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arXiv 1908.06645astro-ph.EP
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海王星外天体(84922)2003 VS2通过恒星掩星

The trans-Neptunian object (84922) 2003 VS2 through stellar occultations

Gustavo Benedetti-Rossi, P. Santos-Sanz, J. L. Ortiz, M. Assafin, B. Sicardy, N. Morales, R. Vieira-Martins, R. Duffard, F. Braga-Ribas, F. L. Rommel, J. I. B. … 展开作者

Gustavo Benedetti-Rossi, P. Santos-Sanz, J. L. Ortiz, M. Assafin, B. Sicardy, N. Morales, R. Vieira-Martins, R. Duffard, F. Braga-Ribas, F. L. Rommel, J. I. B. Camargo, J. Desmars, A. F. Colas, F. Vachier, Alvarez-Candal, E. Fernández-Valenzuela, L. Almenares, R. Artola, T. -P. Baum, R. Behrend, D. Bérard, F. Bianco, N. Brosch, A. Ceretta, C. A. Colazo, A. R. Gomes-Junior, V. D. Ivanov, E. Jehin, S. Kaspi, J. Lecacheux, A. Maury, R. Melia, S. Moindrot, B. Morgado, C. Opitom, A. Peyrot, J. Pollock, A. Pratt, S. Roland, J. Spagnotto, G. Tancredi, J. -P. Teng, P. Cacella, M. Emilio, F. Feys, R. Gil-Hutton, C. Jacques, D. I. Machado, M. Malacarne, I. Manulis, A. C. Milone, G. Rojas, R. Sfair

摘要:

本文介绍了三次全球性的观测活动的结果,这三次观测活动导致了冥王星天体(84922)2003~VS $_2$探测到两次单弦和一次多弦恒星掩星。从2013年和2014年的单弦掩星中,我们获得了该物体的精确天体测量位置,而从2014年11月7日的多弦掩星中,我们获得了掩星时最适合身体边缘的椭圆的参数。我们还获得了短期的测光数据的机构,以获得其在掩星的旋转相位。旋转光变曲线呈现出0.141 $\pm$ 0.009马格的峰-峰振幅。这使我们能够重建该天体的三维形状,其主半轴为$a = 313.8 \pm 7.1$ km、$b = 265.5^{+8.8}_{-9.8}$ km和$c = 247.3^{+26.6}_{-43.6}$ km,这与雅可比三轴平衡图不一致。计算得到的球体积当量直径$548.3 ^{+29.5}_{-44.6}$ km比由Herschel数据计算得到的2003~VS $_2$的辐射直径$523 \pm 35$ km大5%,但在误差范围内仍与之一致。从这些结果中,我们还可以导出几何常数($0.123 ^{+0.015}_{-0.014}$),并在假设该物体是麦克劳林椭球体的情况下,导出冥王星的密度$ρ= 1400^{+1000}_{-300}$。恒星在掩星期间的消失和重现并没有显示出任何令人信服的证据来证明一个全球性的大气,考虑到纯氮大气的压力上限约为1微巴,也没有在主体周围的次要特征(例如环或卫星)。

英文摘要:

We present results from three world-wide campaigns that resulted in the detections of two single-chord and one multi-chord stellar occultations by the Plutino object (84922) 2003~VS$_2$. From the single-chord occultations in 2013 and 2014 we obtained accurate astrometric positions for the object, while from the multi-chord occultation on November 7th, 2014, we obtained the parameters of the best-fitting ellipse to the limb of the body at the time of occultation. We also obtained short-term photometry data for the body in order to derive its rotational phase during the occultation. The rotational light curve present a peak-to-peak amplitude of 0.141 $\pm$ 0.009 mag. This allows us to reconstruct the three-dimensional shape of the body, with principal semi-axes $a = 313.8 \pm 7.1$ km, $b = 265.5^{+8.8}_{-9.8}$ km, and $c = 247.3^{+26.6}_{-43.6}$ km, which is not consistent with a Jacobi triaxial equilibrium figure. The derived spherical volume equivalent diameter of $548.3 ^{+29.5}_{-44.6}$ km is about 5\% larger than the radiometric diameter of 2003~VS$_2$ derived from Herschel data of $523 \pm 35$ km, but still compatible with it within error bars. From those results we can also derive the geometric albedo ($0.123 ^{+0.015}_{-0.014}$) and, under the assumption that the object is a Maclaurin spheroid, the density $ρ= 1400^{+1000}_{-300}$ for the plutino. The disappearances and reappearances of the star during the occultations do not show any compelling evidence for a global atmosphere considering a pressure upper limit of about 1 microbar for a pure nitrogen atmosphere, nor secondary features (e.g. rings or satellite) around the main body.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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