Time-resolved spectral fits of single-peaked gamma-ray bursts (GRBs) with a physically computed synchrotron model show that about 95% of the time-resolved Fermi/GBM spectra of such single-peaked bursts can be described by synchrotron radiation from electrons that are often not fully cooled ('cool synchrotron'), with a soft electron injection index p≈3.5p\approx3.5 and a mix of cooling regimes (Burgess et al. 2020). This interpretation survives later consistency checks but leaves its cause unidentified: no known dissipation and particle-acceleration process in the moderately magnetized, ultra-relativistic outflow has been shown, analytically or in kinetic (particle-in-cell) simulations, to simultaneously produce the soft injection index, the observed incomplete cooling (effective reheating), and the radiative efficiency needed to power the observed luminosities without violating opacity and deceleration-radius constraints.

Background

Gamma-ray bursts (GRBs) are flashes of 104210^{42}–104710^{47} J of gamma radiation marking the collapse of massive stars or compact-object mergers; the flash itself, lasting milliseconds to minutes, is called the prompt emission. Its physical origin has been debated for fifty years. The observed prompt spectrum is usually described by the empirical Band function, a smoothly broken power law; its low-energy photon index α\alpha long argued against synchrotron emission — the radiation of relativistic electrons spiraling in magnetic fields — because elementary synchrotron theory forbids photon indices above the 'line of death' α=−2/3\alpha=-2/3, while many observed spectra appeared harder. Synchrotron models come in two cooling regimes: in fast cooling, electrons radiate away their energy almost immediately and the photon index below the spectral peak is fixed near −3/2-3/2; in slow or partial cooling, electrons retain energy, giving α=−(p−1)/2\alpha=-(p-1)/2, where pp is the index of the injected electron energy distribution ne(γ)∝γ−pn_e(\gamma)\propto\gamma^{-p}. Standard diffusive shock acceleration in relativistic shocks predicts p≈2.2p\approx2.2, and shocks are inefficient at dissipation, so they require complete (fast) cooling. The magnetization σ\sigma (ratio of magnetic to particle energy flux) measures how magnetically dominated the outflow is; Burgess et al. (2020) reparameterize the problem in terms of the fractional magnetization ξB=UB/Ue\xi_B = U_B/U_e, the ratio of the magnetic energy density UB=B2/(8π)U_B=B^2/(8\pi) to the energy density UeU_e in the heated electrons, scanning ξB\xi_B from 10−210^{-2} to 11 and finding the fits favor ξB∼1\xi_B\sim1, i.e. moderate magnetization; in strongly magnetized jets the dissipation must instead come from plasma processes such as magnetic reconnection or turbulence, possibly with internal mini-jets moving with Lorentz factor Γem\Gamma_{\rm em} relative to the flow. Particle-in-cell (PIC) simulations — kinetic plasma simulations resolving electron scales — are the standard tool for computing the electron index pp that a given acceleration process actually produces; second-order Fermi acceleration is stochastic reheating by plasma turbulence. Burgess et al. (2020, Nature Astronomy 4, 174; preprint arXiv:1810.06965) fitted proper (non-empirical), time-dependent synchrotron spectra to time-resolved Fermi Gamma-ray Burst Monitor (GBM) data of single-peaked GRBs, letting the electron distribution cool during the observation interval. They found synchrotron fits ~95% of time-resolved spectra, so the line-of-death argument had been misleading; but the electrons are injected with a very soft p≈3.5p\approx3.5 (versus the shock prediction 2.24), many spectra are not fast-cooling, and the implied energetics are challenging: reconciling the absence of a photospheric component with the pair-opacity constraint (transparency of the outflow to photon–photon pair production, which sets a lower limit on the bulk Lorentz factor) requires a magnetized jet with ξB∼1\xi_B\sim1 and mini-jet Γem>10\Gamma_{\rm em}>10 emitting at large radii that still lie below the deceleration radius, where the jet begins to slow down by sweeping up the surrounding medium, and the high observed luminosities are hard to reach when electrons are not fully cooled. The model also fixed the injection Lorentz factor γinj=105\gamma_{\rm inj}=10^{5} (leaving all scales degenerate), assumed a single pulse and a single dissipation episode, and neglected particle escape, inverse-Compton and adiabatic cooling, geometry, and the evolution of the magnetic field BB.

Problem Statement

Identify a physically plausible dissipation and particle-acceleration process operating in the moderately magnetized (ξB∼1\xi_B\sim1 up to high magnetization σ\sigma) ultra-relativistic outflow of gamma-ray bursts, and demonstrate quantitatively — through analytic theory or kinetic (PIC) simulations in the magnetization regime inferred for the emitting region — that it simultaneously reproduces what the cool-synchrotron spectral fits of Burgess et al. (2020) of time-resolved Fermi/GBM spectra of single-peaked bursts infer: (1) a soft electron injection index p≈3.5p\approx3.5, markedly softer than the canonical relativistic-shock value p≈2.2p\approx2.2; (2) the observed mix of cooling regimes, i.e. many time-resolved spectra showing incomplete cooling or effective reheating rather than universal fast cooling; and (3) radiatively efficient, energetically self-consistent emission — a combination of electron energy fraction εe\varepsilon_e, re-acceleration, emitting-region Lorentz factor Γem\Gamma_{\rm em}, and magnetization ξB\xi_B that yields the observed luminosities without violating pair-opacity limits (transparency to photon–photon pair production, which bounds the bulk Lorentz factor from below) or the deceleration-radius constraint (the emission radius must remain below the radius at which the jet begins to decelerate as it sweeps up the surrounding medium).

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