- Ho, Anna YQ;
- Goldstein, Daniel A;
- Schulze, Steve;
- Khatami, David K;
- Perley, Daniel A;
- Ergon, Mattias;
- Gal-Yam, Avishay;
- Corsi, Alessandra;
- Andreoni, Igor;
- Barbarino, Cristina;
- Bellm, Eric C;
- Blagorodnova, Nadia;
- Bright, Joe S;
- Burns, E;
- Cenko, S Bradley;
- Cunningham, Virginia;
- De, Kishalay;
- Dekany, Richard;
- Dugas, Alison;
- Fender, Rob P;
- Fransson, Claes;
- Fremling, Christoffer;
- Goldstein, Adam;
- Graham, Matthew J;
- Hale, David;
- Horesh, Assaf;
- Hung, Tiara;
- Kasliwal, Mansi M;
- Kuin, N Paul M;
- Kulkarni, SR;
- Kupfer, Thomas;
- Lunnan, Ragnhild;
- Masci, Frank J;
- Ngeow, Chow-Choong;
- Nugent, Peter E;
- Ofek, Eran O;
- Patterson, Maria T;
- Petitpas, Glen;
- Rusholme, Ben;
- Sai, Hanna;
- Sfaradi, Itai;
- Shupe, David L;
- Sollerman, Jesper;
- Soumagnac, Maayane T;
- Tachibana, Yutaro;
- Taddia, Francesco;
- Walters, Richard;
- Wang, Xiaofeng;
- Yao, Yuhan;
- Zhang, Xinhan
We present detailed observations of ZTF18abukavn (SN2018gep), discovered in high-cadence data from the Zwicky Transient Facility as a rapidly rising (1.4 ± 0.1 mag hr-1) and luminous (Mg,peak = -20 mag) transient. It is spectroscopically classified as a broad-lined stripped-envelope supernova (Ic-BL SN). The high peak luminosity (Lbol ≳ 3 × 1044 erg s-1), the short rise time (trise = 3 days in g band), and the blue colors at peak (g-r ∼ -0.4) all resemble the high-redshift Ic-BL iPTF16asu, as well as several other unclassified fast transients. The early discovery of SN2018gep (within an hour of shock breakout) enabled an intensive spectroscopic campaign, including the highest-temperature (Teff ≳ 40,000 K) spectra of a stripped-envelope SN. A retrospective search revealed luminous (Mg ∼ Mr ≈ mag) emission in the days to weeks before explosion, the first definitive detection of precursor emission for a Ic-BL. We find a limit on the isotropic gamma-ray energy release E γ,iso < 4.9 × 10 48 erg, a limit on X-ray emission LX < 1040 erg s-1, and a limit on radio emission ν Lν ≲ 1037 erg s-1. Taken together, we find that the early (< 10 days) data are best explained by shock breakout in a massive shell of dense circumstellar material (0.02 M⊙) at large radii (3 × 1014 cm) that was ejected in eruptive pre-explosion mass-loss episodes. The late-time (> 10 days) light curve requires an additional energy source, which could be the radioactive decay of Ni-56.