AI summary · arXiv: 2610.35539v1 · astro-ph.SR

An Intermediate Mass Stripped Star in a 4.2-hour Orbit around a Compact Object

Bethany Ludwig, Maria R. Drout, Ylva Götberg, Alexander Laroche, Katie Auchettl, Alejandro Vigna-Gómez, Katelyn Breivik, Cole Johnston,
and 3 more authorsEva Laplace, Vikram S. Dhillon, Hugues Sana
Original paper Submitted to arXiv on 26 Oct. 2026 Submitted to Nature License: NONEXCLUSIVE-DISTRIB 1.0 Also in: fr

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The essentials

DGL-3 is a 4.2-hour stripped-star binary whose unseen companion is most likely a neutron star, and models predict it can form a merging double neutron star.

Question

Can a stripped star immediately preceding the formation of a double neutron star be observed, and what does its companion and future evolution reveal about that pathway? The study characterizes DGL-3, whose unseen companion could otherwise be a main-sequence star, another stripped star, or a compact object.

Method

The authors analyze 38 Magellan/MagE spectra from 2019–2022, continuous ULTRACAM photometry with approximately 20-second exposures, and 14 archival XMM-Newton observations plus two Chandra observations. They derive the orbit and companion-mass constraints from radial velocities and ellipsoidal variability, test for a second stripped star in the spectra, and use MESA to model future binary evolution and gravitational-wave-driven merger.

Findings

  • Result The measured orbit has a period of about 4.2 hours and is consistent with being circular.
    See the passage in the paper
    The preferred fit yields a very short period ($P$) of only $\sim 4.2$ hours and is consistent with a circular orbit ($e<0.045$; 95% credible upper limit), which we adopt for subsequent analyses.
  • Result The minimum companion mass is 1.38 ± 0.25 solar masses, and the light-curve analysis makes a white dwarf companion unlikely.
    See the passage in the paper
    The corresponding companion mass distribution (Fig. 2, b) only has $0.6\%$ of the posterior below the Chandrasekhar limit of $1.4$ M⊙ which makes a WD companion unlikely.
  • Result The orbit rules out a main-sequence companion that massive, while spectral tests find no detectable second stripped star, supporting a compact-object companion.
    See the passage in the paper
    We therefore conclude that the unseen companion to DGL-3 can neither be a MS star, nor another stripped star. The unseen companion must therefore be a compact object.
  • Result In the fiducial evolution model, the stripped star undergoes Case BB mass transfer and a supernova, leaving a bound neutron-star binary that merges after 220 million years.
    See the passage in the paper
    The binary then radiates gravitational waves at such high rates that the NSs merge after only 220 Myr (Fig. 3, Peters (1964)).
  • Authors’ interpretation The predicted merger depends most strongly on assumptions about angular-momentum loss during non-conservative Case BB mass transfer.
    See the passage in the paper
    The largest uncertainty arises during the Case BB mass transfer phase, because of how poorly understood angular momentum loss is during non-conservative mass transfer (Kovacevic et al., 2026, e.g.,).

Limitations

  • The companion is not directly identified as a neutron star; the inference is probabilistic, and the X-ray nondetection does not exclude one.
    See the passage in the paper
    Overall, between our derived companion mass distribution and the current measured masses of Galactic double neutron stars (Chattaraj et al., 2026), a neutron star is the most probable companion.
  • The future evolutionary outcome is sensitive to uncertain angular-momentum loss during mass transfer; a circumbinary disk could instead cause the system to merge before the second supernova.
    See the passage in the paper
    If, for example, such mass transfer forms a circumbinary disk, it could drain angular momentum so efficiently that the stars merge before the second supernova.

Why it matters

The authors present DGL-3 as the first detailed observational benchmark of a critical phase in double-neutron-star formation, previously constrained mainly by theory. They argue that such systems can directly test binary-interaction physics and connect stripped-star evolution to gravitational-wave merger sources.

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: stripped stars binary evolution neutron stars mass transfer gravitational-wave mergers

Read further

  • Comprehensive Summary
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  • Original abstract
The paper investigates whether DGL-3—a hot, hydrogen-poor stripped star in the Small Magellanic Cloud—is paired with a compact object and could be a direct precursor to a merging double neutron star. Such systems represent a poorly observed stage of binary evolution: after a star has lost most of its envelope but before it undergoes core collapse. Measuring their properties can help test how binary interactions produce the tight orbits required for neutron stars to merge. The authors combine 38 optical spectra collected between 2019 and 2022 with high-speed ULTRACAM photometry, archival XMM-Newton observations, and two Chandra observations from 2025. They measure changes in the stripped star’s radial velocity and fit its orbit, using the resulting orbital parameters and an estimate of the star’s mass to constrain the unseen companion. They also model the photometric variations, search the spectra for evidence of a second stripped star, compare X-ray limits with predictions for accretion from the stripped star’s wind, and use stellar and binary-evolution calculations to project the system’s future. The radial velocities indicate a nearly circular orbit with a period of 4.169 hours and a velocity semi-amplitude of 151.4 km/s. The mass function implies a minimum companion mass of about 1.38 solar masses, with a 68% interval of 1.13–1.64 solar masses. A main-sequence star at least this massive would be too large to fit within its Roche lobe. A second stripped star could fit, but simulations indicate that it should have been detectable in the spectra. Since none is found, the authors conclude that the companion is a compact object. The photometry varies by about 2.5%, with two maxima per orbit, consistent with tidal distortion of the stripped star. Modeling this ellipsoidal variation favors a companion mass of 1.58 solar masses. Only 0.6% of the inferred mass distribution lies below the Chandrasekhar limit, making a white dwarf unlikely and a neutron star the most probable interpretation. The 68% highest-density interval is 1.40–2.41 solar masses. Chandra did not detect X-rays, placing a 2–7 keV luminosity limit of 7.8 × 10³² erg/s. A neutron-star wind-accretion estimate is slightly above this limit, but depends strongly on uncertain wind mass-loss rates and speeds. A faster wind, lower mass-loss rate, or suppression of accretion by the neutron star’s magnetic field and rotation could explain the non-detection. In the fiducial evolutionary model, the stripped star expands after about 1.4 million years and transfers mass to its companion for roughly 26,000 years. This phase removes about 1.2 solar masses from the star and shrinks the orbit to 1.9 hours. The star then undergoes a hydrogen-free supernova. Assuming a 1.4-solar-mass neutron-star remnant and no natal kick, the system remains bound, forming a neutron-star pair in a 4.4-hour orbit. The pair merges through gravitational-wave emission in about 220 million years. This forecast is uncertain, particularly because the amount of orbital angular momentum lost during the brief, highly non-conservative mass-transfer phase is poorly constrained. In one tested scenario, a circumbinary disk causes the stars to merge before the supernova. Several other tested assumptions still produce a neutron-star merger, with delays ranging from 160 million to 7.9 billion years. The authors present DGL-3 as a valuable observational benchmark and a likely merger progenitor, while emphasizing the need for better constraints on mass transfer, wind properties, and possible supernova kicks.

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Weekly letter Presented in "Astronomy and space this week" of 2 November 2026. Astronomy and space this week: Hidden worlds, stellar futures and the temperature of uncertainty

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