Abstract
Let m and n be fixed positive integers. Suppose that is a von Neumann algebra with no central summands of type , and is a Lie-type higher derivation. In continuation of the rigorous and versatile framework for investigating the structure and properties of operators on Hilbert spaces, more facts are needed to characterize Lie-type higher derivations of von Neumann algebras with local actions. In the present paper, our main aim is to characterize Lie-type higher derivations on von Neumann algebras and prove that in cases of zero products, there exists an additive higher derivation and an additive higher map , which annihilates every commutator with such that We also demonstrate that the result holds true for the case of the projection product. Further, we discuss some more related results.
Keywords:
Lie derivation; multiplicative Lie-type derivation; multiplicative Lie-type higher derivation; von Neumann algebra MSC:
47B47; 16W25; 46K15
1. Introduction
One of the mathematical disciplines called von Neumann algebras, pioneered by John von Neumann, not only plays a pivotal role in advancing pure mathematics but also finds crucial applications in quantum mechanics, functional analysis and other areas of theoretical physics, underscoring its enduring relevance and impact on diverse scientific domains. Let be a commutative ring with unity, be an algebra over and be the center of . Recall that an -linear map is called a derivation on if for all . An -linear map is called a Lie derivation (resp. Lie triple derivation) on if for all ), where is the usual Lie product. Let be the set of non-negative integers and be a family of additive mappings such that , the identity map on . Then, is called
- a higher derivation of if for every for all
- a Lie higher derivation of if for every for all
- a triple-higher derivation of if for every for all
Abdullaev [1] initiated the study of Lie n-derivations on von Neumann algebras. Define the sequence of polynomials: and for all with . Here, is known as the -commutator. For a fixed positive integer an additive (linear) map is called a Lie n-higher derivation if
for all . In particular, by giving different values to n, we obtain Lie higher derivation, Lie triple-higher derivation and Lie n-higher derivations. These derivations collectedly are referred to as Lie-type higher derivations. Since the last few decades, examining the various properties of derivations defined through the well-known rule given by Leibniz under the influence of various algebraic structures is a vast topic of study among the algebraists. Bresar [2] characterized an additive Lie derivation as the sum of a derivation and an additive map on a prime ring with , where denotes the characteristic of . Johnson [3] worked on Lie derivations on -algebras and proved that every continuous linear Lie derivation from a -algebra into a Banach -bimodule can be written as (i.e., every continuous linear Lie derivation from a -algebra into a Banach -bimodule is standard), where is a derivation and (here, denotes the center of ), vanishing at each commutator. Mathieu and Villena [4] proved that on -algebra, every linear Lie derivation is standard. Qi and Hou [5] worked on nest algebras and proved that the additive Lie derivation of nest algebras on Banach spaces is standard.
Recent questions involving finding the condition under which a linear map becomes a Lie derivation or simply a derivation influenced the observations of so many researchers (see Ashraf et al. [6], Liu [7], Ashraf et al. [8], Ji et al. [9], Qi [10], Qi et al. [11] and the references therein). The purpose of the above studies in most of cases was to obtain the restrictions under which Lie derivations or derivations can be completely determined by the action on some subsets of the algebras. There are several articles on the study of local actions of the Lie derivations of operator algebras. Lu and Jing [12] proved that for a Banach space of dimensions greater than two and a linear map such that for all (resp. , where is a fixed nontrivial idempotent), then there exists an operator and a linear map vanishing at all the commutators with such that for all . Ji and Qi [13] proved that if is a triangular algebra over a commutative ring , then under certain restrictions on , if is an -linear map satisfying , where is the standard idempotent of ), then , where is a derivation and is an -linear map vanishing at all the commutators with . Qi and Hou [11] characterized Lie derivations on von Neumann algebras without central summands of type . Qi and Ji [14] proved the same result for , where is a core-free projection. Qi [10] characterized Lie derivations on -subspace lattice algebras and proved the same result due to Lu and Jing [12] on -subspace lattice algebra Alg, where is a -subspace lattice on a Banach space over the real or complex field with a dimension greater than two. Liu [15] studied the characterization of Lie triple derivations on von Neumann algebras with no central abelian projections. For further references see Bruno et al. [16], Wang [17], Wang et al. [18] and references therein. Recently, Ashraf and Jabeen [19] characterized the Lie-type derivations on von Neumann algebras with no central summands of type , where they showed that every Lie-type derivation on von Neumann algebras has a standard form at zero products as well as at projection products.
The objective of this paper is to investigate Lie-type higher derivations on von Neumann algebras with no central summands of type and to prove that on a von Neumann algebra, every Lie-type higher derivation has standard form at zero products as well as at projection products. Precisely, we prove that every additive map satisfying for all with is of the form for all where is an additive higher derivation and is an additive higher map whose range is in Further, we discuss some more related results.
2. Main Results
In this section, we discuss the characterization of Lie-type higher derivation on von Neumann algebras having no central summands of type at zero products.
Remark 1.
Let be a von Neumann algebra with center . For each self-adjoint operator , we define the core of T, denoted by to be . One has . Further, if and , then . If P is a projection, then is the largest central projection . We call a such projection core-free if and is the central carrier of P.
In proving our main results, we use the following known lemmas. Lemma 1 gives a sufficient condition for a fixed projection T of von Neumann algebra to be a central element of A if it commutes with and for all .
Lemma 1
(Miers [20], Lemma 5). For projections with , if commutes with and for all , then T commutes with and for all .
Lemma 2
(Bresar and Miers [21], Lemma 5). Let be a von Neumann algebra with no central summands of type . If such that , then .
Lemma 3
(Miers [20], Lemma 14). Let be a von Neumann algebra such that is a core-free projection in . Then, .
Lemma 4
(Ashraf and Jabeen [19], Lemma 2.5). Let If
Lemma 5
(Miers [20], Lemma 4). If is a von Neumann algebra with no central summands of type , then each nonzero central projection of is the central carrier of a core-free projection of .
The first main result of this paper is the following theorem:
Theorem 1.
Let be a von Neumann algebra with no central summands of type and an additive map satisfying
for all with Then, there exists an additive higher derivation and an additive higher map , which annihilates every -commutator with such that
Henceforward, let be a von Neumann algebra with no central summands of type and an additive map satisfying the hypotheses of Theorem 1. For projections , let and let us define a map as an inner higher derivation for all Clearly, is a Lie n-higher derivation. Since
One easily obtains Accordingly, it suffices to consider only those Lie n-higher derivations, which satisfy
We give proof of Theorem 1 in a series of lemmas. We begin with the following lemmas:
Lemma 6.
For projections and
Proof.
To prove this lemma, we use the principle of mathematical induction on , and the result was shown to be true by Ashraf and Jabeen [19]. Assume that the result holds for all . Then, we want to prove that it also holds for . Since for all , we have
This implies
Premultiplying by to the above equation, we obtain
and by postmultiplying to the same equation, we obtain Then, by using Lemma 4, we have Knowing the fact that one can write
which implies Now, using and applying similar calculations as above, we obtain that Hence, and holds for all □
Lemma 7.
,
Proof.
We show that The other case, i.e., can be shown similarly. For , it was shown to be true by Ashraf and Jabeen [19]. Now suppose that it holds for all . We want to show that it also holds for . Using Lemma 6 and Equation (1), we have From this equation, one can easily obtain , and if n is even, then But when n is odd, then for all as one can easily see that
which can be written as . From this equation, we obtain Now put . Then,
This implies that and therefore Since , we have Therefore, Hence, for all □
Lemma 8.
There exists maps on such that for any .
Proof.
Using Lemma 6 and knowing the fact that we have
From which we obtain To complete the proof of the lemma, we need to show that For this, take any and we have
This implies that By pre- and postmultiplying , we obtain This implies , which means there exists some such that and therefore
Since we have From the above equations, we have Then, by Lemma 3, and thus One can also define a map on by Then, by comparing it with Equation (3), we obtain for all With the similar steps, there exists a map on such that and for all □
Now define two maps by and by for all . Then, one can easily observe that
Lemma 9.
Let be a map such that where is a Lie-type higher derivation and Then, is an additive map.
Proof.
As , we need to show that are additive. For this, take any and we have
and
By combining all the above three expressions, one can easily find that Since and , we know that by Lemma 3. We have Hence, This implies that is additive. Similarly, we can show that is additive. Therefore, is an additive map. □
Our next lemma is also important to complete the proof of Theorem 1.
Lemma 10.
For any and be a map. Then,
- ,
- .
Proof.
Here, we give proof of part , and the second part can be proved similarly. Lets us prove the lemma with the help of mathematical induction on m. For , it was shown to be true by Ashraf and Jabeen [19]. Suppose it is true for all . Now, we show that it also holds for Note that is a Lie-type higher derivation. Since for we have
Similarly, one can prove . □
Lemma 11.
For any We have
Proof.
Lemma 12.
For any We have .
Proof.
To prove our lemma, we use the principle of mathematical induction. For it was shown to be true by Ashraf and Jabeen [19]. Suppose it holds for all . We show that it also holds for Since for any and , we have
This implies that But, we know that for all Therefore, one can easily arrive at
Premultiplying the above equation by and using Lemma 9, we obtain
and by postmultiplying the same equation by , we obtain
By comparing Equations (6) and (7), we obtain
Then, through the application of Lemma 10, we obtain
Now, we prove that For any let be its polar decomposition. This implies that and thus , which follows that
On the other hand, we similarly can show that
Then, by multiplying with Equation (6) and using Equations (9) and (10), we obtain
Now, by using Lemma 8 and Equations (9) and (10), one can find that
and
Thus, Equation (11) implies that , and hence Therefore, from Equations (6) and (7) and using Lemma 11, we obtain and for all . This proves that the lemma is also true for Hence, the lemma is true for all □
We have all the pieces to carry the proof of our first main result of this paper.
Proof of Theorem 1.
In view of Lemmas 10–12, one can easily see that is an additive higher derivation, and it can be observed that for and for We now show that for all
We can now conclude from the above observations that if is an additive Lie n-higher derivation, then there exists an additive higher derivation of and a map that vanishes at with for all such that □
Note that every additive derivation is an inner derivation Semrl [22]. Nowicki [23] proved that if every additive(linear) derivation of is inner, then every additive (linear) higher derivation of is inner (see Wei and Xiao [24] for details). Hence, by Theorem 1, the following corollaries are immediate:
Corollary 1.
Let be a von Neumann algebra with no central summands of type and a linear map satisfying
for all , with . Then, there exists an operator and a linear map , which annihilates every -commutator with such that for all
Corollary 2.
Let be a von Neumann algebra with no central summands of type and a linear map satisfying
for all . Then, is an additive Lie higher derivation if and only if there exists an additive higher derivation and an additive map , which annihilates every -commutator such that for all
In the next segment, we study the characterization of Lie derivations on general von Neumann algebras having no central summands of type by taking action at the projection products. Now, we state and prove the second main result of this paper.
Theorem 2.
Let be a von Neumann algebra with no central summands of type and an additive higher map satisfying for all with where P is a core-free projection with the central carrier Then, there exists an additive higher derivation and an additive higher map that annihilates every -commutator with such that
Let and let us define a map as an inner higher derivation for all Clearly, is also a Lie n-higher derivation. Since
one easily obtains Accordingly, it suffices to consider only those Lie n-higher derivations which satisfy
Lemma 13.
Proof.
For , it was shown to be true by Ashraf and Jabeen [19]. Suppose that it holds for all . We show that it also holds for . Since for all , we can write
From which we obtain
Now, by premultiplying and postmultiplying to the above equation, one finds that
Since , by using the above equation and Lemma 4, we obtain . Now, by using , it follows that
which gives It follows that On the other hand, by using and making similar calculations as above, one obtains that Hence, for all □
Lemma 14.
Proof.
We prove the lemma with the help of the principle of mathematical induction. For , it was shown to be true by Ashraf and Jabeen [19]. Suppose that the lemma holds for all . We will prove that it is also true for First, consider the case for ; the other case will be proved in a similar way. By using Equation (12) and , we have By pre- and postmultiplying and to the above equation, we obtain , respectively. Hence, Since we can write
This follows that
Then, by multiplying on both sides to the above equation, one obtains , and by multiplying from the right-hand side and using , we find that Then, by linearizing, we obtain for all Now it can be easily observed that
which implies
As is semiprime, one can easily see that and therefore . Hence, , which shows that the lemma also holds for . Therefore, holds for all Similarly, we can easily prove that □
Lemma 15.
There exists maps such that and , for any
Proof.
We will prove the lemma with the help of the principle of mathematical induction. For , it was shown to be true by Ashraf and Jabeen [19]. Suppose that the lemma holds for all . We will show that it also holds for . Here, we give the proof for the case , and the proof for the case follows similar steps. Suppose is invertible; this implies that there exists , such that . Therefore, we can write
Also, since and by using Lemma 13, we have
Upon comparing the above two equations, we have It can be easily observed from the above equation that , from which we obtain as and . Then, for any and , it can be easily seen that
and
Comparing Equations (13) and (14), we obtain
which leads to Then, multiplying both sides of the above equation by , one arrives at and therefore . This implies that there exists some such that If is not invertible in , then one can find a sufficiently large number, say r, in a way such that is invertible in following the preceding cases and . As , we have and Without a loss of generality, we denote Therefore, for any , we have
We define a map, say , on by , and then by combining it with the above equation, we obtain for any . Hence, the lemma is true for . Therefore, the lemma is true for all . For the case when , we take to obtain , and then following similar steps as that for , we find that
for any , which completes the proof of the lemma. □
We now define maps and by and for all One can easily observe that
Lemma 16.
is an additive map.
Proof.
The proof is similar to that of Lemma 9. □
Lemma 17.
For any , we have,
- (a)
- ,
- (b)
Proof.
(a) We prove it with the help of the principle of mathematical induction. For , it was shown to be true by Ashraf and Jabeen [19]. Suppose that it holds for all We prove that it is also true for We take the case for . If is invertible, then for any , we have . Therefore, we have
and
since and is additive. From the above two equations, we obtain
By replacing with in the above equation, we obtain
Now, if is not invertible in , we can find a sufficiently large number, say r, such that is invertible in . Then, . Since is invertible in , from the above equation, we obtain
For since , we have
Since is additive, the above equation gives
Which follows that
i.e, for all and
(b) For by considering and using the same approach as above, one can easily obtain for all and , and for the case when , by considering , we can easily prove that for all □
Lemma 18.
For any , we have
Proof.
The proof of this lemma is same as that of Lemma 11. □
Lemma 19.
For any , we have
Proof.
We prove the lemma with the help of the principle of mathematical induction. For , it was shown to be true by Ashraf and Jabeen [19]. Suppose that the lemma holds for all . We prove that it is true for Take any since Then,
From this, we obtain since for all We have
by using Lemma 12 and applying similar steps to obtain Then, from the above relation, we obtain
and
for all This shows that the lemma is true for all . □
Proof of Theorem 2.
The proof is similar to that of Theorem 1 and by using Lemmas 13–19 instead of Lemmas 10–12. □
As a direct consequence of Theorem 2, we have the following corollary:
Corollary 3.
Let be a von Neumann algebra with no central summands of type and a linear map satisfying
for all , with , where is a core-free projection with the central carrier I. Then, there exists an operator and a linear map , which annihilates every -commutator with such that for all
3. Conclusions
In the present paper, firstly, we studied the action of Lie-type higher derivations of von Neumann algebras and described their structures. Precisely, we established that every additive Lie-type higher derivation of von Neumann algebras has a standard form at zero products as well as the projection products; that is, every additive map from von Neumann algebra into itself can be written as where is an additive higher derivation and is an additive higher map, which annihilates every -commutator with Secondly, we characterized Lie derivations on general von Neumann algebras with no central summands of type by using the actions at projection products. Finally, we described the structures of linear maps via core-free projections with the central carrier.
In view of Ferreira et al. [16], these results are still open for alternative rings, where one can study and characterize the Lie-type higher derivations of alternative rings.
Author Contributions
Writing—original draft, A.H.K.; Writing—review & editing, S.N.H.; Visualization, B.A.W.; Supervision, S.A.; Funding acquisition, T.A. All authors have read and agreed to the published version of the manuscript.
Funding
This study was carried out with financial support from King Saud University, College of Science, Riyadh, Saudi Arabia.
Data Availability Statement
Data sharing is not applicable to this article as no data sets were generated or analyzed during the current study.
Acknowledgments
The authors would like to thank the reviewers for their valuable suggestions and useful comments, which helped us improve the presentation of the manuscript. Moreover, the authors extend their appreciation to King Saud University, College of Science, for funding this research under the Researchers Supporting Project Number: RSPD2023R934.
Conflicts of Interest
The authors declare no conflict of interest.
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