Relative Power Levels of Multiple RPI/IMAGE Field-Aligned Magnetospheric Echoes R. F. Benson, Goddard Space Flight Center, Greenbelt, MD 20771, 301-286-4037, u2rfb@lepvax.gsfc.nasa.gov; S. F. Fung, Goddard Space Flight Center, Greenbelt, MD 20771, 301-286-6301, fung@nssdca.gsfc.nasa.gov; J. L. Green, Goddard Space Flight Center, Greenbelt, MD 20771, 301-286-7354, green@nssdca.gsfc.nasa.gov; B. W. Reinisch, University of Massachusetts Lowell, Lowell, MA 01854, 978-934-4903, bodo_reinisch@uml.edu The Radio Plasma Imager (RPI) (B. W. Reinisch et al., Geophys. Res Lett., 28, 1167-1170, 2001) on the Imager for Magnetopause-to-Aurora Global Exploration (IMAGE) satellite (J. L. Burch, EOS, Trans. AGU, 82, 241 and 245, 2001) often detects discrete long-range echoes when IMAGE is located in the general vicinity of the plasmapause. The long time delays indicate that these echoes, which extend over a few hundred kilohertz up to at least 600 kHz, do not correspond to signal returns from the nearby plasmapause. Some echoes include traces that do not extend toward zero virtual range. These "floating" traces often have an "epsilon" shape similar to those observed at low altitudes in the topside ionosphere by ISIS 1 when it was immersed within equatorial plasma bubbles. The ISIS 1 observations were interpreted in terms of ducted propagation along field-aligned electron-density irregularities (FAI) that were maintained from one hemisphere to the other (P. L. Dyson and R. F. Benson, Geophys. Res Lett., 5, 795-798, 1978) following the earlier work based on Alouette 1 observations at higher (1,000 km) altitude (D. B. Muldrew, J. Geophys. Res., 68, 5355-5370, 1963). An investigation of the relative power levels of these magnetospheric epsilon signatures was carried out in order to determine the degree of signal loss between the various echo components (which are attributed to different magnetospheric path lengths). At each frequency, the power level corresponding to the signal received on the x dipole antenna (the same one used for transmission) for each echo component was recorded. The results indicate that the path length of the signal is not a major contributor to differences observed in the received power among the echo components. Thus the magnetospheric "epsilon" shaped echoes appear to be due to nearly loss-free propagation along FAI that are maintained from one hemisphere to the other in the vicinity of the plasmapause in a manner similar to their ionospheric counterparts.