Wave Polarization of Field-Aligned Propagating Modes Using IMAGE/RPI G. Sales, X. Huang, B. Reinisch, I. Galkin Center for Atmospheric Research University of Massachusetts Lowell Field-aligned propagation (FAP) modes have been observed extensively during the lifetime of the IMAGE/RPI satellite project. Both direction-of-arrival and time delay measurements have supported the hypothesis that these modes are directed along the geomagnetic field lines from the satellite down to altitudes where reflection back to the satellite occurs. The plasmagram inversion technique, developed at UMLCAR, has determined that these "guided" modes have, primarily, extraordinary polarization. With the orthogonal antenna system on the IMAGE satellite, used first to determine the arrival angle, it is now also possible to analyze the polarization of the arriving waves over a range of frequencies. From the measured amplitude and phase on the three antennas we can reconstruct the polarization ellipse at the satellite. We have selected one of the many sequences of plasmagrams to analyze the polarization characteristics of these FAPs. These FAP modes are predominately observed for 2 < L < 5 with a median value of L = 3. Of these, approximately 40% are in sequences of more than one plasmagram and the median is between two and three plasmagrams. On Aug. 25, 2000 as IMAGE/RPI approached the plasmasphere, at L = 4.75, a sequence of three plasmagrams recorded these field aligned propagation modes over a period of 8 minutes. The sequence ended at L = 4.45, a significant travel distance for the satellite from the beginning to the end. We discuss the extensive passive and active calibration analyses that were required to determine the correct arrival-angles for these modes. Building on the success in the arrival-angle analysis we turned our attention to the polarization characteristics of the FAP modes. The RPI plasmagram is used to determine the local electron gyro frequency and the local plasma frequency. Combining these with the arrival-angle measurements and with the received amplitude and phase on the antenna system we can determine the received polarization as a function of frequency and time. _______________ Presented at the January 2002 URSI meeting, Boulder, Colorado