A Lie group is a smooth manifold equipped with smooth maps , , and , , for which multiplication is associative, there is an identity , and every has the inverse . In equations,Thus the group axioms and the smooth structure are compatible.
In a coordinate chart centred at the identity, smooth multiplication has a local group lawThe identity gives and , while associativity gives the functional equation . Smooth inversion determines coordinates with . Changes of local coordinates alter the symmetric part of , whereas its antisymmetric part supplies the coordinate-independent Lie bracket on the tangent space at the identity.
Write in a matrix representation and . Direct multiplication givessoThe cancellation of the constant and linear terms explains why the group commutator first detects the Lie bracket at quadratic order.
The matrix is invertible precisely when , andThe largest group is thereforethe real affine group under .
As a smooth manifold, . It has two connected components, distinguished by the sign of : each of and is connected, and a continuous path in cannot cross .
The defining two-dimensional group representation is reducible, because the line is an invariant subspace:For , the complementary line is not invariant, so this representation need not split as a direct sum of one-dimensional representations.
The map is a surjective group homomorphism with kernel , so is a normal subgroup and . The subgroup is not normal: for a translation ,which leaves when and . Finally, is a surjective homomorphism onto with kernel , so and the quotient group .
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