2010ApJ...716..332S


Query : 2010ApJ...716..332S

2010ApJ...716..332S - Astrophys. J., 716, 332-340 (2010/June-2)

Stellar population gradients in ultraluminous infrared galaxies: implications for gas inflow timescales.

SOTO K.T. and MARTIN C.L.

Abstract (from CDS):

Using longslit, optical spectra of ultraluminous infrared galaxies, we measure the evolution in the star formation intensity during galactic mergers. In individual galaxies, we resolve kiloparsec scales allowing comparison of the nucleus, inner disk, and outer disk. We find that the strength of the Hβ absorption line increases with the projected distance from the center of the merger, typically reaching about 9 Å around 10 kpc. At these radii, the star formation intensity must have rapidly decreased about 300-400 Myr ago; only stellar populations deficient in stars more massive than Type A produce such strong Balmer absorption. In contrast, we find the star formation history in the central kiloparsec consistent with continuous star formation. Our measurements indicate that gas depletion occurs from the outer disk inward during major mergers. This result is consistent with merger-induced gas inflow and empirically constrains the gas inflow timescale. Numerical simulations accurately calculate the total amount of infalling gas but often assume the timescale for infall. These new measurements are therefore central to modeling merger-induced star formation and active galactic nucleus activity.

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Journal keyword(s): galaxies: evolution - galaxies: starburst - galaxies: star formation - galaxies: stellar content

Simbad objects: 26

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Number of rows : 26
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 2MASX J00180398+5511129 G 00 18 03.983 +55 11 12.99           ~ 17 0
2 2MASX J00212652-0839261 LIN 00 21 26.5135306416 -08 39 25.967117268   18.37       ~ 124 1
3 2MASX J00285413+4308149 LIN 00 28 54.132 +43 08 14.91     16.0     ~ 32 0
4 LEDA 89903 AGN 01 32 21.39936 -07 29 08.3112   19.04       ~ 67 0
5 LEDA 75350 Sy1 05 27 16.3183736063 +01 06 00.130727400       17.50   ~ 30 1
6 IRAS 08030+5243 rG 08 06 50.8068272808 +52 35 07.225461240           ~ 25 0
7 NAME IRAS 09111-1007W Sy2 09 13 36.4577885664 -10 19 30.001760292   15.7 16.10     ~ 93 1
8 IRAS 10378+1109 Sy1 10 40 29.1640944744 +10 53 18.202070076   17.79 17.18     ~ 115 1
9 IRAS 10494+4424 LIN 10 52 23.56560 +44 08 47.4250           ~ 73 0
10 IRAS 10565+2448 LIN 10 59 18.12811 +24 32 34.7357   15.7       ~ 302 0
11 LEDA 125693 LIN 11 12 03.37008 -02 54 22.7232   17.45 17.40     ~ 113 1
12 IRAS 11506+1331 rG 11 53 14.22000 +13 14 27.6400   17.77       ~ 67 0
13 NVSS J152657+100901 rG 15 26 57.469 +10 09 00.31           ~ 17 0
14 LEDA 90237 LIN 16 11 40.4280459768 -01 47 06.566246232   16.6       ~ 95 0
15 SDSS J164914.09+342513.1 G 16 49 14.09177 +34 25 13.1998           ~ 55 0
16 IRAS 16474+3430 PaG 16 49 14.20173 +34 25 09.6170           ~ 61 0
17 IRAS 16487+5447 LIN 16 49 46.9430396033 +54 42 35.317832914   17.5       ~ 68 1
18 LEDA 90270 LIN 17 03 41.92968 +58 13 44.5512           ~ 62 0
19 LEDA 60189 LIN 17 23 21.96264 -00 17 00.8088   15.1       ~ 454 0
20 LEDA 90294 G 17 59 52.8 +06 29 18           ~ 16 0
21 IRAS 18368+3549 Sy2 18 38 35.40744 +35 52 19.9884           ~ 40 0
22 LEDA 90308 AGN 18 42 55.56240 +74 36 26.5536           ~ 31 0
23 LEDA 90350 Sy1 20 07 18.669 -06 14 27.32   17.24   16.18   ~ 23 1
24 LEDA 90352 LIN 20 11 23.86872 -02 59 50.7588   17.80   16.41   ~ 78 0
25 2MASS J23351192+2930002 LIN 23 35 11.92032 +29 30 00.2124           ~ 56 0
26 LEDA 90429 SyG 23 39 01.26960 +36 21 08.5896   16.17       ~ 232 1

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