Searcharxiv⌕ Search

arXiv · 2610.28034

Rapid Variability of Radiative Signatures from Driven Relativistic Reconnection

Abstract

Rapid variability in energetic flares is a distinctive feature of high-energy emission from many magnetically dominated astrophysical sources. We investigate the radiative variability of driven relativistic magnetic reconnection using Particle-in-Cell simulations of strongly magnetized flux tubes pushed to merge at driving speed $v_{\rm push}$. This setup captures the onset of reconnection and provides a controlled model for single reconnection-driven flares near compact objects, where magnetic structures can be twisted, sheared, and forced to merge by turbulent accretion flows or relativistic frame dragging. We find that the merger efficiently accelerates particles into nonthermal distributions, producing synchrotron emission whose variability tracks the reconnection phases. We identify two regimes: a quasi-steady, weakly driven regime for $v_{push}\leq0.1\,c$, and strongly driven regime for $v_{\rm push}>0.1\,c$. The transition occurs when the driving exceeds the typical inflow-to-outflow velocity ratio of $\sim0.1$ in steady collisionless relativistic reconnection, i.e., the average rate at which reconnection can process incoming flux, potentially providing an additional source of variability. The lightcurves rise on $1$--$3$ light-crossing times of the reconnecting region, and the particle spectra develop power laws with index $p\simeq1.8$--$2.4$. These timescales are compatible with observed variability in high-energy sources, including the very-high-energy flares of M87$^*$ and the $γ$-ray flares of the Crab Nebula, making this model a viable framework for rapid flaring in active galactic nuclei and pulsar wind nebulae.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

Clarissa Mora, Fabio Bacchini, Camille Granier, Daniel Groselj. 2026-10-20. Rapid Variability of Radiative Signatures from Driven Relativistic Reconnection. https://arxiv.org/abs/2610.28034

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

Causality and perturbative-QCD constraints on first-order phase transitions in neutron stars

Causality bounds the compactness and maximum mass of neutron stars. We generalise this bound to equations of state (EOSs) with a first-order phase transition between maximally stiff phases. In units of the transition energy density, the problem depends only on $q=\ptr/\etr$ and $j=Δ\ve/\etr$. The maximum compactness equals the smooth value $\mathcal{C}=0.354$ for $q\to0$ or $j\to0$, is unaffected for $q\gtrsim0.67$, and is otherwise reduced by typically $\lesssim0.04$ when the maximum-mass star is a hybrid star and by up to $0.13$ when it is the last hadronic star. Matching to a Baym--Pethick--Sutherland crust and a chiral-EFT polytrope at $n_m=1.1\,n_0$ and inverting the bound, no causal EOS supports $2.01\,\Msun$ if the energy-density jump exceeds $\simeq460$--$495~{\rm MeV\,fm^{-3}}$. Additionally, imposing radius constraint of $R\ge11.6$~km it shrinks to $\simeq235$--$395~{\rm MeV\,fm^{-3}}$. These limits hold whatever the matter above the transition, for onsets within $\simeq0.2\,n_0$ of $n_m$. Relaxing maximal stiffness, we build EOSs with a transition at $μ_{\rm tr}=1000$--$1300$~MeV, matched to perturbative QCD (pQCD) at $2.6$~GeV. pQCD limits the jump; EOSs compatible with PSR J0740+6620, J1614$-$2230, J0437$-$4715, J0614$-$3329, GW170817, and XTE J1814-338 appear only at $μ_{\rm tr}=1200$ and $1250$~MeV; and inside the causal window, the largest jump agrees with the bound within the grid resolution. Finally, inserting a transition at $2.01\,\Msun$ into hadronic EOSs that satisfy five pulsar observations, the EOS with the lowest break density gives a narrow stable hybrid window ($ΔM\simeq0.005\,\Msun$), compatible with XTE J1814-338 for jumps of $6$--$8\,n_0$ and with pQCD; three EOSs with higher break densities give none.

astro-ph.HE↗

The Life and Death of Stars That Capture Primordial Black Holes

Primordial black holes (PBHs) in the asteroid mass window ($10^{17}-10^{23}\,{\rm g}$) remain viable dark matter candidates and can be captured by stars. We develop the first global framework for the evolution of stars that capture PBHs, combining analytic calculations, stellar evolution models, 3D general-relativistic magnetohydrodynamic simulations, and Monte Carlo population synthesis. We find that the fate of these systems bifurcates: PBHs that form an accretion disk before consuming the host drive explosive disruption, whereas PBHs captured too late or growing too slowly consume the star quietly. Capture is dominated by three-body interactions with planetary or stellar companions. For a solar-type host with a Jupiter analog, inspiral within a main-sequence lifetime requires $M_{\rm BH}^{\rm crit}\gtrsim 10^{22}\,{\rm g}$, while lighter PBHs generally require tighter companions. Once deposited at the center, the PBH grows through inefficient quasi-spherical Bondi accretion; if it reaches the angular-momentum threshold before consuming the host, the inflow circularizes into a disk. Our Monte Carlo calculations yield sizable quiet-consumption and explosive-disruption populations, with final PBH masses $M_{\rm BH}\sim0.01-1\,M_\odot$ and disk-forming PBH spins $a_\ast\approx0.8$. Disk formation is the point of no return: disk winds and relativistic jets of $\sim10^{45}-10^{50}\,{\rm erg\,s^{-1}}$ disrupt the star within minutes. The resulting transients may include a $\sim$day-long UV/blue signal, radio afterglow, and, if the jet escapes, an X-ray-flash/low-luminosity gamma-ray-burst (XRF/llGRB) signal. For an $O(1)$ PBH dark matter fraction and optimistic capture assumptions, the event rate can reach that of llGRBs. The low-mass, high-spin remnants offer a complementary PBH probe and possible source for subsolar BH mergers.

astro-ph.HE↗

A New Scaling of Neutron Star Tidal Deformability for Directly Probing the Central Equation of State Parameter

The dimensionless tidal deformability, $Λ$, of neutron stars (NSs), inferred from gravitational-wave (GW) observations, has thus far been used primarily to constrain the pressure of dense matter near twice nuclear saturation density, leaving the core equation of state (EOS) largely inaccessible to inspiral-phase GW observations. We show that a fundamental central EOS parameter can be probed directly through $Λ$ using a perturbative analysis of the dimensionless stellar-structure and tidal-response equations formulated in terms of scaled intrinsic variables, without invoking any specific EOS model. We uncover a remarkable EOS-insensitive scaling relation between $Λ$ and the central EOS parameter $\rm{X}\equiv P_{\rm c}/\varepsilon_{\rm c}$, where $P_{\rm c}$ and $\varepsilon_{\rm c}$ denote the central pressure and energy density, respectively. The relation is validated against a broad ensemble of physically viable EOSs. Applying it to tidal deformabilities inferred from events such as GW170817 enables a direct determination of $\rm{X}$. By adopting the previously established effective upper bound $\rm{X}\lesssim0.381$, we infer a tight lower bound, $Λ_{\rm{TOV}}\gtrsim9.1^{+0.5}_{-0.5}$, for maximum-mass NSs along stable mass-radius sequences, quantitatively demonstrating that even the most compact stable NSs remain distinctly separated from black holes, for which $Λ_{\rm{BH}}=0$. These findings reveal a previously unrecognized connection between inspiral-phase tidal deformability and the central EOS parameter $\rm{X}$, establishing a direct link between GW observables and the microphysics of ultradense matter in the strong-gravity regime. The resulting scaling establishes inspiral-phase tidal deformability as a direct and largely model-insensitive probe of the central EOS parameter $\rm{X}$, and hence of key properties of NS cores.

astro-ph.HE↗