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Monthly Notices of the Royal Astronomical Society | 2014

Superluminous supernovae from PESSTO

M. Nicholl; S. J. Smartt; A. Jerkstrand; C. Inserra; J. P. Anderson; Charles Baltay; Stefano Benetti; T.-W. Chen; N. Elias-Rosa; U. Feindt; M. Fraser; Avishay Gal-Yam; E. Hadjiyska; D. A. Howell; R. Kotak; A. Lawrence; G. Leloudas; S. Margheim; Seppo Mattila; M. McCrum; R. McKinnon; Alexander Mead; Peter E. Nugent; D. Rabinowitz; Armin Rest; K. W. Smith; Jesper Sollerman; M. Sullivan; F. Taddia; S. Valenti

We present optical spectra and light curves for three hydrogen-poor superluminous supernovae followed by the Public ESO Spectroscopic Survey of Transient Objects (PESSTO). Time series spectroscopy from a fewdays aftermaximum light to 100 d later shows them to be fairly typical of this class, with spectra dominated by Ca II, MgII, FeII, and Si II, which evolve slowly over most of the post-peak photospheric phase. We determine bolometric light curves and apply simple fitting tools, based on the diffusion of energy input by magnetar spin-down, Ni-56 decay, and collision of the ejecta with an opaque circumstellar shell. We investigate how the heterogeneous light curves of our sample (combined with others from the literature) can help to constrain the possible mechanisms behind these events. We have followed these events to beyond 100-200 d after peak, to disentangle host galaxy light from fading supernova flux and to differentiate between the models, which predict diverse behaviour at this phase. Models powered by radioactivity require unrealistic parameters to reproduce the observed light curves, as found by previous studies. Both magnetar heating and circumstellar interaction still appear to be viable candidates. A large diversity is emerging in observed tail-phase luminosities, with magnetar models failing in some cases to predict the rapid drop in flux. This would suggest either that magnetars are not responsible, or that the X-ray flux from the magnetar wind is not fully trapped. The light curve of one object shows a distinct rebrightening at around 100 d after maximum light. We argue that this could result either from multiple shells of circumstellar material, or from a magnetar ionization front breaking out of the ejecta.


Monthly Notices of the Royal Astronomical Society | 2013

A statistical analysis of circumstellar material in type Ia supernovae

K. Maguire; M. Sullivan; Ferdinando Patat; Avishay Gal-Yam; Isobel M. Hook; S. Dhawan; Dale Andrew Howell; Paolo A. Mazzali; P. Nugent; Y.-C. Pan; Philipp Podsiadlowski; J. D. Simon; Assaf Sternberg; S. Valenti; Charles Baltay; D. F. Bersier; N. Blagorodnova; T.-W. Chen; Nancy E. Ellman; U. Feindt; Francisco Forster; M. Fraser; S. González-Gaitán; M. L. Graham; C. P. Gutiérrez; S. Hachinger; E. Hadjiyska; C. Inserra; C. Knapic; Russ R. Laher

A key tracer of the elusive progenitor systems of Type Ia supernovae (SNe Ia) is the detection of narrow blueshifted time-varying Na I D absorption lines, interpreted as evidence of circumstellar material surrounding the progenitor system. The origin of this material is controversial, but the simplest explanation is that it results from previous mass-loss in a system containing a white dwarf and a non-degenerate companion star. We present new single-epoch intermediate-resolution spectra of 17 low-redshift SNe Ia taken with XShooter on the European Southern Observatory Very Large Telescope. Combining this sample with events from the literature, we confirm an excess (similar to 20 per cent) of SNe Ia displaying blueshifted narrow Na I D absorption features compared to redshifted Na I D features. The host galaxies of SNe Ia displaying blueshifted absorption profiles are skewed towards later-type galaxies, compared to SNe Ia that show no Na I D absorption and SNe Ia displaying blueshifted narrow Na I D absorption features have broader light curves. The strength of the Na I D absorption is stronger in SNe Ia displaying blueshifted Na I D absorption features than those without blueshifted features, and the strength of the blueshifted Na I D is correlated with the B - V colour of the SN at maximum light. This strongly suggests the absorbing material is local to the SN. In the context of the progenitor systems of SNe Ia, we discuss the significance of these findings and other recent observational evidence on the nature of SN Ia progenitors. We present a summary that suggests that there are at least two distinct populations of normal, cosmologically useful SNe Ia.


The Astrophysical Journal | 2015

LSQ14bdq: a type Ic Super-luminous Supernova with a double-peaked light curve

M. Nicholl; S. J. Smartt; A. Jerkstrand; S. A. Sim; C. Inserra; J. P. Anderson; Charles Baltay; Stefano Benetti; K. C. Chambers; T.-W. Chen; N. Elias-Rosa; U. Feindt; H. Flewelling; M. Fraser; Avishay Gal-Yam; L. Galbany; M. E. Huber; T. Kangas; E. Kankare; R. Kotak; T. Krühler; K. Maguire; R. McKinnon; D. Rabinowitz; S. Rostami; S. Schulze; K. W. Smith; M. Sullivan; John L. Tonry; S. Valenti

We present data for LSQ14bdq, a hydrogen-poor super-luminous supernova (SLSN) discovered by the La Silla QUEST survey and classified by the Public ESO Spectroscopic Survey of Transient Objects. The spectrum and light curve are very similar to slow-declining SLSNe such as PTF12dam. However, detections within ~1 day after explosion show a bright and relatively fast initial peak, lasting for ~15 days, prior to the usual slow rise to maximum light. The broader, main peak can be fit with either central engine or circumstellar interaction models. We discuss the implications of the precursor peak in the context of these models. It is too bright and narrow to be explained as a normal 56Ni-powered SN, and we suggest that interaction models may struggle to fit the two peaks simultaneously. We propose that the initial peak may arise from the post-shock cooling of extended stellar material, and reheating by a central engine drives the second peak. In this picture, we show that an explosion energy of ~2x10^{52} erg and a progenitor radius of a few hundred solar radii would be required to power the early emission. The competing engine models involve rapidly spinning magnetars (neutron stars) or fall-back accretion onto a central black hole. The prompt energy required may favour the black hole scenario. The bright initial peak effectively rules out a compact Wolf-Rayet star as a progenitor, since the inferred energies and ejected masses become unphysical.


Monthly Notices of the Royal Astronomical Society | 2018

On the nature of hydrogen-rich superluminous supernovae

C. Inserra; S. J. Smartt; E.E.E. Gall; G. Leloudas; T.-W. Chen; S. Schulze; A. Jerkstrand; M. Nicholl; J. P. Anderson; I. Arcavi; Stefano Benetti; R. Cartier; Michael J. Childress; M. Della Valle; H. Flewelling; M. Fraser; Avishay Gal-Yam; C. P. Gutiérrez; G. Hosseinzadeh; D. A. Howell; M. Huber; E. Kankare; T. Krühler; E. A. Magnier; K. Maguire; Curtis McCully; S. Prajs; N. Primak; Richard Allen Scalzo; Brian Paul Schmidt

We present two hydrogen-rich superluminous supernovae (SLSNe): SN2103hx and PS15br. These objects, together with SN2008es, are the only SLSNe showing a distinct, broad H α feature during the photospheric phase; also, they show no sign of strong interaction between fast moving ejecta and circumstellar shells in their early spectra. Despite the fact that the peak luminosity of PS15br is fainter than that of the other two objects, the spectrophotometric evolution is similar to SN2103hx and different from any other supernova in a similar luminosity space. We group all of them as SLSNe II and hence they are distinct from the known class of SLSN IIn. Both transients show a strong, multicomponent H α emission after 200 d past maximum, which we interpret as an indication of the interaction of the ejecta with an asymmetric, clumpy circumstellar material. The spectra and photometric evolution of the two objects are similar to Type II supernovae, although they have much higher luminosity and evolve on slower time-scales. This is qualitatively similar to how SLSNe I compare with normal type Ic, in that the former are brighter and evolve more slowly. We apply a magnetar and an interaction semi-analytical code to fit the light curves of our two objects and SN2008es. The overall observational data set would tend to favour the magnetar, or central engine, model as the source of the peak luminosity, although the clear signature of late-time interaction indicates that interaction can play a role in the luminosity evolution of SLSNe II at some phases.


The Astrophysical Journal | 2016

A decam search for an optical counterpart to the ligo gravitational-wave event GW151226

S. J. Smartt; K. C. Chambers; K. W. Smith; M. Huber; D. R. Young; T.-W. Chen; C. Inserra; D. Wright; M. W. Coughlin; Larry Denneau; H. Flewelling; A. Heinze; A. Jerkstrand; E. A. Magnier; K. Maguire; Bernhard Mueller; Armin Rest; A. Sherstyuk; B. Stalder; A. S. B. Schultz; C. W. Stubbs; John L. Tonry; C. Waters; R. J. Wainscoat; M. Della Valle; M. Dennefeld; G. Dimitriadis; R. E. Firth; M. Fraser; C. Frohmaier

We report the results of a Dark Energy Camera optical follow-up of the gravitational-wave (GW) event GW151226, discovered by the Advanced Laser Interferometer Gravitational-wave Observatory detectors. Our observations cover 28.8 deg2 of the localization region in the i and z bands (containing 3% of the BAYESTAR localization probability), starting 10 hr after the event was announced and spanning four epochs at 2--24 days after the GW detection. We achieve 5sigma point-source limiting magnitudes of i≈ 21.7 and z≈ 21.5, with a scatter of 0.4 mag, in our difference images. Given the two-day delay, we search this area for a rapidly declining optical counterpart with ≳ 3sigma significance steady decline between the first and final observations. We recover four sources that pass our selection criteria, of which three are cataloged active galactic nuclei. The fourth source is offset by 5.8 arcsec from the center of a galaxy at a distance of 187 Mpc, exhibits a rapid decline by 0.5 mag over 4 days, and has a red color of i-z≈ 0.3 mag. These properties could satisfy a set of cuts designed to identify kilonovae. However, this source was detected several times, starting 94 days prior to GW151226, in the Pan-STARRS Survey for Transients (dubbed as PS15cdi) and is therefore unrelated to the GW event. Given its long-term behavior, PS15cdi is likely a Type IIP supernova that transitioned out of its plateau phase during our observations, mimicking a kilonova-like behavior. We comment on the implications of this detection for contamination in future optical follow-up observations.


The Astrophysical Journal | 2018

The Cow: Discovery of a Luminous, Hot, and Rapidly Evolving Transient

Simon Prentice; K. Maguire; S. J. Smartt; M. R. Magee; Patricia Schady; S. A. Sim; T.-W. Chen; Peter Clark; Christelle Colin; M Fulton; Owen McBrien; David O'Neill; K. W. Smith; C. Ashall; K. C. Chambers; Larry Denneau; H. Flewelling; A. Heinze; T. W.-S. Holoien; M. E. Huber; C. S. Kochanek; Paolo A. Mazzali; J.L. Prieto; A. Rest; B. J. Shappee; B. Stalder; K. Z. Stanek; M. D. Stritzinger; Todd A. Thompson; John L. Tonry

We present the ATLAS discovery and initial analysis of the first 18 days of the unusual transient event, ATLAS18qqn/AT2018cow. It is characterized by a high peak luminosity (~1.7 × 1044 erg s−1), rapidly evolving light curves (>5 mag rise to peak in ~3.5 days), and hot blackbody spectra, peaking at ~27,000 K that are relatively featureless and unchanging over the first two weeks. The bolometric light curve cannot be powered by radioactive decay under realistic assumptions. The detection of high-energy emission may suggest a central engine as the powering source. Using a magnetar model, we estimated an ejected mass of 0.1–0.4 M


Monthly Notices of the Royal Astronomical Society | 2018

SNe 2013K and 2013am: observed and physical properties of two slow, normal Type IIP events

L. Tomasella; E. Cappellaro; M. L. Pumo; A. Jerkstrand; Stefano Benetti; N. Elias-Rosa; M. Fraser; C. Inserra; Andrea Pastorello; M. Turatto; J. P. Anderson; L. Galbany; C. P. Gutiérrez; E. Kankare; Giuliano Pignata; G. Terreran; S. Valenti; C. Barbarino; F. E. Bauer; M. T. Botticella; T.-W. Chen; Avishay Gal-Yam; A. Harutyunyan; D. A. Howell; K. Maguire; A. Morales Garoffolo; P. Ochner; S. J. Smartt; S. Schulze; D. R. Young

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Nature | 2016

Corrigendum: Slowly fading super-luminous supernovae that are not pair-instability explosions

M. Nicholl; Stephen J. Smartt; A. Jerkstrand; C. Inserra; M. McCrum; R. Kotak; M. Fraser; D. Wright; T.-W. Chen; K. W. Smith; D. R. Young; S. A. Sim; S. Valenti; Dale Andrew Howell; Fabio Bresolin; R. P. Kudritzki; John L. Tonry; M. Huber; A. Rest; Andrea Pastorello; L. Tomasella; Enrico Cappellaro; Stefano Benetti; Seppo Mattila; E. Kankare; T. Kangas; G. Leloudas; Jesper Sollerman; F. Taddia; Edo Berger

, which lies between that of low-energy core-collapse events and the kilonova, AT2017gfo. The spectra cooled rapidly from 27,000 to 15,000 K in just over two weeks but remained smooth and featureless. Broad and shallow emission lines appear after about 20 days, and we tentatively identify them as He i although they would be redshifted from their rest wavelengths. We rule out that there are any features in the spectra due to intermediate mass elements up to and including the Fe group. The presence of r-process elements cannot be ruled out. If these lines are due to He, then we suggest a low-mass star with residual He as a potential progenitor. Alternatively, models of magnetars formed in neutron star mergers, or accretion onto a central compact object, give plausible matches to the data.


Epilepsy & Behavior | 2015

FV-082: A safer orally active broad-spectrum antiepileptic drug candidate

Malik Slassi; Peter Dove; Shane Climie; David O'Neill; Zezhou Wang; Lilly Tsirulnikov; Henrianna; David K.H. Lee; Inés de Lannoy; T.-W. Chen; Jim Stables; Winnie Lau; Leo B. Silenieks; Guy A. Higgins

We present 1 yr of optical and near-infrared photometry and spectroscopy of the Type IIP SNe 2013K and 2013am. Both objects are affected by significant extinction, due to their location in dusty regions of their respective host galaxies, ESO 009-10 and NGC 3623 (M65). From the photospheric to nebular phases, these objects display spectra congruent with those of underluminous Type IIP SNe (i.e. the archetypal SNe 1997D or 2005cs), showing low photospheric velocities (~2 × 10 3 km s -1 at 50 d) together with features arising from Ba II that are particularly prominent in faint SNe IIP. The peak V-band magnitudes of SN 2013K (-15.6mag) and SN 2013am (-16.2mag) are fainter than standard-luminosity Type IIP SNe. The ejected nickel masses are 0.012 ± 0.010 and 0.015 ± 0.006 M ⊙ for SN 2013K and SN 2013am, respectively. The physical properties of the progenitors at the time of explosion are derived through hydrodynamical modelling. Fitting the bolometric curves, the expansion velocity and the temperature evolution, we infer total ejected masses of 12 and 11.5 M ⊙ , pre- SN radii of~460 and~360 R ⊙ , and explosion energies of 0.34 foe and 0.40 foe for SN 2013K and SN 2013am. Late time spectra are used to estimate the progenitormasses from the strength of nebular emission lines, which turn out to be consistent with red supergiant progenitors of ~15 M ⊙ . For both SNe, a low-energy explosion of a moderate-mass red supergiant star is therefore the favoured scenario.


Epilepsy & Behavior | 2015

FV-137 candidate drug: Novel and selective ion channel modulation for epilepsy and pain

Malik Slassi; Peter Dove; Shane Climie; David O'Neill; Zezhou Wang; Lilly Tsirulnikov; Henrianna; David K.H. Lee; Inés de Lannoy; T.-W. Chen; Jim Stables; Winnie Lau; Leo B. Silenieks; Guy A. Higgins

This corrects the article DOI: 10.1038/nature12569

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M. Fraser

University College Dublin

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C. Inserra

University of Southampton

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S. J. Smartt

Queen's University Belfast

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K. Maguire

Queen's University Belfast

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K. W. Smith

Queen's University Belfast

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Avishay Gal-Yam

Weizmann Institute of Science

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J. P. Anderson

European Southern Observatory

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S. Valenti

University of California

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