This paper characterizes Lie-type derivations on nest algebras over Banach spaces, showing they decompose into derivations and central maps that vanish on specific commutators.
Contribution
It provides a complete description of linear maps satisfying a Lie-type derivation rule on nest algebras, extending understanding of their structure.
Findings
01
Lie-type derivations are sums of derivations and maps vanishing on commutators.
02
Characterization holds for all nest algebras on Banach spaces.
03
The result generalizes previous work on derivations in operator algebras.
Abstract
Let X be a Banach space over the complex field C and B(X) be the algebra of all bounded linear operators on X. Let N be a non-trivial nest on X, AlgN be the nest algebra associated with N, and L:AlgNβΆB(X) be a linear mapping. Suppose that pnβ(x1β,x2β,β―,xnβ) is an (nβ1)-th commutator defined by n indeterminates x1β,x2β,β―,xnβ. It is shown that L satisfies the rule L(pnβ(A1β,A2β,β―,Anβ))=k=1βnβpnβ(A1β,β―,Akβ1β,L(Akβ),Ak+1β,β―,Anβ) for all A1β,A2β,β―,AnββAlgN if and only if there exist a linear derivation D:AlgNβΆB(X) and a linear mapping H:AlgNβΆCI vanishing onβ¦
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Taxonomy
TopicsAdvanced Topics in Algebra Β· Advanced Operator Algebra Research Β· Algebraic structures and combinatorial models
Full text
Lie-Type Derivations of Nest Algebras on Banach Spaces
Yuhao Zhang and Feng Wei
Zhang: School of Mathematics and Statistics, Beijing Institute of
Technology, Beijing, 100081, P. R. China
Let X be a Banach space over the complex field C and B(X) be the algebra of all bounded linear operators on X. Let N be a non-trivial nest on X, AlgN be the nest algebra associated with N, and L:AlgNβΆB(X) be a linear mapping. Suppose that pnβ(x1β,x2β,β―,xnβ) is an (nβ1)-th commutator
defined by n indeterminates x1β,x2β,β―,xnβ. It is shown that L satisfies the rule
[TABLE]
for all A1β,A2β,β―,AnββAlgN if and only if there exist a linear derivation
D:AlgNβΆB(X) and a linear mapping H:AlgNβΆCI vanishing
on each (nβ1)-th commutator pnβ(A1β,A2β,β―,Anβ) for all A1β,A2β,β―,AnββAlgN such that L(A)=D(A)+H(A) for all AβAlgN.
Key words and phrases:
Lie-type derivation, nest algebra, rank one operator
2000 Mathematics Subject Classification:
47L35, 47B47, 17B40
1. Introduction
Let A be an associative algebra over the complex field C, M be an (A,A)-bimodule and
ZAβ(M) be the center of M relative to A, where ZAβ(M):={mβM:aβ m=mβ aΒ Β forΒ allΒ Β aβA}. We shall write just Z(A) to denote ZAβ(A). A linear mapping d:AβΆM is called an (associative)* derivation* if d(xy)=d(x)y+xd(y) holds true for all x,yβA. Let us denote the Lie (resp. Jordan) product of arbitrary elements x,yβA by [x,y]=xyβyx (resp. xβy=xy+yx). A Lie derivation (resp. Lie triple derivation) is a linear mapping L:AβΆM which satisfies the derivation rule according to the Lie product, i.e.,
[TABLE]
for all x,y,zβA. Recall that a linear mapping Ξ΄:AβΆM is a Jordan derivation if Ξ΄(xβy)=Ξ΄(x)βy+xβΞ΄(y) holds true for all x,yβA. Clearly, every derivation is a Lie
derivation as well as a Jordan derivation, and every Lie derivation is a Lie triple derivation. But, the converse statements are not true in general. It should be remarked that every Jordan derivation is also a Lie triple derivation, which is due to the formula [[x,y],z]=xβ(yβz)βyβ(xβz) for all x,y,zβA. Consequently, the class of Lie triple derivations include both classes of Jordan derivations and Lie derivations simultaneously.
Inspired by the definitions of
Lie derivation and Lie triple derivation, one naturally expect to extend them in
one more general way. Suppose that nβ₯2 is a fixed positive
integer. Let us see a sequence of polynomials
[TABLE]
The polynomial pnβ(x1β,x2β,β―,xnβ) is said to be an
(nβ1)-th commutator (nβ₯2).
A Lie n-derivation is a C-linear mapping L:AβΆM which satisfies the rule
[TABLE]
for all x1β,x2β,β―,xnββA. Lie n-derivations were introduced by Abdullaev
[1], where the form of Lie n-derivations of a certain
von Neumann algebra (or of its skew-adjoint part) was described.
According to the definition, each Lie derivation is a Lie 2-derivation and each Lie triple derivation is a Lie
3-derivation. FoΕ‘ner et al [8] showed that every Lie n-derivation
from A into M is a Lie (n+k(nβ1))-derivation for each kβN0β.
Lie 2-derivations, Lie 3-derivations and Lie n-derivations are collectively referred to as Lie-type derivations. Moreover, if
D:AβΆM is an associative derivation and H:AβΆZAβ(M) is a linear mapping vanishing on each (nβ1)-th commutator pnβ(A1β,A2β,β―,Anβ) for all A1β,A2β,β―,AnββA, then the mapping L=D+H is a Lie-type derivation. We
shall say that a Lie-type derivation is of standard form in the case where it can be expressed in the
preceding form. Lie-type derivations and their standard decomposition problems in different backgrounds are extensively studied by a number of people, see [1, 2, 3, 7, 8, 10, 13, 15, 16, 17, 18, 19, 24, 26, 27].
Nest algebras of operators on Hilbert space were introduced in 1965-1966 by
Ringrose [21, 22] and generalize in a certain way the set of all nΓn matrices to infinite dimensions. There has been a great intrest in studying structure theory and various linear mappings of nest algebras on (Hilbert)Banach spaces, culminating in the elegant monograph by Davidson [5]. It was Marcoux and Sourour who initiated the study of Lie-type mappings on nest algebras in [14]. They extended the analysis of Lie automorphisms of non-selfadjoint operator algebras to the infinite dimensional setting by characterizing Lie isomorphisms of nest algebras. Let H be a complex, separable Hilbert space. Let AlgN and AlgM be the nest algebras associated with nests N and M, respectively. A linear mapping Ξ¦:AlgNβΆAlgM is a Lie isomorphism if and only if for all AβAlgN,Ξ¦(A)=Ξ¨(A)+h(A)I, where Ξ¨ is an isomorphism or the negative of an anti-isomorphism and h maps AlgN into the center of AlgM vanishing on all commutators. In the spirit of Marcoux and Sourourβs work, Wang and Lu [25], Qi et al [20] independently obtained similar results for nest algebras on Banach spaces. In another direction, Christensen [4] proved every derivation on a nest algebra to be continuous and implemented. Spivack [23] developed the notion of nest
algebras to sets of operators on Banach space and proved that every continuous derivation on such a nest algebra is implemented by a bounded operator. Lu [13] and Zhang et al [27] independently investigated Lie triple derivations of nest algebras on Hilbert spaces and observed that every Lie triple drivation has the standard form. Sun and Ma [24] generalized this result to nest algebras on Banach spaces by a series of complicated computations. Donsig et al [6] investigated derivations of semi-nest algebras and established a close tie between derivations and cohomology theory of semi-nest algebras.
Motivated by the above works, we will totally characterize all Lie-type derivations of nest algebras on Banach spaces in the current work. It turns out that every Lie-type derivation of nest algebras on Banach spaces is of standard form. It seems to us that this is the ultimate version of this line of characterization theorems in the case of nest algebra setting. It is clear that our main Theorem 3.1 is not only one more common generalization of the afore-mentioned results, but our approach is quite different from that of existing works. For instance, Sun and Ma [24] derived their results by a tedious and complicated computational process. Adopting their methods to achieve our result, it would be an unbelievable task. Our approach is by far more conceptial, and reflects constructive skills strongly. This can be seen by the combinatorial applications of two crucial toolsβrank one operators and the well-known Hanh-Banach theorem.
The outline of this article is organized as follows. We give some basic and necessary facts concerning on nest algebras in the second Section 2. The third Section 3 is devoted to our main Theorem 3.1. Its proof will be realized by a systemic analysis for several different cases.
2. Preliminaries
Let X,Y be complex Banach spaces. Let us denote by B(X,Y) and Hom(X,Y) the Banach space of all bounded linear operators from X to Y and the linear space of all linear operators from X to Y, respectively. We write B(X):=B(X,X) for the algebra of all boundend linear operators from X to itself, and B(X) has an identity, namely the identity operator I. The topological dual spaceXβ of X is defined to be Xβ:=B(X,C), i.e., the Banach space of all bounded linear functionals on X. For arbitrary elements xβX and fβXβ, one can define a rank-one operatorxβf by xβf(y)=f(y)x(βyβX). xβf is an element of B(X) and has the property β₯xβfβ₯=β₯xβ₯β₯fβ₯. For any TβB(X,Y), its adjoint operatorTβ is refered to Tβf(x)=f(Tx)(βfβYβ,xβX). Then β:B(X,Y)βB(Yβ,Xβ) is an isometric embedding. For an arbitrary subset NβX, we denote by Nβ₯:={fβXββ£f(x)=0,βxβN} the annihilator of N. For a subspace VβX, the codimensioncodimV of V in X is defined as the dimension dimX/V of the quotient space X/V. Let us present two elementary results concerning dimension and codimension.
Lemma 2.1**.**
Let X be a normed space, and V be a closed subspace of X. If codimV>1, then there exists fβXββ{0} such that V+span{x}βkerf for all xβX.
Proof.
For an arbitrary xβX, let us set W=V+span{x}. Then W is closed, whch is due to the closedness of V. In addition, codimV>1 implies codimWβ₯1, namely dimX/Wβ₯1. By Hahn-Banach theorem, we know that there is fββ(X/W)ββ{0}. Since W is closed, the quotient mapping ΞΈ:XβX/W,xβ¦x+W is continuous [11, Theorem 1.5.8]. Let us write f=fββΞΈ. And then fβWβ₯ and f is non-vanishing.
β
Lemma 2.2**.**
Let X be a linear space over the complex field C. Suppose that V and W are subspaces of X with codimV=codimW<β. If VβW, then V=W.
Proof.
In view of the fact X/Wβ (X/V)/(W/V),
we have
[TABLE]
which entails W=V.
β
Let X be a Banach space over the complex field C, B(X) be the algebra of all bounded linear operators on X. Let Ξ be an index set. A nest
is a set N={NΞ»β}Ξ»βΞβ of closed subspaces of X
satisfying the following conditions:
(1)
{0},XβN;
2. (2)
If N1β,N2ββN, then
either N1ββN2β or N2ββN1β;
3. (3)
If {NΞ»β}Ξ»βΞββN,
then βΞ»βΞβNΞ»ββN;
4. (4)
If {NΞ»β}Ξ»βΞββN, then the
norm closure of the linear span of βiβΞβNΞ»β also lies
in N.
If N={{0},X}, then N is called a
trivial nest, otherwise it is called a non-trivial nest. As usual, we set βΞ»βΞβNΞ»β:=βΞ»βΞβNΞ»β, βΞ»βΞβNΞ»β:=spanβΞ»βΞβNΞ»ββ.
The nest algebra associated with the nest N, denoted by
AlgN, is the weakly closed operator algebra
consisting of all operators that leave N invariant,
i.e.,
[TABLE]
It should be remarked that every finite dimensional nest algebra
is isomorphic to a real of complex block upper triangular matrix
algebra. If N is trivial, then
AlgN=B(X), which is a prime algebra over
the real or complex field C. In this paper we only
consider the nontrivial nest algebras.
Let N be a nest on a complex Banach space
X such that there exists a NβN
complemented in X and AlgN be the
nest algebra associated with N. Then AlgN is a
triangular algebra over C. Indeed, Since NβN is complemented in X, there is a bounded
idempotent operator P with range N. It is easy to check that
PβAlgN. Let us denote M=(IβP)(X),
and let A=PAlgNβ£Nβ,M=PAlgNβ£Mβ and
B=(IβP)AlgNβ£Mβ. Then
AβMBβ is faithful as left
A-module and right B-module. We therefore say that
[TABLE]
Note that AlgN is a central algebra over its center Z(AlgN)=CI.
In particular, if X is a Hilbert space, then every nontrivial nest algebra is a
triangular algebra. Indeed, if NβN\{{0},X}
and E is the orthogonal projection onto N, then
N1β=E(N) and
N2β=(1βE)(N) are nests of N and Nβ₯,
respectively. Moreover,
AlgN1β=EAlgNE,AlgN2β=(1βE)AlgN(1βE) are
nest algebras and
[TABLE]
However, it is not always the case for a nest N on a
general Banach space X, since NβN may be not
complemented. We refer the reader to [5] for the theory
of nest algebras.
For a Banach space X, if N is a non-trivial nest on X, then there exist an NβNβ{{0},X} and a non-vanishing fβNβ₯ (By Hahn-Banach theorem we get a non-vanishing fββ(X/N)β, where N is a closed subspace. And hence the mapping g:XβX/N is continuous. It suffices to take f=fββg). We therefore have X/kerfβ C. By the fact dimkerfβ₯1, we know that the dimension of X is no less than 2. For an arbitrary NβN, one can define
[TABLE]
and we set {0}ββ:={0}, X+β:=X.
Lemma 2.3**.**
([24, LemmaΒ 2.1])*
Let N be a nest on a Banach space X. Then xβfβAlgN if and only if there exists NβN such that xβN and fβNββ₯β:=(Nββ)β₯ and equivalently, if and only if there exists NβN such that xβN+β and fβNβ₯.*
Let A be an associative algebra over the complex field C, M be an (A,A)-bimodule and
ZAβ(M) be the center of M relative to A.
Proposition 2.4**.**
([8, Proposition 1.1])*
Let L:AβM be a Lie n-derivation. Then for each kβN, L is also a Lie n+k(nβ1)-derivation. In particular, if L a derivation, then L is also a Lie n-derivation.*
Proposition 2.5**.**
Let D:AβM be a derivation and H:AβZAβ(M) be a linear mappping. Then D+H is a Lie n-derivation if and only if H is a linear mapping vanishing on each (nβ1)-th commutator pnβ(A1β,β―,Anβ) for all A1β,A2β,β―,AnββA.
Proof.
The sufficiency is straightforward and we only prove the necessity. If L=D+H is a Lie n-derivation, then H=LβD is a linear mapping. It follows from Proposition 2.4 that
[TABLE]
for all A1β,β―,AnββA. And hence H(pnβ(A1β,β―,Anβ))=0.
β
The following lemma is one common generalization of [9, Problem 230].
Lemma 2.6**.**
Let A,BβB(X), Ξ»βC. If [A,B]=Ξ»I, then Ξ»=0.
Proof.
According to the assumption [A,B]=Ξ»I, we see that
[TABLE]
A direct induction on n shows that AnBβBAn=nΞ»Anβ1. If the nilpotent index of A is nβN, then Ξ»=0. If A is not nilpotent, then
*If {0}ξ =NβN and TβB(X) satisfy TA=AT *(on N) for all AβAlgN, then there exists Ξ»βC such that T=Ξ»I on N.
2. (2)
ZAlgNβ(B(X))=CI.
Taking into account Lemma 2.6 and Lemma 2.8 and using induction on n, it is not difficult to prove
Lemma 2.9**.**
Let N be a nest on a Banach space X and L:AlgNβB(X) be a Lie n-derivation. Then L(I)=Ξ»I for some Ξ»βC.
3. Lie-Type Derivations of Nest Algebras
Let us first state our main theorem of this article.
Theorem 3.1**.**
Let X be a Banach space, N be a non-trivial nest on X and AlgN be the nest algebra associated with N. Then every Lie-type derivaion from AlgN into B(X) is of standard form.
More precisely, L:AlgNβB(X) is a Lie n-derivation if and only if there exist a derivation D:AlgNβB(X) and a linear mapping H:AlgNβCI vanishing on each (nβ1)-th commutator on AlgN such that L=D+H. In particular, if L is continuous, then D and H are continuous as well.
As a matter of fact, we will investigate more general cases, i.e., on certain subalgebras of AlgN. For reading convenience, we have to introduce some notations. Let N be a non-trivial nest on a Banach space X, and A be a subalgebra of AlgN. Define
[TABLE]
and
[TABLE]
We put forward the following conditions.
(β 1)
Xββ₯β(A)ξ ={0} is a linear space.
2. (β 2)
For each fβXββ₯β(A), there exists yβXβXββ such that yβfβA.
3. (β 3)
The set of all rank-one operators in A contains {xβfβ£xβX(A),fβXββ₯β(A)}.
4. (β 4)
For any AβA, xβX(A) and fβXββ₯β(A), AxβX(A) and AβfβXββ₯β(A) hold true.
It is not difficult to figure out that not all subalgebras satisfy the above conditions, while there are certain subalgebras satisfying all these conditions (e.g. AlgN itself). (β 3) implies that X(A) and Xββ₯β(A) are normed linear spaces which inherite the norm of X and that of Xβ, respectively. The condition (β 4) implies that the dimension X is greater than 2. As you see, we will address the standard form question of Lie-type derivations of a subalgebra A satisfying some of the above conditions in the next several subsections.
By Proposition 2.5 and Lemma 2.8, the sufficiency of our main Theorem 3.1 is clear. We shall give the proof of its necessity by a systemic analysis for several different cases.
3.1. The case of dimXββ₯β=1
Under this case, one can loosen the condition of LemmaΒ 2.8 slightly as follows.
Lemma 3.2**.**
Let N be a nest on a Banach space X with dimXββ₯β=1. If A is a subalgebra of AlgN satisfying the conditions (β 1) and (β 5), then ZAβ(B(X))=CI.
Proof.
By dimXββ₯β=1 we know that Xβββ«X. The condition (β 1) implies that Xββ₯β=Xββ₯β(A). For any yβXβXββ, by Hahn-Banach theorem (pick fββ(X/Xββ)β such that fβ(y+Xββ)=1, and let f=fββΞΈ, where ΞΈ is the quotient mapping), it follows that there exists fβXββ₯β such that f(y)=1. Since dimXββ₯β(A)=1 and X(A)=X, we get xβfβA(βxβX). Thus for any AβZAβ(B(X)), we have A(xβf)y=(xβf)Ay. That is, Ax=f(Ay)x. By the arbitrariness of x, we assert that AβCI.
β
Theorem 3.3**.**
Let N be a non-trivial nest of a Banach space X with dimXββ₯β=1. Suppose that A is a subalgebra of AlgN satisfying (β 1), (β 2), XβββX(A) and IβA. Then each Lie-type derivation from AlgN into B(X) is of standard form. Precisely speaking, for any Lie n-derivation L:AβB(X), there exists a derivation D:AβB(X) and a linear mapping H:AβCI vanishing on all (nβ1)-th commutators of A such that L=D+H. Moreover, if L is continuous, then D and H are continuous.
Remark 3.4**.**
The conditions what the subalgebra A satisfies amount to saying (β 1), X(A)=X and IβA.
Proof.
By dimXββ₯β=1 and (β 1) it follows that Xββ₯β=Xββ₯β(A). If codimXββ>1, then there are linear independent elements x1β+Xββ and x2β+Xββ in X/Xββ. By an analogous proof of LemmaΒ 2.1, one can construct f1β,f2ββXββ₯β satisfying fiβ(xjβ)=Ξ΄ijβ, where Ξ΄ijβ is the Kronecker sign. Then f1β,f2β are linear independent, which contradicts with dimXββ₯β=1. Thus we assert codimXββ=1. Basing on this fact, we know that for any fβXββ₯ββ{0}, kerf=Xββ holds true. Fixing certain f0ββXββ₯β(A)β{0}=Xββ₯ββ{0}, by (β 2), there exists yβXβXβ such that yβf0ββA. Denote M=span{y}, and then X=XβββM. Indeed, since Ο:MβX/Xββ,yβ¦y+Xββ is an isomorphism, and then for any fβXββ₯ββ{0}, Οfβ:X/XβββC,y+Xβββ¦f(y) is also an isomorphism by fundamental theorem of homomorphism. We therefore have Mβ ΟfββΟC. Let us take xβX and fβXββ₯ββ{0}. Then there exists yβM with f(y)=ΟfββΟ(y)=f(x). Henceforth xβyβkerf=Xββ, i.e., XβXββ+M.
Let us choose x0ββM such that f0β(x0β)=1, and define P=x0ββf0ββA and set Q=IβP. Then P and Q are idempotents satisfying PQ=QP=0, PX=M and QX=Xββ. We get the Peirce decomposition B(X)=PB(X)PβPB(X)QβQB(X)PβQB(X)Q. For any AβA, since dimXββ₯β=1 and Aβf0ββXββ₯β=Xββ₯β(A), there exists Ξ»AββC such that Aβf0β=Ξ»Aβf0β. Therefore
[TABLE]
Thus A=A11ββA21ββA22β, where A11β=PAP, A21β=QAP, A22β=QAQ.
We assert that there is a derivation D:AβB(X) such that the Lie n-derivation L=LβD satisfy the following conditions: if AβAiiβ(i=1,2), then L(A)βHiiβ(A)IβBiiβ, where Hiiβ:AiiββC is a linear mapping, and B11β=PB(X)P, B22β=QB(X)Q; if AβA21β, then L(A)βB21β:=QB(X)P. Let us prove this assertion in two cases.
Case 1: n is odd. For an arbitrary AβA21β, we have AQ=0 and QA=A. A direct computation shows that
[TABLE]
Multiplying Q (resp. P) from the left (resp. right) side of (3.1), we obtain
[TABLE]
For any xβXββ, since XβββX(A) and Xββ₯β(A)=Xββ₯β is 1-dimensional, we thus get A0β=xβf0ββA. Obviously, A0β=QA0βPβA21β and hence
[TABLE]
Using (3.2) to act on x0β, we have
[TABLE]
The arbitrariness of xβXββ implies that
[TABLE]
A direct verification gives
[TABLE]
Combining (3.3) with (3.4) we obtain
[TABLE]
Let us write T=PL(Q)QβQL(Q)P, and define DTβ(β )=[T,β ]. Then DTβ is a (continuous) derivation of A satisfying the condition
[TABLE]
Let us put L=LβDTβ. Then L is a Lie n-derivation on A and L(Q)=f0β(L(Q)x0β)I. A straightforward computation yields that
[TABLE]
For any Aβ²βA21β and BβA, we get
[TABLE]
By LemmaΒ 2.6, LemmaΒ 3.2 and a recursive computation, we arrive at [L(A),Aβ²]+[A,L(Aβ²)]=Ξ»I, where Ξ»βC. Thus
[TABLE]
We therefore have [PL(A)Q,Aβ²]=21βΞ»I. By LemmaΒ 2.6, it follows that [PL(A)Q,Aβ²]=0. Multiplying by P on the left side, we get PL(A)QAβ²=0. In particular, PL(A)QA0β=0. Considering its action on x0β, we obtain PL(A)Qx=0. Note that QM={0}, and thus PL(A)Q=0. And hence L(A)=QL(A)PβB21β.
For an arbitrary AβA22β, we have
[TABLE]
So 0=QL(A)P=PL(A)Q. This gives that L(A)=QL(A)Q+PL(A)P. For any BβA11β and Aβ²βA, we get
[TABLE]
Taking into account LemmaΒ 2.6 and LemmaΒ 3.2 and using a recursive computation, we conclude that [L(A),B]+[A,L(B)]=ΞΌI, where ΞΌβC. Since BβA11β, [L(A),B]=[PL(A)P,B]. Thus we obtain
[TABLE]
Looking on the above equation as an operator equation over PX=M and using Lemma 2.6, we see that ΞΌ=0. In particular, take B=xβf0ββA11β, where xβM. Considering the action of [PL(A)P,xβf0β]=0 on x0β, we get
[TABLE]
where H22β(A)=f0β(PL(A)x0β)IβCI. The preceding equality shows the linearity and boundedness (if L is bounded) of H22β(A) for all AβA22β. Moreover, we have
[TABLE]
By an analogous manner, one can prove that for any AβA11β, there exists a linear operator (and bounded if L is bounded) H11β:A11ββCI such that L(A)βH11β(A)βB11β.
Case 2: n is even. For an arbitrary AβA21β, a direct calculation shows that
[TABLE]
Multiplying by Q on the left side of (3.5) and by P on the right side of (3.5), we obtain
[TABLE]
Adopting the same discussion as in Case 1, we have
[TABLE]
Denote DTβ(β )=[T,β ] and L=LβDTβ. Then L(Q)=f0β(L(Q)x0β)I. Thus
[TABLE]
Therefore L(A)=QL(A)PβPL(A)Q. For an arbitrary Aβ²βA21β and BβA, a straightforward computation shows that
[TABLE]
By LemmaΒ 2.6, LemmaΒ 3.2 and a recursive computation, we conclude
[TABLE]
where Ξ»βC. And hence
[TABLE]
This forces Ξ»=0. By (3.6) we get
[TABLE]
Multiplying by Q on the right side of (3.7), we obtain (L(A)Aβ²+L(Aβ²)A)Q=0. Multiplying by P on the left side of (3.7), we have P(L(A)Aβ²+L(Aβ²)A)=0. Let us put S=L(A)Aβ²+L(Aβ²)A. Then we see that
[TABLE]
On the other hand, since L(Aβ²)=QL(Aβ²)PβPL(Aβ²)Q, we by (3.6) arrive at
[TABLE]
Thus
[TABLE]
Therefore PL(A)Aβ²=PL(Aβ²)A and AL(Aβ²)Q=Aβ²L(A)Q. Applying the fact PS=0 yields that PL(A)Aβ²=0. In particular, for Aβ²=xβf0ββA21β, where xβXββ, the relation
[TABLE]
holds true. Considering its action on x0β, we observe that PL(A)Qx=0. Since QM=0, we get PL(A)Q=0 and hence L(A)=QL(A)PβB21β.
For an arbitrary AβA22β, a direct calculation shows that
[TABLE]
This gives QL(A)P=PL(A)Q=0. Thus L(A)=QL(A)Q+PL(A)P. The remainder proving process and the discussion for AβA11β are identical with the counterparts of Case 1, we do not repeat them here. Unitl now we complete the proof of the assertion.
We now come back and continue to prove this theorem. For an arbitrary A=A1β+A2β+A3ββA=A11ββA21ββA22β, we establish a mapping
[TABLE]
The linearity of Hiiβ(i=1,2) implies that H is linear. If L is continuous, by properties of direct product, it is not difficult to verify the continuity of H. Define a mapping D:AβB(X) via the relation D=LβH. Then D is a linear mapping such that D(A1β)βB11β, D(A2β)βB21β and D(A3β)βB22β.
We next illustrate that D is a derivation. In light of the fact
[TABLE]
we see that
[TABLE]
For an arbitrary A3β²ββA22β, it follows that
[TABLE]
On the other hand, we have
[TABLE]
Comparing the relations (3.8) with (3.9) yields
[TABLE]
In particular, take A2β=xβf0β, where xβXββ. Using (3.10) to act on x0β, we obtain
[TABLE]
In view of the fact QM={0}, we know that
[TABLE]
For the case of
[TABLE]
its discussion is parallel with that of case A3βA2β, and for the case of A1βA1β²β (where A1β²ββA11β), its proving process is totally similar to the proof of the case A3βA3β²β.
For arbitrary elements A=A1β+A2β+A3β, B=B1β+B2β+B3ββA=A11ββA21ββA22β, we eventually get
[TABLE]
This shows that D is a derivation. Let D=D+DTβ (DTβ is the derivation established in the previous assertion). Then D is a (continuous, if L is continuous) derivation, and has the decomposition
[TABLE]
By PropositionΒ 2.5, we know that H:AβCI vanishes on each (nβ1)-th commutator on A.
β
In particular, if X is a 2-dimensional Banach space, then a consequence of Theorem 3.3 is
Corollary 3.5**.**
Suppose that dimX=2 and that N={{0},N,X} is a non-trivial nest on X. Then each Lie-type derivation from AlgN into B(X) is of standard form. Precisely speaking, for any Lie n-derivation L:AlgNβB(X), there exists a derivation D:AlgNβB(X) and a linear mapping H:AlgNβCI vanishing on all (nβ1)-th commutators of AlgN such that L=D+H. Moreover, if L is continuous, then D and H are both continuous.
3.2. The case of dimXββ₯β>1
Lemma 3.6**.**
Let X be a Banach space with dimX>2, Xβββ«X and N be a non-trivial nest on X. If a subalgebra AβAlgN satisfies the conditions (β 1)β(β 4), and L:AβB(X) is a Lie n-derivation, then there is a bilinear mapping h:X(A)ΓXββ₯β(A)βC such that
The case of f=0 is trivial. We next assume that fβXββ₯β(A)β{0}. If xβkerf, by (β 2), there exists yβXβXββ such that f(y)=1 and yβfβA. Let us put yβ²=y+x. Then yβ²βX(A) and y,yβ²,x are linearly independent. For any zβkerf, a direct computation shows that
[TABLE]
By an analogous manner, we have
[TABLE]
The linear independence of y,yβ²,x implies that f(L(xβf)z)=0. We therefore have L(xβf)zβCx.
Thus h(x,f) is continuous at x for a fixed fβXββ₯β(A). Since X(A)=X is a linear space, the linear functional hfβ(x):=h(x,f) is continuous. Namely, h(x,f) is continuous for x.
β
Suppose that A is a subalgebra of AlgN satisfying the conditions (β 1)β(β 5) and that L:AβB(X) is a Lie n-derivation. For an arbitrary fβXββ₯β(A)β{0}, denote I(f)={yβX(A)β£f(y)=1}ξ =β . For any yβI(f), one can define a mapping Ξ¦f,yβ:X(A)βX as follows
[TABLE]
By linearity of L and bilinearity of h, we can see that Ξ¦af,yβ=Ξ¦f,ayβ(ayβI(f),aβCβ{0}). By Lemma 3.6, the following relation
Οx,fβ* is not related with the choice of x. In this case, we write Οfβ for Οx,fβ, and write Οf,yβ for Οx,f,yβ.*
Proof.
Let us take fβXββ₯β(A)β{0} and yβI(f). For linearly independent x1β,x2ββXβ{0}, we arbitrarily pick zβkerf. By LemmaΒ 3.7 it follows that
[TABLE]
from which we get (note that Οx,f,yβ is an extension of Οx,fβ)
[TABLE]
We therefore have Οx1β,fβ=Οx1β+x2β,fβ=Οx2β,fβ. Since dimXββ₯β>1, we see that dimX>1. For linearly dependent x1β,x2ββX, we can choose x3β such that x3β,x1β are linearly independent. In view of the previous proof, we conclude that Οx1β,fβ=Οx3β,fβ=Οx2β,fβ.
β
Lemma 3.9**.**
For any f1β,f2ββXββ₯β(A)β{0} and yjββI(fjβ)(j=1,2), we have
[TABLE]
Proof.
If f1β and f2β are linearly independent, then by [11, Proposition 1.1.1], kerf1β and kerf2β do not contain mutually. Thus there are x1β,x2ββX=X(A) such that fiβ(xjβ)=Ξ΄ijβ, where Ξ΄ijβ is the Kronecker sign. For any xβX, it follows that
[TABLE]
where yβ²βI(f1β+f2β). Applying (3.14) to x1ββx2β yields
[TABLE]
If f1β and f2β are linearly dependent, then we can assume f1β=af2β and aξ =0. It is easy to see that ay1ββI(f2β). We now arrive at
Thus f(Ξ¦f,yβz)+Οf,yβ(z)=h(z,f)=0. Then by f(Ξ¦f,yβy)=f(L(yβf)y)βh(y,f)=0, Οf,yβ(y)=0 and kerf+I(f)=X, we finish the proof.
β
We are in a position to give our main result of this subsection.
Theorem 3.11**.**
Let X be a Banach space with dimX>2 and N be a non-trivial nest on X. Suppose that A is a subalgebra of AlgN satisfying (β 1)β(β 6) and dimXββ₯β(A)>1. Then each Lie-type derivation is of standard form. More precisely, for any Lie n-derivation L:AβB(X), there exists a derivation D:AβB(X) and a linear mapping H:AβCI vanishing on all (nβ1)-commutators on A such that L=D+H. In particular, if L is continuous, then D and H are continuous as well.
Proof.
For any xβXβ{0}, by Lemma 2.1, there exists fβXββ₯β(A)β{0} such that f(x)=0. For a fixed yβI(f), let us define a mapping D(β )=[Ξ¦f,yβ,β ]:AβHom(X,X). In view of Lemma 3.9, we can say that D is a linear operator (bounded and D:AβB(X), if L is continuous) which is not related with the choice of f,y. Let us first consider the case of n>2. For an arbitrary AβA, by Lemma 3.7, a straightforward computation shows that
[TABLE]
On the other hand, we have
[TABLE]
We shall calculate those terms of (3.16) in turn. Let us see the first term in (3.16).
[TABLE]
The second term in (3.16) is
[TABLE]
The remainder terms in β (for the case of 3β€jβ€n) of (3.16) are
[TABLE]
Combining equation (3.15) with equation (3.16) and considering their actions on x, we obtain
[TABLE]
Thus h(Ax,f)βf(Ax)h(y,f)=0. In the case of n is odd with n>3. Using (3.15) and (3.16) to act on y, we arrive at
[TABLE]
In the case of n is even with n>3. Taking into account the actions of (3.15) and (3.16) on y, we get
[TABLE]
For the case of n=3, by an analogous calculation we have
[TABLE]
Therefore, for the case of n>3, there exist aA,f,yβ,bA,f,yββC such that
[TABLE]
Since dimX>2, dimkerf>1. Thus there exists zβkerf such that z,x are linearly independent. Then x,y,y+z are linearly independent. Indeed, if ax+by+c(y+z)=0 (a,b,cβC), then ax+(b+c)y+cz=0. While yβ/kerf, and hence b+c=0. By the fact that x,z are linearly independent, it follows that a=b=c=0. Note that y+zβI(f). Repeating the above discussion again gives
[TABLE]
Note that D(A)=[Ξ¦f,yβ,A]=[Ξ¦f,y+zβ,A]. By (3.17) and (3.18) we conclude
[TABLE]
which entails bA,f,yβ=0. It follows from (3.17) that (L(A)βD(A))xβkerf. For an arbitrary yβ²βI(f), applying f to the following equation
[TABLE]
we then obtain bA,f,yβ²β=0. So (L(A)βD(A))x=βaA,f,yβ²βx. The arbitrariness of yβ² shows that aA,f,yβ is not related with the choice of yβI(f). Thus we denote it by aA,fβ. Similarly, changing fβXββ₯β(A)β{0} satisfying the condition f(x)=0, we can see that aA,fβ is merely related with the choice of x. Thus we may write Hxβ(A):=βaA,fβ. Therefore the following equality holds:
[TABLE]
For the case of n=2, if Aβfξ =0, fixing yβ²βI(Aβf), by Lemma 3.9 we assert that Ξ¦Aβf,yβ²ββΞ¦f,yβ=cI. Let us put ΟAβfβ=Οf,yβ+cf. Furthermore, we can calculate
[TABLE]
and
[TABLE]
Thus we arrive at
[TABLE]
By an analogous manner, we also have (Let us write y1β=y, y2β=y+x)
[TABLE]
If Aβf=0, adopting similar discussion we can also obtain equation (3.20) and equation (3.21) only if we substitute [math] for ΟAβfβ and h(β ,Aβf). Applying (3.20) to y yields
[TABLE]
Applying (3.21) to x gives
[TABLE]
It is not difficult to see that x and yiβ(i=1,2) are linearly independent. So h(Ay1β,f)βh(y1β,Aβf)=0 and h(Ay2β,f)βh(y2β,Aβf)=0. Their difference gives h(Ax,f)βh(x,Aβf)=0. By invoking (3.22) we know that f(L(A)y)+Οf,yβ(Ay)βΟAβfβ(y) is merely related with the choice of x and A, and we denote it by Hxβ(A). Therefore for any xβX, the equality (3.19) still holds true in the case of n=2. That is,
Let X be a Banach space with dimX>2 and N be a non-trivial nest on X. If Xβββ«X, then each Lie-type derivation on AlgN is of standard form. That is, for any Lie n-derivation L:AlgNβB(X), there exists a derivation D:AlgNβB(X) and a linear mapping H:AlgNβCI vanishing on all (nβ1)-commutators on AlgN such that L=D+H. In particular, if L is continuous, then D and H are continuous as well.
Proof.
If codimXββ>1, then by Hahn-Banach theorem we can construct x1β,x2ββXββ and f1β,f2ββXββ₯β such that fiβ(xjβ)=Ξ΄ijβ, where Ξ΄ijβ is the Kronecker sign. Thus f1β and f2β are linearly independent, which entails dimXββ₯β>1. Then by Theorem 3.11 and Lemma 2.8, we immediately get the conclusion.
If codimXββ=1, then for any fβXββ₯ββ{0}, we have codimkerf=1 and Xβββkerf. By Lemma 2.2 it follows that Xββ=kerf. Taking into account [11, PropositionΒ 1.1.1] we get dimXββ₯β=1. In view of Theorem 3.3, the proof is completed.
β
Let X be a normed space with a nest N. We denote the null element of Xβ by 0. Define Nβ:={Nβ₯β£NβN}. It is not difficult to verify that Nβ is a nest of Xβ. We will see that the condition Xβββ«X is dual with {0}β«{0}+β in the following sense.
Proposition 3.13**.**
Let N be a nest on a normed space X. Then Xβββ«X if and only if {0}β«{0}+β.
Proof.
It follows from Xβββ«X that {0}=Xβ₯β«Xββ₯β, in which the strict inclusion relation is given by Hahn-Banach theorem. For any fβXβ, we have
[TABLE]
Thus Xββ₯β={0}+β, and hence {0}β«{0}+β.
Take fβ{0}+ββ{0}, and then for any xβNβ«X, we have f(x)=0. The continuity of f implies that f\Big{(}\bigvee_{N\subsetneqq\mathcal{X}}N\Big{)}=\{0\}. Since fξ =0, we get f(X)ξ ={0}. Therefore Xβββ«X.
β
Remark 3.14**.**
By an analogous manner, one can show that Xββββ«Xβ if {0}β«{0}+β. Indeed, for an arbitrary f\in\mathcal{X}^{*}_{-}=\big{(}\bigvee_{N^{\bot}\subsetneqq\mathcal{X}^{*}}N^{\bot}\big{)}, we know that f=limnβββfnβ holds true, where fnβββNβ₯β«XββNβ₯. It follows that f\in\big{(}\bigwedge_{N\neq\{0\}}N\big{)}^{\bot}. Thus Xββββ{0}+β₯ββ«{0}β₯=Xβ.
For a nest N on a Banach space X, we define (AlgN)β={Aββ£AβAlgN}. It is easy to figure out that (AlgN)β is a subalgebra of AlgNβ. Since β:B(X)βB(Xβ) is an isometry, the completeness of AlgN entails that (AlgN)β is complete. Thus (AlgN)β is a closed subalgebra of AlgNβ.
Lemma 3.15**.**
If L:AlgNβB(X) is a Lie n-derivation, then the mapping
[TABLE]
is a Lie n-derivation on (AlgN)β. If L is continuous, then Lβ is continuous.
Proof.
Linearity of Lβ is straightforward. If L is continuous, since β is continuous, the continuity of Lβ follows. For arbitrary elements A1β,β―,AnββAlgN, we obtain
[TABLE]
This shows that Lβ is a Lie n-derivation.
β
Note that (xβf)β=fβxββ(xβX,fβXβ), from which it is easy to see that if dimX>2 and {0}β«{0}+β. Then A:=(AlgN)β, as a subalgebra of AlgNβ, satisfies (β 1)β(β 6). Indeed, (Xβ)ββ₯β(A)={xβββ£xβ{0}+β} is a linear space, and hence A satisfies (β 1). Applying Remark 3.14 yields (β 2). Considering Lemma 2.3, one can see that (β 5) holds true (For any fβXβ, pick xβ{0}+ββ{0} and we get (xβf)ββA); other conditions are easily to be verified.
Corollary 3.16**.**
Let X be a Banach space with dimX>2 and N be a non-trivial nest on X. If {0}β«{0}+β, then each Lie-type derivation on AlgN is of standard form. More precisely, for any Lie n-derivation L:AlgNβB(X), there exist a derivation D:AlgNβB(X) and a linear mapping H:AlgNβCI vanishing on all (nβ1)-commutators on AlgN such that L=D+H. In particular, if L is continuous, then D and H are continuous as well.
Suppose that N0ββNβ{{0},X} is of finite codimension. Then the set {NβNβ£N0ββ«Nβ«X} is a finite set. Indeed, for N0ββ«N, by the fact X/Nβ (X/N0β)/(N/N0β), dimX/N has at most dimX/N0β=codimN0β<β possible choices. Moreover, since N is totally ordered, we see that X/N has at most codimN0β possible choices. Let us write {NβNβ£N0ββ«Nβ«X}={Njβ}j=0mβ, which is an increasing sequence under inclusion relation. Then
(3) We use reduction to absurdity. If NΞ»ββkerf holds true for any Ξ»βΞ, then βΞ»βΞβNΞ»β=X. This implies that kerf=X, a contradiction.
β
Without loss of generality, we next assume that {NΞ»β}Ξ»βΞββNβ{{0},X} is a net satisfying βΞ»βΞβNΞ»β=X. For fβXββ{0}, put I(f):={yβXβ£f(y)=1}ξ =β .
Lemma 3.18**.**
Let X be a Banach space and N be a non-trivial nest satisfying (β£) β£ 3.3. If L:AlgNβB(X) is a Lie n-derivation, then for any Ξ»βΞ, there exists a bilinear functional hΞ»β:NΞ»βΓ(NΞ»β)ββ₯ββC such that
[TABLE]
In particular, if L is continuous, then hΞ»β(x,f) is continuous for x.
Then by linear independence, the above two equalities (3.24) and (3.25) entail f1β(L(xβf)y1β)=f2β(L(xβf)y2β). Let us define hΞ»β(x,f)=f1β(L(xβf)y1β), which is well-defined by the above deduction. It is clear that hΞ»β(x,f) is continuous for xβNΞ»β if L is continuous.
That is, hΞ»β(x,f) is linear regarding to f as well.β
For an arbitrary fβ(NΞ»β)ββ₯ββ{0} and yβI(f), with similar discussion as in Section 3.2, one can define a linear operator (bounded if L is continuous) Φλ,f,yβ:NΞ»ββX by
Let X be a Banach space and N is a non-trivial nest on X satisfying the condition (β£) β£ 3.3.
(1)
For any Ξ»βΞ, xβNΞ»β and fβ(NΞ»β)ββ₯β, we have
[TABLE]
2. (2)
ΟΞ»,x,fβ* is not related with the choice of xβNΞ»β, and thus we write ΟΞ»β for ΟΞ»,xβ, and write ΟΞ»,f,yβ for ΟΞ»,x,f,yβ.*
3. (3)
For any fjββ(NΞ»β)ββ₯ββ{0} and any yjββI(fjβ)(j=1,2), we have Φλ,f1β,y1βββΦλ,f2β,y2βββCIβ£NΞ»ββ.
The proof of this lemma is parallel with proofs of Lemma 3.7, Lemma 3.8 and Lemma 3.9, and hence we do not repeat them here.
Lemma 3.20**.**
Let X be a Banach space and N be a non-trivial nest on X satisfying the condition (β£) β£ 3.3. If L:AlgNβB(X) is a Lie n-derivation, then for any AβAlgN and Ξ»βΞ, the equality L(A)β£NΞ»ββ=DΞ»β(A)+HΞ»β(A) holds true, where DΞ»β:AlgNβB(NΞ»β,X) is a derivation given by DΞ»β(A)x=Φλ,f,yβAxβAΦλ,f,yβx(βfβNΞ»β₯ββ{0},βyβI(f),βxβNΞ»β) and HΞ»β:AlgNβCIβ£NΞ»ββ is a linear mapping. Moreover, if L is continuous, then DΞ»β and HΞ»β are continuous.
Remark 3.21**.**
For any BβB(NΞ»β,X) (or Hom(NΞ»β,X)) and AβAlgN, let us define BAβB(NΞ»β,X) (or Hom(NΞ»β,X)) by BAx=B(Ax)(βxβNΞ»β). Then B(NΞ»β,X) (or Hom(NΞ»β,X)) becomes an (AlgN,AlgN)-bimodule. For any fjββNΞ»β₯ββ{0} and yjββI(Fjβ), we by Lemma 3.19 assert that [Φλ,f1β,y1ββ,A]=[Φλ,f2β,y2ββ,A] for all AβAlgN. Thus DΞ»β:AlgNβHom(NΞ»β,X) is well-defined. In what follows we will prove the fact that DΞ»β:AlgNβB(NΞ»β,X).
Given fβ²βNΞ»β₯ββ{0} and yβ²βI(f), by invoking Lemma 3.19 we see that Φλ,f,yββΦλ,fβ²,yβ²β=cΞ»,fβ²,yβ²βIβ£NΞ»ββ, and we define ΟΞ»,fβ²β:=ΟΞ»,f,yβ+cΞ»,fβ²,yβ²βI, where cΞ»,fβ²,yβ²β=0 if fβ²=f, yβ²=y. Then by Lemma 3.19 we get
[TABLE]
Under the above notations, for arbitrary xβNΞ»β, a direct computation shows that
[TABLE]
On the other hand, we have
[TABLE]
Let us calculate each term in the right side of (3.28). The first and second terms in the right side of (3.28) are
Comparing (3.27) with (3.28), noticing that I has infinitely rank, we have that hΞ»β(Ax,g)βf(Ay)hΞ»β(x,g)=0. Combining (3.27) with (3.28) and considering their actions to z, we obtain
It follows from yβ/NΞ»β that the coefficient of y in (3.29) is [math] (otherwise yβspan{(L(A)β[Φλ,f,yβ,A])x,Ax,x}βNΞ»β, a contradiction). Observing the coefficients of Ax and x in (3.29), we can find that
[TABLE]
where cΞ»ββC is merely related with Ξ»,f,y and is not related with the choice of x, and HΞ»β(A)βCI is only related with Ξ»,A,f,y and is nothing relation with the choice of x.
Let us next show that cΞ»β=0. We use reduction to absurdity. Suppose that cΞ»βξ =0. For any A1β,β―,AnββAlgN and an arbitrary xβNΞ»β, by what has been proved we have
[TABLE]
Here, the last equality is due to the fact that DΞ»β is a derivation and hence a Lie n-derivation (Proposition 2.4). this shows that
[TABLE]
Restricting the above equation to NΞ»β, by Lemma 2.6 we obtain that
[TABLE]
That is, pnβ(A1β,β―,Anβ)β£NΞ»ββ=0, which is obviously absurd. Indeed, for an arbitrary NβNβ{{0}} satisfying Nβ«NΞ»β and vβNΞ»ββN, we define a bounded linear functional w0β on the subspace span{v+N} of X/N by w0β(av+N):=a. By Hahn-Banach theorem, we get an extension wβ(X/N)β. Let w=wβΟ, where Ο:XβX/N is the quotient mapping. Then wβNβ₯ and w(v)=1. For any uβNβ{0}, we have uβw=pnβ(uβw,vβw,β―,vβw)=0, while uβw(v)=uξ =0, a contradiction.
Let us now consider the case of n=2. For any fβNΞ»β₯ββ{0}, yβI(f) and an arbitrary xβNΞ»β, we get
[TABLE]
and
[TABLE]
Combining (3.30) with (3.31) gives
[TABLE]
Since I is of infinite rank, we arrive at
[TABLE]
Considering the action of (3.32) on y, we finish the proof of this case.
Finally, the equality L(β )β£NΞ»ββ=DΞ»β(β )+HΞ»β(β ) entails that DΞ»β(β )=L(β )β£NΞ»βββHΞ»β(β ):AlgNβB(NΞ»β,X). If L is continuous, then Φλ,f,yβ is continuous and hence DΞ»β is bounded. By the relation L(β )β£NΞ»ββ=DΞ»β(β )+HΞ»β(β ), we get the continuity of HΞ»β.
β
Theorem 3.22**.**
Let X be a Banach space with dimXββ₯β=0 and N be a non-trivial nest on X. Then each Lie-type derivation on AlgN is of standard form. More precisely, for any Lie n-derivation L:AlgNβB(X), there exists a derivation D:AlgNβB(X) and a linear mapping H:AlgNβCI vanishing on all (nβ1)-commutators on AlgN such that L=D+H. In particular, if L is continuous, then D and H are continuous as well.
Proof.
As we mention at the beginning of this subsection, it suffices to consider the case of dimX>2, Xββ=X and {0}={0}+β. For arbitrary Ξ±,Ξ²βΞ, suppose that NΞ±ββNΞ²β. For any xβNΞ±β, fixing fβNΞ²β₯ββ{0} and yβI(f), then by relation (3.26) we know that the equality
[TABLE]
holds true for any f1ββNΞ±β₯β, f2ββNΞ²β₯β and yjββI(fjβ). Note that I has infinitely rank, and thus hΞ²β(x,f)βhΞ±β(x,f)=0. Considering the action of (3.33) on y, we obtain Φα,f1β,y1βββΦβ,f2β,y2βββ£NΞ±βββCIβ£NΞ±ββ. By Lemma 3.20 we conclude that
[TABLE]
And hence HΞ±β(A)=HΞ²β(A)β£NΞ±ββ. For each Ξ»βΞ, let us denote HΞ»β(A)Iβ£NΞ»ββ=HΞ»β(A). By Lemma 3.20 it follows that HΞ»β:AlgNβCI is a (continuous, if L is continuous) linear functional, and HΞ±β(A)=HΞ²β(A). Define H(A):=HΞ»β(A)I for some Ξ»βΞ and write D:=LβH. Thus H:AlgNβCI is a (bounded, if L is continuous) linear operator. For any A,BβAlgN and xββΞ»βΞβNΞ»β, there is a Ξ»βΞ such that xβNΞ»β. By Lemma 3.20 it follows that
[TABLE]
Taking into account the fact X=spanβΞ»βΞβNΞ»ββ=βΞ»βΞβNΞ»ββ (Since N is totally ordered, βΞ»βΞβNΞ»β is a linear space), we know that D:AlgNβB(X) is a (continuous, if L is continuous) derivation. By invoking Proposition 2.4 we see that H vanishes on all (nβ1)-th commutators on AlgN.
β
Remark 3.23**.**
We would like to point out that the main results in [13, 24, 27] are direct consequences of our main Theorem 3.1.
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