AI summary · arXiv: 2610.34806v1 · astro-ph.EP

The anomalously large transiting planet around Boyajian's star: evidence for a circumplanetary ring

Wei Zhu (Tsinghua), Quanyi Liu (Tsinghua)

Original paper Submitted to arXiv on 26 Oct. 2026 9 pages, 3 figures, 1 table; submitted License: CC BY 4.0

The essentials

An opaque ring around a Jupiter-sized companion can explain Boyajian’s star’s unusually deep planetary transit, but the single available transit provides only marginal statistical support.

Question

Can circumplanetary rings explain the anomalously large radius inferred for the massive, cool transiting companion to Boyajian’s star? Does the TESS transit distinguish a ringed planet from a bare spherical planet?

Method

The authors analyzed the TESS Sector 15 single transit at 2-minute cadence, detrended a ±1.5-day segment, and fitted spherical and ringed-planet models. Their JoJo ring code integrates occulted stellar intensity using boundary integrals; ring fits fixed the planet radius at 1.1 Jupiter radii, assumed full opacity, and tested inner ring radii of 1.0 and 1.1 planetary radii. Posterior sampling used 64 walkers with 10,000 steps each, discarding the first 3,000; model-comparison statistics used 718 points within ±0.5 days of mid-transit.

Findings

  • Result The spherical fit reproduces the previously reported anomalous companion radius of approximately 1.7 Jupiter radii.
    See the passage in the paper
    Consequently, the derived companion radius from our fit, $R_{\rm c}\simeq 1.74\,R_{\rm Jup}$, is consistent with their $1.7\pm 0.1\,R_{\rm Jup}$, confirming that it is unusually large.
  • Result With the planetary radius fixed at 1.1 Jupiter radii, the ring fits yield an extended, highly flattened annulus with an outer radius of approximately 3.1–4.4 planetary radii.
    See the passage in the paper
    With the planetary radius fixed at $R_{\rm p}/R_{\star}=0.070$, the ring outer radius is $r_{\rm out}\simeq 0.22$–$0.31\,R_{\star}$, corresponding to $\sim 3.1$–$4.4\,R_{\rm p}$, and the ring has a flatness of $f_{\rm r}\simeq 0.8$–$0.9$ and a projected obliquity of $\theta_{\perp}\simeq 74$–$81^{\circ}$.
  • Result The ring improves chi-squared by approximately 14 for two additional parameters, but the BIC differences leave the models statistically nearly indistinguishable.
    See the passage in the paper
    After the penalty due to two more free parameters is taken into account, the two interpretations are statistically nearly indistinguishable, with $\Delta{\rm BIC}\simeq-0.4$ to $-1.3$ in favour of the ring model.
  • Authors’ interpretation The authors interpret the inferred ring as a possible debris annulus near the Roche limit, potentially supplied by the minor-body reservoir associated with the star’s historic dimming.
    See the passage in the paper
    First, the ring extends nearly to the companion’s Roche limit. Given the location of the companion, it is a debris ring likely sustained by the disruption of comets or small satellites, which may be the same minor-body reservoir invoked to explain the historic dipping activity of this star.

Limitations

  • The ring orientation is weakly constrained by a single noisy transit, and spot crossing could partly explain the feature favoring the ring.
    See the passage in the paper
    We caution, however, that the ring orientation is only weakly constrained by the single available transit of relatively poor data quality, and that the apparent feature that drives the ring fit could in part be spot crossing (Sect. IV).
  • A single transit does not constrain the orbital period or shape, so these were fixed in the modeling.
    See the passage in the paper
    Because a single transit does not constrain the orbital period or the orbital shape, we fixed $P=1030$ d, $e=0$ and $\omega=90^{\circ}$.
  • The ring’s inner radius is poorly constrained, with larger assumed inner radii requiring potentially implausible outer radii.
    See the passage in the paper
    As will be shown later in the case of Boyajian’s star, $r_{\rm in}$ of the ring model is not well constrained by itself, but a larger $r_{\rm in}$ pushes $r_{\rm out}$ out of the physically plausible range because the cross-sectional area should be conserved.

Why it matters

The authors offer a geometric explanation for the apparent radius anomaly without requiring an intrinsically inflated cool giant planet, rather than establishing a ring detection. They argue that precise repeat-transit photometry, particularly during ingress and egress, can distinguish the competing interpretations.

Written by AI from the paper. Passages are checked word for word against the text we analysed; the rest may contain errors.

AI-generated keywords: Circumplanetary rings; Boyajian’s star; Transit photometry; Radius anomaly; TESS observations

Read further

  • Comprehensive Summary
  • Layman's Summary
  • Blog article
  • Original abstract
Wei Zhu and Quanyi Liu investigate whether circumplanetary rings could explain the unexpectedly large apparent size of a transiting companion to Boyajian’s star, also known as Tabby’s star. An earlier study reported a companion mass of 9.4 Jupiter masses, with uncertainties of +4.9 and −4.1 Jupiter masses, and a radius of 1.7 ± 0.1 Jupiter radii. This radius is difficult to reconcile with standard models: a cool, massive giant planet with an estimated equilibrium temperature of 270 K and an age of approximately 1.2 billion years should have a radius of about 1.0–1.1 Jupiter radii. The authors therefore explore whether opaque rings around a smaller planet could provide enough additional occulting area to make the companion appear 60–70% larger than expected. The analysis uses two-minute-cadence TESS observations from Sector 15, covering a single, approximately 21-hour transit on September 3–4, 2019, with a depth of about 1.1%. The authors remove the local baseline trend using a quadratic polynomial fitted to out-of-transit data, then compare conventional spherical-planet and ringed-planet models using Markov chain Monte Carlo sampling. Because a single transit cannot establish the orbital period or eccentricity, both models assume a 1,030-day period and a circular orbit. The spherical-planet fit reproduces the earlier results, yielding a planet-to-star radius ratio of 0.1090, an impact parameter of 0.77, and a companion radius of approximately 1.74 Jupiter radii. For the ring calculations, the authors extend the JoJo transit code to calculate the light blocked by a planet and a projected elliptical annulus across a limb-darkened stellar disk. They report that the ring module is more than 20 times faster than PYPPLUSS at comparable precision. To limit model flexibility, they fix the planet’s radius at 1.1 Jupiter radii, assume fully opaque rings, and test inner ring edges at either 1.0 or 1.1 planetary radii. They assess physical plausibility using the Roche limit, within which tidal forces inhibit ring particles from assembling into satellites. Both ring models fit the observations acceptably. Their inferred outer ring radii range from approximately 3.1 to 4.4 planetary radii, and their projected shapes are strongly flattened, with flattening parameters of about 0.82–0.89. The projected ring orientations range from approximately 74° to 81°, implying nearly polar configurations if the inferred geometry is correct. Representative true obliquities are about 80° or 100°. The rings would extend nearly to the estimated Roche limit. Compared with the spherical-planet model, the ring models reduce chi-squared by approximately 14 while adding two free parameters. However, the Bayesian information criterion improves by only 0.4–1.3, indicating marginal statistical support and leaving the two interpretations nearly indistinguishable. The authors conclude that rings offer a physically motivated explanation for the radius anomaly, but the results do not constitute a confirmed detection. Several limitations remain. The normal planetary radius is imposed in the ring fits rather than independently measured, and the inferred ring geometry has substantial uncertainties and degeneracies. Much of the fit improvement depends on a feature approximately 0.25 days after mid-transit that could instead reflect a starspot crossing. Excluding this feature reverses the model preference. A rocky debris ring might connect the companion to the dusty environment implicated in the star’s historic irregular dimmings, but this possibility remains speculative. Precise observations of repeat transits, particularly during ingress and egress, could test predicted differences of a few parts in ten thousand. Multiband photometry and future astrometric constraints on the companion’s mass and orbit would provide additional tests.

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