KMT-2019-BLG-2073: Fourth Free-floating Planet Candidate with θ E < 10 μas
We analyze the very short Einstein timescale ( t E ≃ 7 hr) event KMT-2019-BLG-2073. Making use of the pronounced finite-source effects generated by the clump giant source, we measure the Einstein radius θ E ≃ 4.8 μ as and so infer a mass M = 59 M ⊕ ( π rel / 16 μ as ) − 1 , where π rel is the lens-s...
Gespeichert in:
Veröffentlicht in: | The Astronomical journal 2021-07, Vol.162 (1), p.15 |
---|---|
Hauptverfasser: | , , , , , , , , , , , , , , , , , , , |
Format: | Artikel |
Sprache: | eng |
Schlagworte: | |
Online-Zugang: | Volltext bestellen |
Tags: |
Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
|
Zusammenfassung: | We analyze the very short Einstein timescale (
t
E
≃ 7 hr) event KMT-2019-BLG-2073. Making use of the pronounced finite-source effects generated by the clump giant source, we measure the Einstein radius
θ
E
≃ 4.8
μ
as and so infer a mass
M
=
59
M
⊕
(
π
rel
/
16
μ
as
)
−
1
, where
π
rel
is the lens-source relative parallax. We find no significant evidence for a host of this planetary-mass object, though one could be present at sufficiently wide separation. If so, it would be detectable after about 10 yr. This is the fourth isolated microlens with a measured Einstein radius
θ
E
< 10
μ
as, which we argue is a useful threshold for a “likely free-floating planet (FFP)” candidate. We outline a new approach to constructing a homogeneous sample of giant-star finite-source/point-lens (FSPL) events, within which the subsample of FFP candidates can be statistically analyzed. We illustrate this approach using 2019 KMTNet data and show that there appears to be a large
θ
E
gap between the two FFP candidates and the 11 other FSPL events. We argue that such sharp features are more identifiable in a sample selected on
θ
E
compared to the traditional approach of identifying candidates based on short
t
E
. |
---|---|
ISSN: | 0004-6256 1538-3881 |
DOI: | 10.3847/1538-3881/abfc4a |