The Cosmic Metronome Loses Its Beat: Ansky's Flares Slow to Half Tempo ✛

Original: "NICER observations reveal doubled timescales in Ansky's quasi-periodic eruptions (QPEs)"
arXiv:2509.16304 · 2025-09-19 · CC BY 4.0 · 3 min
Over six months, Ansky's quasi-periodic eruptions halved in frequency, doubled in duration, and quadrupled in energy.

At the core of the distant galaxy SDSS J1335+0728, 2.5 billion light-years from Earth, a supermassive black hole beats out a rhythm. Every few days it flares in X-rays like a cosmic metronome, but in 2025 that metronome suddenly shifted from allegro to andante. NICER aboard the ISS, having accumulated 283 kiloseconds of observations, recorded that the interval between flares grew from ~4.5 to ~10 days, and each flare's duration increased from ~1.5 to ~2.8 days. The total radiated energy per flare jumped fourfold, reaching (3.98±0.4)×$10^{48}$ erg. It's as if a musician playing a fast waltz suddenly switched to a slow adagio, keeping the same notes but making each one four times louder.

Ansky is the brightest known QPE source: its peak luminosity reaches 2×$10^{43}$ erg/s, ten times brighter than any other. Yet in 2020–2023 it showed no X-ray emission at all; the flares only began after an optical outburst in 2019.

What makes the metronome falter? Astrophysicists have long debated what governs the QPE rhythm: instabilities in the accretion disk (a rotating gas disk around the black hole) or the orbital motion of a companion star in an extreme-mass-ratio inspiral (EMRI). The 2025 observations provide an unexpected answer: the orbit could not have changed that quickly. The period doubled in six months, yet a star's orbital period changes slowly, driven by gravitational waves. The authors propose an elegant scenario: debris from a disrupted star, passing through the accretion disk, generates shock waves. Previously, these shocks punched through the disk, producing two flares per passage; now they don't, so there's one flare, but twice as long and more energetic. The transition from double-sided to single-sided shocks explains both the period doubling and the energy increase, as well as the profile asymmetry: the decay time doubled, while the rise time barely changed.

Within the 2025 season, the interval between flares is systematically increasing at a rate of ~0.1 days per flare. If the trend continues, the period will stabilize around 10 days, but rapid switches between 5 and 10 days are also possible.

This work is the first observational evidence for the evolution of the emission mechanism in QPEs. Previously, researchers noted the presence of flares or their link to tidal disruption events, but no one had seen the source parameters change in real time. Now theorists have a test: models must explain not only the average parameters but also their rapid changes. If the proposed scenario is correct, numerical simulations of stellar ablation and disk evolution will reproduce the observed energies and profiles. Future observations with NICER and XMM-Newton, already approved, will continue to track the period and shape of the flares. Detecting period doubling in other long-period QPEs would be the "smoking gun" for the collision scenario.

The cosmic metronome keeps ticking, but now we know its rhythm can change not because of an orbital shift, but because of how stellar debris interacts with the gas disk. This discovery challenges old models and opens a new chapter in the study of quasi-periodic eruptions. For future missions like LISA and TianQin, which will detect gravitational waves from EMRI systems, understanding the electromagnetic counterparts of such events will be key to deciphering the invisible dances of black holes and their companions.

Ansky is the brightest known QPE source: its peak luminosity reaches 2×$10^{43}$ erg/s, ten times brighter than any other. Yet in 2020–2023 it showed no X-ray emission at all; the eruptions only began after an optical flare in 2019.

F_{\mathrm{QPE}} = \begin{cases} A\lambda e^{\tau_1/(t_{\mathrm{peak}}-t_{\mathrm{as}}-t)} & t < t_{\mathrm{peak}} \\ A e^{-(t-t_{\mathrm{peak}})/\tau_2} & t \ge t_{\mathrm{peak}} \end{cases}
A is the amplitude, τ1 and τ2 are the exponential rise and decay times, λ is a normalization, and tas is the asymptotic time
R_{\mathrm{bb}} = \sqrt{\frac{L_{\mathrm{bol}}}{4\pi\sigma_{\mathrm{SB}} T^4}}
Rbb is the blackbody radius, Lbol is the bolometric luminosity, T is the temperature, and σSB is the Stefan-Boltzmann constant
Concepts
quasi periodic eruptions black hole activity cycles quasi biennial oscillation changing agn activity quasar feedback blazar flare starburst microquasar active galactic nucleus quasar tidal disruption event black hole outburst