2017MNRAS.470.2599C


Query : 2017MNRAS.470.2599C

2017MNRAS.470.2599C - Mon. Not. R. Astron. Soc., 470, 2599-2610 (2017/September-3)

A break in the high-redshift stellar mass Tully-Fisher relation.

CHRISTENSEN L. and HJORTH J.

Abstract (from CDS):

We investigate the stellar-mass Tully-Fisher relation (TFR) between the stellar mass and the integrated gas velocity dispersion, quantified by the kinematic estimator S0.5 measured from strong emission lines in spectra of galaxies at 0 < z < 5. We combine luminosity-selected galaxies ('high-luminosity sample') with galaxies selected in other ways ('low-luminosity sample') to cover a range in stellar mass that spans almost five orders of magnitude: 7.0 <= log M*/M☉ <= 11.5. We find that the logarithmic power-law slope and normalization of the TFR are independent of redshift out to z ∼ 3. The scatter in the TFR is <0.5 dex such that the gas velocity dispersion can be used as a proxy for the stellar mass of a galaxy independently of its redshift. At z > 3, the scatter increases and the existence of a correlation is not obvious. The high-luminosity sample exhibits a flatter slope of 1.5 ± 0.2 at z < 3 compared to the low-luminosity sample slope of 2.9 ± 0.3, suggesting a turnover in the TFR. The combined sample is well fit with a break in the TFR at a characteristic stellar-mass scale of M* ∼ 1010 M☉, with no significant evolution out to z ∼ 3. We demonstrate that a break in the TFR with a steeper slope at the low-mass end is a natural consequence of galaxy models with a mass-dependent stellar-to-halo mass ratio.

Abstract Copyright: © 2017 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society

Journal keyword(s): galaxies: evolution - galaxies: fundamental parameters - galaxies: high-redshift - galaxies: kinematics and dynamics - galaxies: kinematics and dynamics

Simbad objects: 39

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Number of rows : 39
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 GRB 021004 gB 00 26 54.68 +18 55 41.6           ~ 560 0
2 GRB 060719 gB 01 13 43.380 -48 22 55.09           ~ 107 0
3 GRB 000210 gB 01 59 15 -40 40.0           ~ 175 0
4 GRB 110918A gB 02 10 09.39 -27 06 19.6           ~ 83 0
5 GRB 000911 gB 02 18 42 +07 48.0           ~ 163 0
6 SN 2009nz SN* 02 26 19.87 -18 57 08.6           ~ 307 1
7 GRB 070802 gB 02 27 35.91 -55 31 39.1           ~ 168 0
8 Fermi bn090926914 gB 03 05 14.30 -38 59 50.9           ~ 149 1
9 SN 2006aj SN* 03 21 39.670 +16 52 02.27 17.96 19.11 17.40     SNIc-BL 1007 1
10 GRB 090407 gB 04 35 54.98 -12 40 45.5           ~ 87 0
11 GRB 050915A gB 05 26 44.804 -28 00 59.27           ~ 88 0
12 GRB 061126 gB 05 46 24.460 +64 12 38.49 18.62 18.79 19.20     ~ 182 1
13 Fermi bn120119170 gB 08 00 06.940 -09 04 53.83           ~ 193 0
14 SN 2003lw SN* 08 02 30.1 -39 51 03       20.23   SNIc: 576 0
15 SN 2012bz SN* 09 07 38.38 +14 01 07.5           SNIb/c 193 1
16 GRB 070306 gB 09 52 23.220 +10 28 55.20           ~ 222 1
17 SN 2003dh SN* 10 44 50.030 +21 31 18.15     16.2     SNIcpec 1261 1
18 GRB 011211 gB 11 15 16 -21 56.0           ~ 305 0
19 Fermi bn120624933 gB 11 23 31.98 +08 55 42.1           ~ 100 0
20 SDSS J112848.22+170418.5 G 11 28 48.22989 +17 04 18.5014           ~ 393 0
21 SN 2013cq SN* 11 32 32.84 +27 41 56.2           SNIc 613 1
22 GRB 000418 gB 12 25 21 +20 05.0           ~ 219 0
23 GRB 050416 gB 12 33 54.600 +21 03 26.69     19.12     ~ 300 1
24 GRB 090426 G 12 36 18.0470 +32 59 09.460           ~ 237 0
25 Fermi bn090323002 gB 12 42 50.28 +17 03 11.9           ~ 244 1
26 GRB 080207 gB 13 50 03.02 +07 30 08.0           ~ 114 0
27 GRB 060814 gB 14 45 21.480 +20 35 11.80           ~ 241 0
28 GRB 100418A gB 17 05 26.96 +11 27 41.9           ~ 198 0
29 GRB 080605 gB 17 28 30.04 +04 00 56.9           ~ 198 0
30 Fermi bn140506880 gB 18 27 06.04 -55 38 08.7           ~ 113 0
31 SN 1998bw SN* 19 35 03.17 -52 50 46.1   14.09       SNIc 1928 2
32 GRB 080805 gB 20 56 55.30 -62 25 58.8           ~ 102 0
33 GRB 100621A gB 21 01 13.12 -51 06 22.5           ~ 204 0
34 GRB 060614 G 21 23 32.140 -53 01 36.10           ~ 714 0
35 Fermi bn081109293 gB 22 03 11.50 -54 42 40.5           ~ 125 1
36 GRB 060505 gB 22 07 03.440 -27 48 51.89           ~ 286 1
37 GRB 071021 gB 22 42 34.33 +23 43 05.4           ~ 104 0
38 NVSS J230126-385839 rG 23 01 26.7650 -38 58 40.422   22.22 21.22 21   ~ 325 1
39 GRB 051022A gB 23 56 04.200 +19 36 32.30           ~ 194 1

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