1.2.7 Tangent Spaces
Lie matrix groups are smooth manifolds that tend to be curved objects, but it turns out that the characteristic mathematics of a matrix group can be encapsulated in the flat space, that is, the tangent space The tangent space of a group consists of smooth paths moving through the identity . Smooth defines that derivatives of these paths exist and if , then is called the tangent vector of at .1 Determining the matrix derivative of centered at the identity to evaluate the smooth paths through is straightforward for the general and special linear groups and The tangent vectors of these groups will take the form of a skew-symmetric matrix defined for , as
For , a square Lie algebra matrix, the exponential mapping yields a smooth path via differentiability, with a tangent vector at the identity. For the group we set a smooth path to represent
and by being smooth, there exists a derivative of that has the following form
Evaluating the paths through the identity means considering when , which yields the tangent vectors that comprise the Lie algebra
For the sake of clarity, the operator notation in the following theorem acting on , is the following: the transpose is denoted as , the conjugate as , and the conjugate transpose is and is equivalent to
Theorem (1.2.145) – The tangent vectors at , for the groups are matrices of the following forms:
- .
Proof – The matrices by way of their orthogonality, satisfy For representing a smooth path that originates at the identity , we evaluate the derivative of
The product rule holds for this derivative expression, given the identity, , is a constant, and the derivative of a constant is zero, . Solving by the product rule yields
and as both , for the above becomes
Therefore, any tangent vector will satisfy the skew-symmetry condition
The matrices , by way of their unitary conditions, satisfy For , a smooth path that originates at the identity , we evaluate the derivative of
The product rule holds for this derivative expression, given the identity, , is a constant, and the derivative of a constant is zero, . Solving by the product rule yields
and as both , for , the above becomes
Therefore, any tangent vector, , will satisfy the skew-symmetry condition, The matrices , by way of their quaternion conditions, satisfy For , a smooth path that originates at the identity, , we evaluate the derivative of
The product rule holds for this derivative expression, given the identity, , is a constant, and the derivative of a constant is zero, . Solving by the product rule yields
and as both , for , the above becomes
Therefore, any tangent vector , will satisfy the skew-symmetry condition
For the skew-symmetry condition , the elements along the diagonals of will be 0, and the transpose of each element in satisfies -. For the cases of the groups, the matrices are called skew-Hermitian, where the matrix entries in satisfy -, and the diagonal entries of are purely imaginary. It should be noted that some tangent spaces at the identity can be shared for specific groups and their subgroups; a case in point is the groups and their subgroups.
- Stillwell, John, "Naive Lie Theory", Springer, 2008