The trace of an square matrix
is defined to be
(1)
|
i.e., the sum of the diagonal elements. The matrix trace is implemented in the Wolfram Language as Tr[list]. In group theory, traces are known as "group characters."
For square matrices and
,
it is true that
(2)
| |||
(3)
| |||
(4)
|
(Lang 1987, p. 40), where denotes the transpose. The
trace is also invariant under a similarity
transformation
(5)
|
(Lang 1987, p. 64). Since
(6)
|
(where Einstein summation is used here to sum over repeated indices), it follows that
(7)
| |||
(8)
| |||
(9)
| |||
(10)
| |||
(11)
|
where
is the Kronecker delta.
The trace of a product of two square matrices is independent of the order of the multiplication since
(12)
| |||
(13)
| |||
(14)
| |||
(15)
| |||
(16)
|
(again using Einstein summation). Therefore, the trace of the commutator of and
is given by
(17)
|
The trace of a product of three or more square matrices, on the other hand, is invariant only under cyclic permutations of the order of multiplication of the matrices, by a similar argument.
The product of a symmetric and an antisymmetric matrix has zero trace,
(18)
|
The value of the trace for a nonsingular matrix can be found using the fact that
the matrix can always be transformed to a coordinate system where the z-axis
lies along the axis of rotation. In the new coordinate system (which is assumed to
also have been appropriately rescaled), the matrix is
(19)
|
so the trace is
(20)
|
where
is interpreted as Einstein summation notation.