\documentclass{article}

% Use the Cactus ThornGuide style file
% (Automatically used from Cactus distribution, if you have a 
%  thorn without the Cactus Flesh download this from the Cactus
%  homepage at www.cactuscode.org)
\usepackage{../../../../doc/latex/cactus}

\begin{document}

\author{Gabrielle Allen} 
\title{Extracting Gravitational Waves and Other Quantities from Numerical Spacetimes}

\date{\today}

\maketitle

% START CACTUS THORNGUIDE

% Add all definitions used in this documentation here 
\def\a   {\alpha}
\def\b   {\beta}
\def\p   {\phi}
\def\t   {\theta}
\def\Y   {Y_{lm}}
\def\Ys  {Y^*_{lm}}
\def\Yt  {Y_{lm,\theta}}
\def\Ytt {Y_{lm,\theta\theta}}
\def\Ytp {Y_{lm,\theta\phi}}
\def\Yp  {Y_{lm,\phi}}
\def\Ypp {Y_{lm,\phi\phi}}
\def\Yz  {Y_{l0}}
\def\Yzt {Y_{l0,\theta}}
\def\Yztt{Y_{l0,\theta\theta}}
\def\c   {\cos\theta}
\def\s   {\sin\theta}

\begin{abstract}

\end{abstract}

\textbf{NB: This documentation is taken from the Extract thorn on which WaveExtractL is based. There may be some differences between WaveExtractL and Extract, which are not documented here.}

\section{Introduction}

Thorn Extract calculates first order gauge invariant waveforms from a
numerical spacetime, under the basic assumption that, at the spheres
of extract the spacetime is approximately Schwarzschild. In addition,
other quantities such as mass, angular momentum and spin can be
determined.

This thorn should not be used blindly, it will always return some
waveform, however it is up to the user to determine whether this is
the appropriate expected first order gauge invariant waveform.

\section{Physical System}

\subsection{Wave Forms}

Assume a spacetime $g_{\alpha\beta}$ which can be written as a Schwarzschild 
background $g_{\alpha\beta}^{Schwarz}$ with perturbations $h_{\alpha\beta}$:
%
\begin{equation}
g_{\alpha\beta} = g^{Schwarz}_{\alpha\beta} + h_{\alpha\beta}
\end{equation}
with
%
\begin{equation}
\{g^{Schwarz}_{\alpha\beta}\}(t,r,\theta,\phi) = 
\left( \begin{array}{cccc}
 -S & 0      & 0   & 0                \\
 0  & S^{-1} & 0   & 0                \\
 0  & 0      & r^2 & 0                \\
 0  & 0      & 0   & r^2 \sin^2\theta
\end{array}\right)
\qquad
S(r)=1-\frac{2M}{r}
\end{equation}
%
The 3-metric perturbations $\gamma_{ij}$ can be decomposed using tensor
harmonics into  $\gamma_{ij}^{lm}(t,r)$ where
$$
  \gamma_{ij}(t,r,\theta,\phi)=\sum_{l=0}^\infty \sum_{m=-l}^l
                       \gamma_{ij}^{lm}(t,r)
$$
%
and
%
$$
  \gamma_{ij}(t,r,\t,\p) = \sum_{k=0}^6 p_k(t,r) {\bf V}_k(\t,\p)
$$
where $\{{\bf V}_k\}$ is some basis for tensors on a 2-sphere
in 3-D Euclidean space.
%
%
%
Working with the Regge-Wheeler basis (see Section~\ref{reggewheeler})
the 3-metric is then expanded in terms of the (six) standard
Regge-Wheeler functions $\{c_1^{\times lm}, c_2^{\times lm},
h_1^{+lm}, H_2^{+lm}, K^{+lm},
G^{+lm}\}$~\cite{regge},~\cite{moncrief74}. Where each of the
functions is either {\it odd} ($\times$) or {\it even} ($+$)
parity. The decomposition is then written
%
\begin{eqnarray}
\gamma_{ij}^{lm} & = & c_1^{\times lm}(\hat{e}_1)_{ij}^{lm}
                   +   c_2^{\times lm}(\hat{e}_2)_{ij}^{lm} 
\nonumber\\
                 & + & h_1^{+lm}(\hat{f}_1)_{ij}^{lm} 
                   +   A^2 H_2^{+lm}(\hat{f}_2)_{ij}^{lm}
                   +   R^2 K^{+lm}(\hat{f}_3)_{ij}^{lm}
                   +   R^2 G^{+lm}(\hat{f}_4)_{ij}^{lm}
\end{eqnarray}
%
which we can write in an expanded form as 
%
\begin{eqnarray}
\gamma_{rr}^{lm} 
  & = & A^2 H_2^{+lm} \Y 
\\
\gamma_{r\t}^{lm} 
  & = & - c_1^{\times lm} \frac{1}{\s} \Yp+h_1^{+lm}\Yt 
\\
\gamma_{r\p}^{lm} 
  & = & c_1^{\times lm} \s \Yt+ h_1^{+lm}\Yp 
\\
\gamma_{\t\t}^{lm} 
  & = & c_2^{\times lm}\frac{1}{\s}(\Ytp-\cot\t \Yp) 
      + R^2 K^{+lm}\Y + R^2 G^{+lm}    \Ytt 
\\
\gamma_{\t\p}^{lm} 
  & = & -c_2^{\times lm}\s \frac{1}{2} 
  \left(
  \Ytt-\cot\t \Yt-\frac{1}{\sin^2\theta}\Y \right)
  + R^2 G^{+lm}(\Ytp-\cot\t \Yp)
\\
\gamma_{\p\p}^{lm}
  & = &  -\s c_2^{\times lm} (\Ytp - \cot\t \Yp)
        +R^2 K^{+lm}\sin^2\t \Y
        +R^2 G^{+lm} (\Ypp+\s\c \Yt)
\end{eqnarray}
%
A similar decomposition allows the four gauge components of the
4-metric to be written in terms of {\it three} even-parity variables
$\{H_0,H_1,h_0\}$ and the {\it one} odd-parity variable $\{c_0\}$
%
\begin{eqnarray}
  g_{tt}^{lm} & = & N^2 H_0^{+lm} \Y 
\\
  g_{tr}^{lm} & = & H_1^{+lm} \Y
\\
  g_{t\t}^{lm} & = & h_0^{+lm} \Yt - c_0^{\times lm}\frac{1}{\s}\Yp
\\
  g_{t\p}^{lm} & = & h_0^{+lm} \Yp + c_0^{\times lm} \s \Yt
\end{eqnarray} 
%        
Also from $g_{tt}=-\alpha^2+\beta_i\beta^i$ we have
%
\begin{equation}
  \alpha^{lm} = -\frac{1}{2}NH_0^{+lm}Y_{lm}
\end{equation}
%
It is useful to also write this with the perturbation split into even and
odd parity parts:
$$
g_{\alpha\beta} = {g}^{background}_{\alpha\beta} +
   \sum_{l,m} g^{lm,odd}_{\alpha\beta}
+\sum_{l,m} g^{lm,even}_{\alpha\beta}
$$
where (dropping some superscripts)
\begin{eqnarray*}
\{g_{\alpha\beta}^{odd}\}
&=&
\left( 
\begin{array}{cccc}
0 & 0 &  - c_0\frac{1}{\s}\Yp
    & c_0 \s \Yt
\\
. & 0 & - c_1\frac{1}{\s} \Yp
  & c_1 \s \Yt
\\
. & . & c_2\frac{1}{\s}(\Ytp-\cot\t \Yp)  
  & c_2\frac{1}{2} \left(\frac{1}{\s}
          \Ypp+\c\Yt-\s\Ytt\right)
\\
.&.&.&c_2 (-\s \Ytp+\c \Yp)
\end{array}
\right)
\\
\{g_{\alpha\beta}^{even}\}
&=&
\left( 
\begin{array}{cccc}
N^2 H_0\Y & H_1\Y       & h_0\Yt          & h_0 \Yp             \\ 
.       & A^2H_2\Y & h_1\Yt          & h_1 \Yp             \\
.       & .           & R^2K\Y+r^2G\Ytt & R^2(\Ytp-\cot\t\Yp) \\
.       & .           & .                & R^2 K\sin^2\t\Y+R^2G(\Ypp+\s\c\Yt)
\end{array}
\right)
\end{eqnarray*}

Now, for such a Schwarzschild background we can define two (and only two)
unconstrained gauge invariant quantities 
  $Q^{\times}_{lm}=Q^{\times}_{lm}(c_1^{\times lm},c_2^{\times lm})$ 
and
  $Q^{+}_{lm}=Q^{+}_{lm}(K^{+ lm},G^{+ lm},H_2^{+lm},h_1^{+lm})$, 
which from
\cite{abrahams96a} are
\begin{eqnarray}
Q^{\times}_{lm} 
  & = & \sqrt{\frac{2(l+2)!}{(l-2)!}}\left[c_1^{\times lm}
        + \frac{1}{2}\left(\partial_r c_2^{\times lm} - \frac{2}{r}
        c_2^{\times lm}\right)\right] \frac{S}{r}
\\
Q^{+}_{lm}
  & = & \frac{1}{\Lambda}\sqrt{\frac{2(l-1)(l+2)}{l(l+1)}}
        (4rS^2 k_2+l(l+1)r k_1) 
\\
  & \equiv &
        \frac{1}{\Lambda}\sqrt{\frac{2(l-1)(l+2)}{l(l+1)}}
        \left(l(l+1)S(r^2\partial_r G^{+lm}-2h_1^{+lm})+
        2rS(H_2^{+lm}-r\partial_r K^{+lm})+\Lambda r K^{+lm}\right)
\end{eqnarray}
where
\begin{eqnarray}
k_1 & = & K^{+lm} + \frac{S}{r}(r^2\partial_r G^{+lm} - 2h^{+lm}_1) \\
k_2 & = & \frac{1}{2S}
          \left[H^{+lm}_2-r\partial_r k_1-\left(1-\frac{M}{rS}\right) 
            k_1 + S^{1/2}\partial_r
          (r^2 S^{1/2} \partial_r G^{+lm}-2S^{1/2}h_1^{+lm})\right]
\\
&\equiv& \frac{1}{2S}\left[H_2-rK_{,r}-\frac{r-3M}{r-2M}K\right]
\end{eqnarray}

\noindent
NOTE: These quantities compare with those in Moncrief \cite{moncrief74} by
\begin{eqnarray*}
\mbox{Moncriefs odd parity Q: }\qquad Q^\times_{lm} &=&
 \sqrt{\frac{2(l+2)!}{(l-2)!}}Q
 \\
\mbox{Moncriefs even parity Q: } \qquad Q^+_{lm} &=&
 \sqrt{\frac{2(l-1)(l+2)}{l(l+1)}}Q
\end{eqnarray*}

Note that these quantities only depend on the purely spatial 
Regge-Wheeler functions, and not the gauge parts. (In the Regge-Wheeler 
and Zerilli gauges, these are just respectively (up to a rescaling)
 the Regge-Wheeler 
and Zerilli functions).
These quantities satisfy the wave equations
\begin{eqnarray*}
  &&(\partial^2_t-\partial^2_{r^*})Q^\times_{lm}+S\left[\frac{l(l+1)}{r^2}-\frac{6M}{r^3}
  \right]Q^{\times}_{lm}  =  0 
  \\
  &&(\partial^2_t-\partial^2_{r^*})Q^+_{lm}+S\left[
    \frac{1}{\Lambda^2}\left(\frac{72M^3}{r^5}-\frac{12M}{r^3}(l-1)(l+2)\left(1-\frac{3M}{r}\right)
    \right)+\frac{l(l-1)(l+1)(l+2)}{r^2\Lambda}\right]Q^+_{lm}=0
\end{eqnarray*}
where
\begin{eqnarray*}
  \Lambda &=& (l-1)(l+2)+6M/r \\
  r^*     &=& r+2M\ln(r/2M-1)
\end{eqnarray*}
 



\section{Numerical Implementation}

The implementation assumes that the numerical solution, on a Cartesian
grid, is approximately Schwarzshild on the spheres of constant
$r=\sqrt(x^2+y^2+z^2)$ where the waveforms are extracted. The general
procedure is then:

\begin{itemize}

  \item Project the required metric components, and radial derivatives
  of metric components, onto spheres of constant coordinate radius
  (these spheres are chosen via parameters).

  \item Transform the metric components and there derivatives on the
  2-spheres from Cartesian coordinates into a spherical coordinate
  system.

  \item Calculate the physical metric on these spheres if a conformal
  factor is being used.

  \item Calculate the transformation from the coordinate radius to an
  areal radius for each sphere.

  \item Calculate the $S$ factor on each sphere. Combined with the
  areal radius This also produces an estimate of the mass.

  \item Calculate the six Regge-Wheeler variables, and required radial
  derivatives, on these spheres by integration of combinations of the
  metric components over each sphere.

  \item Contruct the gauge invariant quantities from these
  Regge-Wheeler variables.

\end{itemize}

\subsection{Project onto Spheres of Constant Radius}

This is performed by interpolating the metric components, and if
needed the conformal factor, onto the spheres. Although 2-spheres are
hardcoded, the source code could easily be changed here to project
onto e.g. 2-ellipsoids.

\subsection{Calculate Radial Transformation}

The areal coordinate $\hat{r}$ of each sphere is calculated by
%
\begin{equation}
  \hat{r}    =  \hat{r}(r) = \left[
            \frac{1}{4\pi}
            \int\sqrt{\gamma_{\t\t}
            \gamma_{\p\p}}d\t d\p \right]^{1/2}
\end{equation}
%
from which
%
\begin{equation}
\frac{d\hat{r}}{d\eta} = \frac{1}{16\pi \hat{r}}
  \int\frac{\gamma_{\t\t,\eta}\gamma_{\p\p}+\gamma_{\t\t}\gamma_{\p\p,\eta}}
  {\sqrt{\gamma_{\t\t}\gamma_{\p\p}}} \ d\t d\p
\end{equation}
%
Note that this is not the only way to combine metric components to get
the areal radius, but this one was used because it gave better values
for extracting close to the event horizon for perturbations of black
holes.

\subsection{Calculate $S$ factor and Mass Estimate}

\begin{equation}
S(\hat{r}) = \left(\frac{\partial\hat{r}}{\partial r}\right)^2 \int \gamma_{rr} \ d\t d\p
\end{equation}

\begin{equation}
M(\hat{r}) = \hat{r}\frac{1-S}{2}
\end{equation}

\subsection{Calculate Regge-Wheeler Variables}

\begin{eqnarray*}
c_1^{\times lm}  &=&  \frac{1}{l(l+1)}
                      \int \frac{\gamma_{\hat{r}\p}Y^*_{lm,\t}
                                -\gamma_{\hat{r}\t} Y^*_{lm,\p} }
                     {\s}d\Omega
\\
c_2^{\times lm} & = & -\frac{2}{l(l+1)(l-1)(l+2)}
                      \int\left\{
           \left(-\frac{1}{\sin^2\t}\gamma_{\t\t}+\frac{1}
           {\sin^4\t}\gamma_{\p\p}\right)
           (\s Y^*_{lm,\t\p}-\c Y^*_{lm,\p})
\right.
\\
&&\left.
           + \frac{1}{\s} \gamma_{\t\p}
           (Y^*_{lm,\t\t}-\cot\t Y^*_{lm,\t}
           -\frac{1}{\sin^2\t}Y^*_{lm,\p\p}) \right\}d\Omega
\\
h_1^{+lm} &=& \frac{1}{l(l+1)}
            \int \left\{
                \gamma_{\hat{r}\t} Y^*_{lm,\t} + \frac{1}{\sin^2\t}
                \gamma_{\hat{r}\p}Y^*_{lm,\p}\right\} d\Omega
\\
H_2^{+lm} &=& S  \int \gamma_{\hat{r}\hat{r}} \Ys d\Omega
\\
K^{+lm}   &=& \frac{1}{2\hat{r}^2} \int \left(\gamma_{\t\t}+
           \frac{1}{\sin^2\t}\gamma_{\p\p}\right)\Ys
           d\Omega
\\
          &&+\frac{1}{2\hat{r}^2(l-1)(l+2)}
\int \left\{
  \left(\gamma_{\t\t}-\frac{\gamma_{\p\p}}{\sin^2\t}\right)
    \left(Y^*_{lm,\t\t}-\cot\t Y^*_{lm,\t}-\frac{1}{\sin^2\t}
    Y^*_{lm,\p\p}\right) 
\right.
\\
&&\left.
   + \frac{4}{\sin^2\t}\gamma_{\t\p}(Y^*_{lm,\t\p}-\cot\t
     Y^*_{lm,\p})
     \right \} d\Omega
\\
G^{+lm}  &=& \frac{1}{\hat{r}^2 l(l+1)(l-1)(l+2)}
  \int \left\{
  \left(\gamma_{\t\t}-\frac{\gamma_{\p\p}}{\sin^2\t}\right)
    \left(Y^*_{lm,\t\t}-\cot\t Y^*_{lm,\t}-\frac{1}{\sin^2\t}
    Y^*_{lm,\p\p}\right) 
\right.
\\
&&\left.
   +\frac{4}{\sin^2\t}\gamma_{\t\p}(Y^*_{lm,\t\p}-\cot\t
   Y^*_{lm,\p})
   \right\}d\Omega
\end{eqnarray*}
where
\begin{eqnarray}
\gamma_{\hat{r}\hat{r}}      & = & \frac{\partial r}{\partial \hat{r}}
                       \frac{\partial r}{\partial \hat{r}}
                       \gamma_{rr} 
\\
\gamma_{\hat{r}\t} & = & \frac{\partial r}{\partial \hat{r}}
                       \gamma_{r\t} 
\\
\gamma_{\hat{r}\p}   & = & \frac{\partial r}{\partial \hat{r}}
                       \gamma_{r\p}
\end{eqnarray}

\subsection{Calculate Gauge Invariant Quantities}

\begin{eqnarray}
Q^{\times}_{lm} 
  & = & \sqrt{\frac{2(l+2)!}{(l-2)!}}\left[c_1^{\times lm}
        + \frac{1}{2}\left(\partial_{\hat{r}} c_2^{\times lm} - \frac{2}{\hat{r}}
        c_2^{\times lm}\right)\right] \frac{S}{\hat{r}}
\\
Q^{+}_{lm}
  & = & \frac{1}{(l-1)(l+2)+6M/\hat{r}}\sqrt{\frac{2(l-1)(l+2)}{l(l+1)}}
        (4\hat{r}S^2 k_2+l(l+1)\hat{r} k_1) 
\end{eqnarray}
where
\begin{eqnarray}
k_1 & = & K^{+lm} + \frac{S}{\hat{r}}(\hat{r}^2\partial_{\hat{r}} G^{+lm} - 2h^{+lm}_1) \\
k_2 & = & \frac{1}{2S}
          [H^{+lm}_2-\hat{r}\partial_{\hat{r}} k_1-(1-\frac{M}{\hat{r}S}) k_1 + S^{1/2}\partial_{\hat{r}}
          (\hat{r}^2 S^{1/2} \partial_{\hat{r}} G^{+lm}-2S^{1/2}h_1^{+lm}
\end{eqnarray}

\section{Using This Thorn}

Use this thorn very carefully. Check the validity of the waveforms by running
tests with different resolutions, different outer boundary conditions, etc
to check that the waveforms are consistent.

\subsection{Basic Usage}

\subsection{Output Files}

Although Extract is really an {\tt ANALYSIS} thorn, at the moment it
is scheduled at {\tt POSTSTEP}, with the iterations at which output is
performed determined by the parameter {\it itout}. Output files from
{\tt Extract} are always placed in the main output directory defined
by {\tt CactusBase/IOUtil}.

Output files are generated for each detector (2-sphere) used, and
these detectors are identified in the name of each output file by {\tt
R1}, {\tt R2}, \ldots.

The extension denotes whether coordinate time ({\.tl}) or proper time
({\.ul}) is used for the first column.

\begin{itemize}

  \item {\tt rsch\_R?.[tu]l} 

	The extracted areal radius on each 2-sphere.

  \item {\tt mass\_R?.[tu]l}

	Mass estimate calculated from $g_{rr}$ on each 2-sphere.

  \item {\tt Qeven\_R?\_??.[tu]l}

	The even parity gauge invariate variable ({\it waveform}) on 
	each 2-sphere. This is a complex quantity, the 2nd column is 
	the real part, and the third column the imaginary part.

  \item {\tt Qodd\_R?\_??.[tu]l}

	The odd parity gauge invariate variable ({\it waveform}) on 
	each 2-sphere. This is a complex quantity, the 2nd column is 
	the real part, and the third column the imaginary part.

  \item {\tt ADMmass\_R?.[tu]l}

	Estimate of ADM mass enclosed within each 2-sphere.
	(To produce this set {\tt doADMmass = ``yes''}).

  \item {\tt momentum\_[xyz]\_R?.[tu]l}

	Estimate of momentum at each 2-sphere.
	(To produce this set {\tt do\_momentum = ``yes''}).

  \item {\tt spin\_[xyz]\_R?.[tu]l}

	Estimate of momentum at each 2-sphere.
	(To produce this set {\tt do\_spin = ``yes''}).


\end{itemize}

\section{History}

Much of the source code
 for Extract comes from a code written outside
of Cactus for extracting waveforms from data generated by the NCSA
G-Code for compare with linear evolutions of waveforms extracted from
the Cauchy initial data.  This work was carried out in collaboration
with Karen Camarda and Ed Seidel.


\section{Appendix: Regge-Wheeler Harmonics}

\label{reggewheeler}

\begin{eqnarray*}
(\hat{e}_1)^{lm} &=& 
\left( \begin{array}{ccc}
0  & -\frac{1}{\s}\Yp & \s \Yt \\
.  & 0                                & 0                        \\
.  & 0                                & 0 
\end{array}\right)
\\
(\hat{e}_2)^{lm} &=& 
\left( \begin{array}{ccc} 
0 & 0 & 0 \\
0 & \frac{1}{\s}(\Ytp-\cot\t \Yp) & . \\
0 & -\frac{\s}{2}[\Ytt-\cot\t 
    \Yt-\frac{1}{\sin^2\t}\Ypp]           & 
            -\s [\Ytp-\cot\t \Yp]
\end{array}\right)
\\
(\hat{f}_1)^{lm} &=& 
\left( \begin{array}{ccc}
  0 & \Yt & \Yp \\
  . & 0   & 0           \\
  . & 0   & 0 
\end{array}\right)
\\
(\hat{f}_2)^{lm} &=& 
\left( \begin{array}{ccc}
\Y & 0 & 0 \\
0      & 0 & 0 \\
0      & 0 & 0 
\end{array}\right)
\\
(\hat{f}_3)^{lm} &=& 
\left( \begin{array}{ccc}
0 & 0  & 0                  \\
0 & \Y & 0                  \\
0 & 0  & \sin^2\t \Y 
\end{array}\right)
\\
(\hat{f}_4)^{lm} &=& 
\left( \begin{array}{ccc}
0 & 0                   & 0 \\
0 & \Ytt & . \\
0 & \Ytp-\cot \t \Yp & \Ypp+ \s \c \Yt
\end{array}\right)
\end{eqnarray*}

\section{Appendix: Transformation Between Cartesian and Spherical Coordinates}

First, the transformations between metric components in $(x,y,z)$ and $(r,\t,\p)$ coordinates. Here, $\rho=\sqrt{x^2+y^2}=r\s$,
\begin{eqnarray*}
  \frac{\partial x}{\partial r}
  &=&
  \sin\t\cos\p 
  =
  \frac{x}{r}
\\
  \frac{\partial y}{\partial r}
  &=&
  \sin\t\sin\p 
  =
  \frac{y}{r}
\\
  \frac{\partial z}{\partial r}
  &=&
  \cos\t 
  =
  \frac{z}{r}
\\
  \frac{\partial x}{\partial \t}
  &=&
  r\cos\t\cos\p 
  =
  \frac{xz}{\rho}
\\
  \frac{\partial y}{\partial \t}
  &=&
  r\cos\t\sin\p 
  =
  \frac{yz}{\rho}
\\
  \frac{\partial z}{\partial \t}
  &=&
  -r\sin\t 
  =
  -\rho
\\
  \frac{\partial x}{\partial \p}
  &=&
  -r\sin\t\sin\p
  =
  -y
\\
  \frac{\partial y}{\partial \p}
  &=&
  r\sin\t\cos\p 
  =
  x
\\
  \frac{\partial z}{\partial \p}
  &=&
  0
\end{eqnarray*}


\begin{eqnarray*}
  \gamma_{rr} &=&
  \frac{1}{r^2}
     (x^2\gamma_{xx}+
      y^2\gamma_{yy}+
      z^2\gamma_{zz}+
      2xy\gamma_{xy}+
      2xz\gamma_{xz}+
      2yz\gamma_{yz})
\\
  \gamma_{r\t} &=&
  \frac{1}{r\rho}
     (x^2 z \gamma_{xx}
     +y^2 z \gamma_{yy}
     -z \rho^2 \gamma_{zz}
     +2xyz \gamma_{xy}
     +x(z^2-\rho^2)\gamma_{xz}
     +y(z^2-\rho^2)\gamma_{yz})
\\
  \gamma_{r\p} &=&
  \frac{1}{r}
     (-xy\gamma_{xx}
      +xy\gamma_{yy}
      +(x^2-y^2)\gamma_{xy}
      -yz \gamma_{xz}
      +xz\gamma_{yz})
\\
  \gamma_{\t\t} &=&
  \frac{1}{\rho^2}
  (x^2z^2\gamma_{xx}
  +2xyz^2\gamma_{xy}
  -2xz\rho^2\gamma_{xz}
  +y^2z^2\gamma_{yy}
  -2yz\rho^2\gamma_{yz}
  +\rho^4\gamma_{zz})
\\
  \gamma_{\t\p} &=&
  \frac{1}{\rho}
  (-xyz\gamma_{xx}
   +(x^2-y^2)z\gamma_{xy}
   +\rho^2 y \gamma_{xz}
   +xyz\gamma_{yy}
   -\rho^2 x \gamma_{yz})
\\
  \gamma_{\p\p} &=&
   y^2\gamma_{xx}
   -2xy\gamma_{xy}
   +x^2\gamma_{yy}
\end{eqnarray*}   
or,
\begin{eqnarray*}
\gamma_{rr}&=&
\sin^2\t\cos^2\p\gamma_{xx}
+\sin^2\t\sin^2\p\gamma_{yy}
+\cos^2\t\gamma_{zz}
+2\sin^2\theta\cos\p\sin\p\gamma_{xy}
+2\sin\t\cos\t\cos\p\gamma_{xz}
\\
&&
+2\s\c\sin\p\gamma_{yz}
\\
\gamma_{r\t}&=&
r(\s\c\cos^2\phi\gamma_{xx}
+2*\s\c\sin\p\cos\p\gamma_{xy}
+(\cos^2\t-\sin^2\t)\cos\p\gamma_{xz}
+\s\c\sin^2\p\gamma_{yy}
\\
&&
+(\cos^2\t-\sin^2\t)\sin\p\gamma_{yz}
-\s\c\gamma_{zz})
\\
\gamma_{r\p}&=&
r\s(-\s\sin\p\cos\p\gamma_{xx}
-\s(\sin^2\p-\cos^2\p)\gamma_{xy}
-\c\sin\p\gamma_{xz}
+\s\sin\p\cos\p\gamma_{yy}
\\
&&
+\c\cos\p\gamma_{yz})
\\
\gamma_{\t\t}&=&
r^2(\cos^2\t\cos^2\p\gamma_{xx}
+2\cos^2\t\sin\p\cos\p\gamma_{xy}
-2\s\c\cos\p\gamma_{xz}
+\cos^2\t\sin^2\p\gamma_{yy}
\\
&&
-2\s\c\sin\p\gamma_{yz}
+\sin^2\t\gamma_{zz})
\\
\gamma_{\t\p}&=&
r^2\s(-\c\sin\p\cos\p\gamma_{xx}
-\c(\sin^2\p-\cos^2\p)\gamma_{xy}
+\s\sin\p\gamma_{xz}
+\c\sin\p\cos\p\gamma_{yy}
\\
&&
-\s\cos\p\gamma_{yz})
\\
\gamma_{\p\p}&=&
r^2\sin^2\t(\sin^2\p\gamma_{xx}
-2\sin\p\cos\p\gamma_{xy}
+\cos^2\phi\gamma_{yy})
\end{eqnarray*}


We also need 
the transformation for the radial derivative of the metric components:
\begin{eqnarray*}
\gamma_{rr,\eta}&=&
\sin^2\t\cos^2\p\gamma_{xx,\eta}
+\sin^2\t\sin^2\p\gamma_{yy,\eta}
+\cos^2\t\gamma_{zz,\eta}
+2\sin^2\theta\cos\p\sin\p\gamma_{xy,\eta}
\\
&&
+2\sin\t\cos\t\cos\p\gamma_{xz,\eta}
+2\s\c\sin\p\gamma_{yz,\eta}
\\
\gamma_{r\t,\eta}&=& 
\frac{1}{r}\gamma_{r\t}+
r(\s\c\cos^2\phi\gamma_{xx,\eta}
+\s\c\sin\p\cos\p\gamma_{xy,\eta}
+(\cos^2\t-\sin^2\t)\cos\p\gamma_{xz,\eta}
\\
&&
+\s\c\sin^2\p\gamma_{yy,\eta}
+(\cos^2\t-\sin^2\t)\sin\p\gamma_{yz,\eta}
-\s\c\gamma_{zz,\eta})
\\
\gamma_{r\p,\eta}&=&
\frac{1}{r}\gamma_{r\p}+
r\s(-\s\sin\p\cos\p\gamma_{xx,\eta}
-\s(\sin^2\p-\cos^2\p)\gamma_{xy,\eta}
-\c\sin\p\gamma_{xz,\eta}
\\
&&
+\s\sin\p\cos\p\gamma_{yy,\eta}
+\c\cos\p\gamma_{yz,\eta})
\\
\gamma_{\t\t,\eta}&=&
\frac{2}{r}\gamma_{\t\t}+
r^2(\cos^2\t\cos^2\p\gamma_{xx,\eta}
+2\cos^2\t\sin\p\cos\p\gamma_{xy,\eta}
-2\s\c\cos\p\gamma_{xz,\eta}
\\
&&
+\cos^2\t\sin^2\p\gamma_{yy,\eta}
-2\s\c\sin\p\gamma_{yz,\eta}
+\sin^2\t\gamma_{zz,\eta})
\\
\gamma_{\t\p,\eta}&=&
\frac{2}{r}\gamma_{\t\p}+
r^2\s(-\c\sin\p\cos\p\gamma_{xx,\eta}
-\c(\sin^2\p-\cos^2\p)\gamma_{xy,\eta}
+\s\sin\p\gamma_{xz,\eta}
\\
&&
+\c\sin\p\cos\p\gamma_{yy,\eta}
-\s\cos\p\gamma_{yz,\eta})
\\
\gamma_{\p\p,\eta}&=&
\frac{2}{r}\gamma_{\p\p}+
r^2\sin^2\t(\sin^2\p\gamma_{xx,\eta}
-2\sin\p\cos\p\gamma_{xy,\eta}
+\cos^2\phi\gamma_{yy,\eta})
\end{eqnarray*}

\section{Appendix: Integrations Over the 2-Spheres}


This is done by using Simpson's rule twice. Once in each coordinate 
direction. Simpson's rule is
\begin{equation}
\int^{x_2}_{x_1} f(x) dx = 
  \frac{h}{3} [f_1+4f_2+2f_3+4f_4+\ldots+2f_{N-2}+4 f_{N-1}+f_N]
  +O(1/N^4)
\end{equation}
$N$ must be an odd number.


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% END CACTUS THORNGUIDE

\end{document}
