ICE IN THE FAR-IR & DIVINER 3. Far-IR Subteam: Ben Greenhagen, Christopher Edwards, Dan McCleese Additional Contributions: Tim Schofield & Paul Hayne

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ICE IN THE FAR-IR & DIVINER 3 Far-IR Subteam: Ben Greenhagen, Christopher Edwards, Dan McCleese Additional Contributions: Tim Schofield & Paul Hayne

WHY FAR IR? ~45µm fundamental ice feature (e.g. Moore & Hudson, 1992) Large body of literature for water ice and other materials related to icy moons Also shorter wavelength features but may be confused with silicate bands Passive spectroscopy technique No illumination source needed for permanently shadowed regions (20-120 K surfaces) Ability to estimate areal fraction of exposed ice based on spatial mixtures Likely looking at macro-scale (>250-1000m) ice deposits (Paige et al., 2010; Morgan & Shemansky, 1991) Can t say anything about sub-surface ice or equatorial OH mobility

WHAT DOES THIS TECHNIQUE ANSWER? Extent of areal mapping the ~45µm infrared ice feature ~45 µm absorption feature is still present (varies to longer λ with decreasing crystallinity) if: Deposited at various Ts (40-160K) Deposited at low T (14K) and warmed Deposited at high (160K) and cooled

Ice Deposited at Indicated Temperatures

Ice Deposited at 14K and Warmed (Amorphous)

Ice Deposited at 160K and Cooled (Crystalline)

WHAT DOES THIS TECHNIQUE ANSWER? Extent of areal mapping the ~45µm infrared ice feature ~45 µm absorption feature is still present (varies to longer λ with decreasing crystallinity) if: Deposited at various Ts (40-160K) Deposited at low T (14K) and warmed Deposited at high (160K) and cooled Also significant particle size effects

PARTICLE SIZE EFFECTS

WHAT DOES THIS TECHNIQUE ANSWER? Extent of areal mapping the ~45µm infrared ice feature ~45 µm absorption feature is still present (varies to longer λ with decreasing crystallinity) if: Deposited at various Ts (40-160K) Deposited at low T (14K) and warmed Deposited at high (160K) and cooled Also significant particle size effects Fortunately most silicate absorption bands are <40 microns but there is some overlap Mitigate with differential observations of warm areas

FIR SPECTRA OF LUNAR SOILS

SUMMARY OF FIR ICE Compounding effects of particle size and crystallinity Can we send a FIR instrument now? Still need to know: What is the form of the ice? (crystalline/amorphous, thin coating, slab, etc.) System performance (next slides) Lab studies of ice are necessary for both FIR/NIR to really answer these questions JPL facilities exist to begin to answer these questions to a level where we can be confident of a mission designed to map these features

DIVINER 3 (DIVINER-CUBED) Is there a simple, very low cost ($1-5M) cubesat concept that could leverage our knowledge of water ice in the FIR to answer (or significantly constrain) a fundamental question? Mars Climate Sounder (MCS) and the Diviner Lunar Radiometer offer a high heritage foundation for the development of a low cost, highly capable instrument Some flight spare components available (e.g. detectors, filters) Build-to-print for other components (e.g. focal plane arrays, optics) Phase A-D costs for MCS and Diviner $M 20ish

DIVINER 3 :A HIGHLY CAPABLE INSTRUMENT 1 month of Diviner data collected at summer solstice

DIVINER 3 ACCOMMODATION The metering structure (optics) for a single MCS/Diviner Telescope is small enough to fit in a single 1U structure Electronics would need to be collocated with cubesat avionics to fit within 3U cube Use Diviner ch. 7 & 8 (26-41 μm & 50-100 μm) filters and procure a single new filter on FIR water ice band

Effective Emissivity DIVINER 3 PERFORMANCE MODEL 1 Amorphous Ice @ 100K (200m spatial res) 0.995 0.99 0.985 0.98 0.975 26-41 μm Diviner Ch. 7 0.97 0.965 0.96 0.955 48-58 μm New Channel 50-100 μm Diviner Ch. 8 0.95 20 30 40 50 60 70 80 90 100 Wavelength (μm)

Effective Emissivity DIVINER 3 PERFORMANCE MODEL 1 Amorphous Ice @ 100K (1km spatial res) 0.995 0.99 0.985 0.98 0.975 26-41 μm Diviner Ch. 7 0.97 0.965 0.96 0.955 48-58 μm New Channel 50-100 μm Diviner Ch. 8 0.95 20 30 40 50 60 70 80 90 100 Wavelength (μm)

Effective Emissivity DIVINER 3 PERFORMANCE MODEL 1 Amorphous Ice @ 100K (3km spatial res) 0.995 0.99 0.985 0.98 0.975 26-41 μm Diviner Ch. 7 0.97 0.965 0.96 0.955 48-58 μm New Channel 50-100 μm Diviner Ch. 8 0.95 20 30 40 50 60 70 80 90 100 Wavelength (μm)

Effective Emissivity DIVINER 3 NEW PASSBAND OPTIMIZATION 1 Amorphous Ice @ 100K (3km spatial res) 0.995 0.99 0.985 Integrated Band Depth Style 0.98 0.975 0.97 0.965 0.96 0.955 Plan to vary the position and width of new channel Will use interpolated temperature-dependent ice spectra and look at range of temperatures 0.95 20 30 40 50 60 70 80 90 100 Wavelength (μm)

DIVINER 3 CALIBRATIONS Space views for calibrations during most of orbit Nadir-pointing, highest resolution observations at the south pole Other schemes involve pitching spacecraft to point at N pole and/or mid-latitudes

FIR & DIVINER 3 CONCLUSIONS There are diagnostic water-ice spectral bands in the FIR that could be used to detect the presence of and constrain the grain size and crystallinity of water-ice Diviner 3 could fit the role of a very low cost, highly capable instrument Other concepts may be even more capable albeit at higher cost/complexity What is the value of a very low cost mission that addresses a specific question vs. a larger concept? This KISS Study needs to decide if it s better to advance the study of lunar volatiles by significantly advancing a single low cost concept, advancing several low cost concepts, improving the technical foundations of a variety of techniques, or promoting a larger concept