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. Bibcode2016A&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. Bibcode2023MNRAS.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. Bibcode2016ApJ...822...86M. 
  8. "Orbital Period Calculator | Binary System" (in en). https://www.omnicalculator.com/physics/orbital-period.