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تسجيل مستخدم جديدReversals in the Direction of Polarization Rotation in OJ 287
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M.H. Cohen
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We have obtained a smooth time series for the Electric Vector Position Angle (EVPA) of the blazar OJ 287 at centimeter wavelengths, by making $pm npi$ adjustments to archival values from 1974 to 2016. The data display rotation reversals in which the EVPA rotates counter-clockwise (CCW) for 180 deg and then rotates clockwise (CW) by a similar amount. The time scale of the rotations is a few weeks to a year, and the scale for a double rotation, including the reversal, is one to three years. We have seen four of these events in 40 years. A model consisting of two successive outbursts in polarized flux density, with EVPAs counter-rotating, superposed on a steady polarized jet, can explain many of the details of the observations. Polarization images support this interpretation. The model can also help to explain similar events seen at optical wavelengths. The outbursts needed for the model can be generated by the super-magnetosonic jet model of Nakamura et al. (2010) and Nakamura and Meier (2014), which requires a strong helical magnetic field. This model produces forward and reverse pairs of fast and slow MHD waves, and the plasma inside the two fast/slow pairs rotates around the jet axis, but in opposite directions.
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The gamma-ray blazar OJ 287 was in a high activity state during December 2015 - February 2016. Coinciding with this high brightness state, we observed this source for photometry on 40 nights in R-band and for polarimetry on 9 epochs in UBVRI bands. D
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We present the results of simultaneous multi-frequency imaging observations at 22, 43, 86, and 129,GHz of OJ,287. We used the Korean VLBI Network as part of the Interferometric MOnitoring of GAmma-ray Bright active galactic nuclei (iMOGABA). The iMOG
ABA observations were performed during 31 epochs from 2013 January 16 to 2016 December 28. We also used 15,GHz OVRO and 225,GHz SMA flux density data. We analyzed four flux enhancements in the light curves. The estimated time scales of three flux enhancements were similar with time scales of $sim$50 days at two frequencies. A fourth flux enhancement had a variability timescale approximately twice as long. We found that 225,GHz enhancements led the 15,GHz enhancements by a range of 7 to 30 days in the time delay analysis. We found the fractional variability did not change with frequency between 43 and 86,GHz. We could reliably measure the turnover frequency, $ u_{rm c}$, of the core of the source in three epochs. This was measured to be in a range from 27 to 50,GHz and a flux density at the turnover frequency, $S_{rm m}$, ranging from 3-6,Jy. The derived SSA magnetic fields, $B_{rm SSA}$, are in a range from $0.157pm0.104$ to $0.255pm0.146$ mG. We estimated the equipartition magnetic field strengths to be in a range from $0.95pm0.15$ to $1.93pm0.30$ mG. The equipartition magnetic field strengths are up to a factor of 10 higher than the values of $B_{rm SSA}$. We conclude that the downstream jet may be more particle energy dominated.
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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 Leh
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