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Embarrassingly I fail to see why the following definition works (see e.g. 1)

Consider the continuous function $U:(0,1] \to GL(V)$. If the limit $\lim_{\epsilon \to 0} [x,y]_\epsilon=\lim_{\epsilon \to 0} U_\epsilon^{-1} [U_\epsilon x,U_\epsilon y]_\epsilon=[x,y]_0$ exists for all $x,y \in V$ then $[-,-]$ is a well-defined Lie bracket.

It is obvious to me why it works for any $\epsilon >0$, but as soon as $U$ is singular I do not see why all the properties of a Lie algebra are still satisfied.

E.g., Why has to be that $[x,y]_0 - [y,x]_0 =0$?

ungerade
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1 Answers1

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A Lie algebra contraction is a special case of a Lie algebra degeneration. For a Lie algebra law $\lambda$, the orbit under the above $GL(V)$-action is denoted by $O(\lambda)$. It is easy to see that a contraction of $\lambda$ lies in the orbit closure of $O(\lambda)$. By a result of Borel, the orbits are constructible sets, and hence the orbit closure with respect to the Euclidean topology is the same as the closure with respect to the Zariski topology. In other words, all invariant polynomial conditions which hold in $O(\lambda)$ also hold in the obit closure. In particular, the Jacobi identity and skew-symmetry are such polynomial conditions. Hence the law $\lambda_0\in\overline{O(\lambda)}$, given by $\lambda_0(x,y)=[x,y]_0$ is again a Lie algebra law.

For details and references see this paper.

Dietrich Burde
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