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Figure 1:
Time evolution of basic quantities
concerning radio emission,
with the solid and dashed lines corresponding to
the continuous and burst SFR, respectively.
The initial conditions are selected to
be the "active'' mode, consistent with
the observations of SBS 0335-052 at ![]() ![]() ![]() ![]() ![]() ![]() |
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Figure 2:
Radio SEDs at t=5 Myr calculated by
a) model A, b) model B, c) model E, d) model F,
e) model G, and f) model H for the same initial
condition as Fig. 1. For
model E, we adopt the best
fit parameter of
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Figure 3: Same as Fig. 1 but for the I Zw 18 "passive'' model. |
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Figure 4:
Radio SED at t=12 Myr calculated for
I Zw 18 by using models E, F, G, and H
(panels a), b), c), and
d), respectively).
The dotted and dashed lines
represent the thermal and nonthermal components,
respectively, and the solid line shows the sum of
those two components.
The squares are observational data taken from
Hunt et al. (2005) and
references therein. The reduced ![]() ![]() |
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Figure 5: Same as Fig. 4 but for t=15 Myr. |
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Figure 6: Time evolution of an "active'' radio SED. The same parameters as used to model SBS 0335-052 are adopted as a representative case for the "active'' mode. Panels a), b), c), and d) represent the SEDs at 3.5, 5, 10, and 15 Myr, respectively. The dotted and dashed lines represent the thermal and nonthermal components, respectively, and the solid line shows the sum of those two components. |
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Figure 7: Same as Fig. 6 but for the "passive'' mode, with the I Zw 18 model as a representative case. |
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Figure 8:
Time evolution of the radio spectral
index defined at 1.5 GHz and 5 GHz
[
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