Polarization of L-Narrow

During September 2000 extensive observations were made to obtain complete characterizations of the polarization properties of all of Arecibo's receiver systems. A memo written by Carl Heiles, et.al (and available here) gives a complete description of the Mueller matrices used and the results. On this page a summary of the L-Narrow results are given.

The LBN system uses a turnstile for its orthomode transducer, which is a relatively narrow-band device; it is tuned to give good dual circular near 1420 MHz, but as one departs from this frequency the polarization becomes dual elliptical. Additionally, the LBN does not have a correlated cal. This means that the Mueller Matrix parameter (psi) has no meaning.

The LBN system is commonly used over a large frequency range. A turnstile is a narrow-band device, and over this range the polarization changes from linear to circular and back again. The solid lines in Figure 1 (below) exhibit the frequency dependence of DeltaG, alpha, epsilon, and phi for the 25 MHz band centered at four frequencies. These particular data were derived from the source B0017+154; we obtained data for two additional sources, and the results are very close. The dashed lines are our adopted analytic expression, which are defined by
DeltaG = 0.034 - 1.78X10-4 f15 + 3.27X10-6 f152
alpha = 47.74 - 0.363 f15
epsilon = 0.0028 + 1.38X10-5
f15 + 1.31X10-6f152
phi = 21 + 1.02 f15
where f15 = f - 1415MHz and angles are in degrees.

The linear dependence of alpha on f15$ is just what's expected for a turnstile junction. However, the variation of epsilon is remarkably complicated, varying rapidly with frequency as one goes away from the 1400 MHz center frequency, and we do not understand the reason. The scatter in phi $ for the 1375 MHz spectrum simply reflects the uncertainty in the angle, which is large because epsilon is small. Of course, DeltaG simply reflects inaccurate relative cal values and not the properties of the turnstile itself.


Figure 1.
Mueller matrix parameters versus frequency for LBN, together with the adopted analytic approximations from the above equations


Figure 2.
Fractional polarization (really gaina-gainb)/(gaina+gainb) since the outputs are circular) versus azimuth and zenith angle, by source




Last Updated Tuesday, 28-Aug-2001 11:26:45 AST