2001A&A...375..566N


Query : 2001A&A...375..566N

2001A&A...375..566N - Astronomy and Astrophysics, volume 375566-578 (2001/8-4)

Global physical conditions of the interstellar medium in nearby galaxies.

NEGISHI T., ONAKA T., CHAN K.-W. and ROELLIG T.L.

Abstract (from CDS):

Far-infrared spectra (43-197µm) of 34 nearby galaxies obtained by the Long Wavelength Spectrometer (LWS) aboard the Infrared Space Observatory (ISO) were analyzed to investigate the general properties of interstellar matter in galaxies. The present sample includes not only normal galaxies but also starbursts and active galactic nuclei (AGNs). Far-infrared forbidden lines, such as [CII]158µm, [OI]63µm, [NII]122µm, and [OIII]88µm, were detected in most of the sample galaxies. [OI]145µm line was detected in 13 galaxies. The line fluxes of [CII]158µm and [NII]122µm relative to the total far-infrared flux (FIR) decrease as the far-infrared color becomes bluer, while the ratio of the [OI]63µm flux to FIR does not show a systematic trend with the color. The [OIII]88µm to FIR ratio shows a large scatter with a weak trend of increase with the color. AGNs do not show any distinguishable trend from normal and starburst galaxies in the far-infrared spectra, suggesting that the far-infrared emission is mainly driven by star-formation activities even in AGNs. We estimate the physical conditions of photodissociation regions (PDRs) in the sample galaxies, such as the far-ultraviolet radiation field intensity G0 and the gas density n by assuming that all the observed [OI]63µm and far-infrared continuum emissions come from PDRs. Comparison with PDR models indicates that G0 ranges from 102-104 and n∼102-104cm–3. The present results also suggest that n varies proportionally with G0. The ratio of [CII]158µm to CO (J=1-0) line emission supports the linear increase in n with G0. We estimate that about a half of [CII]158µm emission originates from PDRs and attribute the rest to the emission as coming from low-density diffuse ionized gas. The estimated intensity of [CII]158µm from the ionized gas is compatible with the observed intensity of [NII]122µm if both lines come from the same diffuse ionized gas. The present analysis suggests that the decrease in [CII]158µm/FIR with the far-infrared color may not be accounted for by the decrease in the photoelectric heating efficiency owing to the increase in positive charges of dust grains because a measure of the efficiency, G0/n, is found to stay constant with the far-infrared color. Instead the decrease can be interpreted in terms of either the increase in the collisional de-excitation of the [CII] transition due to the increase in the gas density or the decrease in the ionized component relative to the far-infrared intensity suggested by the decrease in [NII]122µm/FIR. Based on the present analysis, we derive average relations of the far-infrared color with G0 and n in galaxies, which can be applied to the investigation of interstellar matter in distant galaxies.

Abstract Copyright: ∼

Journal keyword(s): galaxies: ISM - infrared: ISM - lines and bands: ISM - radiation mechanisms: thermal

Simbad objects: 40

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Number of rows : 40
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 253 SyG 00 47 33.134 -25 17 19.68   8.03   6.94 8.1 ~ 3588 2
2 MCG+12-02-001 AG? 00 54 03.943 +73 05 05.23   16       ~ 120 1
3 NGC 520 AGN 01 24 35.07120 +03 47 32.6760 12.41 12.24 11.42     ~ 528 3
4 NGC 891 H2G 02 22 32.907 +42 20 53.95 11.08 10.81 9.93 7.86   ~ 1741 2
5 UGCA 39 GiG 02 41 55.092 +59 36 14.73   16       ~ 360 1
6 M 77 Sy2 02 42 40.7091669408 -00 00 47.859690204 9.70 9.61 8.87 10.1 9.9 ~ 4897 2
7 NGC 1097 LIN 02 46 19.059 -30 16 29.68 10.46 9.97 9.48 8.72 9.8 ~ 1448 3
8 NGC 1365 Sy1 03 33 36.458 -36 08 26.37 10.48 10.08 9.63 8.79 9.7 ~ 1987 2
9 NGC 2146 AGN 06 18 37.710 +78 21 25.27 11.67 11.38 10.59     ~ 765 2
10 M 82 AGN 09 55 52.430 +69 40 46.93 9.61 9.30 8.41     ~ 6156 6
11 IC 2554 AG? 10 08 50.563 -67 01 51.07   12.43 13.20 11.24 11.9 ~ 66 0
12 NGC 3256 Sy2 10 27 51.284 -43 54 13.55   11.83 11.33 10.62 11.9 ~ 920 2
13 NGC 3690 IG 11 28 31.0 +58 33 41   13.19 12.86     ~ 1015 4
14 NGC 3690B GiP 11 28 31.02 +58 33 40.7   11.8       ~ 635 4
15 NGC 3690NE AGN 11 28 33.07 +58 33 54.2   11.8       ~ 635 4
16 NGC 4038 EmG 12 01 53.002 -18 52 03.32   10.91   9.74 11.0 ~ 1364 1
17 NAME Antennae IG 12 01 53.170 -18 52 37.92           ~ 1749 0
18 NGC 4039 GiP 12 01 53.51 -18 53 10.3   11.08   9.77   ~ 1173 1
19 NGC 4041 SyG 12 02 12.2376697152 +62 08 14.096124312   11.6       ~ 270 1
20 NGC 4414 GiC 12 26 27.1276893168 +31 13 24.626206488 11.12 10.96 10.12     ~ 593 2
21 NGC 4945 Sy2 13 05 27.279 -49 28 04.44   9.31 14.40 7.55   ~ 1582 2
22 NAME Centaurus A BLL 13 25 27.61521044 -43 01 08.8050291   8.18 6.84 6.66   ~ 4774 3
23 ESO 173-15 AGN 13 27 23.774 -57 29 22.14   14.9   14.3 13.7 ~ 81 1
24 M 51 Sy2 13 29 52.698 +47 11 42.93   9.26 8.36 8.40   ~ 4565 4
25 M 83 SBG 13 37 00.91920 -29 51 56.7400 8.85 8.11 7.52 7.21   ~ 2778 2
26 NGC 5430 AGN 14 00 45.820 +59 19 43.14   12.7       ~ 261 1
27 NAME Circinus Galaxy Sy2 14 13 09.906 -65 20 20.47   10.89 9.84 10.6 10.0 ~ 1331 1
28 NGC 5713 GiG 14 40 11.528 -00 17 21.16 11.88 11.84 11.20     ~ 421 2
29 NGC 5937 Sy2 15 30 46.1177972544 -02 49 46.042511232   13.1       ~ 96 1
30 NGC 6156 AGN 16 34 52.5448490040 -60 37 07.867951500   12.30   11.05 12.0 ~ 85 0
31 NGC 6240 Sy2 16 52 58.9 +02 24 03   14.31 13.37     ~ 1734 2
32 NGC 6764 LIN 19 08 16.4036066688 +50 55 59.519979084   15.00 14.32     ~ 307 1
33 NGC 6810 Sy2 19 43 34.4178888528 -58 39 20.192400540   12.34 11.22 10.71   ~ 163 1
34 NGC 6824 GiG 19 43 40.7700366600 +56 06 34.012787400   13.1       ~ 72 1
35 NGC 6946 H2G 20 34 52.332 +60 09 13.24   10.5       ~ 2661 2
36 NGC 7469 Sy1 23 03 15.6 +08 52 26 12.60 13.00 12.34     ~ 2253 3
37 NGC 7552 Sy1 23 16 10.66 -42 35 04.7 11.34 11.22 10.57 10.08 11.1 ~ 574 3
38 NGC 7582 Sy2 23 18 23.60 -42 22 13.3 11.62 10.92 10.62     ~ 978 3
39 NGC 7714 AGN 23 36 14.1257730600 +02 09 18.197422668   14.91 14.36     ~ 788 1
40 APG 284 PaG 23 36 19 +02 09.3   12.6       ~ 608 0

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