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 law
The 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 gives
so
The 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 , and
The largest group is therefore
the 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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