The Double-Burst Nature and Early Afterglow Evolution of Long GRB 110801A

TL;DR

This paper analyzes the complex temporal and spectral features of long GRB 110801A, revealing a double-burst structure, chromatic afterglow evolution, and constraining key physical parameters through broadband modeling.

Contribution

It provides a detailed multi-component spectral and temporal analysis of GRB 110801A, highlighting the double-burst nature and early afterglow evolution with physical parameter constraints.

Findings

The gamma-ray emission shows a distinct double-episode structure.

Optical and X-ray afterglow behaviors suggest different physical origins.

A two-component spectral model fits the data better than single-component models.

Abstract

We present a comprehensive temporal and spectral analysis of the long-duration gamma-ray burst GRB 110801A, utilizing multi-band data from the Neil Gehrels Swift Observatory and ground-based telescopes. The $\gamma$-ray emission exhibits a distinct two-episode (``double-burst'') structure. Rapid follow-up observations in the optical and X-ray bands provide full coverage of the second burst. The optical light curve begins to rise approximately 135 s after the trigger, significantly preceding the second emission episode observed in X-rays and $\gamma$-rays at $\sim 320$ s. This chromatic behavior suggests different physical origins for the optical and high-energy emissions. Joint broadband spectral fitting (optical to $\gamma$-rays) during the second episode reveals that a two-component model, consisting of a power-law plus a Band function, provides a superior fit compared to single-component models. We interpret the power-law component as the afterglow of the first burst (dominating the optical band), while the Band component is attributed to the prompt emission of the second burst (dominating the high-energy bands). A physical synchrotron model is also found to be a viable candidate to explain the high-energy emission. Regarding the afterglow, the early optical light curve displays a sharp transition from a rise of $\sim t^{2.5}$ to $\sim t^{6.5}$, which is well-explained by a scenario involving both reverse shock (RS) and forward shock (FS) components. We constrain the key physical parameters of the burst, deriving an initial Lorentz factor $\Gamma_0 \sim 60$, a jet half-opening angle $\theta_j \sim 0.09$, and an isotropic kinetic energy $E_{\rm k,iso} \sim 10^{54.8}$ erg.