Gas inflows towards the nucleus of the Seyfert 2 galaxy NGC1667

TL;DR

This study uses optical integral field spectroscopy to analyze gas inflows and outflows in the Seyfert 2 galaxy NGC1667, revealing complex kinematics and quantifying mass transfer rates that influence AGN feeding and star formation.

Contribution

It provides detailed measurements of gas inflow and outflow rates and identifies the kinematic components responsible for feeding the AGN in NGC1667, a novel detailed case study.

Findings

Ionized gas outflow rate of ~0.16 solar masses per year.

Maximum inflow rate of ~2.8 solar masses per year at 800pc.

Most inflowing gas does not reach the nucleus, accumulating instead in the inner regions.

Abstract

We use optical spectra from the inner 2$\times$3kpc$^2$ of the Seyfert 2 galaxy NGC1667, obtained with the GMOS integral field spectrograph on the Gemini South telescope at a spatial resolution of $\approx$ 240pc, to assess the feeding and feedback processes in this nearby AGN. We have identified two gaseous kinematical components in the emission line profiles: a broader component ($\sigma\approx$ 400km s$^{-1}$) which is observed in the inner 1-2arcsec and a narrower component ($\sigma\approx$ 200km s$^{-1}$) which is present over the entire field-of-view. We identify the broader component as due to an unresolved nuclear outflow. The narrower component velocity field shows strong isovelocity twists relative to a rotation pattern, implying the presence of strong non-circular motions. The subtraction of a rotational model reveals that these twists are caused by outflowing gas in the inner $\approx$ 1arcsec, and by inflows associated with two spiral arms at larger radii. We calculate an ionized gas mass outflow rate of $\dot{M}_{out}\approx$ 0.16M$_{\odot}$yr$^{-1}$. We calculate the net gas mass flow rate across a series of concentric rings, obtaining a maximum mass inflow rate in ionized gas of $\approx$ 2.8M$_{\odot}$year$^{-1}$ at 800pc from the nucleus, which is two orders of magnitude larger than the accretion rate necessary to power this AGN. However, as the mass inflow rate decreases at smaller radii, most of the gas probably will not reach the AGN, but accumulate in the inner few hundred parsecs. This will create a reservoir of gas that can trigger the formation of new stars.