http://arxiv.org/abs/2110.05037

This paper is the fourth in a series presenting (galaxy morphology, and thus galaxy formation)-dependent black hole mass, $M_{\rm BH}$, scaling relations. We have used a sample of 119 galaxies with directly-measured $M_{\rm BH}$ and host spheroid parameters obtained from multi-component decomposition of, primarily, $3.6\,\mu$m Spitzer images. Here, we investigate the correlations between $M_{\rm BH}$ and the projected luminosity density $\mu$, the projected stellar mass density $\Sigma$, and the deprojected (internal) stellar mass density $\rho$, for various spheroid radii. We discover the predicted $M_{\rm BH}$–$\mu_{\rm 0,sph}$ relation and present the first $M_{\rm BH}$–$\mu_{\rm e, sph}$ and $M_{\rm BH}$–$\rho_{\rm e,int, sph}$ diagrams displaying slightly different (possibly curved) trends for early- and late-type galaxies (ETGs and LTGs) and an offset between ETGs with (fast-rotators, ES/S0) and without (slow-rotators, E) a disk. The scatter about various $M_{\rm BH}$–$\langle\Sigma\rangle_{\rm R,sph}$ (and $\langle\rho\rangle_{\rm r,sph}$) relations is shown to systematically decrease as the enclosing aperture (and volume) increases, dropping from 0.69~dex when using the spheroid \enquote{compactness}, $\langle\Sigma\rangle_{\rm 1kpc,sph}$, to 0.59~dex when using $\langle\Sigma\rangle_{\rm 5kpc,sph}$. We also reveal that $M_{\rm BH}$ correlates with the internal density, $\rho_{\rm soi,sph}$, at the BH’s sphere-of-influence radius, such that core-S\’ersic (high S\’ersic index, $n$) and (low-$n$) S\’ersic galaxies define different relations with total rms scatters 0.21~dex and 0.77~dex, respectively.(Abridged)

Read this paper on arXiv…

N. Sahu, A. Graham and B. Davis
Tue, 12 Oct 21
43/73

Comments: 27 pages, 12 figures, 2 tables, submitted to ApJ