10199 Chariklo (asteroid or centaur) is the largest known centaur in the outer Solar System, orbiting between Saturn and Uranus every 62.5 years. Discovered in 1997 by the University of Arizona's Spacewatch project at Kitt Peak National Observatory, Chariklo has a dark, reddish surface featuring water ice, silicate minerals, amorphous carbon, and complex organic compounds called tholins. Its ring system—the first discovered around a minor planet—was found in 2013 during a stellar occultation. The rings’ stability is uncertain, possibly maintained by unseen shepherd moons, with origins hypothesized to involve outgassing or tidal forces.
Discovery and naming
Chariklo was discovered on 15 February 1997 by the University of Arizona's Spacewatch project at Kitt Peak National Observatory.4 James V. Scotti made the discovery observations using the Spacewatch 0.9-meter telescope,56 although NASA and the Minor Planet Center (MPC) do not mention him as the official discoverer.789 Other observatories from Canada, Czech Republic, and China continued observing Chariklo until the discovery was announced by the MPC on 24 February 1997. The MPC gave the object its provisional designation of 1997 CU26.10 Chariklo was the seventh centaur discovered.11: 457 12
Shortly after the discovery of Chariklo, astronomers began conducting detailed observations to characterize its properties, including its color,13 size,14 and surface composition.15 On 2 March 1999, the MPC gave Chariklo its minor planet catalog number of 10199.16: 89 Chariklo was officially named on 28 September 1999.17: 365
This minor planet is named after the nymph Chariclo (Χαρικλώ), the wife of Chiron in Greek mythology.18 Chariclo has sometimes been characterized as a sea nymph, female centaur, or the mother of the blind prophet Tiresias.19 An astrological symbol for Chariklo, , was devised in the late 1990s by German astrologer Robert von Heeren. Chariklo's symbol was derived from the astrological symbol used for the centaur 2060 Chiron, , where the letter C replaces the letter K.20
Orbit
Chariklo orbits the Sun between Saturn and Uranus21: 1 with an average orbital distance of 15.7 astronomical units (AU) and an orbital period of 62.5 years.22 It follows an inclined and elliptical orbit that brings it within 13.1 AU from the Sun at perihelion to as far as 18.4 AU at aphelion.23 Chariklo is close to, but not in a 4:3 orbital resonance with Uranus; its mean orbital distance lies within 0.09 AU from the resonance.24: 802
Chariklo is classified as a centaur, a type of minor planet that orbits between Jupiter and Neptune.25: 1 26: 1 Centaurs, which share characteristics of both asteroids and comets,27 are thought to have originated from the Kuiper belt and the scattered disc beyond Neptune.28: 1 The centaurs are strongly influenced by the gravity of the giant planets, which leads to chaotic or unpredictable changes in their orbits.29: 1–2 Such changes can lead to centaurs escaping their orbital region by either getting ejected from the Solar System, impacting a planet, or becoming a short-period comet whose orbit enters the inner Solar System.30: 1
Compared to other centaurs, Chariklo's orbit is relatively more stable31: 1 with a 50% chance of escaping the centaur region 732: 4772 or 10.333: 802 million years in the future.34 Chariklo's orbital evolution is primarily influenced by Uranus; simulations predict that Chariklo will frequently make close approaches to Uranus during the next 100 million years.35: 1, 3 However, Chariklo's less frequent future encounters with Jupiter and Saturn will have greater effects on its orbit and can potentially disrupt Chariklo's ring system.36: 4, 6
Simulations show that there is a 99% chance that Chariklo was implanted in the centaur region sometime in the past 20 million years.37: 5 There is a 50% chance that Chariklo could have been implanted as recently as 9.38 million years ago.38: 802 39: 2 A 2016 study suggested that Jupiter and Saturn were responsible for transferring Chariklo to the centaur region,40: 6 whereas a 2017 study suggested Neptune was more likely responsible.41: 6
Observation
Chariklo's brightness or apparent magnitude lies between 17 and 19, depending on its distance from Earth.42 Chariklo appeared brightest from Earth in 2003 when it was simultaneously at perihelion and opposition.43 Independent of distance, Chariklo's intrinsic brightness or absolute magnitude (H) changes over time due to the changing viewing angle of Chariklo's rings as seen from Earth.44: 11 During the late 1990s and early 2000s, Chariklo appeared brighter (H=6.8) because more of its rings' surface area was visible from Earth.45: 11 On the other hand, during 2008, Chariklo appeared fainter (H=7.3) because its rings were seen edge-on (minimum visible surface area) from Earth.46: 11
Chariklo and its rings are too small and too far away to be resolved by current telescopes.4748: 2 Chariklo's rings span an angular diameter of 80 milliarcseconds in the sky, close to the diffraction limit of some of the highest-resolution telescopes like the Hubble Space Telescope.49: 2 These telescopes have not been able to detect Chariklo's rings through direct imaging.5051: 2 Chariklo's rings may be imageable in the future with even larger telescopes such as the Extremely Large Telescope.52: 29
During 2013 to 2022, Chariklo was passing in front of the Galactic Center in the sky.53: 29 Because the Galactic Center is densely packed with stars, this meant Chariklo would occult or pass in front of multiple stars.54: 29 Stellar occultations allow for accurate measurements of a Solar System object's position, size, shape, and surrounding features (i.e. moons and rings) at kilometre-scale resolutions.55: 2 Chariklo was first observed via stellar occultation on 3 June 2013, which resulted in the discovery of Chariklo's rings.56: 1 Between 2014 and 2022, about twenty observing campaigns were organized by astronomers to observe predicted occultations by Chariklo.57: 29 These campaigns involved international collaboration between professional and amateur astronomers.58: 2 59: 29
Physical characteristics
Size, shape, and mass
Multiple years of occultation observations show that Chariklo is a flattened or elongated body60: 22 with dimensions of approximately 288 km × 270 km × 198 km (179 mi × 168 mi × 123 mi).61 The volume-equivalent mean diameter of Chariklo is about 250 km (160 mi).62: 11 This makes Chariklo the largest known centaur.63: 1
Chariklo's shape is consistent with a triaxial ellipsoid,64: 1 although slight differences between occultation measurements hint at topographic variation or irregularities in its shape.65: 9 66: 19 Chariklo's topographic deviations from an ellipsoid may be as low as −5.52 km (−3.43 mi) to as high as 7.78 km (4.83 mi) (standard deviation 4.11 km or 2.55 mi).67: 9 The amount of topographic variation seen in Chariklo is similar to those seen in Saturn's small icy moons Phoebe and Hyperion.68: 20 Simulations of Chariklo's rings predict that ring particles can fall and accumulate on Chariklo's equator to form an equatorial ridge, similar to that on Saturn's moon Iapetus.69: 149
Chariklo is not in hydrostatic equilibrium because its dimensions and rotation period are incompatible with this state.70: 9 Although Chariklo's mass and density have not been measured due to its lack of known moons,71: 7 a range of possible masses and densities can be estimated by assuming Chariklo's rings are in a 1:3 spin-orbit resonance with Chariklo's rotation, similar to other ringed minor planets.72: 9 This gives a density range of 0.73–0.85 g/cm3,73: 9 which is expected for an icy body.74: 22 This density range corresponds to a mass range of (5.9–6.9)×1018 kg for Chariklo.75 If Chariklo was in hydrostatic equilibrium, it should have a density between 0.8–1.25 g/cm3 and a mass between (6–8)×1018 kg, depending on its dimensions.76: 22
Rotation
Chariklo has a synodic rotation period of 7.004 hours, with an uncertainty of 0.036 hours (2.2 minutes).7778: 8 Due to Chariklo's elongated shape, its apparent brightness from Earth changes as it rotates, although the amount of change depends on the viewing angle of Chariklo as seen from Earth.79: 3 Chariklo's brightness can vary as much as 0.13 magnitudes when looking at its equator, whereas its brightness changes may be undetectable when looking at its poles.80: 10 81: 1 Astronomers first attempted to measure Chariklo's rotation period in 1997, but were unable to detect any brightness changes since Chariklo was viewed pole-on from Earth at the time.82: 10 It was not until 2013 that astronomers were able to measure Chariklo's rotation period.83: 2
If Chariklo's rotation is aligned with its rings, then its rotational north pole would point in the direction (RA, Dec) = (151.0°, +41.8°).84 This translates to ecliptic coordinates (λ, β) = (137.6°, +27.9°),85 which means Chariklo's axial tilt is 62.1° with respect to the ecliptic.86
Surface composition and spectrum
The surface of Chariklo is dark and reddish with a low geometric albedo of 3.7%.87: 14 88: 10 In visible light, the reflectance spectrum of Chariklo appears featureless, lacking clear absorption features associated with compounds on its surface.89: 1 These characteristics led astronomers to classify Chariklo as a D-type asteroid.9091: 232 Astronomers have also classified Chariklo as part of the BR class of centaurs and trans-Neptunian objects, whose colors are considered intermediate between "spectrally neutral" (gray) and "very red".92: 1292 93: 181, 183
In near-infrared wavelengths, Chariklo's spectrum shows several absorption features that suggest its surface is composed of water ice, silicate minerals, amorphous carbon, and various complex organic compounds (also known as tholins).9495 Spectroscopic observations over different years have shown varying levels of water ice in Chariklo's near-infrared spectrum, which astronomers attribute to the changing viewing angle of Chariklo's water ice-rich rings.96 Near-infrared spectroscopy by the James Webb Space Telescope in 2022 has shown that Chariklo's surface contains water ice in crystalline form,97 contrary to initial beliefs that all water ice was concentrated in Chariklo's rings.98 Crystalline water ice is expected to be short-lived in space due to irradiation by high-energy particles, so astronomers hypothesize that Chariklo experiences continuous micro-impacts that either expose pristine material or trigger crystallization processes.99
No cometary activity
Chariklo does not appear to exbibit cometary activity, in contrast to the other ringed centaur 2060 Chiron.100: 4 101: 2 A 2014 analysis of Chariklo's appearance in high-resolution telescope images from 2007–2013 found no evidence of a dust coma surrounding Chariklo, placing an upper limit dust production rate of 2.5 kg/s.102: 4 Likewise, observations by the Very Large Telescope and Hubble Space Telescope in 2015 did not detect any signs of cometary jets or dust beyond 300 km (190 mi) from Chariklo.103104: 2 Chariklo is likely too cold and too far away from the Sun to exhibit cometary activity today.105: 12 However, the unstable nature of Chariklo's orbit suggests it is possible that it could have orbited closer to the Sun, meaning Chariklo could have been warmer and active in the past.106: 7 107: 12
Rings
Main article: Rings of Chariklo
A stellar occultation in 2013108109 revealed that Chariklo has two rings with radii 386 and 400 km and widths of about 6.9 km and 0.12 km respectively.110 The rings are approximately 14 km apart.111 This makes Chariklo the smallest known object to have rings. These rings are consistent with an edge-on orientation in 2008, which can explain Chariklo's dimming before 2008 and brightening since. Nonetheless, the elongated shape of Chariklo explains most of the brightness variability resulting in darker rings than previously determined.112 Furthermore, the rings can explain the gradual disappearance of the water-ice features in Chariklo's spectrum before 2008 and their reappearance thereafter if the water ice is in Chariklo's rings.113114115
The existence of a ring system around a minor planet was unexpected because it had been thought that rings could only be stable around much more massive bodies.116 Ring systems around minor bodies had not previously been discovered despite the search for them through direct imaging and stellar occultation techniques.117 Chariklo's rings should disperse over a period of at most a few million years, so either they are very young, or they are actively contained by shepherd moons with a mass comparable to that of the rings.118119120121 However, other research suggests that Chariklo's elongated shape combined with its fast rotation can clear material in an equatorial disk through Lindblad resonances and explain the survival and location of the rings, a mechanism valid also for the ring of Haumea.122
The team nicknamed the rings Oiapoque (the inner, more substantial ring) and Chuí (the outer ring), after the two rivers that form the northern and southern coastal borders of Brazil. A request for formal names will be submitted to the IAU at a later date.123
It has been confirmed that 2060 Chiron may have a similar pair of rings.124
Rings of Chariklo125: 11 126: 28Name | Nickname | Orbital radius (km) | Width (km) | Eccentricity | Normal optical depth | Surface density (g/cm2)127: 73 | Mass-equivalent diameter (km)128: 73 | Pole direction (RA) | Pole direction (Dec) | Radial separation (km) |
---|---|---|---|---|---|---|---|---|---|---|
C1R | Oiapoque | 385.9±0.4 | 4.8 to 9.1 | 0.005 to 0.022 | 0.4 (average)129 | 30–100 | ~2 | 151.03°±0.14° | +41.81°±0.07° | 13.9+5.2−3.4 |
C2R | Chuí | 399.8±0.6 | 0.1 to 1 | <0.017 | >0.1 | ? | ~1 | 150.91°±0.22° | +41.60°±0.12° |
Exploration
Main article: Camilla (spacecraft)
Camilla is a mission concept published in June 2018 that would launch a robotic probe to perform a single flyby of Chariklo and drop off a 100 kg (220 lb) impactor made of tungsten to excavate a crater approximately 10 m (33 ft) deep for remote compositional analysis during the flyby.130 The mission would be designed to fit under the cost cap of NASA's New Frontiers program, although it has not been formally proposed to compete for funding. The spacecraft would be launched in September 2026, using one gravity assist from Venus in February 2027 and Earth in December 2027 and 2029 to accelerate it out toward Jupiter.
See also
- List of centaurs (small Solar System bodies) § 10199
- 2060 Chiron, a large ringed centaur exhibiting cometary activity
Notes
External links
Wikimedia Commons has media related to 10199 Chariklo.- Barnett, Amanda (3 November 2024). "Asteroid Chariklo". science.nasa.gov. NASA.
- Johnston, Wm. Robert (21 September 2014). "(10199) Chariklo and ring system". Asteroids with Satellites Database--Johnston's Archive.
- 10199 Chariklo at AstDyS-2, Asteroids—Dynamic Site
- 10199 Chariklo at the JPL Small-Body Database
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Wood, Jeremy; Horner, Jonti; Hinse, Tobias C.; Marsden, Stephen C. (June 2017). "The Dynamical History of Chariklo and Its Rings". The Astronomical Journal. 153 (6). arXiv:1705.02378. Bibcode:2017AJ....153..245W. doi:10.3847/1538-3881/aa6981. S2CID 59151174. 245. https://doi.org/10.3847%2F1538-3881%2Faa6981 ↩
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Horner, J.; Evans, N. W.; Bailey, M. E. (November 2004). "Simulations of the Population of Centaurs I: The Bulk Statistics". Monthly Notices of the Royal Astronomical Society. 354 (3): 798–810. arXiv:astro-ph/0407400. Bibcode:2004MNRAS.354..798H. doi:10.1111/j.1365-2966.2004.08240.x. S2CID 16002759. https://doi.org/10.1111%2Fj.1365-2966.2004.08240.x ↩
The times given here are the "dyanamical half-lives", which is the time interval at which 50% of copies ("clones") of an object (in this case, Chariklo) are lost in an orbit simulation.[24]: 802 [27]: 4772 /wiki/Half-life ↩
Araujo, R. A. N.; Sfair, R.; Winter, O. C. (June 2016). "The Rings of Chariklo under Close Encounters with the Giant Planets". The Astrophysical Journal. 824 (2). arXiv:1604.07323. Bibcode:2016ApJ...824...80A. doi:10.3847/0004-637X/824/2/80. S2CID 119118722. 80. https://doi.org/10.3847%2F0004-637X%2F824%2F2%2F80 ↩
Araujo, R. A. N.; Sfair, R.; Winter, O. C. (June 2016). "The Rings of Chariklo under Close Encounters with the Giant Planets". The Astrophysical Journal. 824 (2). arXiv:1604.07323. Bibcode:2016ApJ...824...80A. doi:10.3847/0004-637X/824/2/80. S2CID 119118722. 80. https://doi.org/10.3847%2F0004-637X%2F824%2F2%2F80 ↩
Wood, Jeremy; Horner, Jonti; Hinse, Tobias C.; Marsden, Stephen C. (June 2017). "The Dynamical History of Chariklo and Its Rings". The Astronomical Journal. 153 (6). arXiv:1705.02378. Bibcode:2017AJ....153..245W. doi:10.3847/1538-3881/aa6981. S2CID 59151174. 245. https://doi.org/10.3847%2F1538-3881%2Faa6981 ↩
Horner, J.; Evans, N. W.; Bailey, M. E. (November 2004). "Simulations of the Population of Centaurs I: The Bulk Statistics". Monthly Notices of the Royal Astronomical Society. 354 (3): 798–810. arXiv:astro-ph/0407400. Bibcode:2004MNRAS.354..798H. doi:10.1111/j.1365-2966.2004.08240.x. S2CID 16002759. https://doi.org/10.1111%2Fj.1365-2966.2004.08240.x ↩
Wood, Jeremy; Horner, Jonti; Hinse, Tobias C.; Marsden, Stephen C. (June 2017). "The Dynamical History of Chariklo and Its Rings". The Astronomical Journal. 153 (6). arXiv:1705.02378. Bibcode:2017AJ....153..245W. doi:10.3847/1538-3881/aa6981. S2CID 59151174. 245. https://doi.org/10.3847%2F1538-3881%2Faa6981 ↩
Araujo, R. A. N.; Sfair, R.; Winter, O. C. (June 2016). "The Rings of Chariklo under Close Encounters with the Giant Planets". The Astrophysical Journal. 824 (2). arXiv:1604.07323. Bibcode:2016ApJ...824...80A. doi:10.3847/0004-637X/824/2/80. S2CID 119118722. 80. https://doi.org/10.3847%2F0004-637X%2F824%2F2%2F80 ↩
Wood, Jeremy; Horner, Jonti; Hinse, Tobias C.; Marsden, Stephen C. (June 2017). "The Dynamical History of Chariklo and Its Rings". The Astronomical Journal. 153 (6). arXiv:1705.02378. Bibcode:2017AJ....153..245W. doi:10.3847/1538-3881/aa6981. S2CID 59151174. 245. https://doi.org/10.3847%2F1538-3881%2Faa6981 ↩
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"AstDys (10199) Chariklo (March 2003) Ephemerides". Department of Mathematics, University of Pisa, Italy. Retrieved 3 April 2009. https://newton.spacedys.com/astdys/index.php?pc=1.1.3.1&n=10199&oc=500&y0=2003&m0=3&d0=9&h0=0&mi0=0&y1=2003&m1=3&d1=20&h1=0&mi1=0&ti=1.0&tiu=days ↩
Leiva, R.; Sicardy, B.; Camargo, J. I. B (August 2017). "Size and shape of Chariklo from multi-epoch stellar occultations". The Astronomical Journal. 154 (4). arXiv:1708.08934. Bibcode:2017AJ....154..159L. doi:10.3847/1538-3881/aa8956. S2CID 54032928. 159. https://doi.org/10.3847%2F1538-3881%2Faa8956 ↩
Leiva, R.; Sicardy, B.; Camargo, J. I. B (August 2017). "Size and shape of Chariklo from multi-epoch stellar occultations". The Astronomical Journal. 154 (4). arXiv:1708.08934. Bibcode:2017AJ....154..159L. doi:10.3847/1538-3881/aa8956. S2CID 54032928. 159. https://doi.org/10.3847%2F1538-3881%2Faa8956 ↩
Leiva, R.; Sicardy, B.; Camargo, J. I. B (August 2017). "Size and shape of Chariklo from multi-epoch stellar occultations". The Astronomical Journal. 154 (4). arXiv:1708.08934. Bibcode:2017AJ....154..159L. doi:10.3847/1538-3881/aa8956. S2CID 54032928. 159. https://doi.org/10.3847%2F1538-3881%2Faa8956 ↩
"Webb Spies Chariklo Ring System With High-Precision Technique". webbtelescope.org. Space Telescope Science Institute. 25 January 2023. Retrieved 27 June 2025. https://webbtelescope.org/contents/early-highlights/webb-spies-chariklo-ring-system-with-high-precision-technique ↩
Morgado, B. E.; Sicardy, B.; Braga-Ribas, F.; Desmars, J.; Gomes-Júnior, A. R.; Bérard, D.; et al. (January 2020). "Refined physical parameters for Chariklo's body and rings from stellar occultations observed between 2013 and 2020". Astronomy & Astrophysics. 652. arXiv:2107.07904. Bibcode:2021A&A...652A.141M. doi:10.1051/0004-6361/202141543. S2CID 236034389. A141. https://doi.org/10.1051%2F0004-6361%2F202141543 ↩
Morgado, B. E.; Sicardy, B.; Braga-Ribas, F.; Desmars, J.; Gomes-Júnior, A. R.; Bérard, D.; et al. (January 2020). "Refined physical parameters for Chariklo's body and rings from stellar occultations observed between 2013 and 2020". Astronomy & Astrophysics. 652. arXiv:2107.07904. Bibcode:2021A&A...652A.141M. doi:10.1051/0004-6361/202141543. S2CID 236034389. A141. https://doi.org/10.1051%2F0004-6361%2F202141543 ↩
Sicardy, B.; Benedetti-Rossi, G.; Buie, M. W.; Langlois, M.; Lellouch, E.; Camargo, J. I. B.; et al. (October 2015). Observations of Chariklo's rings in 2015 (PDF). European Planetary Science Congress 2015. Nantes, France. Bibcode:2015EPSC...10..750S. EPSC2015-750. https://meetingorganizer.copernicus.org/EPSC2015/EPSC2015-750-9.pdf ↩
Morgado, B. E.; Sicardy, B.; Braga-Ribas, F.; Desmars, J.; Gomes-Júnior, A. R.; Bérard, D.; et al. (January 2020). "Refined physical parameters for Chariklo's body and rings from stellar occultations observed between 2013 and 2020". Astronomy & Astrophysics. 652. arXiv:2107.07904. Bibcode:2021A&A...652A.141M. doi:10.1051/0004-6361/202141543. S2CID 236034389. A141. https://doi.org/10.1051%2F0004-6361%2F202141543 ↩
Sicardy, Bruno; Braga-Ribas, Felipe; Buie, Marc W.; Ortiz, José Luis; Roques, Françoise (December 2024). "Stellar occultations by trans-Neptunian objects". The Astronomy and Astrophysics Review. 32 (1). arXiv:2411.07026. Bibcode:2024A&ARv..32....6S. doi:10.1007/s00159-024-00156-x. S2CID 273963101. 6. /wiki/ArXiv_(identifier) ↩
Sicardy, Bruno; Braga-Ribas, Felipe; Buie, Marc W.; Ortiz, José Luis; Roques, Françoise (December 2024). "Stellar occultations by trans-Neptunian objects". The Astronomy and Astrophysics Review. 32 (1). arXiv:2411.07026. Bibcode:2024A&ARv..32....6S. doi:10.1007/s00159-024-00156-x. S2CID 273963101. 6. /wiki/ArXiv_(identifier) ↩
Sicardy, Bruno; Braga-Ribas, Felipe; Buie, Marc W.; Ortiz, José Luis; Roques, Françoise (December 2024). "Stellar occultations by trans-Neptunian objects". The Astronomy and Astrophysics Review. 32 (1). arXiv:2411.07026. Bibcode:2024A&ARv..32....6S. doi:10.1007/s00159-024-00156-x. S2CID 273963101. 6. /wiki/ArXiv_(identifier) ↩
Morgado, B. E.; Sicardy, B.; Braga-Ribas, F.; Desmars, J.; Gomes-Júnior, A. R.; Bérard, D.; et al. (January 2020). "Refined physical parameters for Chariklo's body and rings from stellar occultations observed between 2013 and 2020". Astronomy & Astrophysics. 652. arXiv:2107.07904. Bibcode:2021A&A...652A.141M. doi:10.1051/0004-6361/202141543. S2CID 236034389. A141. https://doi.org/10.1051%2F0004-6361%2F202141543 ↩
Morgado, B. E.; Sicardy, B.; Braga-Ribas, F.; Desmars, J.; Gomes-Júnior, A. R.; Bérard, D.; et al. (January 2020). "Refined physical parameters for Chariklo's body and rings from stellar occultations observed between 2013 and 2020". Astronomy & Astrophysics. 652. arXiv:2107.07904. Bibcode:2021A&A...652A.141M. doi:10.1051/0004-6361/202141543. S2CID 236034389. A141. https://doi.org/10.1051%2F0004-6361%2F202141543 ↩
Sicardy, Bruno; Braga-Ribas, Felipe; Buie, Marc W.; Ortiz, José Luis; Roques, Françoise (December 2024). "Stellar occultations by trans-Neptunian objects". The Astronomy and Astrophysics Review. 32 (1). arXiv:2411.07026. Bibcode:2024A&ARv..32....6S. doi:10.1007/s00159-024-00156-x. S2CID 273963101. 6. /wiki/ArXiv_(identifier) ↩
Morgado, B. E.; Sicardy, B.; Braga-Ribas, F.; Desmars, J.; Gomes-Júnior, A. R.; Bérard, D.; et al. (January 2020). "Refined physical parameters for Chariklo's body and rings from stellar occultations observed between 2013 and 2020". Astronomy & Astrophysics. 652. arXiv:2107.07904. Bibcode:2021A&A...652A.141M. doi:10.1051/0004-6361/202141543. S2CID 236034389. A141. https://doi.org/10.1051%2F0004-6361%2F202141543 ↩
Sicardy, Bruno; Braga-Ribas, Felipe; Buie, Marc W.; Ortiz, José Luis; Roques, Françoise (December 2024). "Stellar occultations by trans-Neptunian objects". The Astronomy and Astrophysics Review. 32 (1). arXiv:2411.07026. Bibcode:2024A&ARv..32....6S. doi:10.1007/s00159-024-00156-x. S2CID 273963101. 6. /wiki/ArXiv_(identifier) ↩
Leiva, R.; Sicardy, B.; Camargo, J. I. B (August 2017). "Size and shape of Chariklo from multi-epoch stellar occultations". The Astronomical Journal. 154 (4). arXiv:1708.08934. Bibcode:2017AJ....154..159L. doi:10.3847/1538-3881/aa8956. S2CID 54032928. 159. https://doi.org/10.3847%2F1538-3881%2Faa8956 ↩
Morgado, B. E.; Sicardy, B.; Braga-Ribas, F.; Desmars, J.; Gomes-Júnior, A. R.; Bérard, D.; et al. (January 2020). "Refined physical parameters for Chariklo's body and rings from stellar occultations observed between 2013 and 2020". Astronomy & Astrophysics. 652. arXiv:2107.07904. Bibcode:2021A&A...652A.141M. doi:10.1051/0004-6361/202141543. S2CID 236034389. A141. https://doi.org/10.1051%2F0004-6361%2F202141543 ↩
Morgado, B. E.; Sicardy, B.; Braga-Ribas, F.; Desmars, J.; Gomes-Júnior, A. R.; Bérard, D.; et al. (January 2020). "Refined physical parameters for Chariklo's body and rings from stellar occultations observed between 2013 and 2020". Astronomy & Astrophysics. 652. arXiv:2107.07904. Bibcode:2021A&A...652A.141M. doi:10.1051/0004-6361/202141543. S2CID 236034389. A141. https://doi.org/10.1051%2F0004-6361%2F202141543 ↩
Morgado, B. E.; Sicardy, B.; Braga-Ribas, F.; Desmars, J.; Gomes-Júnior, A. R.; Bérard, D.; et al. (January 2020). "Refined physical parameters for Chariklo's body and rings from stellar occultations observed between 2013 and 2020". Astronomy & Astrophysics. 652. arXiv:2107.07904. Bibcode:2021A&A...652A.141M. doi:10.1051/0004-6361/202141543. S2CID 236034389. A141. https://doi.org/10.1051%2F0004-6361%2F202141543 ↩
Morgado, B. E.; Sicardy, B.; Braga-Ribas, F.; Desmars, J.; Gomes-Júnior, A. R.; Bérard, D.; et al. (January 2020). "Refined physical parameters for Chariklo's body and rings from stellar occultations observed between 2013 and 2020". Astronomy & Astrophysics. 652. arXiv:2107.07904. Bibcode:2021A&A...652A.141M. doi:10.1051/0004-6361/202141543. S2CID 236034389. A141. https://doi.org/10.1051%2F0004-6361%2F202141543 ↩
Morgado, B. E.; Sicardy, B.; Braga-Ribas, F.; Desmars, J.; Gomes-Júnior, A. R.; Bérard, D.; et al. (January 2020). "Refined physical parameters for Chariklo's body and rings from stellar occultations observed between 2013 and 2020". Astronomy & Astrophysics. 652. arXiv:2107.07904. Bibcode:2021A&A...652A.141M. doi:10.1051/0004-6361/202141543. S2CID 236034389. A141. https://doi.org/10.1051%2F0004-6361%2F202141543 ↩
Leiva, R.; Sicardy, B.; Camargo, J. I. B (August 2017). "Size and shape of Chariklo from multi-epoch stellar occultations". The Astronomical Journal. 154 (4). arXiv:1708.08934. Bibcode:2017AJ....154..159L. doi:10.3847/1538-3881/aa8956. S2CID 54032928. 159. https://doi.org/10.3847%2F1538-3881%2Faa8956 ↩
Morgado, B. E.; Sicardy, B.; Braga-Ribas, F.; Desmars, J.; Gomes-Júnior, A. R.; Bérard, D.; et al. (January 2020). "Refined physical parameters for Chariklo's body and rings from stellar occultations observed between 2013 and 2020". Astronomy & Astrophysics. 652. arXiv:2107.07904. Bibcode:2021A&A...652A.141M. doi:10.1051/0004-6361/202141543. S2CID 236034389. A141. https://doi.org/10.1051%2F0004-6361%2F202141543 ↩
Leiva, R.; Sicardy, B.; Camargo, J. I. B (August 2017). "Size and shape of Chariklo from multi-epoch stellar occultations". The Astronomical Journal. 154 (4). arXiv:1708.08934. Bibcode:2017AJ....154..159L. doi:10.3847/1538-3881/aa8956. S2CID 54032928. 159. https://doi.org/10.3847%2F1538-3881%2Faa8956 ↩
Sicardy, B.; Leiva, R.; Renner, S.; Roques, F.; El Moutamid, M.; Santos-Sanz, P. (November 2018). "Ring dynamics around non-axisymmetric bodies with application to Chariklo and Haumea" (PDF). Nature Astronomy. 3: 146–153. arXiv:1811.09437. Bibcode:2019NatAs...3..146S. doi:10.1038/s41550-018-0616-8. S2CID 119236027. https://digital.csic.es/bitstream/10261/194408/1/IAA_2019_NatureA_PabloSantos.pdf ↩
Morgado, B. E.; Sicardy, B.; Braga-Ribas, F.; Desmars, J.; Gomes-Júnior, A. R.; Bérard, D.; et al. (January 2020). "Refined physical parameters for Chariklo's body and rings from stellar occultations observed between 2013 and 2020". Astronomy & Astrophysics. 652. arXiv:2107.07904. Bibcode:2021A&A...652A.141M. doi:10.1051/0004-6361/202141543. S2CID 236034389. A141. https://doi.org/10.1051%2F0004-6361%2F202141543 ↩
Leiva, R.; Sicardy, B.; Camargo, J. I. B (August 2017). "Size and shape of Chariklo from multi-epoch stellar occultations". The Astronomical Journal. 154 (4). arXiv:1708.08934. Bibcode:2017AJ....154..159L. doi:10.3847/1538-3881/aa8956. S2CID 54032928. 159. https://doi.org/10.3847%2F1538-3881%2Faa8956 ↩
Morgado, B. E.; Sicardy, B.; Braga-Ribas, F.; Desmars, J.; Gomes-Júnior, A. R.; Bérard, D.; et al. (January 2020). "Refined physical parameters for Chariklo's body and rings from stellar occultations observed between 2013 and 2020". Astronomy & Astrophysics. 652. arXiv:2107.07904. Bibcode:2021A&A...652A.141M. doi:10.1051/0004-6361/202141543. S2CID 236034389. A141. https://doi.org/10.1051%2F0004-6361%2F202141543 ↩
Morgado, B. E.; Sicardy, B.; Braga-Ribas, F.; Desmars, J.; Gomes-Júnior, A. R.; Bérard, D.; et al. (January 2020). "Refined physical parameters for Chariklo's body and rings from stellar occultations observed between 2013 and 2020". Astronomy & Astrophysics. 652. arXiv:2107.07904. Bibcode:2021A&A...652A.141M. doi:10.1051/0004-6361/202141543. S2CID 236034389. A141. https://doi.org/10.1051%2F0004-6361%2F202141543 ↩
Leiva, R.; Sicardy, B.; Camargo, J. I. B (August 2017). "Size and shape of Chariklo from multi-epoch stellar occultations". The Astronomical Journal. 154 (4). arXiv:1708.08934. Bibcode:2017AJ....154..159L. doi:10.3847/1538-3881/aa8956. S2CID 54032928. 159. https://doi.org/10.3847%2F1538-3881%2Faa8956 ↩
Chariklo's mass is calculated by multiplying density (ρ; kg/m3 units) by ellipsoid volume (V; m3 units): M = ρ V {\displaystyle M=\rho V} . Volume of an ellipsoid with semi-axes 143.8 × 135.2 × 99.1 km is approximately V = {\displaystyle V=} 8.07×1015 m3.[34] ↩
Leiva, R.; Sicardy, B.; Camargo, J. I. B (August 2017). "Size and shape of Chariklo from multi-epoch stellar occultations". The Astronomical Journal. 154 (4). arXiv:1708.08934. Bibcode:2017AJ....154..159L. doi:10.3847/1538-3881/aa8956. S2CID 54032928. 159. https://doi.org/10.3847%2F1538-3881%2Faa8956 ↩
Fornasier, S.; Lazzaro, D.; Alvarez-Candal, A.; Snodgrass, C.; Tozzi, G. P.; Carvano, J. M.; et al. (August 2014). "The Centaur 10199 Chariklo: investigation into rotational period, absolute magnitude, and cometary activity". Astronomy & Astrophysics. 568. Bibcode:2014A&A...568L..11F. doi:10.1051/0004-6361/201424439. S2CID 122707843. L11. https://doi.org/10.1051%2F0004-6361%2F201424439 ↩
Morgado, B. E.; Sicardy, B.; Braga-Ribas, F.; Desmars, J.; Gomes-Júnior, A. R.; Bérard, D.; et al. (January 2020). "Refined physical parameters for Chariklo's body and rings from stellar occultations observed between 2013 and 2020". Astronomy & Astrophysics. 652. arXiv:2107.07904. Bibcode:2021A&A...652A.141M. doi:10.1051/0004-6361/202141543. S2CID 236034389. A141. https://doi.org/10.1051%2F0004-6361%2F202141543 ↩
Fornasier, S.; Lazzaro, D.; Alvarez-Candal, A.; Snodgrass, C.; Tozzi, G. P.; Carvano, J. M.; et al. (August 2014). "The Centaur 10199 Chariklo: investigation into rotational period, absolute magnitude, and cometary activity". Astronomy & Astrophysics. 568. Bibcode:2014A&A...568L..11F. doi:10.1051/0004-6361/201424439. S2CID 122707843. L11. https://doi.org/10.1051%2F0004-6361%2F201424439 ↩
Morgado, B. E.; Sicardy, B.; Braga-Ribas, F.; Desmars, J.; Gomes-Júnior, A. R.; Bérard, D.; et al. (January 2020). "Refined physical parameters for Chariklo's body and rings from stellar occultations observed between 2013 and 2020". Astronomy & Astrophysics. 652. arXiv:2107.07904. Bibcode:2021A&A...652A.141M. doi:10.1051/0004-6361/202141543. S2CID 236034389. A141. https://doi.org/10.1051%2F0004-6361%2F202141543 ↩
Fornasier, S.; Lazzaro, D.; Alvarez-Candal, A.; Snodgrass, C.; Tozzi, G. P.; Carvano, J. M.; et al. (August 2014). "The Centaur 10199 Chariklo: investigation into rotational period, absolute magnitude, and cometary activity". Astronomy & Astrophysics. 568. Bibcode:2014A&A...568L..11F. doi:10.1051/0004-6361/201424439. S2CID 122707843. L11. https://doi.org/10.1051%2F0004-6361%2F201424439 ↩
Morgado, B. E.; Sicardy, B.; Braga-Ribas, F.; Desmars, J.; Gomes-Júnior, A. R.; Bérard, D.; et al. (January 2020). "Refined physical parameters for Chariklo's body and rings from stellar occultations observed between 2013 and 2020". Astronomy & Astrophysics. 652. arXiv:2107.07904. Bibcode:2021A&A...652A.141M. doi:10.1051/0004-6361/202141543. S2CID 236034389. A141. https://doi.org/10.1051%2F0004-6361%2F202141543 ↩
Fornasier, S.; Lazzaro, D.; Alvarez-Candal, A.; Snodgrass, C.; Tozzi, G. P.; Carvano, J. M.; et al. (August 2014). "The Centaur 10199 Chariklo: investigation into rotational period, absolute magnitude, and cometary activity". Astronomy & Astrophysics. 568. Bibcode:2014A&A...568L..11F. doi:10.1051/0004-6361/201424439. S2CID 122707843. L11. https://doi.org/10.1051%2F0004-6361%2F201424439 ↩
Morgado, B. E.; Sicardy, B.; Braga-Ribas, F.; Desmars, J.; Gomes-Júnior, A. R.; Bérard, D.; et al. (January 2020). "Refined physical parameters for Chariklo's body and rings from stellar occultations observed between 2013 and 2020". Astronomy & Astrophysics. 652. arXiv:2107.07904. Bibcode:2021A&A...652A.141M. doi:10.1051/0004-6361/202141543. S2CID 236034389. A141. https://doi.org/10.1051%2F0004-6361%2F202141543 ↩
"Coordinate Calculator". NASA/IPAC Extragalactic Database. California Institute of Technology. Retrieved 28 June 2025. Equatorial → Ecliptic, J2000 for equinox and epoch. NOTE: When inputting equatorial coordinates, specify the units in the format "RA 10h04m07.20s Dec +41d48m36.0s" instead of "RA 151.03° Dec 41.81°". https://ned.ipac.caltech.edu/coordinate_calculator?in_csys=Equatorial&in_equinox=J2000.0&obs_epoch=2000.0&ra=10h04m07.20s&dec=%2B41d48m36.0s&pa=0.0&out_csys=Ecliptic&out_equinox=J2000.0 ↩
The axial tilt or obliquity i is given by: i = 90 − β {\displaystyle i=90-\beta } . β is the ecliptic latitude of Chariklo's north pole direction, in degrees. ↩
Leiva, R.; Sicardy, B.; Camargo, J. I. B (August 2017). "Size and shape of Chariklo from multi-epoch stellar occultations". The Astronomical Journal. 154 (4). arXiv:1708.08934. Bibcode:2017AJ....154..159L. doi:10.3847/1538-3881/aa8956. S2CID 54032928. 159. https://doi.org/10.3847%2F1538-3881%2Faa8956 ↩
Morgado, B. E.; Sicardy, B.; Braga-Ribas, F.; Desmars, J.; Gomes-Júnior, A. R.; Bérard, D.; et al. (January 2020). "Refined physical parameters for Chariklo's body and rings from stellar occultations observed between 2013 and 2020". Astronomy & Astrophysics. 652. arXiv:2107.07904. Bibcode:2021A&A...652A.141M. doi:10.1051/0004-6361/202141543. S2CID 236034389. A141. https://doi.org/10.1051%2F0004-6361%2F202141543 ↩
Guilbert, A.; Barucci, M. A.; Brunetto, R.; Delsanti, A.; Merlin, F.; Alvarez-Candal, A.; et al. (July 2009). "A portrait of Centaur 10199 Chariklo". Astronomy & Astrophysics. 501 (2): 777–784. Bibcode:2009A&A...501..777G. doi:10.1051/0004-6361/200911660. S2CID 53477316. https://doi.org/10.1051%2F0004-6361%2F200911660 ↩
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Barucci, A.; Belskaya, I. N.; Fulchignoni, M.; Birlan, M.; et al. (September 2005). "Taxonomy of Centaurs and Trans-Neptunian Objects". The Astronomical Journal. 130 (3): 1291–1298. Bibcode:2005AJ....130.1291B. doi:10.1086/431957. S2CID 32008426. https://doi.org/10.1086%2F431957 ↩
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Duffard, R.; Pinilla-Alonso, N.; Ortiz, J. L.; Alvarez-Candal, A.; Sicardy, B.; Santos-Sanz, P.; et al. (August 2014). "Photometric and spectroscopic evidence for a dense ring system around Centaur Chariklo". Astronomy & Astrophysics. 568. arXiv:1407.4599. Bibcode:2014A&A...568A..79D. doi:10.1051/0004-6361/201424208. S2CID 56440733. A79. https://doi.org/10.1051%2F0004-6361%2F201424208 ↩
"Webb Spies Chariklo Ring System With High-Precision Technique". webbtelescope.org. Space Telescope Science Institute. 25 January 2023. Retrieved 27 June 2025. https://webbtelescope.org/contents/early-highlights/webb-spies-chariklo-ring-system-with-high-precision-technique ↩
Duffard, R.; Pinilla-Alonso, N.; Ortiz, J. L.; Alvarez-Candal, A.; Sicardy, B.; Santos-Sanz, P.; et al. (August 2014). "Photometric and spectroscopic evidence for a dense ring system around Centaur Chariklo". Astronomy & Astrophysics. 568. arXiv:1407.4599. Bibcode:2014A&A...568A..79D. doi:10.1051/0004-6361/201424208. S2CID 56440733. A79. https://doi.org/10.1051%2F0004-6361%2F201424208 ↩
"Webb Spies Chariklo Ring System With High-Precision Technique". webbtelescope.org. Space Telescope Science Institute. 25 January 2023. Retrieved 27 June 2025. https://webbtelescope.org/contents/early-highlights/webb-spies-chariklo-ring-system-with-high-precision-technique ↩
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The edges of the C1R ring are more opaque than the center of the C1R ring.[32]: 28 ↩
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