Redshift evolution of the Fundamental Plane relation in the IllustrisTNG simulation

Author:

Lu Shengdong12ORCID,Xu Dandan3,Wang Yunchong43ORCID,Mao Shude31,Ge Junqiang1,Springel Volker5ORCID,Wang Yuan6,Vogelsberger Mark7ORCID,Naiman Jill89ORCID,Hernquist Lars8

Affiliation:

1. National Astronomical Observatories, Chinese Academy of Sciences, 20A Datun Road, Chaoyang District, Beijing 100101, China

2. University of Chinese Academy of Sciences, Beijing 100049, China

3. Department of Astronomy and Tsinghua Center for Astrophysics, Tsinghua University, Beijing 100084, China

4. Department of Physics, Tsinghua University, Beijing 100084, China

5. Max-Planck-Institut für Astrophysik, Karl-Schwarzschild-Str. 1, D-85748 Garching, Germany

6. School of Physics, Nankai University, Tianjin 300071, China

7. Kavli Institute for Astrophysics and Space Research, Department of Physics, MIT, Cambridge, MA 02139, USA

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

9. The School of Information Sciences at the University of Illinois Urbana-Champaign, 501 E Daniel St, Champaign, IL 61820, USA

Abstract

ABSTRACT We investigate the Fundamental Plane (FP) evolution of early-type galaxies in the IllustrisTNG-100 simulation (TNG100) from redshift z = 0 to z = 2. We find that a tight plane relation already exists as early as z = 2. Its scatter stays as low as ∼0.08 dex across this redshift range. Both slope parameters b and c (where R ∝ σbIc with R, σ, and I being the typical size, velocity dispersion, and surface brightness) of the plane evolve mildly since z = 2, roughly consistent with observations. The FP residual $\rm Res$ ($\equiv \, a\, +\, b\log \sigma \, +\, c\log I\, -\, \log R$, where a is the zero-point of the FP) is found to strongly correlate with stellar age, indicating that stellar age can be used as a crucial fourth parameter of the FP. However, we find that 4c + b + 2 = δ, where δ ∼ 0.8 for FPs in TNG, rather than zero as is typically inferred from observations. This implies that a tight power-law relation between the dynamical mass-to-light ratio Mdyn/L and the dynamical mass Mdyn (where Mdyn ≡ 5σ2R/G, with G being the gravitational constant) is not present in the TNG100 simulation. Recovering such a relation requires proper mixing between dark matter and baryons, as well as star formation occurring with correct efficiencies at the right mass scales. This represents a powerful constraint on the numerical models, which has to be satisfied in future hydrodynamical simulations.

Funder

Deutsche Forschungsgemeinschaft

National Natural Science Foundation of China

Publisher

Oxford University Press (OUP)

Subject

Space and Planetary Science,Astronomy and Astrophysics

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