Direct Far-infrared Metal Abundances (FIRA). I. M101
Direct Far-infrared Metal Abundances (FIRA). I. M101
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DOI:
10.3847/1538-4357/ac3b4f
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发表时间:
2021-11
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影响因子:
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通讯作者:
C. Lamarche;J. Smith;K. Kreckel;S. Linden;N. Rogers;E. Skillman;D. Berg;E. Murphy;R. Pogge;G. P. Donnelly;R. Kennicutt;A. Bolatto;K. Croxall;B. Groves;C. Ferkinhoff
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作者:
C. Lamarche;J. Smith;K. Kreckel;S. Linden;N. Rogers;E. Skillman;D. Berg;E. Murphy;R. Pogge;G. P. Donnelly;R. Kennicutt;A. Bolatto;K. Croxall;B. Groves;C. Ferkinhoff
Accurately determining gas-phase metal abundances within galaxies is critical as metals strongly affect the physics of the interstellar medium. To date, the vast majority of widely used gas-phase abundance indicators rely on emission from bright optical lines, whose emissivities are highly sensitive to the electron temperature. Alternatively, direct-abundance methods exist that measure the temperature of the emitting gas directly, though these methods usually require challenging observations of highly excited auroral lines. Low-lying far-infrared (FIR) fine structure lines are largely insensitive to electron temperature and thus provide an attractive alternative to optically derived abundances. Here, we introduce the far-infrared abundance (FIRA) project, which employs these FIR transitions, together with both radio free–free emission and hydrogen recombination lines, to derive direct, absolute gas-phase oxygen abundances. Our first target is M101, a nearby spiral galaxy with a relatively steep abundance gradient. Our results are consistent with the O++ electron temperatures and absolute oxygen abundances derived using optical direct-abundance methods by the CHemical Abundance Of Spirals (CHAOS) program, with a small difference (∼1.5σ) in the radial abundance gradients derived by the FIR/free–free-normalized versus CHAOS/direct-abundance techniques. This initial result demonstrates the validity of the FIRA methodology—with the promise of determining absolute metal abundances within dusty star-forming galaxies, both locally and at high redshift.