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patrick gaulme edited begin_deluxetable_lccc_tablecolumns_4__.tex
almost 9 years ago
Commit id: c51bdcdfc484d7b1f577468ab2df53b3ff3367e5
deletions | additions
diff --git a/begin_deluxetable_lccc_tablecolumns_4__.tex b/begin_deluxetable_lccc_tablecolumns_4__.tex
index 9794cb3..15dc308 100644
--- a/begin_deluxetable_lccc_tablecolumns_4__.tex
+++ b/begin_deluxetable_lccc_tablecolumns_4__.tex
...
\tablecolumns{4}
%\tablewidth{0pt}
\tabletypesize{\small}
\tablecaption{Physical parameters of KIC 9246715 from ELC photodynamic
modeling.} modeling. {\bf{HOW CAN THE ERRORBAR BE THAT LOW ON MASS WHEN USING LC SEGMENTS??}}}
\centering
\tablehead{
\colhead{Parameter} & \colhead{All-eclipse model} & \colhead{LC segment RMS} & \colhead{Comment}
...
\label{table1}
\tablenotetext{\dagger}{The triangular limb darkening law (Kipping 2013) re-parameterizes the quadratic limb darkening law, $I(\mu)/I(1) = 1 - u_1(1 - \mu) - u_2(1 - \mu)^2$, with new coefficients $q_1 \equiv (u_1 + u_2)^2$ and $q_2 \equiv 0.5(u_1 + u_2)^{-1}$.}
\end{deluxetable}