4.7 Article

SUPER-LUMINOUS TYPE Ic SUPERNOVAE: CATCHING A MAGNETAR BY THE TAIL

Journal

ASTROPHYSICAL JOURNAL
Volume 770, Issue 2, Pages -

Publisher

IOP PUBLISHING LTD
DOI: 10.1088/0004-637X/770/2/128

Keywords

stars: magnetars; supernovae: general; supernovae: individual (PTF10hgi, PTF11rks, SN 2011ke, SN 2011kf, SN 2012il)

Funding

  1. European Research Council under the European Union's Seventh Framework Programme (FP7) ERC [291222]
  2. PRIN-INAF
  3. Transient Universe: from ESO Large to PESSTO
  4. Swedish Research Council [623-2011-7117]
  5. ERC-StG [EGGS-278202]
  6. DNRF
  7. TRR 33 The Dark universe of the German Research Foundation
  8. National Aeronautics and Space Administration [NNX08AR22G]
  9. National Science Foundation [AST-1238877]
  10. Alfred P. Sloan Foundation
  11. National Science Foundation
  12. U.S. Department of Energy Office of Science
  13. Division Of Astronomical Sciences
  14. Direct For Mathematical & Physical Scien [1009749] Funding Source: National Science Foundation
  15. Division Of Astronomical Sciences
  16. Direct For Mathematical & Physical Scien [1238877] Funding Source: National Science Foundation
  17. Science and Technology Facilities Council [ST/G009465/1, ST/I001123/1] Funding Source: researchfish
  18. STFC [ST/G009465/1, ST/I001123/1] Funding Source: UKRI

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We report extensive observational data for five of the lowest redshift Super-Luminous Type Ic Supernovae (SL-SNe Ic) discovered to date, namely, PTF10hgi, SN2011ke, PTF11rks, SN2011kf, and SN2012il. Photometric imaging of the transients at +50 to +230 days after peak combined with host galaxy subtraction reveals a luminous tail phase for four of these SL-SNe. A high-resolution, optical, and near-infrared spectrum from xshooter provides detection of a broad He I lambda 10830 emission line in the spectrum (+50 days) of SN2012il, revealing that at least some SL-SNe Ic are not completely helium-free. At first sight, the tail luminosity decline rates that we measure are consistent with the radioactive decay of Co-56, and would require 1-4 M-circle dot of Ni-56 to produce the luminosity. These Ni-56 masses cannot be made consistent with the short diffusion times at peak, and indeed are insufficient to power the peak luminosity. We instead favor energy deposition by newborn magnetars as the power source for these objects. A semi-analytical diffusion model with energy input from the spin-down of a magnetar reproduces the extensive light curve data well. The model predictions of ejecta velocities and temperatures which are required are in reasonable agreement with those determined from our observations. We derive magnetar energies of 0.4 less than or similar to E(10(51) erg) less than or similar to 6.9 and ejecta masses of 2.3 less than or similar to M-ej(M-circle dot) less than or similar to 8.6. The sample of five SL-SNe Ic presented here, combined with SN 2010gx-the best sampled SL-SNe Ic so far-points toward an explosion driven by a magnetar as a viable explanation for all SL-SNe Ic.

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