Abstract

Using the multi-integral field spectrograph GIRAFFE at VLT, we have derived the K-band Tully-Fisher relation (TFR) at z ∼ 0.6 for a representative sample of 65 galaxies with emission lines (W0(OII) ≥ 15 A). We confirm that the scatter in the z ∼ 0. 6T FR is caused by galaxies with anomalous kinematics, and find a positive and strong correlation between the complexity of the kinematics and the scatter that they contribute to the TFR. Considering only relaxed-rotating disks, the scatter, and possibly also the slope, of the TFR, do not appear to evolve with redshift. We detect an evolution of the K-band TFR zero point between z ∼ 0. 6a ndz = 0, which, if interpreted as an evolution of the K-band luminosity of rotating disks, would imply that a brightening of 0.66 ± 0.14 mag occurs between z ∼ 0. 6a ndz = 0. Any disagreement with the results of Flores et al. (2006, A&A, 455, 107) are attributed to both an improvement of the local TFR and the more detailed accurate measurement of the rotation velocities in the distant sample. Most of the uncertainty can be explained by the relatively coarse spatial-resolution of the kinematical data. Because most rotating disks at z ∼ 0.6 are unlikely to experience further merging events, one may assume that their rotational velocity, which is taken as a proxy of the total mass, does not evolve dramatically. If true, our result implies that rotating disks observed at z ∼ 0.6 are rapidly transforming their gas into stars, to be able to double their stellar masses and be observed on the TFR at z = 0. The rotating disks observed are indeed emission-line galaxies that are either starbursts or LIRGs, which implies that they are forming stars at a high rate. Thus, a significant fraction of the rotating disks are forming the bulk of their stars within 6 to 8 Gyr, in good agreement with former studies of the evolution of the mass-metallicity relationship.

Highlights

  • Since the first rotation curves were measured at intermediate redshifts (Vogt et al 1993), many studies have been devoted to the evolution of the Tully-Fisher Relation (TFR, Tully & Fisher 1977), given its prominent role in constraining galaxy-formation models (e.g., Dutton et al 2007)

  • We confirm that the scatter in the z ∼ 0.6 Tully-Fisher relation (TFR) is caused by galaxies with anomalous kinematics, and find a positive and strong correlation between the complexity of the kinematics and the scatter that they contribute to the TFR

  • We have studied the evolution of the K-band TFR, using a representative sample of 65 emission line, intermediate-mass galaxies at z ∼ 0.6, unaffected by field-to-field variations within Poisson statistics, and observed using 3D spectroscopy

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Summary

Introduction

Since the first rotation curves were measured at intermediate redshifts (Vogt et al 1993), many studies have been devoted to the evolution of the Tully-Fisher Relation (TFR, Tully & Fisher 1977), given its prominent role in constraining galaxy-formation models (e.g., Dutton et al 2007). Böhm & Ziegler (2007) showed that this effect could be attributed to an incompleteness in magnitude provided that the scatter decreased by a factor of at least three between z ∼ 0.5 and z = 0, with no evolution of slope or zero point. In almost all of these studies, the B-band TFR shows a large dispersion in comparison with the local relation, especially at the low-luminosity (or velocity) end (e.g., Böhm et al 2004). They proposed a possible luminosity-dependent evolution, in which distant lowluminosity galaxies would have lower mass-to-light ratios [M/L]. The situation for B-band data remains unclear, concerning the large scatter in measurements found at high redshift

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