Abstract
The bright blazar OJ 287 is the best-known candidate for hosting a nanohertz gravitational wave (GW) emitting supermassive binary black hole (SMBBH) in the present observable universe. The binary black hole (BBH) central engine model, proposed by Lehto and Valtonen in 1996, was influenced by the two distinct periodicities inferred from the optical light curve of OJ 287. The current improved model employs an accurate general relativistic description to track the trajectory of the secondary black hole (BH) which is crucial to predict the inherent impact flares of OJ 287. The successful observations of three predicted impact flares open up the possibility of using this BBH system to test general relativity in a hitherto unexplored strong field regime. Additionally, we briefly describe an ongoing effort to interpret observations of OJ 287 in a Bayesian framework.
Highlights
It is well established that most massive active and normal galaxies contain supermassive black holes (SMBHs) at their centers [1,2,3]
The bright blazar OJ 287 is a natural candidate for hosting an supermassive binary black hole (SMBBH) at its center
Its optical LC shows quasi-periodic doubly peaked high brightness flares with a period of ∼12 years which leads to the binary black hole (BBH) central engine model for OJ 287
Summary
It is well established that most massive active and normal galaxies contain supermassive black holes (SMBHs) at their centers [1,2,3]. Many aspects of the BBH impact model, detailed in Lehto & Valtonen [8], Sundelius et al [13], were improved in the subsequent years These developments include better descriptions for the astrophysical processes causing impact outbursts [23,24], accurate general relativistic orbital description [9] as well as the addition of a large number of archived impact outburst data sets [25]. The BBH dynamics is described using the post-Newtonian approximation to general relativity that incorporates the effects of periastron advance, black hole spin, and GW emission This detailed prescription makes it possible to test general relativity in strong field regimes not tackled by relativistic binaries present in PSR J0737-3039, LIGO/VIRGO GW events, and stars orbiting the central massive BH of our galaxy [26,27,28,29].
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