2013A&A...557A.131M


Query : 2013A&A...557A.131M

2013A&A...557A.131M - Astronomy and Astrophysics, volume 557A, 131-131 (2013/9-1)

The DiskMass Survey. VII. The distribution of luminous and dark matter in spiral galaxies.

MARTINSSON T.P.K., VERHEIJEN M.A.W., WESTFALL K.B., BERSHADY M.A., ANDERSEN D.R. and SWATERS R.A.

Abstract (from CDS):

We present dynamically-determined rotation-curve mass decompositions of 30 spiral galaxies, which were carried out to test the maximum-disk hypothesis and to quantify properties of their dark-matter halos. We used measured vertical velocity dispersions of the disk stars to calculate dynamical mass surface densities (Σdyn). By subtracting our observed atomic and inferred molecular gas mass surface densities from Σdyn, we derived the stellar mass surface densities (Σ*), and thus have absolute measurements of all dominant baryonic components of the galaxies. Using K-band surface brightness profiles (IK), we calculated the K-band mass-to-light ratio of the stellar disks (Υ**/IK) and adopted the radial mean (<Υ*>) for each galaxy to extrapolate Σ* beyond the outermost kinematic measurement. The derived <Υ*> of individual galaxies are consistent with all galaxies in the sample having equal Υ*. We find a sample average and scatter of <Υ*≥0.31 ±0.07. Rotation curves of the baryonic components were calculated from their deprojected mass surface densities. These were used with circular-speed measurements to derive the structural parameters of the dark-matter halos, modeled as either a pseudo-isothermal sphere (pISO) or a Navarro-Frenk-White (NFW) halo. In addition to our dynamically determined mass decompositions, we also performed alternative rotation-curve decompositions by adopting the traditional maximum-disk hypothesis. However, the galaxies in our sample are submaximal, such that at 2.2 disk scale lengths (hR) the ratios between the baryonic and total rotation curves (Fb2.2hR) are less than 0.75. We find this ratio to be nearly constant between 1-6hR within individual galaxies. We find a sample average and scatter of <Fb2.2hR≥0.57±0.07, with trends of larger Fb2.2hR for more luminous and higher-surface-brightness galaxies. To enforce these being maximal, we need to scale Υ* by a factor 3.6 on average. In general, the dark-matter rotation curves are marginally better fit by a pISO than by an NFW halo. For the nominal-Υ* (submaximal) case, we find that the derived NFW-halo parameters have values consistent with ΛCDM N-body simulations, suggesting that the baryonic matter in our sample of galaxies has only had a minor effect on the dark-matter distribution. In contrast, maximum-Υ* decompositions yield halo-concentration parameters that are too low compared to the ΛCDM simulations.

Abstract Copyright:

Journal keyword(s): techniques: imaging spectroscopy - galaxies: spiral - galaxies: structure - galaxies: kinematics and dynamics - galaxies: fundamental parameters

Simbad objects: 33

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Number of rows : 33
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 IC 43 GiG 00 42 22.065 +29 38 29.81   14.4       ~ 72 0
2 M 31 G 00 42 44.330 +41 16 07.50 4.86 4.36 3.44     ~ 12164 1
3 NGC 234 EmG 00 43 32.3817530400 +14 20 33.397671804   13.5       ~ 117 0
4 NGC 575 G 01 30 46.6479600768 +21 26 25.538745840   13.65 13.02 12.51 11.81 ~ 62 0
5 UGC 1087 LSB 01 31 26.634 +14 16 38.99   15.1       ~ 71 0
6 M 33 GiG 01 33 50.8965749232 +30 39 36.630403128 6.17 6.27 5.72     ~ 5634 1
7 IC 193 G 02 02 31.0015834896 +11 05 34.843944156   14.70       ~ 47 0
8 IC 208 GiP 02 08 27.736 +06 23 41.53   14.8       ~ 67 0
9 UGC 1862 LSB 02 24 24.7899528672 -02 09 44.324915904   13.4   13.4 13.3 ~ 70 0
10 NGC 927 G 02 26 37.2835891560 +12 09 18.739894248   14.5       ~ 48 0
11 Z 393-38 G 04 33 56.142 +01 06 49.73   15.4       ~ 24 1
12 NGC 1642 G 04 42 54.9218742384 +00 37 06.970318968   12.9   12.6 12.8 ~ 64 0
13 UGC 3701 GiG 07 11 42.691 +72 10 09.14   15.2       ~ 38 0
14 UGC 3997 LSB 07 44 38.7438929880 +40 21 58.944211344   16.0       ~ 35 1
15 NGC 2441 GiG 07 51 54.6864254040 +73 00 56.553791256   12.7       ~ 97 0
16 UGC 4107 EmG 07 57 01.8519816768 +49 34 02.360995104   13.90       ~ 106 0
17 NGC 2532 G 08 10 15.1864372560 +33 57 23.768999208   12.90       ~ 157 0
18 NGC 2575 GiG 08 22 44.9549844864 +24 17 48.999119856   14.3       ~ 76 0
19 UGC 4380 G 08 24 31.8638980200 +54 51 13.997538468   15.1       ~ 36 0
20 NGC 2599 Q? 08 32 11.3215409472 +22 33 38.005300296   13.4       ~ 109 1
21 NGC 2649 G 08 44 08.2654636584 +34 43 02.218776276   13.10       ~ 79 0
22 UGC 4622 G 08 50 20.1917726256 +41 17 21.916681620   15.3       ~ 30 0
23 UGC 6903 EmG 11 55 36.866 +01 14 14.43   13.623 13.011 12.508 11.890 ~ 106 0
24 NGC 3982 Sy1 11 56 28.1445516072 +55 07 30.859586652   12.20 11.70 11.18   ~ 524 1
25 NGC 4195 LSB 12 14 18.054 +59 36 55.06   15.5       ~ 32 0
26 NGC 4662 SyG 12 44 26.1944883144 +37 07 16.360496112   14.10       ~ 76 0
27 NGC 4977 LIN 13 06 04.4476519368 +55 39 21.720847932   14.5       ~ 37 0
28 UGC 9177 GiG 14 20 30.4898570136 +10 25 55.520547240   14.9       ~ 28 0
29 NAME Ursa Major Cluster ClG 15 08.8 +67 07           ~ 407 0
30 UGC 9837 LSB 15 23 51.735 +58 03 11.23   14.6       ~ 73 0
31 IC 1132 GiG 15 40 06.7557453288 +20 40 50.086879464   14.4       ~ 66 0
32 NGC 6691 G 18 39 12.2418567600 +55 38 30.376882104   14.1       ~ 36 0
33 NGC 7495 G 23 08 57.1757147664 +12 02 52.868867964   14.7       ~ 79 0

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2023.03.22-20:01:31

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