A Candidate Active Galactic Nucleus with a Pure Soft Thermal X-ray Spectrum

TL;DR

This paper reports the discovery of a candidate AGN with a unique pure soft thermal X-ray spectrum, resembling Galactic black hole binaries, and discusses its spectral properties and implications for black hole mass and accretion state.

Contribution

It presents the identification and analysis of a new AGN with an unusual soft thermal X-ray spectrum, highlighting its spectral variability and potential high Eddington ratio.

Findings

Soft X-ray spectrum dominated with no hard emission detected

Spectral variability consistent with strong Comptonization

Implied black hole mass smaller than ~10^5 solar masses

Abstract

We report the discovery of a candidate active galactic nucleus (AGN), 2XMM J123103.2+110648 at z = 0.13, with an X-ray spectrum represented purely by soft thermal emission reminiscent of Galactic black hole (BH) binaries in the disk-dominated state. This object was found in the second XMM serendipitous source catalogue as a highly variable X-ray source. In three separate observations, its X-ray spectrum can be represented either by a multicolor disk blackbody model with an inner temperature of kT_in~0.16-0.21 keV or a Wien spectrum Comptonized by an optically thick plasma with kT~0.14-0.18 keV. The soft X-ray luminosity in the 0.5--2 keV band is estimated to be (1.6-3.8)x10^42 erg/s. Hard emission above ~2 keV is not detected. The ratio of the soft to hard emission is the strongest among AGNs observed thus far. Spectra selected in high/low flux time intervals are examined in order to study spectral variability. In the second observation with the highest signal-to-noise ratio, the low energy (below 0.7 keV) spectral regime flattens when the flux is high, while the shape of the high energy part (1-1.7 keV) remains unchanged. This behavior is qualitatively consistent with being caused by strong Comptonization. Both the strong soft excess and spectral change consistent with Comptonization in the X-ray spectrum imply that the Eddington ratio is large, which requires a small BH mass (smaller than ~10^5M_solar.