Abstract

We study the core shift effect in the parsec scale jet of the blazar 3C 454.3 using the 4.8 GHz - 36.8 GHz radio light curves obtained from three decades of continuous monitoring. From a piecewise Gaussian fit to each flare, time lags ΔtΔt between the observation frequencies νν and spectral indices αα based on peak amplitudes AA are determined. From the fit Δt∝ν1/krΔt \propto ν^{1/k_r}, kr=1.10±0.18k_r = 1.10 \pm 0.18 indicating equipartition between the magnetic field energy density and the particle energy density. From the fit A∝ναA \propto ν^α, αα is in the range −0.24-0.24 to 1.521.52. A mean magnetic field strength at 1 pc, B1=0.5±0.2B_1 = 0.5 \pm 0.2 G, and at the core, Bcore=46±16B_{\rm core} = 46 \pm 16 mG, are inferred, consistent with previous estimates. The measure of core position offset is Ωrν=6.4±2.8Ω_{rν} = 6.4 \pm 2.8 pc GHz1/kr^{1/k_r} when averaged over all frequency pairs. Based on the statistical trend shown by the measured core radius rcorer_{\rm core} as a function of νν, we infer that the synchrotron opacity model may not be valid for all cases. A Fourier periodogram analysis yields power law slopes in the range −1.6-1.6 to −3.5-3.5 describing the power spectral density shape and gives bend timescales in the range 0.52−0.66 0.52 - 0.66~yr. This result, and both positive and negative αα, indicate that the flares originate from multiple shocks in a small region. Important objectives met in our study include: the demonstration of the computational efficiency and statistical basis of the piecewise Gaussian fit; consistency with previously reported results; evidence for the core shift dependence on observation frequency and its utility in jet diagnostics in the region close to the resolving limit of very long baseline interferometry observations.

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