# Galaxy And Mass Assembly (GAMA): The galaxy stellar mass function to   $z=0.1$ from the r-band selected equatorial regions

**Authors:** A. H. Wright, A. S. G. Robotham, S. P. Driver, M. Alpaslan, S. K., Andrews, I. K. Baldry, J. Bland-Hawthorn S. Brough, M. J. I. Brown, M., Colless, E. da Cunha, L. J. M. Davies, Alister W. Graham, B. W. Holwerda, A., M. Hopkins, P. R. Kafle, L. S. Kelvin, J. Loveday, S. J. Maddox, M. J. Meyer,, A. J. Moffett, P. Norberg, S. Phillipps, K. Rowlands, E. N. Taylor, L. Wang,, S. M. Wilkins

arXiv: 1705.04074 · 2017-06-28

## TL;DR

This paper derives the low-redshift galaxy stellar mass function from the GAMA dataset, correcting for dust effects, and explores its shape down to very low masses, providing new insights into galaxy distribution and stellar mass density.

## Contribution

It presents a detailed measurement of the galaxy stellar mass function to very low masses using GAMA data, including dust corrections and analysis of the distribution's shape down to $10^{6} M_\odot$, which was not previously achieved.

## Key findings

- The GSMF is well fit by a double Schechter function.
- Surface brightness effects do not bias the mass function above 10$^{7.5}$ M$_{\odot}$.
- The distribution maintains a power-law slope down to $10^{6.5}$ M$_{\odot}$.

## Abstract

We derive the low redshift galaxy stellar mass function (GSMF), inclusive of dust corrections, for the equatorial Galaxy And Mass Assembly (GAMA) dataset covering 180 deg$^2$. We construct the mass function using a density-corrected maximum volume method, using masses corrected for the impact of optically thick and thin dust. We explore the galactic bivariate brightness plane ($M_\star-\mu$), demonstrating that surface brightness effects do not systematically bias our mass function measurement above 10$^{7.5}$ M$_{\odot}$. The galaxy distribution in the $M-\mu$-plane appears well bounded, indicating that no substantial population of massive but diffuse or highly compact galaxies are systematically missed due to the GAMA selection criteria. The GSMF is {fit with} a double Schechter function, with $\mathcal M^\star=10^{10.78\pm0.01\pm0.20}M_\odot$, $\phi^\star_1=(2.93\pm0.40)\times10^{-3}h_{70}^3$Mpc$^{-3}$, $\alpha_1=-0.62\pm0.03\pm0.15$, $\phi^\star_2=(0.63\pm0.10)\times10^{-3}h_{70}^3$Mpc$^{-3}$, and $\alpha_2=-1.50\pm0.01\pm0.15$. We find the equivalent faint end slope as previously estimated using the GAMA-I sample, although we find a higher value of $\mathcal M^\star$. Using the full GAMA-II sample, we are able to fit the mass function to masses as low as $10^{7.5}$ $M_\odot$, and assess limits to $10^{6.5}$ $M_\odot$. Combining GAMA-II with data from G10-COSMOS we are able to comment qualitatively on the shape of the GSMF down to masses as low as $10^{6}$ $M_\odot$. Beyond the well known upturn seen in the GSMF at $10^{9.5}$ the distribution appears to maintain a single power-law slope from $10^9$ to $10^{6.5}$. We calculate the stellar mass density parameter given our best-estimate GSMF, finding $\Omega_\star= 1.66^{+0.24}_{-0.23}\pm0.97 h^{-1}_{70} \times 10^{-3}$, inclusive of random and systematic uncertainties.

## Full text

_Full body text omitted from this summary view._ Fetch the complete paper as Markdown: https://tomesphere.com/paper/1705.04074/full.md

## Figures

15 figures with captions in the complete paper: https://tomesphere.com/paper/1705.04074/full.md

## References

93 references — full list in the complete paper: https://tomesphere.com/paper/1705.04074/full.md

---
Source: https://tomesphere.com/paper/1705.04074