Rafael Sfair

Dr. Rafael Sfair

Unesp, São Paulo, Brazil
+1
orcid

Research Focus & Metrics

Academic Career Length

22Years (2005-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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26 March 2014 in Nature
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FBF. Braga-Ribas
F. Braga-Ribas
BSB. Sicardy
B. Sicardy
JOJ. L. Ortiz
J. L. Ortiz
CSC. Snodgrass
C. Snodgrass
FRF. Roques
F. Roques
DLD. G. Lambas
D. G. Lambas

8 February 2023 in Nature
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Journal Article
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BMB. E. Morgado
B. E. Morgado
BSB. Sicardy
B. Sicardy
FBF. Braga-Ribas
F. Braga-Ribas
JOJ. L. Ortiz
J. L. Ortiz
HSH. Salo
H. Salo
JWJ. de Wit
J. de Wit

25 August 2021 in Astronomy & Astrophysics
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Journal Article
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BMB. E. Morgado
B. E. Morgado
BSB. Sicardy
B. Sicardy
FBF. Braga-Ribas
F. Braga-Ribas
JDJ. Desmars
J. Desmars
AGA. R. Gomes-Júnior
A. R. Gomes-Júnior
CZC. A. Zuluaga
C. A. Zuluaga
Context. The Centaur (10199) Chariklo has the first ring system discovered around a small object. It was first observed using stellar occultation in 2013. Stellar occultations allow sizes and shapes to be determined with kilometre accuracy, and provide the characteristics of the occulting object and its vicinity. Aims. Using stellar occultations observed between 2017 and 2020, our aim is to constrain the physical parameters of Chariklo and its rings. We also determine the structure of the rings, and obtain precise astrometrical positions of Chariklo. Methods. We predicted and organised several observational campaigns of stellar occultations by Chariklo. Occultation light curves were measured from the datasets, from which ingress and egress times, and the ring widths and opacity values were obtained. These measurements, combined with results from previous works, allow us to obtain significant constraints on Chariklo’s shape and ring structure. Results. We characterise Chariklo’s ring system (C1R and C2R), and obtain radii and pole orientations that are consistent with, but more accurate than, results from previous occultations. We confirm the detection of W-shaped structures within C1R and an evident variation in radial width. The observed width ranges between 4.8 and 9.1 km with a mean value of 6.5 km. One dual observation (visible and red) does not reveal any differences in the C1R opacity profiles, indicating a ring particle size larger than a few microns. The C1R ring eccentricity is found to be smaller than 0.022 (3σ), and its width variations may indicate an eccentricity higher than ~0.005. We fit a tri-axial shape to Chariklo’s detections over 11 occultations, and determine that Chariklo is consistent with an ellipsoid with semi-axes of 143.8−1.5+1.4, 135.2−2.8+1.4, and 99.1−2.7+5.4 km. Ultimately, we provided seven astrometric positions at a milliarcsecond accuracy level, based on Gaia EDR3, and use it to improve Chariklo’s ephemeris.

15 June 2016 in The Astrophysical Journal
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RAR. A. N. Araujo
R. A. N. Araujo
RSRafael Sfair
Rafael Sfair
OWO. C. Winter
O. C. Winter
The Centaur population is composed of minor bodies wandering between the giant planets that frequently perform close gravitational encounters with these planets, leading to a chaotic orbital evolution. Recently, the discovery of two well-defined narrow rings was announced around the Centaur 10199 Chariklo. The rings are assumed to be in the equatorial plane of Chariklo and to have circular orbits. The existence of a well-defined system of rings around a body in such a perturbed orbital region poses an interesting new problem. Are the rings of Chariklo stable when perturbed by close gravitational encounters with the giant planets? Our approach to address this question consisted of forward and backward numerical simulations of 729 clones of Chariklo, with similar initial orbits, for a period of 100 Myr. We found, on average, that each clone experiences during its lifetime more than 150 close encounters with the giant planets within one Hill radius of the planet in question. We identified some extreme close encounters that were able to significantly disrupt or disturb the rings of Chariklo. About 3% of the clones lose their rings and about 4% of the clones have their rings significantly disturbed. Therefore, our results show that in most cases (more than 90%), the close encounters with the giant planets do not affect the stability of the rings in Chariklo-like systems. Thus, if there is an efficient mechanism that creates the rings, then these structures may be common among these kinds of Centaurs.

31 May 2012 in Icarus
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RFRobert S. French
Robert S. French
MSMark R. Showalter
Mark R. Showalter
RSRafael Sfair
Rafael Sfair
CACarlos A. Argüelles
Carlos A. Argüelles
MPMyriam Pajuelo
Myriam Pajuelo
PNPhilip D. Nicholson
Philip D. Nicholson

13 November 2021 in Monthly Notices of the Royal Astronomical Society
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GVG Valvano
G Valvano
OWO C Winter
O C Winter
RSRafael Sfair
Rafael Sfair
ROR Machado Oliveira
R Machado Oliveira
GBG Borderes-Motta
G Borderes-Motta
TMT S Moura
T S Moura
The 99942 Apophis close encounter with Earth in 2029 may provide information about asteroid’s physical characteristics and measurements of Earth’s effects on the asteroid surface. In this work, we analysed the surface and the nearby dynamics of Apophis. The possible effects of its 2029 encounter on the surface and environment vicinity are also analysed. We consider a 340 m polyhedron with a uniform density (1.29, 2.2, and 3.5 g cm−3). The slope angles are computed, as well their variation that arises during the close approach. Such variation reaches 4° when low densities are used in our simulations and reaches 2° when the density is high. The zero-velocity curves, the equilibrium points, and their topological classification are obtained. We found four external equilibrium points and two of them are linearly stable. We also perform numerical simulations of bodies orbiting the asteroid, taking into account the irregular gravitational field of Apophis and two extra scenarios of perturbations: the solar radiation pressure and the Earth’s perturbation during the close approach. The radiation pressure plays an important role in the vicinity of the asteroid, only cm-sized particles survived for the time of integration. For densities of 2.2 and 3.5 g cm−3, a region of 5 cm radius particles survived for 30 yr of the simulation, and for 1.29 g cm−3, only particles with 15 cm of radius survived. The ejections and collisions are about 30–50 times larger when the close encounter effect is added but around 56–59 per cent of particles still survive the encounter.