# Deep Long Asymmetric Occultation in EPIC 204376071

**Authors:** S. Rappaport, G. Zhou, A. Vanderburg, A. Mann, M.H. Kristiansen, K., Olah, T.L. Jacobs, E. Newton, M.R. Omohundro, D. LaCourse, H.M. Schwengeler,, I.A. Terentev, D.W. Latham, A. Bieryla, M. Soares-Furtado, L.G. Bouma, M.J., Ireland, J. Irwin

arXiv: 1902.08152 · 2019-03-06

## TL;DR

A young M star exhibits a rare, deep occultation event likely caused by orbiting dust or transient dusty material, with implications for understanding circumstellar environments and transient phenomena.

## Contribution

This study reports the discovery of a unique deep occultation in a young M star and models potential dust-based causes, advancing knowledge of circumstellar dust structures.

## Key findings

- Deep occultation lasting 1 day observed in a young M star.
- Possible causes include orbiting dust or transient accretion events.
- Estimated dust mass required is at least 10^19 grams.

## Abstract

We have discovered a young M star of mass $0.16\,M_\odot$ and radius $0.63\,R_\odot$, likely in the Upper Sco Association, that exhibits only a single $80\%$ deep occultation of 1-day duration. The star has frequent flares and a low-amplitude rotational modulation, but is otherwise quiet over 160 days of cumulative observation during K2 Campaigns C2 and C15. We discuss how such a deep eclipse is not possible by one star crossing another in any binary or higher-order stellar system in which no mass transfer has occurred. The two possible explanations we are left with are (1) orbiting dust or small particles (e.g., a disk bound to a smaller orbiting body, or unbound dust that emanates from such a body); or (2) a transient accretion event of dusty material near the corotation radius of the star. In either case, the time between such occultation events must be longer than $\sim$80 days. We model a possible orbiting occulter both as a uniform elliptically shaped surface (e.g., an inclined circular disk) and as a `dust sheet' with a gradient of optical depth behind its leading edge. The required masses in such dust features are then $\gtrsim 3 \times 10^{19}$ g and $\gtrsim 10^{19}$ g, for the two cases, respectively.

## Full text

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## Figures

23 figures with captions in the complete paper: https://tomesphere.com/paper/1902.08152/full.md

## References

98 references — full list in the complete paper: https://tomesphere.com/paper/1902.08152/full.md

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Source: https://tomesphere.com/paper/1902.08152