For every vector , the Hermitian inner product gives
The norm vanishes only on the zero vector, so for every and . In contrast,
is a nonzero nilpotent matrix. Multiplying a matrix by its conjugate transpose detects column norms; multiplying it by itself has no corresponding positivity property.
The cyclic property of the trace implies
Taking the matrix trace of the asserted equality therefore gives . For a positive integer over the complex numbers this requires . It is also sufficient: choose , or any two commuting matrices. Thus a finite-dimensional operator commutator cannot be a nonzero scalar multiple of the identity matrix.
The anticommutator condition and invertibility give the matrix similarities
Since matrix trace is invariant under matrix similarity,
Hence . Taking determinants in the first matrix similarity also gives
Since is an invertible matrix, , and . In terms of eigenvalues, the same matrix similarity pairs each nonzero eigenvalue with , with the same algebraic multiplicity, so an odd number of them is impossible.
Termwise differentiation of the absolutely convergent matrix exponential series gives
Because and commute, also commutes with every power of and hence with . The product rule therefore gives
Direct differentiation gives , and both initial values are . The uniqueness theorem for ordinary differential equations, applied to the finitely many matrix entries, implies . One can see uniqueness directly: the difference obeys and , so
and the product is identically zero. At this yields
Let . The product rule and differentiation of the matrix exponential give
where brackets are the operator commutator. Evaluating at zero gives , and . The Taylor series at zero is consequently
In particular , which also follows by multiplying the two matrix exponential series through quadratic order. For fixed finite matrices the remainder has the stated Big O notation in any matrix norm.

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