Reports from Observers The Short Gamma-Ray Burst Revolution Jens Hjorth1 the afterglow light-curve properties and Afterglows – found! Andrew Levan ,3 possible high-redshift origin of some Nial Tanvir 4 short bursts suggests that more than Finally, in May 005 Swift discovered the Rhaana Starling 4 one progenitor type may be involved. first X-ray afterglow to a short GRB. Sylvio Klose5 This was made possible because of the Chryssa Kouveliotou6 rapid ability of Swift to slew across the Chloé Féron1 A decade ago studies of gamma-ray sky, pointing at the approximate location Patrizia Ferrero5 bursts (GRBs) were revolutionised by the of the burst only a minute after it hap- Andy Fruchter 7 discovery of long-lived afterglow emis- pened and pinpointing a very faint X-ray Johan Fynbo1 sion at X-ray, optical and radio wave- afterglow. The afterglow lies close to a Javier Gorosabel 8 lengths. The afterglows provided precise massive elliptical galaxy in a cluster of Páll Jakobsson positions on the sky, which in turn led galaxies at z = 0.225 (Gehrels et al. 005; David Alexander Kann5 to the discovery that GRBs originate at Pedersen et al. 005; Figure ). Many ex- Kristian Pedersen1 cosmological distances, and are thus the tremely deep observations, including Enrico Ramirez-Ruiz 9 most luminous events known in the Uni- those at the VLT, failed to locate either a Jesper Sollerman1 verse. These afterglows also provided fading optical afterglow, or a rising super- Christina Thöne1 essential information for our understand- nova component at later times (Hjorth Darach Watson1 ing of what creates these extraordinary et al. 005a). The lack of an accompany- Klaas Wiersema10 explosions. Observations from the VLT ing supernova (Figure 3), and the pur- Dong Xu1 finally showed them to be associated with ported elliptical host galaxy (Figure ), the final, catastrophic collapse of massive strongly suggest that the progenitors stars (Hjorth et al. 003). for these short bursts are different from 1 Dark Cosmology Centre, Niels Bohr those of long bursts. In particular, any Institute, University of Copenhagen, But the picture was not yet complete. In radioactive material produced in the ex- Denmark particular, these results applied only to plosion must be far less. Centre for Astrophysics Research, the bursts with durations of > s, while University of Hertfordshire, United the burst duration distribution was clearly Kingdom bimodal (Kouveliotou et al. 1993) split- Figure 1: The hardness-duration diagram for GRBs. 3 Department of Physics, University of ting into long and short GRBs, with the The x-axis shows the duration over which 90 % of Warwick, United Kingdom short bursts also exhibiting markedly the observed total flux is detected, while the y-axis 4 Department of Physics and Astron- harder gamma-ray spectra (see Figure 1). shows the ratio of fluxes in the 50–100 keV over the 0–50 keV bands, and is essentially a gamma-ray omy, University of Leicester, United The short bursts proved even more colour. Two groups (blue points) are seen, those with Kingdom elusive than their long-duration cousins, durations > s and soft gamma-ray spectra and 5 Thüringer Landessternwarte Tauten- and despite significant effort no after- those with durations < s and harder gamma-ray burg, Germany glows could be found, maintaining our emission. These GRBs are taken from the BATSE 6 catalogue. Also shown (in red) are the short bursts NASA Marshall Space Flight Center, ignorance of their distance scales, detected by Swift and HETE-2 over the past Huntsville, Alabama, USA energies and, of course, physical origin. 18 months. 7 Space Telescope Science Institute, Baltimore, Maryland, USA 10 8 Instituto de Astrofísica de Andalucía, Granada, Spain 9 Institute for Advanced Study, Princeton, New Jersey, USA 10 Astronomical Institute, University of Amsterdam, the Netherlands ] 0 060801 −5 060502B 20 060313 Swift, a dedicated gamma-ray burst /S 050509B 00 (GRB) satellite with ultrarapid slew- −1 050813 051221 ing capability, and a suite of ground- 50 050709 [S based (ESO) telescopes have recently 1 050925 050724 achieved a major breakthrough: de- 050906 tecting the first afterglows of short- duration GRBs. The faintness of these afterglows and the diversity of old and young host galaxies lend support to the emerging ‘standard model’, in which they are created during the merg- 0.01 0.1 1 10 100 1000 ing of two compact objects. However, t90 (s) 16 The Messenger 126 – December 006 Figure 2: The diverse possible host galaxies of sev- GRB 050509B GRB 0505813 GRB 050906 eral short duration GRBs. GRB 050509B, the first localised short GRB, had no optical afterglow, no supernova (Figure 3) but was localised to an elliptical galaxy at z = 0.225 (image from VLT). GRB 050813 had no optical afterglow. In its error circle several galaxies at z = 1.7 were found (image from VLT). GRB 050906 had no afterglow either but inside the error circle (which is much larger than the image shown) the galaxy IC 38 (z = 0.031) was present (image from VLT). Inside the large IPN error box of GRB 051103 several galaxies from the nearby M81/M8 group were found (image from GALEX). GRB 051103 GRB 060121 GRB 060313 GRB 06011 had a faint optical afterglow and was localised to a very faint galaxy (image from HST). GRB 060313 had a bright afterglow discovered at ESO and was localised to a very faint galaxy (image from VLT). Optical emission from a short GRB was star – black hole (NS-BH). These systems that the afterglows have been less well finally found for the HETE- GRB 050709 merge following orbital decay due to sampled and few good spectral ener- (Hjorth et al. 005b) using the Danish emission of gravitational radiation. Based gy distributions have been secured. For 1.5-m telescope at La Silla. Gemini obser- on observations of known systems in this work 8-m telescopes are required, vations pinpointed the burst to a dwarf the Milky Way, it is clear that this can take even at early times. By far the best early galaxy at z = 0.16. This emission is likely billions of years. Also, on creation, a neu- optical light curve for a short GRB comes to be synchrotron emission, just as in tron star obtains a large ‘kick’ from the from GRB 060313, with observations long GRBs. Another short burst with an supernova, removing it from the region of beginning on the ground (from the Danish optical afterglow was GRB 051221 at star formation in which it was made, and, 1.5-m telescope) only six minutes after z = 0.54. These results firmly place short potentially pushing the binary far from the burst and continuing for several hours. GRBs at cosmological distances. How- its host galaxy at the time of the merger. At the VLT, following a Rapid Response ever, the evidence so far indicates that This has made compact binary mergers Mode activation, a total of twenty seven they are at moderate redshifts, closer the most popular model for short GRB 100-second observations were obtained. than the mean for the long GRBs which origin, yet some observations continue to These high-S/N and high-cadence ob- now lies at z = .8 (Jakobsson et al. challenge this suggestion. servations allowed rapid, small amplitude 006), a result which in itself relies signifi- variability to been seen. This suggests cantly on ESO efforts. that energy is being input into the after- Light curves glow out to late times post-burst. This is problematic for merger models, since Host galaxies So far, the optical afterglows of short the final coalescence should occur very GRBs have typically been fainter than for rapidly, with little material remaining to One of the striking differences between long GRBs (Figure 4). This has meant fuel the burst afterwards. One possible long and short GRBs is in the properties of their host galaxies. Long GRB hosts 20 are mostly blue, sub-luminous and star- forming, and the GRBs preferentially oc- SN Ia cur in their brightest regions (Fruchter 22 et al. 006). In contrast, short GRB host SN1998bw Figure 3: No supernova associated galaxies seem to be a more varied class, ) with short GRB 050509B. The upper and can be red, old and non-starform- ag limits (red arrows) on variable sources 24 inside the GRB 050509B error cir- ing, with the GRBs originating at occa- V (m SN1991bg sionally large radial separations from the cle (see Figure ) compared to the light curves of different SNe redshifted to host core. Any model for the origin of SN1994I z = 0.225 (blue: Type Ic; green: Type Ia; the short GRBs must naturally explain 26 thick curves: bright supernovae; thin curves: faint supernovae). The stringent these observations; so far the prevailing GRB 050509B choice is therefore compact objects – upper limits obtained with the VLT rule out the presence of a super-nova compact object mergers, e.g., neutron 0 10 20 30 40 accompanying the first localised short star – neutron star (NS-NS) or neutron Time since GRB (days) burst, GRB 050509B. The Messenger 126 – December 006 17 Reports from Observers Hjorth J. et al., The Short Gamma-Ray Burst Revolution Figure 4: Illustrative light curves of long GRBs (black) and short GRBs (red). The light curves have been interpolated, corrected for extinction and shifted to a common redshift of z = 1. The afterglows of short GRBs are much fainter in the mean than those of long GRBs. The curve for GRB 050813 represents an upper limit. The redshift of GRB 06011 has been assumed to be z = 4.6. solution of this puzzle is that after the merger, a neutron star/magnetar rather 14 than a black hole is formed.