1. Introduction
The Yang-Baxter equation is a cornerstone of mathematical physics that arises in the study of integrable systems, quantum groups, and quantum information theory. Its origins trace back to foundational papers by Yang [
1] and Baxter [
2]. Let
V be a vector space. A solution of the Yang-Baxter equation is a linear mapping
such that the equality
of operators holds in the space
. The problem of describing all possible solutions is highly complex, so some simplifications have been introduced.
A particularly nice class of solutions is provided by set-theoretic solutions proposed by Drinfel’d [
3]. Let
X be a set and
a bijective mapping.
r is called a set-theoretic solution of the Yang-Baxter equation if the following braid relation holds:
It is clear that a set-theoretic solution extends to a linear one, but, more importantly, set-theoretic solutions lead to their own remarkable algebraic and combinatorial structures. Set-theoretic solutions of the Yang-Baxter equation have found applications in several areas of theoretical and mathematical physics. For example, in the theory of integrable systems, they describe how multi-particle scattering factorizes into pairwise interactions satisfying the Yang-Baxter equation. More recently, involutive non-degenerate set-theoretic solutions have been applied in quantum information theory, where they are related to quantum entanglement and the construction of quantum gates via unitary representations of the braid group. Set-theoretic solutions of the Yang-Baxter equation also have interesting applications in several areas of mathematics, such as non-commutative algebra, knot theory, low-dimensional topology, and the theory of tensor categories. During the last three decades, the study of set-theoretic solutions and related structures has notably intensified; see, for instance, [
4,
5,
6,
7,
8,
9,
10,
11,
12,
13].
Among the various algebraic structures, skew braces have emerged as a particularly noteworthy concept. Skew braces were introduced in [
12], inspired by the earlier works [
14,
15]. Every skew brace yields a non-degenerate set-theoretic solution of the Yang-Baxter equation (not necessarily involutive) [
12]. Moreover, the theory of skew braces is closely connected to the study of indecomposable solutions and multipermutation solutions [
8,
16,
17]. On the algebra side, each set-theoretic solution
associates a quadratic Yang-Baxter algebra
as proposed in [
10], Section 6. If
X is finite and
r is non-degenerate and involutive, then
has remarkable algebraic, homological, and combinatorial properties [
11,
18]. A natural question that arises is how to use the theory of Yang-Baxter algebras to study solutions of the Yang-Baxter equation. The motivation of this paper is to find more ways to study properties of Yang-Baxter algebras.
Deformation theory is very useful in the study of algebraic structures. In light of the deep connections between set-theoretic solutions of the Yang-Baxter equation and various algebraic structures, it is meaningful to investigate the relationships between the deformations of these algebraic structures.
It is known that there is a one-to-one correspondence between non-degenerate involutive set-theoretic solutions of the Yang-Baxter equation and involutive biracks. A birack is an algebra such that is a left quasigroup, is a right quasigroup, and some additional identities are satisfied. Such a correspondence allows us to study solutions of the Yang-Baxter equations via involutive biracks.
In quasigroup theory (see, e.g., [
19], Section II.2), isotopy is a standard method for transforming one quasigroup into another. In their work on involutive set-theoretic solutions of the Yang-Baxter equation of multipermutation level 2, Jedlička, Pilitowska, and Zamojska-Dzienio used a special form of isotope to construct non-distributive solutions from distributive solutions [
20]. Based on their work, in
Section 3, we introduce the notions of an
-graded birack and its isotope and then discuss their properties. Our main theorem is presented in
Section 4. Each involutive
-graded birack
determines an
-graded Yang-Baxter algebra
. We find that, under some conditions, the algebra
determined by an isotope
of the birack
is isomorphic to a Zhang twist of the algebra
(Theorem 1). The Zhang twist is a twist of graded algebras introduced by J.J. Zhang in order to describe graded algebras whose graded module categories are equivalent [
21]. Many important properties of graded algebras, including the Gelfand–Kirillov dimension, and the Noetherian property, being a domain, global dimension, and Artin–Schelter regularity, are preserved under Zhang twist. In fact, our work is inspired by the observation that, in a certain sense, both Zhang twists and isotopes can be viewed as deformations that modify “left translations”.
We provide some examples. Especially, we show that the Yang-Baxter algebras arising from distributive solutions are Zhang twists of polynomial algebras. This class of algebras is believed to share properties similar to those of polynomial algebras. We will discuss them in detail in a subsequent paper.
2. Preliminaries
Throughout, is a base field of characteristic zero. All vector spaces and algebras are over .
2.1. Quasigroups and Biracks
A
left quasigroup is an algebra
with two binary operations ∘ and
such that, for every
, the following conditions hold:
A
right quasigroup is defined analogously as an algebra
with two binary operations • and
such that, for every
, the following conditions hold:
Let
be a left quasigroup. For each
, the
left translation by
x is denoted by
, i.e.,
for any
. Condition (
1) guarantees that each
is bijective, with
. Similarly, Condition (
2) guarantees that each
right translation by
x is bijective with
for any
.
For a left quasigroup
, a bijection
is called an
automorphism of
if
for every
. It is easy to see that a bijection
is an automorphism of
if and only if
for every
.
An automorphism of a right quasigroup can be defined analogously. A bijection is an automorphism of if and only if for every .
A left quasigroup is called
An algebra
with four binary operations is called a
birack if
is a left quasigroup,
is a right quasigroup, and the following holds for any
:
If the set
X is finite, we call the birack
finite.
Example 1. Let X be a non-empty set. An algebra such that, for every ,is certainly a birack. It is called a projection birack. Let be a birack.
It is called
involutive if it additionally satisfies
for any
.
It is said to satisfy Condition
lri provided that
for any
. That is,
for all
.
Remark 1. An involutive birack satisfies Condition lri if and only iffor any . In fact, in an involutive birack, . Hence, The following one-to-one correspondence between involutive biracks and non-degenerate right cyclic left quasigroups is well-known (see, e.g., [
22], Proposition 1.5).
Lemma 1. - (1)
Let be an involutive birack. Then, is a non-degenerate right cyclic left quasigroup.
- (2)
Conversely, let be a non-degenerate right cyclic left quasigroup. For every , define Then, the algebra is an involutive birack.
The operations
and
are connected by
2.2. Set-Theoretic Solution of the Yang-Baxter Equation
By a
quadratic set, we mean a pair
, where
X is a nonempty set and
is a bijective mapping. We write the image of
under
r as
The above equation defines two binary operations on
X:
a left action given by ;
a right action given by ,
for all
. In other words, the maps
and
are precisely the first and second components of
r, respectively. That is,
A quadratic set is called
non-degenerate if the mappings and are bijections for all ;
involutive if ;
square-free if for every ;
a quantum binomial set if it is non-degenerate, involutive, and square-free.
A
set-theoretic solution of the Yang-Baxter equation (YBE) is a quadratic set
such that the braid relation holds:
In this case,
is also called a
braided set.A solution is called
non-degenerate (
involutive, or
square-free) if it is non-degenerate (involutive, or square-free) as a quadratic set. If
X is finite, then
is called a
finite solution.
Convention In the following, by a solution (of the YBE), we mean a set-theoretic, non-degenerate, and involutive solution of the YBE.
Each quadratic set
determines a set of quadratic defining relations
defined by
The unital semigroup
, with generators
X and relations
, is called the semigroup associated with
. The
group associated with is defined analogously. The
algebra associated with is defined as
. When
is a solution of the YBE,
, resp.
,
is called the
Yang-Baxter (
YB)
semigroup, resp. the
YB group, the
YB algebra.
Let
be a non-degenerate quadratic set. It is well-known that
is a set-theoretic solution of the YBE if and only if the following conditions hold for all
(e.g., [
9] (Lemma 2.5)):
For every non-degenerate solution of the YBE, Condition
l1 implies that the mapping
extends canonically to a group homomorphism
where
is the symmetric group on
X. The homomorphism
defines the
canonical left action of
on the set
X. Similarly,
r1 provides the
canonical right action of
on the set
X.
The YB permutation group of a solution is the subgroup of the symmetric group on X generated by .
Example 2. Let X be a set with , and define the map τ by for all . Then, the pair is called the trivial solution.
One can see that is the trivial solution if and only iffor all , or, equivalently,for all . In this case, the YB algebra is just the commutative polynomial algebra , and is the trivial group.
Example 3 ([
3])
. Let X be a set with and f a bijection on X. Define the map asfor all . Then, is a non-degenerate involutive solution of the YBE. Clearly, and for all . Moreover, is a trivial solution if and only if . It is known (see, e.g., [
22], Lemma 1.2) that there is a one-to-one correspondence between solutions of the YBE and involutive biracks.
Lemma 2. - (1)
If is an involutive birack, then defining yields a solution of the YBE.
- (2)
Let be a solution of the YBE with . Defining we obtain an involutive birack .
Such a correspondence allows us to treat each solution as an involutive birack.
3. Isotopes of Quasigroups
This section serves as preparation for
Section 4. We introduce the notion of an
-graded birack and generalize the isotope construction of [
20] to this graded setting.
We say a left quasigroup
is
-
graded if there is a partition on
X:
and, for any
,
If
, then the
degree vector is assigned as
where the 1 is in the
i-th position.
A map is called graded if for any , or equivalently for . If, in addition, f is an automorphism of , then f is called a graded automorphism.
Condition (
4) means that all left translation is graded.
Let
be a sequence of commuting graded bijections of
X. For a degree vector
, set
. Define on the set
X new binary operations:
The algebra
is called the
ϕ-isotope of
.
It is easy to see that
and
So, the
-isotope
is also a left quasigroup. Moreover, the grading of
induces an
-grading on
.
Lemma 3. Let be a non-degenerate -graded left quasigroup and let be a sequence of commuting graded bijections of X. Then, the ϕ-isotope is also non-degenerate.
Proof. The left quasigroup
is
-graded, say
All left translations are graded. By the non-degeneracy of the left quasigroup, for each subset
, the mapping
is bijective. Each
is bijective, so the mapping
is also bijective. Further, (
5) is a partition of
X. Therefore, the mapping
is bijective. The
-isotope
is also non-degenerate. □
Lemma 4. Let be an -graded right cyclic left quasigroup, and be a sequence of commuting -graded automorphisms of such thatfor every and any . Then, the ϕ-isotope is also right cyclic. Proof. We need to prove
for every
. Note that
is a sequence of automorphisms of
. Then,
for every
and
. In this case, Condition (
6) is equivalent to
That is, every
commutes with all left translations.
By the definition of the
-isotope, for the left-hand side of (
7), we have that
Since the quasigroup
is
-graded, all the left translation
is graded. Moreover, each
,
, is graded. Hence,
It follows from Condition (
6) that
. Therefore,
Similarly, for the right-hand side of (
7), we have
The quasigroup is right cyclic, so for any . Taking inverses yields for any .
In conclusion, we obtain that (
7) holds that, for every
, the
-isotope
is also right cyclic. □
We know that involutive biracks are in one-to-one correspondence with non-degenerate right cyclic left quasigroups. We now define the isotope of an -graded birack.
A birack
is called
-
graded if there is a partition
such that, for any
,
Remark 2. If is an involutive birack, then is a non-degenerate right cyclic left quasigroup. The birack is an -graded birack if and only if is an -graded left quasigroup.
Let
be an
-graded involutive birack. Then,
is an
-graded non-degenerate right cyclic left quasigroup. Let
be a sequence of commuting graded bijection of the set
X such that the
-isotope
of
is right cyclic. Then, the left quasigroup
uniquely determines the involutive birack
as follows:
The birack
is called the
ϕ-isotope of
.
All left translations in and , are graded, so is also an -graded birack.
Lemma 5. Let be an -graded involutive birack satisfying Condition
lri
and be a sequence of commuting graded bijections. Then, the ϕ-isotope satisfies Condition
lri
if and only if in ,for any . In this case,for any . Proof. By the definition of Condition
lri, we only need to prove that Condition (
6) is equivalent to
for all
.
Indeed,
satisfies Condition
lri. Then, for every
, we have
Therefore,
satisfies Condition
lri if and only if
satisfies Condition (
10). □
Remark 3. It is easy to see that in an birack , Condition (6) implies Condition (10). Proposition 1. Let be an -graded involutive birack satisfying Condition lri and be a sequence of commuting graded automorphisms of satisfying Condition (6). Then, the ϕ-isotope of is also an -graded involutive birack satisfying Condition lri.
Proof. The birack is an -graded involutive birack, and then is a non-degenerate right cyclic left quasigroup by Lemma 1. By Lemmas 3 and 4, the -isotope is also non-degenerate right cyclic. It determines the -graded involutive birack . By Lemma 5, also satisfies Condition lri. □
4. Isotopes and Zhang Twists
In this section, we will show the relation between the isotopes of involutive biracks and the Zhang twists of algebras.
Recall that, in this paper, the term solution refers to a set-theoretic, non-degenerate, and involutive solution of the YBE. By Lemma 2, solutions of the YBE are in one-to-one correspondence with involutive biracks; hence, every solution can be realized by an involutive birack.
Let us recall the notions needed in this section. Let be an involutive birack.
For each
,
denotes the left translation by
x, and
denotes the right translation by
x. That is,
for any
.
It determines a solution
of the YBE, where
for any
.
It determines an algebra
, generated by
X with quadratic relations
defined by
for any
. If the birack is
-graded, then the grading on
X naturally defines a grading on
A so that
A is an
-graded algebra.
Remark 4.
- (1)
For an (-graded) involutive birack , the (-graded) algebra is precisely the YB algebra of the solution corresponding to the involutive birack. In some cases, we simply call the algebra associated with the birack .
- (2)
Under the correspondence between a solution of the YBE and an involutive birack, the left action coincides with the left translation, and both are denoted by . Similarly, the right action coincides with the right translation, and both are denoted by .
Let
B be any
-graded algebra. Let
be a sequence of commuting
-graded algebra automorphisms of
B. Then, the
Zhang twist of
B by
is defined as follows:
as an
-graded vector space, and the new multiplication ⋆ of
is determined by
where
if the degree of
a is
. We refer to [
21] for basic properties of twisted algebras. The following lemma can be derived from [
21], Proposition 2.5.
Lemma 6. Let B be an -graded algebra. If an -graded algebra C is a Zhang twist of B, then B is a Zhang twist of C.
Now we outline the following main theorem.
Theorem 1. Let be an -graded involutive birack satisfying Condition
lri. It determines an -graded algebra . Let be a sequence of commuting graded automorphisms of satisfying Condition (6). - (1)
The automorphisms naturally induce a sequence of commuting -graded automorphisms on the algebra A.
- (2)
The ϕ-isotope of is also an -graded involutive birack satisfying Condition
lri. It determines an -graded algebra .
- (3)
The algebra obtained by the isotope is isomorphic to the Zhang twist of A by ϕ.
Proof. (1) It is direct.
(2) The fact that the -isotope of is also an -graded involutive birack satisfying Condition lri follows from Proposition 1. Then, it determines an -graded algebra .
(3) The isotope
satisfies Condition
lri. Hence,
for any
. Then, for the algebra
, the relation
is defined by
The multiplication of the Zhang twist
is determined by
for any
. Recall that relation
of
A is defined by
for any
. We have
The last equation follows from that
is an
-graded birack and each
,
, are graded automorphisms of
. So,
and
for any
.
With (
11) and (
12), the map
defined by
for any
is an isomorphism of algebras; the Zhang twist
of
A is isomorphic to the algebra
. □
The Zhang twist preserves many important properties of graded algebras. Thus, by Theorem 1, the study of a structurally complex YB algebra can be reduced—via isotopy—to that of a simpler one.
5. Examples
In this section, we provide some examples illustrating Theorem 1.
5.1. Distributive Solutions
We first show that YB algebras of distributive solutions are Zhang twists of polynomial algebras.
A birack
is called
distributive if, for every
,
If the birack
is involutive, then it is distributive if and only if, for every
,
i.e.,
[
20], Corollary 5.7. Following from [
20], Corollary 5.4 and [
8], Lemma 7.1, we know that an involutive distributive birack satisfies Condition
lri.
A solution of the YBE is called distributive if it corresponds to a distributive involutive birack.
For the rest of this subsection,
is a finite distributive involutive birack. There is an equivalence ∼ defined on
X:
This equivalence provides a partition on
X. That is,
where
By Lemma 3.1 and Corollary 5.4 in [
20], a distributive involutive birack is
2-reductive, i.e.,
for any
. Then, for any
and
,
, (
14) provides a grading on the birack. Assume that
X is partitioned into
p equivalence classes, numbering them as
. The birack
is an
-graded birack.
In each equivalence class
, select a representative element
. We have
for any
. We denote the inverse of these equal mappings as
; i.e.,
. Directly from (
13) and (
15), we obtain that all left translations are automorphisms of the birack satisfying Condition (
6). Moreover, the permutation groups generated by the left transformations are abelian. So,
is a sequence of commuting graded automorphisms of the birack satisfying Condition (
6). In the
-isotope
of the birack
, for any
,
All left and right translations are the identity, so the birack
is a projection birack. It corresponds to a trivial solution of the YBE, whose YB algebra
is just the polynomial algebra
. By Theorem 1, the algebra
is isomorphic to a Zhang twist of the algebra
A, the algebra associated with the birack
. Symmetrically, the algebra
A is a Zhang twist of the algebra
by Lemma 6.
In conclusion, we obtain the following proposition.
Proposition 2. The YB algebra of a finite distributive solution of the YBE is a Zhang twist of the polynomial algebra over the set X.
We provide a concrete example.
Example 4. Let be the following involutive distributive birack:That is, and . The partitionprovides an -grading on the birack. That is, and . The birack determines a solution , where for . The associated YB algebra is the algebra A generated by with relations defined byBy defining and , the algebra A is an -graded algebra. Define and . It is direct to check that is a sequence of commuting graded automorphisms of the birack satisfying Condition (6). The ϕ-isotope is a projection birack. On the other hand, the maps induce a sequence of commuting graded automorphisms of A by definingThe Zhang twist is just the polynomial algebra . 5.2. A Non-Distributive Solution
In this subsection, we present an example of non-distributive solution whose YB algebra is an iterated Zhang twist of a polynomial algebra.
Let
be an involutive birack, where the set
X is
and the left and right translations are given by the following permutations:
It satisfies Condition
lri. Direct calculation shows that
. Hence, the birack is not distributive.
The partition
, where
yields an
-grading on the birack. Set
Then,
is a sequence of commuting
-graded automorphisms of
. The
-isotope is the birack
, where the left and right translations are given by
It is a distributive birack. Then, by Theorem 1, Proposition 2, and the symmetry of Zhang twists (Lemma 6), the algebra associated with the birack
can be obtained from the polynomial algebra
by applying two successive Zhang twists.
6. Conclusions
In this paper, we have introduced the notion of an -graded birack and developed its isotope theory. By the well-established correspondence between set-theoretic involutive non-degenerate solutions of the YBE and involutive biracks, we extended this correspondence to the graded setting. Each involutive -graded birack naturally associates an -graded YB algebra. Our main result establishes a precise algebraic link between isotopy and Zhang twisting: under suitable conditions, the YB algebra arising from an isotope of a given birack is isomorphic to a Zhang twist of the original algebra.
This connection not only enriches the interplay between combinatorial structures (biracks and their isotopes) and noncommutative graded algebras but also provides a new perspective on deformation techniques in the context of the YBE. Since Zhang twists preserve many homological and ring-theoretic properties, such as being Noetherian, having a finite Gelfand–Kirillov dimension, or satisfying Artin–Schelter regularity, our result suggests that isotopic biracks give rise to YB algebras with closely related algebraic behaviors, even when their underlying combinatorial structures may differ significantly.
As a concrete illustration, we have shown that YB algebras associated with finite distributive solutions are Zhang twists of commutative polynomial algebras. This places such algebras within a well-understood class of deformations of polynomial rings, offering a pathway to transfer known results from commutative algebra to this noncommutative setting. In future work, we plan to explore the full implications of this viewpoint, particularly with regard to (i) the classification of multipermutation solutions through their associated graded algebras and (ii) the role of higher-grade isotopies in constructing new families of solutions whose algebraic properties are prescribed in advance.