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On the Derived Length of Lie Solvable Group Algebras

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1.2 ASSOCIATED LIE ALGEBRA OF GROUP ALGEBRAS 5<br />

Evidently, γ2(G) coincides with <strong>the</strong> commutator subgroup G ′ . For<br />

H ⊆ G we will denote by CG(H) <strong>the</strong> centralizer <strong>of</strong> <strong>the</strong> subset H in G.<br />

Fur<strong>the</strong>rmore, denote by Cn <strong>the</strong> cyclic group <strong>of</strong> order n and by Cg <strong>the</strong><br />

conjugacy class including <strong>the</strong> element g ∈ G.<br />

The upper integral part <strong>of</strong> a real number r is denoted by ⌈r⌉.<br />

1.2 Associated <strong>Lie</strong> algebra <strong>of</strong> group algebras<br />

Let (L, +) be a vector space over <strong>the</strong> field F and assume that a<br />

second binary operation [a, b] is defined in L and <strong>the</strong> identities<br />

• α[a, b] = [αa, b] = [a, αb];<br />

• [a + b, c] = [a, c] + [b, c] and [a, b + c] = [a, b] + [a, c];<br />

• [a, a] = 0;<br />

• [a, b], c + [b, c], a + [c, a], b = 0<br />

hold for all a, b, c ∈ L and α ∈ F . Then we say that L is a <strong>Lie</strong> algebra<br />

over <strong>the</strong> field F .<br />

Let A be an associative algebra over <strong>the</strong> field F and x, y ∈ A. The<br />

element [x, y] = xy − yx will be called <strong>the</strong> <strong>Lie</strong> commutator <strong>of</strong> x and y.<br />

Let us introduce in A <strong>the</strong> new operation [x, y] = xy − yx. Then A is<br />

a <strong>Lie</strong> algebra with respect to <strong>the</strong> operations + and [ , ], which is said<br />

to be <strong>the</strong> associated <strong>Lie</strong> algebra <strong>of</strong> A.<br />

For <strong>the</strong> sequence (xi) <strong>of</strong> elements <strong>of</strong> A we define <strong>the</strong> left n-normed<br />

<strong>Lie</strong> commutator by induction as<br />

[x1, x2, . . . , xn] = <br />

[x1, x2, . . . , xn−1], xn .<br />

We shall use freely <strong>the</strong> identities<br />

[x, yz] = [x, y]z + y[x, z], [xy, z] = x[y, z] + [x, z]y,

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