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Physical Review Letters | 2013

Catalog of 174 Binary Black Hole Simulations for Gravitational Wave Astronomy

Abdul H. Mroué; Mark A. Scheel; Bela Szilagyi; Harald P. Pfeiffer; Michael Boyle; Daniel A. Hemberger; Lawrence E. Kidder; Geoffrey Lovelace; Serguei Ossokine; Nicholas W. Taylor; Anil Zenginoglu; Luisa T. Buchman; Tony Chu; Evan Foley; Matthew Giesler; Robert Owen; Saul A. Teukolsky

This Letter presents a publicly available catalog of 174 numerical binary black hole simulations following up to 35 orbits. The catalog includes 91 precessing binaries, mass ratios up to 8∶1, orbital eccentricities from a few percent to 10(-5), black hole spins up to 98% of the theoretical maximum, and radiated energies up to 11.1% of the initial mass. We establish remarkably good agreement with post-Newtonian precession of orbital and spin directions for two new precessing simulations, and we discuss other applications of this catalog. Formidable challenges remain: e.g., precession complicates the connection of numerical and approximate analytical waveforms, and vast regions of the parameter space remain unexplored.


Classical and Quantum Gravity | 2015

Improved methods for simulating nearly extremal binary black holes

Mark A. Scheel; Matthew Giesler; Daniel A. Hemberger; Geoffrey Lovelace; Kevin Kuper; Michael Boyle; Bela Szilagyi; Lawrence E. Kidder

Astrophysical black holes could be nearly extremal (that is, rotating nearly as fast as possible); therefore, nearly extremal black holes could be among the binaries that current and future gravitational-wave observatories will detect. Predicting the gravitational waves emitted by merging black holes requires numerical-relativity simulations, but these simulations are especially challenging when one or both holes have mass m and spin S exceeding the Bowen–York limit of S/m^2 = 0.93. We present improved methods that enable us to simulate merging, nearly extremal black holes (i.e., black holes with S/m^2 > 0.93) more robustly and more efficiently. We use these methods to simulate an unequal-mass, precessing binary black hole (BBH) coalescence, where the larger black hole has S/m^2 = 0.99. We also use these methods to simulate a non-precessing BBH coalescence, where both black holes have S/m^2 = 0.994, nearly reaching the Novikov–Thorne upper bound for holes spun up by thin accretion disks. We demonstrate numerical convergence and estimate the numerical errors of the waveforms; we compare numerical waveforms from our simulations with post-Newtonian and effective-one-body waveforms; we compare the evolution of the black hole masses and spins with analytic predictions; and we explore the effect of increasing spin magnitude on the orbital dynamics (the so-called ‘orbital hangup’ effect).


Physical Review D | 2018

On choosing the start time of binary black hole ringdowns

S. Bhagwat; Maria Okounkova; S. Ballmer; D. A. Brown; Matthew Giesler; Mark A. Scheel; Saul A. Teukolsky

The final stage of a binary black hole merger is ringdown, in which the system is described by a Kerr black hole with quasinormal mode perturbations. It is far from straightforward to identify the time at which the ringdown begins. Yet determining this time is important for precision tests of the general theory of relativity that compare an observed signal with quasinormal mode descriptions of the ringdown, such as tests of the no-hair theorem. We present an algorithmic method to analyze the choice of ringdown start time in the observed waveform. This method is based on determining how close the strong field is to a Kerr black hole (Kerrness). Using numerical relativity simulations, we characterize the Kerrness of the strong-field region close to the black hole using a set of local, gauge-invariant geometric and algebraic conditions that measure local isometry to Kerr. We produce a map that associates each time in the gravitational waveform with a value of each of these Kerrness measures; this map is produced by following outgoing null characteristics from the strong and near-field regions to the wave zone. We perform this analysis on a numerical relativity simulation with parameters consistent with GW150914---the first gravitational-wave detection. We find that the choice of ringdown start time of 3 ms after merger used in the GW150914 study [B. P. Abbott et al. (Virgo Collaboration and LIGO Scientific Collaboration), Phys. Rev. Lett. 116, 221101 (2016).] to test general relativity corresponds to a high dimensionless perturbation amplitude of


Physical Review D | 2018

Measuring the properties of nearly extremal black holes with gravitational waves

Katerina Chatziioannou; Geoffrey Lovelace; Michael P. Boyle; Matthew Giesler; Daniel A. Hemberger; Reza Katebi; Lawrence E. Kidder; Harald P. Pfeiffer; Mark A. Scheel; Bela Szilagyi

\ensuremath{\sim}7.5\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}3}


Monthly Notices of the Royal Astronomical Society | 2018

Low-mass X-ray binaries from black hole retaining globular clusters

Matthew Giesler; Drew Clausen; Christian D. Ott

in the strong-field region. This suggests that in higher signal-to-noise detections, one would need to start analyzing the signal at a later time for studies that depend on the validity of black hole perturbation theory.


arXiv: General Relativity and Quantum Cosmology | 2013

A catalog of 171 high-quality binary black-hole simulations for gravitational-wave astronomy

Abdul H. Mroué; Mark A. Scheel; Bela Szilagyi; Harald P. Pfeiffer; Michael Boyle; Daniel A. Hemberger; Lawrence E. Kidder; Geoffrey Lovelace; Sergei Ossokine; Nicholas W. Taylor; Anil Zenginoglu; Luisa T. Buchman; Tony Chu; Evan Foley; Matthew Giesler; Robert Owen; Saul A. Teukolsky

Characterizing the properties of black holes is one of the most important science objectives for gravitational-wave observations. Astrophysical evidence suggests that black holes that are nearly extremal (i.e., spins near the theoretical upper limit) might exist and, thus, might be among the merging black holes observed with gravitational waves. In this paper, we explore how well current gravitational wave parameter estimation methods can measure the spins of rapidly spinning black holes in binaries. We simulate gravitational-wave signals using numerical-relativity waveforms for nearly-extremal, merging black holes. For simplicity, we confine our attention to binaries with spins parallel or antiparallel with the orbital angular momentum. We find that recovering the holes’ nearly extremal spins is challenging. When the spins are nearly extremal and parallel to each other, the resulting parameter estimates do recover spins that are large, though the recovered spin magnitudes are still significantly smaller than the true spin magnitudes. When the spins are nearly extremal and antiparallel to each other, the resulting parameter estimates recover the small effective spin but incorrectly estimate the individual spins as nearly zero. We study the effect of spin priors and argue that a commonly used prior (uniform in spin magnitude and direction) hinders unbiased recovery of large black-hole spins.


Bulletin of the American Physical Society | 2018

Low-mass X-ray binaries from black-hole retaining globular clusters

Matthew Giesler; Drew Clausen; Christian D. Ott

Recent studies suggest that globular clusters (GCs) may retain a substantial population of stellar-mass black holes (BHs), in contrast to the long-held belief of a few to zero BHs. We model the population of BH low-mass X-ray binaries (BH-LMXBs), an ideal observable proxy for elusive single BHs, produced from a representative group of Milky Way GCs with variable BH populations. We simulate the formation of BH-binaries in GCs through exchange interactions between binary and single stars in the company of tens to hundreds of BHs. Additionally, we consider the impact of the BH population on the rate of compact binaries undergoing gravitational wave driven mergers. The characteristics of the BH-LMXB population and binary properties are sensitive to the GCs structural parameters as well as its unobservable BH population. We find that GCs retaining


Bulletin of the American Physical Society | 2018

On choosing the start time of binary black hole ringdown II: Results

S. Bhagwat; Maria Okounkova; S. Ballmer; D. A. Brown; Matthew Giesler; Mark A. Scheel; Saul A. Teukolsky

\sim 1000


Bulletin of the American Physical Society | 2018

On choosing the start time of binary black hole ringdown I: Theory

Maria Okounkova; S. Bhagwat; Stephan Ballmer; D. A. Brown; Matthew Giesler; Mark A. Scheel; Saul A. Teukolsky

BHs produce a galactic population of


Bulletin of the American Physical Society | 2017

The population of low-mass X-ray binaries ejected from black-hole retaining globular clusters

Matthew Giesler; Drew Clausen; Christian D. Ott

\sim 150

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Mark A. Scheel

California Institute of Technology

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Christian D. Ott

California Institute of Technology

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