X-ray obscuration from a variable ionized absorber in PG 1114+445

TL;DR

This study analyzes X-ray observations of quasar PG 1114+445, revealing significant variability in ionized absorbers over 20 months, indicating dynamic, clumpy outflows that can obscure the X-ray source.

Contribution

First detailed analysis of long-term variability of ionized absorbers in PG 1114+445, showing evidence of changing column density and ionization state over months.

Findings

Detected a fully covering absorber with higher column density than previous observations.

Observed a low flux state with increased obscuration.

Estimated the ionized absorber's minimum distance at over 0.5 parsecs.

Abstract

Photoionized absorbers of outflowing gas are commonly found in the X-ray spectra of active galactic nuclei (AGN). While most of these absorbers are seldom significantly variable, some ionized obscurers have been increasingly found to substantially change their column density on a wide range of time scales. These $N_\text{H}$ variations are often considered as the signature of the clumpy nature of the absorbers. Here we present the analysis of a new Neil Gehrels Swift Observatory campaign of the type-1 quasar PG 1114+445, which was observed to investigate the time evolution of the multiphase outflowing absorbers previously detected in its spectra. The analyzed dataset consists of 22 observations, with a total exposure of $\sim90$ ks, spanning about $20$ months. During the whole campaign, we report an unusually low flux state with respect to all previous X-ray observations of this quasar. From the analysis of the stacked spectra we find a fully covering absorber with a column density $\log(N_\text{H}/\text{cm}^{-2})=22.9^{+0.3}_{-0.1}$. This is an order of magnitude higher than the column density measured in the previous observations. This is either due to a variation of the known absorbers, or by a new one, eclipsing the X-ray emitting source. We also find a ionization parameter of $\log(\xi/\text{erg cm s}^{-1})=1.4^{+0.6}_{-0.2}$. Assuming that the obscuration lasts for the whole duration of the campaign, i.e. more than $20$ months, we estimate the minimum distance of the ionized clump, which is located at $r\gtrsim0.5$ pc.