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arXiv 1003.0677astro-ph.COgr-qc
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利用脉冲星定时阵的引力波观测测量大质量黑洞二元系统的参数

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

Alberto Sesana, Alberto Vecchio

摘要:

利用脉冲星定时阵观测大质量黑洞双星是引力波天文学未来的目标之一。大质量(>10^8太阳质量)和低红移(< 1.5)源预计将被即将到来的PTA单独分辨,我们将它们用作天体物理探测器的能力将取决于它们参数测量的准确性。在本文中,我们估计这样的测量精度使用费舍尔信息矩阵形式主义。我们仅限于“单色”光源。在这种近似下,系统由七个参数描述,我们确定它们的预期统计误差作为阵列中的天线数量、阵列天空覆盖范围和信号的信噪比(SNR)的函数。在固定信噪比下,PTA的引力波天文学能力是用~20个微扰子实现的;在阵列中增加更多的微扰子(最多1000个)将天空中的源误差框ΔΩ减小到~5倍,并且对其他参数的统计误差的影响可以忽略不计。ΔΩ提高为1/SNR ^2,其他参数提高为1/SNR。对于天空中均匀分布的100个双星的基准PTA和相干SNR = 10,我们发现ΔΩ约为40 ° ^[2],信号幅度的分数误差约为30%(这对啁啾质量-光度距离组合M_c^{5/3}/D_L的约束很差),源倾角和偏振角恢复到约0.3 rad水平。正在进行的帕克斯PTA对位于南半球的系统特别敏感,在SNR = 10时,可以用ΔΩ~10 deg^2确定源位置,但对北半球的源性能较差。(节录)

英文摘要:

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 ΔΩby a factor ~5 and has negligible consequences on the statistical errors on the other parameters. ΔΩimproves 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 ΔΩ~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 ΔΩ~10 deg^2, but has poorer performance for sources in the northern hemisphere. (Abridged)

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