\(\newcommand{\W}[1]{ \; #1 \; }\) \(\newcommand{\R}[1]{ {\rm #1} }\) \(\newcommand{\B}[1]{ {\bf #1} }\) \(\newcommand{\D}[2]{ \frac{\partial #1}{\partial #2} }\) \(\newcommand{\DD}[3]{ \frac{\partial^2 #1}{\partial #2 \partial #3} }\) \(\newcommand{\Dpow}[2]{ \frac{\partial^{#1}}{\partial {#2}^{#1}} }\) \(\newcommand{\dpow}[2]{ \frac{ {\rm d}^{#1}}{{\rm d}\, {#2}^{#1}} }\)
erf_reverse¶
View page sourceError Function Reverse Mode Theory¶
Notation¶
We use the reverse theory standard math function definition for the functions \(H\) and \(G\).
Positive Orders Z(t)¶
For order \(j > 0\), suppose that \(H\) is the same as \(G\).
For \(k = 1 , \ldots , j\), the partial of \(H\) with respect to \(x^{(k)}\) is given by
For \(k = 1 , \ldots , j\) The partial of \(H\) with respect to \(y^{j-k}\), is given by
Order Zero Z(t)¶
The \(z^{(0)}\) coefficient is expressed as a function of the Taylor coefficients for \(X(t)\) and \(Y(t)\) as follows: In this case,