lines 6-109 of file: xrst/theory/log_reverse.xrst {xrst_begin log_reverse} Logarithm Function Reverse Mode Theory ###################################### We use the reverse theory :ref:`standard math function` definition for the functions :math:`H` and :math:`G`. The zero order forward mode formula for the :ref:`logarithm` is .. math:: z^{(0)} = F( x^{(0)} ) and for :math:`j > 0`, .. math:: z^{(j)} = \frac{1}{ \bar{b} + x^{(0)} } \frac{1}{j} \left( j x^{(j)} - \sum_{k=1}^{j-1} k z^{(k)} x^{(j-k)} \right) where .. math:: \bar{b} = \left\{ \begin{array}{ll} 0 & \R{if} \; F(x) = \R{log}(x) \\ 1 & \R{if} \; F(x) = \R{log1p}(x) \end{array} \right. We note that for :math:`j > 0` .. math:: :nowrap: \begin{eqnarray} \D{ z^{(j)} } { x^{(0)} } & = & - \frac{1}{ \bar{b} + x^{(0)} } \frac{1}{ \bar{b} + x^{(0)} } \frac{1}{j} \left( j x^{(j)} - \sum_{k=1}^{j-1} k z^{(k)} x^{(j-k)} \right) \\ & = & - \frac{z^{(j)}}{ \bar{b} + x^{(0)} } \end{eqnarray} Removing the zero order partials are given by .. math:: :nowrap: \begin{eqnarray} \D{H}{ x^{(0)} } & = & \D{G}{ x^{(0)} } + \D{G}{ z^{(0)} } \D{ z^{(0)} }{ x^{(0)} } \\ & = & \D{G}{ x^{(0)} } + \D{G}{ z^{(0)} } \frac{1}{ \bar{b} + x^{(0)} } \end{eqnarray} For orders :math:`j > 0` and for :math:`k = 1 , \ldots , j-1` .. math:: :nowrap: \begin{eqnarray} \D{H}{ x^{(0)} } & = & \D{G}{ x^{(0)} } + \D{G}{ z^{(j)} } \D{ z^{(j)} }{ x^{(0)} } \\ & = & \D{G}{ x^{(0)} } - \D{G}{ z^{(j)} } \frac{ z^{(j)} }{ \bar{b} + x^{(0)} } \\ \D{H}{ x^{(j)} } & = & \D{G}{ x^{(j)} } + \D{G}{ z^{(j)} } \D{ z^{(j)} }{ x^{(j)} } \\ & = & \D{G}{ x^{(j)} } + \D{G}{ z^{(j)} } \frac{1}{ \bar{b} + x^{(0)} } \\ \D{H}{ x^{(j-k)} } & = & \D{G}{ x^{(j-k)} } - \D{G}{ z^{(j)} } \frac{1}{ \bar{b} + x^{(0)} } \frac{k}{j} z^{(k)} \\ \D{H}{ z^{(k)} } & = & \D{G}{ z^{(k)} } - \D{G}{ z^{(j)} } \frac{1}{ \bar{b} + x^{(0)} } \frac{k}{j} x^{(j-k)} \end{eqnarray} {xrst_end log_reverse}