Classification of low-dimensional real Lie algebras

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This mathematics-related list provides Mubarakzyanov's classification of low-dimensional real Lie algebras, published in Russian in 1963.[1] It complements the article on Lie algebra in the area of abstract algebra.

An English version and review of this classification was published by Popovych et al.[2] in 2003.

Mubarakzyanov's Classification

Let 𝔤n be n-dimensional Lie algebra over the field of real numbers with generators e1,…,en, n≤4.[clarification needed] For each algebra 𝔤 we adduce only non-zero commutators between basis elements.

One-dimensional

Two-dimensional

  • 2𝔤1, abelian ℝ2;
  • 𝔤2.1, solvable 𝔞𝔣𝔣(1)={(ab00):a,b∈ℝ},
[e1,e2]=e1.

Three-dimensional

  • 3𝔤1, abelian, Bianchi I;
  • 𝔤2.1⊕𝔤1, decomposable solvable, Bianchi III;
  • 𝔤3.1, Heisenberg–Weyl algebra, nilpotent, Bianchi II,
[e2,e3]=e1;
  • 𝔤3.2, solvable, Bianchi IV,
[e1,e3]=e1,[e2,e3]=e1+e2;
  • 𝔤3.3, solvable, Bianchi V,
[e1,e3]=e1,[e2,e3]=e2;
[e1,e3]=e1,[e2,e3]=αe2,−1≤α<1,α≠0;
  • 𝔤3.5, solvable, Bianchi VII,
[e1,e3]=βe1−e2,[e2,e3]=e1+βe2,β≥0;
  • 𝔤3.6, simple, Bianchi VIII, 𝔰𝔩(2,ℝ),
[e1,e2]=e1,[e2,e3]=e3,[e1,e3]=2e2;
  • 𝔤3.7, simple, Bianchi IX, 𝔰𝔬(3),
[e2,e3]=e1,[e3,e1]=e2,[e1,e2]=e3.

Algebra 𝔤3.3 can be considered as an extreme case of 𝔤3.5, when β→∞, forming contraction of Lie algebra.

Over the field ℂ algebras 𝔤3.5, 𝔤3.7 are isomorphic to 𝔤3.4 and 𝔤3.6, respectively.

Four-dimensional

  • 4𝔤1, abelian;
  • 𝔤2.1⊕2𝔤1, decomposable solvable,
[e1,e2]=e1;
  • 2𝔤2.1, decomposable solvable,
[e1,e2]=e1[e3,e4]=e3;
  • 𝔤3.1⊕𝔤1, decomposable nilpotent,
[e2,e3]=e1;
  • 𝔤3.2⊕𝔤1, decomposable solvable,
[e1,e3]=e1,[e2,e3]=e1+e2;
  • 𝔤3.3⊕𝔤1, decomposable solvable,
[e1,e3]=e1,[e2,e3]=e2;
  • 𝔤3.4⊕𝔤1, decomposable solvable,
[e1,e3]=e1,[e2,e3]=αe2,−1≤α<1,α≠0;
  • 𝔤3.5⊕𝔤1, decomposable solvable,
[e1,e3]=βe1−e2[e2,e3]=e1+βe2,β≥0;
  • 𝔤3.6⊕𝔤1, unsolvable,
[e1,e2]=e1,[e2,e3]=e3,[e1,e3]=2e2;
  • 𝔤3.7⊕𝔤1, unsolvable,
[e1,e2]=e3,[e2,e3]=e1,[e3,e1]=e2;
  • 𝔤4.1, indecomposable nilpotent,
[e2,e4]=e1,[e3,e4]=e2;
  • 𝔤4.2, indecomposable solvable,
[e1,e4]=βe1,[e2,e4]=e2,[e3,e4]=e2+e3,β≠0;
  • 𝔤4.3, indecomposable solvable,
[e1,e4]=e1,[e3,e4]=e2;
  • 𝔤4.4, indecomposable solvable,
[e1,e4]=e1,[e2,e4]=e1+e2,[e3,e4]=e2+e3;
  • 𝔤4.5, indecomposable solvable,
[e1,e4]=αe1,[e2,e4]=βe2,[e3,e4]=γe3,αβγ≠0;
  • 𝔤4.6, indecomposable solvable,
[e1,e4]=αe1,[e2,e4]=βe2−e3,[e3,e4]=e2+βe3,α>0;
  • 𝔤4.7, indecomposable solvable,
[e2,e3]=e1,[e1,e4]=2e1,[e2,e4]=e2,[e3,e4]=e2+e3;
  • 𝔤4.8, indecomposable solvable,
[e2,e3]=e1,[e1,e4]=(1+β)e1,[e2,e4]=e2,[e3,e4]=βe3,−1≤β≤1;
  • 𝔤4.9, indecomposable solvable,
[e2,e3]=e1,[e1,e4]=2αe1,[e2,e4]=αe2−e3,[e3,e4]=e2+αe3,α≥0;
  • 𝔤4.10, indecomposable solvable,
[e1,e3]=e1,[e2,e3]=e2,[e1,e4]=−e2,[e2,e4]=e1.

Algebra 𝔤4.3 can be considered as an extreme case of 𝔤4.2, when β→0, forming contraction of Lie algebra.

Over the field ℂ algebras 𝔤3.5⊕𝔤1, 𝔤3.7⊕𝔤1, 𝔤4.6, 𝔤4.9, 𝔤4.10 are isomorphic to 𝔤3.4⊕𝔤1, 𝔤3.6⊕𝔤1, 𝔤4.5, 𝔤4.8, 2𝔤2.1, respectively.

See also

Notes

References