If all four polarisation products are measured, a full polarimetric
calibration is possible. We generally solve for the leakage terms (
and
) the gains (
and 
), a bandpass function (possibly) and calibrator Q
and U .
In the solution process, we must consider the time variability of the
various parameters. The gains vary fairly rapidly with time, and
we typically solve for them every hour or so, with the
assumption that they are steady over a solution interval of a few
minutes -- the calibrator scan. On the other hand, the leakage terms
are assumed to be steady over the entire length of the observation. Our
experience so far appears to support this. The bandpass function and
the calibrator Q
and U
can also be assumed to remain unchanged during
an observation. It is not possible to solve for a calibrators
V
(circularly polarised flux density)
However, a calibrator's V
is unlikely to be significant ( 
%).
If the calibrator is weakly polarised ( < 5%), one quantity that it is difficult to solve for is the absolute XY phase, absolute feed alignment and absolute feed ellipticity. Generally these quantites on the reference antenna has to be either assumed, or measured, or derived from observations of a strongly polarised calibrator. Unfortunately most calibrators are only weakly polarised. Fortunately, however, the alignment and ellipticity errors are small (assuming Faraday rotation is negligible). Additionally, since November 1992, the ATCA makes a good measurement of the absolute XY phase (accurate to a few degrees). If we assume that the absolute alignment and ellipiticity errors of the reference antenna are zero and that the XY phase measurements are accurate, a ``polarisation position angle calibrator'' is not needed.
The recommended strategy for calibrating ATCA data is thus to observe
a primary flux density calibrator, normally 1934-638, as well as a secondary phase calibrator
close to the source. As the polarisation of 1934-638 is known (in fact it
is 
), and the flux density is strong,
it is possible to derive polarisation leakages from it given only a short
observation (5-10 minutes). If you have good parallactic angle coverage of
the secondary, it is possible
to independently determine the polarisation leakages as well as Q
and U
for the secondary. This will be the normal case for a 12 hour observation of one source. Alternatively if there is poor parallactic angle coverage of the secondary (e.g. resulting from snapshot observations), the instrumental polarisation derived from 1934-638 can be used, and the Q and U of the secondary can still be determined.
The above strategy differs from that in the previous version of this guide. This is as prior to November 1992, the hardware to measure the XY phase produced unreliable results, particularly at 20 and 13 cm. Thus an observation of a strongly polarised calibrator was strongly advisable to determine XY phase. The strategy used for calibrating data prior to November 1992 will be somewhat different to that presented here.