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authorallen <allen@6a3ddf76-46e1-4315-99d9-bc56cac1ef84>2002-06-04 18:59:59 +0000
committerallen <allen@6a3ddf76-46e1-4315-99d9-bc56cac1ef84>2002-06-04 18:59:59 +0000
commitc6eee0bab612c5586d906090941d51efef5a2370 (patch)
treee76b9b26ad226e38054b96bcaedd18a28e856760
parent09bb4100121f8561ab7efc41a8ded40780d7f12c (diff)
Fixing name clashes in citations
git-svn-id: http://svn.einsteintoolkit.org/cactus/EinsteinInitialData/IDAnalyticBH/trunk@118 6a3ddf76-46e1-4315-99d9-bc56cac1ef84
-rw-r--r--doc/documentation.tex20
1 files changed, 10 insertions, 10 deletions
diff --git a/doc/documentation.tex b/doc/documentation.tex
index 2a47bdf..d9ea1f4 100644
--- a/doc/documentation.tex
+++ b/doc/documentation.tex
@@ -82,7 +82,7 @@ associated parameters in turn.
The Schwarzschild metric corresponds to a single, static, black hole.
If the Cactus metric is specified as a conformal metric (by setting
\texttt{admbase::metric\_type="yes"}), then the metric is
-set using isotropic coordinates \cite{mtw-isotropic}:
+set using isotropic coordinates \cite{CactusEinstein_IDAnalytic_mtw-isotropic}:
\begin{equation}
ds^2 = -\left(\frac{2r - M}{2r + M}\right)^2
+ \left(1 + \frac{M}{2r}\right)^4 \left(dr^2 + r^2(d\theta^2
@@ -150,7 +150,7 @@ could modify your parameter file as follows:
\section{Kerr}
Kerr initial data for an isolated rotating black hole is specified
-using the ``quasi-isotropic'' coordinates \cite{brandt-seidel:1996}:
+using the ``quasi-isotropic'' coordinates \cite{CactusEinstein_IDAnalytic_brandt-seidel:1996}:
\begin{equation}
ds^2 = \psi^4 (dr^2 + r^2(d\theta^2 + \chi^2\sin^2\theta d\phi^2)),
\end{equation}
@@ -213,12 +213,12 @@ intial data with mass $M=1$ and angular momentum $a=0.3$ are:
The earliest suggestion for initial data that might be said to
corresponding to multiple black holes was given by Misner in 1960
-\cite{misner:1960}. He provided a prescription for writing a metric
+\cite{CactusEinstein_IDAnalytic_misner:1960}. He provided a prescription for writing a metric
connecting a pair of massive bodies, instaneously at rest, whose
throats are connected by a wormhole. Using the method of images, this
solution was generalised to describe any number of black holes whose
throats connect two identical asymptotically flat spacetimes
-\cite{misner:1963}.
+\cite{CactusEinstein_IDAnalytic_misner:1963}.
\begin{figure}
\centering
\ifpdf
@@ -346,7 +346,7 @@ data which differs from the Misner data mainly in its choice of
spacetime topology. Whereas the Misner data presumes that the throats
connect a pair of asymptotically flat spacetimes which are identical
to each other, the Brill-Lindquist data connects each throat to a
-separate asymptotically flat region \cite{brill-lindquist:1963}.
+separate asymptotically flat region \cite{CactusEinstein_IDAnalytic_brill-lindquist:1963}.
\begin{figure}
\centering
\ifpdf
@@ -396,24 +396,24 @@ parameters such as the following could be used:
\end{verbatim}
\begin{thebibliography}{9}
- \bibitem{mtw-isotropic}
+ \bibitem{CactusEinstein_IDAnalyticBH_mtw-isotropic}
See, for instance, p. 840 of:
Misner, C. W., Thorne, K. S., and Wheeler, J. A. (1973)
\emph{Gravitation}, W. H. Freeman, San Francisco.
- \bibitem{brandt-seidel:1996}
+ \bibitem{CactusEinstein_IDAnalyticBH_brandt-seidel:1996}
Brandt, Steven R. and Seidel, Edward (1996)
\emph{Evolution of distorted rotating black holes. III. Initial
data},
Phys. Rev., \textbf{D54}, 1403--1416.
- \bibitem{misner:1960}
+ \bibitem{CactusEinstein_IDAnalyticBH_misner:1960}
Misner, Charles W. (1960)
\emph{Wormhole Initial Conditions},
Phys. Rev., \textbf{118}, 1110--1111.
- \bibitem{misner:1963}
+ \bibitem{CactusEinstein_IDAnalyticBH_misner:1963}
Misner, Charles W. (1963)
\emph{The Method of Images in Geometrostatics},
Ann. Phys., \textbf{24}, 102--117.
- \bibitem{brill-lindquist:1963}
+ \bibitem{CactusEinstein_IDAnalyticBH_brill-lindquist:1963}
Brill, Dieter R., and Lindquist, Richard W. (1963)
\emph{Interaction Energy in Geometrostatics}
Phys. Rev., \textbf{131}, 471--476.