49th Lunar and Planetary Science Conference 2018 (LPI Contrib. No. 2083) 1585.pdf 1 MINI-RF BISTATIC OBSERVATIONS OF COPERNICAN CRATER EJECTA. A. M. Stickle , G. W. Patterson1, J. T. S. Cahill1, P. Prem1, and the Mini-RF team 1Johns Hopkins Applied Physics Laboratory, 11100 Johns Hopkins Rd., Laurel, MD, USA 20723,
[email protected]. Introduction: The Mini-RF instrument onboard Observations: A common product derived from the NASA’s Lunar Reconnaissance Orbiter (LRO) is cur- Stokes parameters is the Circular Polarization Ratio rently acquiring bistatic radar data of the lunar surface (CPR), or µc = (S1-S4)/(S1+S4). CPR information is com- at both S-band (12.6 cm) and X-band (4.2 cm) wave- monly used in analyses of planetary radar data [4-7], and lengths in an effort to understand the scattering proper- is a representation of surface roughness at the wave- ties of lunar terrains as a function of bistatic angle. Pre- length scale of the radar (i.e., surfaces that are smoother vious work, at optical wavelengths, has demonstrated at the wavelength scale will have lower CPR values and that the material properties of lunar regolith can be sen- surfaces that are rougher will have higher CPR values). sitive to variations in phase (bistatic) angle [1-3]. This High CPR values can also serve as an indicator of the sensitivity gives rise to the lunar opposition effect and presence of water ice [9]. likely involves contributions from shadow hiding at low As part of the Mini-RF bistatic observation cam- phase angles and coherent backscatter near zero phase paign, CPR information for a variety lunar terrains is be- [1].