From 6f0b2f884a1737ed3e8ea21bf9afe4115dbf5dea Mon Sep 17 00:00:00 2001 From: Thomas Ng Date: Tue, 17 Oct 2023 12:26:15 +0800 Subject: [PATCH] fix bug --- src/tex/ms.tex | 2 +- 1 file changed, 1 insertion(+), 1 deletion(-) diff --git a/src/tex/ms.tex b/src/tex/ms.tex index bbcac97..a65b9c4 100644 --- a/src/tex/ms.tex +++ b/src/tex/ms.tex @@ -204,7 +204,7 @@ \subsection{Single-event parameter estimation} We analyze the 71 \acp{BBH} that were detected with $\mathrm{FAR} < 1/\mathrm{yr}$, less stringent than the typical \ac{LVK} threshold of $1/1000\,\mathrm{yr}$ \cite{LIGOScientific:2020tif,LIGOScientific:2021sio}. The \ac{FAR} values are typically determined by \ac{GR} pipelines, which could down-rank signals beyond \ac{GR} \cite{LIGOScientific:2020tif,Chia:2020psj,tgrsel}; however, since detectability through matched-filtering is most sensitive to the phase, not the amplitude, we expect only a minor decrease in sensitivity to the kind of birefringent signals explored here. To avoid extended computations on longer signals and considering these are generally at closer distances, we do not analyze systems involving neutron stars in this work. -We procure strain data from \add{the} Gravitational Wave Open Science Center \citep{GWOSC}. +We procure strain data from \added{the} Gravitational Wave Open Science Center \citep{GWOSC}. We estimate source parameters using a custom version of the \textsc{Bilby} software \citep{Bilby}, modified from the baseline version to apply Eq.~\eqref{eq:waveform_modification} for any \ac{GR} baseline waveform. We take the \ac{PE} configuration in \citep{GWTC-2.1, GWTC-3, GWTC-2.1_dataset, GWTC-3_dataset} as a starting point, with \textsc{IMRPhenomXPHM} \citep{Pratten:2020ceb} as the reference waveform.