The Red Edge Problem in asteroid band parameter analysis

Meteoritics and Planetary Science Wiley 51:4 (2016) 806-817

Authors:

Sean S Lindsay, Tasha L Dunn, Joshua P Emery, Neil E Bowles

Inflight Radiometric Calibration of New Horizons' Multispectral Visible Imaging Camera (MVIC)

(2016)

Authors:

CJA Howett, AH Parker, CB Olkin, DC Reuter, K Ennico, WM Grundy, AL Graps, KP Harrison, HB Throop, MW Buie, JR Lovering, SB Porter, HA Weaver, LA Young, SA Stern, RA Beyer, RP Binzell, BJ Buratti, AF Cheng, JC Cook, DP Cruikshank, CM Dalle Ore, AM Earle, DE Jennings, IR Linscott, AW Lunsford, J Wm Parker, S Phillippe, S Protopapa, E Quirico, PM Schenk, B Schmitt, KN Singer, JR Spencer, JA Stansberry, CCC Tsang, GE Weigle, AJ Verbiscer

New temperature and pressure retrieval algorithm for high-resolution infrared solar occultation spectroscopy: analysis and validation against ACE-FTS and COSMIC

Atmospheric Measurement Techniques Copernicus Publications 9:3 (2016) 1063-1082

Authors:

Kevin S Olsen, Geoffrey C Toon, Chris D Boone, Kimberly Strong

Simulated stellar kinematics studies of high-redshift galaxies with the HARMONI Integral Field Spectrograph

Monthly Notices of the Royal Astronomical Society Oxford University Press 458:3 (2016) 2405-2422

Authors:

S Kendrew, S Zieleniewski, RCW Houghton, Niranjan Thatte, J Devriendt, M Tecza, F Clarke, K O'Brien, B Häussler

Abstract:

We present a study into the capabilities of integrated and spatially resolved integral field spectroscopy of galaxies at z = 2–4 with the future HARMONI spectrograph for the European Extremely Large Telescope (E-ELT) using the simulation pipeline, HSIM. We focus particularly on the instrument's capabilities in stellar absorption line integral field spectroscopy, which will allow us to study the stellar kinematics and stellar population characteristics. Such measurements for star-forming and passive galaxies around the peak star formation era will provide a critical insight into the star formation, quenching and mass assembly history of high-z, and thus present-day galaxies. First, we perform a signal-to-noise study for passive galaxies at a range of stellar masses for z = 2–4, assuming different light profiles; for this population, we estimate that integrated stellar absorption line spectroscopy with HARMONI will be limited to galaxies with M* ≳ 1010.7 M⊙. Secondly, we use HSIM to perform a mock observation of a typical star-forming 1010 M⊙ galaxy at z = 3 generated from the high-resolution cosmological simulation NUTFB. We demonstrate that the input stellar kinematics of the simulated galaxy can be accurately recovered from the integrated spectrum in a 15-h observation, using common analysis tools. Whilst spatially resolved spectroscopy is likely to remain out of reach for this particular galaxy, we estimate HARMONI's performance limits in this regime from our findings. This study demonstrates how instrument simulators such as HSIM can be used to quantify instrument performance and study observational biases on kinematics retrieval; and shows the potential of making observational predictions from cosmological simulation output data.

Thermal properties of Rhea's poles: Evidence for a meter-deep unconsolidated subsurface layer

Icarus Elsevier 272 (2016) 140-148

Authors:

Cja Howett, Jr Spencer, T Hurford, A Verbiscer, M Segura

Abstract:

Cassini's Composite Infrared Spectrometer (CIRS) observed both of Rhea's polar regions during a close (2000 km) flyby on 9th March 2013 during orbit 183. Rhea's southern pole was again observed during a more distant (51,000 km) flyby on 10th February 2015 during orbit 212. The results show Rhea's southern winter pole is one of the coldest places directly observed in our Solar System: surface temperatures of 25.4 ± 7.4 K and 24.7 ± 6.8 K are inferred from orbit 183 and 212 data, respectively. The surface temperature of the northern summer pole inferred from orbit 183 data is warmer: 66.6 ± 0.6 K. Assuming the surface thermophysical properties of the two polar regions are comparable then these temperatures can be considered a summer and winter seasonal temperature constraint for the polar region. Orbit 183 will provide solar longitude (LS) coverage at 133° and 313° for the summer and winter poles respectively, while orbit 212 provides an additional winter temperature constraint at LS 337°. Seasonal models with bolometric albedo values between 0.70 and 0.74 and thermal inertia values between 1 and 46 J m−2 K−1 s−1/2 (otherwise known as MKS units) can provide adequate fits to these temperature constraints (assuming the winter temperature is an upper limit). Both these albedo and thermal inertia values agree within the uncertainties with those previously observed on both Rhea's leading and trailing hemispheres. Investigating the seasonal temperature change of Rhea's surface is particularly important, as the seasonal wave is sensitive to deeper surface temperatures (∼tens of centimeters to meter depths) than the more commonly reported diurnal wave (typically less than a centimeter), the exact depth difference dependent upon the assumed surface properties. For example, if a surface porosity of 0.5 and thermal inertia of 25 MKS is assumed then the depth of the seasonal thermal wave is 76 cm, which is much deeper than the ∼0.5 cm probed by diurnal studies of Rhea (Howett et al., 2010). The low thermal inertia derived here implies that Rhea's polar surfaces are highly porous even at great depths. Analysis of a CIRS focal plane 1 (10–600 cm−1) stare observation, taken during the orbit 183 encounter between 16:22:33 and 16:23:26 UT centered on 71.7°W, 58.7°S provides the first analysis of a thermal emissivity spectrum on Rhea. The results show a flat emissivity spectrum with negligible emissivity features. A few possible explanations exist for this flat emissivity spectrum, but the most likely for Rhea is that the surface is both highly porous and composed of small particles (<∼50 µm).