Opacity Build-up in Impulsive Relativistic Sources

TL;DR

This paper models the time-dependent opacity to pair production in impulsive relativistic sources like GRBs, revealing how spectra evolve and photons escape during transient emission episodes.

Contribution

It introduces a semi-analytic model for the time and energy dependence of optical depth in impulsive relativistic sources, extending previous steady-state analyses.

Findings

Time integrated spectra develop a power-law tail above a certain photon energy.

High-energy photons escape mainly at the onset of emission episodes.

Spectral cutoff behavior varies with source duration and state.

Abstract

Opacity effects in relativistic sources of high-energy gamma-rays, such as gamma-ray bursts (GRBs) or Blazars, can probe the Lorentz factor of the outflow and the distance of the emission site from the source, and thus help constrain the composition of the outflow (protons, pairs, magnetic field) and the emission mechanism. Most previous works consider the opacity in steady state. Here we study time dependent effects of the opacity to pair production ($\gamma\gamma \to e^+e^-$) in impulsive relativistic sources. We present a simple, yet rich, semi-analytic model for the time and energy dependence of the optical depth, $\tau$, where an ultra-relativistic thin spherical shell emits isotropically in its own rest frame over a finite range of radii, $R_0 < R < R_0 + \Delta R$. This is very relevant for GRB internal shocks. We find that in an impulsive source ($\Delta R <~ R_0$), while the instantaneous spectrum has an exponential cutoff above the photon energy $\epsilon_1(T)$ where $\tau = 1$, the time integrated spectrum has a power-law high-energy tail above a photon energy $\epsilon_{1*} \sim \epsilon_1(\Delta T)$ where $\Delta T$ is the duration of the emission episode. Furthermore, photons with $\epsilon > \epsilon_{1*}$ will arrive mainly near the onset of the spike or flare from to the short emission episode, as in impulsive sources it takes time to build-up the (target) photon field, and thus $\tau(\epsilon)$ initially increases with time and $\epsilon_1(T)$ decreases with time, so that photons of energy $\epsilon > \epsilon_{1*}$ are able to escape the source mainly very early on while $\epsilon_1(T) > \epsilon$. As the source approaches a quasi-steady state ($\Delta R >> R_0$), the time integrated spectrum develops an exponential cutoff, while the power-law tail becomes increasingly suppressed.