19–21 Feb 2019
"Sapienza" University, Phys. Dept. Marconi
Europe/Rome timezone

An improved analytical representation of the postmerger and ringdown

20 Feb 2019, 18:00
1m
I Floor (Phys. Dept. Marconi)

I Floor

Phys. Dept. Marconi

poster Gravitational Waves Poster session

Speaker

Mr Gunnar Riemenschneider (INFN sezione di Torino, Universitá degli studi di Torino)

Description

The postmerger-ringdown waveform of coalescing, non-precessing, spinning
binary black holes in the \texttt{TEOBresumS} model is given by a closed form, analytic,
time-domain family of template waveforms, informed by a large set of
Numerical Relativity waveforms from different codes such as the BAM code, the SpEC code and
state-of-the-art test-particle waveforms. The NR waveforms cover the parameter space
from the equal mass case till the test-particle limit. This includes 5 waveforms generated by the BAM
code with mass ratio $m_1/m_2=18$ and with the heavier BH spinning with spins up to $\pm 0.8$.
The peak is fitted with an error of at most $2\%$ in both amplitude and frequency. The phase (amplitude)
is fitted with an accuracy of at least $0.1rad$ ($10\%$) over the first 10-15M
after the peak, with the exception of 3 outliers.

Stand alone the model can be used for several studies independently as well.
The postmerger and ringdown of very heavy black hole binary systems,
such as GW170729, will still be in the observable band of 2nd generation
gravitational wave detectors such as advanced LIGO and advanced Virgo.
Analyzing the signals directly in the time-domain, using the analytical
postmerger-ringdown waveform model, gives a fully independent
measurement of source parameters. Further, it was demonstrated in arXiv:1811.08744 that
fits of key waveform characteristics, such as peak amplitude and frequency,
could be used for consistency tests of general relativity in the strong-field
regime.

After a pedagogical introduction to the analytic setup I will discuss the
set of Numerical Relativity waveforms used to inform the model and highlight
several technical details of the fitting procedure. I will discuss the fitting of the
peak structures for the complex multipolar waveforms. I will conclude by showing
results of the application of the model to the analysis of real gravitational wave data.

Primary author

Mr Gunnar Riemenschneider (INFN sezione di Torino, Universitá degli studi di Torino)

Presentation materials