Published July 15, 2021 | Version Accepted Version + Published
Journal Article Open

Fixing the BMS frame of numerical relativity waveforms

  • 1. ROR icon California Institute of Technology
  • 2. ROR icon Pennsylvania State University
  • 3. ROR icon Cornell University
  • 4. ROR icon University of Mississippi
  • 5. ROR icon Max Planck Institute for Gravitational Physics

Abstract

Understanding the Bondi-Metzner-Sachs (BMS) frame of the gravitational waves produced by numerical relativity is crucial for ensuring that analyses on such waveforms are performed properly. It is also important that models are built from waveforms in the same BMS frame. Up until now, however, the BMS frame of numerical waveforms has not been thoroughly examined, largely because the necessary tools have not existed. In this paper, we show how to analyze and map to a suitable BMS frame for numerical waveforms calculated with the Spectral Einstein Code (SpEC). However, the methods and tools that we present are general and can be applied to any numerical waveforms. We present an extensive study of 13 binary black hole systems that broadly span parameter space. From these simulations, we extract the strain and also the Weyl scalars using both SpECTRE's Cauchy-characteristic extraction module and also the standard extrapolation procedure with a displacement memory correction applied during postprocessing. First, we show that the current center-of-mass correction used to map these waveforms to the center-of-mass frame is not as effective as previously thought. Consequently, we also develop an improved correction that utilizes asymptotic Poincaré charges instead of a Newtonian center-of-mass trajectory. Next, we map our waveforms to the post-Newtonian (PN) BMS frame using a PN strain waveform. This helps us find the unique BMS transformation that minimizes the L² norm of the difference between the numerical and PN strain waveforms during the early inspiral phase. We find that once the waveforms are mapped to the PN BMS frame, they can be hybridized with a PN strain waveform much more effectively than if one used any of the previous alignment schemes, which only utilize the Poincaré transformations.

Additional Information

© 2021 American Physical Society. Received 11 May 2021; accepted 17 June 2021; published 20 July 2021. Computations were performed with the High Performance Computing Center and the Wheeler cluster at Caltech. This work was supported in part by the Sherman Fairchild Foundation and by NSF Grants No. PHY-2011961, No. PHY-2011968, and No. OAC-1931266 at Caltech, NSF Grants No. PHY-1912081 and No. OAC-1931280 at Cornell, and NSF Grant No. PHY-1806356, Grant No. UN2017-92945 from the Urania Stott Fund of the Pittsburgh Foundation, and the Eberly research funds of Penn State at Penn State.

Attached Files

Published - PhysRevD.104.024051.pdf

Accepted Version - 2105.02300.pdf

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2105.02300.pdf

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Additional details

Identifiers

Eprint ID
110367
Resolver ID
CaltechAUTHORS:20210821-163947559

Related works

Funding

Sherman Fairchild Foundation
NSF
PHY-2011961
NSF
PHY-2011968
NSF
OAC-1931266
NSF
PHY-1912081
NSF
OAC-1931280
NSF
PHY-1806356
Pittsburgh Foundation
UN2017-92945
Pennsylvania State University

Dates

Created
2021-08-21
Created from EPrint's datestamp field
Updated
2023-04-28
Created from EPrint's last_modified field

Caltech Custom Metadata

Caltech groups
TAPIR , Physics Department