Observation data Epoch J2000 Equinox J2000 | |
---|---|
Constellation | Draco [1] |
Right ascension | 19h 06m 09.60253s [2] |
Declination | +49° 26′ 14.3969″ [2] |
Characteristics | |
Spectral type | K7 V + M1 V [3] |
Astrometry | |
Proper motion (μ) | RA: 2.635 mas/yr [2] Dec.: −16.375 mas/yr [2] |
Parallax (π) | 4.5538±0.5562 mas [2] |
Distance | approx. 720 ly (approx. 220 pc) |
Details [4] | |
Kepler-296 A | |
Mass | 0.498+0.067 −0.087 M☉ |
Radius | 0.480+0.066 −0.087 R☉ |
Surface gravity (log g) | 4.774+0.091 −0.059 cgs |
Temperature | 3740±130 K |
Metallicity [Fe/H] | −0.08+0.28 −0.30 dex |
Kepler-296 B | |
Mass | 0.326+0.070 −0.079 M☉ |
Radius | 0.322+0.060 −0.068 R☉ |
Surface gravity (log g) | 4.993+0.087 −0.063 cgs |
Temperature | 3440±75 K |
Metallicity [Fe/H] | −0.08+0.28 −0.30 dex |
Other designations | |
Kepler-296, KOI-1422, KIC 11497958, 2MASS J19060960+4926143 [5] | |
Database references | |
SIMBAD | data |
Exoplanet Archive | data |
KIC | data |
Kepler-296 is a binary star system [4] in the constellation Draco. The primary star appears to be a late K-type main-sequence star, while the secondary is a red dwarf. [3]
Five exoplanets have been detected around the system; all are believed to be orbiting the primary star rather than its dimmer companion. [4] Two planets in particular, Kepler-296e and Kepler-296f, are likely located in the habitable zone. [4] For the planetary system to remain stable, no additional giant planets can be located up to orbital radius 10.1 AU. [7]
Companion (in order from star) | Mass | Semimajor axis (AU) | Orbital period (days) | Eccentricity | Inclination | Radius |
---|---|---|---|---|---|---|
c | — | 0.0521+0.0088 −0.0086 | 5.8416366±0.000010 | <0.33 | — | 2.00+0.33 −0.32 R🜨 |
b | — | 0.079±0.013 | 10.864384+0.000051 −0.000046 | <0.33 | — | 1.61+0.29 −0.27 R🜨 |
d | — | 0.118±0.020 | 19.850291+0.000061 −0.000057 | <0.33 | — | 2.09+0.33 −0.32 R🜨 |
e | — | 0.169+0.029 −0.028 | 34.14211±0.00025 | <0.33 | — | 1.53+0.27 −0.25 R🜨 |
f | — | 0.255+0.043 −0.042 | 63.33627+0.00060 −0.00062 | <0.33 | — | 1.80+0.31 −0.30 R🜨 |