lines 6-79 of file: xrst/theory/atan_forward.xrst

{xrst_begin atan_forward}

Inverse Tangent and Hyperbolic Tangent Forward Mode Theory
##########################################################

Derivatives
***********

.. math::
   :nowrap:

   \begin{eqnarray}
   \R{atan}^{(1)} (x)  & = & 1 / ( 1 + x * x )
   \\
   \R{atanh}^{(1)} (x) & = & 1 / ( 1 - x * x )
   \end{eqnarray}

If :math:`F(x)` is :math:`\R{atan} (x)` or :math:`\R{atanh} (x)`,
the corresponding derivative satisfies the equation

.. math::

   (1 \pm x * x ) * F^{(1)} (x) - 0 * F (x)  = 1

and in the
:ref:`standard math function differential equation<forward_theory@Standard Math Functions@Differential Equation>` ,
:math:`A(x) = 0`,
:math:`B(x) = 1 \pm x * x`,
and :math:`D(x) = 1`.
We use :math:`a`, :math:`b`, :math:`d` and :math:`z` to denote the
Taylor coefficients for
:math:`A [ X (t) ]`,
:math:`B [ X (t) ]`,
:math:`D [ X (t) ]`,
and :math:`F [ X(t) ]` respectively.

Taylor Coefficients Recursion
*****************************
For :math:`j = 0 , 1, \ldots`,

.. math::
   :nowrap:

   \begin{eqnarray}
   z^{(0)} & = & F( x^{(0)} )
   \\
   b^{(j)}
   & = &  \left\{ \begin{array}{ll}
      1 \pm x^{(0)} * x^{(0)}            & {\rm if} \; j = 0 \\
      \pm \sum_{k=0}^j x^{(k)} x^{(j-k)} & {\rm otherwise}
   \end{array} \right.
   \\
   e^{(j)}
   & = & d^{(j)} + \sum_{k=0}^{j} a^{(j-k)} * z^{(k)}
   \\
   & = & \left\{ \begin{array}{ll}
      1 & {\rm if} \; j = 0 \\
      0 & {\rm otherwise}
   \end{array} \right.
   \\
   z^{(j+1)} & = & \frac{1}{j+1} \frac{1}{ b^{(0)} }
   \left(
      \sum_{k=0}^j e^{(k)} (j+1-k) x^{(j+1-k)}
      - \sum_{k=1}^j b^{(k)} (j+1-k) z^{(j+1-k)}
   \right)
   \\
   z^{(j+1)} & = & \frac{1}{j+1} \frac{1}{ b^{(0)} }
   \left(
      (j+1) x^{(j+1)}
      - \sum_{k=1}^j k z^{(k)}  b^{(j+1-k)}
   \right)
   \end{eqnarray}

{xrst_end atan_forward}