Measuring the parameters of massive black hole binary systems with Pulsar Timing Array observations of gravitational waves

Details Measuring the parameters of massive black hole binary systems with Pulsar Timing Array observations of gravitational waves Measuring the parameters of massive black hole binary systems with Pulsar Timing Array observations of gravitational waves

2010-03-02

arxiv.org/abs/1003.0677v1

Phys.Rev.D81:104008,2010

Astronomy and Astrophysics

Astrophysics

Cosmology and Extragalactic Astrophysics

20 pages, 12 figures, 2 color figures, submitted to Phys. Rev. D

Scientific paper

10.1103/PhysRevD.81.104008

The observation of massive black hole binaries (MBHBs) with Pulsar Timing Arrays (PTAs) is one of the goals of gravitational wave astronomy in the coming years. Massive (>10^8 solar masses) and low-redshift (< 1.5) sources are expected to be individually resolved by up-coming PTAs, and our ability to use them as astrophysical probes will depend on the accuracy with which their parameters can be measured. In this paper we estimate the precision of such measurements using the Fisher-information-matrix formalism. We restrict to "monochromatic" sources. In this approximation, the system is described by seven parameters and we determine their expected statistical errors as a function of the number of pulsars in the array, the array sky coverage, and the signal-to-noise ratio (SNR) of the signal. At fixed SNR, the gravitational wave astronomy capability of a PTA is achieved with ~20 pulsars; adding more pulsars (up to 1000) to the array reduces the source error-box in the sky \Delta\Omega by a factor ~5 and has negligible consequences on the statistical errors on the other parameters. \Delta\Omega improves as 1/SNR^2 and the other parameters as 1/SNR. For a fiducial PTA of 100 pulsars uniformly distributed in the sky and a coherent SNR = 10, we find \Delta\Omega~40 deg^2, a fractional error on the signal amplitude of ~30% (which constraints only very poorly the chirp mass - luminosity distance combination M_c^{5/3}/D_L), and the source inclination and polarization angles are recovered at the ~0.3 rad level. The ongoing Parkes PTA is particularly sensitive to systems located in the southern hemisphere, where at SNR = 10 the source position can be determined with \Delta\Omega ~10 deg^2, but has poorer performance for sources in the northern hemisphere. (Abridged)

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