Pole, Pericenter, and Nodes of the Interstellar Minor Body A/2017 U1

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Published November 2017 © 2017. The American Astronomical Society. All rights reserved.
, , Citation Carlos de la Fuente Marcos and Raúl de la Fuente Marcos 2017 Res. Notes AAS 1 5 DOI 10.3847/2515-5172/aa96b4

This article is corrected by 2017 Res. Notes AAS 1 9

2515-5172/1/1/5

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Interstellar minor bodies can be identified by their positive barycentric energy (i.e., they follow hyperbolic paths as their orbital eccentricities, e, are $\gt 1$) and/or by their unusual chemical composition even if their $e\lt 1$—e.g., the comets C/1996 B2 (Hyakutake) (Mumma et al. 1996) or 96P/Machholz 1 (Langland-Shula & Smith 2007; Schleicher 2008). They can come from deep space or be produced locally, after close encounters with the planets or the Sun—e.g., comet C/1980 E1 (Bowell) was ejected from the solar system with e = 1.0577 after a flyby with Jupiter (Buffoni et al. 1982; Meech et al. 2009; Branham 2013). Captured interstellar minor bodies can be returned to deep space after flybys—e.g., comet 96P/Machholz 1 may be ejected in the relatively near future (de la Fuente Marcos et al. 2015). Interstellar minor bodies represent a rare and unique opportunity to have direct access to material from beyond the solar system and the likelihood of observing them has been studied thoroughly (McGlynn & Chapman 1989; Kresak 1992; Sen & Rama 1993; Moro-Martín et al. 2009; Jura 2011; Cook et al. 2016; Engelhardt et al. 2017).

Here, we explore some peculiar orbital features of the recently discovered asteroid A/2017 U1 (Bacci et al. 2017) 1 that may help in understanding its nature. The discussion presented here is based on data publicly available from JPL's Small-Body Database, 2 but the results are novel and have not appeared elsewhere. Its heliocentric orbit determination (barycentric values in parentheses) as of 2017 October 28 is: perihelion distance, q = 0.254 ± 0.002 au (0.257 au), e = 1.196 ± 0.004 (1.199), inclination, i = 122fdg6 ± 0fdg2 (122fdg9), longitude of the ascending node, Ω = 24fdg605 ± 0fdg007 (24fdg791), and argument of perihelion, ω = 241fdg5 ± 0fdg3 (241fdg8); 3 this solution is based on 59 observations for a data-arc span of 12 days. The number of known hyperbolic comets stands at 333 and there are five objects with $e\gt 1.01$—C/1947 F1 (Rondanina-Bester), e = 1.0165, C/1980 E1, e = 1.0577, C/1997 P2 (Spacewatch), e = 1.0279, C/1999 U2 (SOHO), e = 1.0162, and C/2008 J4 (McNaught), e = 1.0279. A/2017 U1 is a clear outlier, at the ∼49σ level, when considering the average value of the eccentricity of known hyperbolic comets, 1.002 ± 0.004. Some, perhaps all, the comets with $e\gt 1.01$ have been ejected after close encounters with the Sun or the planets.

Regarding the orientation of its orbit in space, the positions of pericenters—ecliptic coordinates at pericenter, $({l}_{q},{b}_{q})$—and poles—projected pole positions, $({l}_{{\rm{p}}},{b}_{{\rm{p}}})$—of known hyperbolic comets computed as described by de la Fuente Marcos & de la Fuente Marcos (2016) are displayed in figure 1, top and middle panels. The orientation of the orbital plane of A/2017 U1 seems to be away from any obvious clusters (real or induced by observational biases). The closest objects in terms of polar separation, ${\alpha }_{{\rm{p}}}$, are C/1970 N1 (Abe) (4fdg79) and C/2014 A4 (SONEAR) (4fdg50). When considering both ${\alpha }_{{\rm{p}}}$ and pericenter separations, ${\alpha }_{q}$, the smallest relative angular separations are $\gt 20^\circ $. The distributions of ${\alpha }_{q}$ and ${\alpha }_{{\rm{p}}}$ of all the pairs in the sample are plotted in the bottom panels. The hyperbolic comets with the closest mutual orbital orientation are the pieces of C/1986 P1 (Wilson), C/1996 J1-A and C/1996 J1-B (Evans-Drinkwater), and C/2011 J2 and C/2011 J2-B (LINEAR), all of them fragmented comets. Some of the clustering visible in figure 1, top and middle panels, may be due to dynamically correlated objects, probably the result of break-ups. The descending node of A/2017 U1 is located at 0.355 au and the ascending node at 1.301 au, well away from the paths of the planets of the solar system and the Sun.

Figure 1.

Figure 1. Pericenters (top panel) and poles (middle panel) of the known hyperbolic minor bodies (334); A/2017 U1 is plotted in red. Distributions of possible angular separations between pericenters (bottom, left-hand side panel) and poles (bottom, right-hand side panel) of the same sample.

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All these orbital properties appear to confirm A/2017 U1 as the first known interstellar asteroid (either truly extrasolar or, far less likely, a returning former solar system minor body that was ejected very long ago).

We thank A. I. Gómez de Castro, I. Lizasoain and L. Hernández Yáñez of the Universidad Complutense de Madrid (UCM) for providing access to computing facilities. This work was partially supported by the Spanish "Ministerio de Economía y Competitividad" (MINECO) under grant ESP2014-54243-R. Part of the calculations and the data analysis were completed on the EOLO cluster of the UCM. EOLO, the HPC of Climate Change of the International Campus of Excellence of Moncloa, is funded by the MECD and MICINN. This is a contribution to the CEI Moncloa. In preparation of this Note, we made use of the NASA Astrophysics Data System and the MPC data server.

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10.3847/2515-5172/aa96b4