Abstract
This paper explores the relationship between fuzzy logic algebra and non associative groupoid. As a groupoid which can satisfy type-2 cyclic associative (T2CA) law, T2CA-groupoid is characterized by generalized symmetry. Fuzzy logic algebra is a major direction in the study of fuzzy logic. Residuated lattices are a class of fuzzy logic algebras with widespread applications. The inflationary pseudo general residuated lattice (IPGRL), a generalization of the residuated lattice, does not need to satisfy the associative law and commutative law. Moreover, the greatest element of IPGRL is no longer the identity element. In this paper, the notion of T2CA-IPGRL (IPGRL in T2CA-groupoid) is proposed and its properties are investigated in combination with the study of IPGRL and T2CA-groupoid. In addition, the generalized symmetry and regularity of T2CA-groupoid are investigated based on the characteristics of commutative elements. Meanwhile, the decomposition of T2CA-root of band with T2CA-unipotent radical is studied as well. The result shows that every T2CA-root of band is the disjoint union of T2CA-unipotent radicals.
Keywords
Introduction
A groupoid will be called a type-2 cyclic associative groupoid (T2CA-groupoid) if it holds the type-2 cyclic associative (T2CA) law [x * (y * z) = (z * x) * y] [1]. In the early literature, there was no distinction between T2CA law and cyclic associative (CA) law [x * (y * z) = z * (x * y)] so both of them were called CA law.
In 1954, Hosszú [2] discussed the function equations that satisfy two types of CA laws. The continuous and strictly monotonic solutions of these two types of equations are given in [3], and the power series solutions in the complex domain are given in [4]. Until 2020, the two different forms of CA laws had not been distinguished in [1]. As a follow-up study of [1], we extend the quasi identity element and study the generalized symmetry of T2CA-groupoid from operational laws perspective.
In 1936, von Neumann put forward the concept of regularity when studying ring theory [5]. As an effective research method, regularity is widely used in semigroups [6–11]. There are also many interesting conclusions about regularity in non associative groupoids (see [12–14]). In order to reveal the regularity of T2CA-groupoid, we study regular T2CA-groupoid, generalized regular T2CA-groupoid, transposition regular T2CA-groupoid and their relationships. In [15], Xiaogang An et al. studied T2CA-band and T2CA-3-band. As a special type of T2CA-groupoid, the squares of all elements of the T2CA-root of band are idempotent, and we study its structural characteristics.
In 2021, Rui Paiva et al. proposed an inflationary general residuated lattice (IGRL) [16] when studying inflationary general overlap function. Rong Liang and Xiaohong Zhang extended the IGRL to the inflationary pseudo general residuated lattice (IPGRL) [17]. The filters of IGRL and IPGRL was studied in [18]. Based on the research in [17], we have studied a special IPGRL which called T2CA-IPGRL because its elements satisfy the T2CA law.
In [17], Rong Liang and Xiaohong Zhang proposed inflationary pseudo general overlap function (PGOF) which proves that an inflationary PGOF is a fuzzy conjunction (see [17] lemma 2). Due to the non commutative and non associative properties of T2CA-groupoid, the inflationary PGOF that satisfies the T2CA law will be a non commutative and non associative fuzzy conjunction. A T2CA-IPGRL can be induced by an inflationary PGOF that satisfies the T2CA law. Therefore, studying the properties of T2CA-groupoid and T2CA-IPGRL is helpful for further research on non commutative and non associative fuzzy logic formal system.
The rest of this paper is organized as follows. In Section 2, we extend the concept of quasi identity element and study the generalized symmetry of T2CA-groupoid from the perspective of operational laws. In Section 3, we study various types of T2CA-groupoid with regularity and their relationships. T2CA-root of band is analyzed in Section 4. The notion of inflationary pseudo general residuated lattice in T2CA-groupoid is proposed, and its properties are studied in Section 5. The final section provides conclusions and future research directions.
Generalized Symmetry of T2CA-Groupoids
In this section, we will discuss the generalized symmetry of T2CA-groupoids, which is the basis of studying regular T2CA-groupoids.
First, we will introduce several basic concepts of groupoid and the research results related to this paper in T2CA-groupoid. For a groupoid (D, *), if for any x, y ∈ D, x * y = y * x, it has commutative property, and if for any x ∈ D, (x * x) * x = x * (x * x), it has monoassociative property. It is obvious that a T2CA-groupoid has monoassociative property.
In [1], Xiaohong Zhang et al. proposed the quasi identity element and gave the relationship between quasi identity element and commutativity in T2CA-groupoids (see Definition 2.1 and Theorem 2.1).
Example 2.1 is from [1], which clearly illustrates Theorem 2.1 and Proposition 2.3.
A T2CA-groupoid with quasi identity element of order 5
A T2CA-groupoid with quasi identity element of order 5
Theorem 2.1 gives a sufficient condition for the T2CA-groupoid to have commutative properties. In fact, we divide a T2CA-groupoid into idempotent sets and non idempotent sets. By Proposition 2.2, every idempotent element in T2CA-groupoid has commutativity. As long as the non idempotent elements are commutative, the T2CA-groupoid is commutative. The following Theorem 2.3 is an extension of Theorem 2.1. In Theorem 2.3, the condition for quasi identity element can be relaxed. For a T2CA-groupoid (D, *), all its idempotent set can be represented by E (D), and all non idempotent elements, that is, the complementary set of E (D), can be represented by
In a T2CA-groupoid (D, *), an element
First, we will prove that a left pre-quasi identity element is a right pre-quasi identity element. Let c be a left pre-quasi identity element in a T2CA-groupoid (D, *). By Definition 2.2, for any
Thus, element c is a right pre-quasi identity element.
Next, we prove that a right pre-quasi identity element is a left pre-quasi identity element. Let c be a right pre-quasi identity element in a T2CA-groupoid (D, *). For any
By Definition 2.2, element c is a left pre-quasi identity element. Thus, the left and right pre-quasi identity elements are equivalent, ending the proof. □
Case 1: f ∈ E (D) or g ∈ E (D), by Proposition 2.2, f * g = g * f;
Case 2:
Case 3:
Theorem 2.3 can be seen as a generalization of Theorem 2.1.
A T2CA-groupoid of order 6 with pre-quasi identity element
The commutative law of binary operations defined on a groupoid reflects its symmetry. As a generalized commutative law, the arbitrary three elements in a groupoid perform binary operations in order. Changing the order of the first two elements does not affect the final result, which is (x * y) * z = (y * x) * z. This is called left commutative law. Correspondingly, there is the right commutative law, where x * (y * z) = x * (z * y). A groupoid is called a left (right) commutative groupoid if it holds the left (right) commutative law. In [19], left (right) commutative groupoid was introduced. Rashad Muhammad et al. extended these concepts and studied left (right) commutative groupoid in Abel-Grassmann’s groupoids (AG-groupoids) [20]. When the left (right) commutative groupoid satisfies the T2CA law, we call it the left (right) commutative T2CA-groupoid, abbreviated as LC-T2CA-groupoid (RC-T2CA-groupoid). A T2CA-groupoid is called a bi-commutative T2CA-groupoid (BC-T2CA-groupoid) if it holds both the left and right commutative laws. The LC-T2CA-groupoid, RC-T2CA-groupoid, and BC-T2CA-groupoid can characterize the generalized symmetry of T2CA-groupoid from a macro perspective.
Example 2.3 and 2.4 illustrate that there is no necessary connection between LC-T2CA-groupoid and RC-T2CA-groupoid.
A LC-T2CA-groupoid that is not a RC-T2CA-groupoid
A RC-T2CA-groupoid that is not a LC-T2CA-groupoid
From Example 2.5, we can see that a BC-T2CA-groupoid may not be a commutative T2CA-groupoid.
A non commutative BC-T2CA-groupoid
In [1], Xiaohong Zhang et al. proved that every commutative T2CA-groupoid is a semigroup. Commutativity is a sufficient condition for a T2CA-groupoid to become a semigroup. We can weaken this condition. See the following Proposition 2.6.
By Proposition 2.2, every idempotent element in T2CA-groupoid has commutativity. According to the latest research, an element in T2CA-groupoid also has commutativity if its third power is equal to itself. With the deepening of research, there are two research directions on the generalized symmetry of T2CA-groupoid. The first is to study from the perspective of operational laws, which characterizes the generalized symmetry of T2CA-groupoid from a macro perspective (see Example 2.3, 2.4, 2.5, and Proposition 2.6). The second is to study the commutativity of individual elements, which characterizes the local symmetry of T2CA-groupoid from a microscopic perspective. We know that when all elements have commutativity, local symmetry becomes global symmetry. This also prompts us to find ways to identify the characteristics of elements with commutative properties in future research.
In this section, we study various types of T2CA-groupoid with regularity and their relationships.
Through Example 3.1, the existance of regular T2CA-groupoid can be demonstrated.
A regular T2CA-groupoid
A regular T2CA-groupoid
c * a is an idempotent element; a * c = c * a; a = (c * a) * a = a * (a * c) = (a * c) * a = a * (c * a).
(2)
(3) It is easy to deduce from (2). □
In [11], the left (right) transposition regular semigroups were introduced. In 2022, Yudan Du et al. studied the left (right) transposition regular AG-groupoids [13] and Xiaogang An discussed the left (right) transposition regular TA-groupoids [14]. Similarly, we will introduce the left (right) transposition regular T2CA-groupoid and investigate the relationship between regularity and left (right) transposition regularity in T2CA-groupoid.
First, we will prove that a LTR-T2CA-groupoid is a regular T2CA-groupoid. Suppose that a is an arbitrary element in a LTR-T2CA-groupoid (D, *). There exists c ∈ D such that (c * a) * a = a. We have
By Definition 3.1, (D, *) is a regular T2CA-groupoid.
Next, we will prove that a regular T2CA-groupoid is a LTR-T2CA-groupoid. It is easily obtained by Proposition 3.1 (3), ending the proof. □
Example 3.2 illustrates the existance of generalized regular T2CA-groupoid.
A generalized regular T2CA-groupoid of order 6
Case 1: if j = i, then a i = a2i, that is, a i = a i * a i , a i is the idempotent element in D.
Case 2: if j > i, then from a i = ai+j we have
a j = a i * aj-i = ai+j * aj-i = a2j = a j * a j .
This means that a j is the idempotent element.
Case 3: if j < i, then from a i = ai+j we have
a i = ai+j = a i * a j = ai+j * a j = ai+2j;
a i = ai+2j = a i * a2j = ai+j * a2j = ai+3j;
……
a i = ai+ij.
Since i, j ∈ Z+, then ij ≥ i. For a i = ai+ij, Case 3 becomes Case 1 when ij = i, and Case 3 becomes Case 2 when ij > i. Therefore, for any element a ∈ D, we can find that a n is a regular element. □
Figure 1 shows the relationships between the generalized regular T2CA-groupoid and regular T2CA-groupoid. Here, A, the upper right sector, represents the finite regular T2CA-groupoid given in Example 3.1; B, the upper left sector, represents the infinite regular T2CA-groupoid; C, the lower right sector, represents the finite generalized regular T2CA-groupoid given in Example 3.2 rather than regular T2CA-groupoid; and D, the lower left sector, represents the infinite generalized regular T2CA-groupoid rather than regular T2CA-groupoid. A+B represents the regular T2CA-groupoid. A+C represents the finite generalized regular T2CA-groupoid. At the same time, A+C also represents the finite T2CA-groupoid, which shows that all finite T2CA-groupoids are generalized regular T2CA-groupoids (see Theorem 3.2). A+B+C+D represents the generalized regular T2CA-groupoid.

The relationships between the generalized regular T2CA-groupoid and regular T2CA-groupoid.
Commutativity is a global symmetric property in a groupoid, while Proposition 3.1 represents a local symmetric property in a regular T2CA-groupoid. When we were looking for examples of regular T2CA-groupoid, we found an interesting phenomenon. In T2CA-groupoid of order 3, 4, 5 and 6, there is no non-commutative regular T2CA-groupoid. Therefore, in the rest of this section, we will study the relationship between commutativity and regular T2CA-groupoid.
Bands and band decompositions [21–29] are one of the most effective methods to study nonassociative algebra. In [15], Xiaogang An et al. studied T2CA-band and T2CA-3-band. However, these two special T2CA-groupoids are commutative, so the study of their decomposition theorems is of little value. In T2CA-groupoid, we study a special band structure (see Definiton 4.1), which is not all commutative, so its decomposition theorem is more valuable (see Theorem 4.1). In a T2CA-groupoid (D, *), there is a class of elements whose square is idempotent, which we denote the set as
Example 4.1 illustrates the existance of T2CA-root of band.
A T2CA-root of band of order 7
A T2CA-root of band of order 7
S
e
is a T2CA-unipotent radical; D = ⋃ e∈E(D)S
e
, that is, every T2CA-root of band is the disjoint union of T2CA-unipotent radicals.
(2) By Definition 4.1, the square of each element in the T2CA-root of band is an idempotent. Suppose that α and β are two different idempotent elements. It is easy to prove that S α∩ S β = ∅. Thus, every T2CA-root of band is the disjoint union of T2CA-unipotent radicals. □
A T2CA-root of band of Example 4.2
In [17], Rong Liang and Xiaohong Zhang studied inflationary pseudo general residuated lattices. As a continuation of [17], we study a special inflationary pseudo general residuated lattice whose star operation satisfies the T2CA law (see Definiton 5.3).
(L, ∧ , ∨ , 0, 1) is a lattice, where element 0 is its lower bound and element 1 is its upper bound; (L, * , 1) is a commutative monoid; x * y ≤ z iff x ≤ y → z, for any x, y, z ∈ L.
is a lattice, where element 0 is its lower bound and element 1 is its upper bound; is a groupoid; x * z ≤ y iff z ≤ x → y, z * x ≤ y iff z ≤ x ⇝ y, for any x, y, z ∈ L.
By Definition 5.1 and 5.2, an IPGRL is a generalization of the residuated lattice. It does not need to satisfy the associative law and commutative law. Moreover, the greatest element of IPGRL is no longer the identity element.
a * (a → b) ≤ b, (a ⇝ b) * a ≤ b; a * b ≤ a * c and b * a ≤ c * a when b ≤ c; a → b ≤ a → c and a ⇝ b ≤ a ⇝ c when b ≤ c; c → a ≤ b → a and c ⇝ a ≤ b ⇝ a when b ≤ c; a * 0 =0 * a = 0; c * (a ∨ b) = (c * a) ∨ (c * b).
Through Example 5.1, the existance of T2CA-IPGRL can be demonstrated.

Lattice structure of Example 5.1.
The * operation table of Example 5.1
The → operation table of Example 5.1
The ⇝ operation table of Example 5.1
(b → c) * a ≤ (a → b) → c; a * (b ⇝ c) ≤ (a ⇝ b) ⇝ c; a ⇝ b ≤ (b → c) → (a → c); a → b ≤ (b ⇝ c) ⇝ (a ⇝ c); a * b → c = a ⇝ (b → c); a * b ⇝ c = b → (a ⇝ c).
(2) For any a, b, c ∈ L, by Proposition 5.1 (1), we have (a ⇝ b) * a ≤ b and (b ⇝ c) * b ≤ c. From Proposition 5.1 (2), (b ⇝ c) * ((a ⇝ b) * a) ≤ (b ⇝ c) * b ≤ c. Because L satisfies the T2CA law, we have (b ⇝ c) * ((a ⇝ b) * a) = (a * (b ⇝ c)) * (a ⇝ b) ≤ c. By Definition 5.2 (3), a * (b ⇝ c) ≤ (a ⇝ b) ⇝ c.
(3) For any a, b, c ∈ L, by (1), we have (b → c) * (a ⇝ b) ≤ ((a ⇝ b) → b) → c. From Proposition 5.1 (1), Definition 5.2 (3) and Proposition 5.1 (4), we have
(4) For any a, b, c ∈ L, by (2), we have (a → b) * (b ⇝ c) ≤ ((a → b) ⇝ b) ⇝ c. By Proposition 5.1 (1), Definition 5.2 (3) and Proposition 5.1 (4) we have
(5) For any a, b, c, x ∈ L, we have
(6) For any a, b, c, x ∈ L, we have
1 is an idempotent element, and 1 * a = a * 1; if there exists c ∈ L such that 1 * c = a then 1 * a = a.
(2) If there exists c ∈ L such that 1 * c = a, we have
Second, we prove that the * operation is closed in T (L). For any s, t ∈ T (L), there exist a, b ∈ L such that s = 1 * a, t = 1 * b. Then
Third, we prove that the * operation has commutativity and associativity in T (L).
Since 1 is the identity element in (T (L) , *), 1 * s = s ≤ s. By Definition 5.2 (3), s ≤ 1 → s. By Proposition 5.1 (4), we have (1 → s) → t ≤ s → t. From Theorem 5.1 (1), 1 * (s → t) = (s → t) *1 ≤ (1 → s) → t ≤ s → t. By Definition 5.2, 1 * (s → t) ≥ s → t. Thus, 1 * (s → t) = s → t. The → operation is closed in T (L). Thus, is a residuated lattice. □

Lattice structure of Example 5.2.
The * operation table of Example 5.2
The → operation table of Example 5.2
The ⇝ operation table of Example 5.2
In this paper, we investigate the generalized symmetry and regularity of T2CA-groupoid. A sufficient condition for the commutativity of T2CA-groupoids is given (see Theorem 2.3). In T2CA-groupoid, regularity and left (right) transposition regularity are equivalent (see Theorem 3.1) and each regular T2CA-groupoid is a commutative semigroup (see Theorem 3.3). Moreover, the decomposition of T2CA-root of band is studied with T2CA-unipotent radical. The result shows that every T2CA-root of band is the disjoint union of T2CA-unipotent radicals (see Theorem 4.1). Finally, the properties of T2CA-IPGRL are studied. The results are shown in Theorem 5.1 and 5.3. The main results obtained in this paper on the T2CA-groupoids are shown in Fig. 4.

The main results on the T2CA-groupoids.
We have two research directions for future research. One is to find the characteristics of elements with commutative properties (as described at the end of Section 2), and the other is to study the relationships among T2CA-IPGRL, pseudo overlap functions and some related algebra systems (see [18, 31–34]).
Footnotes
Acknowledgments
This research was supported by the National Natural Science Foundation of China (Grant No. 12271319).
