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Lie algebra theory is to a large extend the classification of the semisimple Lie algebras which are direct sums of the simple algebras listed in the previous paragraph, i.e. to show that those are all simple Lie algebras there are. Their counterpart are solvable Lie algebras, e.g. the Heisenberg algebra ##\mathfrak{H}=\langle X,Y,Z\,:\, [X,Y]=Z\rangle\,.## They have less structure each and are less structured as a whole as well. In physics, they don't play such a prominent role as simple Lie algebras do, although the reader might have recognized, that e.g. the Poincaré algebra - the tangent space of the Poincaré group at its identity matrix - wasn't among the simple ones. It isn't among the solvable Lie algebras either like ##\mathfrak{H}## is, so what is it then? It is the tangent space of the Lorentz group plus translations: something orthogonal plus something Abelian (solvable).
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