Bibcode
Roy, R.; Sollerman, J.; Silverman, J. M.; Pastorello, A.; Fransson, C.; Drake, A.; Taddia, F.; Fremling, C.; Kankare, E.; Kumar, B.; Cappellaro, E.; Bose, S.; Benetti, S.; Filippenko, A. V.; Valenti, S.; Nyholm, A.; Ergon, M.; Sutaria, F.; Kumar, B.; Pandey, S. B.; Nicholl, M.; Garcia-Álvarez, D.; Tomasella, L.; Karamehmetoglu, E.; Migotto, K.
Referencia bibliográfica
Astronomy and Astrophysics, Volume 596, id.A67, 21 pp.
Fecha de publicación:
12
2016
Revista
Número de citas
29
Número de citas referidas
23
Descripción
Context. Research on supernovae (SNe) over the past decade has confirmed
that there is a distinct class of events which are much more luminous
(by 2 mag) than canonical core-collapse SNe (CCSNe). These events with
visual peak magnitudes ≲-21 are called superluminous SNe (SLSNe).
The mechanism that powers the light curves of SLSNe is still not well
understood. The proposed scenarios are circumstellar interaction, the
emergence of a magnetar after core collapse, or disruption of a massive
star through pair production. Aims: There are a few intermediate
events which have luminosities between these two classes. They are
important for constraining the nature of the progenitors of these two
different populations and their environments and powering mechanisms.
Here we study one such object, SN 2012aa. Methods: We observed
and analysed the evolution of the luminous Type Ic SN 2012aa. The event
was discovered by the Lick Observatory Supernova Search in an anonymous
galaxy (z ≈ 0.08). The optical photometric and spectroscopic
follow-up observations were conducted over a time span of about 120
days. Results: With an absolute V-band peak of - 20 mag, the SN
is an intermediate-luminosity transient between regular SNe Ibc and
SLSNe. SN 2012aa also exhibits an unusual secondary bump after the
maximum in its light curve. For SN 2012aa, we interpret this as a
manifestation of SN-shock interaction with the circumstellar medium
(CSM). If we assume a 56Ni-powered ejecta, the
quasi-bolometric light curve requires roughly 1.3 M⊙ of
56Ni and an ejected mass of 14M⊙. This also
implies a high kinetic energy of the explosion, 5.4 ×
1051 erg. On the other hand, the unusually broad light curve
along with the secondary peak indicate the possibility of interaction
with CSM. The third alternative is the presence of a central engine
releasing spin energy that eventually powers the light curve over a long
time. The host of SN 2012aa is a star-forming Sa/Sb/Sbc galaxy.
Conclusions: Although the spectral properties of SN 2012aa and its
velocity evolution are comparable to those of normal SNe Ibc, its broad
light curve along with a large peak luminosity distinguish it from
canonical CCSNe, suggesting that the event is an intermediate-luminosity
transient between CCSNe and SLSNe at least in terms of peak luminosity.
In comparison to other SNe, we argue that SN 2012aa belongs to a
subclass where CSM interaction plays a significant role in powering the
SN, at least during the initial stages of evolution.