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Table 2:

Observed H$\alpha $ fluxes of IC4662 A1 and A2 from optical HST/F658N imaging (6 arcsec radii), compared to radio and mid-IR results.
QuantityUnitsA1A2
F(H$\alpha $+[N  II])(erg s-1 cm-2) $1.94\times 10^{-12}$ $1.61 \times 10^{-12}$
F[N  II]/F(H$\alpha $) 0.030.03
F(H$\alpha $)(erg s-1 cm-2) $1.89\times 10^{-12}$ $1.56 \times 10^{-12}$
E(B-V)(mag)0.1620.165
I(H$\alpha $)(erg s-1 cm-2) $2.75\times10^{-12}$ $2.30\times10^{-12}$
L(H$\alpha $)(erg s-1) $1.96\times10^{39}$ $1.63\times10^{39}$
Q0(H$\alpha $)(1049 s-1)145121
    
Q0(3 cm)$^{\ast}$(1049 s-1)227242
Q0(Hu$\alpha $)$\ddag $(1049 s-1)345256
$^{\ast}$ Johnson et al. (2003) adjusted to 2.44 Mpc.
$^\ddag $ Gilbert & Vacca (2009) adjusted to 2.44 Mpc.

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