The Centroid of a Lie Triple Algebra
Abstract
General results on the centroids of Lie triple algebras are developed. Centroids of the tensor product of a Lie triple algebra and a unitary commutative associative algebra are studied. Furthermore, the centroid of the tensor product of a simple Lie triple algebra and a polynomial ring is completely determined.
1. Introduction
In recent years, Lie triple algebras (i.e., Lie-Yamaguti algebras or general Lie triple systems) have attracted much attention in Lie theories. They contain Lie algebras and Lie triple systems as special cases ([1–6]). So, it is of vital importnce to study some properties of Lie triple algebras. The concept of Lie triple algebra has been introduced, originally, by Yamaguti as general Lie triple system by himself, Sagle, and others. Since Lie triple algebras are generalization of Lie algebras and Lie triple system, it is natural for us to imagine whether or not some results of Lie algebras and Lie triple system hold in Lie triple algebras. Now, as a generalization of Lie triple algebra, Hom-Lie-Yamaguti was introduced by Lister in [7].
Benkart and Neher studied centroid of Lie algebras in [8], and Melville investigated centroid of nilpotent Lie algebras in [9]. It turns out that result on the centroid of Lie algebras is a key ingredient in the classification of extended affine Lie algebras. The centroids of Lie triple systems were mentioned by Benito et al. [10]. Now, some results on centroids of Lie triple system and n-Lie algebras were developed in [11, 12].
In this paper we present new results concerning the centroids of Lie triple algebras and give some conclusion of the tensor product of a Lie triple algebra and a unitary commutative associative algebra. Furthermore, we completely determine the centroid of the tensor product of a simple Lie triple algebra and a polynomial ring. The organization of the rest of this paper is as follows. Section 1 is for basic notions and facts on Lie triple algebras. Section 2 is devoted to the structures and properties of the centroids of Lie triple algebras. Section 3 describes the structures of the centroids of tensor product of Lie triple algebras.
2. Preliminaries
Definition 1 (see [1].)A Lie triple algebra (also called a Lie-Yamaguti algebra or a general Lie triple system) 𝔤 is a vector space over an arbitrary field F with a bilinear map denoted by xy of 𝔤 × 𝔤 into 𝔤 and a ternary map denoted by [x, y, z] of 𝔤 × 𝔤 × 𝔤 into 𝔤 satisfying the following axioms:
- (a)
xx = 0,
- (b)
[x, x, y] = 0,
- (c)
(xy)z + (yz)x + (zx)y + [x, y, z]+[y, z, x]+[z, x, y] = 0,
- (d)
[xy, z, w]+[yz, x, w]+[zx, y, w] = 0,
- (e)
[x, y, zw] = ([x, y, z])w + z([x, y, w]),
- (f)
([x, y, v])([z, w, v]) = [[x, y, z], w, v]+[z[x, y, w], v],
Remark 2. Any Lie algebra is a Lie triple algebra relative to xy = [x, y] and D(x, y)z = [[x, y], z], for x, y, z ∈ 𝔤. If D(x, y)z = 0, for all x, y, z ∈ 𝔤, the axioms stated earlier reduce to that of Lie algebra, and if xy = 0, for all x, y ∈ 𝔤, the axioms stated earlier reduce to that of Lie triple system. In this sense, the Lie triple algebra is a more general concept than that of the Lie algebra and Lie triple system.
Definition 3 (see [1], [2].)A derivation of a Lie triple algebra 𝔤 is a linear transformation D of 𝔤 into 𝔤 satisfying the following conditions:
- (1)
D(xy) = (Dx)y + x(Dy),
- (2)
D([x, y, z]) = [Dx, y, z]+[x, Dy, z]+[x, y, Dz], for all x, y, z ∈ 𝔤.
Let Der(𝔤) be the set of all derivation of 𝔤; then Der(𝔤) is regarded as a subalgebra of the general Lie algebra gl(𝔤) and is called the derivation algebra of 𝔤.
Definition 4. A Lie triple subalgebra I of 𝔤 is called an ideal if 𝔤I⊆I and [𝔤, I, 𝔤]⊆I.
Definition 5. A Lie triple algebra 𝔤 is perfect if 𝔤 = 𝔤𝔤 = [𝔤, 𝔤, 𝔤].
Definition 6. Let I be a nonempty subset of 𝔤; we call Z𝔤(I) = {x ∈ 𝔤∣xa = [x, a, y] = 0, for all a ∈ I, y ∈ 𝔤} the centralizer of I in 𝔤. In particular, Z(𝔤) = {x ∈ 𝔤∣x𝔤 = [x, 𝔤, 𝔤] = 0} is the center of 𝔤.
Definition 7. Suppose that I is an ideal of the Lie triple algebra 𝔤, on the quotient vector space
3. The Centroids of Lie Triple Algebras
Definition 8. Let 𝔤 be a Lie triple algebra over a field F. The centroid of 𝔤 is the transform on 𝔤 given by Γ(𝔤) = {ψ ∈ EndF(𝔤)∣ψ([x, y, z]) = [ψ(x), y, z], ψ(xy) = (ψ(x))y, for all x, y, z, ∈𝔤}.
By (a)–(f), we can conclude that if ψ ∈ Γ(𝔤), then we have ψ([x, y, z]) = [ψ(x), y, z] = [x, ψ(y), z] = [x, y, ψ(z)], ψ(xy) = (ψ(x))y = x(ψ(y)), for all x, y, z, ∈𝔤.
From the definition, it is clear that the scalars will always be in the centroid.
Proposition 9. If 𝔤 is perfect, then the centroid Γ(𝔤) is commutative.
Proof. For all x, y, z ∈ 𝔤, ϕ, ψ ∈ Γ(𝔤), we have ϕψ([x, y, z]) = [ψ(x), ϕ(y), z] = ψϕ([x, y, z]), ϕψ(xy) = ψ(x)ϕ(y) = ψϕ(xy).
Proposition 10. Let 𝔤 be a Lie triple algebra over a field F and B a subset of 𝔤. Then;
- (1)
Z𝔤(B) is invariant under Γ(𝔤),
- (2)
every perfect ideal of 𝔤 is invariant under Γ(𝔤).
Proof. (1) For any ψ ∈ Γ(𝔤), x ∈ Z𝔤(B), y ∈ B, z ∈ 𝔤, we have [ψ(x), y, z] = [ψ(x), y, z] = ψ[x, y, z] = 0, (ψ(x))z = ψ(xz) = 0, and [z, y, ψ(x)] = ψ[z, y, x] = 0, z(ψ(x)) = ψ(zx) = 0. Therefore, ψ(x) ∈ Γ(𝔤), which implies that Z𝔤(B) is invariant under Γ(𝔤).
(2) Let J be any perfect ideal of 𝔤; then J = JJ = [J, J, J]. For any y ∈ J, there exist a, b, c, d, e ∈ J, such that y = ab = [c, d, e], and then we have ψ(y) = ψ(ab) = (ψ(a))b ∈ J𝔤⊆J, ψ(y) = ψ([c, d, e]) = [c, ψ(d), e]∈[J, 𝔤, 𝔤]⊆J. Hence J is invariant under Γ(𝔤).
Definition 11. Let φ(𝔤)⊆Z(𝔤) and φ(𝔤𝔤) = φ([𝔤, 𝔤, 𝔤]) = 0; then φ is called a central derivation.
The set of all central derivation of 𝔤 is denoted by C(𝔤). Clearly, C(𝔤)⊆Γ(𝔤) and C(𝔤) is an ideal of Γ(𝔤). A more precise relationship is summarized as follows.
Next, we will develop some general results on centroids of Lie triple algebra.
Proposition 12. If 𝔤 has no nonzero ideals I and J with [𝔤, I, J] = 0, IJ = 0, then Γ(𝔤) is an integral domain.
Proof. Clearly, id ∈ Γ(𝔤). If there exist ψ, φ ∈ Γ(𝔤), ψ ≠ 0, ϕ ≠ 0 such that ψφ = 0, then there exist x, y ∈ 𝔤 such that ψ(x) ≠ 0 and ϕ(y) ≠ 0. Then, [𝔤, ψ(x), ϕ(y)] = ψϕ([𝔤, x, y]) = 0, (ψ(x))(ϕ(y)) = ψϕ(xy) = 0. Therefore, ψ(x) and ϕ(y) can span two nonzero ideals I, J of 𝔤 such that [𝔤, I, J] = IJ = 0, which is a contradiction. Hence, Γ(𝔤) has no zero divisor; it is an integral domain.
Theorem 13. If 𝔤 is a simple Lie triple algebra over an algebraically closed field F, then Γ(𝔤) = F id .
Proof. Let ϕ ∈ Γ(𝔤)⊆EndF(𝔤). Since F is algebraically closed, ϕ has an eigenvalue λ. We denote the corresponding eigenspace to be Eλ(ϕ) = {v ∈ 𝔤∣ϕ(v) = λ(v)}, so Eλ(ϕ) ≠ 0, for any v ∈ Eλ(ϕ), x, y ∈ 𝔤, and we have ϕ([v, x, y]) = [ϕ(v), x, y] = λ[v, x, y], ϕ((vx)) = ϕ(v)x = (λv)x = λ(vx), so [v, x, y] ∈ Eλ(ϕ), vx ∈ Eλ(ϕ). It follows that Eλ(ϕ) is an ideal of 𝔤. But, 𝔤 is simple, so Eλ(ϕ) = 𝔤; that is, Eλ(ϕ) = λid𝔤. This proves the theorem.
When Γ(𝔤) = Fid, the Lie triple algebra 𝔤 is said to be central. Furthermore, if 𝔤 is simple, 𝔤 is said to be central simple. Every simple Lie triple algebra is central simple over its centroid.
Proposition 14. Let 𝔤 be a Lie triple algebra over a field F; then
- (1)
𝔤 is indecomposable if and only if Γ(𝔤) does not contain idempotents except 0 and id ;
- (2)
if 𝔤 is perfect, then every ϕ ∈ Γ(𝔤) is symmetric (f([a, b, c], d) = f(a[d, c, b]), f(ab, c) = f(a, bc)) with respect to any invariant form on 𝔤.
Proof. (1) If there exists ϕ ∈ Γ(𝔤) which is an idempotent and satisfies ϕ ≠ 0, id, then ϕ2(x) = ϕ(x), for all x ∈ 𝔤. We assert that Ker ϕ and Im ϕ are ideals of 𝔤. In fact, for any x ∈ Ker ϕ and y, z ∈ 𝔤, we have ϕ([x, y, z]) = [ϕ(x), y, z] = 0, ϕ(xy) = (ϕ(x))y = 0y = 0, which implies [x, y, z] ∈ Ker ϕ, xy ∈ Ker ϕ. For any x ∈ Im ϕ, there exists a ∈ 𝔤 such that x = ϕ(a). Then, we have
On the other hand, suppose 𝔤 has a decomposition 𝔤 = 𝔤1 ⊕ 𝔤2. Then for any x ∈ 𝔤, we have x = x1 + x2, xi ∈ 𝔤i, i = 1,2. We choose ϕ ∈ Γ(𝔤) such that ϕ(x1) = x1 and ϕ(x2) = 0. Then, ϕ2(x) = ϕ(x1) = x1 = ϕ(x). Hence, ϕ is an idempotent. By assumption, we have ϕ = 0 or ϕ = id. If ϕ = 0, then x1 = 0, implying 𝔤 = 𝔤2. If ϕ = id, then x2 = 0, implying 𝔤 = 𝔤1.
(2) Let f be an invariant F-bilinear form on 𝔤. Then f([a, b, c], d) = f(a[d, c, b]), f(ab, c) = f(a, bc), for all a, b, c, d ∈ 𝔤. Since 𝔤 is perfect, for ϕ ∈ Γ(𝔤), we have
The result follows.
Remark 15. Set L(x)(y) = xy, L(x, y)(z) = [x, y, z], R(x)(y) = yx, R(x, y)(z) = [z, x, y], for all x, y, z, ∈𝔤; then we call L(x), and L(x, y) the left multiplication operator of 𝔤; R(x) and R(x, x) right multiplication operator of 𝔤. Denote by Mult(𝔤) = MultF(𝔤) the subalgebra of EndF(𝔤) generated by the left and right multiplication operators of 𝔤. Then, Γ(𝔤) is the centralizer of Mult(𝔤).
Theorem 16. Let π : 𝔤1 → 𝔤2 be an epimorphism of Lie triple algebra; for any f ∈ End F(𝔤1; Ker π): = {g ∈ End F(𝔤2)∣g(Ker π)⊆Ker π}, there exists a unique satisfying . Moreover, the following results hold.
- (1)
The map π End : End F(𝔤1; Ker π) → End F(𝔤2), is a homomorphism with the following properties:
-
π End ( Mult (𝔤1)) = Mult (𝔤2), π End (Γ(𝔤1)∩ End F(𝔤1; Ker π))⊆Γ(𝔤2). There is a homomorphism .
If Ker π = Z(𝔤1), then every ϕ ∈ Γ(𝔤1) leaves Ker π invariant; that is, πΓ is defined on all of Γ(𝔤1).
- (2)
Suppose 𝔤1 is perfect and Ker π⊆Z(𝔤1); then is injective.
- (3)
If 𝔤1 is perfect, Z(𝔤2) = 0, and Ker π⊆Z(𝔤1), then πΓ : Γ(𝔤1) → Γ(𝔤2) is a monomorphism.
Proof. (1) It is easy to see that πEnd is a homomorphism. Since Ker π is an ideal of 𝔤1 and all left and right multiplication operators of 𝔤1 leave Ker π invariant, Mult(𝔤1)⊆EndF(𝔤1; Ker π). Furthermore, for the left multiplication operator L(x, y), L(x) on 𝔤1, we have π∘L(x, y) = L(π(x), π(y))∘π, π∘L(x) = L(π(x))∘π, so πEnd(L(x, y)) = L(π(x), π(y)), πEnd(L(x)) = L(π(x)). For the right multiplication, we have the analogous formula πEnd(R(x, y)) = R(π(x), π(y)), πEnd(R(x)) = R(π(x)). Moreover, π is an epimorphism, so πEnd(Mult(𝔤1)) = Mult(𝔤2). Now, we show that πEnd(Γ(𝔤1)∩EndF(𝔤1; Ker π))⊆Γ(𝔤2). Let ϕ ∈ Γ(𝔤1)∩EndF(𝔤1; Ker π). For any x′, y′, z′ ∈ 𝔤2, there exist x, y, z ∈ 𝔤1 such that π(x) = x′, π(y) = y′, π(z) = z′. Then, we have
(2) If for, ϕ ∈ Γ(𝔤1)∩EndF(𝔤1; Ker π), then , which means that ϕ(𝔤1)⊆Ker π⊆Z(𝔤1). Hence, ϕ([x, y, z]) = [ϕ(x), y, z] = 0, ϕ(xy) = (ϕ(x)y) = 0, for all x, y, z ∈ 𝔤1. Furthermore, since 𝔤1 is a perfect ideal, we can get ϕ = 0.
(3) We can see that π(Z(𝔤1))⊆Z(𝔤2) = 0, which follows that Z(𝔤1)⊆Ker π. So, Ker π⊆Z(𝔤1). From (1), we know that πΓ : Γ(𝔤1) → Γ(𝔤2) is a well-defined homomorphism, which is an injection by (2).
Proposition 17. If the characteristic of F is not 2, then
Proof. If ψ ∈ Γ(𝔤)∩Der(𝔤), then by the definition of Γ(𝔤) and Der(𝔤), for all x, y, z ∈ 𝔤, we have ψ(xy) = (ψ(x))y + x(ψ(y)), ψ([x, y, z]) = [ψ(x), y, z]+[x, ψ(y), z]+[x, y, ψ(z)], and ψ(xy) = (ψ(x))y = x(ψ(y)), ψ([x, y, z]) = [ψ(x), y, z] = [x, ψ(y), z] = [x, y, ψ(z)], so ψ(𝔤𝔤) = ψ([𝔤, 𝔤, 𝔤]) = 0 and ψ(𝔤)⊆C(𝔤). It follows easily that Γ(𝔤)∩Der(𝔤)⊆C(𝔤).
To show the inverse inclusion, let ψ ∈ C(𝔤); then 0 = ψ([x, y, z]) = [ψ(x), y, z] = [x, ψ(y), z] = [x, y, ψ(z)], 0 = ψ(xy) = (ψ(x))y = x(ψ(y)). Thus, ψ ∈ Γ(𝔤)∩Der(𝔤).
This implies that C(𝔤) = Γ(𝔤)∩Der(𝔤).
Lemma 18. Let I be a nonzero Γ(𝔤)-invariant ideal of 𝔤, V(I) = {ψ ∈ Γ(𝔤)ψ(I) = 0}, and let Hom(𝔤/I, Z𝔤(I)) be the vector space of all linear maps from 𝔤/I to Z𝔤(I) over F. Define , where . Then one has the following.
- (1)
T(I) is a subspace of Hom(𝔤/I, Z𝔤(I)) and V(I)≅T(I) as vector spaces.
- (2)
If Γ(I) = F id I, then Γ(𝔤) = F id 𝔤 ⊕ V(I) as vector spaces.
Proof. (1) It is easily seen that V(I) is an ideal of the associative algebra Γ(𝔤). To prove (1) consider the following map α : V(I) → T(I) given by
We now prove (2). If Γ(I) = F id I, then for all ψ ∈ Γ(𝔤), ψ∣I = λidI, for some λ ∈ F. If ψ ≠ λid𝔤, let φ(x) = λx, for all x ∈ 𝔤; then ψ ∈ Γ(𝔤) and ψ − φ ∈ V(I). Clearly, ψ = φ + (ψ − φ). Furthermore, Fid𝔤∩V(I) = 0, and so (2) is proved.
Lemma 19. Let 𝔤 be a Lie triple algebra; then φD is a derivation for φ ∈ Γ(𝔤), D ∈ Der(𝔤).
Proof. If x, y, z ∈ 𝔤, then
Theorem 20. Let 𝔤 be a Lie triple algebra, and for any φ ∈ Γ(𝔤), D ∈ Der(𝔤), then one has the following.
- (1)
Der(𝔤) is contained in the normalizer of Γ(𝔤) in End (𝔤).
- (2)
Dφ is contained in Γ(𝔤) if and only if φD is a central derivation of 𝔤.
- (3)
φD is a derivation of 𝔤 if and only if [D, φ] is a central derivation of 𝔤.
Proof. For any φ ∈ Γ(𝔤), D ∈ Der(𝔤), and x, y, z ∈ 𝔤,
Then, we get (Dφ − φD)(xy) = ((Dφ − φD)(x))y. On the other hand, we have
Now, we study the relationship between the centroid of a decomposable Lie triple algebra and the centroid of its factors.
Theorem 21. Suppose that 𝔤 is a Lie triple algebra over F and 𝔤 = 𝔤1 ⊕ 𝔤2 with 𝔤1 and 𝔤2 being ideals of 𝔤; then
Proof. Let πi : 𝔤 → 𝔤i be canonical projections for i = 1,2; then π1, π2 ∈ Γ(𝔤) and π1 + π2 = id𝔤. So we have for φ ∈ Γ(𝔤),
Next, we prove that Γ(𝔤) 12≅C2. If φ ∈ Γ(𝔤) 12 there exists φ0 in Γ(𝔤) such that φ = π1φ0π2. For , where and k = 1,2, 3, we have
Conversely, for φ ∈ C2, expending φ on 𝔤 (also denoted by φ) or by φ(𝔤1𝔤1) = φ[𝔤1, 𝔤1, 𝔤1] = 0, we have π1φπ2 = φ and φ ∈ Γ(𝔤) 12. This proves that Γ(𝔤) 12 is isomorphic to C2 with the following isomorphism:
The proof is completed.
A generalized version of Theorem 21 is stated next without proof.
Theorem 22. Suppose that 𝔤 is a Lie triple algebra over F and with a decomposition of ideals 𝔤 = 𝔤1 ⊕ 𝔤2 ⊕ ⋯⊕𝔤m. Then, one has
4. The Centroids of Tensor Product of Lie Triple Algebras
Definition 23. Let A be an associative algebra over a field F, where the centroid of A is the space of F-linear transforms on A given by Γ(A) = {φ ∈ EndF(A)φ(ab) = aφ(b) = φ(a)b, for all a, b ∈ A}; then Γ(A) is an associative algebra of EndF(A). If 𝔤 is be a finite-dimensional Lie triple algebra over F, let 𝔤 ⊗ A be a tensor product of the underlying vector spaces A and 𝔤. Then, 𝔤 ⊗ A over a field F with respect to the following 2-ary and 3-ary multilinear operation:
Definition 24. The transformation ϕ ∈ Γ(𝔤 ⊗ A) is said to have finite 𝔤-image, if for any a ∈ A, there exist finitely many a1, …, an ∈ A such that
Lemma 25. Let 𝔤 be a Lie triple algebra over F and A a unitary commutative associative over F. Let {ar} r∈ℜ be a basis of A, and let ϕ ∈ Γ(𝔤 ⊗ A). Define ϕr ∈ End F(𝔤) by
Proof. For x1, x2, x3 ∈ 𝔤, we have
Proposition 26. Let 𝔤 be a perfect Lie triple algebra over F, and let A be a unitary commutative associative over F which is free as a F-module. Then, one has the following.
- (1)
If 𝔤 is perfect, then 𝔤 ⊗ A is perfect too.
- (2)
If 𝔤 is finitely generated as a Mult (𝔤)-module (or as a Γ(𝔤)-module), or if 𝔤 is a central and a torsion-free F-module, then every ϕ ∈ Γ(𝔤 ⊗ A) has finite 𝔤-image.
- (3)
If Γ(𝔤) is a free F-module and the map ω of Definition 23 is injective, then has finite 𝔤-image}.
Proof. The definition of perfect shows that (1) holds. Let M = Mult(𝔤). It follows that from A is unital. Since 𝔤 is finitely generated as a Mult(𝔤)-module, we can suppose 𝔤 = Mx1 + ⋯+Mxn for x1, …, xn ∈ 𝔤. Fix ϕ ∈ Γ(𝔤 ⊗ A) and a ∈ A. There exist finite families {xij}⊆𝔤 and {aij}⊆A such that
Now, suppose that Γ(𝔤) = Fid and that 𝔤 is a torsion-free F-module. Then there exist scalars kr ∈ F such that ϕr = krid. Hence,
From the aforementione discussion above, we get
Next, we will determine the centroid of the tensor product of a simple Lie triple algebra and a polynomial ring. Here after we study the centroid of Lie triple algebra over a filed F. Let {ek} be a basis of the central derivation C(𝔤) and {φj} a maximal subset of Γ(𝔤) such that {φj∣𝔤𝔤} and {φj∣[𝔤,𝔤,𝔤]} are linear independent. Then, we have the following result.
Theorem 27. Let Ψ denote the subspace of Γ(𝔤) spanned by {φj}. Then {ek, φj} is a basis of Γ(𝔤) and Γ(𝔤) = Ψ ⊕ C(𝔤) as vector spaces.
Proof. Since {φj∣𝔤𝔤} and {φj∣[𝔤,𝔤,𝔤]} are linear independent, {φj} is linear independent in Γ(𝔤). By definition of {ek, φj}, the {ek, φj} is independent in Γ(𝔤). For φ ∈ Γ(𝔤) since {φj∣𝔤𝔤} is a basis of vector spaces {φ∣𝔤𝔤∣φ ∈ Γ(𝔤)}, and {φj∣[𝔤,𝔤,𝔤]} is a basis of vector spaces {φ∣[𝔤,𝔤,𝔤]∣φ ∈ Γ(𝔤)}, there exist gs ∈ F, s ∈ J (J is a finite set of positive integers) such that
Lemma 28. Let 𝔤 be a simple Lie triple algebra, R = F[x1, …, xn], and ; then one has .
Proof. Let ψ ∈ Γ(𝔤), m ∈ R. Then, we have
Theorem 29. Let 𝔤 be a simple Lie triple algebra, R = F[x1, …, xn], and . Then .
Proof. From Lemma 28, we get . Now we prove the opposite inclusion. Let {mi} be a basis for , and let ηi(−, p) be suitable maps in EndF(𝔤) such that
Thus, we may write
Acknowledgments
The authors would like to thank the referee for valuable comments and suggestions on this paper. The works was supported by NNSF of China (no. 11171057), Natural Science Foundation of Jilin province (no. 201115006), the Fundamental Research Funds for the Central Universities (no. 12SSXT139), and Scientific Research Foundation for Returned Scholars, Ministry of Education of China.