A recent method for acquiring new solutions of the Yang–Baxter equation involves deforming the classical solution associated with a skew brace. In this work, we demonstrate the applicability of this method to a dual weak brace (S,+,o) and prove that all elements generating deformed solutions belong precisely to the set Dr(S) ={z ∈ S |∀a,b ∈ S (a + b) ◦ z = a◦z−z+b◦z}, which we term the distributor of S. We show it is a full inverse subsemigroup of (S,◦) and prove it is an ideal for certain classes of braces. Additionally, we express the distributor of a brace S in terms of the associativity of the operation ·, with ◦,representing the circle or adjoint operation. In this context, (Dr(S),+,·) constitutes a Jacobson radical ring contained within S. Furthermore, we explore parameters leading to non-equivalent solutions, emphasizing that even deformed solutions by idempotents may not be equivalent. Lastly, considering S as a strong semilattice [Y, Bα,φα,β] of skew braces Bα, we establish that a deformed solution forms a semilattice of solutions on each skew brace Bα if and only if the semilattice Y is bounded by an element 1 and the deforming element z lies in B1.
Deformed solutions of the Yang–Baxter equation associated to dual weak braces
Marzia Mazzotta;Paola Stefanelli
2025-01-01
Abstract
A recent method for acquiring new solutions of the Yang–Baxter equation involves deforming the classical solution associated with a skew brace. In this work, we demonstrate the applicability of this method to a dual weak brace (S,+,o) and prove that all elements generating deformed solutions belong precisely to the set Dr(S) ={z ∈ S |∀a,b ∈ S (a + b) ◦ z = a◦z−z+b◦z}, which we term the distributor of S. We show it is a full inverse subsemigroup of (S,◦) and prove it is an ideal for certain classes of braces. Additionally, we express the distributor of a brace S in terms of the associativity of the operation ·, with ◦,representing the circle or adjoint operation. In this context, (Dr(S),+,·) constitutes a Jacobson radical ring contained within S. Furthermore, we explore parameters leading to non-equivalent solutions, emphasizing that even deformed solutions by idempotents may not be equivalent. Lastly, considering S as a strong semilattice [Y, Bα,φα,β] of skew braces Bα, we establish that a deformed solution forms a semilattice of solutions on each skew brace Bα if and only if the semilattice Y is bounded by an element 1 and the deforming element z lies in B1.| File | Dimensione | Formato | |
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