Astronomy:Kepler-1513

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Short description: Main-sequence star in the constellation Lyra
Kepler-1513
Observation data
Equinox J2000.0]] (ICRS)
Constellation Lyra[1]
Right ascension  19h 19m 09.99418s[2]
Declination +39° 17′ 06.9287″[2]
Apparent magnitude (V) 12.888±0.100 (Kepler band)
Characteristics
Evolutionary stage Main sequence
Spectral type K0V[3] or late G[4]
Apparent magnitude (G) 12.946±0.003[2]
Apparent magnitude (J) 11.758±0.027[5]
Apparent magnitude (H) 11.397±0.030[5]
Apparent magnitude (K) 11.309±0.020[5]
Astrometry
Radial velocity (Rv)−0.42±1.41[2] km/s
Proper motion (μ) RA: 20.439[2] mas/yr
Dec.: 1.745[2] mas/yr
Parallax (π)2.8446 ± 0.0134[2] mas
Distance1,147 ± 5 ly
(352 ± 2 pc)
Details[6]
Mass0.943±0.037 M☉
Radius0.950+0.077
−0.055
 R☉
Luminosity (bolometric)0.743+0.148
−0.100
 L☉
Surface gravity (log g)4.46±0.10 cgs
Temperature5491±100 K
Metallicity0.17±0.06 [M/H]
Age7.0+4.0
−4.2
 Gyr
Other designations
Kepler-1513, KOI-3678, KIC 4150804, 2MASS J19190999+3917070[5]
Database references
SIMBADdata

Kepler-1513 is a main-sequence star about 1,150 light-years (350 parsecs) away in the constellation Lyra. It has a late-G[4] or early-K[3] spectral type, and it hosts at least one, and likely two, exoplanets.

Planetary system

Kepler-1513b (KOI-3678.01) was confirmed in 2016 as part of a study statistically validating hundreds of Kepler planets.[7] In November 2022, an exomoon candidate was reported around Kepler-1513b based on transit-timing variations (TTVs). Unlike previous giant exomoon candidates in the Kepler-1625 and Kepler-1708 systems, this exomoon would have been terrestrial-mass, ranging from 0.76 Lunar masses to 0.34 Earth masses depending on the planet's mass and the moon's orbital period.[4]

In October 2023, a follow-up study by the same team of astronomers using additional observations found that the observed TTVs cannot be explained by an exomoon, but can be explained by a second, outer planet, Kepler-1513c, with a mass comparable to Saturn.[6]

The Kepler-1513 planetary system[6]
Companion
(in order from star)
Mass Semimajor axis
(AU)
Orbital period
(days)
Eccentricity Inclination Radius
b 0.152+0.104
−0.061
 MJ
0.53+0.04
−0.03
160.8842+0.0011
−0.0028
0.306+0.093
−0.097
— 8.05+0.58
−0.40
 R⊕
c 0.266+0.098
−0.063
 MJ
1.7106[8] 841.4+8.1
−5.3
0.125+0.018
−0.019
— —

See also

References

  1. ↑ "Finding the constellation which contains given sky coordinates". 2 August 2008. http://djm.cc/constellation.html. 
  2. ↑ 2.0 2.1 2.2 2.3 2.4 2.5 Vallenari, A. et al. (2022). "Gaia Data Release 3. Summary of the content and survey properties". Astronomy & Astrophysics. doi:10.1051/0004-6361/202243940  Gaia DR3 record for this source at VizieR.
  3. ↑ 3.0 3.1 Frasca, A. et al. (October 2016). "Activity indicators and stellar parameters of the Kepler targets. An application of the ROTFIT pipeline to LAMOST-Kepler stellar spectra". Astronomy & Astrophysics 594: A39. doi:10.1051/0004-6361/201628337. Bibcode: 2016A&A...594A..39F. 
  4. ↑ 4.0 4.1 4.2 Kipping, David; Yahalomi, Daniel A. (January 2023). "A search for transit timing variations within the exomoon corridor using Kepler data". Monthly Notices of the Royal Astronomical Society 518 (3): 3482–3493. doi:10.1093/mnras/stac3360. Bibcode: 2023MNRAS.518.3482K. 
  5. ↑ 5.0 5.1 5.2 5.3 "Kepler-1513". SIMBAD. Centre de données astronomiques de Strasbourg. http://simbad.u-strasbg.fr/simbad/sim-basic?Ident=Kepler-1513. 
  6. ↑ 6.0 6.1 6.2 Yahalomi, Daniel A. et al. (2024). "Not So Fast Kepler-1513: A Perturbing Planetary Interloper in the Exomoon Corridor". Monthly Notices of the Royal Astronomical Society 527: 620–639. doi:10.1093/mnras/stad3070. 
  7. ↑ Morton, Timothy D. et al. (May 2016). "False Positive Probabilities for all Kepler Objects of Interest: 1284 Newly Validated Planets and 428 Likely False Positives". The Astrophysical Journal 822 (2): 86. doi:10.3847/0004-637X/822/2/86. Bibcode: 2016ApJ...822...86M. 
  8. ↑ "Orbital Period Calculator | Binary System" (in en). https://www.omnicalculator.com/physics/orbital-period.