MeerKAT discovers a jet-driven bow shock near GRS 1915+105. How an invisible large-scale jet sculpts a microquasar's environment

(2025)

Authors:

SE Motta, P Atri, James H Matthews, Jakob van den Eijnden, Rob P Fender, James CA Miller-Jones, Ian Heywood, Patrick Woudt

Quantifying jet-interstellar medium interactions in Cyg X-1: Insights from dual-frequency bow shock detection with MeerKAT

(2025)

Authors:

P Atri, SE Motta, Jakob van den Eijnden, James H Matthews, James CA Miller-Jones, Rob Fender, David Williams-Baldwin, Ian Heywood, Patrick Woudt

Measurement of the power spectrum turnover scale from the cross-correlation between CMB lensing and Quaia

The Open Journal of Astrophysics Maynooth University 8 (2025)

Authors:

David Alonso, Oleksandr Hetmantsev, Giulio Fabbian, Anze Slosar, Kate Storey-Fisher

Abstract:

<jats:p>We use the projected clustering of quasars in the Gaia-unWISE quasar catalog, Quaia, and its cross-correlation with CMB lensing data from Planck, to measure the large-scale turnover of the matter power spectrum, associated with the size of the horizon at the epoch of matter-radiation equality. The turnover is detected with a significance of between <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mn>2.3</mml:mn></mml:math> and <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mn>3.1</mml:mn><mml:mi>σ</mml:mi></mml:mrow></mml:math>, depending on the method used to quantify it. From this measurement, the equality scale is determined at the <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn>20</mml:mn><mml:mi>%</mml:mi></mml:mrow></mml:math> level. Using the turnover scale as a standard ruler alone (suppressing information from the large-scale curvature of the power spectrum), in combination with supernova data through an inverse distance ladder approach, we measure the current expansion rate to be . The addition of information coming from the power spectrum curvature approximately halves the standard ruler uncertainty. Our measurement in combination with calibrated supernovae from Pantheon <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mo>+</mml:mo></mml:math> and SH0ES constrains the CMB temperature to be , independently of CMB data. Alternatively, assuming the value of from COBE-FIRAS, we can constrain the effective number of relativistic species in the early Universe to be .</jats:p>

Jets from a stellar-mass black hole are as relativistic as those from supermassive black holes

(2025)

Authors:

Xian Zhang, Wenfei Yu, Francesco Carotenuto, Rob Fender, Sara Motta, Arash Bahramian, James CA Miller-Jones, Thomas D Russell, Stephane Corbel, Patrick A Woudt, Pikky Atri, Christian Knigge, Gregory R Sivakoff, Andrew K Hughes, Jakob van den Eijnden, James Matthews, Maria C Baglio, Payaswini Saikia

Blast waves and reverse shocks: from ultra-relativistic GRBs to moderately relativistic X-ray binaries

Monthly Notices of the Royal Astronomical Society Oxford University Press 539:3 (2025) 2665-2684

Authors:

James H Matthews, Alex J Cooper, Lauren Rhodes, Katherine Savard, Rob Fender, Francesco Carotenuto, Fraser J Cowie, Emma L Elley, Joe Bright, Andrew K Hughes, Sara E Motta

Abstract:

Blast wave models are commonly used to model relativistic outflows from ultra-relativistic gamma-ray bursts (GRBs), but are also applied to lower Lorentz factor ejections from X-ray binaries (XRBs). Here, we revisit the physics of blast waves and reverse shocks in these systems and explore the similarities and differences between the ultra-relativistic () and moderately relativistic () regimes. We first demonstrate that the evolution of the blast wave radius as a function of the observer frame time is recovered in the on-axis ultra-relativistic limit from a general energy and radius blast wave evolution, emphasizing that XRB ejections are off-axis, moderately relativistic cousins of GRB afterglows. We show that, for fixed blast wave or ejecta energy, reverse shocks cross the ejecta much later (earlier) on in the evolution for less (more) relativistic systems, and find that reverse shocks are much longer lived in XRBs and off-axis GRBs compared to on-axis GRBs. Reverse shock crossing should thus typically finish after 10–100 of days (in the observer frame) in XRB ejections. This characteristic, together with their moderate Lorentz factors and resolvable core separations, makes XRB ejections unique laboratories for shock and particle acceleration physics. We discuss the impact of geometry and lateral spreading on our results, explore how to distinguish between different shock components, and comment on the implications for GRB and XRB environments. Additionally, we argue that identification of reverse shock signatures in XRBs could provide an independent constraint on the ejecta Lorentz factor.