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The weak dependence of velocity dispersion on disc fractions, mass-to-light ratio, and redshift: implications for galaxy and black hole evolution

The weak dependence of velocity dispersion on disc fractions, mass-to-light ratio, and redshift: implications for galaxy and black hole evolution
The weak dependence of velocity dispersion on disc fractions, mass-to-light ratio, and redshift: implications for galaxy and black hole evolution
Velocity dispersion (σ) is a key driver for galaxy structure and evolution. We here present a comprehensive semi-empirical approach to compute σ via detailed Jeans modelling assuming both a constant and scale-dependent mass-to-light ratio M*/L. We compare with a large sample of local galaxies from MaNGA and find that both models can reproduce the Faber–Jackson (FJ) relation and the weak dependence of σ on bulge-to-total (B/T) ratio (for B/T ≳ 0.25). The dynamical-to-stellar mass ratio within R ≲ Re can be fully accounted for by a gradient in M*/L. We then build velocity dispersion evolutionary tracks σap[M*, z] (within an aperture) along the main progenitor dark matter haloes assigning stellar masses, effective radii, and Sérsic  indices via a variety of abundance matching and empirically motivated relations. We find: (1) clear evidence for downsizing in σap[M*, z] along the progenitor tracks; (2) at fixed stellar mass σ ∝ (1 + z)0.2−0.3 depending on the presence or not of a gradient in M*/L. We extract σap[M*, z] from the TNG50 hydrodynamic simulation and find very similar results to our models with constant M*/L. The increasing dark matter fraction within Re tends to flatten the σap[M*, z] along the progenitors at z ≳ 1 in constant M*/L models, while σap[M*, z] have a steeper evolution in the presence of a stellar gradient. We then show that a combination of mergers and gas accretion is likely responsible for the constant or increasing σap[M*, z] with time. Finally, our σap[M*, z] are consistent with a nearly constant and steep Mbh − σ relation at z ≲ 2, with black hole masses derived from the LX − M* relation.
1365-2966
5639–5660
Marsden, Christopher
ccd1ecc8-3eb4-4699-a87e-0bfba0dd40b0
Shankar, F.
b10c91e4-85cd-4394-a18a-d4f049fd9cdb
Fu, Hao
09d6267e-c26d-4ac1-a653-2c5886c12b1e
Bernardi, Mariangela
51f0929c-ba65-4d9c-a814-673442f48d75
Sheth, Ravi K.
94b203a4-bea4-461b-a237-14d548264e15
Lapi, Andrea
126b5f87-60fa-4a57-8b84-802d5ffb1f17
Marsden, Christopher
ccd1ecc8-3eb4-4699-a87e-0bfba0dd40b0
Shankar, F.
b10c91e4-85cd-4394-a18a-d4f049fd9cdb
Fu, Hao
09d6267e-c26d-4ac1-a653-2c5886c12b1e
Bernardi, Mariangela
51f0929c-ba65-4d9c-a814-673442f48d75
Sheth, Ravi K.
94b203a4-bea4-461b-a237-14d548264e15
Lapi, Andrea
126b5f87-60fa-4a57-8b84-802d5ffb1f17

Marsden, Christopher, Shankar, F., Fu, Hao, Bernardi, Mariangela, Sheth, Ravi K. and Lapi, Andrea (2021) The weak dependence of velocity dispersion on disc fractions, mass-to-light ratio, and redshift: implications for galaxy and black hole evolution. Monthly Notices of the Royal Astronomical Society, 510 (4), 5639–5660. (doi:10.1093/mnras/stab3705).

Record type: Article

Abstract

Velocity dispersion (σ) is a key driver for galaxy structure and evolution. We here present a comprehensive semi-empirical approach to compute σ via detailed Jeans modelling assuming both a constant and scale-dependent mass-to-light ratio M*/L. We compare with a large sample of local galaxies from MaNGA and find that both models can reproduce the Faber–Jackson (FJ) relation and the weak dependence of σ on bulge-to-total (B/T) ratio (for B/T ≳ 0.25). The dynamical-to-stellar mass ratio within R ≲ Re can be fully accounted for by a gradient in M*/L. We then build velocity dispersion evolutionary tracks σap[M*, z] (within an aperture) along the main progenitor dark matter haloes assigning stellar masses, effective radii, and Sérsic  indices via a variety of abundance matching and empirically motivated relations. We find: (1) clear evidence for downsizing in σap[M*, z] along the progenitor tracks; (2) at fixed stellar mass σ ∝ (1 + z)0.2−0.3 depending on the presence or not of a gradient in M*/L. We extract σap[M*, z] from the TNG50 hydrodynamic simulation and find very similar results to our models with constant M*/L. The increasing dark matter fraction within Re tends to flatten the σap[M*, z] along the progenitors at z ≳ 1 in constant M*/L models, while σap[M*, z] have a steeper evolution in the presence of a stellar gradient. We then show that a combination of mergers and gas accretion is likely responsible for the constant or increasing σap[M*, z] with time. Finally, our σap[M*, z] are consistent with a nearly constant and steep Mbh − σ relation at z ≲ 2, with black hole masses derived from the LX − M* relation.

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2112.09720 - Accepted Manuscript
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Accepted/In Press date: 15 December 2021
e-pub ahead of print date: 26 December 2021
Additional Information: arXiv:2112.09720

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Local EPrints ID: 456254
URI: http://eprints.soton.ac.uk/id/eprint/456254
ISSN: 1365-2966
PURE UUID: 30285c0e-37a7-4832-86e9-b81c1ff39df1

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Date deposited: 26 Apr 2022 23:51
Last modified: 16 Mar 2024 16:32

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Contributors

Author: Christopher Marsden
Author: F. Shankar
Author: Hao Fu
Author: Mariangela Bernardi
Author: Ravi K. Sheth
Author: Andrea Lapi

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