D. A. Kann
Spanish National Research Council
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Featured researches published by D. A. Kann.
Nature | 2006
E. Pian; Paolo A. Mazzali; N. Masetti; P. Ferrero; Sylvio Klose; Eliana Palazzi; Enrico Ramirez-Ruiz; S. E. Woosley; C. Kouveliotou; J. S. Deng; A. V. Filippenko; Ryan J. Foley; J. P. U. Fynbo; D. A. Kann; Weidong Li; J. Hjorth; K. Nomoto; Ferdinando Patat; Daniel Sauer; Jesper Sollerman; Paul M. Vreeswijk; E. W. Guenther; A. Levan; Paul T. O'Brien; Nial R. Tanvir; R. A. M. J. Wijers; Christophe Dumas; Olivier R. Hainaut; Diane S. Wong; Dietrich Baade
Long-duration γ-ray bursts (GRBs) are associated with type Ic supernovae that are more luminous than average and that eject material at very high velocities. Less-luminous supernovae were not hitherto known to be associated with GRBs, and therefore GRB–supernovae were thought to be rare events. Whether X-ray flashes—analogues of GRBs, but with lower luminosities and fewer γ-rays—can also be associated with supernovae, and whether they are intrinsically ‘weak’ events or typical GRBs viewed off the axis of the burst, is unclear. Here we report the optical discovery and follow-up observations of the type Ic supernova SN 2006aj associated with X-ray flash XRF 060218. Supernova 2006aj is intrinsically less luminous than the GRB–supernovae, but more luminous than many supernovae not accompanied by a GRB. The ejecta velocities derived from our spectra are intermediate between these two groups, which is consistent with the weakness of both the GRB output and the supernova radio flux. Our data, combined with radio and X-ray observations, suggest that XRF 060218 is an intrinsically weak and soft event, rather than a classical GRB observed off-axis. This extends the GRB–supernova connection to X-ray flashes and fainter supernovae, implying a common origin. Events such as XRF 060218 are probably more numerous than GRB–supernovae.
Astrophysical Journal Supplement Series | 2009
J. P. U. Fynbo; P. Jakobsson; Jason X. Prochaska; Daniele Malesani; Cedric Ledoux; A. de Ugarte Postigo; M. Nardini; Paul M. Vreeswijk; K. Wiersema; J. Hjorth; Jesper Sollerman; H.-. W. Chen; C. C. Thöne; G. Björnsson; J. S. Bloom; A. J. Castro-Tirado; L. Christensen; A. De Cia; Andrew S. Fruchter; J. Gorosabel; John F. Graham; Andreas O. Jaunsen; B. L. Jensen; D. A. Kann; C. Kouveliotou; Andrew J. Levan; Justyn R. Maund; N. Masetti; B. Milvang-Jensen; Eliana Palazzi
We present a sample of 77 optical afterglows (OAs) of Swift detected gamma-ray bursts (GRBs) for which spectroscopic follow-up observations have been secured. Our first objective is to measure the redshifts of the bursts. For the majority (90%) of the afterglows, the redshifts have been determined from the spectra. We provide line lists and equivalent widths (EWs) for all detected lines redward of Lyα covered by the spectra. In addition to the GRB absorption systems, these lists include line strengths for a total of 33 intervening absorption systems. We discuss to what extent the current sample of Swift bursts with OA spectroscopy is a biased subsample of all Swift detected GRBs. For that purpose we define an X-ray-selected statistical sample of Swift bursts with optimal conditions for ground-based follow-up from the period 2005 March to 2008 September; 146 bursts fulfill our sample criteria. We derive the redshift distribution for the statistical (X-ray selected) sample and conclude that less than 18% of Swift bursts can be at z > 7. We compare the high-energy properties (e.g., γ-ray (15-350 keV) fluence and duration, X-ray flux, and excess absorption) for three subsamples of bursts in the statistical sample: (1) bursts with redshifts measured from OA spectroscopy; (2) bursts with detected optical and/or near-IR afterglow, but no afterglow-based redshift; and (3) bursts with no detection of the OA. The bursts in group (1) have slightly higher γ-ray fluences and higher X-ray fluxes and significantly less excess X-ray absorption than bursts in the other two groups. In addition, the fractions of dark bursts, defined as bursts with an optical to X-ray slope βOX 39% in group (3). For the full sample, the dark burst fraction is constrained to be in the range 25%-42%. From this we conclude that the sample of GRBs with OA spectroscopy is not representative for all Swift bursts, most likely due to a bias against the most dusty sight lines. This should be taken into account when determining, e.g., the redshift or metallicity distribution of GRBs and when using GRBs as a probe of star formation. Finally, we characterize GRB absorption systems as a class and compare them to QSO absorption systems, in particular the damped Lyα absorbers (DLAs). On average GRB absorbers are characterized by significantly stronger EWs for H I as well as for both low and high ionization metal lines than what is seen in intervening QSO absorbers. However, the distribution of line strengths is very broad and several GRB absorbers have lines with EWs well within the range spanned by QSO-DLAs. Based on the 33 z > 2 bursts in the sample, we place a 95% confidence upper limit of 7.5% on the mean escape fraction of ionizing photons from star-forming galaxies. Based on observations collected at the European Organisation for Astronomical Research in the Southern Hemisphere, Chile, under programs 275.D-5022 (PI: Chincarini), 075.D-0270 (PI: Fynbo), 077.D-0661 (PI: Vreeswijk), 077.D-0805 (PI: Tagliaferri), 177.A-0591 (PI: Hjorth), 078.D-0416 (PI: Vreeswijk), 079.D-0429 (PI: Vreeswijk), 080.D-0526 (PI: Vreeswijk), 081.A-0135 (PI: Greiner), 281.D-5002 (PI: Della Valle), and 081.A-0856 (PI: Vreeswijk). Also based on observations made with the Nordic Optical Telescope, operated on the island of La Palma jointly by Denmark, Finland, Iceland, Norway, and Sweden, in the Spanish Observatorio del Roque de los Muchachos of the Instituto de Astrofisica de Canarias. Some of the data obtained herein were obtained at the W.M. Keck Observatory, which is operated as a scientific partnership among the California Institute of Technology, the University of California, and the National Aeronautics and Space Administration. The Observatory was made possible by the generous financial support of the W.M. Keck foundation.
The Astrophysical Journal | 2010
D. A. Kann; Sylvio Klose; Bin-Bin Zhang; Daniele Malesani; Ehud Nakar; Alexei S. Pozanenko; A. C. Wilson; N. Butler; P. Jakobsson; S. Schulze; M. Andreev; L. A. Antonelli; I. Bikmaev; Vadim Biryukov; M. Böttcher; R. A. Burenin; J. M. Castro Cerón; A. J. Castro-Tirado; Guido Chincarini; Bethany Elisa Cobb; S. Covino; P. D'Avanzo; Valerio D'Elia; M. Della Valle; A. de Ugarte Postigo; Yu. S. Efimov; P. Ferrero; Dino Fugazza; J. P. U. Fynbo; M. Gålfalk
We have gathered optical photometry data from the literature on a large sample of Swift-era gamma-ray burst (GRB) afterglows including GRBs up to 2009 September, for a total of 76 GRBs, and present an additional three pre-Swift GRBs not included in an earlier sample. Furthermore, we publish 840 additional new photometry data points on a total of 42 GRB afterglows, including large data sets for GRBs 050319, 050408, 050802, 050820A, 050922C, 060418, 080413A, and 080810. We analyzed the light curves of all GRBs in the sample and derived spectral energy distributions for the sample with the best data quality, allowing us to estimate the host-galaxy extinction. We transformed the afterglow light curves into an extinction-corrected z = 1 system and compared their luminosities with a sample of pre-Swift afterglows. The results of a former study, which showed that GRB afterglows clustered and exhibited a bimodal distribution in luminosity space, are weakened by the larger sample. We found that the luminosity distribution of the two afterglow samples (Swift-era and pre-Swift) is very similar, and that a subsample for which we were not able to estimate the extinction, which is fainter than the main sample, can be explained by assuming a moderate amount of line-of-sight host extinction. We derived bolometric isotropic energies for all GRBs in our sample, and found only a tentative correlation between the prompt energy release and the optical afterglow luminosity at 1 day after the GRB in the z = 1 system. A comparative study of the optical luminosities of GRB afterglows with echelle spectra (which show a high number of foreground absorbing systems) and those without, reveals no indication that the former are statistically significantly more luminous. Furthermore, we propose the existence of an upper ceiling on afterglow luminosities and study the luminosity distribution at early times, which was not accessible before the advent of the Swift satellite. Most GRBs feature afterglows that are dominated by the forward shock from early times on. Finally, we present the first indications of a class of long GRBs, which form a bridge between the typical high-luminosity, high-redshift events and nearby low-luminosity events (which are also associated with spectroscopic supernovae) in terms of energetics and observed redshift distribution, indicating a continuous distribution overall.
Archive | 2017
Ligo Sci, Virgo, Antares; other Collaborations; Z. Cano; Antonio de Ugarte Postigo; Cristina Carina Thöne; G. Hodosan; D. A. Kann; L. Izzo; Alberto J. Castro-Tirado; J. C. Tello; Y. D. Hu; Bin-Bin Zhang; Ronan Cunniffe; I. Agudo
On 2017 August 17 a binary neutron star coalescence candidate (later designated GW170817) with merger time 12:41:04 UTC was observed through gravitational waves by the Advanced LIGO and Advanced Virgo detectors. The Fermi Gamma-ray Burst Monitor independently detected a gamma-ray burst (GRB 170817A) with a time delay of
The Astrophysical Journal | 2006
D. A. Kann; Sylvio Klose; A. Zeh
\sim 1.7\,{\rm{s}}
The Astrophysical Journal | 2011
D. A. Kann; Sylvio Klose; Bing Zhang; S. Covino; N. Butler; Daniele Malesani; Ehud Nakar; A. C. Wilson; L. A. Antonelli; Guido Chincarini; Bethany Elisa Cobb; Paolo D'Avanzo; Valerio D'Elia; M. Della Valle; P. Ferrero; Dino Fugazza; J. Gorosabel; G. L. Israel; F. Mannucci; S. Piranomonte; S. Schulze; L. Stella; G. Tagliaferri; K. Wiersema
with respect to the merger time. From the gravitational-wave signal, the source was initially localized to a sky region of 31 deg2 at a luminosity distance of
Astronomy and Astrophysics | 2011
T. Krühler; J. Greiner; Patricia Schady; Sandra Savaglio; P. Afonso; C. Clemens; J. Elliot; R. Filgas; D. Gruber; D. A. Kann; Sylvio Klose; A. Küpcü-Yoldaş; Sheila McBreen; F. E. Olivares; D. Pierini; A. Rossi; M. Nardini; A. Nicuesa Guelbenzu; V. Sudilovsky; Adria C. Updike
{40}_{-8}^{+8}
Astronomy and Astrophysics | 2006
P. Jakobsson; J. P. U. Fynbo; Cedric Ledoux; Paul M. Vreeswijk; D. A. Kann; J. Hjorth; Robert S. Priddey; Nial R. Tanvir; Daniel E. Reichart; J. Gorosabel; Sylvio Klose; D. Watson; Jesper Sollerman; Andrew S. Fruchter; A. de Ugarte Postigo; Klaas Wiersema; G. Björnsson; R. Chapman; C. C. Thöne; B. L. Jensen
Mpc and with component masses consistent with neutron stars. The component masses were later measured to be in the range 0.86 to 2.26
Astronomy and Astrophysics | 2010
S. McBreen; T. Krühler; J. Greiner; D. A. Kann; Sandra Savaglio; P. Afonso; C. Clemens; R. Filgas; Sylvio Klose; A. Küpüc Yoldas; A. Rossi; G. P. Szokoly; Adria C. Updike; Aybuke Kupcu Yoldas
\,{M}_{\odot }
The Astrophysical Journal | 2006
A. Zeh; Sylvio Klose; D. A. Kann
. An extensive observing campaign was launched across the electromagnetic spectrum leading to the discovery of a bright optical transient (SSS17a, now with the IAU identification of AT 2017gfo) in NGC 4993 (at