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Table 2.

Input parameters of Cloudy models.

Fixed parameters
Stellar population BPASS v2.1(1) (Eldridge et al. 2017)
Broken power-law IMF
α1 (0.1 M – 0.5 M) = −1.30
α2 (0.5 M – 100 M) = −2.35
Single burst, including binary stars
X-ray component Multicolor blackbody(Mitsuda et al. 1984),Tout = 103K, variable Tin
Other fields Cosmic microwave background
Cosmic ray background 0.5log

Grains SMC graphite/silicate model (Weingartner & Draine 2001)
Zdust, qPAH Values scaled with metallicity based on the analytical fits from Galliano et al. (2021)
X/O profiles (2) N(1), C(1), Ne(2), S(2), Ar(2), Fe(2), Si(3), Cl(4)
Other elements Table ISM from Cloudy

Density law nH = nH, HII× (1+N(H)/[1021 cm−2])
Stopping criteria AV = 10 or Te = 10K

8 varied parameters

log(L*/L) [7, 9]
LX/L* [0, 0.001, 0.01, 0.1]
log(TX, in) [5, 6, 7] K
log([O/H]) [−2.190, −1.889, −1.190,−0.889, −0.667, −0.491,−0.190, 0.111]
Age of burst [1,2,3,4,5,6,8,10] Myr
log(nH) [0,1,2,3,4] cm−3
log(Uin) (3) [−4, −3, −2, −1, 0]
Cut (4) [0,4], step = 0.25

Notes.

(1)

Metallicity bins in BPASS are Z = 10−5, 10−4, 0.001, 0.002, 0.003, 0.004, 0.006, 0.008, 0.010, 0.014, 0.020, 0.030 and 0.040 (i.e. 0.05% of solar to twice solar). We note that Z = 0.02 while the default value we use here is Z = 0.014.

(3)

The input ionization parameter, Uin, is set by varying the inner radius for a given luminosity. It is described in Sect. 3.2.3.

(4)

The cut parameter controls the stopping depth of a given model. It is described in Sect. 3.2.3.

References.

(2)

References for elemental abundances. (1): Nicholls et al. 2017, (2): Izotov et al. 2006, (3): Izotov & Thuan 1999, (4): fixed at −3.4.

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