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Temperature inhomogeneities cause the abundance discrepancy in H II regions.

Authors :
Méndez-Delgado JE
Esteban C
García-Rojas J
Kreckel K
Peimbert M
Source :
Nature [Nature] 2023 Jun; Vol. 618 (7964), pp. 249-251. Date of Electronic Publication: 2023 May 17.
Publication Year :
2023

Abstract

H II regions are ionized nebulae surrounding massive stars. They exhibit a wealth of emission lines that form the basis for estimation of chemical composition. Heavy elements regulate the cooling of interstellar gas, and are essential to the understanding of several phenomena such as nucleosynthesis, star formation and chemical evolution <superscript>1,2</superscript> . For over 80 years <superscript>3</superscript> , however, a discrepancy exists of a factor of around two between heavy-element abundances derived from collisionally excited lines and those from the weaker recombination lines, which has thrown our absolute abundance determinations into doubt <superscript>4,5</superscript> . Here we report observational evidence that there are temperature inhomogeneities within the gas, quantified by t <superscript>2 </superscript> (ref. <superscript>6</superscript> ). These inhomogeneities affect only highly ionized gas and cause the abundance discrepancy problem. Metallicity determinations based on collisionally excited lines must be revised because these may be severely underestimated, especially in regions of lower metallicity such as those recently observed with the James Webb Space Telescope in high-z galaxies <superscript>7-9</superscript> . We present new empirical relations for estimation of temperature and metallicity, critical for a robust interpretation of the chemical composition of the Universe over cosmic time.<br /> (© 2023. The Author(s), under exclusive licence to Springer Nature Limited.)

Details

Language :
English
ISSN :
1476-4687
Volume :
618
Issue :
7964
Database :
MEDLINE
Journal :
Nature
Publication Type :
Academic Journal
Accession number :
37198488
Full Text :
https://doi.org/10.1038/s41586-023-05956-2