ON THE DYNAMICAL AND PHYSICAL STATE OF THE DIFFUSE IONIZED MEDIUM IN NEARBY SPIRAL GALAXIES

Citation
J. Wang et al., ON THE DYNAMICAL AND PHYSICAL STATE OF THE DIFFUSE IONIZED MEDIUM IN NEARBY SPIRAL GALAXIES, The Astrophysical journal, 491(1), 1997, pp. 114
Citations number
55
Journal title
ISSN journal
0004637X
Volume
491
Issue
1
Year of publication
1997
Part
1
Database
ISI
SICI code
0004-637X(1997)491:1<114:OTDAPS>2.0.ZU;2-#
Abstract
We report the initial results from a program to study the morphology, physical state, and kinematics of the ''diffuse ionized medium'' (DIM) in a sample of the nearest and brightest late-type galaxies. For each of five galaxies (NGC 2403, M81, NGC 4395, M51, and M101), we have an alyzed deep narrowband H alpha images of the entire star-forming disk and long-slit spectra of the inner (similar to 10 kpc) disk with a res olution of 40-75 km s(-1). We find that the DIM covers most of the sta r-forming disk and is morphologically related to the presence of high surface brightness gas (the giant H II regions). The DIM and the giant H II regions differ systematically in their physical and dynamical st ate. The DIM is characterized by enhanced emission in the low-ionizati on forbidden lines ([O I], [N II], and [S II]), and even the high-ioni zation [O III] lambda 5007 line is moderately strong in the DIM in at least three cases. This last result contrasts with upper limits on the [O III] surface brightness in the local DIM of our own Galaxy (the '' Reynolds Layer''). We directly verify the inference made by Lehnert an d Heckman that the DIM contributes significantly to the spatially inte grated (global) emission-line ratios measured in late-type galaxies. W e also find that the DIM is more disturbed kinematically than the gas in the giant H II regions. The deconvolved (intrinsic) widths of the H alpha and [N II] lambda 6584 lines range from 30 to 100 km s(-1) (FWH M) in the DIM compared to 20-50 km s(-1) in the giant H II regions. Th e high-ionization gas in the DIM is more kinematically disturbed than the low-ionization gas: the [O III] lambda 5007 lines have intrinsic w idths of 70-150 km s(-1). The differing kinematics implies that the DI M is not a single monolithic phase of the ISM. Instead, it may consist of a ''quiescent'' DIM with a low ionization state and small scale he ight (few hundred parsec) and a ''disturbed'' DIM with a high ionizati on state and moderate scale height (0.5-1 kpc). We argue that the quie scent DIM is most likely photoionized by radiation from O stars leakin g out of giant H II regions (although this requires fine-tuning the op acity of galactic disks to ionizing radiation). The disturbed DIM is m ost likely heated by the mechanical energy supplied by supernovae and stellar winds. Since the disturbed DIM accounts for only a minority (< 20%) of the H alpha emission in the regions we have studied, there is no fundamental energetics problem with this model, but it does require mechanically heated gas to have a high areal covering factor in the i nner disk (which needs to be confirmed observationally). We find no cl ear discontinuity between the physical and dynamical properties of the giant H II regions and the quiescent DIM. The quiescent DIM is morpho logically related to the giant H II regions and there is a smooth depe ndence of the emission-line ratios and emission-line widths on the sur face brightness of the emission. Thus, we suggest that a unified appro ach to the study of the DIM and giant H II regions in star-forming gal axies will prove fruitful.