AI summary · arXiv: 2611.12504v1 · astro-ph.EP

ALMA detection of continuum emission from GQ Lup B

Pietro Pirola, Stefano Facchini, Gabriele Cugno, Myriam Benisty, Tomas Stolker, Jaehan Bae, Ruobing Dong, Brendan P. Bowler,
and 4 more authorsYa-Lin Wu, Richard Teague, Pietro Curone, Felipe Alarcon
Original paper Submitted to arXiv on 09 Nov. 2026 12 pages, 11 figures, 2 tables including appendices. Accepted for publication in A&A License: CC BY 4.0

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The essentials

ALMA detects unresolved 0.89 mm emission at GQ Lup B, consistent with a compact dusty companion disk, but its emission mechanism and disk properties remain uncertain.

Question

Does GQ Lup B emit millimeter continuum that can be associated with a disk around the companion? What constraints does this detection provide on the disk’s size, dust mass, and relationship to the companion’s accretion?

Method

The authors combined ALMA Band 7 observations from two programs, comprising 16 execution blocks across 13 nights and five baseline setups, and applied self-calibration and visibility alignment before imaging. They tested the detection across imaging weightings and cleaning thresholds, then modeled the measured 0.89 mm emission under optically thin and optically thick assumptions to estimate dust mass and emitting radius.

Findings

  • Result The authors report a 5.8σ point-source detection at the companion’s location, with peak intensity 54.5 ± 9.4 μJy beam−1.
    See the passage in the paper
    The most significant detection ($5.8\sigma$) is obtained with robust = 2, with a peak intensity of $54.5\,\mu\rm Jy\,beam^{-1}$ and a 9.4 $\mu\rm Jy\,beam^{-1}$ rms calculated in the same emission-free annulus described in the previous section.
  • Result The emission is unresolved, giving an upper limit of 2.3 au on the dust emission radius.
    See the passage in the paper
    Therefore we adopt $\sim 2.3$ au as a conservative upper limit on the outer radius of the dust component of the disk.
  • Result Under the optically thin dust-emission assumption, the inferred dust mass is 0.0032 Earth masses.
    See the passage in the paper
    We find a mass of 0.0032 $M_{\oplus}$, less than half of and a quarter of the analog estimates we obtain for PDS 70 c and SR 12 c (0.006 and 0.012 $M_{\oplus}$), respectively.
  • Result Under the optically thick model, the flux corresponds to a smaller emitting radius of 0.20 au; the authors caution this may be a lower limit.
    See the passage in the paper
    We obtain an outer radius of 0.20 au (418 RJup), smaller than SR 12 c (0.34 au) and PDS 70 c (0.38 au, setting $\phi=1^{\circ}$).
  • Authors’ interpretation The short inferred depletion timescale may be reconciled with ongoing accretion if the companion’s orbit replenishes its gas reservoir by crossing the primary disk.
    See the passage in the paper
    This periodic interaction could continuously replenish the gas reservoir of the disk of GQ Lup B, naturally explaining the observed high accretion rate due to an increased inflow of material.

Limitations

  • A single-band measurement cannot distinguish thermal dust emission from other possible mechanisms, including free-free emission from accretion shocks.
    See the passage in the paper
    Only a multi-band characterization and thorough radiative transfer modeling can distinguish between different scenarios.
  • The disk’s exact mass and radius are not determined by the unresolved single-band detection and depend on modeling assumptions.
    See the passage in the paper
    To carry out our analysis, we had to make use of several assumptions (dust opacity, gas mass, inclination, radial extent, temperature), which often have no direct observational measurement.
  • The depletion-time interpretation is uncertain because the accretion rate may vary and depends on the extinction correction.
    See the passage in the paper
    First, the inferred $\dot{M}$ depends on the correction adopted for the extinction ($A_{V}\sim 2.3$ mag); previous work adopting lower estimates (Wu et al. 2015), inferred an accretion rate lower by an order of magnitude.

Why it matters

The detection adds a third millimeter-continuum detection of a gravitationally bound planetary-mass object and provides a benchmark for the sensitivity needed to find such faint disks. The authors argue that a larger sample and multiwavelength observations are needed to determine whether disks around substellar companions resemble scaled-down circumstellar disks or involve additional physical processes.

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: GQ Lup B; protoplanetary disks; ALMA; millimeter continuum; accretion

Read further

  • Comprehensive Summary
  • Layman's Summary
  • Blog article
  • Original abstract
The paper reports an ALMA search for millimeter continuum emission from GQ Lup B, a young, massive companion orbiting the T Tauri star GQ Lup A at a projected distance of about 110 astronomical units. Earlier infrared observations suggested that GQ Lup B has a dusty disk, but previous millimeter observations did not detect it. Millimeter emission can probe cooler dust and help constrain a disk’s material and extent. The authors investigate whether this emission can now be detected and what the observations reveal about the companion’s disk and accretion. The study combines ALMA Band 7 observations at approximately 0.89 millimeters from two observing programs conducted between July 2024 and June 2025. The data cover several baseline configurations, including observations with the Atacama Compact Array and the 12-meter array. The team calibrated and aligned the datasets, then applied self-calibration to improve image quality and sensitivity. They produced images using different weighting choices and tested whether the faint source might be an imaging artifact or contamination from the bright disk around the primary star. The authors detect a point-like source at GQ Lup B’s position, with a peak intensity of 54.5 ± 9.4 microjanskys per beam and a nominal significance of 5.8 sigma. The source is about 0.02 arcseconds from the companion’s position measured by GRAVITY astrometry. Its peak brightness is consistent across images with different angular resolutions, and tests of the residual images support the conclusion that it is not simply a sidelobe from the primary disk. The detection also lies near the position of the companion’s infrared emission. The authors therefore interpret it as emission associated with a disk around GQ Lup B, most likely thermal radiation from dust grains. The emission remains unresolved, even with the finest useful synthesized beam, approximately 29 by 25 milliarcseconds. At the system’s distance of 154.1 parsecs, this corresponds to an upper limit of about 2.3 astronomical units for the dust-emitting radius. Assuming optically thin dust emission, a mean dust temperature of about 56 kelvin, and an opacity appropriate for millimeter-sized grains, the authors estimate a dust mass of 0.0032 Earth masses. In a separate optically thick model, the observed flux is consistent with a much smaller emitting radius of about 0.20 astronomical units. These are conditional estimates, not direct measurements of the disk’s actual size or mass. The authors also compare the inferred disk reservoir with GQ Lup B’s reported accretion rate of about 10 to the minus 9.5 solar masses per year. Assuming a gas-to-dust mass ratio of 100 and a constant accretion rate, they estimate a depletion time of roughly 10,000 years—far shorter than the system’s estimated age of 3–5 million years. They suggest that the companion’s highly inclined orbit, which crosses the primary’s gas disk about twice during each roughly 1,000-year orbit, could replenish its gas reservoir. This explanation is plausible but is not demonstrated by the continuum measurement. The conclusions are limited by the single millimeter-frequency measurement and the source’s unresolved appearance. The inferred mass and radius depend on assumptions about temperature, dust opacity, optical depth, disk geometry, and the gas-to-dust ratio. The authors also cannot rule out a contribution from free-free emission associated with accretion shocks. Observations at multiple millimeter wavelengths and more complete radiative-transfer modeling are needed to distinguish emission mechanisms and better constrain the disk’s properties.

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