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Upsilon Leonis

From Wikipedia, the free encyclopedia
Star in the constellation Leo
υ Leonis
Location of υ Leonis (circled in red)
Observation data
EpochJ2000.0      EquinoxJ2000.0 (ICRS)
ConstellationLeo
Right ascension11h 36m 56.92983s[1]
Declination+00° 49′ 25.8758″[1]
Apparent magnitude (V)4.33[2]
Characteristics
Evolutionary stagered clump[3]
Spectral typeG9 III[4]
U−Bcolor index+0.76[2]
B−Vcolor index+1.00[2]
Astrometry
Radial velocity (Rv)1.79±0.16[5] km/s
Proper motion (μ)RA: +1.76[1]mas/yr
Dec.: +43.37[1]mas/yr
Parallax (π)17.97±0.22 mas[1]
Distance182 ± 2 ly
(55.6 ± 0.7 pc)
Absolute magnitude (MV)0.59[6]
Details
Mass2.58[6] M
Radius11.38±0.16[7] R
Luminosity56[5] L
Surface gravity (log g)2.7[5] cgs
Temperature4,842[5] K
Metallicity[Fe/H]–0.34[5] dex
Rotational velocity (v sin i)0.0[5] km/s
Age4.12±2.08[8] Gyr
Other designations
υ Leo,91 Leo,BD−00°2458,FK5 437,HD 100920,HIP 56647,HR 4471,SAO 138298[9]
Database references
SIMBADdata
Exoplanet Archivedata

Upsilon Leonis (υ Leo) is astar in thezodiacconstellation ofLeo. It is visible to the naked eye with anapparent visual magnitude of 4.33.[2] The distance to this star, as determined usingparallax measurements,[1] is about 182 light years. At that distance, the visual magnitude of the star is diminished by an estimatedextinction factor of 0m.02 because ofinterstellar dust.[6]

With an age of around 4 billion years, this star hasevolved into aG-typegiant star with astellar classification of G9 III.[4] It has 2.6 times theSun's mass,[6] but has expanded to 11.4 times thesolar radius[7] and shines with 56 times theluminosity of the Sun at aneffective temperature of 4,842 K.[5] The rate of rotation is too small to be measured, with aprojected rotational velocity of 0.0 km/s.[5] The chemical abundance of elements other than hydrogen and helium, what astronomers term the star'smetallicity, is less than half that in the Sun.[5] It is most likely a member of the galacticthin disk population.[8]

Planetary system

[edit]

In 2021, a gas giant planet was detected byradial velocity method.[10] In 2024, this object's true mass was measured usingastrometry from theGaia spacecraft. The method consists of taking the host star's RUWE level—an astrometirc indicator— from the astrometric solution. A large RUWE could imply that there is an unseen companion around the star, or that there are systematic calibration errors in the astrometric solution. Assuming the former scenario, the mass of Upsilon Leonis b is measured at29.2 MJ, indicating that it is a brown dwarf, but the latter scenario is still a possibility, which means that this measured mass is likely an upper limit.[11]

The Upsilon Leonis planetary system[10]
Companion
(in order from star)
MassSemimajor axis
(AU)
Orbital period
(days)
EccentricityInclinationRadius
b≥0.51+0.06
−0.26
[10] and ≤29.2[11] MJ
1.18+0.11
−0.32
385.2+2.8
−1.3
0.320+0.134
−0.218

References

[edit]
  1. ^abcdefvan Leeuwen, F. (2007), "Validation of the new Hipparcos reduction",Astronomy and Astrophysics,474 (2):653–664,arXiv:0708.1752,Bibcode:2007A&A...474..653V,doi:10.1051/0004-6361:20078357,S2CID 18759600.
  2. ^abcdMermilliod, J.-C. (1986), "Compilation of Eggen's UBV data, transformed to UBV (unpublished)",Catalogue of Eggen's UBV Data,SIMBAD,Bibcode:1986EgUBV........0M.
  3. ^Soubiran, C.; Bienaymé, O.; Mishenina, T. V.; Kovtyukh, V. V. (2008), "Vertical distribution of Galactic disk stars. IV. AMR and AVR from clump giants",Astronomy and Astrophysics,480 (1): 91,arXiv:0712.1370,Bibcode:2008A&A...480...91S,doi:10.1051/0004-6361:20078788.
  4. ^abBuscombe, W. (1962), "Spectral classification of Southern fundamental stars",Mount Stromlo Observatory Mimeogram,4: 1,Bibcode:1962MtSOM...4....1B.
  5. ^abcdefghiMassarotti, Alessandro; et al. (January 2008), "Rotational and radial velocities for a sample of 761 HIPPARCOS giants and the role of binarity",The Astronomical Journal,135 (1):209–231,Bibcode:2008AJ....135..209M,doi:10.1088/0004-6256/135/1/209,S2CID 121883397.
  6. ^abcdTakeda, Yoichi; et al. (February 2005), "Stellar Parameters and Photospheric Abundances of Late-G Giants: Properties of the Targets of the Okayama Planet Search Program",Publications of the Astronomical Society of Japan,57 (1):109–125,Bibcode:2005PASJ...57..109T,doi:10.1093/pasj/57.1.109.
  7. ^abBaines, Ellyn K.; Clark, James H.; Kingsley, Bradley I.; Schmitt, Henrique R.; Stone, Jordan M. (2025-05-07), "Vintage NPOI: New and Updated Angular Diameters for 145 Stars",The Astronomical Journal,169 (6): 293,arXiv:2506.02912,Bibcode:2025AJ....169..293B,doi:10.3847/1538-3881/adc930,ISSN 1538-3881.
  8. ^abSoubiran, C.; et al. (March 2008), "Vertical distribution of Galactic disk stars. IV. AMR and AVR from clump giants",Astronomy and Astrophysics,480 (1):91–101,arXiv:0712.1370,Bibcode:2008A&A...480...91S,doi:10.1051/0004-6361:20078788,S2CID 16602121.
  9. ^"* ups Leo".SIMBAD.Centre de données astronomiques de Strasbourg. Retrieved2016-09-29.
  10. ^abcTeng, Huan-Yu; Sato, Bun'ei; Takarada, Takuya; Omiya, Masashi; Harakawa, Hiroki; Izumiura, Hideyuki; Kambe, Eiji; Takeda, Yoichi; Yoshida, Michitoshi; Itoh, Yoichi; Ando, Hiroyasu; Kokubo, Eiichiro (2022), "Regular radial velocity variations in nine G- and K-type giant stars: Eight planets and one planet candidate",Publications of the Astronomical Society of Japan,74:92–127,arXiv:2112.07169,doi:10.1093/pasj/psab112
  11. ^abWallace, A. L.; Casey, A. R.; Brown, A. G. A.; Castro-Ginard, A. (2024-11-10), "Detection and Characterisation of Giant Planets with Gaia Astrometry",Monthly Notices of the Royal Astronomical Society,536 (3): 2485,arXiv:2411.06705,Bibcode:2025MNRAS.536.2485W,doi:10.1093/mnras/stae2769.
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