinality, every square n2n^2, every prime power pnp^n with n>1n>1, and every cardinality p2np^2 n for which the prime pp divides q−1q-1 for each prime divisor qq of nn, plus sporadic examples of cardinalities 12 and 27. Whether a simple solution exists for every cardinality of the form m2nm^2 n with integers m,n>1m,n>1 — the generic non-square-free shape — was claimed by Cedó and Okniński in 2021, retracted in a 2024 corrigendum, and is explicitly recorded as open in their 2024/2026 work. In particular, concrete cardinalities such as 18, 24, and 45 lie outside all verified families.

Background

The Yang–Baxter equation (YBE) asks for a linear map R:V⊗V→V⊗VR:V\otimes V\to V\otimes V satisfying R12R23R12=R23R12R23R_{12}R_{23}R_{12}=R_{23}R_{12}R_{23}; it originated in statistical mechanics and in the theory of quantum groups. Drinfeld (1992) proposed studying its set-theoretic solutions: pairs (X,r)(X,r) where XX is a set and r:X×X→X×Xr:X\times X\to X\times X is a bijection satisfying the same braid relation r12r23r12=r23r12r23r_{12}r_{23}r_{12}=r_{23}r_{12}r_{23}, where r12,r23r_{12},r_{23} act as rr on the indicated pair of factors of X3X^3. Writing r(x,y)=(σx(y),γy(x))r(x,y)=(\sigma_x(y),\gamma_y(x)), a solution is called non-degenerate if all maps σx,γy:X→X\sigma_x,\gamma_y:X\to X are bijections, and involutive if r2=idr^2=\mathrm{id}. The finite involutive non-degenerate solutions form the most developed branch of the theory, initiated by Etingof–Schedler–Soloviev (1999), who introduced the structure group G(X,r)G(X,r) (generated by the elements of XX subject to the relations xy=σx(y)γy(x)xy=\sigma_x(y)\gamma_y(x)) and proved, in particular, that up to isomorphism there is a unique indecomposable solution of each prime cardinality.

Several structural notions organize the classification. A solution is indecomposable if G(X,r)G(X,r) acts transitively on XX. The retract identifies x,y∈Xx,y\in X whenever σx=σy\sigma_x=\sigma_y, producing a quotient solution; a solution equal to its own retract is irretractable, and one whose iterated retracts eventually reach cardinality 1 is a multipermutation solution. Following Vendramin and Castelli, a solution (X,r)(X,r) with ∣X∣>1|X|>1 is simple if every epimorphism of solutions f:(X,r)→(Y,s)f:(X,r)\to(Y,s) is either an isomorphism or satisfies ∣Y∣=1|Y|=1. Simple solutions matter because every finite involutive non-degenerate solution is built from simple ones by iterated dynamical extensions, so they are the atoms of Drinfeld's classification problem. A basic lemma (Cedó–Okniński): a finite simple solution is indecomposable if ∣X∣>2|X|>2 and irretractable if ∣X∣|X| is not prime. Rump (2007) introduced left braces — sets BB carrying an abelian group operation ++ and a second group operation ∘\circ linked by a∘(b+c)=a∘b−a+a∘ca\circ(b+c)=a\circ b-a+a\circ c — which encode involutive non-degenerate solutions; the permutation group G(X,r)\mathcal{G}(X,r) (generated by the σx\sigma_x) is naturally a left brace whose ideals control the congruences of (X,r)(X,r), and this is the main technical tool for proving simplicity.

The cardinality problem asks which finite cardinalities occur as sizes of simple solutions. The known obstruction is sharp: no indecomposable irretractable solution has square-free cardinality (Cedó–Okniński, Adv. Math. 430 (2023)); since a finite simple solution of composite cardinality is indecomposable and irretractable by the basic lemma above, no simple solution has composite square-free cardinality, while prime cardinalities are exempt and occur uniquely. So m2nm^2n is precisely the generic cardinality shape not excluded. On the positive side: each prime cardinality occurs (uniquely, by Etingof–Schedler–Soloviev); every square n2n^2 occurs (Cedó–Okniński 2021, explicit solutions on (Z/(n))2(\mathbb{Z}/(n))^2); every prime power pnp^n with n>1n>1 occurs (Cedó–Okniński 2024/2026); cardinality p2np^2n occurs under the congruence condition that pp divides q−1q-1 for every prime divisor qq of nn (Cedó–Okniński, J. Pure Appl. Algebra 229 (2025)); cardinality p2p^2 is completely classified (Dietzel–Properzi–Trappeniers, Comm. Algebra 53 (2025): indecomposable plus irretractable already forces simplicity); and Castelli (Proc. Amer. Math. Soc. 151 (2023)) gave sporadic examples of cardinalities 12 and 27. In 2021 Cedó and Okniński claimed the general case — an explicit simple solution of cardinality m2nm^2n for all m,n>1m,n>1 (Theorem 4.12 of their Advances in Mathematics paper) — but the proof was incorrect and the claim was retracted in a 2024 corrigendum, which does however give one example of a simple solution of non-square cardinality. Both of their subsequent papers state the general existence question as open, and it is the natural completion of the cardinality picture.

Problem Statement

For arbitrary integers m,n>1m,n>1, does there exist a finite simple involutive non-degenerate set-theoretic solution (X,r)(X,r) of the Yang–Baxter equation with ∣X∣=m2n|X|=m^2n? Here 'simple' means: ∣X∣>1|X|>1 and every epimorphism of solutions f:(X,r)→(Y,s)f:(X,r)\to(Y,s) is either an isomorphism or satisfies ∣Y∣=1|Y|=1 (Definition 1.1 of Cedó–Okniński, Publ. Mat. 70 (2026)), a notion that coincides with Vendramin's simplicity for finite indecomposable solutions. This is the open problem recorded explicitly by Cedó and Okniński after the retraction of their 2021 Theorem 4.12, which had claimed such solutions for all m,n>1m,n>1. Because simple solutions of every prime, prime-power, and square cardinality already exist, an affirmative answer would establish that every non-square-free cardinality — equivalently, every cardinality not excluded by the square-free obstruction — admits a simple solution, completing the determination of which finite cardinalities occur; a negative answer for some m2nm^2n would reveal the first cardinality obstruction beyond square-freeness. Concretely, no construction from the verified infinite families covers cardinalities such as 18=32⋅218=3^2\cdot 2 or 45=32⋅545=3^2\cdot 5, which fail the congruence condition of the strongest partial result (J. Pure Appl. Algebra 229 (2025), Theorem 5.3).

References

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