Evidence for Late-stage Eruptive Mass Loss in the Progenitor to SN2018gep, a Broad-lined Ic Supernova: Pre-explosion Emission and a Rapidly Rising Luminous Transient
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Citations
The Zwicky Transient Facility Bright Transient Survey. II. A Public Statistical Sample for Exploring Supernova Demographics
The Koala: A Fast Blue Optical Transient with Luminous Radio Emission from a Starburst Dwarf Galaxy at z = 0.27
The Koala: A Fast Blue Optical Transient with Luminous Radio Emission from a Starburst Dwarf Galaxy at $z=0.27$
SN 2019ehk: A Double-peaked Ca-rich Transient with Luminous X-Ray Emission and Shock-ionized Spectral Features
SN2019dge: A Helium-rich Ultra-stripped Envelope Supernova
References
Matplotlib: A 2D Graphics Environment
SciPy 1.0--Fundamental Algorithms for Scientific Computing in Python
The Two Micron All Sky Survey (2MASS)
Planck 2015 results - XIII. Cosmological parameters
Stellar population synthesis at the resolution of 2003
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Frequently Asked Questions (15)
Q2. What future works have the authors mentioned in the paper "Evidence for late-stage eruptive mass loss in the progenitor to sn2018gep, a broad-lined ic supernova: pre-explosion emission and a rapidly rising luminous transient" ?
This rise rate is second only to that of SN 2016gkg ( Bersten et al. 2018 ), which was attributed to shock breakout in extended material surrounding a Type IIb progenitor. Radioactive decay is one possibility, but further monitoring is needed to test this. The luminosity of these detections ( M=−14 ) and evidence for variability suggests that they arise from eruptive mass loss, rather than the luminosity of a quiescent progenitor. From an NLTE spectral synthesis model, the authors find that this can be reproduced with a carbon and oxygen composition.
Q3. How do the authors determine a reference epoch?
To establish a reference epoch, the authors fit a second-order polynomial to the first three days of the g-band light curve in flux space, and define t0 as the time at which the flux is zero.
Q4. What was the method used to estimate the uncertainty on the flux measurements?
To estimate the uncertainty on the flux measurements made on these subtractions, the authors employed a Monte Carlo technique, in which thousands of PSF fluxes were measured at random locations on the image, and the PSF-flux uncertainty was taken to be the 1σ dispersion in these measurements.
Q5. How do the authors solve the equations of radiation hydrodynamics?
The authors assume spherical symmetry and solve the coupled equations of radiation hydrodynamics using a gray flux-limited nonequilibrium diffusion approximation.
Q6. How did the authors extend the light curve further back in time?
To extend the light curve further back in time, the authors performed forced photometry at the position of SN2018gep on single-epoch difference images from the IPAC ZTF difference imaging pipeline.
Q7. What motivated us to model one of the early spectra?
The lack of comparison data at such early epochs (high temperatures) motivated us to model one of the early spectra in order to determine the composition and density profile of the ejecta.
Q8. What is the effect of the CSM mass on the peak luminosity?
The peak luminosity is relatively independent of the CSM mass, which instead affects the photospheric velocity and temperature (i.e., a larger CSM mass slows down the post-interaction velocity to a greater extent and increases the shock-heated temperature).
Q9. How many optical spectra were obtained from the LT?
Twenty-three optical spectra were obtained from D =t 0.7–61.1 days using SPRAT, the Andalusia Faint Object Spectrograph and Camera (ALFOSC) on the Nordic Optical Telescope (NOT), the Double Spectrograph (DBSP; Oke & Gunn 1982) on the 200 inch Hale telescope at Palomar Observatory, the Low Resolution Imaging Spectrometer (LRIS; Oke et al. 1995) on the Keck The author10 m telescope, and the Xinglong 2.16 m telescope (XLT+BFOSC) of NAOC, China (Wang et al. 2018).
Q10. What is the code used to produce the results described in this paper?
The code used to produce the results described in this paper was written in Python and is available online in an open-source GitHub repository41 and it is archived on Zenodo (doi:10.5281/zenodo.3534067).
Q11. What was the extinction curve used to calibrate the spectra?
The spectra were further corrected for continuum atmospheric extinction during flux calibration, using mean extinction curves obtained at Xinglong Observatory.
Q12. How did the authors measure the flux of SN2018gep?
the authors report the maximum flux within pixels contained in a circular region centered on the optical position of SN2018gep with radius comparable to the FWHM of the VLA synthesized beam at the appropriate frequency.
Q13. What is the first definitive detection of preexplosion emission in a SN?
Assuming that the rapid rise the authors detected was close to the time of explosion, this is the first definitive detection of preexplosion emission in a Ic-BL SN.
Q14. Why have these models been difficult to test?
These models have been difficult to test because the majority of fast-luminous transients have been discovered post facto and located at cosmological distances (z∼0.1).
Q15. What is the effective date of the extended prediscovery detections?
The effective dates of these extended prediscovery detections are determined by taking an inverse-flux variance weighted average of the input image dates.