M. Nardini
Max Planck Society
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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
Context. The afterglows and host galaxies of long gamma-ray bursts (GRBs) offer unique opportunities to study star-forming galaxies in the high-z Universe. Until recently, however, the information inferred from GRB follow-up observations was mostly limited to optically bright afterglows, biasing all demographic studies against sight-lines that contain large amounts of dust. Aims. Here we present afterglow and host observations for a sample of bursts that are exemplary of previously missed ones because of high visual extinction (A GRB 1 mag) along the sight-line. This facilitates an investigation of the properties, geometry, and location of the absorbing dust of these poorly-explored host galaxies, and a comparison to hosts from optically-selected samples. Methods. This work is based on GROND optical/NIR and Swift/XRT X-ray observations of the afterglows, and multi-color imaging for eight GRB hosts. The afterglow and galaxy spectral energy distributions yield detailed insight into physical properties such as the dust and metal content along the GRB sight-line and galaxy-integrated characteristics such as the host’s stellar mass, luminosity, color-excess, and star-formation rate. Results. For the eight afterglows considered in this study, we report for the first time the redshift of GRB 081109 (z = 0.9787±0.0005), and the visual extinction towards GRBs 081109 (A GRB = 3.4 +0.4 −0.3 mag) and 100621A (A GRB V = 3.8 ± 0.2 mag), which are among the largest ever derived for GRB afterglows. Combined with non-extinguished GRBs, there is a strong anti-correlation between the afterglow’s metal-to-dust ratio and visual extinction. The hosts of the dustiest afterglows are diverse in their properties, but on average redder (� (R − K)AB �∼ 1.6 mag), more luminous (� L �∼ 0.9L ∗ ), and massive (� log M∗[M� ] �∼ 9.8) than the hosts of optically-bright events. Hence, we probe a different galaxy population, suggesting that previous host samples miss most of the massive and metal-rich members. This also indicates that the dust along the sight-line is often related to host properties, and thus probably located in the diffuse ISM or interstellar clouds and not in the immediate GRB environment. Some of the hosts in our sample, are blue, young, or of low stellar mass illustrating that even apparently non-extinguished galaxies possess very dusty sight-lines owing to a patchy dust distribution. Conclusions. The afterglows and host galaxies of the dustiest GRBs provide evidence of a complex dust geometry in star-forming galaxies. In addition, they establish a population of luminous, massive, and correspondingly chemically evolved GRB hosts. This suggests that GRBs trace the global star-formation rate better than studies based on optically selected host samples indicate, and that the previously claimed deficiency of high-mass hosts was at least partially a selection effect.
Astronomy and Astrophysics | 2012
Patricia Schady; T. Dwelly; Mat Page; T. Krühler; J. Greiner; S. R. Oates; M. De Pasquale; M. Nardini; Peter W. A. Roming; A. Rossi; Martin Still
The composition and amount of interstellar dust within gamma-ray burst (GRB) host galaxies is of key importance when addressing selection effects in the GRB redshift distribution, and when studying the properties of their host galaxies. As well as the implications for GRB research, probing the dust within the high-z hosts of GRBs also contributes to our understanding of the conditions of the interstellar medium and star-formation in the distant Universe. Nevertheless, the physical properties of dust within GRB host galaxies continues to be a highly contended issue. In this paper we explore the mean extinction properties of dust within the host galaxies of a sample of 17 GRBs with total host galaxy visual extinction AV 1), which may be indicative of there being a dependence between dust abundance and the wavelength dependence of dust extinction, as has been previously speculated.
Astronomy and Astrophysics | 2012
Patricia Schady; J. Greiner; M. Salvato; M. Ajello; E. Bottacini; N. Gehrels; P. Afonso; J. Elliot; R. Filgas; D. A. Kann; Sylvio Klose; T. Krühler; M. Nardini; A. Nicuesa Guelbenzu; A. Rossi; V. Sudilovsky; Adria C. Updike; Dieter H. Hartmann
Context. Observations of the gamma-ray sky with Fermi led to significant advances towards understanding blazars, the most extreme class of Active Galactic Nuclei. A large fraction of the population detected by Fermi is formed by BL Lacertae (BL Lac) objects, whose sample has always suffered from a severe redshift incompleteness due to the quasi-featureless optical spectra. Aims. Our goal is to provide a significant increase of the number of confirmed high-redshift BL Lac objects contained in the 2 LAC Fermi/LAT catalog. Methods. For 103 Fermi/LAT blazars, photometric redshifts using spectral energy distribution fitting have been obtained. The photometry includes 13 broad-band filters from the far ultraviolet to the near-IR observed with Swift/UVOT and the multi-channel imager GROND at the MPG/ESO 2.2m telescope. Data have been taken quasi-simultaneously and the remaining source-intrinsic variability has been corrected for. Results. We release the UV-to-near-IR 13-band photometry for all 103 sources and provide redshift constraints for 75 sources without previously known redshift. Out of those, eight have reliable photometric redshifts at z > or approx. 1.3, while for the other 67 sources we provide upper limits. Six of the former eight are BL Lac objects, which quadruples the sample of confirmed high-redshift BL Lac. This includes three sources with redshifts higher than the previous record for BL Lac, including CRATES J0402-2615, with the best-fit solution at z approx. = 1.9.
Astronomy and Astrophysics | 2011
R. Filgas; T. Krühler; J. Greiner; Eliana Palazzi; Sylvio Klose; Patricia Schady; A. Rossi; P. Afonso; L. A. Antonelli; C. Clemens; S. Covino; Paolo D'Avanzo; A. Küpcü Yoldas; M. Nardini; A. Nicuesa Guelbenzu; F. E. Olivares; E. A. C. Updike; Aybuke Kupcu Yoldas
Aims. The quick and precise localization of GRBs by the Swift telescope allows the early evolution of the afterglow light curve to be captured by ground-based telescopes. With GROND measurements we can investigate the optical/near-infrared light curve of the afterglow of gamma-ray burst 080413B in the context of late rebrightening. Methods. Multi-wavelength follow-up observations were performed on the afterglow of GRB 080413B. X-ray emission was detected by the X-ray telescope onboard the Swift satellite and obtained from the public archive. Optical and near-infrared photometry was performed with the seven-channel imager GROND mounted at the MPG/ESO 2.2 m telescope and additionally with the REM telescope, both in La Silla, Chile. The light curve model was constructed using the obtained broad-band data. Results. The broad-band light curve of the afterglow of GRB 080413B is well fitted with an on-axis two-component jet model. The narrow ultra-relativistic jet is responsible for the initial decay, while the rise of the moderately relativistic wider jet near its deceleration time is the cause of the rebrightening of the light curve. The later evolution of the optical/NIR light curve is then dominated by the wide component, the signature of which is almost negligible in the X-ray wavelengths. These components have opening angles of θn ∼ 1.7 ◦ and θw ∼ 9 ◦ , and Lorentz factors of Γn > 188 and Γw ∼ 18.5. We calculated the beaming-corrected energy release to be Eγ = 7.9 × 10 48 erg.
Astronomy and Astrophysics | 2012
J. Greiner; Patricia Schady; Sylvio Klose; T. Krühler; P. Afonso; Adria C. Updike; M. Nardini; R. Filgas; A. Nicuesa Guelbenzu; C. Clemens; J. Elliott; D. A. Kann; A. Rossi; V. Sudilovsky
Context. The first observational evidence of a connection between supernovae (SNe) and gamma-ray bursts (GRBs) was found about a decade ago. Since then, only half a dozen spectroscopically confirmed associations have been discovered and XRF 100316D/SN 2010bh is among the latest. Aims. We constrain the progenitor radius, the host-galaxy extinction, and the physical parameters of the explosion of XRF 100316D and its associated SN 2010bh at z = 0.059. We study the brightness and colours of SN 2010bh in the context of GRB-SNe. Methods. We began observations 12 h after the GRB trigger and continued until 80 days after the burst. The Gamma-Ray burst Optical and Near-infrared Detector (GROND) provided excellent photometric data of XRF 100316D/SN 2010bh in six filter bands covering a wavelength range from approximately 350 to 1800 nm, significantly expanding the pre-existing data set for this event. Combining GROND and Swift data, the early broad-band spectral energy distribution (SED) is modelled with a blackbody and afterglow component attenuated by dust and gas absorption. The temperature and radius evolution of the thermal component are analysed and combined with earlier measurements available from the literature. Templates of SN 1998bw are fitted to the SN itself to directly compare the light-curve properties. Finally, a two-component parametrised model is fitted to the quasi-bolometric light curve, which delivers physical parameters of the explosion. Results. The best-fit models to the broad-band SEDs imply moderate reddening along the line of sight through the host galaxy (AV,host = 1.2 ± 0.1 mag). Furthermore, the parameters of the blackbody component reveal a cooling envelope at an apparent initial radius of 7 × 10 11 cm, which is compatible with a dense wind surrounding a Wolf-Rayet star. A multicolour comparison shows that SN 2010bh is 60–70% as bright as SN 1998bw. It proves to be the most rapidly evolving GRB-SNe to date, reaching maximum brightness at 8–9 days after the burst in the blue bands. Modelling of the quasi-bolometric light curve yields MNi = 0.21 ± 0.03 M� and Mej = 2.6 ± 0.2 M� , typical of values within the GRB-SN population. The kinetic energy is Ek = (2.4 ± 0.7) × 10 52 erg, which is making this SN the second most energetic GRB-SN after SN 1998bw. Conclusions. This supernova has one of the earliest peaks ever recorded and thereafter fades more rapidly than other GRB-SNe, hypernovae, or typical type-Ic SNe. This implies that a thin envelope is possibly expanding at very high velocities and is, therefore, unable to retain the γ-rays that would prolong the duration of the SN event.
Astronomy and Astrophysics | 2011
R. Filgas; J. Greiner; Patricia Schady; T. Krühler; Adria C. Updike; Sylvio Klose; M. Nardini; D. A. Kann; A. Rossi; V. Sudilovsky; P. Afonso; C. Clemens; J. Elliott; A. Nicuesa Guelbenzu
Aims. Using high-quality, broad-band afterglow data for GRB 091127, we investigate the validity of the synchrotron fireball model for gamma-ray bursts (GRBs), and infer physical parameters of the ultra-relativistic outflow. Methods. We used multi-wavelength (NIR to X-ray) follow-up observations obtained with GROND simultaneously in the grizJH filters and the XRT onboard the Swift satellite in the 0.3 to 10 keV energy range. The resulting afterglow light curve is of excellent accuracy with relative photometric errors as low as 1%, and the spectral energy distribution (SED) is well-sampled over 5 decades in energy. These data present one of the most comprehensive observing campaigns for a single GRB afterglow and allow us to test several proposed emission models and outflow characteristics in unprecedented detail. Results. Both the multi-color light curve and the broad-band SED of the afterglow of GRB 091127 show evidence of a cooling break moving from high to lower energies. The early light curve is well described by a broken power-law, where the initial decay in the optical/NIR wavelength range is considerably flatter than at X-rays. Detailed fitting of the time-resolved SED shows that the break is very smooth with a sharpness index of 2.2 ± 0.2, and evolves towards lower frequencies as a power-law with index −1.23 ± 0.06. These are the first accurate and contemporaneous measurements of both the sharpness of the spectral break and its time evolution. Conclusions. The measured evolution of the cooling break (νc ∝ t ∼−1.2 ) is not consistent with the predictions of the standard model, wherein νc ∝ t ∼−0.5 is expected. A possible explanation for the observed behavior is a time dependence of the microphysical parame- ters, in particular the fraction of the total energy in the magnetic fieldB. This conclusion provides further evidence that the standard fireball model is too simplistic, and time-dependent micro-physical parameters may be required to model the growing number of well-sampled afterglow light curves.
Astronomy and Astrophysics | 2011
M. Nardini; J. Greiner; T. Krühler; R. Filgas; Sylvio Klose; P. M. J. Afonso; C. Clemens; A. N. Guelbenzu; F. E. Olivares; A. Rossi; Adria C. Updike; A. Küpcü Yoldas; A. Yoldas; D. Burlon; J. Elliot; D. A. Kann
Context. After the launch of the Swift satellite, the gamma-ray burst (GRB) optical light-curve smoothness paradigm has been questioned thanks to the faster and better sampled optical follow-up, which has unveiled a very complex behaviour. This complexity is triggering the interest of the whole GRB community. The GROND multi-channel imager is used to study optical and near-infrared (NIR) afterglows of GRBs with unprecedented optical and near-infrared temporal and spectral resolution. The GRB 081029 has a very prominent optical rebrightening event and is an outstanding example of the application of the multi-channel imager to GRB afterglows. Aims. Here we exploit the rich GROND multi-colour follow-up of GRB 081029 combined with XRT observations to study the nature of late-time rebrightenings that appear in the optical-NIR light-curves of some GRB afterglows. Methods. We analyse the optical and NIR observations obtained with the seven-channel Gamma-Ray burst Optical and Near-infrared Detector (GROND) at the 2.2 m MPI/ESO telescope and the X-ray data obtained with the XRT telescope on board the Swift observatory. The multi-wavelength temporal and spectral evolution is discussed in the framework of different physical models. Results. The extremely steep optical and NIR rebrightening observed in GRB 081029 cannot be explained in the framework of the standard forward shock afterglow model. The absence of a contemporaneous X-ray rebrightening and the evidence of a strong spectral evolution in the optical-NIR bands during the rise suggest two separate components that dominate in the early and late-time lightcurves, respectively. The steepness of the optical rise cannot be explained even in the framework of the alternative scenarios proposed in the literature unless a late-time activity of the central engine is assumed.
Astronomy and Astrophysics | 2011
T. Krühler; Patricia Schady; J. Greiner; P. Afonso; E. Bottacini; C. Clemens; R. Filgas; Sylvio Klose; T. S. Koch; A. Kupcu-Yoldas; S. R. Oates; Mat Page; Sheila McBreen; M. Nardini; A. Nicuesa Guelbenzu; P. W. A. Roming; A. Rossi; Adria C. Updike; Aybuke Kupcu Yoldas
Aims. We present a framework to obtain photometric redshifts (photo-zs) for gamma-ray burst afterglows. Using multi-band photometry from GROND and Swift/UVOT, photo-zs are derived for five GRBs for which spectroscopic redshifts are not available. Methods. We use UV/optical/NIR data and synthetic photometry based on afterglow observations and theory to derive the photometric redshifts of GRBs and their accuracy. Taking into account the afterglow synchrotron emission properties, we investigate the application of photometry to derive redshifts in a theoretical range between z ∼ 1t oz ∼ 12. Results. The measurement of photo-zs for GRB afterglows provides a quick, robust and reliable determination of the distance scale to the burst, particularly in those cases where spectroscopic observations in the optical/NIR range cannot be obtained. Given a sufficiently bright and mildly reddened afterglow, the relative photo-z accuracy η =Δ z/(1 + z) is better than 10% between z = 1. 5a nd z ∼ 7 and better than 5% between z = 2a ndz = 6. We detail the approach on 5 sources without spectroscopic redshifts observed with
Astronomy and Astrophysics | 2011
D. Gruber; T. Krühler; S. Foley; M. Nardini; D. Burlon; E. Bissaldi; A. von Kienlin; S. McBreen; J. Greiner; P. N. Bhat; M. S. Briggs; J. M. Burgess; Vandiver Chaplin; V. Connaughton; R. Diehl; G. J. Fishman; M. H. Gibby; Adam Goldstein; S. Guiriec; A. J. van der Horst; R. M. Kippen; C. Kouveliotou; Lin Lin; Charles A. Meegan; W. S. Paciesas; Robert D. Preece; D. Tierney; C. Wilson-Hodge
Aims. In this paper we examine gamma-ray and optical data of GRB 091024, a gamma-ray burst (GRB) with an extremely long duration of T90 ≈ 1020 s, as observed with the Fermi Gamma-ray Burst Monitor (GBM). Methods. We present spectral analysis of all three distinct emission episodes using data from Fermi/GBM. Because of the long nature of this event, many ground-based optical telescopes slewed to its location within a few minutes and thus were able to observe the GRB during its active period. We compare the optical and gamma-ray light curves. Furthermore, we estimate a lower limit on the bulk Lorentz factor from the variability and spectrum of the GBM light curve and compare it with that obtained from the peak time of the forward shock of the optical afterglow. Results. From the spectral analysis we note that, despite its unusually long duration, this burst is similar to other long GRBs, i.e. there is spectral evolution (both the peak energy and the spectral index vary with time) and spectral lags are measured. We find that the optical light curve is highly anti-correlated to the prompt gamma-ray emission, with the optical emission reaching the maximum during an epoch of quiescence in the prompt emission. We interpret this behavior as the reverse shock (optical flash), expected in the internal-external shock model of GRB emission but observed only in a handful of GRBs so far. The lower limit on the initial Lorentz factor deduced from the variability time scale (Γmin = 195 +90 −110) is consistent within the error to the one obtained using the peak time of the forward shock (Γ0 = 120) and is also consistent with Lorentz factors of other long GRBs.
Astronomy and Astrophysics | 2011
A. Nicuesa Guelbenzu; Sylvio Klose; A. Rossi; D. A. Kann; T. Krühler; J. Greiner; F. E. Olivares; P. Afonso; R. Filgas; A. Küpcü Yoldas; Sheila McBreen; M. Nardini; Patricia Schady; S. Schmidl; Adria C. Updike; A. Yoldas
Context. The link between the duration of GRBs and the nature of their progenitors remains disputed. Short bursts (with durations of less than ∼2 s) are less frequently observed, technically more difficult to localize, and exhibit significantly fainter afterglows. Aims. It is of critical importance to establish whether the burst duration can reliably distinguish the different GRB population models of collapsars and compact stellar mergers. The Swift GRB 090426 provides an unique opportunity to address this question. Its duration (T90 = 1.28 s) places GRB 090426 firmly in the short burst population, while the high redshift (z = 2.609), host galaxy properties, and prompt emission spectral characteristics are more similar to those of long-duration GRBs. Methods. On the basis of data obtained with the Tautenburg 2 m telescope (Germany) and the 7-channel imager GROND (La Silla, Chile), we compiled the most finely sampled light curve available for a short burst optical/NIR afterglow. The light curve was then analysed in a standard fashion. GROND and XRT data were used to determine the broad-band spectral energy distribution of the afterglow across more than three orders of magnitude. Results. Our data show that a light curve break exists at 0.4 days, which is followed by a steep decay. This light curve decay is achromatic in the optical/NIR bands, and interpreted as a post-jet break phase. The X-ray data do not disagree with this interpretation. Conclusions. The half-opening angle of the suspected jet as well as the luminosity of the optical afterglow provide additional evidence that GRB 090426 is probably linked to the death of a massive star rather than to the merger of two compact objects.