2013
DOI: 10.1016/j.icarus.2013.04.023
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Refractive index and density of ammonia ice at different temperatures of deposition

Abstract: Despite its relevance in astrophysical scenarios, optical properties and density of ammonia have been scarcely studied. This work presents new data on the real part of the refractive index of ammonia at 632.8 nm and density at different temperatures of deposition from 13 K up to its desorption temperature around 110 K. The results show a significant variability for both parameters versus temperature, representing an increase of 50 % for density and a 10 % for refractive index as temperature increases in the ra… Show more

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Cited by 30 publications
(37 citation statements)
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“…The deposition was monitored using helium-neon (He-Ne) laser interferometry to determine the thickness of the ice (Hudgins et al 1993;Westley et al 1998;Fulvio et al 2009). With a refractive index of the mixed ice of 1.3±0.1 determined via the method outlined by Baratta & Palumbo (1998), Romanescu et al (2010), and Satorre et al (2013), we calculate the thickness of the deposited ice to be 500±50 nm. The ratio of ammonia (NH 3 ) to carbon monoxide (CO) after the deposition was determined to be 4±1 to 1, as calculated via infrared spectroscopy using known column densities as derived from the integrated absorption coefficients of the infrared absorption features of ammonia and carbon monoxide: the CO υ 1 band at 2139 cm −1 with 1.1×10 −17 cm mol −1 (Gerakines et al 1995) and the NH 3 υ 2 band at 1092 cm −1 with 1.7×10 −17 cm mol…”
Section: Methodsmentioning
confidence: 99%
“…The deposition was monitored using helium-neon (He-Ne) laser interferometry to determine the thickness of the ice (Hudgins et al 1993;Westley et al 1998;Fulvio et al 2009). With a refractive index of the mixed ice of 1.3±0.1 determined via the method outlined by Baratta & Palumbo (1998), Romanescu et al (2010), and Satorre et al (2013), we calculate the thickness of the deposited ice to be 500±50 nm. The ratio of ammonia (NH 3 ) to carbon monoxide (CO) after the deposition was determined to be 4±1 to 1, as calculated via infrared spectroscopy using known column densities as derived from the integrated absorption coefficients of the infrared absorption features of ammonia and carbon monoxide: the CO υ 1 band at 2139 cm −1 with 1.1×10 −17 cm mol −1 (Gerakines et al 1995) and the NH 3 υ 2 band at 1092 cm −1 with 1.7×10 −17 cm mol…”
Section: Methodsmentioning
confidence: 99%
“…(taken from Satorre et al 2013). The column densities were calculated using the integrated optical depth of the bands in the near-and mid-IR at 1070, 1625, 3373, 4480, and 4995 cm −1 .…”
Section: Nh 3 Icementioning
confidence: 99%
“…The film thickness was chosen to give a high band contrast with respect to the infrared absorptions, without saturating the bands. At such thicknesses, the ion beam passes through the film with an almost constant energy deposition of about 250 eV/Å (Zn projectile) and 130 eV/Å (Ne projectile), for a mean density of 0.73 g cm −3 for the NH 3 :CH 3 OH ice mixture (assuming a density of 0.67 g cm −3 for NH 3 ice (Satorre et al 2013) and the liquid value of 0.79 g/cm −3 for CH 3 OH). A Nicolet FTIR spectrometer (Magna 550) with a spectral resolution of 1 cm −1 was used.…”
Section: Heavy Ionsmentioning
confidence: 99%