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arxiv: 1010.4337 · v2 · pith:6SZLXM5Dnew · submitted 2010-10-20 · 🌌 astro-ph.HE · astro-ph.CO· astro-ph.GA· gr-qc

Pulsar timing arrays as imaging gravitational wave telescopes: angular resolution and source (de)confusion

classification 🌌 astro-ph.HE astro-ph.COastro-ph.GAgr-qc
keywords pulsardeltasourcesourcestimingarrayscharacterizedistances
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Pulsar timing arrays (PTAs) will be sensitive to a finite number of gravitational wave (GW) "point" sources (e.g. supermassive black hole binaries). N quiet pulsars with accurately known distances d_{pulsar} can characterize up to 2N/7 distant chirping sources per frequency bin \Delta f_{gw}=1/T, and localize them with "diffraction limited" precision \delta\theta \gtrsim (1/SNR)(\lambda_{gw}/d_{pulsar}). Even if the pulsar distances are poorly known, a PTA with F frequency bins can still characterize up to (2N/7)[1-(1/2F)] sources per bin, and the quasi-singular pattern of timing residuals in the vicinity of a GW source still allows the source to be localized quasi-topologically within roughly the smallest quadrilateral of quiet pulsars that encircles it on the sky, down to a limiting resolution \delta\theta \gtrsim (1/SNR) \sqrt{\lambda_{gw}/d_{pulsar}}. PTAs may be unconfused, even at the lowest frequencies, with matched filtering always appropriate.

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