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This article is meant to provide a quick reference guide to Lie algebras: the terminology, important theorems, and a brief overview of the subject. Physicists usually call the elements of Lie algebras generators, as for them they are merely differentials of trajectories, tangent vector fields generated by some operators. Thus the distinction between Lie groups and Lie algebras sometimes gets lost. It is the distinction between manifolds and their tangent spaces. If terms as commutator, adjoint, or representation, in general, are used, which apply to both, it is often unclear which of them is meant. The underlying connection is Noether's theorem, which establishes a correspondence between physical invariants and symmetric groups, Lie groups. The approximation of curved objects - the Lie group elements - by first-order approximations - the Lie algebra elements - is a standard procedure in physics, which might partially explain the neglect. However, the following lays the emphasis on the algebra part from a terminological point of view. The corresponding concept for groups will be named whenever there is an appropriate one. I cannot write another textbook about Lie algebras here, and there is no need to, as there are already many excellent ones! Instead, we will focus on the definitions and theorems, driven by the importance Lie algebras have to physics.
Lie algebras are algebras, are vector spaces. They have an internal multiplication, the commutators, as well as a scalar multiplication by elements of the underlying field - and right in the middle of some common misconceptions we are.
Continue reading ...
Lie algebras are algebras, are vector spaces. They have an internal multiplication, the commutators, as well as a scalar multiplication by elements of the underlying field - and right in the middle of some common misconceptions we are.
Continue reading ...
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