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On split Lie color triple systems

  • Yan Cao EMAIL logo , Jian Zhang and Yunan Cui
Published/Copyright: April 9, 2019

Abstract

In order to begin an approach to the structure of arbitrary Lie color triple systems, (with no restrictions neither on the dimension nor on the base field), we introduce the class of split Lie color triple systems as the natural generalization of split Lie triple systems. By developing techniques of connections of roots for this kind of triple systems, we show that any of such Lie color triple systems T with a symmetric root system is of the form T = U + ∑[α]∈Λ1/∼ I[α] with U a subspace of T0 and any I[α] a well described (graded) ideal of T, satisfying {I[α], T, I[β]} = 0 if [α] ≠ [β]. Under certain conditions, in the case of T being of maximal length, the simplicity of the triple system is characterized.

MSC 2010: 17A32; 17A60; 17B22; 17B65

1 Introduction

The concept of Lie triple systems was introduced by Nathan Jacobson in 1949 to study subspaces of associative algebras closed under triple commutators [[u, v], w]. The role played by Lie triple systems in the theory of symmetric spaces is parallel to that of Lie algebras in the theory of Lie groups: the tangent space at every point of a symmetric space has the structure of a Lie triple system. Because of close relation to Lie algebras and theoretical physics, Lie triple systems have recently been widely studied [1, 2, 3, 4]. The notion of Lie color algebras was introduced as generalized Lie algebras in 1960 by Ree [5]. So far, many results of this kind of algebras have been considered in the frameworks of enveloping algebras, representations and related problems [6, 7, 8]. Lie color triple systems were introduced as generalized Lie triple systems by Zhang in his doctoral thesis in 2007. Furthermore, Lie color triple systems are related to Lie color algebras in the same way that Lie triple systems related to Lie algebras. So it is natural to prove analogs of results from the theory of Lie triple systems to Lie color triple systems.

In the framework of infinite dimensional Lie algebras, Neeb, Stumme and other authors have successfully developed over the recent years a theory of split and locally finite Lie algebras [9, 10]. Calderón introduced the concept of split Lie triple systems of arbitrary dimension [11, 12, 13]. In [14], Calderón introduced techniques of connections of roots in the field of split Lie color algebras. Recently, the structure of different classes of split algebras have been studied by using techniques of connections of roots (see for instance [15, 16, 17, 18]). Our work is based on [13, 14] and our aim is to consider the structure of split Lie color triple systems by the techniques of connections of roots.

Throughout this paper, Lie color triple systems T are considered of arbitrary dimension and over an arbitrary base field 𝕂. This paper proceeds as follows. In section 2, we establish the preliminaries on split Lie color triple systems theory. In section 3, we show that such an arbitrary split Lie color triple system with a symmetric root system is of the form T = U + ∑[α]∈Λ1/∼ I[α] with U a subspace of T0 and any I[α] a well described (graded) ideal of T, satisfying {I[α], T, I[β]} = 0 if [α] ≠ [β]. In section 4, we show that under certain conditions, in the case of T being of maximal length, the simplicity of the triple system is characterized.

2 Preliminaries

First we recall the definitions of Lie color algebras and Lie triple systems.

Definition 2.1

[14] Let Γ be an abelian group. A bi-character on Γ is a map ε : Γ × Γ → 𝕂 ∖ {0} satisfying

  1. ε(α, β)ε(β, α) = 1,

  2. ε(α, β + γ) = ε(α, β)ε(α, γ),

  3. ε(α + β, γ) = ε(α, γ)ε(β, γ)

for all α, β, γΓ.

It is clear that ε(α, 0) = ε(0, α) = 1 for any αΓ, where 0 denotes the identity element of Γ.

Definition 2.2

[14] Let L = ⊕gΓLg be a Γ-graded 𝕂-vector space. For a nonzero homogeneous element vL, denote by the unique group element in Γ such that vL, which will be called the homogeneous degree of v. We shall say that L is a Lie color algebra if it is endowed with a 𝕂-bilinear map [⋅, ⋅] : L × LL satisfying

  1. [v, w] = −ε(, )[w, v], (Skew- symmetry)

  2. [v, [w, t]] = [[v, w], t] + ε(, )[w, [v, t]] (Jacobi identity)

for all homogeneous elements v, w, tL.

Lie superalgebras are examples of Lie color algebras with Γ = ℤ2 and ε(i, j) = (−1)ij, for any i, j ∈ ℤ2. We also note that L0 is a Lie algebra.

Definition 2.3

[13] A Lie triple system is a vector space T endowed with a trilinear map {⋅, ⋅, ⋅} : T × T × TT satisfying

  1. {x, y, z} = −{y, x, z},

  2. {x, y, z} + {y, z, x} + {z, x, y} = 0,

  3. {x, y, {a, b, c}} = {{x, y, a}, b, c} + {a, {x, y, b}, c} + {a, b, {x, y, c}}

    for x, y, z, a, b, cT.

Definition 2.4

Let T = ⊕gΓTg be a Γ-graded 𝕂-vector space. For a nonzero homogeneous element vT, denote by the unique group element in Γ such that vT, which will be called the homogeneous degree of v. We shall say that T is a Lie color triple system if it is endowed with a 𝕂-trilinear map

  1. {x, y, z} = −ε(, ȳ){y, x, z},

  2. ε(, ){x, y, z} + ε(, ȳ){y, z, x} + ε(ȳ, ){z, x, y} = 0,,

  3. {x, y, {a, b, c}} = {{x, y, a}, b, c} + ε( + ȳ, ā){a, {x, y, b}, c}

+ε( + ȳ, ā + ){a, b, {x, y, c}}

for all homogeneous elements x, y, z, a, b, cT.

Example 2.5

Lie triple systems are examples of Lie color triple systems with Γ = {0} and ε(0,0) = 1.

Example 2.6

Lie triple supersystems are examples of Lie color triple systems with Γ = {ℤ2} = {0, 1} and ε(, β̄) = (−1)β̄, for any , β̄ ∈ ℤ2.

Example 2.7

If L is a Lie color algebra with product [⋅, ⋅], then L becomes a Lie color triple system by putting {x, y, z} = [[x, y], z].

Definition 2.8

Let I = ⊕gΓIg be a graded subspace of a Lie color triple system T. Then I is called a subsystem of T, if {I, I, I} ⊆ I; I is called an ideal of T, if {I, T, T} ⊆ I.

Definition 2.9

The standard embedding of a Lie color triple system T is the2-graded Lie color algebra L = L0L1, L0 being the 𝕂-span of {L(x, y) : x, yT}, where L(x, y) denotes the left multiplication operator in T, L(x, y)(z) := {x, y, z}; L1 := T and where the product is given by

[(L(x,y),z),(L(u,v),w)]:=(L({x,y,u},v)+ε(x¯+y¯,u¯)L(u,{x,y,v})+L(z,w),{x,y,w}ε(z¯,u¯+v¯){u,v,z}).

Let us observe that L0 with the product induced by the one in L = L0L1 becomes a Lie color algebra.

Let us recall the concept of split Lie color algebra. Denote by H = ⊕gΓHg a maximal abelian (graded) subalgebra, (MAGSA), of a Lie color algebra L. For a linear functional

α:H0K,

we define the root space of L (with respect to H) associated to α as the subspace

Lα={vαL:[h0,vα]=α(h0)vαforanyh0H0}.

The elements α : H0 → 𝕂 satisfying Lα ≠ 0 are called roots of L with respect to H. We denote Λ := {α H0 ∖ {0} : Lα ≠ 0}. We say that L is a split Lie color algebra, with respect to H, if L = H ⊕ (⊕αΛLα). We also say that Λ is the root system of L.

Definition 2.10

Let T be a Lie color triple system, L = L0L1 be its standard embedding, and H0 = ⊕gΓ Hg0 be a maximal abelian (graded) subalgebra (MAGSA) of L0. For a linear functional α (H00) , we define the root space of T (with respect to H0) associated to α as the subspace Tα := {tαT : [h, tα] = α(h)tα for any h H00 }. The elements α (H00) satisfying Tα ≠ 0 are called roots of T with respect to H0 and we denote Λ1 := {α (H00) ∖ {0} : Tα ≠ 0}.

Let us observe that T0 := {t0T : [h, t0] = 0 for any h H00 }. In the following, we shall denote by Λ0 the set of all nonzero α (H00) such that Lα0:={vα0L0:[h,vα0]=α(h)vα0 for any h H00 } ≠ 0.

Lemma 2.11

Let T be a Lie color triple system, L = L0L1 be its standard embedding, and H0 be a MAGSA of L0. For α, β, γΛ1 ∪ {0} and ξ, qΛ0 ∪ {0}, the following assertions hold.

  1. If [Tα, Tβ] ≠ 0, then α + βΛ0 ∪ {0} and [Tα, Tβ] ⊆ Lα+β0.

  2. If [Lξ0,Tα]0, then ξ + αΛ1 ∪ {0} and [Lξ0,Tα]Tξ+α.

  3. If [Lξ0,Lq0]0, then ξ + qΛ0 ∪ {0} and [Lξ0,Lq0]Lξ+q0.

  4. If {Tα, Tβ, Tγ} ≠ 0, then α + β + γΛ1 ∪ {0} and {Tα, Tβ,Tγ} ⊆ Tα+β+γ.

Proof

  1. For any xTα, yTβ and h H00 , by Definition 2.2 (2), one has [h, [x, y]] = ε(0, )[x, [h, y]] + [[h, x], y] = [x, β(h)y] + [α(h)x, y] = (α + β)(h)[x, y].

  2. For any x Lξ0 , yTα and h H00 , by Definition 2.2 (2), one has [h, [x, y]] = [x, [h, y]] + [[h, x], y] = ε(0, )[x, α(h)y] + [ξ(h)x, y] = (ξ + α)(h)[x, y].

  3. For any x Lξ0 , y Lq0 and h H00 , by Definition 2.2 (2), one has [h, [x, y]] = ε(0, )[x, [h, y]] + [[h, x], y] = [x, q(h)y] + [ξ(h)x, y] = (ξ + q)(h)[x, y].

  4. It is a consequence of Lemma 2.11 (1) and (2).□

Definition 2.12

Let T be a Lie color triple system, L = L0L1 be its standard embedding, and H0 = ⊕gΓ Hg0 be a MAGSA of L0. We shall call that T is a split Lie color triple system (with respect to H0) if T = T0 ⊕ (⊕αΛ1 Tα). We say that Λ1 is the root system of T.

We observe that it is straightforward to prove that if T is a split Lie color triple system with respect to H0 and we let L = L0L1 be its standard embedding algebra, then L0 is a split Lie color algebra with respect to the splitting Cartan subalgebra H0, with set of nonzero roots Λ0. We also note that the facts H0L0 = [T, T] and T = T0 ⊕ (⊕αΛ1 Tα) imply

H0=[T0,T0]+αΛ1[Tα,Tα]. (2.1)

Lemma 2.13

Let T = ⊕gΓTg be a split Lie color triple system with corresponding root space decomposition T = T0 ⊕ (⊕αΛ1 Tα). If we denote by Tα,g = TαTg, the following assertions hold.

  1. Tα = ⊕gΓ Tα,g for any αΛ1 ∪ {0}.

  2. Hg0=g1+g2=g,g1,g2Γ[T0,g1,T0,g2]+αΛ1g1+g2=g,g1,g2Γ[Tα,g1,Tα,g2].

  3. T0 is a split Lie triple system, with respect to H00 , with root space decomposition T0 = T0,0 ⊕ (⊕αΛ1Tα,0).

Proof

  1. By the Γ-grading of T we may express any vαTα, αΛ1 ∪ {0}, in the form vα = vα,g1 + ⋯ + vα,gn with vα,giTgi for distinct g1, ⋯ ,gnΓ. If h0 H00 then [h0, vα,gi] = α(h0)vα,gi for i = 1, ⋯, n. Hence Tα = ⊕gΓ(TαTg) and we can write Tα = ⊕gΓTα,g for any αΛ1 ∪ {0}.

  2. Consequence of Eq. (2.1) and Lemma 2.13 (1).

  3. By considering g = 0 we get T0 = T0,0 ⊕ (⊕αΛ1Tα,0). Hence, the direct character of the sum and the fact that α ≠ 0 for any αΛ1 give us that H00 is a maximal abelian subalgebra of the Lie algebra L00 . Hence T0 is a split Lie triple system respect to H00 .□

Definition 2.14

A root system Λ1 of a split Lie color triple system T is called symmetric if it satisfies that αΛ1 impliesαΛ1.

A similar concept applies to the set Λ0 of nonzero roots of L0.

In the following, T denotes a split Lie color triple system with a symmetric root system Λ1, and T = T0 ⊕ (⊕αΛ1 Tα) the corresponding root decomposition. We begin the study of split Lie color triple system by developing the concept of connections of roots.

Definition 2.15

Let α and β be two nonzero roots, we shall say that α and β are connected if there exists a family {α1, α2, ⋯, α2n, α2n+1} ⊂ Λ1 ∪ {0} of roots of T such that

  1. {α1, α1 + α2 + α3, α1 + α2 + α3 + α4 + α5, ⋯, α1 + ⋯ + α2n + α2n+1} ⊂ Λ1;

  2. {α1 + α2, α1 + α2 + α3 + α4, ⋯, α1 + ⋯ + α2n} ⊂ Λ0;

  3. α1 = α and α1 + ⋯ + α2n + α2n+1 ∈ ±β.

    We shall also say that {α1, α2, ⋯, α2n, α2n+1} is a connection from α to β.

    We denote by

    Λα1:={βΛ1:αandβareconnected},

    we can easily get that {α} is a connection from α to itself and to −α. Therefore ±α Λα1 .

Definition 2.16

A subset Ω1 of a root system Λ1, associated to a split Lie color triple system T, is called a root subsystem if it is symmetric, and for α, β, γΩ1 ∪ {0} such that α + βΛ0 and α + β + γΛ1 then α + β + γΩ1.

Let Ω1 be a root subsystem of Λ1. We define

T0,Ω1:=spanK{{Tα,Tβ,Tγ}:α+β+γ=0;α,β,γΩ1{0}}T0

and VΩ1 := ⊕αΩ1Tα. Taking into account the fact that {T0, T0, T0} = 0, it is straightforward to verify that TΩ1 := T0,Ω1VΩ1 is a subsystem of T. We will say that TΩ1 is a subsystem associated to the root subsystem Ω1.

Proposition 2.17

If Λ0 is symmetric, then the relationin Λ1, defined by αβ if and only if β Λα1 , is of equivalence.

Proof

{α} is a connection from α to itself and therefore αα.

If αβ and {α1, α2, ⋯, α2n, α2n+1} is a connection from α to β, then

{α1++α2n+1,α2n+1,α2n,,α2}

is a connection from β to α in the case α1 + ⋯ + α2n + α2n+1 = β, and

{α1α2n+1,α2n+1,α2n,,α2}

in the case α1 + ⋯ + α2n + α2n+1 = −β. Therefore βα.

Finally, suppose αβ and βγ, {α1, α2, ⋯, α2n, α2n+1} is a connection from α to β and {β1, ⋯, β2m+1} is a connection from β to γ. If m ≠ 0, then

{α1,,α2n+1,β2,,β2m+1}

is a connection from α to γ in the case α1 + ⋯ + α2n + α2n+1 = β, and

{α1,,α2n+1,β2,,β2m+1}

in the case α1 + ⋯ + α2n + α2n+1 = −β. If m = 0, then γ ∈ ± β and so

{α1,α2,,α2n,α2n+1}

is a connection from α to γ. Therefore αγ and ∼ is of equivalence.□

Proposition 2.18

Let α be a nonzero root and suppose Λ0 is symmetric. Then Λα1 is a root subsystem.

Proof

If β Λα1 then there exists a connection {α1, α2, ⋯, α2n, α2n+1} from α to β. It is clear that {α1, α2, ⋯, α2n, α2n+1} also connects α to −β and therefore −β Λα1 . Let β1, β2, β3 Λα1 ∪ {0} be such that β1 + β2Λ0 and β1 + β2 + β3Λ1. If β1 = 0, as β1 + β2Λ0 then β2 ≠ 0 and there exists a connection {α1, α2, ⋯, α2n, α2n+1} from α to β2. We have {α1, α2, ⋯, α2n+1, 0, β3} is a connection from α to β2 + β3 in case α1 + ⋯ + α2n + α2n+1 = β2 and {α1, α2, ⋯, α2n+1, 0, −β3} in case α1 + ⋯ + α2n + α2n+1 = −β2. So β1 + β2 + β3 = β2 + β3 Λα1 . Suppose β1 ≠ 0, then there exists a connection {α1, α2, ⋯, α2n, α2n+1} from α to β1. Hence, {α1, α2, ⋯, α2n+1,β2, β3} is a connection from α to β1 + β2 + β3 in case α1 + ⋯ + α2n + α2n+1 = β1 and {α1, α2, ⋯, α2n+1, −β2, −β3} in case α1 + ⋯ + α2n + α2n+1 = −β1. Therefore β1 + β2 + β3 Λα1 .□

3 Decompositions

In this section, we will state a series of previous results in order to show that for a fixed α0Λ1, the subsystem TΛα01 associated to the root subsystem Λα01 is an ideal of T.

Lemma 3.1

The following assertions hold.

  1. If α, βΛ1 with [Tα, Tβ] ≠ 0, then α is connected with β.

  2. If α, βΛ1, αΛ0 and [Lα0,Tβ]0, then α is connected with β.

  3. If α, βΛ1, α, βΛ0 and [Lα0,Lβ0]0, then α is connected with β.

  4. If α, βΛ1 such that α is not connected with β, then [Tα, Tβ] = 0, [Lα0,Tβ¯]=0 and [Tβ¯,Lα0]=0 if furthermore αΛ0. If α, βΛ1 such that α is not connected with β, then [Lα0,Lβ¯0]=0 if furthermore α, βΛ0.

Proof

  1. Suppose [Tα, Tβ] ≠ 0, by Lemma 2.11 (1), one gets α + βΛ0 ∪ {0}. If α + β = 0, then β = −α and so α is connected with β. Suppose α + β ≠ 0. Since α + βΛ0, one gets {α, β, −α} is a connection from α to β.

  2. Suppose [Lα0,Tβ]0, by Lemma 2.11 (2), one gets α + βΛ1 ∪ {0}. If α + β = 0, then β = −α and so α is connected with β. Suppose α + β ≠ 0. Since α + βΛ1, we obtain {α, 0, −αβ} is a connection from α to β.

  3. Suppose [Lα0,Lβ0]0, by Lemma 2.11 (3), one has α + βΛ0 ∪ {0}. If α + β = 0, then β = −α and so α is connected with β. Suppose α + β ≠ 0. Since α + βΛ0, one gets {α, β, −α} is a connection from α to β.

  4. It is a consequence of Lemma 3.1 (1), (2) and (3).□

Lemma 3.2

If α, βΛ1 are not connected, then {Tα, Tα, Tβ} = 0.

Proof

If [Tα, Tα] = 0, it is clear. One may suppose that [Tα, Tα] ≠ 0 and {Tα, Tα, Tβ} ≠ 0. By the definition of Lie color triple systems, one has {Tα, Tβ, Tα} ≠ 0 or {Tβ, Tα, Tα} ≠ 0, contradicting Lemma 3.1 (4). Hence, {Tα, Tα, Tβ} = 0.□

Lemma 3.3

Fix α0Λ1 and suppose Λ0 is symmetric. For α Λα01 and β, γΛ1 ∪ {0}, then the following assertions hold.

  1. If {Tα, Tβ, Tγ} ≠ 0, then β, γ, α + β + γ Λα01 ∪ {0}.

  2. If {Tγ, Tα, Tβ} ≠ 0, then γ, β, γ + α + β Λα01 ∪ {0}.

  3. If {Tβ, Tγ, Tα} ≠ 0, then β, γ, β + γ + α Λα01 ∪ {0}.

Proof

  1. It is easy to see that [Tα, Tβ] ≠ 0, for α Λα01 and βΛ1 ∪ {0}. By Lemma 3.1 (1), one gets αβ in the case β ≠ 0. From here, β Λα01 ∪ {0}. In order to complete the proof, we will show γ, α + β + γ Λα01 ∪ {0}. We distinguish two cases.

    1. Suppose α + β + γ = 0. It is clear that α + β + γ Λα01 ∪ {0}. The fact that {T0, T0, T0} = 0 and {Tα, Tα, T0} = 0 for αΛ1 gives us γ ≠ 0. By Lemma 2.11 (1), one gets α + βΛ0. As α + β = −γ, {α, β, 0} would be a connection from α to γ and we conclude γ Λα01 ∪ {0}.

    2. Suppose α + β + γ ≠ 0. We treat separately two cases.

      Suppose α + β ≠ 0. By Lemma 2.11 (1), one gets α + βΛ0 and so {α, β, γ} is a connection from α to α + β + γ. Hence α + β + γ Λα01 ∪ {0}. In the case γ ≠ 0, {α, β, −αβγ} is a connection from α to γ. So γ Λα01 . Hence γ Λα01 ∪ {0}.

      Suppose α + β = 0. Then necessarily γ Λα01 ∪ {0}. Indeed, if γ ≠ 0 and α is not connected with γ, by Lemma 3.2, {Tα, Tβ, Tγ} = {Tα, Tα, Tγ} = 0, a contradiction. We also have α + β + γ = γ Λα01 ∪ {0}.

  2. The fact that [Tγ, Tα] ≠ 0 implies by Lemma 3.1 (1) that αγ in the case γ ≠ 0. From here, γ Λα01 ∪ {0}. In order to complete the proof, we will show β, γ + α + β Λα01 ∪ {0}. We distinguish two cases.

    1. Suppose γ + α + β = 0. It is clear that γ + α + β Λα01 ∪ {0}. The fact that {T0, T0, T0} = 0 and {Tα, Tα, T0} = 0 for αΛ1 gives us β ≠ 0. By Lemma 2.11 (1), one has γ + αΛ0. As γ + α = −β, {α, γ, 0} would be a connection from α to β and we conclude β Λα01 ∪ {0}.

    2. Suppose γ + α + β ≠ 0. We treat separately two cases.

      Suppose γ + α ≠ 0. By Lemma 2.11 (1), one gets γ + αΛ0 and so {α, γ, β} is a connection from α to γ + α + β. Hence γ + α + β Λα01 ∪ {0}. In the case β ≠ 0, we have {α, γ, −αγβ} is a connection from α to β. So β Λα01 . Hence β Λα01 ∪ {0}.

      Suppose γ + α = 0. Then necessarily β Λα01 ∪ {0}. Indeed, if β ≠ 0 and α is not connected with β, by Lemma 3.2, {Tγ, Tα, Tβ} = {Tα, Tα, Tβ} = 0, a contradiction. We also have γ + α + β = β Λα01 ∪ {0}.

  3. By the definition of Lie color triple systems, one has

    ε(α¯,β¯){Tβ,Tγ,Tα}ε(γ¯,α¯){Tα,Tβ,Tγ}+ε(β¯,γ¯){Tγ,Tα,Tβ}.

    So either {Tα, Tβ, Tγ} ≠ 0 or {Tγ, Tα, Tβ} ≠ 0. By Lemma 3.3 (1) and (2), one gets β, γ Λα01 ∪ {0}. Next we will show that β + γ + α Λα01 ∪ {0}. We treat separately three cases.

    1. Suppose β ≠ 0, then β Λα01 . By Lemma 3.3 (1), one has β + γ + α Λα01 ∪ {0}.

    2. Suppose β = 0 and γ ≠ 0, then γ Λα01 . By Lemma 3.3 (2), one has β + γ + α Λα01 ∪ {0}.

    3. Suppose β = 0 and γ = 0, then β + γ + α = α Λα01 , we also have β + γ + α Λα01 ∪ {0}.

Lemma 3.4

Fix α0Λ1 and suppose Λ0 is symmetric. For α, β, γ Λα01 ∪ {0} with α + β + γ = 0 and τ, ϵΛ1 ∪ {0}, the following assertions hold.

  1. If {{Tα, Tβ, Tγ}, Tτ, Tϵ} ≠ 0, then τ, ϵ, τ + ϵ Λα01 ∪ {0}.

  2. If {Tϵ, {Tα, Tβ, Tγ}, Tτ} ≠ 0, then τ, ϵ, ϵ + τ Λα01 ∪ {0}.

  3. If {Tτ, Tϵ, {Tα, Tβ, Tγ}} ≠ 0, then τ, ϵ, τ + ϵ Λα01 ∪ {0}.

Proof

  1. From the fact that α + β + γ = 0, {T0, T0, T0} = 0 and {Tα, Tα, T0} = 0 whenever αΛ1, one may suppose that at least two distinct elements in {α, β, γ} are nonzero and one may consider the case {Tα, Tβ, Tγ} ≠ 0, α + β ≠ 0 and γ ≠ 0. Since

    0{{Tα,Tβ,Tγ},Tτ,Tϵ}{Tα,Tβ,{Tγ,Tτ,Tϵ}}ε(α¯+β¯,γ¯){Tγ,{Tα,Tβ,Tτ},Tϵ}ε(α¯+β¯,γ¯+τ¯){Tγ,Tτ,{Tα,Tβ,Tϵ}},

    any of the above three summands is nonzero. In order to complete the proof, we first will show τ, ϵ Λα01 ∪ {0}. We distinguish three cases.

    1. Suppose {Tα, Tβ, {Tγ, Tτ, Tϵ}} ≠ 0. As γ ≠ 0 and {Tγ, Tτ, Tϵ} ≠ 0, Lemma 3.3 (1) shows that τ, ϵ are connected with γ in the case of being nonzero roots and so τ, ϵ Λα01 ∪ {0}.

    2. Suppose {Tγ, {Tα, Tβ, Tτ}, Tϵ} ≠ 0. As α + β ≠ 0 and γ ≠ 0. So either α ≠ 0 or β ≠ 0. By Lemma 3.3 (1) and (2), one has τ, ϵ Λα01 ∪ {0}.

    3. Suppose {Tγ, Tτ, {Tα, Tβ, Tϵ}} ≠ 0. As α + β ≠ 0 and γ ≠ 0. So either α ≠ 0 or β ≠ 0. By Lemma 3.3 (1) and (2), one has τ, ϵ Λα01 ∪ {0}.

      Finally, we will show τ + ϵ Λα01 ∪ {0}. From the fact that α + β + γ = 0, {T0, T0, T0} = 0 and {{Tα, Tβ, Tγ}, Tτ, Tϵ} ≠ 0, let us suppose that at least one element in {τ, ϵ} is nonzero. So either τ Λα01 or ϵ Λα01 . Then {{Tα, Tβ, Tγ}, Tτ, Tϵ} ⊂ {T0, Tτ, Tϵ}. By Lemma 3.3 (2) and (3), one has τ + ϵ Λα01 ∪ {0}.

  2. From the fact that α + β + γ = 0, {T0, T0, T0} = 0 and {Tα, Tα, T0} = 0 whenever αΛ1, one may suppose that at least two distinct elements in {α, β, γ} are nonzero and one may consider the case {Tα, Tβ, Tγ} ≠ 0, α + β ≠ 0 and γ ≠ 0. Since

    0ε(α¯+β¯,ϵ¯){Tϵ,{Tα,Tβ,Tγ},Tτ}{Tα,Tβ,{Tϵ,Tγ,Tτ}}ε(α¯+β¯,ϵ¯+γ¯){Tϵ,Tγ,{Tα,Tβ,Tτ}}{{Tα,Tβ,Tϵ},Tγ,Tτ},

    any of the above three summands is nonzero. In order to complete the proof, we firstly will show τ, ϵ Λα01 ∪ {0}. We distinguish three cases.

    1. Suppose {Tα, Tβ, {Tϵ, Tγ, Tτ}} ≠ 0. As γ ≠ 0 and {Tϵ, Tγ, Tτ} ≠ 0, Lemma 3.3 (2) shows that ϵ, τ are connected with γ in the case of being nonzero roots and so ϵ, τ Λα01 ∪ {0}.

    2. Suppose {Tϵ, Tγ, {Tα, Tβ, Tτ}} ≠ 0. As α + β ≠ 0 and γ ≠ 0. So either α ≠ 0 or β ≠ 0. By Lemma 3.3 (1) and (2), one has ϵ, τ Λα01 ∪ {0}.

    3. Suppose {{Tα, Tβ, Tϵ}, Tγ, Tτ} ≠ 0. As α + β ≠ 0 and γ ≠ 0. So either α ≠ 0 or β ≠ 0. By Lemma 3.3 (1) and (2), one has ϵ, τ Λα01 ∪ {0}.

      Finally, we will show ϵ + τ Λα01 ∪ {0}. From the fact that α + β + γ = 0, {T0, T0, T0} = 0 and {Tϵ, {Tα, Tβ, Tγ}, Tτ} ≠ 0, let us suppose that at least one element in {ϵ, τ} is nonzero. So either ϵ Λα01 or τ Λα01 . Then {Tϵ, {Tα, Tβ, Tγ}, Tτ} ⊂ {Tϵ, T0, Tτ}. By Lemma 3.3 (1) and (3), one has ϵ + τ Λα01 ∪ {0}.

  3. By the definition of Lie color triple systems, one has

    0{Tτ,Tϵ,{Tα,Tβ,Tγ}}{{Tα,Tβ,Tγ},Tτ,Tϵ}ε(τ¯,ϵ¯){Tϵ,{Tα,Tβ,Tγ},Tτ}.

    Suppose {{Tα, Tβ, Tγ}, Tτ, Tϵ} ≠ 0, by Lemma 3.4 (1), one has τ, ϵ, τ + ϵ Λα01 ∪ {0}. Suppose {Tϵ, {Tα, Tβ, Tγ}, Tτ} ≠ 0, by Lemma 3.4 (2), one has τ, ϵ, ϵ + τ Λα01 ∪ {0}. Therefore, in these two cases, we get τ, ϵ, τ + ϵ Λα01 ∪ {0}.□

Lemma 3.5

Fix α0Λ1and suppose Λ0 is symmetric. If α1, α2, α3 Λα01 ∪ {0} with α1 + α2 + α3 = 0 and ϵΛ1 Λα01 , then the following assertions hold.

  1. [{Tα1, Tα2, Tα3}, Tϵ] = 0.

  2. In case ϵΛ0, then [{Tα1, Tα2, Tα3}, Lϵ¯0 ] = 0.

  3. [[{Tα1, Tα2, Tα3}, T0], Tϵ] = 0.

Proof

  1. From the fact α1 + α2 + α3 = 0, {T0, T0, T0} = 0 and {Tα, Tα, T0} = 0 for αΛ1, it is clear that if α3 = 0 one gets [{Tα1, Tα2, Tα3}, Tϵ] = 0. Let us consider the case α3 ≠ 0. By the definition of Lie color triple systems, we have

    [{Tα1,Tα2,Tα3},Tϵ¯][[Tα1,Tα2],[Tα3,Tϵ¯]]ε(α1¯+α2¯,α3¯)[Tα3,[[Tα1,Tα2],Tϵ¯]]. (3.2)

    Let us consider the first summand in Eq. (3.2). As α3 ≠ 0, one has α3 Λα01 . For ϵΛ1 Λα01 and Lemma 3.1 (4), one easily gets [Tα3, Tϵ] = 0. Therefore [[Tα1, Tα2], [Tα3, Tϵ]] = 0.

    Let us now consider the second summand in Eq. (3.2), it is sufficient to verify that

    [Tα3,[[Tα1,Tα2],Tϵ¯]]=0.

    To do so, we first assert that [[Tα1, Tα2], Tϵ] = 0. Indeed, by the definition of Lie color algebras, we have

    [[Tα1,Tα2],Tϵ¯][Tα1,[Tα2,Tϵ¯]]ε(α1¯,α2¯)[Tα2,[Tα1,Tϵ¯]], (3.3)

    where α1, α2 Λα01 ∪ {0}, ϵΛ1 Λα01 . In the following, we distinguish three cases.

    1. α1 ≠ 0 and α2 ≠ 0. As α1 Λα01 and ϵΛ1 Λα01 , by Lemma 3.1 (1), one gets [Tα1, Tϵ] = 0. As α2 Λα01 and ϵΛ1 Λα01 , by Lemma 3.1 (1), one gets [Tα2, Tϵ] = 0. Therefore by Eq. (3.3), one can show that [[Tα1, Tα2], Tϵ] = 0.

    2. α1 ≠ 0 and α2 = 0. As α1 Λα01 and ϵΛ1 Λα01 , by Lemma 3.1 (1), one gets [Tα1, Tϵ] = 0. That is [Tα2,[Tα1, Tϵ]] = 0. As α2 = 0, [Tα2, Tϵ] = [T0, Tϵ] ⊂ Lϵ¯0. . By Lemma 3.1 (4), one gets [Tα1, [Tα2, Tϵ]] = 0. Therefore by Eq. (3.3), one can show that [[Tα1, Tα2], Tϵ] = 0.

    3. α1 = 0 and α2 ≠ 0. As α2 Λα01 and ϵΛ1 Λα01 , by Lemma 3.1 (1), one gets [Tα2, Tϵ] = 0. That is [Tα1, [Tα2, Tϵ]] = 0. As α1 = 0, [Tα1, Tϵ] = [T0, Tϵ] ⊂ Lϵ¯0. By Lemma 3.1 (5), we get [ Tα2,[Tα1, Tϵ]] = 0. Therefore by (3.3), one can show that [[Tα1, Tα2], Tϵ] = 0.

      So [Tα3,[[Tα1, Tα2], Tϵ]] = 0 is a consequence of [[Tα1, Tα2], Tϵ] = 0. By (3.2), one gets [{Tα1, Tα2, Tα3}, Tϵ] = 0. The proof is complete.

  2. From the fact α1 + α2 + α3 = 0, {T0, T0, T0} = 0 and {Tα, Tα, T0} = 0 for αΛ1, one gets if α3 = 0 then it is clear that [{Tα1, Tα2, Tα3}, Lϵ¯0 ] = 0. Let us consider the case α3 ≠ 0. Note that

    [{Tα1,Tα2,Tα3},Lϵ¯0][[Tα1,Tα2],[Tα3,Lϵ¯0]]ε(α1¯+α2¯,α3¯)[Tα3,[[Tα1,Tα2],Lϵ¯0]]. (3.4)

    Let us consider the first summand in Eq. (3.4). As α3 ≠ 0, one gets [[Tα1, Tα2], [Tα3, Lϵ¯0 ]] = 0 by Lemma 3.1 (4). Let us now consider the second summand in Eq. (3.4). As either α1 ≠ 0 or α2 ≠ 0, the definition of Lie color algebras, the fact [T0, Lϵ¯0 ] ⊂ Tϵ and Lemma 3.1 (4), we obtain that [Tα3,[[Tα1, Tα2], Lϵ¯0 ]] = 0. So, the second summand in Eq. (3.4) is also zero and then [{Tα1, Tα2, Tα3}, Lϵ¯0 ] = 0.

  3. It is a consequence of Lemma 3.5 (1), (2) and

    [[{Tα1,Tα2,Tα3},T0],Tϵ¯][[T0,Tϵ¯],{Tα1,Tα2,Tα3}]+[[Tϵ¯,{Tα1,Tα2,Tα3}],T0].

Definition 3.6

A Lie color triple system T is said to be simple, if {T, T, T} ≠ 0 and its only ideals are {0} and T.

Theorem 3.7

Suppose Λ0 is symmetric, the following assertions hold.

  1. For any α0Λ1, the subsystem

    TΛα01=T0,Λα01VΛα01

    of T associated to the root subsystem Λα01 is an ideal of T.

  2. If T is simple, then there exists a connection from α to β for any α, βΛ1.

Proof

  1. Recall that

    T0,Λα01:=spanK{{Tα,Tβ,Tγ}:α+β+γ=0;α,β,γΛα01{0}}T0

    and VΛα01:=γΛα01Tγ. In order to complete the proof, it is sufficient to show that

    {TΛα01,T,T}TΛα01.

    We first check that {TΛα01,T,T}TΛα01. It is easy to see that

    {TΛα01,T,T}={T0,Λα01VΛα01,T,T}={T0,Λα01,T,T}+{VΛα01,T,T}.

    Next, we will show that {T0,Λα01,T,T}TΛα01. Note that

    {T0,Λα01,T,T}={T0,Λα01,T0(αΛ1Tα),T0(αΛ1Tα)}={T0,Λα01,T0,T0}+{T0,Λα01,T0,αΛ1Tα}+{T0,Λα01,αΛ1Tα,T0}+{T0,Λα01,αΛ1Tα,βΛ1Tβ}.

    Here, it is clear that { T0,Λα01, T0, T0} ⊂ {T0, T0, T0} = 0. Taking into account { T0,Λα01, T0, Tα}, for αΛ1, Lemma 3.4 (1) and the fact that either α Λα01 or α Λα01 , give us that { T0,Λα01, T0, Tα} ⊂ VΛα01 or { T0,Λα01, T0, Tα} = 0. Similarly, one gets that { T0,Λα01, Tα, T0} ⊂ VΛα01 or { T0,Λα01, Tα, T0} = 0. Next, we will consider { T0,Λα01, Tα, Tβ}, where α, βΛ1. We treat five cases.

    1. If α Λα01 , β Λα01 and α + β = 0. One has

      {T0,Λα01,Tα,Tβ}T0,Λα01.
    2. If α Λα01 , β Λα01 and α + β ≠ 0. By Λα01 is a root subsystem, one gets

      {T0,Λα01,Tα,Tβ}VΛα01.
    3. If α Λα01 and β Λα01 . By Lemma 3.4 (1), one has

      {T0,Λα01,Tα,Tβ}=0.
    4. If β Λα01 and α Λα01 . By Lemma 3.4 (1), one has

      {T0,Λα01,Tα,Tβ}=0.
    5. If β Λα01 and α Λα01 . By Lemma 3.4 (1), one has

      {T0,Λα01,Tα,Tβ}=0.

      Therefore, { T0,Λα01, T, T} ⊂ TΛα01 .

      Next, we will show that { VΛα01 , T, T} ⊂ TΛα01 . It is obvious that

      {VΛα01,T,T}={γΛα01Tγ,T0(αΛ1Tα),T0(αΛ1Tα)}={γΛα01Tγ,T0,T0}+{γΛα01Tγ,T0,αΛ1Tα}+{γΛα01Tγ,αΛ1Tα,T0}+{γΛα01Tγ,αΛ1Tα,βΛ1Tβ}.

      Here, it is clear that {Tγ, T0, T0} ⊂ VΛα01 , for γ Λα01 . Next, we will consider {Tγ, T0, Tα}, for γ Λα01 , αΛ1. We treat three cases.

    1. If γ Λα01 , α Λα01 . By Lemma 3.3 (1), one has

      {Tγ,T0,Tα}=0.
    2. If γ Λα01 , α Λα01 and γ + α ≠ 0. By Λα01 is a root subsystem, one has

      {Tγ,T0,Tα}VΛα01.
    3. If γ Λα01 , α Λα01 and γ + α = 0. It is clear that

      {Tγ,T0,Tα}T0,Λα01.

      Hence, {Tγ, T0, Tα} ⊂ TΛα01 , for γ Λα01 , αΛ1. Similarly, it is easy to get {Tγ, Tα, T0} ⊂ TΛα01 , for γ Λα01 , αΛ1. At last, we will consider {γΛα01 Tγ, ⊕αΛ1 Tα, ⊕βΛ1 Tβ}, for γ Λα01 , αΛ1 and βΛ1. We treat five cases.

    1. If γ Λα01 , α Λα01 , β Λα01 and γ + α + β = 0, one gets

      {Tγ,Tα,Tβ}T0,Λα01.
    2. If γ Λα01 , α Λα01 , β Λα01 and γ + α + β ≠ 0, one gets

      {γΛα01Tγ,αΛ1Tα,βΛ1Tβ}VΛα01.
    3. If γ Λα01 , α Λα01 and β Λα01 . By Lemma 3.3 (1) and (2), one gets

      {Tγ,Tα,Tβ}=0.
    4. If γ Λα01 , α Λα01 and β Λα01 . By Lemma 3.3 (1) and (3), one gets

      {Tγ,Tα,Tβ}=0.
    5. If γ Λα01 , α Λα01 and β Λα01 . By Lemma 3.3 (1), one gets

      {Tγ,Tα,Tβ}=0.

      So, { VΛα01 , T, T} ⊂ TΛα01 . Therefore { TΛα01 , T, T} ⊂ TΛα01 is a consequence of { T0,Λα01, T, T} ⊂ TΛα01 and { VΛα01 , T, T} ⊂ TΛα01 . Consequently, this proves that TΛα01 is an ideal of T.

  2. The simplicity of T implies TΛα01 = T. Hence Λα01 = Λ1.□

Theorem 3.8

Suppose Λ0 is symmetric. Then for a vector space complement U of span𝕂{{Tα, Tβ, Tγ} : α + β + γ = 0, where α, β, γΛ1 ∪ {0}} in T0, we have

T=U+[α]Λ1/I[α],

where any I[α] is one of the ideals TΛα01 of T described in Theorem 3.7. Moreover

{I[α], T, I[β]} = 0 if [α] ≠ [β].

Proof

Let us denote ξ0 := span𝕂{{Tα, Tβ, Tγ} : α + β + γ = 0, where α, β, γΛ1 ∪ {0}} in T0. By Proposition 2.17, we can consider the quotient set Λ1/∼ := {[α]: αΛ1}. By denoting I[α]:=TΛα1,T0,[α]:=T0,Λα1 and V[α] := VΛα1 , one gets I[α] := T0,[α]V[α]. From

T=T0(αΛ1Tα)=(U+ξ0)(αΛ1Tα),

it follows

αΛ1Tα=[α]Λ1/V[α],ξ0=[α]Λ1/T0,[α],

which implies

T=U+ξ0(αΛ1Tα)=U+[α]Λ1/I[α],

where each I[α] is an ideal of T by Theorem 3.7.

Next, it is sufficient to show that {I[α], T, I[β]} = 0 if [α] ≠ [β]. Note that,

{I[α],T,I[β]}={T0,[α]V[α],T0(γΛ1Tγ),T0,[β]V[β]}={T0,[α],T0,T0,[β]}+{T0,[α],T0,V[β]}+{T0,[α],γΛ1Tγ,T0,[β]}+{T0,[α],γΛ1Tγ,V[β]}+{V[α],T0,T0,[β]}+{V[α],T0,V[β]}+{V[α],γΛ1Tγ,T0,[β]}+{V[α],γΛ1Tγ,V[β]}.

Here, it is clear that {T0,[α], T0, T0,[β]} ⊂ {T0, T0, T0} = 0. If [α] ≠ [β], by Lemmas 3.3 and 3.4, it is easy to see {T0,[α], T0, V[β]} = 0, {T0,[α], ⊕γΛ1Tγ, V[β]} = 0, {V[α], T0, T0,[β]} = 0, {V[α], T0, V[β]} = 0, {V[α], ⊕γΛ1Tγ, T0,[β]} = 0, {V[α], ⊕γΛ1Tγ, V[β]} = 0.

Next, we will show {T0,[α], ⊕γΛ1Tγ, T0,[β]} = 0. Indeed, for {Tα1, Tα2, Tα3} ∈ T0,[α] with α1, α2, α3 Λα1 ∪ {0}, α1 + α2 + α3 = 0, and for {Tβ1, Tβ2, Tβ3} ∈ T0,[β] with β1, β2, β3 Λβ1 ∪ {0}, β1 + β2 + β3 = 0, by the definition of Lie color triple systems, one gets

{{Tα1,Tα2,Tα3},γΛ1Tγ,{Tβ1,Tβ2,Tβ3}}ε(γ1¯,β1¯+β2¯){Tβ1,Tβ2,{{Tα1,Tα2,Tα3},γΛ1Tγ,Tβ3}}+{{{Tα1,Tα2,Tα3},γΛ1Tγ,Tβ1},Tβ2,Tβ3}+ε(γ1¯,β1¯){Tβ1,{{Tα1,Tα2,Tα3},γΛ1Tγ,Tβ2},Tβ3}.

By Lemma 3.4, it is easy to see that

{Tβ1,Tβ2,{{Tα1,Tα2,Tα3},γΛ1Tγ,Tβ3}}=0,{{{Tα1,Tα2,Tα3},γΛ1Tγ,Tβ1},Tβ2,Tβ3}=0,{Tβ1,{{Tα1,Tα2,Tα3},γΛ1Tγ,Tβ2},Tβ3}=0.

for α1, α2, α3 Λα1 ∪ {0}, α1 + α2 + α3 = 0, β1, β2, β3 Λβ1 ∪ {0}, β1 + β2 + β3 = 0, [α] ≠ [β]. So {I[α], T, I[β]} = 0 if [α] ≠ [β].□

Definition 3.9

The annihilator of a Lie color triple system T is the set Ann(T) = {xT : {x, T, T} = 0}.

Corollary 3.10

Suppose Λ0 is symmetric. If Ann(T) = 0, and {T, T, T} = T, then T is the direct sum of the ideals given in Theorem 3.8,

T=[α]Λ1/I[α].

Proof

From {T, T, T} = T and Theorem 3.8, we have

{U+[α]Λ1/I[α],U+[α]Λ1/I[α],U+[α]Λ1/I[α]}=U+[α]Λ1/I[α].

Taking into account UT0, Lemma 3.3 and the fact that {I[α], T, I[β]} = 0 if [α] ≠ [β] (see Theorem 3.8) give us that U = 0. That is,

T=[α]Λ1/I[α].

To finish, it is sufficient to show the direct character of the sum. For xI[α] [β]Λ1/βα̸ I[β], using again the equation {I[α], T, I[β]} = 0 for [α] ≠ [β], we obtain

{x,T,I[α]}={x,T,[β]Λ1/βα̸I[β]}=0.

So {x, T, T} = {x, T, I[α] + [β]Λ1/βα̸ I[β]} = {x, T, I[α]} + {x, T, [β]Λ1/βα̸ I[β]} = 0+0 = 0. That is, x ∈ Ann(T) = 0. Thus x = 0, as desired.□

4 The simple components

In this section we study if any of the components in the decomposition given in Corollary 3.10 is simple. Under certain conditions we give an affirmative answer. From now on char(𝕂) = 0.

Lemma 4.1

Let T = T0 ⊕ (⊕αΛ1Tα) be a split Lie color triple system. If I is an ideal of T then I = (IT0) ⊕ (⊕αΛ1(ITα)).

Proof

We can see that T = T0 ⊕ (⊕αΛ1Tα) as a weight module with respect to the split Lie color algebra L0 with MAGSA H0. The character of the ideal of I and the fact L0 = [T, T] give us that I is a submodule of T. It is well-known that a submodule of a weight module is again a weight module. From here, I is a weight module with respect to L0 (and H0) and so I = (IT0) ⊕ (⊕αΛ1(ITα)).

Taking into account the above lemma, observe that the grading of I and Lemma 2.13 (1) let us write

I=gΓIg=gΓ((IgT0,g)(αΛ1(IgTα,g))). (4.5)

Let us introduce the concepts of root-multiplicativity and maximal length in the frame work of split Lie color triple systems. For each gΓ, we denote by Λg1 := {αΛ1, Tα,g ≠ 0} and Λg0:={αΛ0,Lα,g00}.

Definition 4.2

We say that a split Lie color triple system T is root-multiplicative if given α Λgi1,βΛgj1 and γ Λgk1, with gi, gj, gkΓ, such that α + βΛ0, and α + β + γΛ1, then {Tα,gi, Tβ,gj, Tγ,gk} ≠ 0.

Definition 4.3

We say that a split Lie color triple system T is of maximal length if for any α Λg1 , gΓ, we have dimTκα,κg = 1 for κ ∈ {±1}.

Observe that if T is of maximal length, then Eq. (4.5) enables us assert that given any nonzero ideal I of T then

I=gΓIg=gΓ((IgT0,g)(αΛg1,ITα,g)). (4.6)

where Λg1,I := {αΛ1 : IgTα,g ≠ 0} for each gΓ.

Lemma 4.4

Let T be a root-multiplicative split Lie color triple system with Ann(T) = 0. If for any αΛ1, we have dimLα0=1 . Then there is not any nonzero ideal of T contained in T0.

Proof

Suppose there exists a nonzero ideal I of T such that IT0. Given αΛ1, as {I, T0, Tα} ⊂ TαT0 and {I, Tα, T0} ⊂ TαT0, {I, T0, Tα} = {I, Tα, T0} = 0. Given also βΛ1 with α + β ≠ 0, {I, Tα, Tβ} ⊂ Tα+βT0 = 0. As Ann(T) = 0, {I, Tα, Tα} ≠ 0 for some αΛ1. Thus, there exist t±αT±α and t0I such that {t0,tα, tα} ≠ 0. Hence 0 ≠ [t0, tα] ∈ Lα0. As dimLα0=1 , the root-multiplicativity of T (consider the roots 0, α, 0 ∈ Λ1 ∪ {0}), and the fact that dimLα0=1 give us the existence of 0 ≠ t0 T0 such that 0 ≠ {t0, tα, t0 } ∈ Tα. As t0I, we conclude 0 ≠ tα := {t0, tα, t0 } ∈ IT0, a contradiction. Hence, I is not contained in T0.□

Theorem 4.5

Let T be a split Lie color triple system of maximal length, root-multiplicative, with Ann(T) = 0 and satisfying T = {T, T, T}. If Λ0 is symmetric and for any αΛ1, we have dimLα01. Then T is simple if and only if it has all its nonzero roots connected.

Proof

The first implication is Theorem 3.7 (2). To prove converse, consider I a nonzero ideal of T, by Lemma 4.4 and Eq. (4.6) we can write

I=gΓIg=gΓ((IgT0,g)(αΛg1,ITα,g)).

with Λg1,I Λg1 for any gΓ and some Λg1,I ≠ ∅. Hence by the maximal length of T, we may choose α0 Λg1,I such that

0Tα0,gI. (4.7)

Given any β0Λ1 with β0 ∉ {α0, −α0}, the fact that α0 and β0 are connected gives us a connection {α1, ⋯, α2n+1} from α0 to β0 such that α1 = α0, α1 + α2 + α3, ⋯, α1 + ⋯ + α2n + α2n+1Λ1, α1 + α2, ⋯, α1 + ⋯ + α2nΛ0 and α1 + ⋯ + α2n + α2n+1 ∈ {β0, −β0}. Consider α1 = α0, α2, α3 and α1 + α2 + α3. Since α2Λ1 there exists g1Γ such that Tα2,g1 ≠ 0. Since α3Λ1 there exists g2Γ such that Tα3,g2 ≠ 0. From here, the root-multiplicativity and maximal length of T shows 0 ≠ {Tα0,g, Tα2,g1, Tα3,g2} = Tα1+α2+α3,g+g1+g2, and by Eq. (4.7)

0Tα1+α2+α3,g+g1+g2I.

We can argue in a similar way from α1 + α2 + α3, α4, α5 and α1 + α2 + α3 + α4 + α5 to get

0Tα1+α2+α3+α4+α5,g3I.

for some g3Γ. Following this process with the connection {α1, ⋯, α2n+1} we obtain that

0Tα1+α2++α2n+1,g4I

and so either Tβ0,g4I or Tβ0,g4I for some g4Γ. That is,

0Tϵβ0,g4I (4.8)

for some ϵ ∈ {±1}, some g4Γ and for any β0Λ1 with β0 ∉ {α0, −α0}.

Taking into account H0 = [T0, T0] + ∑αΛ1 [Tα, Tα], the grading of T gives us Hg0=g1+g2=g,g1,g2Γ[T0,g1,T0,g2]+αΛ1g1+g2=g,g1,g2Γ[Tα,g1,Tα,g2]. We can suppose that either H00 = ∑gΓ[T0,g, T0,−g] or H00 = ∑αΛ1,gΓ[Tα,g, Tα,−g]. We treat two cases.

In the first case, by Eq. (4.8), there exists g5Γ such that

[[T0,g5,T0,g5],Tϵβ0,g4]0. (4.9)

By the Jacobi identity of the Lie color algebras, either [T0,g5, Tϵβ0,g4] ≠ 0 or [T0,−g5, Tϵβ0,g4] ≠ 0 and so Lϵβ0,g4+g500 or Lϵβ0,g4g500. That is

0Lϵβ0,κg5+g40I (4.10)

for some κ ∈ {±1}. Since ϵβ0 Λg41, we have by the maximal length of T such that −ϵβ0 Λg41. By Eq. (4.10), and the root-multiplicativity and maximal length of T, we obtain

0[Lϵβ0,κg5+g40,Tϵβ0,g4]=T0,κg5I. (4.11)

Taking into account Eq. (4.11) and that Eq. (4.9) gives us

β0([T0,g5,T0,g5])0,

we have that for any g6Γ such that Tϵβ0,g6 ≠ 0 necessarily

0[[T0,g5,T0,g5],Tϵβ0,g6]=Tϵβ0,g6I,

and so

Tϵβ0I, (4.12)

for any β0Λ1 with β0 ∉ {α0, −α0}, and some ϵ ∈ {±1}.

In the second case, by Eq. (4.8), there exists g7Γ such that

[[Tα,g7,Tα,g7],Tϵβ0,g4]0. (4.13)

By the Jacobi identity of the Lie color algebras, either

[Tα,g7,Tϵβ0,g4]0,

or

[Tα,g7,Tϵβ0,g4]0,

and so Lα+ϵβ0,g4+g700 or Lα+ϵβ0,g4g700. That is

0Lκα+ϵβ0,κg7+g40I, (4.14)

for some κ ∈ {±1}. Since ϵβ0 Λg41, we have by the maximal length of T such that −ϵβ0 Λg41. By Eq. (4.14), and the root-multiplicativity and maximal length of T we obtain

0[Lκα+ϵβ0,κg7+g40,Tϵβ0,g4]=Tκα,κg7I. (4.15)

Taking into account Eq. (4.15) and that Eq. (4.13) gives us

β0([Tα,g7,Tα,g7])0,

we have that for any g8Γ such that Tϵβ0,g8 ≠ 0 necessarily

0[[Tα,g7,Tα,g7],Tϵβ0,g8]=Tϵβ0,g8I,

and so

Tϵβ0I, (4.16)

for any β0Λ1 with β0 ∉ {α0, −α0}, and some ϵ ∈ {±1}.

Observe that as a consequence of T = {T, T, T}, we have

T0=α+β+γ=0α,β,γΛ1{0}{Tα,Tβ,Tγ}. (4.17)

Let us study the products {Tα, Tβ, Tγ} of Eq. (4.17) in order to show T0I. Taking into account {T0, T0, T0} = 0, and the fact α + β + γ = 0 with α, β, γΛ1 ∪ {0}, we can suppose γ ≠ 0 and either α ≠ 0 or β ≠ 0. Suppose α ≠ 0 and β = 0 (resp. α = 0 and β ≠ 0), then α = −γ (resp. β = −γ) and by Eqs. (4.12) and (4.16), {Tα, Tβ, Tγ} = {Tγ, T0, Tγ} ⊂ I, (resp. {Tα, Tβ, Tγ} = {T0,Tγ, Tγ} ⊂ I). If the three elements in {α, β, γ} are nonzero, in case some TϵI, ϵ ∈ {α, β, γ}, then clearly {Tα, Tβ, Tγ} ⊂ I. Finally, consider the case in which any of the Tϵ does not belong to I. If {Tα, Tβ, Tγ} = 0 then {Tα, Tβ, Tγ} ⊂ I. If {Tα, Tβ, Tγ} ≠ 0, necessarily α + β ≠ 0 and so α + βΛ0. From here, we have by root-multiplicativity {Tα, Tβ, Tβ} = Tα. Eqs. (4.12) and (4.16) give us TβI, then TαI and so {Tα, Tβ, Tγ} ⊂ I. Therefore Eq. (4.17) implies

T0I. (4.18)

Fix now any α0Λ1. By Eqs. (4.12) and (4.16), either Tα0I or Tα0I. Write Tρα0I with ρ ∈ ± 1, then we can show Tρα0I. Indeed, since α0 ≠ 0, there exists h0 H00 such that α0(h0) ≠ 0 and so we have

tρα0=ρα0(h0)1[h0,tρα0], (4.19)

for any tρα0Tρα0.

As

H00=gΓ[T0,g,T0,g]+αΛ1,gΓ[Tα,g,Tα,g],

we can suppose that either h0=[t0,g,t0,g] with t0,gT0,g, t0,g T0,−g or h0 = [tα,g, tα,−g] with tα,gTα,g, tα,−gTα,−g. From here, in order to prove that T±α0I for any α0Λ1. we treat two cases.

In the first case, we have by Eqs (4.18) and (4.19), that

tρα0=ρα0(h0)1[[t0,g,t0,g],tρα0]I, (4.20)

for any tρα0Tρα0.

In the second case, we have by Eqs (4.18) and (4.19), that

tρα0=ρα0(h0)1[[tα,g,tα,g],tρα0]I, (4.21)

for any tρα0Tρα0.

Since dimTρα0 = 1, we conclude Tρα0I and so T±α0I for any α0Λ1. From here, and taking into account Eqs (4.16) and (4.18), we conclude I = T and so T is simple.□

Acknowledgement

The authors would like to thank the referee for valuable comments and suggestions on this article.

Supported by NNSF of China (Nos. 11801121 and 11871181), NSF of Heilongjiang province(No. QC2018006) and the Fundamental Research Fundation for Universities of Heilongjiang Province (No. LGYC2018JC002).

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Received: 2018-09-06
Accepted: 2019-02-14
Published Online: 2019-04-09

© 2019 Cao et al., published by De Gruyter

This work is licensed under the Creative Commons Attribution 4.0 Public License.

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