Let A be a unital algebra with nontrivial idempotents. We considered A as a superalgebra according to Ghahramani and Zadeh's method. We provided a description of supercommuting maps on A. As a consequence, we gave a description of supercommuting maps on matrix algebras, which is different from the result on commuting maps of matrix algebras. Finally, we proved that every supercommuting map on triangular algebras is a commuting map.
Citation: Yingyu Luo, Yu Wang. Supercommuting maps on unital algebras with idempotents[J]. AIMS Mathematics, 2024, 9(9): 24636-24653. doi: 10.3934/math.20241200
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Let A be a unital algebra with nontrivial idempotents. We considered A as a superalgebra according to Ghahramani and Zadeh's method. We provided a description of supercommuting maps on A. As a consequence, we gave a description of supercommuting maps on matrix algebras, which is different from the result on commuting maps of matrix algebras. Finally, we proved that every supercommuting map on triangular algebras is a commuting map.
Let A be an associative algebra over R, a commutative ring with unity. By Z(A), we denote the center of A. Set [x,y]=xy−yx and x∘y=xy+yx.
A linear map f on A is called a commuting map if [f(x),x]=0 for all x∈A. It is clear that f(x)=λx+τ(x) is a commuting map, where λ∈Z(A) and τ:A→Z(A), which is said to be a proper commuting map.
In 1991, Brešar [1] proved that a commuting map on noncommutative Lie ideals of prime rings is always proper. In 1993, Brešsar [2] discussed centralizing mappings and derivations in prime rings. In the same year, Brešsar [3] discussed commuting traces of biadditive mappings, commutativity-preserving mappings and Lie mappings. In 2020, Jia and Xiao [4] discussed commuting maps on certain incidence algebras. Results related to commuting maps are discussed in [5,6,7].
It should be mentioned that the study of commuting maps on rings initiated the theory of functional identities on rings (see [8] for details).
An associative algebra A is said to be a superalgebra if A is the direct sum of two R-submodules A0 and A1 such that AiAj⊆Ai+j (modulo 2). We call A0 the even part and A1 the odd part of A. Elements in H=A0⋃A1 are called homogeneous, and we write |a|=i to mean a∈Ai. For a,b∈H, the supercommutator of a and b is defined to be
[a,b]s=ab−(−1)|a||b|ba. |
It is clear that [a,b]s=a∘b if both a and b are odd, and [a,b]s=[a,b] if either a or b is even. The definition can be extended linearly to arbitrary a,b∈A.
Let A=A0⨁A1 be a superalgebra. A linear map f:A→A is said to be supercommuting if
[f(x),x]s=0 |
for all x∈A.
In 2002, Beidar, Chen, Fong, and Ke [9] discussed graded polynomial identities with an antiautomorphism. In 2003, Beidar, Bresǎr, and Chebotar [10] discussed Jordan superhomomorphisms on superalgebras. In 2008, Wang [11] discussed skew-supercommuting maps in superalgebras. In 2009, Wang [12] gave a description of supercentralizing superautomorphisms on prime superalgebras. In the same year, Lee and Wang [13] gave a description of supercommuting maps of prime superalgebras. In 2017, Fan and Dai [14] investigated Super-biderivations on Lie superalgebras. In 2019, Cheng and Sun [15] discussed Super-biderivations and linear supercommuting maps on the super-BMS3 algebras.
Let A be a unital algebra with an idempotent e≠0,1. Let f denote the idempotent 1−e. In this case, A can be represented in the so-called Peirce decomposition form
A=eAe+eAf+fAe+fAf, |
where eAe and fAf are subalgebras with unitary elements e and f, respectively, eAf is an (eAe,fAf)-bimodule and fAe is an (fAf,eAe)-bimodule, which is said to be a generalized matrix algebra (see [16] for details).
For brevity, we set
A=eAe,M=eAf,N=fAe,B=fAf. |
It is clear that
{AM⊆M,MA=0,AN=0,NA⊆N,AB=0,BA=0,MN⊆A,BM=0,MB⊆M,BN⊆N,NB=0,NM⊆B,MM=0,NN=0. |
In 2012, Benkovič and Širovnik [17] defined the following useful condition:
{a∈A,aM=0=Na⇒a=0;b∈B,Mb=0=bN⇒b=0. | (1.1) |
Some examples of unital algebras with nontrivial idempotents having the property (1.1) are triangular algebras, matrix algebras, and prime (and hence in particular simple) algebras with nontrivial idempotents (see [17]).
In 2010, Xiao and Wei [16] initiated the study of commuting mappings of generalized matrix algebras, which generalized a typical result on commuting maps of triangular algebras (see [18] for details). In 2019, Li, Wei, and Fošner [19] discussed k-commuting mappings of generalized matrix algebras, which generalized a result on k-commuting maps of triangular algebras (see [20] for details). In 2002, Du and Wang [21] gave a description of Lie derivations of generalized matrix algebras. In 2018, Benkovič [22] discussed generalized Lie derivations of unital algebras with idempotents. Additional results on mappings of generalized matrix algebras can be found in [23,24,25].
In 2024, Ghahramani and Zadeh [26] considered A as a superalgebra by:
A=A0⊕A1, |
where
A0=A+BandA1=M+N. |
They determined the class of generalized matrix algebras for which every Lie superderivation is proper (see [26, Theorem 5.1]. As a consequence, they gave some descriptions of Lie superderivations on both matrix algebras and triangular algebras (see [26] for details).
Recently, Chen [27] discussed Jordan superderivations of unital algebras with idempotents. As a consequence, she gave some descriptions of Jordan superderivations of matrix algebras and triangular algebras.
In the present paper, we give a description of supercommuting maps of unital algebras with idempotents. As a consequence, we give some descriptions of supercommuting maps of matrix algebras and triangular algebras.
We organize the paper as follows: In Section 2, we give preliminaries and the definition of proper supercommuting maps. In Section 3, we give a description of supercommuting maps of degree 0 on unital algebras. In Section 4, we give a description of supercommuting maps of degree 1 on unital algebras. In Section 5, we give the main result of the paper. In Section 6, we give a description of supercommuting maps on matrix algebras. As a consequence, we prove that every supercommuting map on matrix algebras over a 2-torsion free unital algebra is supercentral. In the last section, we prove that every supercommuting map on triangular algebras is a commuting map.
Let A=A0⨁A1 be a superalgebra. The supercenter of A is the set
Z(A)s={a∈A|[a,x]s=0for all x∈A}. |
We set
Z(A)0=Z(A)∩A0andZ(A)1=Z(A)∩A1. |
It is easy to check that Z(A)=Z(A)0⨁Z(A)1 is a graded subalgebra of A (see [4, Section 2] for details). It is clear that Z(A)0⊆Z(A)s.
We begin with the following definition.
Definition 2.1. Let A=A0⨁A1 be a superalgebra. We call a linear map f:A→A a proper supercommuting map if
f(x)=λx+τ(x) |
for all x∈A, where λ∈Z(A)0 with 2λA21={0}, and τ:A→Z(A)s is a linear map. In particular, if f(x)∈Z(A)s for all x∈A, we call f a supercentral map.
The following result shows that a proper supercommuting map is a supercommuting map.
Lemma 2.1. Let A=A0⨁A1 be a superalgebra. Then
f(x)=λx+τ(x) |
for all x∈A, is a supercommuting map of A, where λ∈Z(A)0 with 2λA21={0}, and τ:A→Z(A)s is a linear map.
Proof. For any x=x0+x1∈A we get
[f(x),x]s=[λx+τ(x),x]s=λ[x,x]s=λ[x0+x1,x0+x1]s=λ[x0,x0]+λ[x0,x1]+λ[x1,x0]+λ[x1,x1]s=λ[x1,x1]s=2λx21=0. |
We obtain that f is a supercommuting map.
Definition 2.2. Let A=A0⨁A1 be a superalgebra. A supercommuting map f on A is said to be a supercommuting map of degree 0 if f(A0)⊆A0 and f(A1)⊆A1. A supercommuting map f of A is said to be a supercommuting map of degree 1 if f(A0)⊆A1 and f(A1)⊆A0.
The following result shows that a supercommuting map is the sum of a supercommuting map of degree 0 and a supercommuting map of degree 1.
Lemma 2.2. Let A=A0⨁A1 be a superalgebra. Let f be a supercommuting map of A. Then
f=f0+f1 |
where f0 is a supercommuting map of degree 0 on A and f1 is a supercommuting map of degree 1 on A.
Proof. For i=0 or 1, let πi be the canonical projection of A. We set
f0=π0fπ0+π1fπ1andf1=π0fπ1+π1fπ0. |
It is easy to check that fi is a linear map of A and f=f0+f1, where i=0,1. Moreover, f0(A0)⊆A0, f0(A1)⊆A1, f1(A0)⊆A1, and f1(A1)⊆A0. We now claim that both f0 and f1 are supercommuting maps on A.
For i=0,1, and any x=x0+x1∈A, we have
0=[f(xi),xi]s=[f0(xi)+f1(xi),xi]s=[f0(xi),xi]s+[f1(xi),xi]s. |
Since [f0(xi),xi]s is even and [f1(xi),xi]s is odd, we obtain that
[f0(xi),xi]s=0and[f1(xi),xi]s=0. | (2.1) |
It follows from (2.1) and the linearity of fi, where i=0,1, that
[f0(x1),x0]s+[f0(x0),x1]s=0 | (2.2) |
and
[f1(x1),x0]s+[f1(x0),x1]s=0. | (2.3) |
For i=0,1, we get from (2.1), (2.2), and (2.3) that
[fi(x),x]s=[fi(x0)+fi(x1),x0+x1]s=[fi(x0),x0]s+[fi(x0),x1]s+[fi(x1),x0]s+[fi(x1),x1]s=0. |
This implies that fi is a supercommuting map of degree i. The proof of the result is complete.
Form now on we always assume that A is a unital algebra with nontrivial idempotents.
The following result is essentially the same as [26, Lemma 2.1].
Lemma 2.3.
Z(A)=Z(A)s={X∈Z(A0)|[X,A1]=0}. |
We define two natural projection πA:A→A and πB:A→B by
πA(a+m+n+b)=aandπB(a+m+n+b)=b. |
The following result is essentially the same as [26, Lemma 2.3].
Lemma 2.4. Let A be a unital algebra with nontrivial idempotents having the property (1.1). Then
Z(A)=Z(A)s={X∈A0|[X,A1]=0}. |
Furthermore, πA(Z(A))⊆Z(A), πB(Z(A))⊆Z(B), and there exists a unique isomorphism φ from πA(Z(A)) to πB(Z(A)) such that am=mφ(a), mb=φ−1(b)m, na=φ(a)n, and bn=nφ−1(b) for all m∈M,n∈N.
We begin with the structure of supercommuting maps of degree 0.
Lemma 3.1. Let f0 be a supercommuting map of degree 0 on A. Then
f0(a+m+n+b)=α1(a)+α4(b)+α1(1)m−mβ1(1)+nα1(1)−β1(1)n+β1(a)+β4(b) |
for all a∈A, m∈M, n∈N, and b∈B, where α1:A→A, α4:B→Z(A), β1:A→Z(B), and β4:B→B are linear maps satisfying the following conditions:
(i) α1 and β4 are commuting mappings of A and B, respectively. In particular, α1(1)∈Z(A),β4(1)∈Z(B);
(ii) α1(a)m−mβ1(a)=a(α1(1)m−mβ1(1)), β1(a)n−nα1(a)=(nα1(1)−β1(1)n)a;
(iii) α4(b)m−mβ4(b)=(mβ1(1)−α1(1)m)b, β4(b)n−nα4(b)=b(nα1(1)−β1(1)n);
(iv) 2α1(1)mn=2mβ1(1)n and 2nα1(1)m=2β1(1)nm.
Proof. Since f0(A0)⊆A0 and f0(A1)⊆A1, we can write
f0(a+m+n+b)=α1(a)+α4(b)+μ2(m)+μ3(n)+ν2(m)+ν3(n)+β1(a)+β4(b) | (3.1) |
for all a∈A, m∈M, n∈N, and b∈B, where α1:A→A, α4:B→A, μ2:M→M, μ3:N→M, ν2:M→N, ν3:N→N, β1:A→B, and β4:B→B are linear maps.
Linearizing [f0(X),X]s=0 leads to
[f0(X),Y]s+[f0(Y),X]s=0 | (3.2) |
for all X,Y∈A. For any m∈M, taking X=1A and Y=m in (3.2) yields
[f0(1A),m]+[f0(m),1A]=0. |
That is
[α1(1A)+β1(1A),m]+[μ2(m)+ν2(m),1A]=0. |
This implies that v2(m)=0 and μ2(m)=α1(1)m−mβ1(1) for all m∈M. Similarly, if we choose X=1A and Y=n in (3.2), then we arrive at μ3(n)=0 and ν3(n)=nα1(1)−β1(1)n for all n∈N. Therefore (3.1) becomes
f0(a+m+n+b)=α1(a)+α4(b)+α1(1)m−mβ1(1)+nα1(1)−β1(1)n+β1(a)+β4(b) | (3.3) |
for all a∈A, m∈M, n∈N, and b∈B. For any a∈A and b∈B, taking X=a and Y=b into (3.3) yields
[f0(a),b]+[f0(b),a]=0. |
That is
[α1(a)+β1(a),b]+[α4(b)+β4(b),a]=0. |
Then [α4(b),a]=0 and [β1(a),b]=0 for all a∈A and b∈B. This implies that α4(B)⊆Z(A) and β1(A)⊆Z(B). By (3.3) we obtain
0=[f0(a+b),a+b]=[α1(a),a]+[β4(b),b]. |
Then [α1(a),a]=0 for all a∈A and [β4(b),b]=0 for all b∈B. This implies that α1 and β4 are commuting mappings of A and B, respectively. It is easy to check that α1(1)∈Z(A) and β4(1)∈Z(B). This proves the statement (ⅰ).
By (3.3) we get
[f0(a),m+n]=α1(a)m−mβ1(a)+β1(a)n−nα1(a) |
and
[f0(m+n),a]=a(mβ1(1)−α1(1)m)+(β1(1)n−nα1(1)a. |
Note that
[f0(a),m+n]+[f0(m+n),a]=0. |
The above three relations imply that α1(a)m−mβ1(a)=a(α1(1)m−mβ1(1)) and β1(a)n−nα1(a)=(nα1(1)−β1(1)n)a for all a∈A, m∈M, and n∈N. This proves the statement (ii). Similarly, taking X=b and Y=m+n in (3.2) we can obtain that α4(b)m−mβ4(b)=(mβ1(1)−α1(1)m)b and β4(b)n−nα4(b)=b(nα1(1)−β1(1)n) for all b∈B, m∈M, and n∈N. This proves the statement (ⅲ).
Since [f0(m+n),m+n]s=0 for all m∈M, n∈N, we get from (3.3) that
[a(mβ1(1)−α1(1)m)+a1(1)n−nα1(1))a,m+n]s=0. |
That is
(a(mβ1(1)−α1(1)m)+a1(1)n−nα1(1))a)(m+n)+(m+n)(a(mβ1(1)−α1(1)m)+a1(1)n−nα1(1))a)=0 |
for all m∈M and n∈N. This implies that
2α1(1)mn=2mβ1(1)nand2nα1(1)m=2β1(1)nm |
for all m∈M, n∈N. This proves the statement (ⅳ). We complete the proof of the result.
The idea of proving the following result is taken from [18, Lemma 1].
Lemma 3.2. Let A be a unital algebra with nontrivial idempotents having the property (1.1). Let f0 be a supercommuting map of degree 0 on A. With notations as above, then β−11(πB(Z(A))) and α−14(πA(Z(A))) are ideals of A and B, respectively. Furthermore, [A,A]⊆β−11(πB(Z(A))) and [B,B]⊆α−14(πA(Z(A))).
Proof. We prove the part of the statement related to β1. The part related to α4 can be proved analogously. For any a,a′∈A, m∈M, and n∈N we get from Lemma 3.1(ⅱ) that
a′a(α1(1)m−mβ1(1))=α1(a′a)m−mβ1(a′a) | (3.4) |
a′a(α1(1)m−mβ1(1))=a′(α1(a)m−mβ1(a)) | (3.5) |
aa′(α1(1)m−mβ1(1))=α1(aa′)m−mβ1(aa′) | (3.6) |
a(α1(1)a′m−a′mβ1(1))=α1(a)a′m−a′mβ1(a). | (3.7) |
From (3.4) and (3.5), we have
α1(a′a)m−mβ1(a′a)−a′(α1(a)m−mβ1(a))=0, | (3.8) |
and from (3.6) and (3.7), we have
α1(aa′)m−mβ1(aa′)−α1(a)a′m+a′mβ1(a)=0. | (3.9) |
Taking the difference of (3.8) and (3.9), we have
(α1([a,a′])−[α1(a),a′])m=mβ1([a,a′]). | (3.10) |
For any a,a′∈A and n∈N, we get from Lemma 3.1(ⅱ) that
(nα1(1)−β1(1)n)a′a=β1(a′a)n−nα1(a′a) | (3.11) |
(nα1(1)−β1(1)n)a′a=(β1(a′)n−nα1(a′))a | (3.12) |
(nα1(1)−β1(1)n)aa′=β1(aa′)n−nα1(aa′) | (3.13) |
(naα1(1)−β1(1)na)a′=β1(a′)na−naα1(a′). | (3.14) |
From (3.11) and (3.12), we have
β1(a′a)n−nα1(a′a)−β1(a′)na+nα1(a′)a=0, | (3.15) |
and from (3.13) and (3.14), we have
β1(aa′)n−nα1(aa′)−β1(a′)na+naα1(a′)=0. | (3.16) |
Taking the difference of (3.15) and (3.16), we have
β1([a,a′])n=n(α1(([a,a′])−[a,α1(a′)]). | (3.17) |
Since α1 is commuting map of A, we get that [a,α1(a′)]=[α1(a),a′]. Thus, we get from (3.17) that
β1([a,a′])n=n(α1(([a,a′])−[α1(a),a′]). | (3.18) |
In view of Lemma 2.4 we get from both (3.10) and (3.18) that β1([a,a′])∈πB(Z(A)). Hence [A,A]⊆β−11(πB(Z(A))).
Suppose that a∈β−11(πB(Z(A))). From both (3.8) and (3.15) we have
mβ1(a′a)=(α1(a′a)−a′α1(a)+a′φ−1(β1(a)))m;β1(a′a)n=n(α1(a′a)−a′α1(a)+a′φ−1(β1(a))). |
By Lemma 2.4 we get that β1(a′a)∈πB(Z(A))). Hence a′a∈β−11(πB(Z(A))). Similarly, from both (3.9) and (3.16) we have
mβ1(aa′)=(α1(aa′)−α1(a)a′+a′φ−1(β1(a)))m;β1(aa′)n=n(α1(aa′)−α1(a)a′+a′φ−1(β1(a))). |
By Lemma 2.4 we get that β1(aa′)∈πB(Z(A))). Hence aa′∈β−11(πB(Z(A))). As a result, β−11(πB(Z(A))) is an ideal of A containing [A,A]. This proves the result.
Now we obtain necessary and sufficient conditions for a supercommuting map of degree 0 on A to be proper. The idea of proving the following result is taken from [18, Theorem 1].
Lemma 3.3. Let A be a unital algebra with nontrivial idempotents having the property (1.1). Let f0 be a supercommuting map of degree 0 on A such that
f0(a+m+n+b)=α1(a)+α4(b)+α1(1)m−mβ1(1)+nα1(1)−β1(1)n+β1(a)+β4(b). |
Then, the following three conditions are equivalent:
(i) f0 is proper;
(ii) β1(A)⊆πB(Z(A)) and α4(B)⊆πA(Z(A));
(iii) α1(1)∈πA(Z(A)) and β1(1)∈πB(Z(A)).
Proof. (ⅱ)⇒ (ⅲ). β1(1)∈β1(A)⊆πB(Z(A)). Taking b=1 in Lemma 3.1(ⅲ), we get
α1(1)m=m(β4(1)+β1(1)−φ(α4(1)))nα1(1)=(β4(1)+β1(1)−φ(α4(1)))n |
for all m∈M and n∈N. By Lemma 2.4 we get that α1(1)∈πA(Z(A)).
(ⅲ) ⇒ (ⅱ). Since β1(1)∈πB(Z(A)), the ideal β−11(πB(Z(A))) of A contains 1. Hence A=β−11(πB(Z(A))). We have that β1(A)⊆πB(Z(A)). By Lemma 3.1(ⅲ), we have α4(b)m−mβ4(b)=(mβ1(1)−α1(1)m)b, which implies
α4(b)m=m(β4(b)+β1(1)b−φ(α1(1))b) | (3.19) |
for all m∈M and b∈B. By Lemma 3.1(ⅲ) again, we have β4(b)n−nα4(b)=b(nα1(1)−β1(1)n), which implies
nα4(b)=(β4(b)+β1(1)b−φ(α1(1))b)n | (3.20) |
for all n∈N and b∈B. In view of Lemma 2.4 we get from both (3.19) and (3.20) that α4(b)∈πA(Z(A)) for all b∈B.
(ⅲ) ⇒ (ⅰ). We set
τ(X)=f0(X)−λX |
for all X∈A, where λ=α1(1)−φ−1(β1(1))+φ(α1(1))−β1(1)∈Z(A). We claim that τ(A)⊆Z(A). Indeed, we have
τ(a+m+n+b)=f0(a+m+n+b)−λ(a+m+n+b)=(α1(a)+α4(b)+α1(1)m−mβ1(1)+nα1(1)−β1(1)n+β1(a)+β4(b) −(α1(1)−φ−1(β1(1))+φ(α1(1))−β1(1)))(a+m+n+b)=α1(a)−(α1(1)−φ−1(β1(1)))+β1(a)+α4(b)+β4(b)−(φ(α1(1))−β1(1))b. |
By Lemma 3.1(ⅱ) we have
(α1(a)−(α1(1)−φ−1(β1(1)))a)m=mβ1(a)n(α1(a)−(α1(1)−φ−1(β1(1)))a)=β1(a)n |
for all a∈A, m∈M, and n∈N. By Lemma 2.4 we get that
α1(a)−(α1(1)−φ−1(β1(1)))a+β1(a)∈Z(A) |
for all a∈A. Similarly, we get from Lemma 3.1(ⅲ) that
α4(b)m=m(β4(b)−(φ(α1(1))−β1(1))b);nα4(b)=(β4(b)−(φ(α1(1))−β1(1))b)n |
for all m∈M, n∈N, and b∈B. By Lemma 2.4 we get that
α4(b)+β4(b)−(φ(α1(1))−β1(1))b∈Z(A) |
for all b∈B. We obtain that τ(a+m+n+b)∈Z(A) for all a∈A, m∈M, n∈N, and b∈B as desired. We next claim that 2λA21={0}.
For any m∈M and n∈N, by Lemma 3.1(ⅳ) we have
2πA(λ)mn=2(α1(1)−φ−1(β1(1)))mn=2α1(1)mn−2mβ1(1)n=0 |
and
2πB(λ)nm=2(φ(α1(1))−β1(1))nm=2nα1(1)m−2β1(1)nm=0. |
It follows that
2λ(m+n)(m′+n′)=2λ(mn′+nm′)=2πA(λ)mn′+2πB(λ)nm′=0 |
for all m,m′∈M, n,n′∈N. This implies that 2λA21={0}.
(ⅰ) ⇒ (ⅲ). Suppose that f0(X)=λX+τ(X) for all X∈A, where λ∈Z(A) with 2λA21={0} and τ:A→Z(A) is a linear map. For any m∈M and n∈N, we have
f0(m+n)=(πA(λ)+πB(λ))(m+n)+τ(m+n). |
By Lemma 3.1 we get that
α1(1)m−mβ1(1)+nα1(1)−β1(1)n=πA(λ)m+πB(λ)n+τ(m+n). |
We get from the last relation that
α1(1)m−mβ1(1)=πA(λ)m;nα1(1)−β1(1)n=πB(λ)n. |
This implies that
(α1(1)−πA(λ))m=mβ1(1);n(α1(1)−πA(λ))=β1(1)n. |
By Lemma 2.4 we get that α1(1)−πA(λ)∈πA(Z(A)) and β1(1)∈πB(Z(A)). Hence, α1(1)∈πA(Z(A)) and β1(1)∈πB(Z(A)) as desired. The proof of the result is complete.
We now give sufficient conditions for every supercommuting map of degree 0 on A to be proper. The idea of proving the following result is taken from [18, Theorem 2].
Theorem 3.1. Let A be a unital algebra with nontrivial idempotents having the property (1.1). Suppose that the following two conditions are satisfied:
(i) Z(B)=πB(Z(A)), or A=[A,A];
(ii) Z(A)=πA(Z(A)), or B=[B,B].
Then every supercommuting map of degree 0 on A is proper.
Proof. Let f0 be a supercommuting mapping of degree 0 on A. With notations as above, we note that α4(B)⊆Z(A) and β1(A)⊆Z(B). By the condition (ⅰ) we note that either Z(B)=πB(Z(A)) or A=[A,A]. Suppose first that Z(B)=πB(Z(A)). We get that β1(A)⊆πB(Z(A)). Suppose next that A=[A,A]. In view of Lemma 3.2 we note that [A,A]⊆β−11(πB(Z(A))). This implies that β1(A)⊆πB(Z(A)).
By the condition (ⅱ) we note that either Z(A)=πA(Z(A)) or B=[B,B]. Suppose first that Z(A)=πA(Z(A)). We get that α4(B)⊆πA(Z(A)). Suppose next that B=[B,B]. In view of Lemma 3.2 we note that [B,B]⊆α−14(πA(Z(A))). We obtain that α4(B)⊆πA(Z(A)). By Lemma 3.3 we obtain that f0 is proper. This proves the result.
We first give the structure of supercommuting map of degree 1 on A.
Lemma 4.1. Let A be a unital algebra with nontrivial idempotents. Let f1 be a commuting mapping of degree 1 on A. Then f1 is of the form
f1(a+m+n+b)=α2(m)+α3(n)+β2(m)+β3(n) |
for all a∈A, m∈M, n∈N, and b∈B, where α2:M→Z(A), α3:N→Z(A), β2:M→Z(B), and β3:N→Z(B) are linear maps satisfying the following conditions:
(i) (α2(m)+α3(n))m=m(β2(m)+β3(n));
(ii) n(α2(m)+α3(n))=(β2(m)+β3(n))n
for all m∈M, n∈N.
Proof. Note that f1(A0)⊆A1 and f1(A1)⊆A0. So f1 is of the form
f1(a+m+n+b)=α2(m)+α3(n)+μ1(a)+μ4(b)+ν1(a)+ν4(b)+β2(m)+β3(m) | (4.1) |
for all a∈A, m∈M, n∈N, and b∈B, where α2:M→A, α3:N→A, μ1:A→M, μ4:B→M, ν1:A→N, ν4:B→N, β2:M→B, and β3:N→B are linear maps. Note that
[f1(1A),1A]=0. |
We get that
[μ1(1)+ν1(1),1A]=0. |
This implies that μ1(1)=0=ν1(1). Linearizing [f1(X),X]s=0 leads to
[f1(X),Y]s+[f1(Y),X]s=0 | (4.2) |
for all X,Y∈A. For any a∈A and b∈B, taking X=a+b and Y=1A into (4.2) yields
[f1(a+b),1A]+[f1(1A),a+b]=0. |
That is
[μ1(a)+μ4(b)+ν1(a)+ν4(b),1A]+[0,a+b]=0. |
This implies that μ1(a)+μ4(b)=0 and ν1(a)+ν4(b)=0 for all a∈A and b∈B. We get that μ1=μ4=0 and ν1=ν4=0. Thus, the relation (4.1) becomes
f1(a+m+n+b)=α2(m)+α3(n)+β2(m)+β3(m) | (4.3) |
for all a∈A, m∈M, n∈N, and b∈B. For any a∈A and b∈B, m∈M, and n∈N, taking X=a+b and Y=m+n in (4.3) yields
[f1(a+b),m+n]+[f1(m+n),a+b]=0. |
It follows from (4.3) that
[α2(m)+α3(n)+β2(m)+β3(n),a+b]=0. |
This implies that [α2(m)+α3(n),a]=0 and [β2(m)+β3(n),b]=0 for all a∈A and b∈B, m∈M, and n∈N. We get that [α2(m),a]=0, [α3(n),a]=0, [β2(m),b]=0, and [β3(n),b]=0 for all a∈A and b∈B, m∈M, and n∈N. That is, α2(m),α3(n)∈Z(A) and β2(m),β3(n)∈Z(B) for all m∈M and n∈N.
For any m∈M and n∈N, we have that
[f1(m+n),m+n]=0. |
It follows from (4.3) that
[α2(m)+α3(n)+β2(m)+β3(n),m+n]=0. |
This implies that (α2(m)+α3(n))m=m(β2(m)+β3(n)) and n(α2(m)+α3(n))=(β2(m)+β3(n))n for all m∈M and n∈N. We complete the proof of the result.
We now give a sufficient condition for every supercommuting map of degree 1 on A to be supercentral.
Theorem 4.1. Let f1 be a supercommuting mapping of degree 1 on A. Suppose that there exists Y1∈A1 such that
Z(A)={X∈Z(A0)|[X,Y1]=0}. |
Then f1(A)⊆Z(A).
Proof. We set
Y1=m0+n0. |
By Lemma 4.1 we note that
f1(a+m+n+b)=α2(m)+α3(n)+β2(m)+β3(m) | (4.4) |
for all a∈A, m∈M, n∈N, and b∈B, where α2:M→Z(A), α3:N→Z(A), β2:M→Z(B), and β3:N→Z(B). Moreover,
(α2(m)+α3(n))m=m(β2(m)+β3(n))n(α2(m)+α3(n))=(β2(m)+β3(n))n |
for all m∈M and n∈N. We set
δ(m,n)=α2(m)+α3(n)+β2(m)+β3(n) |
for all m∈M and n∈N. It is easy to check that
Z(A0)=Z(A)+Z(B). |
It follows that δ(m,n)∈Z(A0) for all m∈M, n∈N. Since
[f1(a+m+n+b),a+m+n+b]s=0 |
for all a∈A, m∈M, n∈N, and b∈B we get from (4.4) that
[δ(m,n),m+n]=0 |
for all m∈M and n∈N. In particular, [δ(m0,n0),Y1]=0. By assumption we have that δ(m0,n0)∈Z(A). Note that
[δ(m+m0,n+n0),m+m0+n+n0]=0 | (4.5) |
for all m∈M and n∈N. It is clear that
δ(m+m0,n+n0)=δ(m,n)+δ(m0,n0) |
for all m∈M and n∈N. We get from (4.5) that
[δ(m,n),m+n]+[δ(m,n),m0+n0]+[δ(m0,n0),m+n]+[δ(m0,n0),m0+n0]=0 |
for all m∈M and n∈N. This implies that
[δ(m,n),m0+n0]=0 |
for all m∈M and n∈N. By assumption again we obtain that δ(m,n)∈Z(A) for all m∈M and n∈N. It follows from (4.4) that f1(A)⊆Z(A). This proves the result.
We are in a position to give the main result of the paper.
Theorem 5.1. Let A be a unital algebra with nontrivial idempotents satisfying (1.1). Suppose that
(i) Z(B)=πB(Z(A)), or A=[A,A];
(ii) Z(A)=πA(Z(A)), or B=[B,B];
(iii) there exists Y1∈A1 such that
Z(A)={X∈Z(A0)|[X,Y1]=0}. |
Then, every supercommuting map of A is proper.
Proof. Let f is a supercommuting map of A. By Lemma 2.2 we have that f=f0+f1, where fi is a supercommuting map of degree i on A, i=0,1. By Theorem 3.1 we have that
f0(X)=λX+τ0(X) |
for all X∈A, where λ∈Z(A) with 2λA21={0} and τ0:A→Z(A) is a linear map. By Theorem 4.1 we have that f1(A)⊆Z(A). We set τ=τ0+f1. Then
f(X)=λX+τ(X) |
for all X∈A. This proves the result.
Let S be a unital algebra over R. Let Mn(S) be the set of all n×n matrices over S, where n≥2. We can view Mn(S) as a unital algebra with nontrivial idempotents:
Mn(S)=A+M+N+B, |
where A=Ms(S), M=Ms,t(S), N=Mt,s(S), B=Mt(S), where s+t=n. Thus, Mn(S) is a generalized matrix algebra (see [16] for details). We set
Mn(S)0=A+BandMn(S)1=M+N. |
It is easy to check that Mn(S)=Mn(S)0⨁Mn(S)1 is a superalgebra (see [26] for details).
Applying Theorem 3.1, we give a description of supercommuting maps of matrix algebras, which is different from the result on commuting maps of matrix algebras (see [16, Corollary 4.1] for details).
Theorem 6.1. Let S be a unital algebra. Let Mn(S) be the n×n matrix algebra. Then every supercommuting map on Mn(R) is the form X→λX+τ(X), where λ∈Z(S) with 2λ=0, and τ:Mn(S)→Z(S)⋅1 is a linear map.
Proof. Note that Mn(S) satisfies the condition (1.1) (see [17, Section 1]). It is easy to check that Z(Mn(S))=Z(S)⋅1. This implies that the conditions (ⅰ) and (ⅱ) in Theorem 5.1 are satisfied. We now claim that the condition (ⅲ) in Theorem 5.1 is satisfied.
We set
W={X∈Z(A0)|[X,e1,s+1]=0}. |
It is clear that Z(S)⋅1⊆W. Note that
Z(A0)=Z(A)+Z(B). |
For any X∈W, we may assume that
X=λ1⋅1A+λ2⋅1B, |
where λ1,λ2∈Z(S). We have that
[λ1⋅1A+λ2⋅1B,e1,s+1]=0. |
This implies that (λ1−λ2)e1,s+1=0. Hence, λ1=λ2. It follows that X∈Z(S)⋅1. Thus, W⊆Z(S)⋅1. Hence, W=Z(S)⋅1, as desired. We obtain that Mn(S) satisfies all conditions in Theorem 5.1.
Let f be a supercommuting map of Mn(S). By Theorem 5.1 we have that there exist λ∈Z(S) with 2λMn(S)21=0, and a supercentral map τ:Mn(S)→Z(S)⋅1 such that
f(X)=λX+τ(X) |
for all X∈Mn(S). It suffices to prove that 2λ=0. It is clear that e1,s+1+es+1,1∈Mn(S)1. It follows that
2λ(e11+es+1,s+1)=2λ(e1,s+1+es+1,1)2=0. |
Hence, 2λ=0. This proves the result.
As a consequence of theorem 6.1 we have the following interesting result.
Corollary 6.1. Let S be a 2-torsion free unital algebra. Let Mn(S) be the n×n matrix algebra with n≥2. Then every supercommuting map on Mn(R) is supercentral.
Proof. Let f is a supercommuting map on Mn(S). By Theorem 6.1 we have that f(X)=λX+τ(X), where λ∈Z(S) with 2λ=0, and τ:Mn(S)→Z(S)⋅1. Since S is 2-torsion free we get that λ=0. This implies that f(Mn(S))⊆Z(S)⋅1. This proves the result.
We conclude the section with an example, which implies that a commuting map is not a supercommuting map in general.
Example 6.1. Let S be a 2-torsion free unital algebra. Let Mn(S) be the n×n matrix algebra with n≥2. We defined a linear map f:Mn(S)→Mn(S) by
f(x)=x |
for all x∈Mn(S). Then f is a commuting map on Mn(S), but f is not a supercommuting map on Mn(S).
Proof. It is clear that f is a commuting map. Assume that f is a supercommuting map. By Corollary 6.1 we get that f(x)=x∈Z(S)⋅1 for all x∈Mn(S). In particular, we have that
f(e12)=e12∈Z(S)⋅1, |
which is a contradiction. Hence, f is not a supercommuting map.
Let A be a unital algebra with a nontrivial idempotent e satisfying (1.1). If fAe=0, we have that
A=eAe+eAf+fAf, |
where M is a faithful (A,B)-bimodule. In this case, A is said to be a triangular algebra (see [18,28] for details). Upper triangular matrix algebras and nest algebras are the two usual examples of triangular algebras (see [18] for details).
In 2001, Cheung [18] initiated the study of commuting maps on triangular algebra. He determined the class of triangular algebras for which every commuting map is proper (see [18, Theorem 8]. In 2003, Cheung [28] gave a description of Lie derivations of triangular algebras. In 2012, Du and Wang [20] discussed k-commuting maps of triangular algebras, where k≥1.
We set
A0=eAe+fAfandA1=eAf. |
Note that A=A0⨁A1 is a superalgebra (see [26] for details).
We begin with the following result, which shows that a supercommutator is a commutator in triangular algebras.
Proposition 7.. Let A be a triangular algebra. Then [x,y]s=[x,y] for all x,y∈A.
Proof. For any a,a′∈eAe, m,m′∈eAf, and b,b′∈fAf, we note that
[m,m′]s=0=[m,m′]. |
We get that
[a+m+b,a′+m′+b′]s=[a+b,a′+b′]+[a+b,m′]+[m,a′+b′]+[m,m′]s=[a+b,a′+b′]+[a+b,m′]+[m,a′+b′]+[m,m′]=[a+b,a′+b′+m′]+[m,a′+b′+m′]=[a+b+m,a′+b′+m′]. |
We obtain that [x,y]s=[x,y] for all x,y∈A. This proves the result.
As a consequence of Proposition 7.1, we have the following interesting result.
Corollary 7.1. Every supercommuting map is the same as a commuting map on triangular algebras.
Let A be a unital algebra with nontrivial idempotents. We consider A as a generalized matrix algebra according to Ghahramani and Zadeh's method. We give a description of supercommuting maps on generalized matrix algebras. As a consequence, we give a description of supercommuting maps on matrix algebras, which is different from the result on commuting maps of matrix algebras. We finally prove that every supercommuting map is the same as a commuting map on triangular algebras.
Yingyu Luo: Writing-riginal draft, Funding acquisition; Yu Wang: Validation, Writing-review & editing.
The authors declare they have not used Artificial Intelligence (AI) tools in the creation of this article.
The first author is supported by Scientific Research Foundation of Jilin Province Education Department (JJKH20241000KJ) and Doctoral research start-up fund project of Changchun Normal University.
The authors declare no conflict of interest.
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