2005ApJ...621..227M


Query : 2005ApJ...621..227M

2005ApJ...621..227M - Astrophys. J., 621, 227-245 (2005/March-1)

Mapping large-scale gaseous outflows in ultraluminous galaxies with Keck II ESI spectra: variations in outflow velocity with galactic mass.

MARTIN C.L.

Abstract (from CDS):

Measurements of interstellar Na I λλ5890, 5896 absorption lines in 18 ultraluminous infrared galaxies (ULIGs) have been combined with published Na I data, to reassess the dependence of galactic outflow speeds on starburst luminosity and galactic mass. The Doppler shifts reveal outflows of relatively cool gas in 15 of 18 ULIGs with an average outflow speed at the line center of 330±100 km/s. The relation between outflow speed and star formation rate (SFR), defined by the distribution's upper envelope over 4 orders of magnitude in SFR, demonstrates that winds from more luminous starbursts accelerate interstellar gas to higher speeds roughly as v∝SFR0.35. This result is surprising since, in the traditional model for starburst-driven winds, these relatively cool gas clouds are accelerated by the ram pressure of a hot, supernova-heated wind that exhibits weak (if any) X-ray temperature variation with increasing galactic mass. The lack of evidence for much hotter winds is partly a sensitivity issue, but the Na I velocities in ultraluminous starbursts actually are consistent with acceleration by the tepid wind, indicating that a hotter component is unlikely to dominate the momentum flux. The Na I velocities in the dwarf starburst winds do not reach the terminal velocity of a hot wind at the measured temperature of kT∼0.73 keV, a result that could be interpreted simply as evidence that the hot superbubbles are too confined in dwarf starbursts to generate a free-flowing wind. A dynamically motivated scenario, however, is that the dwarf starburst winds simply lack enough momentum to accelerate the clouds to the velocity of the hot wind. Among the subsample of starbursts with well-constrained dynamical masses, the terminal outflow velocities are always found to approach the galactic escape velocity. Motivated by a similar scaling relation for stellar winds, the galactic Eddington luminosity for dusty starbursts is shown to be within the range measured for ULIGs. If radiation pressure on dust grains, coupled to the cool wind, is indeed important for galactic wind dynamics, then feedback is stronger in massive galaxies than previously thought, helping shape the high-mass end of the galaxy luminosity function. Regardless of the nature of the acceleration mechanism in ULIGs, the mass flux of cool gas estimated from these data demonstrates that starburst-driven winds transport significant gas during the assembly stage of field elliptical galaxies, a factor that helps explain the rapid decline in SFR in these systems inferred from elemental abundance ratios.

Abstract Copyright: ∼

Journal keyword(s): Galaxies: Evolution - Galaxies: Formation - Galaxies: Fundamental Parameters - ISM: Evolution - ISM: Kinematics and Dynamics - ISM: Structure

Simbad objects: 29

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Number of rows : 29
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 55 rG 00 14 53.602 -39 11 47.86 8.54 8.58 7.87 7.84   ~ 828 2
2 2MASX J00180398+5511129 G 00 18 03.983 +55 11 12.99           ~ 17 0
3 2MASX J00212652-0839261 LIN 00 21 26.5135306416 -08 39 25.967117268   18.37       ~ 124 1
4 2MASX J00285413+4308149 LIN 00 28 54.132 +43 08 14.91     16.0     ~ 32 0
5 NGC 891 H2G 02 22 32.907 +42 20 53.95 11.08 10.81 9.93 7.86   ~ 1741 2
6 IRAS 03158+4227 AGN 03 19 11.9490689880 +42 38 25.463172912           ~ 67 0
7 2MASX J03191239+4238436 Sy2 03 19 12.3947640576 +42 38 43.501651404           ~ 43 0
8 IRAS 03521+0028 AGN 03 54 42.14640 +00 37 03.3280           ~ 104 0
9 NGC 1569 rG 04 30 49.186 +64 50 52.52 11.72 11.86 11.03     ~ 1297 3
10 LEDA 2816449 Sy2 05 04 36.53952 -19 37 03.1332           ~ 39 1
11 IRAS 08030+5243 rG 08 06 50.8068272808 +52 35 07.225461240           ~ 25 0
12 M 82 AGN 09 55 52.430 +69 40 46.93 9.61 9.30 8.41     ~ 6156 6
13 IRAS 10494+4424 LIN 10 52 23.56560 +44 08 47.4250           ~ 73 0
14 IRAS 10565+2448 LIN 10 59 18.12811 +24 32 34.7357   15.7       ~ 302 0
15 IRAS 11119+3257 Sy1 11 14 38.8902542640 +32 41 33.483258276   19.22 17.96     ~ 165 0
16 IRAS 11506+1331 rG 11 53 14.22000 +13 14 27.6400   17.77       ~ 67 0
17 NGC 4228 SBG 12 15 39.174 +36 19 36.80 10.63 10.30 9.93 9.74   ~ 1017 1
18 NGC 4449 EmG 12 28 11.118 +44 05 36.81 10.11 9.98 9.64 9.45   ~ 1192 1
19 NAME MS 1512-cB58 AGN 15 14 22.2751 +36 36 25.674     20.64   20.35 ~ 326 0
20 FIRST J151422.4+363620 rG 15 14 22.482 +36 36 21.08           ~ 146 1
21 NVSS J152657+100901 rG 15 26 57.469 +10 09 00.31           ~ 17 0
22 LEDA 90237 LIN 16 11 40.4280459768 -01 47 06.566246232   16.6       ~ 95 0
23 IRAS 16487+5447 LIN 16 49 46.9430396033 +54 42 35.317832914   17.5       ~ 68 1
24 LEDA 60189 LIN 17 23 21.96264 -00 17 00.8088   15.1       ~ 454 0
25 IRAS 18368+3549 Sy2 18 38 35.40744 +35 52 19.9884           ~ 40 0
26 NVSS J193222-040000 rG 19 32 22.2962473608 -04 00 01.797249204   18.85   17.04   ~ 122 0
27 NVSS J194815+095203 rG 19 48 15.69984 +09 52 04.5912           ~ 40 0
28 LEDA 90352 LIN 20 11 23.86872 -02 59 50.7588   17.80   16.41   ~ 78 0
29 LEDA 90429 SyG 23 39 01.26960 +36 21 08.5896   16.17       ~ 232 1

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