2022ApJ...930..135L


Query : 2022ApJ...930..135L

2022ApJ...930..135L - Astrophys. J., 930, 135-135 (2022/May-2)

Elevated Hot Gas and High-mass X-Ray Binary Emission in Low-metallicity Galaxies: Implications for Nebular Ionization and Intergalactic Medium Heating in the Early Universe.

LEHMER B.D., EUFRASIO R.T., BASU-ZYCH A., GAROFALI K., GILBERTSON W., MESINGER A. and YUKITA M.

Abstract (from CDS):

High-energy emission associated with star formation has been proposed as a significant source of interstellar medium (ISM) ionization in low-metallicity starbursts and an important contributor to the heating of the intergalactic medium (IGM) in the high-redshift (z >= 8) universe. Using Chandra observations of a sample of 30 galaxies at D ≃ 200-450 Mpc that have high specific star formation rates of 3-9 Gyr–1 and metallicities near Z ≃ 0.3Z☉, we provide new measurements of the average 0.5-8 keV spectral shape and normalization per unit star formation rate (SFR). We model the sample-combined X-ray spectrum as a combination of hot gas and high-mass X-ray binary (HMXB) populations and constrain their relative contributions. We derive scaling relations of \mathrm{log}{L}_{0.5\mbox{--}8\ \mathrm{keV}}^{\mathrm{HMXB}}/SFR = 40.19 ± 0.06 and \mathrm{log}{L}_{0.5\mbox{--}2\ \mathrm{keV}}^{\mathrm{gas}}/SFR =\,{39.58}_{-0.28}^{+0.17}; significantly elevated compared to local relations. The HMXB scaling is also somewhat higher than {L}_{0.5\mbox{--}8\ \mathrm{keV}}^{\mathrm{HMXB}}-SFR-Z relations presented in the literature, potentially due to our galaxies having relatively low HMXB obscuration and young and X-ray luminous stellar populations. The elevation of the hot gas scaling relation is at the level expected for diminished attenuation due to a reduction of metals; however, we cannot conclude that an {L}_{0.5\mbox{--}2\ \mathrm{keV}}^{\mathrm{gas}}-SFR-Z relation is driven solely by changes in ISM metal content. Finally, we present SFR-scaled spectral models (both emergent and intrinsic) that span the X-ray-to-IR band, providing new benchmarks for studies of the impact of ISM ionization and IGM heating in the early universe.

Abstract Copyright: © 2022. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): High mass x-ray binary stars - Metallicity - Star formation - Starburst galaxies - X-ray binary stars - X-ray astronomy - Compact objects

VizieR on-line data: <Available at CDS (J/ApJ/930/135): table1.dat table2.dat table4.dat>

Simbad objects: 39

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Number of rows : 39
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 UM 228 Sy1 00 21 01.0301998368 +00 52 48.159552756   17 17.0     ~ 66 0
2 NGC 253 SyG 00 47 33.134 -25 17 19.68   8.03   6.94 8.1 ~ 3588 2
3 IC 1623 IG 01 07 47.24 -17 30 25.0   15       ~ 338 2
4 NAME Chandra Deep Field-South reg 03 32 28.0 -27 48 30           ~ 2282 1
5 SDSS J074915.48+225342.1 H2G 07 49 15.48533 +22 53 42.1376           ~ 5 0
6 SDSS J080619.49+194927.3 H2G 08 06 19.4981154336 +19 49 27.296864868           ~ 16 0
7 LEDA 3403103 G 08 07 07.219 +35 21 30.40           ~ 4 0
8 SDSS J081420.79+575007.9 QSO 08 14 20.7859896312 +57 50 08.060181468           ~ 9 0
9 SDSS J082527.65+295739.3 H2G 08 25 27.6039246696 +29 57 38.764762344           ~ 8 0
10 SDSS J084219.07+300703.5 G 08 42 19.0773823872 +30 07 03.559972116           ~ 9 0
11 SDSS J092429.82+514301.1 G 09 24 29.8282058112 +51 43 00.715016100           ~ 3 0
12 SDSS J092705.72+044251.8 G 09 27 05.72691 +04 42 51.8737           ~ 4 0
13 Mrk 116 AGN 09 34 02.1 +55 14 25           ~ 1179 1
14 RX J0957.9+6903 ULX 09 57 53.290 +69 03 48.20           ~ 246 4
15 SDSS J095817.54+183858.0 G 09 58 17.5419852864 +18 38 57.996930192           ~ 3 0
16 SDSS J101815.08+462623.9 G 10 18 15.0870437352 +46 26 23.957050236           ~ 3 0
17 HS 1018+3619 EmG 10 21 06.3314685288 +36 04 08.933325816   17.3       ~ 5 0
18 NGC 3256 Sy2 10 27 51.284 -43 54 13.55   11.83 11.33 10.62 11.9 ~ 920 2
19 NGC 3310 AGN 10 38 45.85707 +53 30 11.8940   12.45 12.15     ~ 809 1
20 [VV2003c] J104642.5+022930 Sy1 10 46 42.4916796288 +02 29 28.999247676     19.17     ~ 4 0
21 LEDA 1336719 G 10 58 54.8033077464 +08 00 44.561338848           ~ 8 0
22 SBSG 1122+590 G 11 25 09.458 +58 47 00.77   18.5       ~ 5 0
23 [VV2003c] J114306.5+680717 Sy1 11 43 06.5480380176 +68 07 17.770070712     18.13     ~ 7 0
24 2MASS J12352590+3556230 G 12 35 25.86264 +35 56 22.9740           ~ 1 0
25 LEDA 41971 G 12 35 38.72557 +04 12 44.8333           ~ 6 0
26 LEDA 1317607 G 13 05 05.039 +07 15 51.93           ~ 6 0
27 HS 1325+4823 H2G 13 27 51.5133445656 +48 08 05.220094848   18.30       ~ 4 0
28 M 83 SBG 13 37 00.91920 -29 51 56.7400 8.85 8.11 7.52 7.21   ~ 2778 2
29 SDSS J135248.26+111410.4 H2G 13 52 48.2603554296 +11 14 10.832828244           ~ 5 0
30 [FK2005] 25 ULX 14 03 19.63 -41 22 58.7           ~ 252 0
31 SDSS J141646.47+144235.1 G 14 16 46.4859288384 +14 42 35.137660824           ~ 5 0
32 LEDA 4416378 G 14 26 15.0677667216 +10 02 13.595061372           ~ 4 0
33 LEDA 1519426 G 14 45 56.84865 +16 53 08.6747           ~ 7 0
34 SDSS J151231.77+090028.0 G 15 12 31.7595716304 +09 00 27.800877888           ~ 4 0
35 SHOC 502 Sy1 15 17 25.860 -00 08 05.48     18.17     ~ 8 0
36 SDSS J155439.96+413846.9 G 15 54 39.96411 +41 38 46.9328           ~ 3 0
37 LEDA 3089351 H2G 16 24 21.38141 +27 04 08.7149           ~ 6 0
38 SDSS J165844.49+351923.0 EmG 16 58 44.4398991960 +35 19 23.843924580           ~ 3 0
39 2MASS J22514028+1327137 H2G 22 51 40.31532 +13 27 13.3723           ~ 13 0

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