E. Lellouch, I. Wong, P. Lavvas, T. Bertrand, G. Villanueva, J. Stansberry, B. Holler, N. Pinilla-Alonso, F. Merlin, A. C. Souza-Feliciano, K. Murray
{"title":"Pluto’s atmosphere gas and haze composition from JWST/MIRI spectroscopy","authors":"E. Lellouch, I. Wong, P. Lavvas, T. Bertrand, G. Villanueva, J. Stansberry, B. Holler, N. Pinilla-Alonso, F. Merlin, A. C. Souza-Feliciano, K. Murray","doi":"10.1051/0004-6361/202453619","DOIUrl":null,"url":null,"abstract":"<i>Context.<i/> Pluto possesses a tenuous, time-variable, N<sub>2<sub/>-dominated atmosphere, with extensive haze. Previous spectroscopic observations from the ground at near-infrared (NIR) and submillimeter (submm) wavelengths and New Horizons in the ultraviolet (UV) have revealed a Titan-like atmosphere with rich N<sub>2<sub/>-CH<sub>4<sub/> photochemistry. The mid-infrared (MIR) range of Pluto’s spectrum, however, has remained out of reach thus far.<i>Aims.<i/> Taking advantage of JWST sensitivity, our goal is to obtain new insights into Pluto’s atmospheric gas and haze composition using mid-IR spectroscopy.<i>Methods.<i/> In May 2023, we used JWST/MIRI MRS to acquire a high signal-to-noise (S/N) spectrum of Pluto over 4.9–27 μm, finally opening up the MIR spectral range for Pluto. The data were analyzed with a standard radiative transfer code, including the solar and thermal components, and the gas and haze emission, using gas vertical distributions from photochemical models as templates.<i>Results.<i/> The Pluto spectrum consists of the superposition of solar light reflected off Pluto’s surface, surface thermal emission, gas thermal and non-thermal emission, and haze emission. The solar reflected component shows absorption by CH<sub>4<sub/>, CH<sub>3<sub/>D, and C<sub>2<sub/>H<sub>4<sub/> surface ices. Spectral signatures of C<sub>2<sub/>H<sub>6<sub/>, C<sub>2<sub/>H<sub>2<sub/>, CH<sub>3<sub/>C<sub>2<sub/>H, and C<sub>4<sub/>H<sub>2<sub/> gases are strongly detected over 12–16 μm, broadly probing the stratopause region (altogether spanning 15–100 km). Unexpectedly, we also detect fluorescence (non-LTE) emission from gas CH<sub>4<sub/> (<i>ν<i/><sub>4<sub/> and hot bands) and CH<sub>3<sub/>D (<i>ν<i/><sub>6<sub/> band) in the 7–9 μm range, indicating excitation temperatures that are much higher than Pluto’s atmosphere kinetic temperature. The C<sub>2<sub/>H<sub>6<sub/> abundance agrees very well with photochemical models, but those of CH<sub>3<sub/>C<sub>2<sub/>H, and C<sub>4<sub/>H<sub>2<sub/> are about five and ten times lower than model predictions, respectively. The C<sub>2<sub/>H<sub>2<sub/> 12.9–14.7 μm emission (<i>ν<i/><sub>5<sub/>) is imperfectly fit and may point to a less steep C<sub>2<sub/>H<sub>2<sub/> profile than in model predictions or (perhaps more likely) to non-LTE effects on this band. Remarkably, C<sub>2<sub/>HD is detected at 14.75 μm, yielding a (D/H)<sub>C<sub>2<sub/>H<sub>2<sub/><sub/> ratio equal to (3±1) terrestrial. Also, HCN has been tentatively observed and upper limits on several other gases (C<sub>2<sub/>H<sub>4<sub/>, C<sub>3<sub/>H<sub>8<sub/>, C<sub>6<sub/>H<sub>6<sub/>, HC<sub>3<sub/>N, and CO<sub>2<sub/>) are obtained. The haze emission is clearly present over 13–20 μm and characterized by emission peaks at 15.45 μm, 14.58 μm, and maybe 13.60 μm. The haze spectrum is very different from Titan’s and points to the presence of pure or mixed ices (e.g., C<sub>4<sub/>H<sub>2<sub/>, C<sub>6<sub/>H<sub>6<sub/>), as previously proposed.<i>Conclusions.<i/> The spectacular JWST MIRI spectrum is giving us a new look at Pluto’s atmosphere. An improved non-LTE modeling of the fluorescent emissions (CH<sub>4<sub/>, CH<sub>3<sub/>D, and possibly C<sub>2<sub/>H<sub>2<sub/>) and of the ice features is expected to yield a broader view of Pluto’s D/H ratio in different gases (CH<sub>4<sub/>, C<sub>2<sub/>H<sub>2<sub/>) and phases (gas and solid). This would bear key information on Pluto’s ice origin and evolution.","PeriodicalId":8571,"journal":{"name":"Astronomy & Astrophysics","volume":"6 1","pages":""},"PeriodicalIF":5.4000,"publicationDate":"2025-04-15","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Astronomy & Astrophysics","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1051/0004-6361/202453619","RegionNum":2,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"ASTRONOMY & ASTROPHYSICS","Score":null,"Total":0}
引用次数: 0
Abstract
Context. Pluto possesses a tenuous, time-variable, N2-dominated atmosphere, with extensive haze. Previous spectroscopic observations from the ground at near-infrared (NIR) and submillimeter (submm) wavelengths and New Horizons in the ultraviolet (UV) have revealed a Titan-like atmosphere with rich N2-CH4 photochemistry. The mid-infrared (MIR) range of Pluto’s spectrum, however, has remained out of reach thus far.Aims. Taking advantage of JWST sensitivity, our goal is to obtain new insights into Pluto’s atmospheric gas and haze composition using mid-IR spectroscopy.Methods. In May 2023, we used JWST/MIRI MRS to acquire a high signal-to-noise (S/N) spectrum of Pluto over 4.9–27 μm, finally opening up the MIR spectral range for Pluto. The data were analyzed with a standard radiative transfer code, including the solar and thermal components, and the gas and haze emission, using gas vertical distributions from photochemical models as templates.Results. The Pluto spectrum consists of the superposition of solar light reflected off Pluto’s surface, surface thermal emission, gas thermal and non-thermal emission, and haze emission. The solar reflected component shows absorption by CH4, CH3D, and C2H4 surface ices. Spectral signatures of C2H6, C2H2, CH3C2H, and C4H2 gases are strongly detected over 12–16 μm, broadly probing the stratopause region (altogether spanning 15–100 km). Unexpectedly, we also detect fluorescence (non-LTE) emission from gas CH4 (ν4 and hot bands) and CH3D (ν6 band) in the 7–9 μm range, indicating excitation temperatures that are much higher than Pluto’s atmosphere kinetic temperature. The C2H6 abundance agrees very well with photochemical models, but those of CH3C2H, and C4H2 are about five and ten times lower than model predictions, respectively. The C2H2 12.9–14.7 μm emission (ν5) is imperfectly fit and may point to a less steep C2H2 profile than in model predictions or (perhaps more likely) to non-LTE effects on this band. Remarkably, C2HD is detected at 14.75 μm, yielding a (D/H)C2H2 ratio equal to (3±1) terrestrial. Also, HCN has been tentatively observed and upper limits on several other gases (C2H4, C3H8, C6H6, HC3N, and CO2) are obtained. The haze emission is clearly present over 13–20 μm and characterized by emission peaks at 15.45 μm, 14.58 μm, and maybe 13.60 μm. The haze spectrum is very different from Titan’s and points to the presence of pure or mixed ices (e.g., C4H2, C6H6), as previously proposed.Conclusions. The spectacular JWST MIRI spectrum is giving us a new look at Pluto’s atmosphere. An improved non-LTE modeling of the fluorescent emissions (CH4, CH3D, and possibly C2H2) and of the ice features is expected to yield a broader view of Pluto’s D/H ratio in different gases (CH4, C2H2) and phases (gas and solid). This would bear key information on Pluto’s ice origin and evolution.
期刊介绍:
Astronomy & Astrophysics is an international Journal that publishes papers on all aspects of astronomy and astrophysics (theoretical, observational, and instrumental) independently of the techniques used to obtain the results.