Matches in SemOpenAlex for { <https://semopenalex.org/work/W4288604611> ?p ?o ?g. }
- W4288604611 endingPage "A115" @default.
- W4288604611 startingPage "A115" @default.
- W4288604611 abstract "Context. The diffuse ionized gas (DIG) constitutes the largest fraction of the total ionized interstellar matter in star-forming galaxies, but it is still unclear whether the ionization is driven predominantly by the ionizing radiation of hot massive stars, as in H II regions, or whether additional sources of ionization have to be considered. Key to understanding the ionization mechanisms in the DIG is the line emission by the ionized gas. Aims. We systematically explore a plausible subset of the parameter space involving effective temperatures and metallicities of the ionizing sources, the effects of the hardening of their radiation by surrounding “leaky” H II regions with different escape fractions, as well as different scenarios for the clumpiness of the DIG, and compute the resulting line strength ratios for a number of diagnostic optical emission lines. Methods. For the ionizing fluxes we computed a grid of stellar spectral energy distributions (SEDs) from detailed, fully non-LTE model atmospheres that include the effects of stellar winds and line blocking and blanketing. To calculate the ionization and temperature structure in the interstellar gas we used spherically symmetric photoionization models and state-of-the-art three-dimensional (3D) non-LTE radiative transfer simulations, considering hydrogen, helium, and the most abundant metals. We first applied these methods to classical H II regions around hot stars, using the model SEDs at different metallicities and effective temperatures as ionizing fluxes, and compute the SEDs of the escaping radiation for different escape fractions of hydrogen-ionizing photons. In a second step, we studied the effects of the escaping radiation on the more dilute and extended DIG. Using 3D models simulating a section of a galactic spiral arm, we computed the ionization structure in the DIG for different scenarios for the inhomogeneity of the gas, assuming ionization by a stellar population SED based on plausible parameters. Results. We provide quantitative predictions of how the line ratios from H II regions and the DIG vary as a function of metallicity Z , stellar effective temperature T eff , and escape fraction f esc from the H II region. The range of predicted line ratios reinforces the hypothesis that the DIG is ionized by (filtered) radiation from hot stars. At one-tenth solar metallicity, radiation hardening is mostly due to hydrogen and helium, whereas at solar metallicity absorption by metals plays a significant role. The effects of hardening are seen primarily in the increase in the emission line ratios of the most important cooling lines of the gas, [N II ]∕H β and [O II ]∕H β at lower T eff , and [O III ]∕H β at higher T eff . For low T eff nearly the entire He I -ionizing radiation is absorbed in the H II regions, thereby preventing the formation of high ionization stages such as O III in the DIG. The ionization structure of the DIG depends strongly on both the clumping factor f cl = 〈 n H 2 〉/〈 n H 2 〉 and the large-scale distribution of the gas. In our simulations about 10% of the ionizing radiation produced by hot massive stars in a spiral arm is sufficient to ionize the DIG up to a height of approximately 1 kpc above the galactic plane for a clumping factor close to the observed value of f cl ~ 5. Even small changes in simulation parameters such as the clumping factor can lead to considerable variation in the ionized volume. Both for a more homogeneous gas and a very inhomogeneous gas containing both dense clumps and channels with low gas density, the ionized region in the dilute gas above the galactic plane can cease to be radiation-bounded, allowing the ionizing radiation to leak into the intergalactic medium. Comparison of observed and predicted line ratios indicates that the DIG is typically ionized with a softer SED than predicted by the chosen stellar population synthesis model." @default.
- W4288604611 created "2022-07-29" @default.
- W4288604611 creator A5004573874 @default.
- W4288604611 creator A5025011905 @default.
- W4288604611 creator A5058123078 @default.
- W4288604611 date "2019-02-01" @default.
- W4288604611 modified "2023-09-27" @default.
- W4288604611 title "Numerical models for the diffuse ionized gas in galaxies" @default.
- W4288604611 cites W1494951942 @default.
- W4288604611 cites W1919467155 @default.
- W4288604611 cites W1967653150 @default.
- W4288604611 cites W1973120086 @default.
- W4288604611 cites W1976579441 @default.
- W4288604611 cites W1979905105 @default.
- W4288604611 cites W1985704664 @default.
- W4288604611 cites W1990541644 @default.
- W4288604611 cites W1997392048 @default.
- W4288604611 cites W2001866435 @default.
- W4288604611 cites W2002433778 @default.
- W4288604611 cites W2003862060 @default.
- W4288604611 cites W2005396945 @default.
- W4288604611 cites W2014783219 @default.
- W4288604611 cites W2016178688 @default.
- W4288604611 cites W2031804266 @default.
- W4288604611 cites W2036551560 @default.
- W4288604611 cites W2050607988 @default.
- W4288604611 cites W2053634873 @default.
- W4288604611 cites W2058304907 @default.
- W4288604611 cites W2059063248 @default.
- W4288604611 cites W2062581825 @default.
- W4288604611 cites W2073811527 @default.
- W4288604611 cites W2081087406 @default.
- W4288604611 cites W2085066178 @default.
- W4288604611 cites W2092266092 @default.
- W4288604611 cites W2100696415 @default.
- W4288604611 cites W2102473635 @default.
- W4288604611 cites W2110197253 @default.
- W4288604611 cites W2118813009 @default.
- W4288604611 cites W2120734553 @default.
- W4288604611 cites W2120900521 @default.
- W4288604611 cites W2140981611 @default.
- W4288604611 cites W2148492013 @default.
- W4288604611 cites W2156522191 @default.
- W4288604611 cites W2167208233 @default.
- W4288604611 cites W2315759414 @default.
- W4288604611 cites W2394881825 @default.
- W4288604611 cites W2770514005 @default.
- W4288604611 cites W2899497983 @default.
- W4288604611 cites W3016417574 @default.
- W4288604611 cites W3047437146 @default.
- W4288604611 cites W3098808441 @default.
- W4288604611 cites W3099601021 @default.
- W4288604611 cites W3100064752 @default.
- W4288604611 cites W3100265020 @default.
- W4288604611 cites W3102983568 @default.
- W4288604611 cites W3104016316 @default.
- W4288604611 cites W3104416848 @default.
- W4288604611 cites W3105344255 @default.
- W4288604611 cites W3106164503 @default.
- W4288604611 cites W3123968462 @default.
- W4288604611 cites W4236154090 @default.
- W4288604611 cites W4292371990 @default.
- W4288604611 cites W4292508300 @default.
- W4288604611 cites W4299293013 @default.
- W4288604611 cites W4299582879 @default.
- W4288604611 cites W4299788627 @default.
- W4288604611 cites W4301256123 @default.
- W4288604611 cites W4302049122 @default.
- W4288604611 cites W51916193 @default.
- W4288604611 doi "https://doi.org/10.1051/0004-6361/201832649" @default.
- W4288604611 hasPublicationYear "2019" @default.
- W4288604611 type Work @default.
- W4288604611 citedByCount "10" @default.
- W4288604611 countsByYear W42886046112019 @default.
- W4288604611 countsByYear W42886046112020 @default.
- W4288604611 countsByYear W42886046112021 @default.
- W4288604611 countsByYear W42886046112022 @default.
- W4288604611 crossrefType "journal-article" @default.
- W4288604611 hasAuthorship W4288604611A5004573874 @default.
- W4288604611 hasAuthorship W4288604611A5025011905 @default.
- W4288604611 hasAuthorship W4288604611A5058123078 @default.
- W4288604611 hasBestOaLocation W42886046111 @default.
- W4288604611 hasConcept C111337013 @default.
- W4288604611 hasConcept C121332964 @default.
- W4288604611 hasConcept C145148216 @default.
- W4288604611 hasConcept C150846664 @default.
- W4288604611 hasConcept C158749347 @default.
- W4288604611 hasConcept C18231593 @default.
- W4288604611 hasConcept C185544564 @default.
- W4288604611 hasConcept C196939603 @default.
- W4288604611 hasConcept C198291218 @default.
- W4288604611 hasConcept C44870925 @default.
- W4288604611 hasConcept C62520636 @default.
- W4288604611 hasConcept C74902906 @default.
- W4288604611 hasConcept C98444146 @default.
- W4288604611 hasConceptScore W4288604611C111337013 @default.
- W4288604611 hasConceptScore W4288604611C121332964 @default.
- W4288604611 hasConceptScore W4288604611C145148216 @default.