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→Diagonalizable matrices: simpler and more accurate |
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* Using scalar Taylor expansion for <math>f(a+\eta b)</math> and replacing scalars with matrices at the end :
:: <math>\begin{
f(a+\eta b) &=
&=
&\to
\end{
The scalar expression assumes commutativity while the matrix expression does not, and thus they cannot be equated directly unless <math>[A,B]=0</math>. For some ''f''(''x'') this can be dealt with using the same method as scalar Taylor series. For example, <math display="inline">f(x) = \frac{1}{x}</math>. If <math>A^{-1}</math> exists then <math>f(A+\eta B) = f(\mathbb{I} + \eta A^{-1}B)f(A)</math>. The expansion of the first term then follows the power series given above,
:<math>f(\mathbb{I} + \eta A^{-1}B) = \mathbb{I} - \eta A^{-1}B + (-\eta A^{-1}B)^
The convergence criteria of the power series then apply, requiring <math>\Vert \eta A^{-1}B \Vert</math> to be sufficiently small under the appropriate matrix norm. For more general problems, which cannot be rewritten in such a way that the two matrices commute, the ordering of matrix products produced by repeated application of the Leibniz rule must be tracked.
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