Testing spacetime symmetry through gravitational waves from extreme-mass-ratio inspirals
Aug 31, 2020
14 pages
Published in:
- Phys.Rev.D 102 (2020) 6, 064041
- Published: Sep 16, 2020
e-Print:
- 2009.00028 [gr-qc]
DOI:
- 10.1103/PhysRevD.102.064041 (publication)
View in:
Citations per year
Abstract: (APS)
One of the primary aims of upcoming spaceborne gravitational wave detectors is to measure radiation in the mHz range from extreme-mass-ratio inspirals. Such a detection would place strong constraints on hypothetical departures from a Kerr description for astrophysically stable black holes. The Kerr geometry, which is unique in general relativity, admits a higher-order symmetry in the form of a Carter constant, which implies that the equations of motion describing test particle motion in a Kerr background are Liouville-integrable. In this article, we investigate whether the Carter symmetry itself is discernible from a generic deformation of the Kerr metric in the gravitational waveforms for such inspirals. We build on previous studies by constructing a new metric which respects current observational constraints, describes a black hole, and contains two non-Kerr parameters, one of which controls the presence or absence of the Carter symmetry, thereby controlling the existence of chaotic orbits, and another which serves as a generic deformation parameter. We find that these two parameters introduce fundamentally distinct features into the orbital dynamics, and evince themselves in the gravitational waveforms through a significant dephasing. Although only explored in the quadrupole approximation, this, together with a Fisher metric analysis, suggests that gravitational wave data analysis may be able to test, in addition to the governing theory of gravity, the underlying symmetries of spacetime.Note:
- 14 pages, 7 figures, matches published version
- General relativity, alternative theories of gravity
- symmetry: space-time
- metric: Kerr
- black hole: stability
- gravitational radiation
- capture
- deformation
- gravitational radiation detector
- general relativity
- field equations: higher-order
References(82)
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- [1]
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- [9]
- [10]
- [11]
- [12]
- [13]
- [14]
- [15]
- [16]
- [17]
- [18]
- [19]
- [20]
- [21]
- [22]
- [23]
- [24]
- [25]