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Table 2.

Time-of-explosion fit data and results.

SN t0 [MJD] Surveys Bands Ref
2003bn 52692 . 21 0.10 + 0.08 $ 52692.21^{+0.08}_{-0.10} $ NEAT, CATS clear + Va 1,2
2006it 54005 . 48 1.15 + 1.59 $ 54005.48^{+1.59}_{-1.15} $ LOSS clear,r 3,4
2010id 55452 . 81 0.72 + 0.49 $ 55452.81^{+0.49}_{-0.72} $ PTF r 5
2013fs 56571 . 05 0.04 + 0.04 $ 56571.05^{+0.04}_{-0.04} $ iPTF r 6
2019luo 58678 . 46 0.86 + 0.79 $ 58678.46^{+0.79}_{-0.86} $ ZTF g, r 7
2020bad 58870 . 99 0.16 + 0.14 $ 58870.99^{+0.14}_{-0.16} $ ZTF g, r 7
2020cvy 58896 . 37 0.11 + 0.18 $ 58896.37^{+0.18}_{-0.11} $ ZTF g, r 7
2021gvv 59294 . 14 0.54 + 0.34 $ 59294.14^{+0.34}_{-0.54} $ ATLAS, ZTF g, r, o 7,8
2021hkf 59299 . 23 0.65 + 0.88 $ 59299.23^{+0.88}_{-0.65} $ ZTF g, r 7
2021acvc 59513 . 87 0.39 + 0.51 $ 59513.87^{+0.51}_{-0.39} $ ATLAS, ZTF r,o 7,8

Notes. aWe combined the deep non-detection (21.0 mag) and detection (20.2 mag) on unfiltered images (Wood-Vasey et al. 2003) with filtered photometry (Anderson et al. 2014). The very blue spectral energy distribution at early times suggests the effective wavelength of the unfiltered images corresponds to a blue band, leading us to adopt the V-band. Whether we combine the unfiltered data with V or B band photometry is inconsequential, however, given the significant magnitude difference between the first detection and the peak (∼3.5 mag). Because the first detection does not have a reported uncertainty, we assumed a significant error of 0.5 mag. (1) Anderson et al. (2014); (2) Wood-Vasey et al. (2003); (3) Lee & Li (2006); (4) Hicken et al. (2017); (5) Gal-Yam et al. (2011); (6) Yaron et al. (2017); (7) Masci et al. (2019, 2023); (8) Tonry et al. (2018), Smith et al. (2020b); Shingles et al. (2021).

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