Abstract
Brown dwarfs serve as ideal laboratories for studying the atmospheres of giant exoplanets on wide orbits, as the governing physical and chemical processes within them are nearly identical1,2. Understanding the formation of gas-giant planets is challenging, often involving the endeavour to link atmospheric abundance ratios, such as the carbon-to-oxygen (C/O) ratio, to formation scenarios3. However, the complexity of planet formation requires further tracers, as the unambiguous interpretation of the measured C/O ratio is fraught with complexity4. Isotope ratios, such as deuterium to hydrogen and 14N/15N, offer a promising avenue to gain further insight into this formation process, mirroring their use within the Solar System5–7. For exoplanets, only a handful of constraints on 12C/13C exist, pointing to the accretion of 13C-rich ice from beyond the CO iceline of the disks8,9. Here we report on the mid-infrared detection of the 14NH3 and 15NH3 isotopologues in the atmosphere of a cool brown dwarf with an effective temperature of 380 K in a spectrum taken with the Mid-Infrared Instrument (MIRI) of JWST. As expected, our results reveal a 14N/15N value consistent with star-like formation by gravitational collapse, demonstrating that this ratio can be accurately constrained. Because young stars and their planets should be more strongly enriched in the 15N isotope10, we expect that 15NH3 will be detectable in several cold, wide-separation exoplanets.
Originalsprache | Englisch |
---|---|
Seiten (von - bis) | 263-266 |
Seitenumfang | 4 |
Fachzeitschrift | Nature |
Jahrgang | 624 |
Ausgabenummer | 7991 |
DOIs | |
Publikationsstatus | Veröffentlicht - 14 Dez. 2023 |
ÖFOS 2012
- 103003 Astronomie
- 103004 Astrophysik
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in: Nature, Band 624, Nr. 7991, 14.12.2023, S. 263-266.
Veröffentlichungen: Beitrag in Fachzeitschrift › Artikel › Peer Reviewed
TY - JOUR
T1 - 15NH3 in the atmosphere of a cool brown dwarf
AU - Barrado, David
AU - Mollière, Paul
AU - Patapis, Polychronis
AU - Min, Michiel
AU - Tremblin, Pascal
AU - Ardevol Martinez, Francisco
AU - Whiteford, Niall
AU - Vasist, Malavika
AU - Argyriou, Ioannis
AU - Samland, Matthias
AU - Lagage, Pierre Olivier
AU - Decin, Leen
AU - Waters, Rens
AU - Henning, Thomas
AU - Morales-Calderón, María
AU - Guedel, Manuel
AU - Vandenbussche, Bart
AU - Absil, Olivier
AU - Baudoz, Pierre
AU - Boccaletti, Anthony
AU - Bouwman, Jeroen
AU - Cossou, Christophe
AU - Coulais, Alain
AU - Crouzet, Nicolas
AU - Gastaud, René
AU - Glasse, Alistair
AU - Glauser, Adrian M.
AU - Kamp, Inga
AU - Kendrew, Sarah
AU - Krause, Oliver
AU - Lahuis, Fred
AU - Mueller, Michael
AU - Olofsson, Göran
AU - Pye, John
AU - Rouan, Daniel
AU - Royer, Pierre
AU - Scheithauer, Silvia
AU - Waldmann, Ingo
AU - Colina, Luis
AU - van Dishoeck, Ewine F.
AU - Ray, Tom
AU - Östlin, Göran
AU - Wright, Gillian
N1 - Funding Information: This work is based (in part) on observations made with the NASA/ESA/CSA James Webb Space Telescope (JWST). The data were obtained from the Mikulski Archive for Space Telescopes (MAST) at the Space Telescope Science Institute, which is operated by the Association of Universities for Research in Astronomy, Inc., under NASA contract NAS 5-03127 for the JWST. These observations are associated with programme 1189. The Mid-Infrared Instrument (MIRI) draws on the scientific and technical expertise of the following organizations: Ames Research Center, USA; Airbus Defence and Space, UK; CEA/IRFU, Saclay, France; Centre Spatial de Liège, Belgium; Consejo Superior de Investigaciones Científicas, Spain; Carl Zeiss Optronics, Germany; Chalmers University of Technology, Sweden; Danish Space Research Institute, Denmark; Dublin Institute for Advanced Studies, Ireland; European Space Agency, the Netherlands; ETCA, Belgium; ETH Zurich, Switzerland; Goddard Space Flight Center, USA; Institut d’Astrophysique Spatiale, France; Instituto Nacional de Técnica Aeroespacial, Spain; Institute for Astronomy, Edinburgh, UK; Jet Propulsion Laboratory, USA; Laboratoire d’Astrophysique de Marseille (LAM), France; Leiden University, the Netherlands; Lockheed Advanced Technology Center, USA; NOVA Opt-IR Group at Dwingeloo, the Netherlands; Northrop Grumman, USA; Max-Planck-Institut für Astronomie (MPIA), Heidelberg, Germany; Laboratoire d’Etudes Spatiales et d’Instrumentation en Astrophysique (LESIA), France; Paul Scherrer Institut, Switzerland; Raytheon Vision Systems, USA; RUAG Aerospace, Switzerland; Rutherford Appleton Laboratory (RAL Space), UK; Space Telescope Science Institute, USA; Toegepast Natuurwetenschappelijk Onderzoek (TNO-TPD), the Netherlands; UK Astronomy Technology Centre, UK; University College London, UK; University of Amsterdam, the Netherlands; University of Arizona, USA; University of Bern, Switzerland; University of Cardiff, UK; University of Cologne, Germany; University of Ghent, Belgium; University of Groningen, the Netherlands; University of Leicester, UK; KU Leuven, Belgium; University of Stockholm, Sweden; and Utah State University, USA. The following national and international funding agencies funded and supported the MIRI development: NASA; ESA; Belgian Science Policy Office (BELSPO); Centre Nationale d’Etudes Spatiales (CNES); Danish National Space Center; Deutsches Zentrum fur Luft und Raumfahrt (DLR); Enterprise Ireland; Ministerio de Economía y Competitividad; Netherlands Research School for Astronomy (NOVA); Netherlands Organisation for Scientific Research (NWO); Science and Technology Facilities Council; Swiss Space Office; Swedish National Space Agency; and UK Space Agency. D.B. and M.M.-C. are supported by Spanish MCIN/AEI/10.13039/501100011033 grant nos. PID2019-107061GB-C61 and MDM-2017-0737. C.C., A.B., P.-O.L., R.G. and A.C. acknowledge funding support from CNES. P.P. thanks the Swiss National Science Foundation (SNSF) for financial support under grant number 200020_200399. N.W. acknowledges funding from NSF award 1909776 and NASA XRP award 80NSSC22K0142. O.A., I.A., B.V. and P.R. thank the European Space Agency (ESA) and the Belgian Science Policy Office (BELSPO) for their support in the framework of the PRODEX Programme. L.D. acknowledges funding from the KU Leuven Interdisciplinary Grant (IDN/19/028), the European Union H2020-MSCA-ITN-2019 under grant no. 860470 (CHAMELEON) and the FWO research grant G086217N. I.K. acknowledges support from grant TOP-1 614.001.751 from the Dutch Research Council (NWO). O.K. acknowledges support from the Federal Ministry of Economy and Energy (BMWi) through the German Space Agency (DLR). J.P. acknowledges financial support from the UK Science and Technology Facilities Council and the UK Space Agency. G.O. acknowledges support from the Swedish National Space Board and the Knut and Alice Wallenberg Foundation. P.T. acknowledges support by the European Research Council (ERC) under grant agreement ATMO 757858. F.A.M. has received funding from the European Union’s Horizon 2020 research and innovation programme under the Marie Skłodowska-Curie grant agreement no. 860470. L.C. acknowledges support by grant PIB2021-127718NB-100 from the Spanish Ministry of Science and Innovation/State Agency of Research MCIN/AEI/10.13039/501100011033. E.F.v.D. acknowledges support from A-ERC grant 101019751 MOLDISK. T.R. acknowledges support from the ERC 743029 EASY. G.Ö. acknowledges support from SNSA. T.H. acknowledges support from the ERC under the European Union’s Horizon 2020 research and innovation programme under grant agreement no. 832428-Origins. We thank the MIRI instrument team and the many others who contributed to the success of the JWST. Funding Information: This work is based (in part) on observations made with the NASA/ESA/CSA James Webb Space Telescope (JWST). The data were obtained from the Mikulski Archive for Space Telescopes (MAST) at the Space Telescope Science Institute, which is operated by the Association of Universities for Research in Astronomy, Inc., under NASA contract NAS 5-03127 for the JWST. These observations are associated with programme 1189. The Mid-Infrared Instrument (MIRI) draws on the scientific and technical expertise of the following organizations: Ames Research Center, USA; Airbus Defence and Space, UK; CEA/IRFU, Saclay, France; Centre Spatial de Liège, Belgium; Consejo Superior de Investigaciones Científicas, Spain; Carl Zeiss Optronics, Germany; Chalmers University of Technology, Sweden; Danish Space Research Institute, Denmark; Dublin Institute for Advanced Studies, Ireland; European Space Agency, the Netherlands; ETCA, Belgium; ETH Zurich, Switzerland; Goddard Space Flight Center, USA; Institut d’Astrophysique Spatiale, France; Instituto Nacional de Técnica Aeroespacial, Spain; Institute for Astronomy, Edinburgh, UK; Jet Propulsion Laboratory, USA; Laboratoire d’Astrophysique de Marseille (LAM), France; Leiden University, the Netherlands; Lockheed Advanced Technology Center, USA; NOVA Opt-IR Group at Dwingeloo, the Netherlands; Northrop Grumman, USA; Max-Planck-Institut für Astronomie (MPIA), Heidelberg, Germany; Laboratoire d’Etudes Spatiales et d’Instrumentation en Astrophysique (LESIA), France; Paul Scherrer Institut, Switzerland; Raytheon Vision Systems, USA; RUAG Aerospace, Switzerland; Rutherford Appleton Laboratory (RAL Space), UK; Space Telescope Science Institute, USA; Toegepast Natuurwetenschappelijk Onderzoek (TNO-TPD), the Netherlands; UK Astronomy Technology Centre, UK; University College London, UK; University of Amsterdam, the Netherlands; University of Arizona, USA; University of Bern, Switzerland; University of Cardiff, UK; University of Cologne, Germany; University of Ghent, Belgium; University of Groningen, the Netherlands; University of Leicester, UK; KU Leuven, Belgium; University of Stockholm, Sweden; and Utah State University, USA. The following national and international funding agencies funded and supported the MIRI development: NASA; ESA; Belgian Science Policy Office (BELSPO); Centre Nationale d’Etudes Spatiales (CNES); Danish National Space Center; Deutsches Zentrum fur Luft und Raumfahrt (DLR); Enterprise Ireland; Ministerio de Economía y Competitividad; Netherlands Research School for Astronomy (NOVA); Netherlands Organisation for Scientific Research (NWO); Science and Technology Facilities Council; Swiss Space Office; Swedish National Space Agency; and UK Space Agency. D.B. and M.M.-C. are supported by Spanish MCIN/AEI/10.13039/501100011033 grant nos. PID2019-107061GB-C61 and MDM-2017-0737. C.C., A.B., P.-O.L., R.G. and A.C. acknowledge funding support from CNES. P.P. thanks the Swiss National Science Foundation (SNSF) for financial support under grant number 200020_200399. N.W. acknowledges funding from NSF award 1909776 and NASA XRP award 80NSSC22K0142. O.A., I.A., B.V. and P.R. thank the European Space Agency (ESA) and the Belgian Science Policy Office (BELSPO) for their support in the framework of the PRODEX Programme. L.D. acknowledges funding from the KU Leuven Interdisciplinary Grant (IDN/19/028), the European Union H2020-MSCA-ITN-2019 under grant no. 860470 (CHAMELEON) and the FWO research grant G086217N. I.K. acknowledges support from grant TOP-1 614.001.751 from the Dutch Research Council (NWO). O.K. acknowledges support from the Federal Ministry of Economy and Energy (BMWi) through the German Space Agency (DLR). J.P. acknowledges financial support from the UK Science and Technology Facilities Council and the UK Space Agency. G.O. acknowledges support from the Swedish National Space Board and the Knut and Alice Wallenberg Foundation. P.T. acknowledges support by the European Research Council (ERC) under grant agreement ATMO 757858. F.A.M. has received funding from the European Union’s Horizon 2020 research and innovation programme under the Marie Skłodowska-Curie grant agreement no. 860470. L.C. acknowledges support by grant PIB2021-127718NB-100 from the Spanish Ministry of Science and Innovation/State Agency of Research MCIN/AEI/10.13039/501100011033. E.F.v.D. acknowledges support from A-ERC grant 101019751 MOLDISK. T.R. acknowledges support from the ERC 743029 EASY. G.Ö. acknowledges support from SNSA. T.H. acknowledges support from the ERC under the European Union’s Horizon 2020 research and innovation programme under grant agreement no. 832428-Origins. We thank the MIRI instrument team and the many others who contributed to the success of the JWST. Publisher Copyright: © 2023, The Author(s), under exclusive licence to Springer Nature Limited.
PY - 2023/12/14
Y1 - 2023/12/14
N2 - Brown dwarfs serve as ideal laboratories for studying the atmospheres of giant exoplanets on wide orbits, as the governing physical and chemical processes within them are nearly identical1,2. Understanding the formation of gas-giant planets is challenging, often involving the endeavour to link atmospheric abundance ratios, such as the carbon-to-oxygen (C/O) ratio, to formation scenarios3. However, the complexity of planet formation requires further tracers, as the unambiguous interpretation of the measured C/O ratio is fraught with complexity4. Isotope ratios, such as deuterium to hydrogen and 14N/15N, offer a promising avenue to gain further insight into this formation process, mirroring their use within the Solar System5–7. For exoplanets, only a handful of constraints on 12C/13C exist, pointing to the accretion of 13C-rich ice from beyond the CO iceline of the disks8,9. Here we report on the mid-infrared detection of the 14NH3 and 15NH3 isotopologues in the atmosphere of a cool brown dwarf with an effective temperature of 380 K in a spectrum taken with the Mid-Infrared Instrument (MIRI) of JWST. As expected, our results reveal a 14N/15N value consistent with star-like formation by gravitational collapse, demonstrating that this ratio can be accurately constrained. Because young stars and their planets should be more strongly enriched in the 15N isotope10, we expect that 15NH3 will be detectable in several cold, wide-separation exoplanets.
AB - Brown dwarfs serve as ideal laboratories for studying the atmospheres of giant exoplanets on wide orbits, as the governing physical and chemical processes within them are nearly identical1,2. Understanding the formation of gas-giant planets is challenging, often involving the endeavour to link atmospheric abundance ratios, such as the carbon-to-oxygen (C/O) ratio, to formation scenarios3. However, the complexity of planet formation requires further tracers, as the unambiguous interpretation of the measured C/O ratio is fraught with complexity4. Isotope ratios, such as deuterium to hydrogen and 14N/15N, offer a promising avenue to gain further insight into this formation process, mirroring their use within the Solar System5–7. For exoplanets, only a handful of constraints on 12C/13C exist, pointing to the accretion of 13C-rich ice from beyond the CO iceline of the disks8,9. Here we report on the mid-infrared detection of the 14NH3 and 15NH3 isotopologues in the atmosphere of a cool brown dwarf with an effective temperature of 380 K in a spectrum taken with the Mid-Infrared Instrument (MIRI) of JWST. As expected, our results reveal a 14N/15N value consistent with star-like formation by gravitational collapse, demonstrating that this ratio can be accurately constrained. Because young stars and their planets should be more strongly enriched in the 15N isotope10, we expect that 15NH3 will be detectable in several cold, wide-separation exoplanets.
UR - http://www.scopus.com/inward/record.url?scp=85178873849&partnerID=8YFLogxK
U2 - 10.1038/s41586-023-06813-y
DO - 10.1038/s41586-023-06813-y
M3 - Article
C2 - 37931645
AN - SCOPUS:85178873849
SN - 0028-0836
VL - 624
SP - 263
EP - 266
JO - Nature
JF - Nature
IS - 7991
ER -