Leibniz algebras with absolute maximal Lie subalgebras

A Lie subalgebra of a given Leibniz algebra is said to be an absolute maximal Lie subalgebra if it has codimension one. In this paper, we study some properties of non-Lie Leibniz algebras containing absolute maximal Lie subalgebras. When the dimension and codimension of their Lie-center are greater...

Ausführliche Beschreibung

Gespeichert in:
Bibliographische Detailangaben
Datum:2020
Hauptverfasser: Biyogmam, G.R., Tcheka, C.
Format: Artikel
Sprache:English
Veröffentlicht: Інститут прикладної математики і механіки НАН України 2020
Schriftenreihe:Algebra and Discrete Mathematics
Online Zugang:https://nasplib.isofts.kiev.ua/handle/123456789/188501
Tags: Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
Назва журналу:Digital Library of Periodicals of National Academy of Sciences of Ukraine
Zitieren:Leibniz algebras with absolute maximal Lie subalgebras / G.R. Biyogmam, C. Tcheka // Algebra and Discrete Mathematics. — 2020. — Vol. 29, № 1. — С. 52–65. — Бібліогр.: 18 назв. — англ.

Institution

Digital Library of Periodicals of National Academy of Sciences of Ukraine
id nasplib_isofts_kiev_ua-123456789-188501
record_format dspace
spelling nasplib_isofts_kiev_ua-123456789-1885012025-02-09T18:18:34Z Leibniz algebras with absolute maximal Lie subalgebras Biyogmam, G.R. Tcheka, C. A Lie subalgebra of a given Leibniz algebra is said to be an absolute maximal Lie subalgebra if it has codimension one. In this paper, we study some properties of non-Lie Leibniz algebras containing absolute maximal Lie subalgebras. When the dimension and codimension of their Lie-center are greater than two, we refer to these Leibniz algebras as s-Leibniz algebras (strong Leibniz algebras). We provide a classification of nilpotent Leibniz s-algebras of dimension up to five. 2020 Article Leibniz algebras with absolute maximal Lie subalgebras / G.R. Biyogmam, C. Tcheka // Algebra and Discrete Mathematics. — 2020. — Vol. 29, № 1. — С. 52–65. — Бібліогр.: 18 назв. — англ. 1726-3255 DOI:10.12958/adm1165 2010 MSC: 17A32, 17B55, 18B99. https://nasplib.isofts.kiev.ua/handle/123456789/188501 en Algebra and Discrete Mathematics application/pdf Інститут прикладної математики і механіки НАН України
institution Digital Library of Periodicals of National Academy of Sciences of Ukraine
collection DSpace DC
language English
description A Lie subalgebra of a given Leibniz algebra is said to be an absolute maximal Lie subalgebra if it has codimension one. In this paper, we study some properties of non-Lie Leibniz algebras containing absolute maximal Lie subalgebras. When the dimension and codimension of their Lie-center are greater than two, we refer to these Leibniz algebras as s-Leibniz algebras (strong Leibniz algebras). We provide a classification of nilpotent Leibniz s-algebras of dimension up to five.
format Article
author Biyogmam, G.R.
Tcheka, C.
spellingShingle Biyogmam, G.R.
Tcheka, C.
Leibniz algebras with absolute maximal Lie subalgebras
Algebra and Discrete Mathematics
author_facet Biyogmam, G.R.
Tcheka, C.
author_sort Biyogmam, G.R.
title Leibniz algebras with absolute maximal Lie subalgebras
title_short Leibniz algebras with absolute maximal Lie subalgebras
title_full Leibniz algebras with absolute maximal Lie subalgebras
title_fullStr Leibniz algebras with absolute maximal Lie subalgebras
title_full_unstemmed Leibniz algebras with absolute maximal Lie subalgebras
title_sort leibniz algebras with absolute maximal lie subalgebras
publisher Інститут прикладної математики і механіки НАН України
publishDate 2020
url https://nasplib.isofts.kiev.ua/handle/123456789/188501
citation_txt Leibniz algebras with absolute maximal Lie subalgebras / G.R. Biyogmam, C. Tcheka // Algebra and Discrete Mathematics. — 2020. — Vol. 29, № 1. — С. 52–65. — Бібліогр.: 18 назв. — англ.
series Algebra and Discrete Mathematics
work_keys_str_mv AT biyogmamgr leibnizalgebraswithabsolutemaximalliesubalgebras
AT tchekac leibnizalgebraswithabsolutemaximalliesubalgebras
first_indexed 2025-11-29T13:43:47Z
last_indexed 2025-11-29T13:43:47Z
_version_ 1850132490624172032
fulltext “adm-n1” — 2020/5/14 — 19:35 — page 52 — #60 © Algebra and Discrete Mathematics RESEARCH ARTICLE Volume 29 (2020). Number 1, pp. 52–65 DOI:10.12958/adm1165 Leibniz algebras with absolute maximal Lie subalgebras G. R. Biyogmam and C. Tcheka Communicated by L. A. Kurdachenko Abstract. A Lie subalgebra of a given Leibniz algebra is said to be an absolute maximal Lie subalgebra if it has codimension one. In this paper, we study some properties of non-Lie Leibniz algebras containing absolute maximal Lie subalgebras. When the dimension and codimension of their Lie-center are greater than two, we refer to these Leibniz algebras as s-Leibniz algebras (strong Leibniz algebras). We provide a classification of nilpotent Leibniz s-algebras of dimension up to five. 1. Introduction Leibniz algebras were introduced by Jean-Louis Loday (see [16]) as noncommutative versions of Lie algebras. Several authors (see [2,3,5,6,11, 12] for examples) have investigated whether the results on Lie algebras can be extended to Leibniz algebras. In [5] for instance, D. Barnes proved an analogue of Levi’s decomposition for Leibniz algebras, which states that every finite dimensional Leibniz algebra g over a field of characteristic zero can be written as a direct sum of its solvable radical and a semisimple Lie subalgebra. Note that in this theorem, the Lie algebra s is not necessarily a maximal Lie subalgebra of g. In this paper, we examine non-Lie Leibniz algebras that can be written as semi-direct sum in which one summand is a maximal Lie subalgebra of codimension one. We will refer to these Lie subalgebras to as absolute maximal Lie subalgebras. Maximal subalgebras 2010 MSC: 17A32, 17B55, 18B99. Key words and phrases: Leibniz algebras, s-Leibniz algebras, Lie-center. https://doi.org/10.12958/adm1165 “adm-n1” — 2020/5/14 — 19:35 — page 53 — #61 G. R. Biyogmam, C. Tcheka 53 of codimension one in Lie algebras have been studied in [1,17,18]. We will particularly focus on the Leibniz algebras containing Lie subalgebras of codimension one, for which the Lie-center has dimension and codimension greater than two. We call them s-Leibniz algebras. We investigate their properties in section 3. This work opens the interesting debate as to evaluate how much properties does an s-Leibniz algebra inherit from its absolute maximal Lie subalgebra structure. For instance, we prove that an s-Leibniz algebra g with absolute maximal Lie subalgebra s is nilpotent and solvable if s is a nilpotent ideal. Also, we provide certain conditions under which a Leibniz algebra is an s-Leibniz algebra. We also show that all absolute maximal Lie subalgebras of an s-Leibniz algebra meet at its Lie-center. In section 4, we provide a classification of nilpotent s-Leibniz algebra of dimension up to five. 2. Leibniz algebras We fix K as a ground field such that 1 2 ∈ K. All vector spaces and tensor products are considered over K. A (left) Leibniz algebra [15, 16] is a vector space g equipped with a bilinear map [−,−] : g⊗ g → g, usually called the Leibniz bracket of g, satisfying the Leibniz identity : [x, [y, z]] = [[x, y], z] + [y, [x, z]], x, y, z ∈ g. Leibniz algebras form a semi-abelian category [7, 14], denoted by Leib, whose morphisms are linear maps that preserve the Leibniz bracket. The Leibniz identity above generalizes the Jacobi identity since g becomes a Lie algebra when this bracket is antisymmetric. This defines the inclusion functor Lie →֒ Leib. For a Leibniz algebra g, we denote by gann the subspace of g spanned by all elements of the form [x, x], x ∈ g. Given a Leibniz algebra g, it is clear that the quotient g Lie = g/gann is a Lie algebra. This defines a left adjoint functor to Lie →֒ Leib, known as the Liezation functor (−)Lie : Leib → Lie, which assigns the Lie algebra g Lie to a given Leibniz algebra g. A subalgebra h of a Leibniz algebra g is said to be left (resp. right) ideal of g if [h, q] ∈ h (resp. [q, h] ∈ h), for all h ∈ h, q ∈ g. If h is both left and right ideal, then h is called two-sided ideal of g. In this case g/h naturally inherits a Leibniz algebra structure. The Lie-center of the Leibniz algebra g is the two-sided ideal ZLie(g) = {z ∈ g | [g, z] + [z, g] = 0 for all g ∈ g}. “adm-n1” — 2020/5/14 — 19:35 — page 54 — #62 54 Leibniz algebras For a Leibniz algebra g and two-sided ideals m and n of g, the Lie-centralizer of m and n over g is CLie g (m, n) = {g ∈ g | [g,m] + [m, g] ∈ n, for all m ∈ m} . In particular, the Lie-centralizer of m is defined by CLie g (m, 0) = {g ∈ g/[g,m] + [m, g] = 0, for all m ∈ m}. These notions of Lie-center and Lie-centralizer were studied in [4,6,8,9] as a result of approaching the relative theory of Leibniz algebras with respect to the Liezation functor. Note that ZLie(g) = {x ∈ g | CLie g ({x}, 0) = g}. Also, [x, y]Lie = [x+ y, x+ y]− [x, x]− [y, y] for all x, y ∈ g. Consequently, [g, g]Lie ⊆ gann. Considering the set T = {t ∈ g | [t, t] = 0}, it is clear that the sets T and g are equal iff g is a Lie algebra. 3. Leibniz algebras with absolute maximal Lie subalgebras In this section, we describe non-Lie Leibniz algebras containing absolute maximal Lie subalgebras. We discuss the cases where dim(ZLie(g)) = n−1 or dim(ZLie(g)) = 1, and pay a particular attention to the non-Lie Leibniz algebras g satisfying 1 < dim(ZLie(g)) < n− 1. Definition 3.1. Let g be a Leibniz algebra. A subalgebra s of g is called absolute maximal Lie subalgebra if s is a maximal Lie subalgebra of g of codimension one. Clearly, if g is a Lie algebra, then all maximal subalgebras of codi- mension one are absolute maximal Lie subalgebras. Studies of maximal subalgebras of codimension one in Lie algebras can be found in [1, 17, 18]. For the remaining of the paper, we are interested in non-Lie Leibniz algebras. Proposition 3.2. Let g be a finite dimensional non-Lie Leibniz algebra and s a maximal Lie subalgebra of g. Then ZLie(g) is a 2-sided ideal of s. Proof. It is enough to show that ZLie(g) ⊆ s since ZLie(g) is a 2-sided ideal of g. Indeed, let g ∈ ZLie(g) and assume that g /∈ s. Then, L := span{g, s} = g since s is a maximal subalgebra of g. Moreover L is a Lie algebra because [g, x] = −[x, g] for all x ∈ g as g ∈ ZLie(g). This contradicts the fact that g is a non-Lie Leibniz algebra. “adm-n1” — 2020/5/14 — 19:35 — page 55 — #63 G. R. Biyogmam, C. Tcheka 55 Lemma 3.3. Let g be a n-dimensional non-Lie Leibniz algebra such that (g− ZLie(g)) ∩ T 6= ∅. The following is true: a) ZLie(g) is not a maximal Lie subalgebra of g, b) dim(ZLie(g)) < n− 1, c) If T is a subalgebra of g and |(g − ZLie(g)) ∩ T | > k, then dim(ZLie(g)) < n− k for any k < n. Proof. To prove a), let a /∈ ZLie(g) and a ∈ T. By definition of ZLie(g), we have [x, a]Lie = 0 for all x ∈ ZLie(g). It follows that h := span{ZLie(g), a} is a Lie subalgebra of g strictly containing ZLie(g). Moreover, if dim(ZLie(g)) = n − 1, then g = h which contradicts the fact that g is a non-Lie Leibniz algebra. This proves b). To prove c), consider k < l < n fixed, and let a1 . . . al /∈ ZLie(g) with [ai, ai] = 0 for all 1 6 i 6 l. Clearly [x, ai]Lie = 0 for all x ∈ ZLie(g) and 1 6 i 6 l. Also, since T is a subalgebra of g, we have [ai, aj ]Lie = [ai + aj , ai + aj ] − [ai, ai] − [aj , aj ] = 0. It follows that h := span{ZLie(g), a1, . . . , al} is a Lie subalgebra of g. Since g is a non-Lie Leibniz algebra of dimension n, it follows that dim(ZLie(g)) + l < n, and thus dim(ZLie(g)) < n− l < n− k. Proposition 3.4. Let g be a n-dimensional non-Lie Leibniz algebra, and s a Lie subalgebra of g such that (g− s) ∩ T 6= ∅. If T is a subalgebra of g, then s is not a maximal Lie subalgebra of g, and dim(s) < n− 1. Proof. Let a /∈ s and a ∈ T, i.e. [a, a] = 0. Since T is a subalgebra of g, we have [x, a]Lie = [x + a, x + a] − [x, x] − [a, a] = 0 for all x ∈ s. It follows that h := span{s, a} is a Lie subalgebra of g strictly containing s. Moreover, if dim(s) = n− 1, then g = h which contradicts the fact that g is a non-Lie Leibniz algebra. Corollary 3.5. Let g be a finite dimensional non-Lie Leibniz algebra such that dim( g ZLie(g) ) = 1. Then ZLie(g) is the unique absolute maximal Lie subalgebra of g. Proof. Since dim(ZLie(g)) = dim(g) − 1, one easily verifies that ZLie(g) is a maximal Lie subalgebra of g. Now by Proposition 3.2, ZLie(g) is contained in all maximal Lie subalgebra of g. The result follows by the maximality of ZLie(g). Example 3.6. Consider the Leibniz algebra g spanned by {a1, a2, a3, a4, a5} with nonzero bracket [a1, a2] = a5, [a2, a1] = −a5, [a3, a4] = “adm-n1” — 2020/5/14 — 19:35 — page 56 — #64 56 Leibniz algebras a5, [a4, a3] = −a5, [a4, a4] = a5. Then one can verify that ZLie(g) = span{a1, a2, a3, a5} is the unique maximal Lie subalgebra of g. Proposition 3.7. Let g be a n-dimensional non-Lie left central Leibniz algebra with one dimensional Lie-center. Then t = span{t ∈ g | [t, t] = 0} is an absolute maximal Lie subalgebra of g. Proof. Since g is left central, then for all t ∈ g, [t, t] ∈ ZLie(g). It follows that g ZLie(g) = span{t + ZLie(g), [t, t] = 0}. Moreover, gann = ZLie(g), so the map g → ZLie(g) defined by t 7→ [t, t] induces an isomorphism g t ∼= ZLie(g). Therefore the set t = span{t ∈ g | [t, t] = 0} is an absolute maximal Lie subalgebra of g. Proposition 3.8. Let g be a n-dimensional nilpotent non-Lie Leibniz algebra with (n−1)-dimensional derived subalgebra. Then dim(ZLie(g)) = 1 and [g, g] is the unique absolute maximal Lie subalgebra of g. Proof. By [2, Lemma 1], g is generated by {x1, x2, x3, . . . , xn} satisfying the conditions [xi, x1] = xi+1 for 1 6 i 6 n− 1, [xi, xj ] = 0 for j > 2. It is easily verified that ZLie(g) = span{xn} and [g, g] = span{x2, x3, . . . , xn} is the only absolute maximal Lie subalgebra of g. The following definition introduces a subclass of Leibniz algebras called strong Leibniz algebras (s-Leibniz algebras). Definition 3.9. A n-dimensional non-Lie Leibniz algebra g is said to be an s-Leibniz algebra if: (S1) dim(ZLie(g)) > 2 and codim(ZLie(g)) > 2; (S2) g contains an absolute maximal Lie subalgebra. Remark 3.10. Leibniz algebras of Corollary 3.5, Proposition 3.7 and Proposition 3.8 do not satisfy the condition (S1). So they are not s-Leibniz algebras. Example 3.11. Consider the Leibniz algebra g spanned by {a, b, c, d, e} with nonzero bracket [a, d] = e, [b, c] = e, [b, d] = e, [c, b] = −e, [c, c] = e, [d, a] = −e and [d, b] = e. Then one can verify that ZLie(g) = span{a, e}, and g contains no absolute maximal Lie subalgebra, and so g is not an s-Leibniz algebra. Example 3.12. Consider the Leibniz algebra g spanned by {a1, a2, a3, a4, a5} with nonzero bracket [a1, a1] = a4, [a1, a2] = a3, [a2, a1] = −a3, [a2, a3] = a5, [a3, a2] = −a5, [a1, a4] = a5. Then one can verify that ZLie(g) = span{a2, a3, a5}, and s = span{a2, a3, a4, a5} is an absolute maximal Lie subalgebra of g. So g is an s-Leibniz algebra. “adm-n1” — 2020/5/14 — 19:35 — page 57 — #65 G. R. Biyogmam, C. Tcheka 57 Remark 3.13. Let g be a finite dimensional s-Leibniz algebra with absolute maximal Lie subalgebra s. By Proposition 3.2, ZLie(g) is a 2- sided ideal of s. Lemma 3.14. Let g be a n-dimensional s-Leibniz algebra with a absolute maximal Lie subalgebra s. If s is a two-sided ideal of g, then [g, g] ⊆ s. Proof. Let 〈x〉 be the complement of s in g. Then [a, x], [x, a], [a, b] ∈ s for all a, b ∈ s. It remains to show that [x, x] ∈ s. Indeed assume that [x, x] = αx+h for some α ∈ R and h ∈ s. Then by linearity and using the Leibniz identity, we have α[x, x] + [h, x] = [αx+ h, x] = [[x, x], x] = 0 ∈ s. Since [h, x] ∈ s, it follows that either α = 0 in which case [x, x] = h or [x, x] = 0. Corollary 3.15. Let g be a finite dimensional s-Leibniz algebra with absolute maximal Lie subalgebra s. If s is a nilpotent two-sided ideal of g, then g is solvable and nilpotent. Proof. Using Lemma 3.14, one can easily verify that if s is nilpotent, then [g, g] is nilpotent, and thus g is nilpotent. Moreover, g is solvable by [13, Corollary 6]. Proposition 3.16. Let g be s-Leibniz algebra and let S be the set of all absolute maximal Lie subalgebras of g. If |S| 6= 1, then ZLie(g) = ⋂ s∈S s. Proof. By Proposition 3.13, ZLie(g) is contained in every absolute maximal Lie subalgebra of g. Conversely, let g ∈ ⋂ s∈S s and assume that g /∈ ZLie(g). Then [x, g] + [g, x] 6= 0 for some x ∈ g. This implies that x /∈ ⋃ s∈S s, otherwise, x, g ∈ s0 for some Lie subalgebra of g, which contradicts [x, g] + [g, x] 6= 0. So we have span{x, s} = g for all s ∈ S, and thus |S| = 1. A contradiction. Recall the following Levi’s Theorem proven by D. Barnes for Leibniz algebras: Theorem 3.17. [5] Every finite-dimensional Leibniz algebra g over a field of characteristic 0 can be written as g = s⊕ Rad(g), where s is a semi- simple Lie subalgebra of g, and Rad(g) is the solvable radical of g. Proposition 3.18. Let g be a Leibniz algebra satisfying (S1), and h an absolute maximal subalgebra of g containing ZLie(g), and such that h/ZLie(g) is a semisimple Lie subalgebra of g/ZLie(g). Then g is an s-Leibniz algebra with absolute maximal Lie subalgebra h. “adm-n1” — 2020/5/14 — 19:35 — page 58 — #66 58 Leibniz algebras Proof. By Theorem 3.17, h = s⊕Rad(h) for some semisimple Lie subalge- bra s of h. But since h/ZLie(g) is a semisimple Lie subalgebra of g/ZLie(g), it follows that h = ZLie(g) + s, which is clearly a Lie-subalgebra of g. Therefore h is an absolute maximal Lie subalgebra of g. Corollary 3.19. Let g be a Leibniz algebra satisfying (S1), and such that g/ZLie(g) contains an absolute maximal semisimple subalgebra. Then g is an s-Leibniz algebra. Proof. Let h/ZLie(g) is an absolute maximal semisimple subalgebra of g/ZLie(g). Then by the proof of Proposition 3.18, h is a Lie subalgebra of g. It is easy to show that h is an absolute maximal subalgebra of g. 4. Classification of all nilpotent s-Leibniz algebras dimension at most 5 In this section, we use the classification of four and five dimensional nilpotent Leibniz Algebras provided in [10] to determine all nilpotent s- Leibniz algebras of dimension four and five. This consists for each Leibniz algebra to find the Lie-center and the absolute maximal Lie subalgebra (if it exists), and verify satisfaction of the condition (S1) on the Lie-center. As pointed out in [10], these Leibniz algebras are non-split, i.e. they cannot be written as a direct sum of two nontrivial ideals. Split Leibniz algebras can be obtained from non split ones. Theorem 4.1. Every four dimensional non-split nilpotent s-Leibniz alge- bra is isomorphic to a Leibniz algebra spanned by {x1, x2, x3, x4} where the nonzero products are given by following: A12: [x1, x1]=x4, [x1, x2]=x3, [x2, x1]=−x3+x4, [x1, x3]=x4=−[x3, x1]. A13: [x1, x2]=x3, [x2, x1]=−x3+x4, [x2, x2]=x4, [x1, x3]=x4=−[x3, x1]. A14: [x1, x1] = x3, [x1, x2] = x4. A15: [x1, x1] = x3, [x2, x1] = x4. A16: [x1, x2] = x4, [x2, x1] = x3, [x2, x2] = −x3. A17: [x1, x1] = x3, [x1, x2] = x4, [x2, x1] = αx4, α ∈ C/{−1, 0} Proof. The result is obtained by checking each Leibniz algebra of Theorem 3.2.3 in [10]. We kept the same numbering of these Leibniz algebras as in [10] for the convenience of the reader. The basis of the corresponding Lie-centers and absolute maximal Lie subalgebras are given in the table below: “adm-n1” — 2020/5/14 — 19:35 — page 59 — #67 G. R. Biyogmam, C. Tcheka 59 4-dimensional non-split nilpotent s-Leibniz algebras s-Leibniz algebra g Lie-center ZLie(g) Absolute maximal Lie subalgebra s A12, A14, A15, A17 {x3, x4} {x2, x3, x4} A13, A16 {x3, x4} {x1, x3, x4} Theorem 4.2. Every five dimensional non-split nilpotent s-Leibniz algebra is isomorphic to a Leibniz algebra spanned by {x1, x2, x3, x4} where the nonzero products are given by following: B1: [x1, x2] = x3, [x2, x1] = −x3 + x5, [x1, x3] = x4 = −[x3, x1].. B3: [x1, x2] = x3, [x2, x1] = −x3 + x5, [x2, x2] = x5, [x1, x3] = x4 = −[x3, x1]. C2: [x1, x2] = x3, [x2, x1] = −x3 + x4, [x2, x2] = x5, [x1, x3] = x5 = −[x3, x1]. C4: [x1, x2] = x3, [x2, x1] = −x3 + x5, [x2, x2] = x4, [x1, x3] = x4 = −[x3, x1]. C8: [x1, x1] = x4, [x1, x2] = x3, [x2, x1] = −x3 + x5, [x1, x3] = x4 = −[x3, x1]. D1: [x1, x1] = x3, [x2, x1] = −x4, [x1, x3] = x5. D8: [x1, x1] = x3, [x1, x2] = x4, [x2, x1] = αx4, [x1, x3] = x5, α ∈ C/{−1}. D14: [x1, x1] = x4, [x1, x2] = x3, [x1, x3] = x5. D15: [x1, x1] = x4, [x1, x2] = x3, [x2, x1] = x5, [x1, x3] = x5 D18: [x1, x1] = x4, [x1, x2] = x3, [x2, x1] = x4, [x1, x3] = x5. E1: [x1, x2] = −x3 + x4, [x2, x1] = x3, [x2, x3] = x5, [x3, x2] = −x5, [x1, x4] = x5. E10: [x1, x1] = x4, [x1, x2] = x3, [x2, x1] = −x3, [x2, x3] = x5, [x3, x2] = −x5, [x1, x4] = x5. F1: [x1, x2] = x3, [x2, x1] = −x3 + x5, [x1, x3] = x4, [x3, x1] = −x4, [x2, x3] = x5, [x3, x2] = −x5. F3: [x1, x2] = x3, [x2, x1] = −x3 + x5, [x2, x2] = x5, [x1, x3] = x4, [x3, x1] = −x4, [x2, x3] = x5, [x3, x2] = −x5. G1: [x1, x2] = x3, [x2, x1] = −x3 + x4, [x2, x2] = αx5, [x1, x3] = x4, [x3, x1] = −x4, [x2, x3] = x5, [x3, x2] = −x5, α ∈ C/{−1}. G3: [x1, x1] = αx5, [x1, x2] = x3, [x2, x1] = −x3 +x4 +x5, [x1, x3] = x4, [x3, x1] = −x4, [x2, x3] = x5, [x3, x2] = −x5, α ∈ C/{−1}. H1: [x1, x2] = x3, [x2, x1] = −x3 + x5, [x1, x3] = x4, [x3, x1] = −x4, [x1, x4] = x5, [x4, x1] = −x5. H3: [x1, x2] = x3, [x2, x1] = −x3 + x5, [x2, x2] = x5, [x1, x3] = x4, [x3, x1] = −x4, [x1, x4] = x5, [x4, x1] = −x5. “adm-n1” — 2020/5/14 — 19:35 — page 60 — #68 60 Leibniz algebras H5: [x1, x2] = x3, [x2, x1] = −x3 + x5, [x2, x2] = αx5, [x1, x3] = x4, [x2, x3] = x5, [x3, x2] = −x5, [x3, x1] = −x4, [x1, x4] = x5, [x4, x1] = −x5, α ∈ C. I6: [x1, x2] = x4, [x2, x1] = −x4, [x1, x3] = x5, [x1, x4] = x5, [x4, x1] = −x5. I8: [x1, x2] = x4, [x2, x1] = −x4, [x2, x3] = x5, [x1, x4] = x5, [x4, x1] = −x5. I13: [x1, x2] = x4, [x2, x1] = −x4 + x5, [x2, x3] = −x5, [x3, x2] = x5, [x1, x4] = x5, [x4, x1] = −x5. I14: [x1, x2] = x4, [x2, x1] = −x4, [x2, x3] = αx5, [x3, x2] = x5, [x1, x4] = x5, [x4, x1] = −x5, α ∈ C. I18: [x1, x2] = x4, [x2, x1] = −x4 + x5, [x2, x2] = x5, [x2, x3] = −x5, [x3, x2] = x5, [x1, x4] = x5, [x4, x1] = −x5. J8: [x1, x1] = x4, [x2, x3] = αx5, [x3, x2] = x5, [x1, x4] = x5. J10: [x1, x2] = x4, [x2, x3] = αx5, [x3, x2] = x5, [x1, x4] = x5. K2: [x1, x2] = x4, [x2, x1] = −x4, [x3, x1] = x5. K4: [x1, x2] = x4, [x2, x1] = −x4, [x1, x3] = x5, [x3, x1] = αx5, α ∈ C/{−1}. K5: [x1, x2] = x4, [x2, x1] = −x4 + x5, [x1, x3] = x5, [x3, x1] = −x5. K6: [x1, x2] = x4, [x2, x1] = −x4, [x1, x3] = x5, [x3, x1] = −αx5, [x3, x3] = x5, α ∈ C/{−1}. K9: [x1, x2] = x4, [x2, x1] = −x4, [x1, x3] = x5, [x3, x2] = x5. K12: [x1, x2] = x4, [x2, x1] = −x4 + x5, [x1, x3] = x5, [x3, x1] = −x5, [x2, x3] = x5, [x3, x2] = −x5. L14: [x1, x2] = x4, [x2, x3] = x5. L18: [x1, x2] = αx4, [x2, x1] = x4, [x2, x3] = x5, α ∈ C/{−1}. L35: [x1, x2] = x5, [x2, x2] = x4, [x2, x3] = x5. L36: [x1, x2] = x4, [x2, x1] = −x4, [x2, x2] = x4, [x2, x3] = x5. L42: [x2, x1] = x4, [x1, x3] = x5, [x2, x3] = −x5, [x3, x2] = x5. L44: [x1, x2] = x4, [x2, x1] = αx4, [x2, x3] = βx5, [x3, x2] = x5, α, β ∈ C/{−1}. L45: [x1, x1] = x5, [x1, x2] = x4, [x2, x1] = αx4, [x2, x3] = βx5, [x3, x2] = x5, α ∈ C/{−1}, β ∈ C. L46: [x1, x2] = x4, [x2, x1] = αx4 + x5, [x2, x3] = αx5, [x3, x2] = x5, α ∈ C/{−1}. L50: [x1, x2] = x4, [x2, x1] = αx4, [x2, x2] = x5, [x2, x3] = x5, [x3, x2] = −x5, α ∈ C/{−1}. L55: [x1, x1] = x4, [x2, x1] = x4, [x1, x3] = αx5, [x2, x3] = −x5, [x3, x2] = x5, α ∈ C/{0}. L56: [x1, x1] = x4, [x2, x1] = x4 + x5, [x2, x3] = x5, [x3, x2] = −x5. “adm-n1” — 2020/5/14 — 19:35 — page 61 — #69 G. R. Biyogmam, C. Tcheka 61 L58: [x1, x1] = x4, [x1, x2] = x4, [x2, x1] = −x4, [x1, x3] = βx5, [x2, x3] = −x5, [x3, x2] = x5, β ∈ C/{0}. L60: [x1, x1] = x4, [x1, x2] = x4 + x5, [x2, x1] = αx4, [x2, x3] = −x5, [x3, x2] = x5, α ∈ C. L61: [x1, x1] = x4, [x1, x2] = x4 + x5, [x2, x1] = x4, [x1, x3] = αx5, [x2, x3] = −x5, [x3, x2] = x5, α ∈ C/{−1, 0}. L63: [x1, x1] = x4, [x1, x2] = x4 + x5, [x2, x1] = αx4, [x1, x3] = βx5, [x2, x3] = −x5, [x3, x2] = x5, α ∈ C/{−1, 0}, β ∈ C/{0}, αβ 6= −1, (α+ 1)β 6= −1 L66: [x1, x1] = x4, [x1, x2] = x4, [x2, x1] = x4 + x5, [x1, x3] = −x5, [x2, x3] = −x5, [x3, x2] = x5. L80: [x1, x2] = x4, [x2, x1] = x5, [x2, x3] = x4. L82: [x1, x2] = x4, [x2, x1] = −x4, [x2, x3] = x4, [x3, x2] = x5. L83: [x1, x2] = x4 + 2x5, [x2, x1] = −x5, [x2, x2] = x5, [x2, x3] = x4, [x3, x2] = x5. L89: [x1, x2] = x4, [x2, x1] = −x4 + x5, [x1, x3] = −x5, [x3, x1] = x5, [x2, x3] = x4. L89′: [x1, x2] = x4, [x2, x1] = −x4 + x5, [x1, x3] = γx5, [x3, x1] = x5, [x2, x3] = x4, γ ∈ C/{−1}. L89′′: [x1, x2] = x4 + αx5, [x2, x1] = βx4 + x5, [x1, x3] = −x5, [x3, x1] = x5, [x2, x3] = x4, α ∈ C/{−1}, β ∈ C. L92: [x1, x2] = x4, [x2, x1] = −x4, [x2, x2] = x5, [x1, x3] = −x5, [x3, x1] = x5, [x2, x3] = x4. L92′: [x1, x2] = x4 + αx5, [x2, x1] = βx4, [x2, x2] = x5, [x1, x3] = −x5, [x3, x1] = x5, [x2, x3] = x4, α, β ∈ C with (α, β) 6= (0,−1). L94: [x1, x2] = x4 − 2βx5, [x2, x1] = αx4 + βx5, [x2, x2] = x5, [x1, x3] = −x5, [x3, x1] = x5, [x2, x3] = x4, α ∈ C, β ∈ C/{−1, 0, 1}. L95: [x1, x2] = x4 + αx5, [x2, x1] = βx5, [x2, x2] = x5, [x1, x3] = −x5, [x3, x1] = x5, [x2, x3] = x4, α ∈ C, β ∈ C/{0}, α 6= −2β, β2 +αβ + 1 6= 0. M1: [x1, x2] = x4 − x5, [x2, x1] = −x4 + x5, [x1, x3] = γx5, [x3, x1] = −γx5, [x2, x3] = x4, [x3, x3] = x5, γ ∈ C. M1′: [x1, x2] = x4 − x5, [x2, x1] = −x4 + x5, [x1, x3] = γx5, [x3, x1] = θx5, [x2, x3] = x4, [x3, x3] = x5, γ, θ ∈ C, γ 6= −θ. M2: [x1, x2] = x4, [x2, x1] = −x4, [x1, x3] = θx5, [x3, x1] = −θx5, [x2, x3] = x4, [x3, x3] = x5, θ ∈ C. M2′: [x1, x2] = x4, [x2, x1] = −x4, [x1, x3] = θx5, [x3, x1] = δx5, [x2, x3] = x4, [x3, x3] = x5, δ, θ ∈ C, δ 6= −θ. M2′′: [x1, x2] = x4 + x5, [x2, x1] = −x4 − x5, [x1, x3] = θx5, [x3, x1] = −θx5, [x2, x3] = x4, [x3, x3] = x5, θ ∈ C. “adm-n1” — 2020/5/14 — 19:35 — page 62 — #70 62 Leibniz algebras M2′′′: [x1, x2] = x4 + x5, [x2, x1] = −x4 − x5, [x1, x3] = θx5, [x3, x1] = δx5, [x2, x3] = x4, [x3, x3] = x5, γ, θ ∈ C, δ 6= −θ. M7: [x1, x1] = x4 + αx5, [x1, x2] = γx5, [x2, x1] = −γx5, [x1, x3] = λx5, [x2, x3] = x4, [x3, x2] = −x4, α, γ, λ ∈ C. M7′: [x1, x1] = x4 + αx5, [x1, x2] = βx4 + γx5, [x2, x1] = θx5, [x1, x3] = λx5, [x2, x3] = x4, [x3, x2] = −x4, α, β, γ, λ ∈ C, β 6= 0 or γ 6= −θ. M9: [x1, x1] = x4 + αx5, [x1, x2] = βx4 + γx5, [x3, x1] = x5, [x1, x3] = −x5, [x2, x3] = x4, [x3, x2] = −x4,, α, β, γ ∈ C, β 6= 0 or γ 6= 0. M9′: [x1, x1] = x4 + αx5, [x1, x2] = βx4 + γx5, [x3, x1] = x5, [x1, x3] = δx5, [x2, x3] = x4, [x3, x2] = −x4, α, β, γ ∈ C, δ 6= −1, β 6= 0 or γ 6= 0. M11: [x1, x1] = x4 + αx5, [x1, x2] = βx4 + γx5, [x2, x1] = θx5, [x2, x3] = −x4, [x3, x2] = x4, α, β, γ, θ ∈ C, β 6= 0 or γ 6= −θ. M12: [x1, x1] = x4, [x1, x2] = αx4 + βx5, [x2, x1] = γx5, [x1, x3] = x5, [x2, x3] = −x4, [x3, x2] = x4, α, β, γ, θ ∈ C, α 6= 0 or γ 6= −β. M13: [x1, x1] = x4 + αx5, [x1, x2] = γx5, [x2, x1] = −γx5, [x3, x1] = x5, [x1, x3] = λx5, [x2, x3] = −x4, [x3, x2] = x4, α, γ, λ ∈ C, λ 6= −1. M13′: [x1, x1] = x4 + αx5, [x1, x2] = βx4 + γx5, [x2, x1] = θx5, [x3, x1] = x5, [x1, x3] = λx5, [x2, x3] = −x4, [x3, x2] = x4, α, β, γ, θ, λ ∈ C, λ 6= −1, and β 6= 0 or γ 6= −θ. M15: [x1, x2] = −x4 + γx5, [x2, x1] = x4 − γx5, [x3, x1] = µx5, [x1, x3] = x4 + λx5, [x2, x3] = ωx5, [x3, x2] = x4, γ, µ, λω ∈ C. Proof. The result is obtained by checking each Leibniz algebra of the following theorems in [10]. Again, for the convenience of the reader, we kept the same numbering as in [10], and just differentiated theorems by the Letters as follows: Theorem 4.2.3 for the Bs, Theorem 4.2.5 for the Cs, Theorem 4.2.6 for the Ds, Theorem 4.2.7 for the Es, Theorem 4.2.9 for the Fs, Theorem 4.2.10 for the Gs, Theorem 4.2.11 for the Hs, Theorem 4.3.1 for the Is, Theorem 4.3.2 for the Js, Theorem 4.3.3 for the Ks, Theorem 4.3.4 for the Ls and Ms. The basis of the corresponding Lie-centers and absolute maximal Lie subalgebras are given in the table below: 5-dimensional non-split nilpotent s-Leibniz algebras s-Leibniz algebra g Lie-center ZLie(g) Maximal Lie subalgebra s B1, B3 {x3, x4, x5} {x1, x3, x4, x5} C2, C4 {x3, x4, x5} {x1, x3, x4, x5} C8 {x3, x4, x5} {x2, x3, x4, x5} “adm-n1” — 2020/5/14 — 19:35 — page 63 — #71 G. R. Biyogmam, C. Tcheka 63 5-dimensional non-split nilpotent s-Leibniz algebras s-Leibniz algebra g Lie-center ZLie(g) Maximal Lie subalgebra s D1, D8, D14, D15, D18 {x3, x4, x5} {x2, x3, x4, x5} E1 {x4, x5} {x2, x3, x4, x5} E10 {x2, x3, x5} {x2, x3, x4, x5} F1 {x3, x4, x5} {x1, x3, x4, x5}, {x2, x3, x4, x5} F3 {x3, x4, x5} {x1, x3, x4, x5} G1 {x3, x4, x5} {x1, x3, x4, x5} G3 {x3, x4, x5} {x2, x3, x4, x5} H1 {x3, x4, x5} {x1, x3, x4, x5}, {x2, x3, x4, x5} H3, H5 {x3, x4, x5} {x1, x3, x4, x5} I6 {x2, x4, x5} {x1, x2, x4, x5}, {x2, x3, x4, x5} I8, I14 {x1, x4, x5} {x1, x2, x4, x5}, {x1, x3, x4, x5} I13 {x3, x4, x5} {x1, x3, x4, x5}, {x2, x3, x4, x5} I18 {x3, x4, x5} {x1, x3, x4, x5} J8 {x2, x3, x5} {x2, x3, x4, x5} J10 {x3, x5} {x2, x3, x4, x5} K2 {x2, x4, x5} {x2, x3, x4, x5} K4 {x2, x4, x5} {x1, x2, x4, x5}, {x2, x3, x4, x5} K5 {x3, x4, x5} {x2, x3, x4, x5} K6 {x2, x4, x5} {x1, x2, x4, x5} K9 {x4, x5} {x1, x2, x4, x5} K12 {x3, x4, x5} {x1, x3, x4, x5}, {x2, x3, x4, x5} L14, L16, L35, L44, L46, L50, L80, L83, L89′′, L92′, L94, L95 {x4, x5} {x1, x3, x4, x5} L36, L89, L92 {x1, x4, x5} {x1, x3, x4, x5} L42, L55, L60, L61, L63, L66 {x4, x5} {x2, x3, x4, x5} L58 {x2, x4, x5} {x2, x3, x4, x5} L45, L56 {x3, x4, x5} {x2, x3, x4, x5} “adm-n1” — 2020/5/14 — 19:35 — page 64 — #72 64 Leibniz algebras 5-dimensional non-split nilpotent s-Leibniz algebras s-Leibniz algebra g Lie-center ZLie(g) Maximal Lie subalgebra s L82, L89′, L92 {x1, x4, x5} {x1, x2, x4, x5} M1,M2,M2′′ {x1, x4, x5} {x1, x2, x4, x5} M1′,M2′,M2′′′,M15 {x4, x5} {x1, x2, x4, x5} M7,M13 {x2, x4, x5} {x2, x3, x4, x5} M8,M10,M12,M14 {x4, x5} {x2, x3, x4, x5} M9,M11 {x3, x4, x5} {x2, x3, x4, x5} References [1] R.K. Amayo: Quasi-ideals of Lie algebras II, Proc. Lond. Math. Soc. , 3 (33), (1976), 37-64. [2] Sh. A. Ayupov and B. A. Omirov: On some classes of nilpotent Leibniz algebras, Sibirsk. Mat. Zh., 42 (1), (2001), 18-29. [3] G. R. Biyogmam and J. M. Casas: On Lie-isoclinic Leibniz algebras, J. Algebra 499 (2018), 337-357. [4] G. R. Biyogmam and J. M. Casas: The c-Nilpotent Shur Lie-Multiplier of Leibniz Algebras, J. Geom. Phys. 138 (2019), 55–69. [5] D. Barnes: On Levi’s theorem for Leibniz algebras, Bull. Aust. Math. Soc. 86 (2012), 184-185 [6] J. M. Casas and E. Khmaladze: On Lie-central extensions of Leibniz algebras, RACSAM (2016), DOI 10.1007/s13398-016-0274-6. [7] J. M. Casas and T. Van der Linden: A relative theory of universal central exten- sions, Pré-Publicaçoes do Departamento de Matemàtica, Universidade de Coimbra Preprint Number 09- (2009). [8] J. M. Casas and M. A. Insua: The Schur Lie-multiplier of Leibniz algebras, Quaes- tiones Mathematicae, 41 (2) (2018). [9] J. M. Casas and T. Van der Linden: Universal central extensions in semi-abelian categories, Appl. Categor. Struct. 22 (1) (2014), 253–268. [10] I. Demir, Classification of 5-Dimensional Complex Nilpotent Leibniz Algebras., Ph.D. Thesis, http://www.lib.ncsu.edu/resolver/1840.20/33418, 138 pages. [11] I. Demir, C. Kailash and E. Stitzinger: On classification of four-dimensional nilpotent Leibniz algebras, Comm. Algebra 45 (3) (2017), 1012–1018. [12] I. Demir, C. Kailash and E. Stitzinger: On some structure of Leibniz algebras, in Recent Advances in Representation Theory, Quantum Groups, Algebraic Geom- etry, and Related Topics, Contemporary Mathematics, 623, Amer. Math. Soc., Providence, RI, 41-54 (2014). [13] V. Gorbatsevich: On some structure of Leibniz algebras, arxiv:1302.3345v2. [14] G. Janelidze, L. Màrki and W. Tholen: Semi-abelian categories, J. Pure Appl. Algebra 168 (2002), 367–386. “adm-n1” — 2020/5/14 — 19:35 — page 65 — #73 G. R. Biyogmam, C. Tcheka 65 [15] J.-L. Loday: Cyclic homology, Grundl. Math. Wiss. Bd. 301, Springer (1992). [16] J.-L. Loday: Une version non commutative des algèbres de Lie: les algèbres de Leibniz, L’Enseignement Mathématique 39 (1993), 269–292. [17] D. Towers: Lie algebras all of whose maximal subalgebras have codimension one, Proc. Edin. Math. Soc. 24 (1981), 217–219. [18] D. Towers: Maximal subalgebras of Lie algebras containing Engel subalgebras, J. Pure Appl. Algebra 216 (2012), 688–693. Contact information G. R. Biyogmam Department of Mathematics, Georgia College & State University, Campus Box 17 Milledgeville, GA 31061-0490 E-Mail(s): guy.biyogmam@gcsu.edu Calvin Tcheka Department of Mathematics, University of Dschang, Dschang, Cameroun E-Mail(s): jtcheka@gmail.com Received by the editors: 15.05.2018. G. R. Biyogmam, C. Tcheka