Table 1.
Sample considered in this work.
Name | D [Mpc] | θ[°] | Ref. | log M•/M⊙ | Rin [pc] | Rout [pc] | Rinfl [pc] |
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log Lbol/erg s−1 | log λEdd |
---|---|---|---|---|---|---|---|---|---|---|
(1) | (2) | (3) | (4) | (5) | (6) | (7) | (8) | (9) | (10) | (11) |
NGC 2960 | 81 | 89 | (a) | 7.09 | 0.13 | 0.31 | 1.92 |
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−2.1 |
NGC 4258 | 7.6 | 72 | (b) | 7.60 | 0.11 | 0.30 | 12.98 |
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−3.9 |
NGC 5765B | 126.3 | 95 | (c) | 7.67 | 0.33 | 1.20 | 7.65 |
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−1.4 |
NGC 6264 | 144 | 90 | (d) | 7.46 | 0.27 | 0.48 | 4.94 |
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−0.8 |
NGC 6323 | 107 | 89 | (e) | 6.99 | 0.15 | 0.31 | 1.67 |
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+0.1 |
UGC 3789 | 49.6 | 91 | (f) | 7.03 | 0.08 | 0.20 | 4.01 |
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−1.5 |
Notes. General properties of the sources considered. (1) – Name of the megamaser galaxy. (2) – Geometric distance in Mpc. (3) – Inclination angle of the maser disk at its innermost radius, rounded to the nearest integer. (4) – Reference for the geometric distance and for the inclination angle: (a) – Impellizzeri et al. (2012); (b) – Humphreys et al. (2013); (c) – Gao et al. (2016); (d) – Kuo et al. (2013); (e) – Kuo et al. (2015); (f) – Reid et al. (2013). (5) – Logarithm of the black hole mass in solar masses. (6)–(7) – Inner and outer masing radii, respectively, in pc. (8) – Radius of the sphere of influence of the BH, computed as Rinfl = GM/σ2. The velocity dispersions σ are from Greene et al. (2016). All maser disks considered here are well within the sphere of influence of the BH, which dominates the gravitational potential. (9) – Logarithm of the BH accretion rate in solar masses per year. The reference for Cols. 5–7, and 9 is Kuo et al. (2018). (10) – Logarithm of the bolometric luminosity in erg s−1, computed as (see text). (11) – Logarithm of the Eddington ratio, computed as Lbol/LEdd, where LEdd = 1.26 × 1038M•/M⊙.
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