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Table 4.

Results of linear regression of R − L relations for OI and RM measurements.

L Definition σlog L log(L0/erg s−1) R N c m σintrin
Lbol Bolometric luminosity in this work 0.3 45.1 OI 25 0 . 55 0.05 + 0.05 $ -0.55_{-0.05}^{+0.05} $ 0 . 45 0.05 + 0.05 $ 0.45_{-0.05}^{+0.05} $ 0.20
RM 29 0 . 95 0.05 + 0.05 $ -0.95_{-0.05}^{+0.05} $ 0 . 44 0.05 + 0.05 $ 0.44_{-0.05}^{+0.05} $ 0.15

L14 − 195 keV 14−195 keV luminosity 0.1 43.6 OI 18 0 . 87 0.05 + 0.05 $ -0.87_{-0.05}^{+0.05} $ 0 . 50 0.07 + 0.07 $ 0.50_{-0.07}^{+0.07} $ 0.21
RM 23 1 . 26 0.04 + 0.04 $ -1.26_{-0.04}^{+0.04} $ 0 . 41 0.06 + 0.06 $ 0.41_{-0.06}^{+0.06} $ 0.19
λ L λ ( 5100 Å ) $ \lambda L_{\lambda}(5100\,\AA) $ Monochromatic luminosity at 5100 Å $ 5100\,\AA $ 0.05 43.9 OI 25 0 . 68 0.04 + 0.04 $ -0.68_{-0.04}^{+0.04} $ 0 . 39 0.04 + 0.04 $ 0.39_{-0.04}^{+0.04} $ 0.20
RM 29 1 . 03 0.04 + 0.04 $ -1.03_{-0.04}^{+0.04} $ 0 . 37 0.03 + 0.03 $ 0.37_{-0.03}^{+0.03} $ 0.17
λLλ(12 μm) Monochromatic luminosity at 12 μm 0.1 44.2 OI 20 0 . 68 0.04 + 0.04 $ -0.68_{-0.04}^{+0.04} $ 0 . 47 0.04 + 0.04 $ 0.47_{-0.04}^{+0.04} $ 0.16
RM 14 1 . 03 0.05 + 0.05 $ -1.03_{-0.05}^{+0.05} $ 0 . 41 0.04 + 0.04 $ 0.41_{-0.04}^{+0.04} $ 0.14

Lbol, 14 − 195 keV Bolometric luminosity from L14 − 195 keV 0.3 44.4 OI 18 0 . 87 0.05 + 0.05 $ -0.87_{-0.05}^{+0.05} $ 0 . 50 0.07 + 0.07 $ 0.50_{-0.07}^{+0.07} $ 0.16
RM 23 1 . 27 0.04 + 0.04 $ -1.27_{-0.04}^{+0.04} $ 0 . 41 0.06 + 0.06 $ 0.41_{-0.06}^{+0.06} $ 0.16
L bol , 5100 Å $ L_{\mathrm{bol, 5100\,\AA}} $ Bolometric luminosity from L λ ( 5100 Å ) $ L_{\lambda}(5100\,\AA) $ 0.3 44.8 OI 25 0 . 68 0.04 + 0.04 $ -0.68_{-0.04}^{+0.04} $ 0 . 46 0.05 + 0.04 $ 0.46_{-0.05}^{+0.04} $ 0.16
RM 29 1 . 01 0.04 + 0.04 $ -1.01_{-0.04}^{+0.04} $ 0 . 44 0.04 + 0.04 $ 0.44_{-0.04}^{+0.04} $ 0.12
Lbol, 12 μm Bolometric luminosity from Lλ(12 μm) 0.3 44.9 OI 20 0 . 68 0.04 + 0.04 $ -0.68_{-0.04}^{+0.04} $ 0 . 46 0.04 + 0.04 $ 0.46_{-0.04}^{+0.04} $ 0.11
RM 14 1 . 03 0.06 + 0.05 $ -1.03_{-0.06}^{+0.05} $ 0 . 41 0.05 + 0.06 $ 0.41_{-0.05}^{+0.06} $ 0.12

Notes. R is the type of the dust size measurements. N is the number of the data pair of each fitting, depending on the data availability of each kind of luminosity measurement. L0, c, and m are defined in Eq. (2), and σintrin is the intrinsic scatter about the relation.

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