Detection of a hydrogen corona at Callisto

Journal of Geophysical Research: Planets (2017)

Authors:

L Roth, J Alday, TM Becker, N Ivchenko, KD Retherford

Inflight radiometric calibration of New Horizons’ Multispectral Visible Imaging Camera (MVIC)

Icarus Elsevier BV 287 (2017) 140-151

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 Binzel, Bj Buratti, Af Cheng, Jc Cook, Dp Cruikshank, Cm Dalle Ore, Am Earle, De Jennings, Ir Linscott, Aw Lunsford, Jwm Parker, S Phillippe, S Protopapa, E Quirico, Pm Schenk, B Schmitt, Kn Singer, Jr Spencer, Ja Stansberry, Ccc Tsang, Ge Weigle, Aj Verbiscer

Abstract:

© 2016 Elsevier Inc. We discuss two semi-independent calibration techniques used to determine the inflight radiometric calibration for the New Horizons’ Multi-spectral Visible Imaging Camera (MVIC). The first calibration technique compares the measured number of counts (DN) observed from a number of well calibrated stars to those predicted using the component-level calibration. The ratio of these values provides a multiplicative factor that allows a conversation between the preflight calibration to the more accurate inflight one, for each detector. The second calibration technique is a channel-wise relative radiometric calibration for MVIC's blue, near-infrared and methane color channels using Hubble and New Horizons observations of Charon and scaling from the red channel stellar calibration. Both calibration techniques produce very similar results (better than 7% agreement), providing strong validation for the techniques used. Since the stellar calibration described here can be performed without a color target in the field of view and covers all of MVIC's detectors, this calibration was used to provide the radiometric keyword values delivered by the New Horizons project to the Planetary Data System (PDS). These keyword values allow each observation to be converted from counts to physical units; a description of how these keyword values were generated is included. Finally, mitigation techniques adopted for the gain drift observed in the near-infrared detector and one of the panchromatic framing cameras are also discussed.

Physical state and distribution of materials at the surface of Pluto from New Horizons LEISA imaging spectrometer

Icarus Elsevier 287 (2017) 229-260

Authors:

B Schmitt, S Philippe, WM Grundy, DC Reuter, R Côte, E Quirico, S Protopapa, LA Young, RP Binzel, JC Cook, DP Cruikshank, CM Dalle Ore, AM Earle, K Ennico, CJA Howett, DE Jennings, IR Linscott, AW Lunsford, CB Olkin, AH Parker, Parker, KN Singer, JR Spencer, JA Stansberry, SA Stern, CCC Tsang, AJ Verbiscer, HA Weaver, the New Horizons Science Team

Pluto’s global surface composition through pixel-by-pixel Hapke modeling of New Horizons Ralph/LEISA data

Icarus Elsevier 287 (2017) 218-228

Authors:

S Protopapa, WM Grundy, DC Reuter, DP Hamilton, CM Dalle Ore, JC Cook, DP Cruikshank, B Schmitt, S Philippe, E Quirico, RP Binzel, AM Earle, K Ennico, CJA Howett, AW Lunsford, CB Olkin, A Parker, KN Singer, A Stern, AJ Verbiscer, HA Weaver, LA Young, the New Horizons Science Team

A precise optical transmission spectrum of the inflated exoplanet WASP-52b

Monthly Notices of the Royal Astronomical Society Oxford University Press 470:1 (2017) 742-754

Authors:

T Louden, PJ Wheatley, Patrick Irwin, J Kirk, I Skillen

Abstract:

We have measured a precise optical transmission spectrum forWASP-52b, a highly inflated hot Jupiter with an equilibrium temperature of 1300 K. Two transits of the planet were observed spectroscopically at low resolution with the auxiliary-port camera on the William Herschel Telescope, covering a wide range of 4000-8750 Å. We use a Gaussian process approach to model the correlated noise in the multiwavelength light curves, resulting in a high precision relative transmission spectrum with errors of the order of a pressure scaleheight.We attempted to fit a variety of different representative model atmospheres to the transmission spectrum, but did not find a satisfactory match to the entire spectral range. For the majority of the covered wavelength range (4000-7750 Å), the spectrum is flat, and can be explained by an optically thick and grey cloud layer at 0.1 mbar, but this is inconsistent with a slightly deeper transit at wavelengths > 7750 Å.We were not able to find an obvious systematic source for this feature, so this opacity may be the result of an additional unknown absorber.