2025ApJ...993..117T


Query : 2025ApJ...993..117T

2025ApJ...993..117T - Astrophys. J., 993, 117 (2025/November-1)

The Significant Contribution of Supersoft X-Ray Sources to Nebular He II Line Emission.

TRIANI D.P., DI STEFANO R., HSIAO T.Y.-Y. and KEWLEY L.J.

Abstract (from CDS):

Nebular spectral lines provide insight into the properties of the interstellar medium and the ionizing radiation within galaxies. The presence of high-energy ionization lines such as He II indicates the existence of ionizing photons with energies exceeding the second ionization energy of helium (54 eV). There is an enigma surrounding the origin of these lines observed in star-forming galaxies because stellar ionization cannot account for such high energy emission. This paper proposes that supersoft X-ray sources (SSSs) may produce the He II ionization lines in star-forming galaxies. We model the spectra of SSSs using blackbody radiation and add them to the young stellar population spectra to represent the overall spectra of galaxies. Using a photoionization model, we predict the resulting He IIλ4686 and Hβ line fluxes and inspect the contribution of SSSs to the elevation of the He IIλ4686 /Hβ ratio in star-forming galaxies, both at low and high redshifts. We find that incorporating a blackbody with temperatures between kT = 10-100 eV can boost the He IIλ4686 /Hβ line ratio to the levels observed in local galaxies by SDSS and in early galaxies by NIRSpec. This blackbody temperature range aligns with the observed temperatures of SSSs. The number of SSSs in spiral galaxies listed in Chandra catalogs, and our estimates of the total population, confirms that SSSs are promising candidates for the source of the He II ionization.

Abstract Copyright: © 2025. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Emission line galaxies - Galaxy spectroscopy - X-ray astronomy - High-redshift galaxies

Simbad objects: 27

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Number of rows : 27
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 IC 10 rG 00 20 17.33520 +59 18 13.6480   13.6 9.5     ~ 1185 1
2 M 31 AGN 00 42 44.330 +41 16 07.50 4.86 4.36 3.44     ~ 13622 1
3 M 33 GiG 01 33 50.8965749232 +30 39 36.630403128 6.17 6.27 5.72     ~ 6226 1
4 NAME Magellanic Clouds GrG 03 00 -71.0           ~ 7988 0
5 JADES-GS+053.12176-27.79763 EmG 03 32 29.21 -27 47 51.2   29.613 29.883     ~ 41 0
6 JADES-GS+053.12259-27.76057 EmG 03 32 29.4096 -27 45 37.800           ~ 16 0
7 JADES-GS+053.17655-27.77111 EmG 03 32 42.367 -27 46 15.73           ~ 22 0
8 JADES-GS+053.17915-27.80147 EmG 03 32 42.9974 -27 48 05.299           ~ 2 0
9 V* KT Eri No* 04 47 54.2014586736 -10 10 42.962267424   14.986 14.705 15.099   ~ 161 0
10 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
11 2E 1550 XB* 05 43 34.1600044704 -68 22 22.191505716   15.9   17.2 16.54 ~ 332 0
12 Mrk 116 AGN 09 34 02.1 +55 14 25           ~ 1179 1
13 M 81 Sy2 09 55 33.1726556496 +69 03 55.062505368   7.89 6.94     ~ 4725 3
14 NGC 3115 GiG 10 05 13.9270507008 -07 43 06.982712292   11   9.37   ~ 1067 2
15 M 105 LIN 10 47 49.600 +12 34 53.87   10.56 9.76 9.12 8.18 ~ 1504 0
16 NGC 4278 LIN 12 20 06.8242 +29 16 50.722 11.54 11.09 10.16     ~ 988 2
17 NGC 4697 GiG 12 48 35.8981498824 -05 48 02.482374564   10.97   9.83   ~ 895 0
18 NAME Centaurus A BLL 13 25 27.61521044 -43 01 08.8050291   8.18 6.84 6.66   ~ 4774 3
19 M 51 Sy2 13 29 52.698 +47 11 42.93   9.26 8.36 8.40   ~ 4565 4
20 M 83 SBG 13 37 00.91920 -29 51 56.7400 8.85 8.11 7.52 7.21   ~ 2778 2
21 M 101 GiP 14 03 12.583 +54 20 55.50   8.46 7.86 7.76   ~ 3138 2
22 [ADF2023] CEERS MSA 355 EmG 14 19 13.5557 +52 52 43.777           ~ 8 0
23 CANDELS EGS F160W J142037.5+530335.6 EmG 14 20 37.503 +53 03 35.64           ~ 4 0
24 V* RS Oph Sy* 17 50 13.1591484960 -06 42 28.480729788   11.884 10.776 11.228   K5.5/M0IIIe 1163 0
25 V* V4743 Sgr No* 19 01 09.3393890856 -22 00 06.016418064           ~ 159 0
26 V* V2491 Cyg CV* 19 43 01.9771342416 +32 19 13.549047276 18.27 18.72 18.03 17.72 17.41 ~ 174 0
27 NAME Local Group GrG ~ ~           ~ 9325 0

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