Delorme 1
Template:Short description Template:Starbox begin Template:Starbox image Template:Starbox observe Template:Starbox character Template:Starbox astrometry Template:Starbox detail Template:Starbox relpos Template:Starbox catalog Template:Starbox reference Template:Starbox end Delorme 1 (2MASS J01033563-5515561) is a binary star with a planetary-mass companion (PMC) or protoplanet in a circumbinary orbit.[1] The PMC is notable for showing signs of accretion, despite being 30-45 Myr old, making it similar to Peter Pan disks.[2][3][4] These disks show characteristics of a gas-rich disk at unexpected high ages.[5]
Binary system
The star was resolved in 2013 with the Very Large Telescope NACO instrument by Delorme et al. A spectrum of the binary was taken with GMOS at Gemini South, which showed a spectral type of M5.5/M6 and strong Hydrogen-alpha emission. The astrometry showed that this star belongs to the Tucana-Horologium association. The binary is separated by around 12 astronomical units (AU).[1] In 2014 Riedel et al. found a better match with the Carina association, which has a similar age as Tuc-Hor. They also found the system to be over-luminous, which might either hint at a younger age or further multiplicity.[6] Other searches do, however, find a better match with Tuc-Hor.[7] Because the Washington Double Star Catalog named the binary ** DLR 1 after the first author of the discovery paper in 2013, Eriksson et al. suggested the name Delorme 1 for the binary.[2] The binary is named after Philippe Delorme.[8]
Circumbinary companion

The binary companion was discovered in 2013 as an object with a mass between 12 and 14 Template:Jupiter mass and a separation of 84 AU from the central binary. It had a spectrum similar to early L-dwarfs, but redder than field L-dwarfs.[1] In 2020 Eriksson et al. discovered Hydrogen-alpha, -beta and Helium I lines from Delorme 1 (AB)b using MUSE. This is seen as a clear sign of accretion on a planetary-mass object. The spectral type of this object was determined to be L0 with very low gravity due to stronger than expected vanadium oxide absorption.[2] H-alpha can be influenced by chromospheric activity, complicating its interpretation. Betti et al. discovered Paschen and Brackett lines in Delorme 1 (AB)b in the near-infrared, using TripleSpec at SOAR. These observations are in agreement with planetary-shock accretion.[3] In 2023 Ringqvist et al. observed Delorme 1 (AB)b with the VLT UVES, detecting neutral hydrogen in the ultraviolet.[4] Both near-infrared and ultraviolet observations show an accretion rate of about (about 1.2 to 2.3 the mass of 10 Hygiea per year).[3][4] The planet and the star were observed with MIRI/IFU, which revealed the circumplanetary disk around the planet. The disk is carbon-rich and contains hydrogen cyanide (HCN), acetylene (C2H2, tentative: 13CCH2) and molecular hydrogen (H2). The disk has a temperature of Template:Convert and a inner cavity with a size of Template:Val. According to simulations the disk will only fill out 40% of the Hill radius, resulting of a theoretical disk size of 7.8 AU. The extended emission by H2 is larger than this disk size, showing that it includes an outflow, maybe a disk wind coming from the circumplanetary disk. Assuming a disk wind is present, the disk has a mass-loss rate of 2 × 10−10 Template:Jupiter mass/year.[9]
Delorme 1 (AB)b has been called a protoplanet candidate and a super-Jupiter.[3][4] The researchers found that the high accretion is in better agreement with a formation via disk fragmentation, hinting that it might have formed from a circumstellar disk.[3] Giant planets and brown dwarfs are thought to form via disk fragmentation in rare cases in the outer regions of a disk (r>50 AU).[10] Teasdale et al. modelled three formation scenarios in which the planet could have formed. In the first two scenarios the planet forms in a massive disk via gravitational instability. The first two scenarios produce planets that have accretion and separation comparable to the observed ones, but the resulting planets are more massive than Delorme 1 (AB)b. In a third scenario the planet forms via core accretion in a less massive disk much closer to the binary. In this third scenario the mass and accretion are similar to the observed ones, but the separation is smaller.[11] The modelling of JWST spectrum showed super-solar metallicity and C/O ratio for the planet, but the authors mention that these values are model dependent. The C/O ratio could be consistent with the formation between water and CO snowlines. Alternatively the carbon-rich circumplanetary disk could enrich the planet in carbon, explaining the elevated C/O ratio.[9]
Template:OrbitboxPlanet begin Template:OrbitboxPlanet Template:Orbitbox end
References
- ↑ Template:Cite journal Cite error:
<ref>tag with name "Blunt2017" defined in<references>is not used in prior text. - ↑ 1.0 1.1 1.2 Template:Cite journal
- ↑ 2.0 2.1 2.2 Template:Cite journal
- ↑ 3.0 3.1 3.2 3.3 3.4 Template:Cite journal
- ↑ 4.0 4.1 4.2 4.3 Template:Cite journal
- ↑ Template:Cite journal
- ↑ Template:Cite journal
- ↑ Template:Cite journal
- ↑ Template:Cite web
- ↑ 9.0 9.1 Template:Cite journal
- ↑ Template:Cite journal
- ↑ Template:Cite journal