PKS 1413+135 : writeup of precessing jet models

The bends in the jet of PKS 1413+135 suggests a precessing jet model. We have attempted to fit a kinematic helical jet model to the western jet (which we believe is beamed towards us) using the methods of Steffen et al (A&A 302, 335, 1995). The model predicts the form of the ridge of emission. The fitting minimized the chi-squared of the difference between the observed and model ridge.

The observed emission ridge was derived from the 15 GHz map of January 4, 2001, by the following method (reference ??): Slices through the image are taken along circular arcs centered at the core position, smoothed by ???, and the maximum flux density along each arc was the location of the emission ridge at that radius.

To estimate the range of model parameters to be searched, we used the measured apparent speeds of components E2, F1, and G, derived by K04, of v/c = 3.9, 5.8, and 7.1. The intrinsic speed, Beta (=v/c) is related to the inclination angle to the line of sight, i, and the apparent speed, Beta_app, as follows:

Beta = Beta_app/[sin(i) + Beta_app * cos(i)]

The curves of Beta versus i are plotted in Figure 8?? for the three values of Beta_app. Also plotted is the curve for Beta_app = 3.9-1.2 = 2.7, subtracting the 1-sigma estimated error. The largest range in Beta and i are allowed by the lowest apparent speed. Thus the allowed range of inclinations is about 0 to 40 degrees, and the the intrinsic Beta is about 0.93 to 1.0.

We have performed a large number (10**6) of simulations covering this allowed range of parameter space. The parameters were optimized by chi-squared minimization of the position differences of the jet ridge data and closest model position. The best fit model conserved angular momentum, linear momentum, and jet opening angle. A common feature of these models is that spacing of helical knots is shorter close to the AGN core, then increases with distance from the core until reaching the "linear" region of the jet, commonly seen for large angular size double lobed radio sources. The model of PKS 1413+135 shares this feature, although the ridge-line data appear straighter than the model.
[or does the model appear straighter than the ridge-line data??]
Figure 8B shows the best-fitting model superimposed on the 15 GHz map of the January 4, 2001 data.

Model Fit Results

The optimum model parameters are as follows:
Inclination to the line of sight 34.5 °
Jet opening half angle 1.2 °
Jet launch speed v/c = 0.7
Phase angle rotation rate -220.6 ° /mas
Size of jet launch region 0.13 mas
Jet orientation on the sky 23.8 °

The rather slow launch rate (v/c = 0.7) and large inclination angle (34.5°) would seem to be inconsistent with the apparent speeds of the faster components. Are components F and G speeding up some time after being launched?