2008A&A...489.1079P


Query : 2008A&A...489.1079P

2008A&A...489.1079P - Astronomy and Astrophysics, volume 489, 1079-1089 (2008/10-3)

On the Fundamental Plane of the Galactic globular cluster system.

PASQUATO M. and BERTIN G.

Abstract (from CDS):

The globular clusters of our Galaxy have been found to lie close to a plane in the logRe, logσ, SBe space, on the continuation of the Fundamental Plane that is known to characterize the global properties of early-type galaxies. There is no apparent reason why such physically different self-gravitating systems should follow the same scaling law. We reexamine the issue by focusing on a sample of 48 globular clusters selected with homogeneity criteria for the photometric data available from the literature.We perform a model-independent analysis of surface brightness profiles and distance moduli, estimating error bars and studying selection effects with robust non-parametric statistical tests.We determine the values of the coefficients that define the Fundamental Plane and their error bars and show that the scatter from the Fundamental Plane relation is likely to be intrinsic, i.e. not due to measurement errors only. Curiously, we find that in the standard Fundamental Plane coordinates the set of points for our sample occupies a rather slim, axisymmetric, cylindrical region of parameter space, which suggests that the relevant scaling relation might be around a line, rather than a plane, confirming results noted earlier. This is likely to be the origin of the difficulties in the fit by a plane, often mentioned in previous investigations. In addition, such a Fundamental Line relation would imply a pure photometric scaling law relating luminosity to the effective radius which might be tested on wider samples and on extra-galactic globular cluster systems. As to the residuals from the Fundamental Plane relation, we find a correlation of the deviations from the plane with the central slope of the surface brightness profile. No other statistically significant correlations are identified. Finally, given the constraint imposed by the virial theorem, we study the distribution of the values of the quantity KV/(M/L) (virial coefficient divided by the relevant mass-to-light ratio); the distribution of the logarithms, reconstructed through kernel density estimation methods, shows evidence for bimodality, which suggests that the galactic globular cluster system may be composed of at least two dynamically different populations. Yet, these populations do not appear to reflect the standard dichotomy between disk and halo clusters.

Abstract Copyright:

Journal keyword(s): Galaxy: globular clusters: general - Galaxy: structure

Simbad objects: 50

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Number of rows : 50
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 104 GlC 00 24 05.359 -72 04 53.20     4.09     ~ 3917 0
2 NGC 288 GlC 00 52 45.24 -26 34 57.4   10 8.13     ~ 1042 0
3 NGC 362 GlC 01 03 14.26 -70 50 55.6     6.58     ~ 1085 0
4 NGC 1851 GlC 05 14 06.76 -40 02 47.6           ~ 1430 0
5 M 79 GlC 05 24 10.59 -24 31 27.3     8.16     ~ 817 0
6 NGC 2419 GlC 07 38 08.51 +38 52 54.9     10.05     ~ 932 0
7 NGC 2808 GlC 09 12 03.10 -64 51 48.6           ~ 1420 0
8 NGC 3201 GlC 10 17 36.82 -46 24 44.9           ~ 885 0
9 NGC 4147 GlC 12 10 06.149 +18 32 31.78   11.45 10.74     ~ 573 0
10 M 68 GlC 12 39 27.98 -26 44 38.6     7.96     ~ 997 0
11 NGC 5053 GlC 13 16 27.09 +17 42 00.9     9.96     ~ 620 0
12 NAME Centaurus A Sy2 13 25 27.61521044 -43 01 08.8050291   8.18 6.84 6.66   ~ 4486 3
13 NGC 5139 GlC 13 26 47.28 -47 28 46.1           ~ 3427 0
14 M 3 GlC 13 42 11.62 +28 22 38.2     6.39     ~ 2479 0
15 NGC 5286 GlC 13 46 26.81 -51 22 27.3           ~ 443 0
16 NGC 5466 GlC 14 05 27.29 +28 32 04.0     9.70     ~ 828 0
17 NGC 5694 GlC 14 39 36.52 -26 32 18.0           ~ 301 0
18 NGC 5824 GlC 15 03 58.612 -33 04 06.70   10.28 9.56     ~ 408 0
19 M 5 GlC 15 18 33.22 +02 04 51.7     5.95     ~ 1978 0
20 NGC 5946 GlC 15 35 28.58 -50 39 35.0           ~ 194 0
21 M 80 GlC 16 17 02.41 -22 58 33.9           ~ 716 0
22 M 4 GlC 16 23 35.22 -26 31 32.7           ~ 1850 0
23 M 107 GlC 16 32 31.86 -13 03 13.6           ~ 786 0
24 M 13 GlC 16 41 41.634 +36 27 40.75     5.8     ~ 2193 0
25 M 12 GlC 16 47 14.18 -01 56 54.7     6.07     ~ 677 0
26 M 10 GlC 16 57 09.05 -04 06 01.1     4.98     ~ 789 0
27 NGC 6256 GlC 16 59 32.68 -37 07 17.1           ~ 153 0
28 M 62 GlC 17 01 12.60 -30 06 44.5           ~ 620 0
29 NGC 6284 GlC 17 04 28.747 -24 45 51.22   10.72 7.43     ~ 278 0
30 NGC 6293 GlC 17 10 10.42 -26 34 54.2           ~ 281 0
31 M 92 GlC 17 17 07.39 +43 08 09.4     6.52     ~ 2116 0
32 NGC 6325 GlC 17 17 59.27 -23 45 57.7           ~ 171 0
33 NGC 6342 GlC 17 21 10.14 -19 35 14.7     10.01     ~ 286 0
34 NGC 6366 GlC 17 27 44.24 -05 04 47.5           ~ 312 0
35 NGC 6362 GlC 17 31 54.99 -67 02 54.0           ~ 585 0
36 NGC 6388 GlC 17 36 17.461 -44 44 08.34           ~ 914 1
37 NGC 6397 GlC 17 40 42.09 -53 40 27.6     5.17     ~ 1976 0
38 NGC 6441 GlC 17 50 13.06 -37 03 05.2           ~ 884 0
39 NGC 6522 GlC 18 03 34.08 -30 02 02.3           ~ 524 0
40 NGC 6535 GlC 18 03 50.51 -00 17 51.5     9.85     ~ 294 0
41 NGC 6624 GlC 18 23 40.51 -30 21 39.7           ~ 886 1
42 M 70 GlC 18 43 12.76 -32 17 31.6           ~ 386 0
43 NGC 6712 GlC 18 53 04.32 -08 42 21.5           ~ 519 0
44 NGC 6752 GlC 19 10 52.11 -59 59 04.4           ~ 2001 0
45 M 55 GlC 19 39 59.71 -30 57 53.1     6.49     ~ 854 0
46 M 75 GlC 20 06 04.841 -21 55 20.14     8.26     ~ 366 0
47 NGC 6934 GlC 20 34 11.37 +07 24 16.1           ~ 422 0
48 M 15 GlC 21 29 58.33 +12 10 01.2           ~ 3140 0
49 M 2 GlC 21 33 27.02 -00 49 23.7     6.25     ~ 1030 1
50 M 30 GlC 21 40 22.12 -23 10 47.5     7.10     ~ 1049 0

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