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Table 4.

Photometric parameters for the complete LRN sample.

LRN name Host thost Distance E(B − V)tot MV(prog) MV(CE) Mpk1 Mpk2 Lpk1/Lpk2 Δt1 dex Mprog
galaxy (Mpc) (mag) (mag) (mag) (mag) (mag) optical (days) (M)
AT 2021afy UGC 10043 4.2 ± 0.7 49.2 ± 8.0 0.43 ± 0.11 >  − 11.66 ± 0.56 >  − 13.20 ± 0.56 −14.44 ± 0.57 −14.57 ± 0.56 1.0 120
UGC12307-2013OT1 UGC 12307 9.8 ± 1.0 39.7 ± 2.8 0.22 ± 0.02 >  − 11.88 ± 0.17 −15.03 ± 0.42
AT 2017jfs NGC 4470 1.9 ± 2.1 35.2 ± 2.7 0.02 ± 0.01 >  − 11.26 ± 0.17 −15.46 ± 0.46 −14.38 ± 0.17 2.6 157
SNhunt248 NGC 5806 3.2 ± 0.8 22.5 ± 3.8 0.04 ± 0.01 −8.99 ± 0.36 −11.18 ± 0.36 −14.87 ± 0.36 −14.07 ± 0.36 2.1 169 58 ± 2 ( ⋆ )
AT 2020kog NGC 6106 5.3 ± 0.6 22.5 ± 4.7 0.37 ± 0.07 >  − 9.82 ± 0.50 −11.17 ± 0.53 −13.17 ± 0.51 −12.68 ± 0.51 2.0 > 100
AT 2018hso NGC 3729 1.3 ± 0.8 21.3 ± 0.6 0.30 ± 0.08 −9.05 ± 0.25 −13.89 ± 0.28 −12.16 ± 0.26 3.7 201
NGC3437-2011OT1 NGC 3437 5.2 ± 0.5 20.9 ± 4.2 0.02 ± 0.01 >  − 9.98 ± 0.43 >  − 10.83 ± 0.43 −13.06 ± 0.48 −13.33 ± 0.43 0.9 174
AT 2014ej NGC 7552 2.4 ± 0.7 20.6 ± 1.5 0.31 ± 0.15 >  − 8.22 ± 0.50 >  − 14.70 ± 0.50 −14.36 ± 0.50 > 2.2 > 98
NGC4490-2011OT1 NGC 4490 7.0 ± 0.4 9.6 ± 1.3 0.32 ± 0.32 0.9 200
AT 1997bs NGC 3627 3.1 ± 0.4 9.2 ± 0.3 0.21 ± 0.04 −7.61 ± 0.21 −13.34 ± 0.15 −11.51 ± 0.17 3.2 62
AT 2021blu UGC 5829 9.8 ± 0.6 8.64 ± 0.61 0.02 ± 0.01 −6.72 ± 0.30 −8.33 ± 0.43 −13.06 ± 0.15 −12.26 ± 0.15 2.4 242
AT 2021biy NGC 4631 6.5 ± 0.7 7.46 ± 0.50 0.27 ± 0.02 −7.93 ± 0.17 −8.78 ± 0.20 −13.81 ± 0.16 −12.65 ± 0.16 2.7 375 20.5 ± 3.5 ( ⋆ )
AT 2018bwo NGC 45 7.8 ± 0.7 6.79 ± 1.13 0.02 ± 0.01 −5.92 ± 0.36 −7.47 ± 0.36 −10.14 ± 0.45 > 72
AT 2015dl M 101 5.9 ± 0.3 6.43 ± 0.57 0.01 ± 0.01 −7.19 ± 0.36 −10.10 ± 0.47 −12.70 ± 0.21 −11.46 ± 0.31 2.0 229 18 ± 1 ( ⋆ )
AT 2020hat NGC 5068 6.0 ± 0.4 5.16 ± 0.21 0.09 ± 0.01 −2.99 ± 0.09 −8.87 ± 0.76 −10.72 ± 0.27 −10.08 ± 0.26 1.5 131
AT 2019zhd M 31 3.0 ± 0.4 0.785 ± 0.009 0.055 ± 0.005 0.17 ± 0.14 −5.74 ± 0.28 −9.08 ± 0.13 −7.59 ± 0.32 5.1 27
M31LRN2015 M 31 3.0 ± 0.4 0.785 ± 0.009 0.35 ± 0.11 −2.25 ± 0.47 −5.41 ± 0.42 −10.12 ± 0.42 −9.13 ± 0.42 2.4 62
M31RV M 31 3.0 ± 0.4 0.785 ± 0.009 0.12 ± 0.02 −5.04 ± 0.32 >  − 7.04 ± 0.15 −9.54 ± 0.15 −8.66 ± 0.15 2.0 110
CK Vul( † ) Galaxy 0.80 ± 0.15 0.7 400
V838 Mon Galaxy 6.1(±0.6)×10−3 0.85 ± 0.02 −1.29 ± 0.22 −6.67 ± 0.22 −9.76 ± 0.22 −9.43 ± 0.22 1.7 82 8 ± 3 ( ⋆ )
V4332 Sgr Galaxy 0.32 ± 0.10 1.0 ± 0.5 ( ⋆ )
V1309 Sco Galaxy 3.5(±1.5)×10−3 0.70 ± 0.15 3.33 ± 1.04 −1.39 ± 1.04 −7.02 ± 1.04 −5.48 ± 1.04 3.1 29 1.54 ± 0.5 ( ⋆ )
OGLE-2002-BLG-360 Galaxy 8.20(±0.15)×10−3 1.0 ± 0.2 (‡) 2.23 ± 0.50 −1.43 ± 0.54 0.10 ± 0.54 0.79 ± 0.65 1.0 837
OGLE-2002-BLG-360 Galaxy 8.20(±0.15)×10−3 1.0 ± 0.2 (‡) 1.13 ± 0.28 −3.54 ± 0.28 −4.56 ± 0.28 −4.65 ± 0.30 1.0 837

Notes. The table reports the LRN name (Col. 1); the host-galaxy name (Col. 2) and its morphological type code (from Hyperleda; Col. 3); the distance (Col. 4); the total colour excess (Col. 5); the V-band absolute magnitude of the quiescent progenitor (Col. 6), the brightest V absolute magnitude of the pre-outburst phase (Col. 7), the first light-curve peak (Col. 8), and the second light-curve peak (Col. 9); the optical luminosity ratio of the first to the second light-curve peak (Col. 10); time taken by the LRN to decrease its luminosity by one order of magnitude from the peak (Col. 11); and the progenitor mass estimate using Eq. (1) or taken from Cai et al. (2022b; Col. 12). ( ⋆ )Mass estimates obtained through the direct detection of the progenitor or via light-curve modelling, as adopted by Cai et al. (2022b). ( ‡ ) The Milky Way reddening towards OGLE-2002-BLG-360 follows a non-standard reddening law (E(B − V)MW = 1 mag, with RV = 2.5; Nataf et al. 2013). While the parameters for the I-band photometry are robust, those inferred for V photometry are uncertain owing to the low-cadence follow-up observations in that filter. The V magnitudes are obtained through an interpolation of the V − I colour curve at the epochs of the I-band peaks. (†) In this table, the parameters for CK Vul are taken from Banerjee et al. (2020).

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