2010A&A...519A..47A


Query : 2010A&A...519A..47A

2010A&A...519A..47A - Astronomy and Astrophysics, volume 519, A47-47 (2010/9-1)

Self-consistent nonspherical isothermal halos embedding zero-thickness disks.

AMORISCO N.C. and BERTIN G.

Abstract (from CDS):

That the rotation curves of spiral galaxies are generally flat in the outer regions is commonly considered an indication that galaxy disks are embedded in quasi-isothermal halos. In practice, disk-halo decompositions of galaxy rotation curves are performed in a parametric way by modeling the halo force contribution by means of expressions that approximately describe the properties of the regular isothermal sphere or other spherical density distributions suggested by cosmological simulations. In this paper we construct self-consistent models of nonspherical isothermal halos embedding a zero-thickness disk, by assuming that the halo distribution function is a Maxwellian. The general method developed here can also be used to study the properties of other physically-based choices for the halo distribution function and to the case of a disk accompanied by a bulge. The construction was performed by means of an iterative procedure that generalizes a method introduced in the past to construct spheroidal models of rotating elliptical galaxies. In a preliminary investigation, which set the empirical framework to study the self-consistent models developed in this paper, we note the existence of a fine tuning between the scalelengths RΩ and h, respectively characterizing the rise of the rotation curve and the luminosity profile of the disk, which surprisingly applies to both high surface brightness and low surface brightness galaxies in similar ways. We show that this empirical correlation identifies a much stronger conspiracy than the one required by the smoothness and flatness of the rotation curve and often referred to as disk-halo conspiracy. As a natural property, the self-consistent models presented in this paper are found to be characterized by smooth and flat rotation curves for very different disk-to-halo mass ratios, hence suggesting that conspiracy is not as dramatic as often imagined. For a typical, observed rotation curve, with asymptotically flat rotation curve at V (the precise value of which can also be treated as a free parameter), and a typical density profile of the disk, the relevant self-consistent models are characterized by two dimensionless parameters, which correspond to the dimensional scales (the disk mass-to-light ratio M/L and the halo central density) of standard disk-halo decompositions. We find that, if the rotation curve is decomposed by means of our self-consistent models, the disk-halo degeneracy is removed and that typical rotation curves are fitted by models that are below the maximum-disk prescription. Similar results are obtained from a study of NGC 3198. Finally, we quantify the flattening of the spheroidal halo, which is significant, especially on the scale of the visible disk.

Abstract Copyright:

Journal keyword(s): galaxies: spiral - galaxies: structure - galaxies: halos - galaxies: kinematics and dynamics - galaxies: individual: NGC 3198

Simbad objects: 40

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Number of rows : 40
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2023
#notes
1 UGC 128 LSB 00 13 50.93 +35 59 36.6   16.5       ~ 96 1
2 M 31 G 00 42 44.330 +41 16 07.50 4.86 4.36 3.44     ~ 12388 1
3 NGC 247 LSB 00 47 08.554 -20 45 37.44 10.11 9.61 9.10 8.87   ~ 426 2
4 NGC 300 GiG 00 54 53.4465638304 -37 41 03.168402396 8.83 8.69 8.13 7.46   ~ 1461 2
5 UGC 1230 LSB 01 45 32.251 +25 31 17.28   17       ~ 85 0
6 IC 2006 EmG 03 54 28.4628183240 -35 58 01.673622516   12.39   10.94 11.9 ~ 205 0
7 NGC 2403 AGN 07 36 51.3381434280 +65 36 09.650825640 9.31 8.84 8.38 8.19   ~ 1758 1
8 AGC 180072 LSB 08 09 32.6 +22 33 34           ~ 49 0
9 LEDA 86666 LSB 08 53 03.9 +18 26 09           ~ 72 0
10 UGC 5005 LSB 09 24 29.387 +22 16 29.37   18       ~ 74 0
11 LEDA 86670 LSB 09 37 36.6 +21 46 15           ~ 51 0
12 NGC 3109 AG? 10 03 06.877 -26 09 34.46 11.10 10.42 10.04 9.91   ~ 759 2
13 NGC 3198 EmG 10 19 54.990 +45 32 58.88 10.83 10.87 10.33     ~ 892 1
14 LSB F568-3 LSB 10 26 59 +22 13.6           ~ 78 0
15 UGC 5750 AG? 10 35 45.12 +20 59 24.9   17       ~ 74 0
16 LEDA 86672 LSB 10 45 02.064 +22 03 15.54           ~ 80 0
17 UGC 5999 LSB 10 52 58.652 +07 37 11.27   18       ~ 52 0
18 UGC 6399 AG? 11 23 23.2200537264 +50 53 33.503083728   14.9       ~ 106 0
19 LEDA 86674 LSB 11 26 18.9 +18 50 08           ~ 50 0
20 UGC 6446 GiC 11 26 40.4656762968 +53 44 48.012539280   14.5       ~ 154 0
21 NGC 3769 GiP 11 37 44.0727836208 +47 53 34.782808956   11.7       ~ 181 0
22 UGC 6667 GiC 11 42 26.309 +51 35 52.82   14.8       ~ 117 0
23 NGC 3877 GiG 11 46 07.782 +47 29 40.20   11.8       ~ 318 0
24 NGC 3893 GiP 11 48 38.207 +48 42 38.84   11.23 10.67     ~ 367 1
25 NGC 3917 GiP 11 50 45.4481861760 +51 49 27.919475076   12.5       ~ 184 0
26 NGC 3972 GiP 11 55 45.09048 +55 19 14.6460   13.14   11.94   ~ 206 1
27 UGC 6917 GiG 11 56 28.773 +50 25 42.22   14.0       ~ 135 0
28 UGC 6923 GiC 11 56 49.526 +53 09 37.21   13.90   12.96   ~ 145 0
29 UGC 6930 EmG 11 57 17.3777198280 +49 17 00.669514488   14.2       ~ 125 0
30 IC 749 GiP 11 58 34.0447608696 +42 44 02.528915820   13.4 12.52     ~ 131 0
31 NGC 4010 GiG 11 58 37.991 +47 15 40.72   13.1       ~ 149 0
32 UGC 6983 GiC 11 59 08.734 +52 42 28.03   14.5       ~ 170 0
33 NGC 4085 GiP 12 05 22.7304442992 +50 21 10.608113412   13.93 12.83     ~ 182 0
34 NGC 4157 GiP 12 11 04.365 +50 29 04.85 12.48 12.15 11.35     ~ 346 2
35 NGC 4183 GiG 12 13 16.860 +43 41 53.77   13.5       ~ 196 0
36 NGC 4217 GiG 12 15 50.900 +47 05 30.44   12.4       ~ 293 2
37 NGC 4236 GiG 12 16 42.118 +69 27 45.25 10.97 10.58 10.08 9.90   ~ 393 1
38 NGC 4389 GiG 12 25 35.098 +45 41 04.81   12.64   11.46   ~ 146 0
39 M 49 Sy2 12 29 46.8 +08 00 01   13.21 12.17     ~ 2070 2
40 NAME Ursa Major Cluster ClG 15 08.8 +67 07           ~ 409 0

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2023.10.03-21:45:53

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