Active galactic nuclei (AGN) are among the brightest persistent sources in the universe. Their energy is born in accretion disks around supermassive black holes. Some of the material is ejected in narrow jets, while some spreads out in broad winds. In X-ray binary systems, where the black hole is only a few times more massive than the Sun, a clear anti-correlation has long been known: when the star launches a jet, the wind dies down, and vice versa. It was natural to expect the same logic to apply unchanged to the giants at the centers of galaxies. But observations say otherwise.
Using high-resolution spectroscopy, the scientists compiled data from the literature on 62 objects of four types: radio-loud FRII quasars, radio-quiet quasars in elliptical galaxies, radio-quiet Seyfert galaxies in spirals, and one jet-dominated narrow-line Seyfert 1. For each, they measured the gas outflow speed (in fractions of the speed of light) and the black hole mass, and for some, the black hole’s spin. Comparison was done using statistical tests: Welch’s t-test and the Mann–Whitney U test.
It turned out that radio-quiet quasars are record-breakers: their winds accelerate to 0,58 the speed of light, with an average of 0,28. In radio-loud quasars, winds are on average weaker—about 0,08, but can be faster, up to 0,28—which is not the case for jet-dominated systems in spirals, where speeds drop to 0,0028. Statistical tests confirmed that radio-quiet and radio-loud populations differ significantly (p ~ 0,004), and radio-quiet quasars and Seyferts in spirals differ even more (p ~ 0,002). Meanwhile, no link was found between wind speed and black hole mass: fast winds occur both in giants of 10 billion solar masses and in dwarfs of 1 million.
This picture doesn’t fit with simply scaling up X-ray binaries. The key to understanding is the direction of rotation of the accretion disk relative to the black hole. If the disk spins the same way (prograde rotation), it gets very close to the horizon, gravitational energy is released with tremendous efficiency (up to 30%), and powerful radiation-driven winds are launched. A jet is suppressed under these conditions. If the disk spins the opposite way (retrograde rotation), it stalls far out—at about 9 gravitational radii—efficiency drops to 5–6%, winds are weaker, and enough magnetic flux remains to power a jet. It is this ‘choice of direction’ that explains why in elliptical galaxies—products of mergers—we sometimes see quasars with simultaneous winds and jets: some galaxies experienced a brief episode of counter-rotation.
Future observatories like Athena and Lynx will enable more detailed study of winds and measure the spins of thousands of active galactic nuclei, while numerical simulations will clarify exactly how magnetic fields are redistributed when the spin direction changes. Objects with borderline spins around 0,7 are especially interesting, where a transition from jet mode to wind mode may occur.
The results will impact our understanding of feedback in galaxy formation: winds and jets heat and expel gas in different ways, regulating star formation.
The sample of objects with reliable spin and wind speed measurements must be enlarged, especially for borderline spins.
The work is directly related to the fundamental problem of the ‘unification of active nuclei’—why, with similar masses and luminosities, some galaxies launch jets and others do not.
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What the work does
The study compares wind speeds and the presence of jets in 62 active galactic nuclei of different types. Using statistical tests, it shows that radio-quiet quasars host the fastest winds, while no correlation with black hole mass is found. The authors propose an explanation based on direct or retrograde accretion disk rotation, which regulates accretion efficiency and jet launching.
Where its strength is
The strength of the work lies in combining observational data on winds and jets across different AGN classes and in the physically intuitive idea about the role of disk rotation direction. This provides a simple mechanism linking accretion geometry to the observed manifestations of nuclear activity.
Where it could go next
Worth trying
Nearby works in our archive
The closest work in the archive sits at 0.65 by meaning — the usual level for our corpus.
as written by the authors arXiv:2607.22418v1
The well-established anti-correlation between disk winds and relativistic jets in X-ray binaries is often interpreted in a scale-invariant black hole accretion context. If so, active galactic nuclei (AGN) should exhibit a direct mass-scaled analog. We test this prediction across FRII radio quasars, radio-quiet quasars, and jetted and non-jetted Narrow Line Seyfert 1 galaxies (NLS1) in spirals, among others. They exclude simple scale invariance. The highest-velocity winds occur exclusively in radio-quiet quasars, while powerful FRII quasars host systematically weaker winds despite equally large black hole masses. Jetted NLS1s show strong wind suppression consistent with X-ray binary behavior, whereas FRII quasars occupy a distinct regime in which jets and winds coexist. Black hole mass and spin magnitude alone cannot account for this dichotomy. We argue that the angular momentum direction of the disk relative to that of the black hole (aligned versus anti-aligned or co-rotation versus counter-rotation) is the critical parameter: secularly fueled spiral systems and most post-merger systems favor co-rotation, which is associated with compact ISCO radii, high radiative efficiency, strong winds, and jet suppression, while the counter-rotating subset of merger-influenced ellipticals can sustain powerful jets alongside moderate winds. Moreover, while spiral AGN and merger-driven radio-quiet quasars experience similar strong jet/wind anti-correlation, they cannot be treated as strict scaled analogs of X-ray binaries, which undergo rapid state transitions involving magnetic flux redistribution absent in AGN. At least two distinct wind-jet regimes therefore operate across the mass scale. We identify the details of this behavior across AGN subclasses.
The fastest known wind — from quasar SDSS J1029+2623—travels at 0,58c, covering the distance from Earth to the Moon in two seconds.