A concordance picture of FRB 121102 as a flaring magnetar embedded in a magnetized ion-electron wind nebula

TL;DR

This paper presents a model of FRB 121102 as a young magnetar embedded in a magnetized nebula, explaining its quiescent radio emission and rotation measure evolution with few constrained parameters.

Contribution

It introduces a time-dependent one-zone model linking the nebula's properties to the magnetar's activity, providing a comprehensive explanation for observed features of FRB 121102.

Findings

The nebula's energy matches that of a millisecond magnetar.

The predicted source age is 10-40 years, consistent with observations.

Secular decay of RM and flux follows specific power laws.

Abstract

The fast radio burst FRB 121102 has repeated multiple times, enabling the identification of its host galaxy and of a spatially-coincident, compact, steady (`quiescent') radio synchrotron source. It was proposed that FRB 121102 is powered by a young flaring magnetar, embedded within a decades-old supernova remnant. Using a time-dependent one-zone model, we show that a single expanding magnetized electron-ion nebula (powered by the same outbursts likely responsible for the FRBs) can explain all the basic properties of the quiescent source (size, flux, self-absorption constraints) and the large but decreasing rotation measure (RM) of the bursts. The quiescent emission is powered by relativistic thermal electrons heated at the termination shock of the magnetar wind, while the RM originates from non-relativistic electrons injected earlier in the nebula's evolution and cooled through expansion and radiative losses. The model contains few free parameters, which are tightly constrained by observations: the total energy injected into the nebula over its history, $\sim 10^{50}-10^{51}$ erg, agrees with the magnetic energy of a millisecond magnetar; the baryon loading of the magnetar outflow (driven by intermittent flares) is close to the neutron star escape speed; the predicted source age $\sim 10-40$ years is consistent with other constraints on the nebula size. For an energy input rate $\dot{E} \propto t^{-\alpha}$ following the onset of magnetar activity, we predict secular decay of the RM and quiescent source flux, which approximately follow ${\rm RM} \propto t^{-(6+\alpha)/2}$ and $F_{\nu} \propto t^{-(\alpha^2+7\alpha-2)/4}$, respectively.