The interplay between accretion, downsizing, and the formation of box/peanut bulges in TNG50

Author:

Anderson Stuart Robert1ORCID,Gough-Kelly Steven1ORCID,Debattista Victor P12ORCID,Du Min3,Erwin Peter45ORCID,Cuomo Virginia6,Caruana Joseph27,Hernquist Lars8,Vogelsberger Mark9ORCID

Affiliation:

1. Jeremiah Horrocks Institute, University of Central Lancashire , Preston PR1 2HE , UK

2. Institute of Space Sciences & Astronomy, University of Malta , Msida MSD 2080 , Malta

3. Department of Astronomy, Xiamen University , Xiamen, Fujian 361005 , China

4. Max-Planck-Insitut für extraterrestrische Physik , Giessenbachstrasse, D-85748 Garching , Germany

5. Universitäts-Sternwarte München , Scheinerstrasse 1, D-81679 München , Germany

6. Instituto de Astronomía y Ciencias Planetarias, Universidad de Atacama , Avenida Copayapu 485, 1350000 Copiapó , Chile

7. Department of Physics, Faculty of Science, University of Malta , Msida MSD 2080 , Malta

8. Harvard–Smithsonian Center for Astrophysics , 60 Garden Street, Cambridge, MA 02138 , USA

9. Department of Physics and Kavli Institute for Astrophysics and Space Research, Massachusetts Institute of Technology , Cambridge, MA 02139 , USA

Abstract

ABSTRACT From the TNG50 cosmological simulation we build a sample of 191 well-resolved barred galaxies with stellar mass $\mbox{$\log (M_{\star }/\mathrm{M}_{\odot })$}\gt 10$ at z = 0. We search for box/peanut bulges (BPs) in this sample, finding them in 55 per cent of cases. We compute $\mbox{$f_{\rm BP}$}$, the BP probability for barred galaxies as a function of M⋆, and find that this rises to a plateau, as found in observations of nearby galaxies. The transition mass where $\mbox{$f_{\rm BP}$}$ reaches half the plateau value is $\mbox{$\log (M_{\star }/\mathrm{M}_{\odot })$}= 10.13\pm 0.07$, consistent with the observational value within measurement errors. We show that this transition in $\mbox{$f_{\rm BP}$}$ can be attributed to the youth of the bars at low M⋆, which is a consequence of downsizing. Young bars, being generally shorter and weaker, have not yet had time to form BPs. At high mass, while we find a plateau, the value is at $\sim 60~{{\ \rm per\ cent}}$ whereas observations saturate at 100 per cent. We attribute this difference to excessive heating in TNG50 due to merger activity and numerical resolution effects. BPs in TNG50 tend to occur in galaxies with more quiescent merger histories. As a result, the main driver of whether a bar hosts a BP in TNG50 is not the galaxy mass, but how long and strong the bar is. Separating the BP sample into those that have visibly buckled and those that have not, we find that fully half of BP galaxies show clear signs of buckling, despite the excessive heating and limited vertical resolution of TNG50.

Funder

Royal Society

Newton Fund

FONDECYT

Publisher

Oxford University Press (OUP)

Subject

Space and Planetary Science,Astronomy and Astrophysics

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