Massimo Della Valle
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Science | 2008
Paolo A. Mazzali; S. Valenti; Massimo Della Valle; Guido Chincarini; Daniel N. Sauer; Stefano Benetti; E. Pian; Tsvi Piran; Valerio D'Elia; N. Elias-Rosa; Raffaella Margutti; F. Pasotti; L. Angelo Antonelli; F. Bufano; Sergio Campana; E. Cappellaro; S. Covino; Paolo D'Avanzo; F. Fiore; Dino Fugazza; Roberto Gilmozzi; Deborah Hunter; K. Maguire; E. Maiorano; Paola Marziani; Nicola Masetti; Felix I. Mirabel; H. Navasardyan; K. Nomoto; Eliana Palazzi
The only supernovae (SNe) to show gamma-ray bursts (GRBs) or early x-ray emission thus far are overenergetic, broad-lined type Ic SNe (hypernovae, HNe). Recently, SN 2008D has shown several unusual features: (i) weak x-ray flash (XRF), (ii) an early, narrow optical peak, (iii) disappearance of the broad lines typical of SN Ic HNe, and (iv) development of helium lines as in SNe Ib. Detailed analysis shows that SN 2008D was not a normal supernova: Its explosion energy (E ≈ 6×1051 erg) and ejected mass [∼7 times the mass of the Sun (\batchmode \documentclass[fleqn,10pt,legalpaper]{article} \usepackage{amssymb} \usepackage{amsfonts} \usepackage{amsmath} \pagestyle{empty} \begin{document} \(M_{{\odot}}\) \end{document})] are intermediate between normal SNe Ibc and HNe. We conclude that SN 2008D was originally a ∼30 \batchmode \documentclass[fleqn,10pt,legalpaper]{article} \usepackage{amssymb} \usepackage{amsfonts} \usepackage{amsmath} \pagestyle{empty} \begin{document} \(M_{{\odot}}\) \end{document} star. When it collapsed, a black hole formed and a weak, mildly relativistic jet was produced, which caused the XRF. SN 2008D is probably among the weakest explosions that produce relativistic jets. Inner engine activity appears to be present whenever massive stars collapse to black holes.
Monthly Notices of the Royal Astronomical Society | 2011
Dan Maoz; Filippo Mannucci; Weidong Li; Alexei V. Filippenko; Massimo Della Valle; Nino Panagia
Recovery of the supernova (SN) delay-time distribution (DTD) – the SN rate versus time that would follow a hypothetical brief burst of star formation – can shed light on SN progenitors and physics, as well as on the time-scales of chemical enrichment. Previous attempts to reconstruct the DTD have been based either on comparison of mean SN rates versus redshift to cosmic star-formation history (SFH), or on the comparison of SN rates among galaxies with different mean ages. Here, we present an approach to recover the SN DTD that avoids the averaging and loss of information of other schemes. We compare the SFHs of individual galaxies to the numbers of SNe discovered by a survey in each galaxy (generally zero, sometimes one SN, rarely a few). We apply the method to a subsample of 3505 galaxies, hosting 82 type-Ia SNe (SNe Ia) and 119 core-collapse supernovae (CC SNe), from the Lick Observatory Supernova Search (LOSS), that have SFHs reconstructed from Sloan Digital Sky Survey (SDSS) spectra. We find a >2σ SN Ia DTD signal in our shortest-delay, ‘prompt’ bin at 99 per cent confidence level. We further find a 4σ indication of SNe Ia that are ‘delayed’ by >2.4 Gyr. Thus, the data support the existence of both prompt and delayed SNe Ia. We measure the time integral over the SN DTD. For CC SNe we find a total yield of 0.010 ± 0.002
The Astrophysical Journal | 2006
Paolo A. Mazzali; J. S. Deng; E. Pian; Daniele Malesani; Nozomu Tominaga; Keiichi Maeda; K. Nomoto; Guido Chincarini; S. Covino; Massimo Della Valle; Dino Fugazza; Gianpiero Tagliaferri; Avishay Gal-Yam
The gamma-ray burst GRB 031203 at a redshift z = 0.1055 revealed a highly reddened Type Ic supernova, SN 2003lw, in its afterglow light. This is the third well-established case of a link between a long-duration GRB and a Type Ic SN. The SN light curve is obtained by subtracting the galaxy contribution and is modeled together with two spectra at near-maximum epochs. A red VLT grism 150I spectrum of the SN near peak is used to extend the spectral coverage, and in particular to constrain the uncertain reddening, the most likely value for which is EG+H(B - V) 1.07 ± 0.05. Accounting for reddening, SN 2003lw is ~0.3 mag brighter than the prototypical GRB-SN 1998bw. Light curve models yield a 56Ni mass of ~0.55 M☉. The optimal explosion model is somewhat more massive (Mej ~ 13 M☉) and more energetic (E ~ 6 × 1052 ergs) than the model for SN 1998bw, implying a massive progenitor (40-50 M☉). The mass at high velocity is not very large (1.4 M☉ above 30,000 km s-1, but only 0.1 M☉ above 60,000 km s-1), but it is sufficient to cause the observed broad lines. The similarity of SNe 2003lw and 1998bw and the weakness of their related GRBs, GRB 031203 and GRB 980425, suggest that both GRBs may be normal events viewed slightly off-axis or a weaker but possibly more frequent type of GRB.
Nature | 2012
Matthew Middleton; J. C. A. Miller-Jones; Sera Markoff; R. P. Fender; Martin Henze; Natasha Hurley-Walker; Anna M. M. Scaife; T. P. Roberts; D. J. Walton; John M. Carpenter; J.-P. Macquart; Geoffrey C. Bower; M. A. Gurwell; W. Pietsch; F. Haberl; J. Harris; M. K. Daniel; Junayd Miah; Chris Done; J. Morgan; H. J. Dickinson; P. A. Charles; Vadim Burwitz; Massimo Della Valle; Michael J. Freyberg; J. Greiner; Margarita Hernanz; Dieter H. Hartmann; D. Hatzidimitriou; Arno Riffeser
A subset of ultraluminous X-ray sources (those with luminosities of less than 1040 erg s−1; ref. 1) are thought to be powered by the accretion of gas onto black holes with masses of ∼5–20, probably by means of an accretion disk. The X-ray and radio emission are coupled in such Galactic sources; the radio emission originates in a relativistic jet thought to be launched from the innermost regions near the black hole, with the most powerful emission occurring when the rate of infalling matter approaches a theoretical maximum (the Eddington limit). Only four such maximal sources are known in the Milky Way, and the absorption of soft X-rays in the interstellar medium hinders the determination of the causal sequence of events that leads to the ejection of the jet. Here we report radio and X-ray observations of a bright new X-ray source in the nearby galaxy M 31, whose peak luminosity exceeded 1039 erg s−1. The radio luminosity is extremely high and shows variability on a timescale of tens of minutes, arguing that the source is highly compact and powered by accretion close to the Eddington limit onto a black hole of stellar mass. Continued radio and X-ray monitoring of such sources should reveal the causal relationship between the accretion flow and the powerful jet emission.
The Astrophysical Journal | 2012
F. Bufano; E. Pian; Jesper Sollerman; Stefano Benetti; Giuliano Pignata; S. Valenti; S. Covino; Paolo D'Avanzo; Daniele Malesani; E. Cappellaro; Massimo Della Valle; Johan Peter Uldall Fynbo; J. Hjorth; Paolo A. Mazzali; Daniel E. Reichart; Rhaana L. C. Starling; Massimo Turatto; S. D. Vergani; K. Wiersema; L. Amati; D. F. Bersier; Sergio Campana; Z. Cano; A. J. Castro-Tirado; Guido Chincarini; Valerio D'Elia; Antonio de Ugarte Postigo; J. S. Deng; P. Ferrero; Alexei V. Filippenko
Wepresentthespectroscopicandphotometricevolutionofthenearby(z = 0.059)spectroscopicallyconfirmedType Ic supernova, SN 2010bh, associated with the soft, long-duration gamma-ray burst (X-ray flash) GRB 100316D. Intensive follow-up observations of SN 2010bh were performed at the ESO Very Large Telescope (VLT) using the X-shooter and FORS2 instruments. Thanks to the detailed temporal coverage and the extended wavelength range (3000‐24800 A), we obtained an unprecedentedly rich spectral sequence among the hypernovae, making SN 2010bh one of the best studied representatives of this SN class. We find that SN 2010bh has a more rapid rise to maximum brightness (8.0 ± 1.0 rest-frame days) and a fainter absolute peak luminosity (Lbol ≈ 3 × 10 42 ergs −1 ) than previously observed SN events associated with GRBs. Our estimate of the ejected 56 Ni mass is 0.12±0.02 M� . From the broad spectral features, we measure expansion velocities up to 47,000 km s −1 , higher than those of SNe 1998bw (GRB 980425) and 2006aj (GRB 060218). Helium absorption lines Hei λ5876 and Hei 1.083 μm, blueshifted by ∼20,000‐30,000 km s −1 and ∼28,000‐38,000 km s −1 , respectively, may be present in the optical spectra. However, the lack of coverage of the Hei 2.058 μm line prevents us from confirming such identifications. The nebular spectrum, taken at ∼186 days after the explosion, shows a broad but faint [Oi] emission at 6340 A. The light curve shape and photospheric expansion velocities of SN 2010bh suggest that we witnessed a highly energetic
The Astrophysical Journal | 2005
Massimo Della Valle; Nino Panagia; Paolo Padovani; E. Cappellaro; Filippo Mannucci; Massimo Turatto
Space Telescope Science Institute, 3700 San Martin Drive, Baltimore, MD 21218Paolo PadovaniEuropean Southern Observatory, Karl-Schwarzschild-Strasse 2, Garching bei Mu¨nchen,GermanyEnrico CappellaroIstituto Nazionale di Astrofisica, Osservatorio Astronomico di CapodimonteSalita Moiariello, 16, I-80131, Napoli, ItalyFilippo MannucciCNR-IRALargo Enrico Fermi 5, I-50125 Florence, ItalyMassimo TurattoIstituto Nazionale di Astrofisica, Osservatorio Astronomico di Padova,Vicolo Osservatorio 5, Padova, ItalyReceived ; acceptedsubmitted to the Ap.J.
The Astrophysical Journal | 2009
Cody Raskin; Evan Scannapieco; James E. Rhoads; Massimo Della Valle
The time delay between the formation of a population of stars and the onset of type Ia supernovae (SNe Ia) sets important limits on the masses and nature of SN Ia progenitors. Here, we use a new observational technique to measure this time delay by comparing the spatial distributions of SNe Ia to their local environments. Previous work attempted such analyses encompassing the entire host of each SN Ia, yielding inconclusive results. Our approach confines the analysis only to the relevant portions of the hosts, allowing us to show that even so-called prompt SNe Ia that trace star formation on cosmic timescales exhibit a significant delay time of 200-500 million years. This implies that either the majority of Ia companion stars have main-sequence masses less than 3 M ☉, or that most SNe Ia arise from double white dwarf binaries. Our results are also consistent with a SNe Ia rate that traces the white dwarf formation rate, scaled by a fixed efficiency factor.
The Astrophysical Journal | 2009
Masaomi Tanaka; Masayuki Yamanaka; Keiichi Maeda; Koji S. Kawabata; Takashi Hattori; Takeo Minezaki; S. Valenti; Massimo Della Valle; D. K. Sahu; G. C. Anupama; Nozomu Tominaga; K. Nomoto; Paolo A. Mazzali; E. Pian
We present optical spectroscopic and photometric observations of supernova (SN) 2008D, associated with the luminous X-ray transient 080109, at >300 days after the explosion (nebular phases). We also give flux measurements of emission lines from the H II region at the site of the SN, and estimates of the local metallicity. The brightness of the SN at nebular phases is consistent with the prediction of the explosion models with an ejected {sup 56}Ni mass of 0.07 M{sub sun}, which explains the light curve at early phases. The [O I] line in the nebular spectrum shows a double-peaked profile while the [Ca II] line does not. The double-peaked [O I] profile strongly indicates that SN 2008D is an aspherical explosion. The profile can be explained by a torus-like distribution of oxygen viewed from near the plane of the torus. We suggest that SN 2008D is a side-viewed, bipolar explosion with a viewing angle of >50 deg. from the polar direction.
The Astrophysical Journal | 2008
Robert E. Williams; E. Mason; Massimo Della Valle; Alessandro Ederoclite
A high-resolution spectroscopic survey of post-outburst novae reveals short-lived heavy element absorption systems in a majority of novae near maximum light, having expansion velocities of 400-1000 km s−1 and velocity dispersions between 35 and 350 km s−1. A majority of systems are accelerated outward, and they all progressively weaken and disappear over timescales of weeks. A few of the systems having narrow, deeper absorption reveal a rich spectrum of singly ionized Sc, Ti, V, Cr, Fe, Sr, Y, Zr, and Ba lines. Analysis of the richest such system, in LMC 2005, shows the excitation temperature to be 104 K and elements lighter than Fe to have abundance enhancements over solar values by up to an order of magnitude. The gas causing the absorption systems must be circumbinary and its origin is most likely mass ejection from the secondary star. The absorbing gas exists before the outburst and may represent episodic mass transfer events from the secondary star that initiate the nova outburst(s). If SNe Ia originate in single degenerate binaries, such absorption systems could be detectable before maximum light.
The Astrophysical Journal | 2012
Xiaofeng Wang; Lifan Wang; Alexei V. Filippenko; E. Baron; M. Kromer; D. Jack; Tianmeng Zhang; G. Aldering; P. Antilogus; W. David Arnett; Dietrich Baade; Brian J. Barris; Stefano Benetti; P. Bouchet; Adam Burrows; R. Canal; E. Cappellaro; Raymond G. Carlberg; Elisa di Carlo; Peter J. Challis; Arlin P. S. Crotts; J. Danziger; Massimo Della Valle; M. Fink; Ryan J. Foley; Claes Fransson; Avishay Gal-Yam; Peter Marcus Garnavich; Christopher Lowell Gerardy; Gerson Goldhaber
We present ultraviolet (UV) spectroscopy and photometry of four Type Ia supernovae (SNe 2004dt, 2004ef, 2005M, and 2005cf) obtained with the UV prism of the Advanced Camera for Surveys on the Hubble Space Telescope. This data set provides unique spectral time series down to 2000 A. Significant diversity is seen in the near-maximum-light spectra (~2000-3500 A) for this small sample. The corresponding photometric data, together with archival data from Swift Ultraviolet/Optical Telescope observations, provide further evidence of increased dispersion in the UV emission with respect to the optical. The peak luminosities measured in the uvw1/F250W filter are found to correlate with the B-band light-curve shape parameter Δm 15(B), but with much larger scatter relative to the correlation in the broadband B band (e.g., ~0.4 mag versus ~0.2 mag for those with 0.8 mag 3σ), being brighter than normal SNe Ia such as SN 2005cf by ~0.9 mag and ~2.0 mag in the uvw1/F250W and uvm2/F220W filters, respectively. We show that different progenitor metallicity or line-expansion velocities alone cannot explain such a large discrepancy. Viewing-angle effects, such as due to an asymmetric explosion, may have a significant influence on the flux emitted in the UV region. Detailed modeling is needed to disentangle and quantify the above effects.