2018A&A...619A..70H


Query : 2018A&A...619A..70H

2018A&A...619A..70H - Astronomy and Astrophysics, volume 619A, 70-70 (2018/11-1)

The Hydra I cluster core. II. Kinematic complexity in a rising velocity dispersion profile around the cD galaxy NGC 3311.

HILKER M., RICHTLER T., BARBOSA C.E., ARNABOLDI M., COCCATO L. and MENDES DE OLIVEIRA C.

Abstract (from CDS):


Context. NGC 3311, the central galaxy of the Hydra I cluster, shows signatures of recent infall of satellite galaxies from the cluster environment.Previous work has shown that the line-of-sight velocity dispersion of the stars and globular clusters in the extended halo of NGC 3311 rises up to the value of the cluster velocity dispersion. In the context of Jeans models, a massive dark halo with a large core is needed to explain this finding. However, position dependent long-slit measurements show that the kinematics are still not understood.
Aims. We aim to find kinematic signatures of sub-structures in the extended halo of NGC 3311.
Methods. We performed multi-object spectroscopic observations of the diffuse stellar halo of NGC 3311 using VLT/FORS2 in MXU mode to mimic a coarse "IFU". The slits of the outermost masks reach out to about 35kpc of galactocentric distance. We usePPXF to extract the kinematic information of velocities, velocity dispersions and the high-order moments h3 and h4.
Results. We find a homogeneous velocity field and velocity dispersion field within a radius of about 10kpc. Beyond this radius, both the velocities and the velocity dispersion start to depend on azimuth angle and show a significant intrinsic scatter. The inner spheroid of NGC 3311 can be described as a slow rotator. Outside 10kpc the cumulative angular momentum is rising, however, without showing an ordered rotation signal. If the radial dependence alone is considered, the velocity dispersion does not simply rise but fills an increasingly large range of dispersion values with two well defined envelopes. The lower envelope is about constant at 200km/s. The upper envelope rises smoothly, joining the velocity dispersion of the outer globular clusters and the cluster galaxies. We interpret this behaviour as the superposition of tracer populations with increasingly shallower radial distributions between the extremes of the inner stellar populations and the cluster galaxies. Simple Jeans models illustrate that a range of mass profiles can account for all observed velocity dispersions, including radial MOND models.
Conclusions. The rising velocity dispersion of NGC 3311 apparently is a result of averaging over a range of velocity dispersions related to different tracer populations in the sense of different density profiles and anisotropies. Jeans models using one tracer population with a unique density profile are not able to explain the large range of the observed kinematics.Previous claims about the cored dark halo of NGC 3311 are therefore probably not valid. This may in general apply to central cluster galaxies with rising velocity dispersion profiles, where infall processes are important.

Abstract Copyright: © ESO 2018

Journal keyword(s): galaxies: clusters: individual: Hydra I - galaxies: elliptical and lenticular, cD - galaxies: haloes - galaxies: individual: NGC 3311 - galaxies: kinematics and dynamics - galaxies: formation

Simbad objects: 25

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Number of rows : 25
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 NGC 507 BiC 01 23 39.950 +33 15 22.22   13.0       ~ 431 3
2 NGC 1016 GiG 02 38 19.5696395016 +02 07 09.482594448   13.3       ~ 90 0
3 ACO 383 ClG 02 48 03.3915 -03 31 45.228           ~ 354 0
4 NGC 1129 BiC 02 54 27.400 +41 34 46.70   14.6 13.6     ~ 118 1
5 NAME HYA SUPERCL SCG 08 57.9 +03 10           ~ 173 0
6 NGC 3158 rG 10 13 50.527 +38 45 53.68   13.4       ~ 116 0
7 NGC 3309 GiG 10 36 35.6607096792 -27 31 05.732321664   11.98 11.78 10.34 10.51 ~ 160 0
8 NAME Hydra I Cluster ClG 10 36 36.0 -27 31 04           ~ 832 1
9 2MASX J10364122-2733392 GiG 10 36 41.1952357848 -27 33 39.785933952   15.7 14.18   12.99 ~ 44 0
10 NGC 3311 EmG 10 36 42.821 -27 31 42.02   11.93 10.93 10.00 9.67 ~ 296 2
11 NGC 3331 Sy1 10 40 08.9621961768 -23 49 13.559619180   13.94   12.94   ~ 32 0
12 ACO 1413 ClG 11 55 12.87 +23 23 46.9           ~ 424 0
13 NGC 4365 GiG 12 24 28.228 +07 19 03.07   11.5       ~ 832 0
14 M 84 Sy2 12 25 03.74333 +12 53 13.1393 12.67 12.09 10.49     ~ 1745 2
15 NAME Virgo Cluster ClG 12 26 32.1 +12 43 24           ~ 6551 0
16 M 87 AGN 12 30 49.42338414 +12 23 28.0436859 10.16 9.59 8.63   7.49 ~ 7066 3
17 NGC 4636 LIN 12 42 49.8333280080 +02 41 15.951929028   12.62 11.84     ~ 1107 1
18 NGC 5846 BiC 15 06 29.253 +01 36 20.29   11.9   9.74   ~ 842 1
19 IC 1101 rG 15 10 56.100 +05 44 41.19   15.10       ~ 155 2
20 ACO 2029 ClG 15 10 56.2 +05 44 42           ~ 939 0
21 NGC 6086 BiC 16 12 35.5357829352 +29 29 05.246712168   14.8       ~ 193 1
22 NGC 6166 Sy2 16 28 38.24470063 +39 33 04.2335319   12.78 11.78     ~ 754 5
23 ACO 2199 ClG 16 28 43.31 +39 34 07.6           ~ 1166 1
24 NGC 6173 LIN 16 29 44.8864037664 +40 48 41.890972320   14.0       ~ 165 0
25 NGC 7242 GiG 22 15 39.507 +37 17 55.48   14.6       ~ 47 0

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2023.11.28-11:16:41

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