Detection of an Extremely Luminous Radio Counterpart to the Be/X-ray Binary A0538-66

(2026)

Authors:

Justine Crook-Mansour, Rob Fender, Alex Andersson, Hao Qiu, Andrew K Hughes, Jakob van den Eijnden, Fraser J Cowie, Sara Motta, Itumeleng Monageng, Lorenzo Ducci, Sandro Mereghetti, Andries Mathiba, Dougal Dobie, Tara Murphy, David L Kaplan, Francesco Carotenuto, Phil Charles

Tomographic constraints on the high-energy cosmic neutrino emission rate

(2026)

Authors:

Alberto Gálvez Ureña, Federico Urban, David Alonso

Bars in low-density environments rotate faster than bars in dense regions

Monthly Notices of the Royal Astronomical Society Oxford University Press (OUP) (2026) stag175

Authors:

Natalia Puczek, Tobias Géron, Rebecca J Smethurst, Chris J Lintott

Abstract:

Abstract Does the environment of a galaxy directly influence the kinematics of its bar? We present observational evidence that bars in high-density environments exhibit significantly slower rotation rates than bars in low-density environments. Galactic bars are central, extended structures composed of stars, dust and gas, present in approximately 30 to 70 per cent of luminous spiral galaxies in the local Universe. Recent simulation studies have suggested that the environment can influence the bar rotation rate, $\mathcal {R}$, which is used to classify bars as either fast ($1\le \mathcal {R}\le 1.4$) or slow ($\mathcal {R}>1.4$). We use estimates of $\mathcal {R}$ obtained with the Tremaine–Weinberg method applied to Integral Field Unit spectroscopy from MaNGA and CALIFA. After cross-matching these with the projected neighbour density, log Σ, we retain 286 galaxies. The analysis reveals that bars in high-density environments are significantly slower (median $\mathcal {R} = 1.65^{+0.13}_{-0.11}$) compared to bars in low-density environments (median $\mathcal {R} =1.39^{+0.09}_{-0.08}$); Anderson–Darling p-value of pAD = 0.002 (3.1 σ). This study marks the first empirical test of the hypothesis that fast bars are formed by global instabilities in isolated galaxies, while slow bars are triggered by tidal interactions in dense environments, in agreement with predictions from numerous N-body simulations. Future studies would benefit from a larger sample of galaxies with reliable Integral Field Unit data, required to measure bar rotation rates. Specifically, more data are necessary to study the environmental influence on bar formation within dense settings (i.e. groups, clusters and filaments).

Improving constraints on primordial non-Gaussianity from Quaia with a new cosmological observable: angular redshift fluctuations

(2026)

Authors:

José Ramón Bermejo-Climent, Carlos Hernández-Monteagudo, Alba Crespo-Pérez, Jorge Martin Camalich, David Alonso, Giulio Fabbian, Kate Storey-Fisher

Dynamic shocks powered by a wide, relativistic, super-Eddington outflow launched by an accreting neutron star in the mid-20th century

Monthly Notices of the Royal Astronomical Society Oxford University Press (OUP) (2026) stag163

Authors:

FJ Cowie, RP Fender, I Heywood, F Carotenuto, JH Matthews, B Reville, L Olivera-Nieto, AJ Cooper, AK Hughes, K Savard, PA Woudt, J van den Eijnden, N Grollimund, P Saikia

Abstract:

Abstract Accreting systems can launch powerful outflows which interact with the surrounding medium. We combine new radio observations of the accreting neutron star X-ray binary (XRB) Circinus X-1 (Cir X-1) with archival radio observations going back 24 years. The ∼3 pc scale wide-angle radio and X-ray emitting caps found around Cir X-1 are identified as synchrotron emitting shocks with significant proper motion and morphological evolution on decade timescales. Proper motion measurements of the shocks reveal they are mildly relativistic and decelerating, with apparent velocity of 0.14c ± 0.03c at a propagation distance of 2 pc. We demonstrate that these shocks are likely powered by a hidden relativistic (≳ 0.3c) wide-angle conical outflow launched in 1972 ± 3, in stark contrast to known structures around other XRBs formed by collimated jets over 1000s of years. The minimum time-averaged power of the outflow required to produce the observed synchrotron emission is ∼0.1LEdd, while the time-averaged power required for the kinetic energy of the shocks is $\sim 40 \left(\frac{n}{10^{-2} \textrm{cm}^{-3}}\right)L_\textrm{Edd}$, where n is the average ambient medium number density. This reveals the outflow powering the shocks is likely significantly super-Eddington. We measure significant linear polarisation up to 52 ± 6% in the shocks demonstrating the presence of an ordered magnetic field of strength ∼200 μG. We show that the shocks are potential PeVatrons, capable of accelerating electrons to ∼0.7 PeV and protons to ∼20 PeV, and we estimate the injection and energetic efficiencies of electron acceleration in the shocks. Finally, we predict that next generation gamma-ray facilities may be able to detect hadronic signatures from the shocks.