Polarization Mixing Correction (Old)

Fig. 1: Parallactic angle for a range of hour angle and declination. There is a large deviation for sources whose Dec = latitude (37 degrees), when they pass directly overhead.

Explanation of Polarization Mixing

The newer 2.1-m antennas [Ants 1-8 and 12] have AzEl (azimuth-elevation) mounts (also referred to as AltAz; the terms Altitude and Elevation are used synonymously), which means that their crossed linear feeds have a constant angle relative to the horizon (the axis of rotation being at the zenith). The older 2.1-m antennas [Ants 9-11 and 13], and the 27-m antenna [Ant 14], have Equatorial mounts, which means that their crossed linear feeds have a constant angle with respect to the celestial equator, the axis of rotation being at the north celestial pole. Thus, the celestial coordinate system is tilted by the local co-latitude (complement of the latitude). This tilt results in a relative feed rotation between the 27-m antenna and the AzEl mounts, but not between the 27-m and the older equatorial mounts. This angle is called the "parallactic angle," and is given by:

$\chi =\arctan(\cos \lambda \sin A,\sin \lambda \cos E-\cos \lambda \sin E\cos A)$,

where $\lambda$ is the site latitude, $A$ is the Azimuth angle [0 north], and $E$ is the Elevation angle [0 on horizon]. This function obviously changes with position on the sky, and as we follow a celestial source (e.g. the Sun) across the sky this rotation angle is continuously changing in a surprisingly complex manner as shown in Figure 1. Note that $\chi =0$ at zero hour angle for declinations less than the local latitude (37.233 degrees at OVRO), but is $\pm \pi$ at higher declinations.

Fig. 2: Illustration of 27-m feed horns (left), 2.1-m feed package (middle), and rotation of feed orientation by parallactic angle $\chi$ (right). Note that the feeds are all oriented at 45-degrees from the horizontal at 0 hour angle, with X (= H) shown in yellow, and Y (=V) shown in blue.

The crossed linear dipole feeds on all antennas are oriented with the X-feed as shown in Figure 2, at 45-degrees from the horizontal, when the antenna is pointed at 0 hour angle. This is the view as seen looking down at the feed from the dish side, although since the feeds are at the prime focus this is the same as the view projected onto the sky. At other positions, the feeds on the AzEl antennas experience a rotation by angle $\chi$ relative to the equatorial antennas.

Because of this rotation, the normal polarization products XX, XY, YX and YY on baselines with dissimilar antennas (one AzEl and the other equatorial) become mixed. The effect of this admixture can be written by the use of Jones matrices (see Hamaker, Bregman & Sault (1996) for a complete description). Consider antenna A whose feed orientation is rotated by $\chi$, cross-correlated with antenna B with unrotated feed. The corresponding Jones matrices, acting on signal vector ${\boldsymbol {e}}_{in}=[X,Y]$ are:

${\boldsymbol {e}}_{A,out}=J_{A}{\boldsymbol {e}}_{A,in}={\begin{bmatrix}\cos \chi &\sin \chi \\-\sin \chi &\cos \chi \end{bmatrix}}{\begin{bmatrix}X_{A}\\Y_{A}\end{bmatrix}}\qquad \qquad {\boldsymbol {e}}_{B,out}=J_{B}{\boldsymbol {e}}_{B,in}={\begin{bmatrix}1&0\\0&1\end{bmatrix}}{\begin{bmatrix}X_{B}\\Y_{B}\end{bmatrix}}$

and the cross-correlation is found by taking the outer product, i.e.

$<{\boldsymbol {e}}_{A,out}\otimes {\boldsymbol {e}}_{B,out}^{*}>=J_{A}\otimes J_{B}^{*}<{\boldsymbol {e}}_{A,in}\otimes {\boldsymbol {e}}_{B,in}^{*}>$

which relates the output polarization products to the input as

${\begin{bmatrix}XX\\XY\\YX\\YY\end{bmatrix}}_{out}={\begin{bmatrix}\cos \chi &0&\sin \chi &0\\0&\cos \chi &0&\sin \chi \\-\sin \chi &0&\cos \chi &0\\0&-\sin \chi &0&\cos \chi \end{bmatrix}}{\begin{bmatrix}XX\\XY\\YX\\YY\end{bmatrix}}_{in}$

where we have dropped the subscripts and complex conjugate notation for brevity. Of course, there are other effects such as unequal gains and cross-talk between feeds that are also at play, but for now we ignore those and focus only on the effect of this polarization mixing due to the parallactic angle.

Ultimately we mean to apply the inverse of the above matrix to the measured polarization products to recover the unrotated polarization products, but for now we will content ourselves with demonstrating, in the next section, that we have the correct expressions by comparing observations with simulations.

Status of tests

Fig. 3: Comparison of observed and simulated observations for 3C84 at a single frequency, while being tracked in hour angle. In all panels, XX = blue, XY = green, YX = red, and YY = cyan.

To make the observations, we observe calibrator sources at different declincations over a broad range of hour angle. The two sources observed so far are 3C84, at declination 41 degrees, and 3C273, at declination 2 degrees. We then plot the observed amplitude and phase for each of the observed polarization products [XX, XY, YX, YY]. For this demonstration, we use the baseline of Ant1-14, where Ant1 has the rotating feed and Ant14 has the non-rotating one (with respect to the celestial coordinate system). Figure 3 shows the 3C84 observation and simulation. The upper-left panel is the observed amplitude of the four polarization products during an observation from 08:30-15:00 UT, and the upper-right panel is the corresponding phase. The lower panels are the simulation amplitude and phase, where the simulation assumed constant polarization products with Amp[XX, XY, YX, YY] = [0.15, 0, 0, 0.23], and Phase[XX, XY, YX, YY] = [3.1, 0, 0, 2.4] (radians). A noise level of 0.015 rms was added. It is clear that the amplitude simulation works very well, but the phase does not have the correct character--the only affect on phase is an abrupt 180-degree phase jump in XY and YX at 0 hour angle. Such phase jumps are seen in the data, but in addition there is a large amount of phase rotation in the observations that is not in the simulation.

Fig. 4: Same as Figure 3, but applying a phase rotation of $2|(\chi )|$.

As a test, a simulation was done applying a phase rotation based on $\chi$, as shown in Figure 4. Applying a rotation by the parallactic angle itself proved to be too small, and did not show the symmetric behavior around 0 hour angle, so the phase rotation applied in Fig. 4 is $2|(\chi )|$. It now looks about right, but there is a curvature in the simulation phase that is not really seen in the data.

Fig. 5: Same as Figure 4, for 3C273, and applying the same phase rotation of $2|(\chi )|$.

As a check, we repeated the exercise on 3C273, again applying a phase rotation of $2|(\chi )|$, with the result shown in Figure 5. As before, the amplitudes match quite well. For this different source, however, the measured phase variation is not symmetric about 0 hour angle, so the simulated phases do not match the observed ones. Finally, we instead apply a phase correction without the absolute value, i.e. just $2(\chi )$, with the result in Figure 6. Clearly this is "better," but still does not match the phase variation precisely.

Fig. 6: Same as Figure 5, but applying the same phase rotation of $2(\chi )$.

Other Possible Reasons for the Observed Phase Variations

It has been suggested that there may be some secular change in phase due to a delay error, perhaps a baseline error, or because the Az and El axes do not cross at a common point. However, the former would seem to be unlikely, because exactly the same character in the phase variations occurs on all of the AzEL antennas. And both seem unlikely for another reason--the phase variation is not frequency dependent. Figure 7 illustrates both of these facts.