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Article

Rota–Baxter (Co)algebra Equation Systems and Rota–Baxter Hopf Algebras

1
School of Physical and Mathematical Sciences, Nanjing Tech University, Nanjing 211816, China
2
Shing-Tung Yau Center, School of Mathematics, Southeast University, Nanjing 210096, China
3
School of Mathematics and Information Science, Henan Normal University, Xinxiang 453007, China
*
Author to whom correspondence should be addressed.
Mathematics 2022, 10(3), 426; https://doi.org/10.3390/math10030426
Submission received: 30 December 2021 / Revised: 22 January 2022 / Accepted: 27 January 2022 / Published: 28 January 2022

Abstract

:
We introduce and discuss the notions of Rota–Baxter bialgebra equation systems and Rota–Baxter Hopf algebras. Then we construct a lot of examples based on Hopf quasigroups.

1. Introduction

Rota–Baxter algebras were introduced in [1] in the context of differential operators on commutative Banach algebras. At present, Rota–Baxter algebras have become a useful tool in many fields in mathematics and mathematical physics such as combinatorics, Loday type algebras, Pre-Lie algebras, Pre-Possion algebras, multiple zeta values, quantum field theory and so on (cf. [2,3,4,5,6,7,8,9,10,11]).
Hopf quasigroups were introduced in [12] in order to capture the quasigroup feature of the 7-sphere and they are not required to be associative as a generalisation of Hopf algebras. Let H be a Hopf quasigroup. In [13], the authors obtained a braided monoidal category equivalence between the category of Yetter–Drinfeld quasimodules over H and the category of two-sided two-cosided Hopf quasimodules over H under some suitable assumption (cf. [14,15,16,17,18]).
Rota–Baxter bialgebras were introduced by Ma and Liu in [19]. As a continue of Ma and Liu’s paper, in this article, we introduce and discuss the notions of Rota–Baxter bialgebra equation systems and Rota–Baxter Hopf algebras. We give a lot of examples of Rota–Baxter Hopf algebras based on Hopf quasigroups. Our ideal may be regarded as a guide for further development.
This paper is organized as follows. In Section 2, we recall and investigate some basic definitions and properties related to Hopf quasigroups and Rota–Baxter bialgebras.
In Section 3, we introduce and study the notions of Rota–Baxter (co)algebra equation systems. We give a construction of creating examples based on a two-side H-Hopf quasimodule bialgebra and Radford’s admissible mapping system for Hopf algebras, respectively.
The final Section 4 is devoted to introduce and study the notion of a compatible Rota–Baxter bialgebra and construct a lot of examples.
Through the paper, we fix a ground field F of characteristic 0 and work on F . We use the Sweedler’s notation to express the coproduct of a coalgebra C as Δ ( c ) = c 1 c 2 (cf. [20]). For a left (resp. right) C-comodule coaction ρ l (resp. ρ r ) on M, we write ρ l ( m ) = m ( 1 ) m 0 (resp. ρ r ( m ) = m 0 m ( 1 ) ) for any m M . Let U , V , W be vector spaces and g : U V and f : V W be two linear maps. Then we write f g simply for the composite f g from U to W. For any vector space V, we use i d V to denote the identity map from V to itself and always write i d simply for i d V . We always write T for the flipping map: V V V V , v w w v . Finally, the natural identification V F V F V is assumed.

2. Preliminaries

In this section, some basic definitions and properties of Rota–Baxter bialgebras and Hopf quasigroups are recalled and investigated.

2.1. Algebras and Coalgebras

The following notions can be found in [21]. An algebra  ( A , ) is a vector space A equipped with a linear map : A A A . The algebra ( A , ) is called associative if ( i d ) = ( i d ) . It is customary to write ( x y ) = x y , x , y A . A unital algebra ( A , , μ ) is a vector space A equipped with two linear maps : A A A and μ : F A such that ( i d μ ) = i d = ( μ i d ) . Generally, we write 1 A for μ ( 1 F ) .
Dually, a coalgebra  ( C , Δ ) and a bialgebra ( A , , Δ ) can be similarly given. In particular, a Hopf algebra is a unital counital associative coassociative bialgebra with an antipode (cf. [20]).

2.2. Rota–Baxter Bialtgebras

Given λ F . Recall from [9] (cf. [1,10,11]) that a quadruple ( A , , P , λ ) is called a Rota–Baxter algebra of weight λ if ( A , ) is an algebra and P is a linear endomorphism of A satisfying
( P P ) = P [ ( i d P ) + ( P i d ) + λ ] .
The map P is called a Rota–Baxter operator. If P 2 = P , we say that ( A , P ) is idempotent. Sometimes, we also say that P is a solution to the Equation (1) on A with the weight λ .
Dually, given γ F . Recall from [22] (cf. [9,19]) that a quadruple ( C , Δ , Q , γ ) is called a Rota–Baxter coalgebra of weight γ if ( C , Δ ) is a coalgebra and Q is a linear endomorphism of C such that
( Q Q ) Δ = [ ( i d Q ) + ( Q i d ) + γ ] Δ Q .
The map Q is called a Rota–Baxter operator. If Q 2 = Q , then Q is called idempotent. We also say that Q is a solution to the Equation (2) on C with the weight γ .
Recall from [19] that a Rota–Baxter bialgebra of weight ( λ , γ ) is a pentuple ( B , P , Q , λ , γ ) , where B is a bialgebra ((co)associative or non-(co)associative), ( B , P , λ ) is a Rota–Baxter algebra of weight λ and ( B , Q , γ ) is a Rota–Baxter coalgebra of weight γ .

2.3. Hopf Quasimodules

Recall from [12] that a Hopf quasigroup is a unital counital coassociative bialgebra ( H , , μ , Δ , ε ) armed with a F -linear map S : H H such that
S ( h 1 ) ( h 2 g ) = ε ( h ) g = h 1 ( S ( h 2 ) g ) , ( h g 1 ) S ( g 2 ) = h ε ( g ) = ( h S ( g 1 ) ) g 2
for any h , g H .
The following notions and examples were investigated in [13] (cf. [14,15,23,24]).
Definition 1.
Let H be a Hopf quasigroup. Let M be a unital right (resp. left) H-action φ r (usually we denote it by ◃) (resp. φ l (usually we denote it by ▹)). We say that M is a right (resp. left)H-quasimoduleif for any h H , x M ,
( x h 1 ) S ( h 2 ) = x ε ( h ) = ( x S ( h 1 ) ) h 2 , x 1 = x , ( r e s p . S ( h 1 ) ( h 2 x ) = ε ( h ) x = h 1 ( S ( h 2 ) x ) , 1 x = x ) .
Furthermore, let M be a counital coassociative right (resp. left) H-comodule with coaction ρ r (resp. ρ l ) in the sense of that satisfying
( i d ε ) ρ r = i d , ( i d Δ ) ρ r = ( ρ r i d ) ρ r ( r e s p . ( ε i d ) ρ l = i d , ( Δ i d ) ρ l = ( i d ρ l ) ρ l ) .
We say that M is a right-right (resp. left-left) H-Hopf quasimodule if
ρ r ( x h ) = ρ r ( x ) Δ ( h ) ( r e s p . ρ l ( h x ) = Δ ( h ) ρ l ( x ) )
for any h H and x M .
Example 1.
Let H be a Hopf quasigroup.
(1) 
Let M be a vector space. Then H M is a left-left H-Hopf quasimodule with structures:
h ( a x ) = h a x , a n d ρ H M l ( a x ) = a 1 ( a 2 x )
for all a , h H and x M . In particular H H and H can be regarded as left-left H-Hopf quasimodules.
(2) 
Let M be a vector space. Then M H is a right-right H-Hopf quasimodule with structures:
( x a ) h = x a h , a n d ρ H M r ( x a ) = ( x a 1 ) a 2
for all a , h H and x M . In particular H H and H can be regarded as right-right H-Hopf quasimodules.
The proofs of the following lemma and proposition are straightforward.
Lemma 1.
Let M be a right and a left H-Hopf quasimodule. We define
P R ( x ) = x 0 S ( x ( 1 ) ) a n d P L ( x ) = S ( x ( 1 ) ) x 0
for any x M . Then we have, for any x M
(1) 
P L 2 = P L , P R 2 = P R .
(2) 
ρ r ( P R ( x ) ) = P R ( x ) 1 , ρ l ( P L ( x ) ) = 1 P L ( x ) .
(3) 
x ( 1 ) P L ( x 0 ) = x , P R ( x 0 ) x ( 1 ) = x .
Proposition 1.
Let M be a right and a left H-Hopf quasimodule. If the following conditions hold:
g ( S ( h ) x ) = ( g ( S ( h ) ) ) x a n d ( x S ( g ) ) h = x ( S ( g ) h ) ,
for any g , h H and x M , then we have
P L ( h x ) = ε ( h ) P L ( x ) a n d P R ( x h ) = P R ( x ) ε ( h ) .
Example 2.
(1) 
If ( M , , ρ l ) is a left-left H-Hopf quasimodule, then ( M , , ρ l ) is a left-left H-Hopf quasimodule with
h m = ( h m ( 1 ) ) P L ( m 0 ) f o r a l l h H , m M .
(2) 
If ( M , , ρ r ) is a right-right H-Hopf quasimodule, then ( M , , ρ r ) is a right-right H-Hopf quasimodule with
m h = P R ( m 0 ) ( m ( 1 ) h ) f o r a l l h H , m M .

2.4. Yetter–Drinfeld Quasimodules

The following notion can be found in [23] (cf. [13,15]). Let H be a Hopf quasigroup. Let M be a counital coassociative left H-comodule with coaction ρ l and a unital left H-quasimodule with the action ▹. Then M is said to be a left-left H-Yetter–Drinfeld quasimodule, or, left H- YD -quasimodule, if the following conditions are satisfied:
h 1 m ( 1 ) h 2 m 0 = ( h 1 m ) ( 1 ) h 2 ( h 1 m ) 0 ,
( m ( 1 ) h ) g m 0 = m ( 1 ) ( h g ) m 0 ,
h ( m ( 1 ) g ) m 0 = ( h m ( 1 ) ) g m 0
for any h H and m M . The Equality (7) is equivalent to ρ l ( h m ) = ( h 1 m ( 1 ) ) S ( h 3 ) h 2 m 0 .
We will denote by H H YDQ the category of left-left Yetter–Drinfeld quasimodules over H with the obvious morphisms. Moreover, if we assume that M is a left H-module we say that M is a left-left Yetter–Drinfeld module over H. Obviously, the category H H YD of left-left Yetter–Drinfeld modules is a subcategory of H H YDQ .
By [23], Proposition 1.8], if the antipode S of H is bijective, then H H YDQ is a strict braided monoidal category with the braiding τ and its inverse τ 1 given by
τ M , N ( m n ) = m ( 1 ) n m 0 a n d τ M , N 1 ( m n ) = n 0 S 1 ( n ( 1 ) ) m
for any m M , n N and M , N H H YDQ .
Recall from [13], Definition 3.7] that a Hopf quasigroup B is called a coquasitriangular Hopf quasigroup if there is a linear map σ : B B F such that σ is invertible and the following conditions hold, for any x , y , z B ,
( Q C T 1 ) σ ( x y , z ) = σ ( y , z 1 ) σ ( x , z 2 ) , ( Q C T 2 ) σ ( x , y z ) = σ ( x 1 , y ) σ ( x 2 , z ) , ( Q C T 3 ) σ ( x 1 , y 1 ) y 2 x 2 = x 1 y 1 σ ( x 2 , y 2 ) .
Example 3.
Let ( B , σ ) be a coquasitriangular Hopf quasigroup and M be a counital coassociative left B-comodule satisfying () and (). We provide M a left H-quasimodule structure a x = σ ( a , x ( 1 ) ) x 0 for any x M and a B . Then M is a left B- YD -quasimodule.
Furthermore, Equation (6) holds. In fact, for any h , g B and x M
g ( S ( h ) x ) = σ ( S ( h ) , x ( 1 ) ) σ ( g , x 0 ( 1 ) ) x 00 = σ ( S ( h ) , x ( 1 ) 1 ) σ ( g , x ( 1 ) 2 ) x 0 = ( Q C T 1 ) σ ( g S ( h ) , x ( 1 ) ) x 0 = ( g ( S ( h ) ) ) x
Similarly for the identity: ( x S ( g ) ) h = x ( S ( g ) h ) , where one provides M a right H-quasimodule structure x a = σ ( x ( 1 ) , a ) x 0 for any x M and a B .

3. Rota–Baxter (Co)algebra Equation Systems

In this section, we introduce and study the notions of Rota–Baxter (co)algebra systems and give an approach to these equation systems.Our ideal may be regarded as a guide for further development.
Definition 2.
Let ( A , ) be an algebra and P a linear endomorphism of A. We say that P satisfiesRota–Baxter algebra equation systemwith regard to ∇, if the one of the following equation systems is satisfied:
( R B a 1 ) : P [ ( P i d ) i d ] = 0 , P ( i d P ) ( P P ) = 0 . ( R B a 2 ) : P [ ( i d P ) i d ] = 0 , P ( P i d ) ( P P ) = 0 .
Dually, we have
Definition 3.
Let ( C , Δ ) be a coalgebra and Q a linear endomorphism of C. We say that Q satisfiesRota–Baxter coalgebra equation systemwith regard to Δ, if the one of the following equation systems is satisfied:
( R B c 1 ) : [ ( Q i d ) i d ] Δ Q = 0 , ( i d Q ) Δ Q ( Q Q ) Δ = 0 . ( R B c 2 ) : [ ( i d Q ) i d ] Δ Q = 0 , ( Q i d ) Δ Q ( Q Q ) Δ = 0 .
For convenience’sake, we have
Lemma 2.
Let ( A , ) be an algebra and P a linear endomorphism of A. Let ( C , Δ ) be a coalgebra and Q a linear endomorphism of C. Let ( B , , Δ ) be a bialgebra and R and L linear endomorphisms of B.
(1) If P is a solution to Rota–Baxter algebra equation system (RBa1) or (RBa2), then ( A , , P , 1 ) is a Rota–Baxter algebra of weight 1 .
(2) If Q is a solution to Rota–Baxter coalgebra equation system (RBc1) or (RBc2), then ( C , Δ , Q , 1 ) is a Rota–Baxter coalgebra of weight 1 .
(3) If R is a solution to Rota–Baxter algebra equation system (RBa1) or (RBa2), and L a solution to Rota–Baxter coalgebra equation system (RBc1) or (RBc2), then the pentuple ( B , R , L , 1 , 1 ) is a Rota–Baxter bialgebra of weight ( 1 , 1 ) .
Example 4.
Let H be a Hopf quasigroup. In Example 1, we have a linear map P L = ε i d M from H M to itself and P R = i d M ε from M H to itself. In particular, we have two linear maps: P L = ε i d H and P R = i d H ε from H H to itself. It is easy to check that ( H , P L , 1 ) and ( H , P R , 1 ) are both Rota–Baxter algebra of weight 1 and Rota–Baxter coalgebra of weight 1 .
Furthermore, ( H , P R , P L , 1 , 1 ) and ( H , P L , P R , 1 , 1 ) are Rota–Baxter bialgebras of weight ( 1 , 1 ) .
Definition 4.
Let ( H , , Δ ) be a Hopf quasigroup and let B be a bialgebra. We say that B is atwo-side H-Hopf quasimodule bialgebraif ( B , , ρ l ) is a left-left H-Hopf quasimodule and ( B , , ρ r ) is a right-right H-Hopf quasimodule as defined in Definition 1, such that
ρ l ( a b ) = ρ l ( a ) ρ l ( b ) , ρ r ( a b ) = ρ r ( a ) ρ r ( b ) ,
Δ ( h a ) = Δ ( h ) Δ ( a ) , Δ ( a g ) = Δ ( a ) Δ ( g ) ,
( i d Δ ) ρ l = ( ρ l i d ) Δ , ( Δ i d ) ρ r = ( i d ρ r ) Δ ,
φ l ( i d ) = ( φ l i d ) , φ r ( i d ) = ( i d φ r ) ,
for any h , g H and a , b B .
Note that if H is a Hopf algebra, then B is called a two-side H-Hopf module bialgebra.
Theorem 1.
Let H be a Hopf quasigroup and let M be a two-side H-Hopf quasimodule bialgebra. Set P R ( x ) = x 0 S ( x ( 1 ) ) and P L ( x ) = S ( x ( 1 ) ) x 0 for any x M . If Equation (6) holds, then ( M , P R , P L , 1 , 1 ) and ( M , P R , P L , 1 , 1 ) are Rota–Baxter bialgebras of weight ( 1 , 1 ) .
Proof. 
We show that P R is a solution to Rota–Baxter algebra equation system (RBa2). For any m , n M , we have
P R ( m P R ( n ) ) = ( m P R ( n ) ) 0 S ( ( m P R ( n ) ) ( 1 ) ) = ( 10 ) ( m 0 P R ( n ) 0 ) S ( m ( 1 ) P R ( n ) ( 1 ) ) = L e m m a 1 ( 2 ) ( m 0 P R ( n ) ) S ( m ( 1 ) ) = ( 13 ) m 0 [ n 0 S ( n ( 1 ) ) S ( m ( 1 ) ) ] = ( 6 ) m 0 [ n 0 S ( m ( 1 ) n ( 1 ) ) ] = ( 13 ) ( m 0 n 0 ) S ( m ( 1 ) n ( 1 ) ) = ( 10 ) P R ( m n )
and
P R ( P R ( m ) n ) = ( P R ( m ) n ) 0 S ( ( P R ( m ) n ) ( 1 ) ) = ( 10 ) ( P R ( m ) 0 n 0 ) S ( P R ( m ) ( 1 ) n ( 1 ) ) = L e m m a 1.3 ( 2 ) ( P R ( m ) n 0 ) S ( n ( 1 ) ) = ( 13 ) P R ( m ) P R ( n ) .
Therefore, we conclude that P R is a solution to Rota–Baxter algebra equation system (RBa2). A similar computation for P L gives rise to that P L is a solution to Rota–Baxter algebra equation system (RBa1).
It follows from Lemma 1(1) that ( M , P R ) and ( M , P L ) are idempotent Rota–Baxter algebras with the weight 1 .
We also compute, for any a M
( ( i d P R ) Δ P R ) ( a ) = ( i d P R ) ( Δ ( a 0 S ( a ( 1 ) ) ) ) = ( 11 ) a 01 S ( a ( 1 ) ) 1 P R ( a 02 S ( a ( 1 ) ) 2 ) = P r o p o s i t i o n 1.4 a 01 S ( a ( 1 ) ) P R ( a 02 ) = a 01 S ( a ( 1 ) ) ( a 020 S ( a 02 ( 1 ) ) ) = ( 12 ) ( a 001 S ( a ( 1 ) ) ) ( a 002 S ( a 0 ( 1 ) ) ) = ( 11 ) ( a 0 S ( a ( 1 ) ) ) 1 ( a 0 S ( a ( 1 ) ) ) 2 = Δ ( a 0 S ( a ( 1 ) ) ) = ( Δ P R ) ( a )
and similarly one can obtain: ( P R i d ) Δ P R = ( P R P R ) Δ . Therefore, P R is a solution to Rota–Baxter coalgebra equation system (RBc2) and so ( M , P R ) is an idempotent Rota–Baxter coalgebra with the weight 1 .
For P L , one has
Δ P L ( a ) = Δ ( S ( a ( 1 ) ) a 0 ) = ( 11 ) ( S ( a ( 1 ) 2 ) a 01 ) ( S ( a ( 1 ) 1 ) a 02 ) = ( S ( a 0 ( 1 ) ) a 001 ) ( S ( a ( 1 ) ) a 002 ) = ( 12 ) ( S ( a 01 ( 1 ) ) a 010 ) ( S ( a ( 1 ) ) a 02 ) = P L ( a 01 ) ( S ( a ( 1 ) ) a 02 ) = P r o p o s i t i o n 1.4 P L ( S ( a ( 1 ) 2 ) a 01 ) ( S ( a ( 1 ) 1 ) a 02 ) = ( 11 ) ( P L i d ) Δ ( S ( a ( 1 ) ) a 1 ) = ( P L i d ) Δ P L ( a )
for any a M . Thus, P L satisfies the first identity in (RBc1). Similarly for the second one in (RBc1) and so P L is a solution to Rota–Baxter coalgebra equation system (RBc1).
Therefore, it follows from Lemma 2(3) and Lemma 1(1) that ( M , P L , P R , 1 , 1 ) and ( M , P R , P L , 1 , 1 ) are idempotent Rota–Baxter bialgebra with the weight ( 1 , 1 ) .
This completes the proof. □
In what follows, we use the notion of Radford’s admissible mapping system for Hopf algberas ([25]) to construct Rota–Baxter bialgebra.
Proposition 2.
Let B be a unital counital associative coassociative bialgebra and H a Hopf algebra with an antipode S. Suppose there are two bialgebra homomorphism p : B H and j : H B such that p j = i d H . Define two linear maps P L : B B by P L ( b ) = j S p ( b 1 ) b 2 and P R : B B by P R ( b ) = b 1 j S p ( b 2 ) for any b B . Then ( B , P L , P R , 1 , 1 ) and ( B , P R , P L , 1 , 1 ) are Rota–Baxter bialgebras with the weight ( 1 , 1 ) . Furthermore, P L 2 = P L and P R 2 = P R .
Proof. 
For this, we want show that P L is a solution to the equation systems (RBa1) and (RBc1), and P R is a solution to the equation systems (RBa2) and (RBc2).
In fact, we have, for any a , b B
P L ( P L ( a ) b ) = P L ( ( j S p ( a 1 ) a 2 ) b ) = [ j S p ( b 1 ) ( j S p ( a 3 ) j S 2 p ( a 2 ) ) ̲ ] [ ( j S p ( a 1 ) a 4 ) b 2 ] = j S p ( b 1 ) ( ( j S p ( a 1 ) a 2 ) b 2 ) = [ j S p ( b 1 ) j S p ( a 1 ) ] [ a 2 b 2 ] = P L ( a b ) .
and
P L ( a P L ( b ) ) = P L ( a ( j S p ( b 1 ) b 2 ) ) = [ ( j S p ( b 3 ) j S 2 p ( b 2 ) ) ̲ j S p ( a 1 ) ] [ a 2 ( j S p ( b 1 ) b 4 ) ] = j S p ( a 1 ) [ a 2 ( j S p ( b 1 ) b 2 ) ] = j S p ( a 1 ) ( a 2 P L ( b ) ) = P L ( a ) P L ( b ) .
This shows that P L is a solution to Rota–Baxter algebra equation system (RBa1).
For (RBc1), we have,
P L ( P L ( a ) 1 ) P L ( a ) 2 = j S p ( ( P L ( a ) 1 ) 1 ) ( P L ( a ) 1 ) 2 P L ( a ) 2 = j S p ( ( ( j S p ( a 1 ) a 2 ) 1 ) 1 ) ( ( j S p ( a 1 ) a 2 ) 1 ) 2 ( j S p ( a 1 ) a 2 ) 2 = P L ( a 2 ) j S p ( a 1 ) a 3 = P L ( a ) 1 P L ( a ) 2 .
and
P L ( a ) 1 P L ( P L ( a ) 2 ) = P L ( a ) 1 j S p ( ( P L ( a ) 2 ) 1 ) ( P L ( a ) 2 ) 2 ) = ( j S p ( a 1 ) a 2 ) 1 j S p ( ( ( j S p ( a 1 ) a 2 ) 2 ) 1 ) ( ( j S p ( a 1 ) a 2 ) 2 ) 2 ) = j S p ( a 11 ) a 12 j S p ( a 21 ) a 22 = P L ( a 1 ) P L ( a 2 ) .
Similarly for P R satisfying (RBa2) and (RBc2).
Therefore, it follows from Lemma 2.3(3) that ( B , P L , P R , 1 , 1 ) and ( B , P R , P L , 1 , 1 ) are Rota–Baxter bialgebras with the weight ( 1 , 1 ) .
Finally, we have
P L 2 ( b ) = j S p [ ( j S p ( b 1 ) b 2 ) 1 ] ( j S p ( b 1 ) b 2 ) 2 = j S p ( j S p ( b 2 ) b 3 ) ( j S p ( b 1 ) b 4 ) = ( j S p ( b 3 ) j S 2 p ( b 2 ) ) ( j S p ( b 1 ) b 4 ) = j S p ( b 1 ) b 2 = P L ( b )
and similarly P R 2 = P R . □
Proposition 3.
Let A be a bialgebra. If P and Q satisfy Rota–Baxter Equation (co)algebra systems (RBa1)and (RBc1) (resp. (RBa2) and (RBc2)) such that P Q = Q P , then the composite Q P of P and Q satisfies Rota–Baxter (co)algebra systems (RBa1) and (RBc1) (resp. (RBa2) and (RBc2)).
Proof. 
For (RBa1), computing we have, for any a , b A
P Q ( a b ) = P Q ( Q ( a ) b ) = Q P ( Q ( a ) b ) = Q P ( P Q ( a ) b ) = P Q ( P Q ( a ) b ) ,
and
P Q ( a ) P Q ( b ) = P ( Q ( a ) P Q ( b ) ) = P ( Q ( a ) Q P ( b ) ) = P Q ( a Q P ( b ) ) = P Q ( a P Q ( b ) ) .
Similar for (RBa2).
For (RBc1), one computes, for any c C
( P Q ) ( c ) 1 ( P Q ) ( c ) 2 = P ( ( P Q ) ( c ) 1 ) ( P Q ) ( c ) 2 = P Q P ( ( Q P ) ( c ) 1 ) ( Q P ) ( c ) 2 = ( P Q ) ( ( P Q ) ( c ) 1 ) ( P Q ) ( c ) 2 .
and
( P Q ) ( c 1 ) ( P Q ) ( c 2 ) = P ( ( Q P ) ( c ) 1 ) Q P ( ( Q P ) ( c ) 2 ) = P ( ( Q P ) ( c ) 1 ) P Q ( ( Q P ) ( c ) 2 ) = P 2 ( Q ( c ) 1 ) P Q ( Q ( c ) 2 ) = P ( Q ( c ) 1 ) P Q ( Q ( c ) 2 ) = P ( Q ( c ) 1 ) Q P ( Q ( c ) 2 ) = ( P Q ) ( c ) 1 ( P Q ) ( ( P Q ) ( c ) 2 ) .
Similar for (RBc2).
This completes the proof. □
We finish this section with the following result.
Proposition 4.
Let B = B 1 B 2 be a direct sum of two bi-ideals B 1 and B 2 of a bialgebra B. Then for any P L i on B i ( i = 1 , 2 ) (resp. P R i on B i ( i = 1 , 2 ) ) satisfying Rota–Baxter (co)algebra equation systems (RBa1) and (RBc1) (resp. (RBa2) and (RBc2)), the linear map P L : B B given by P L ( x 1 , x 2 ) = ( P L 1 ( x 1 ) , P L 2 ( x 2 ) ) (resp. P R : B B given by P R ( x 1 , x 2 ) = ( P R 1 ( x 1 ) , P R 2 ( x 2 ) ) ) for any x 1 A 1 , x 2 A 2 , solves Rota–Baxter (co)algebra equation systems (RBa1) and (RBc1) (resp. (RBa2) and (RBc2)).

4. Compatible Rota–Baxter Bialgebras and Rota–Baxter Hopf Algebras

We begin with the notion of a compatible Rota–Baxter bialgebra by modifying the definition of a Rota–Baxter bialgebra given in [19] as follows.
Definition 5.
A septuple ( B , , Δ , P , Q , λ , γ ) is called acompatible Rota–Baxter bialgebraof weight ( λ , γ ) if ( B , , Δ ) is a bialgebra, ( B , , P , λ ) is a Rota–Baxter algebra of weight λ, and ( B , Δ , Q , γ ) is a Rota–Baxter coalgebra of weight γ such that
( R B b 1 ) : ( P P ) P ( i d P ) = Q ( Q i d ) + λ ( Q ) , ( Q Q ) Δ ( i d Q ) Δ Q = ( P i d ) Δ P + γ ( Δ P )
or
( R B b 2 ) : ( P P ) P ( P i d ) = Q ( i d Q ) + λ ( Q ) , ( Q Q ) Δ ( Q i d ) Δ Q = ( i d P ) Δ P + γ ( Δ P )
As a matter of convenience, we have
Lemma 3.
Let P and Q be two linear endomorphisms of a bialgebra ( B , , Δ ) . Let P be a solution to Rota–Baxter algebra equation system (RBa1) and (RBa2), and let Q be a solution to Rota–Baxter coalgebra equation system (RBc1) and (RBc2). Then ( B , , Δ , P , Q , 1 , 1 ) and ( B , , Δ , Q , P , 1 , 1 ) are Rota–Baxter bialgebra of weight ( 1 . 1 ) .
Proposition 5.
With the notations as in Proposition 2. Then ( B , , Δ , P L , P R , 1 , 1 ) and ( B , , Δ , P R , P L , 1 , 1 ) are compatible Rota–Baxter bialgebras of weight ( 1 . 1 ) .
Definition 6.
An octuple ( H , , Δ , S , P , Q , λ , γ ) is called aRota–Baxter Hopf algebraof weight ( λ , γ ) if the quadruple ( H , , Δ , S ) is a Hopf algebra with antipode S and the septuple ( H , , Δ , P , Q , λ , γ ) is a compatible Rota–Baxter bialgebra, such that the antipode S of H is compatible with P and Q in the following sense that
S P = P S a n d S Q = Q S
Example 5.
Let H be a Hopf algebra and A a braided Hopf algebra in the Yetter–Drinfeld module category H H YD . Recall from [25] that the Radford’s biproduct A H have the following Hopf algebra structures:
( a h ) ( b g ) = a ( h 1 b ) h 2 g , 1 A H = 1 A 1 H , ε A H = ε A ε H , Δ A H ( a h ) = ( a 1 a 2 ( 1 ) h 1 ) ( a 2 ( 0 ) h 2 ) , S A H ( a h ) = ( 1 S H ( a ( 1 ) h ) ) ( S A ( a 0 ) 1 )
for all a , b A and h , g H . Then there are two bialgebra homomorphisms p : A H H , a h ε ( a ) h and j : H A H , h 1 h such that p j = i d H . By Proposition 2, we can define two linear maps P L , P R : A H A H by
P L ( a h ) = S H ( a ( 1 ) 2 h 2 ) a 0 S H ( a ( 1 ) 1 h 1 ) h 3
and P R ( a h ) = a ε ( h ) 1 . Therefore, P L is a solution to Rota–Baxter algebra equation system (RBa1) and coalgebra equation system (RBc1), and P R is a solution to Rota–Baxter algebra equation system (RBa2) and coalgebra equation system (RBc2).
Furthermore, one can directly show that S A H P L = P R S A H as follows:
( S A H P L ) ( a h ) = S A H [ ( 1 S H ( a ( 1 ) h 1 ) ) ( a 0 h 2 ) ] = S A H ( a 0 h 2 ) S A H ( 1 S H ( a ( 1 ) h 1 ) ) = ( 1 S H ( a 0 ( 1 ) h 2 ) ) ( S A ( a 00 ) 1 ) ( 1 S H [ S H ( a ( 1 ) h 1 ) ] ) = ( 1 S H ( a 0 ( 1 ) h 2 ) ) ( S A ( a 00 ) S H [ S H ( a ( 1 ) h 1 ) ] ) = S H ( a 0 ( 1 ) h 2 ) 1 S A ( a 00 ) S H ( a 0 ( 1 ) h 2 ) 2 S H [ S H ( a ( 1 ) h 1 ) ] = S H ( a ( 1 ) h ) 1 S A ( a 00 S H ( a ( 1 ) h ) 2 S H [ ( S H ( a ( 1 ) h ) 3 ] = S H ( a ( 1 ) h ) S ( a 0 ) 1 = P R [ ( 1 S H ( a ( 1 ) h ) ) ( S A ( a 0 ) 1 ) ] = ( P R S A H ) ( a h ) .
Furthermore, similar for P L S A H = S A H P R . Thus, P L and P R satisfy the Condition (14).
Therefore, ( A H , , Δ A H , S A H , P L , P R , 1 , 1 ) is a Rota–Baxter Hopf algebra of weight ( 1 , 1 ) .
Proposition 6.
Let ( H , , Δ ) be a Hopf algebra with antipode S. Let A be a Hopf algebra with antipode S. If A is a two-side H-Hopf module bialgebra such that, for h , g H , a A
S ( a h ) = S ( h ) S ( a ) , S ( g a ) = S ( a ) S ( g ) ,
ρ l ( S ( a ) ) = ( S S ) T ρ r ( a ) , ρ r ( S ( a ) ) = ( S S ) T ρ l ( a ) ,
then ( H , , Δ , S , P L , P R , 1 , 1 ) is a Rota–Baxter Hopf algebra of weight ( 1 , 1 ) .
Proof. 
By Theorem 1, we only show that P R S = S P L and P L S = S P R . In fact, we have
( P R S ) ( a ) = S ( a ) 0 S ( S ( a ) ( 1 ) ) = ( 16 ) S ( a 0 ) S [ S ( a ( 1 ) ) ] = ( 15 ) S [ S ( a ( 1 ) ) a 0 ] = ( S P L ) ( a )
and similarly for P L S = S P R .
This completes the proof. □
Theorem 2.
With the notations as in Proposition 2. If B is a Hopf algebra with antipode S, then ( B , , Δ , P L , P R , 1 , 1 ) is a Rota–Baxter Hopf algebra of weight ( 1 , 1 ) .
Proof. 
By Proposition 5, we only show that P R S = S P L and P L S = S P R . Actually, we have
( S P L ) ( b ) = S [ j S p ( b 1 ) b 2 ] = S ( b 2 ) S j S p ( b 1 ) = S ( b 2 ) j S p S ( b 1 ) = S ( b ) 1 j S p S ( b ) 2 = ( P R S ) ( b )
and similarly for P L S = S P R . □
Example 6.
With the notations as in Proposition 2. Then B can be made into a two-side H-Hopf module bialgebra with the following H-module and H-comodule structures, for any h H and b B
h b = j ( h ) b , ρ l : B H B , b p ( b 1 ) b 2 , b h = b j ( h ) , ρ r : B B H , b b 1 p ( b 2 ) .
It is easy to check that the conditions: (10)–() are satisfied.
Equation (6) also holds. In order to check Equation (15), we have
S ( h b ) = S [ j ( h ) b ] = S ( b ) S j ( h ) = S ( b ) j S ( h ) = S ( b ) S ( h )
and similarly for S ( h b ) = S ( b ) S ( h ) .
Doing calculation one has
ρ l ( S ( b ) ) = p S ( b 2 ) S ( b 1 ) = ( S S ) ( p ( b 2 ) b 1 ) = ( S S ) T ρ r ( b )
and ρ r ( S ( b ) ) = ( S S ) T ρ l ( b ) . This proves Equation ().
Then we have two linear maps P L , P R : B B by
P L ( b ) = S ( b ( 1 ) ) b 0 = S p ( b 1 ) b 2 = j S p ( b 1 ) b 2
and
P R ( b ) = b 0 S ( b ( 1 ) ) = b 1 S p ( b 2 ) = b 1 j S p ( b 2 )
for any b B .
It follows from Proposition 6 that we also can obtain Theorem 2.

Author Contributions

Conceptualization, Y.G. and T.M.; Investigation, S.W. All authors did research, calculations and studied. All authors have read and agreed to the published version of the manuscript.

Funding

The National Natural Science Foundation of China (Grant No. 11871144).

Institutional Review Board Statement

Not applicable.

Informed Consent Statement

Not applicable.

Data Availability Statement

Not applicable.

Acknowledgments

The authors are very grateful to the anonymous referee for their thorough review of this work and their comments. The first author thanks the “Start-up fund for scientific research of talents introduced by Nanjing Tech University” and the second author thanks the financial support of the National Natural Science Foundation of China (Grant No. 11871144).

Conflicts of Interest

The authors declare no conflict of interest.

References

  1. Rota, G. Baxter algebras and combinatorial identities. Bull. Am. Math. Soc. 1969, 75, 325–329. [Google Scholar] [CrossRef] [Green Version]
  2. Bai, R.P.; Guo, L.; Li, J.Q.; Wu, Y. Rota–Baxter 3-Lie algebras. J. Math. Phys. 2013, 54, 063504. [Google Scholar] [CrossRef] [Green Version]
  3. Bai, C.M.; Guo, L.; Ni, X. Relative Rota–Baxter operators and tridendriform algebras. J. Algebra Appl. 2013, 12, 1350027. [Google Scholar] [CrossRef]
  4. Bokut, L.A.; Chen, Y.Q.; Qiu, J.J. Gröbner-Shirshov bases for associative algebras with multiple operators and free Rota–Baxter algebras. J. Pure Appl. Algebra 2010, 214, 89–100. [Google Scholar] [CrossRef] [Green Version]
  5. Chen, Y.Q.; Mo, Q.H. Embedding dendriform algebra into its universal enveloping Rota–Baxter algebra. Proc. Am. Math. Soc. 2011, 139, 4207–4216. [Google Scholar] [CrossRef] [Green Version]
  6. Connes, A.; Kreimer, D. Renormalization in quantum field theory and the Riemann-Hilbert problem, I: The Hopf algebra structure of graphs and the main theorem. Comm. Math Phys. 2000, 210, 249–273. [Google Scholar] [CrossRef] [Green Version]
  7. Ebrahimi-Fard, K.; Guo, L. Multiple zeta values and Rota–Baxter algebras. Integers 2008, 8, A4. [Google Scholar]
  8. Ebrahimi-Fard, K.; Guo, L. Free Rota–Baxter algebras and rooted trees. J. Algebra Appl. 2008, 7, 167–194. [Google Scholar] [CrossRef] [Green Version]
  9. Guo, L. Properties of free Baxter algebras. Adv. Math. 2000, 151, 346–374. [Google Scholar] [CrossRef] [Green Version]
  10. Guo, L. An Introduction to Rota–Baxter Algebras; Higher Education Press: Beijing, China, 2012. [Google Scholar]
  11. Guo, L.; Keigher, W. Baxter algebras and shuffle products. Adv. Math. 2000, 150, 117–149. [Google Scholar] [CrossRef] [Green Version]
  12. Klim, J.; Majid, S. Hopf quasigroups and the algebraic 7-sphere. J. Algebra 2010, 323, 3067–3110. [Google Scholar] [CrossRef] [Green Version]
  13. Zhang, T.; Wang, S.H.; Wang, D.G. A new approach to braided monoidal categories. J. Math. Phys. 2019, 60, 013510. [Google Scholar] [CrossRef]
  14. Fang, X.L.; Wang, S.H. Twisted smash product for Hopf quasigroups. J. Southeast Univ. (English Ed.) 2011, 27, 343–346. [Google Scholar]
  15. Gu, Y.; Wang, S.H. Hopf quasicomodules and Yetter-Drinfel’d quasicomodules. Comm. Algebra 2020, 48, 351–379. [Google Scholar] [CrossRef]
  16. Gu, Y.; Wang, S.H. Double centralizer properties related to (co)triangular Hopf coquasigroups. Comm. Algebra 2021, 49, 662–686. [Google Scholar] [CrossRef]
  17. Zhang, S.L.; Wang, S.H. Fundamentals of quasigroup Hopf group coalgebras. J. Southeast Univ. (English Ed.) 2021, 37, 114–118. [Google Scholar]
  18. Zhang, T.; Gu, Y.; Wang, S.H. Hopf quasimodules and Yetter-Drinfel’d modules over Hopf Quasigroups. Algebra Colloq. 2021, 28, 213–242. [Google Scholar] [CrossRef]
  19. Ma, T.S.; Liu, L.L. Rota–Baxter coalgebras and Rota–Baxter bialgebras. Linear Multilinear Algebra 2016, 64, 968–979. [Google Scholar] [CrossRef] [Green Version]
  20. Sweedler, M.E. Hopf Algebras; Benjami: New York, NY, USA, 1969. [Google Scholar]
  21. Pérez-Izquierdo, J.M. Algebras, hyperalgebras, nonassociative bialgebras and loops. Adv. Math. 2007, 208, 834–876. [Google Scholar] [CrossRef]
  22. Ebrahimi-Fard, K. Rota–Baxter Algebras and the Hopf Algebra of Renormalization. Ph.D. Dissertation, University of Bonn, Bonn, Germany, 2006. [Google Scholar]
  23. Alonso Álvarez, J.N.; Fernéz Vilaboa, J.M.; González Rodríguez, R.; Soneira Calvo, C. Projections and Yetter-Drinfel’d modules over Hopf (co)quasigroups. J. Algebra 2015, 443, 153–199. [Google Scholar] [CrossRef]
  24. Brzeziński, T.; Jiao, Z.M. Actions of Hopf quasigroups. Comm. Algebra 2012, 40, 681–696. [Google Scholar] [CrossRef] [Green Version]
  25. Radford, D.E. The structure of a Hopf algebra with a projection. J. Algebra 1985, 92, 322–347. [Google Scholar] [CrossRef] [Green Version]
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Gu, Y.; Wang, S.; Ma, T. Rota–Baxter (Co)algebra Equation Systems and Rota–Baxter Hopf Algebras. Mathematics 2022, 10, 426. https://doi.org/10.3390/math10030426

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Gu Y, Wang S, Ma T. Rota–Baxter (Co)algebra Equation Systems and Rota–Baxter Hopf Algebras. Mathematics. 2022; 10(3):426. https://doi.org/10.3390/math10030426

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Gu, Yue, Shuanhong Wang, and Tianshui Ma. 2022. "Rota–Baxter (Co)algebra Equation Systems and Rota–Baxter Hopf Algebras" Mathematics 10, no. 3: 426. https://doi.org/10.3390/math10030426

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