eROSITA X-ray Analysis of the PeVatron Candidate Westerlund 1

TL;DR

This study used eROSITA X-ray data to analyze the PeVatron candidate Westerlund 1 and its associated gamma-ray source, aiming to distinguish between leptonic and hadronic particle acceleration scenarios, but found no definitive evidence favoring either.

Contribution

First, it provided constraints on the magnetic field and particle populations of HESS J1646-458 using X-ray observations, and second, it assessed the thermal versus nonthermal nature of Wd 1's diffuse emission.

Findings

No clear distinction between thermal and nonthermal emission for Wd 1.

No evidence of X-ray synchrotron emission from HESS J1646-458.

Upper bound on magnetic field strength of 7 microGauss.

Abstract

It is unclear which fraction of cosmic rays above an energy of 1 PeV is accelerated by the observed Galactic PeVatron population. These sources' gamma-ray data is typically degenerate between hadronic and leptonic emission scenarios, which hinders their straightforward association with the cosmic ray population. Here, we aimed to distinguish between leptonic and hadronic particle acceleration scenarios for the PeVatron candidate HESS J1646-458, associated with the star cluster Westerlund 1 (Wd 1). We first studied the diffuse X-ray emission from Wd 1 to better understand if its origin is of thermal or nonthermal nature. In addition, we searched for X-ray synchrotron emission from the associated PeVatron candidate HESS J1646-458 to put new constraints on the magnetic field strength and the leptonic particle population of this source. We used data from eROSITA on board the SRG orbital platform to spectrally analyze the diffuse emission from Wd 1 and HESS J1646-458. For Wd 1, we compared a purely thermal model and a model with a thermal and a nonthermal component. Next, we analyzed the spectra of four annuli around Wd 1 which coincide with HESS J1646-458 to search for synchrotron radiation. We find that eROSITA data cannot distinguish between thermal and nonthermal source scenarios for the diffuse emission from Wd 1 itself. In the case of HESS J1646-458, we find no evidence of synchrotron emission. We estimated an upper confidence bound of the synchrotron flux up to 40' around Wd 1 of 1.9e-3 keV-1 cm-2 s-1, which we used to study the spectral energy distribution of the source. From this, we obtained an upper 1 sigma bound on the magnetic field strength of HESS J1646-458 of 7 uG. This is compatible with a previous estimate in the literature for a fully leptonic source scenario. A purely leptonic emission scenario, a hadronic, and a hybrid one are compatible with our results.