2000ApJ...530..213H


Query : 2000ApJ...530..213H

2000ApJ...530..213H - Astrophys. J., 530, 213-221 (2000/February-2)

X-ray emission from rotating elliptical galaxies.

HANLAN P.C. and BREGMAN J.N.

Abstract (from CDS):

The slow inward flow of the hot gas in elliptical galaxy cooling flows is nearly impossible to detect directly because of instrumental limitations. However, in rotating galaxies, if the inflowing gas conserves angular momentum, it will eventually form a disk. The X-ray signature of this phenomenon is a flattening of the X-ray isophotes in the inner 1-10 kpc region. This effect is observable, so we have searched for it in X-ray observations of six rotating and nonrotating early-type galaxies, obtained mainly with the ROSAT PSPC and HRI imagers. The ellipticities of the X-ray emission never increase toward the central region, nor are the X-ray ellipticities significantly greater than the ellipticities for the optical stellar emission. Central ellipticities in excess of 0.5 were expected in rotating ellipticals, whereas values of 0-0.2 are measured. The failure to detect the expected signature requires a modification to the standard cooling-flow picture, possibly including partial galactic winds, rapid mass dropout, or turbulent redistribution of angular momentum.

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Journal keyword(s): galaxies: individual (NGC 1395, NGC 1404) - Galaxies: Kinematics and Dynamics - Galaxies: ISM - X-Rays: Galaxies

Simbad objects: 7

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Number of rows : 7
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 NGC 1399 rG 03 38 29.083 -35 27 02.67 11.05 9.74 9.59 8.12   ~ 1636 1
2 NGC 1395 SyG 03 38 29.789 -23 01 39.69   10.71   8.99   ~ 289 0
3 NGC 1404 rG 03 38 51.917 -35 35 39.81 11.53 10.69 10.00 9.03   ~ 787 1
4 M 84 Sy2 12 25 03.74333 +12 53 13.1393 12.67 12.09 10.49     ~ 1841 2
5 M 49 Sy2 12 29 46.8 +08 00 01   13.21 12.17     ~ 2174 2
6 M 89 Sy2 12 35 39.80733343 +12 33 22.8308657 11.29 10.73 9.75     ~ 1037 2
7 NGC 5322 SyG 13 49 15.24 +60 11 25.8   11.3       ~ 432 2

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