Abstract
Representations and cohomologies of Hom--Jordan Lie supertriple systems are established. As an application, Nijenhuis operators and abelian extensions of Hom--Jordan Lie supertriple systems are discussed. We obtain the infinitesimal deformation generated by virtue of a Nijenhuis operator. It is obtained that the sufficient and necessary condition for the equivalence of abelian extensions of Hom--Jordan Lie supertriple systems.
Keywords:
Hom-δ-Jordan Lie supertriple system; cohomology; deformation; Nijenhuis operator; abelian extension MSC:
17B40; 17B56; 17B75
1. Introduction
In this paper, we pay our main attention to Hom--Jordan Lie supertriple systems over an arbitrary field. As is well-known, Lie triple systems have important applications in elementary particle theory and the theory of quantum mechanics [1]. Some results on Lie triple systems, including simple Lie triple systems over an algebraically closed field [2], the Yamaguti cohomology theory [3,4], infinitesimal deformations, abelian extensions [5], etc. were studied. Okubo reformulated the para-statistics as Lie supertriple systems and explained the relationship between Lie supertriple systems and ortho-symplectic supertriple systems [6]. In [7], the authors introduced -Jordan Lie supertriple systems, which are a generalization of Lie supertriple systems. Some examples of quasi-classical -Lie supertriple systems were given over a field of characteristic not two [8]. The Jordan superalgebra of F-type from Jordan Lie supertriple systems were discussed [9]. Later, Ma and Chen obtained the cohomology and deformations of -Jordan Lie triple systems in 2017 [10]. In [11], the authors determined derivations and deformations of -Jordan Lie supertriple systems. In 2022, we obtained 1-parameter formal deformations and abelian extensions of Lie color triple systems [12].
In recent years, structures and representations of many Hom-type algebras have been obtained [13,14,15,16,17,18,19,20,21,22,23,24]. In particular, the notion of Hom-Lie triple systems was introduced in [14]. Hom-Lie triple systems are ternary Hom–Nambu algebras whose triple product is left anti-symmetric. When the twisting maps of Hom–Lie triple systems are all equal to the identity map, one recovers Lie triple systems. In 2019, Chen and his students gave that cohomologies and 1-parameter formal deformations of Hom--Jordan Lie triple systems [25]. In 2022, we obtained central extensions and Nijenhuis operators of Hom--Jordan Lie triple systems [26].
The purpose of this paper is to consider the cohomology theory and deformations of Hom--Jordan Lie supertriple systems based on some work in [3,4,10,12,13,25,26,27]. The paper is organized as follows. Section 2 is devoted to some basic definitions and the cohomology theory of multiplicative Hom--Jordan Lie supertriple systems. In Section 3, we discuss Nijenhuis operators of Hom--Jordan Lie supertriple systems and obtain the infinitesimal deformation generated using a Nijenhuis operator. Section 4 is dedicated to the abelian extension theory of multiplicative Hom--Jordan Lie supertriple systems. We show the sufficient and necessary condition for the equivalence of abelian extensions.
Throughout this paper, denotes an arbitrary field, and its characteristic is zero.
2. Preliminaries
We first recall some basic facts and definitions of Hom-Lie triple systems.
Definition 1
([14]). A Hom-Lie triple system consists of an -vector space T, a trilinear map , and linear maps for , called twisted maps, such that for all ,
If occurs in some expression in this paper, we always regard x as a -homogeneous element and as the -degree of x.
Definition 2
([28]). A Hom-Lie supertriple system consists of a -graded vector space over together with a trilinear map , and even linear maps for , called twisted maps, such that for all ,
Definition 3.
A Hom-δ-Jordan Lie supertriple system consists of a -graded vector space over together with a trilinear map , and even linear maps for , called twisted maps, such that for all ,
Clearly, is a Hom--Jordan Lie triple system, and the case of defines a Lie triple system, so any Hom--Jordan Lie supertriple system is the generalization of a Lie triple system.
A Hom--Jordan Lie supertriple system is said to be multiplicative if and , and denoted by .
A morphism of Hom--Jordan Lie supertriple system is a linear map satisfying and for . An isomorphism is a bijective morphism.
Following the representation theory of Lie triple systems was studied by Yamaguti, we generalize the notion of the representation to Hom--Jordan Lie supertriple systems.
Definition 4.
Let be a multiplicative Hom-δ-Jordan Lie supertriple system, V a -graded vector space over , and . V is called a -module with respect to A if there exists a bilinear map , such that for all ,
where .
Then, θ is called the representation of on V with respect to A. In the case , V is called the trivial -module with respect to A.
In particular, let , , and . Then, and (7)–(10) hold. In this case, T is said to be the adjoint -module and is called the adjoint representation of on itself with respect to .
As is the case of general algebras, we introduce the semidirect product of a multiplicative Hom--Jordan Lie supertriple systems and its module.
Proposition 1.
Let θ be a representation of a multiplicative Hom-δ-Jordan Lie supertriple system on V with respect to A. Define the operation by
and define the twisted map by
Then is a multiplicative Hom-δ-Jordan Lie supertriple system.
Proof.
Using , we obtain
and
Note that is a linear map and, using (7), we have
Thus, is a multiplicative Hom--Jordan Lie supertriple system. □
Let be a representation of on V with respect to A. If an n-linear map satisfies
then f is called an n-Hom-cochain on T. Denote by the set of all n-Hom-cochains, .
Definition 5.
For , the coboundary operator is defined as follows.
- If then
- If then
- If then
- If then
Theorem 1.
The coboundary operator defined above satisfies
Proof.
From the definition of the coboundary operator it follows immediately that implies . Then we only need to prove In fact, by (7)–(10), we get
Therefore, the proof is complete. □
For , the map is called an n-Hom-cocycle if . We denote by the subspace spanned by n-Hom-cocycles and .
Since , is a subspace of . Hence, we can define a cohomology space of as the factor space
3. Nijenhuis Operators of Hom--Jordan Lie Supertriple Systems
In this section, we study infinitesimal deformations of Hom--Jordan Lie supertriple systems. We introduce the notion of Nijenhuis operators for Hom--Jordan Lie supertriple systems, and obtain trivial deformations using this kind of Nijenhuis operators.
Let be a Hom--Jordan Lie supertriple system and be an even trilinear map. Consider a -parametrized family of linear operations:
where is a formal variable, and
If endow T with Hom--Jordan Lie supertriple system structure, which is denoted by , then we call that generates a -parameter infinitesimal deformation of Hom--Jordan Lie supertriple system.
Theorem 2.
ψ generates a λ-parameter infinitesimal deformation of Hom-δ-Jordan Lie supertriple system T is equivalent to (i) ψ itself defines a Hom-δ-Jordan Lie supertriple system structure on T and (ii) ψ is a 3-Hom-cocycle of T.
Proof.
and
we have
From the equality
it follows that
For the equality
the left hand side is equal to
and the right hand side is equal to
Thus, we have
and
A deformation is said to be trivial if there exists an even linear map such that for we have
It is clear that
and
Thus, we have
From the cohomology theory discussed in Section 2, (16) can be represented in terms of 1-coboundary as . Moreover, it follows from (16) and (17) that N must satisfy the following condition
Definition 6.
Theorem 3.
Let N be a Nijenhuis operator for T. Then, a deformation of T can be obtained by putting
Furthermore, this deformation is a trivial one.
4. Abelian Extensions of Hom--Jordan Lie Supertriple Systems
In this section, we show that associated with any abelian extension, there is a representation and a 3-Hom-cocycle.
An ideal of a Hom--Jordan Lie supertriple system T is a subspace I such that An ideal I of a Hom--Jordan Lie supertriple system is called an abelian ideal if, moreover, Notice that implies that and
Definition 7.
Let , , and be Hom-δ-Jordan Lie supertriple systems and , be homomorphisms. The following sequence of Hom-δ-Jordan Lie supertriple systems is a short exact sequence if and
In this case, we call an extension of T by V, and denote it by . It is called an abelian extension if V is an abelian ideal of , i.e., for all
A section of consists of linear maps such that
Definition 8.
Two extensions of Hom-δ-Jordan Lie supertriple systems and are equivalent. If there exists a Hom-δ-Jordan Lie supertriple system homomorphism such that the following diagram commutes
Let be an abelian extension of T by V, and a linear mapping be a section. Define maps by
Clearly, the following fact holds, i.e.,
for all
Let be a section of the abelian extension. Define the following map :
for all
Theorem 4.
Proof.
By the equality
The left hand side shows that
Similarly, the right side is equal to
Thus, it follows that
Therefore, is a 3-Hom-cocycle. □
Theorem 5.
Let T be a Hom-δ-Jordan Lie surpetriple system, be a T-module and ω be a 3-Hom-cocycle, then is a Hom-δ-Jordan Lie surpetriple system under the following multiplication:
and
Theorem 6.
Two abelian extensions of -δ- Lie supertriple systems and are equivalent ⟺ ω and are in the same cohomology class.
Proof.
Let be the corresponding homomorphism. Thus,
Note that F is an equivalence of extensions, so there is such that
Then we obtain that
Therefore, , we get and are in the same cohomology class.
If and are in the same cohomology class, we assume that , then F defined by (27) is an equivalence. □
Author Contributions
Writing—original draft, Q.L.; Writing—review & editing, L.M. All authors have read and agreed to the published version of the manuscript.
Funding
Supported by NNSF of China (No. 11801211), Science Foundation of Heilongjiang Province (No. QC2016008), the Fundamental Research Funds in Heilongjiang Provincial Universities (No. 145209132).
Data Availability Statement
Not applicable.
Conflicts of Interest
The authors declare no conflict of interest.
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