Mysteries Department
Sign inRequest access
Evidence · Tabby's star (KIC 8462852)

The deep Kepler dips are all skewed; the 2019 dip is not

At Kepler's 29.4-minute cadence every Kepler dip deeper than 0.3 per cent (D140, D792, D1495, D1519, D1540, D1568) has a half-depth ingress shorter than its egress, with ratios of 0.57 to 0.77 and 35 to 44 per cent of the deficit before minimum; the 2019 dip gives 1.29 and 59 per cent, and its best model is symmetric.

Supported0

What it means

Key questionWhat blocks the light during the deep, irregular dips?
Most likely: clumps of fine dust orbiting the star, released by comets, planetesimals or other bodies close to it
Most likelyunchanged
Still possiblewas No evidence yet

Next steps 4

1
Extract a Sector 75 light curve from the FFIs with TESScut and run the same dip search; it is the one covered sector with no light-curve product.
~3 h
—not judged
2
Fit the 2019 transit with a free eccentric orbit and a ring (Zhu et al. 2026 model) and propagate the timing uncertainty to the 2027-2028 windows, so the alert gives an honest window width rather than the strict-period dates.
~6 h
—not judged
3
Close the 1,301.44-1,301.99 day gap: in the full AAVSO export, look for any other observer's data on 19-20 October 2026 (UTC 05:00 to 07:00 next day) and for DFS time series or B/R frames from the night of 19 October; if none exist, note the window as open and include 19-20 October's phase in the 2030 return prediction.
~1 h
—not judged
4
Post an observing request (AAVSO alert notice or forum) for the next predicted returns: 15-16 January 2027 (if window 4 is 1,355-1,356 d as the coverage map suggests), 28 February to 2 March 2027 (window 5), and 17-23 February 2028 (window 1), with the expected depth of 1.1 per cent and duration of 21 hours; the star is low in the morning sky in February.
~1 h
—not judged
Ranked by how likely each is to move the key question, for the time it takes

How it was found 1 run

Result. The limb-darkened transit is the preferred shape by a wide margin and its duration is consistent with a thousand-day circular orbit around this star; the deep Kepler dips are uniformly skewed in the opposite sense. Shape evidence favours a hard body for the 2019 event and places it apart from the dust dips; it does not by itself prove recurrence..
BIC per model; derived transit parameters; ingress/egress ratio and deficit fraction before minimum per dip{'dBIC': {'planet': 0, 'gaussian': 195.8, 'skewgauss': 201, 'trapezoid': 26.8}, 'planet': {'b': 0.79, 'a_rs': 296, 'rp_rs': 0.11, 't0_BTJD': 1730.156, 'depth_pct': 1.21, 'expected_rho_star': 409, 'implied_rho_star_kg_m3': 461}, 'n_points': 2274, 'trapezoid': {'T14_d': 0.856, 'egress_d': 0.29, 'depth_pct': 1.17, 'ingress_d': 0.186}, 'planet_chi2': 2365, 'skewgauss_asymmetry': 0.89, 'asymmetry_2019_binned': {'A': 1.29, 'depth_pct': 1.25, 'deficit_before': 0.59}, 'asymmetry_kepler_deep': {'D140': [0.75, 0.44], 'D792': [0.77, 0.42], 'D1495': [0.6, 0.38], 'D1519': [0.65, 0.36], 'D1540': [0.57, 0.36], 'D1568': [0.6, 0.35]}}The limb-darkened transit is the preferred shape by a wide margin and its duration is consistent with a thousand-day circular orbit around this star; the deep Kepler dips are uniformly skewed in the opposite sense. Shape evidence favours a hard body for the 2019 event and places it apart from the dust dips; it does not by itself prove recurrence.
Notes from the run

D260 and D426 are dropped from the asymmetry table (too shallow for stable half-depth crossings). The 2019 model-free asymmetry is noisy; the model comparison is the primary result.

Sources 1

Cite it

Mysteries Department. (2026). The deep Kepler dips are all skewed; the 2019 dip is not [Evidence EVD0DEC1DA7KBCT]. https://mysteriesdept.com/r/EVD0DEC1DA7KBCT
Private beta Downloads are for beta members

We're in a private beta while we get things right. Everything here is free to read; downloading datasets, sources and code is open to members for now.

It takes a couple of minutes. We'll reply by email.