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Featured researches published by Ehud Nakar.


Physics Reports | 2007

Short-Hard Gamma-Ray Bursts

Ehud Nakar

Two types of gamma-ray bursts (GRBs) are observed: short-duration hard spectrum GRBs and long-duration soft spectrum GRBs. For many years long GRBs were the focus of intense research while the lack of observational data limited the study of short-hard GRBs (SHBs). In 2005 a breakthrough occurred following the first detections of SHB afterglows, longer wavelength emission that follows the burst of gamma-rays. Similarly to long GRBs, afterglow detections led to the identification of SHB host galaxies and measurement of their redshifts. These observations established that SHBs are cosmological relativistic sources that, unlike long GRBs, do not originate from the collapse of massive stars, and therefore constitute a distinct physical phenomenon. One viable model for SHB origin is the coalescence of compact binary systems (double neutron stars or a neutron star and a black hole), in which case SHBs are the electromagnetic counterparts of strong gravitational-wave sources. The theoretical and observational study of SHBs following the recent pivotal discoveries is reviewed, along with new theoretical results that are presented here for the first time.


Nature | 2005

The afterglow of GRB 050709 and the nature of the short-hard gamma-ray bursts.

Derek B. Fox; Dale A. Frail; Paul A. Price; S. R. Kulkarni; Edo Berger; Tsvi Piran; Alicia M. Soderberg; S. B. Cenko; P. B. Cameron; Avishay Gal-Yam; Mansi M. Kasliwal; D.-S. Moon; Fiona A. Harrison; Ehud Nakar; Brian Paul Schmidt; Bryan E. Penprase; Roger A. Chevalier; Pawan Kumar; Kathy Roth; D. Watson; Brian Leverett Lee; Stephen A. Shectman; Mark M. Phillips; M. Roth; Patrick J. McCarthy; M Rauch; L. L. Cowie; Bruce A. Peterson; Joshua Rich; Nobuyuki Kawai

The final chapter in the long-standing mystery of the γ-ray bursts (GRBs) centres on the origin of the short-hard class of bursts, which are suspected on theoretical grounds to result from the coalescence of neutron-star or black-hole binary systems. Numerous searches for the afterglows of short-hard bursts have been made, galvanized by the revolution in our understanding of long-duration GRBs that followed the discovery in 1997 of their broadband (X-ray, optical and radio) afterglow emission. Here we present the discovery of the X-ray afterglow of a short-hard burst, GRB 050709, whose accurate position allows us to associate it unambiguously with a star-forming galaxy at redshift z = 0.160, and whose optical lightcurve definitively excludes a supernova association. Together with results from three other recent short-hard bursts, this suggests that short-hard bursts release much less energy than the long-duration GRBs. Models requiring young stellar populations, such as magnetars and collapsars, are ruled out, while coalescing degenerate binaries remain the most promising progenitor candidates.


Nature | 2006

Relativistic ejecta from X-ray flash XRF 060218 and the rate of cosmic explosions

Alicia M. Soderberg; S. R. Kulkarni; Ehud Nakar; Edo Berger; P. B. Cameron; Derek B. Fox; Dale A. Frail; Avishay Gal-Yam; R. Sari; S. B. Cenko; M. M. Kasliwal; R. A. Chevalier; Tsvi Piran; Paul A. Price; Brian Paul Schmidt; Guy G. Pooley; D.-S. Moon; Bryan E. Penprase; Eran O. Ofek; A. Rau; N. Gehrels; J. A. Nousek; D. N. Burrows; S. E. Persson; P. J. McCarthy

Over the past decade, long-duration γ-ray bursts (GRBs)—including the subclass of X-ray flashes (XRFs)—have been revealed to be a rare variety of type Ibc supernova. Although all these events result from the death of massive stars, the electromagnetic luminosities of GRBs and XRFs exceed those of ordinary type Ibc supernovae by many orders of magnitude. The essential physical process that causes a dying star to produce a GRB or XRF, and not just a supernova, is still unknown. Here we report radio and X-ray observations of XRF 060218 (associated with supernova SN 2006aj), the second-nearest GRB identified until now. We show that this event is a hundred times less energetic but ten times more common than cosmological GRBs. Moreover, it is distinguished from ordinary type Ibc supernovae by the presence of 1048 erg coupled to mildly relativistic ejecta, along with a central engine (an accretion-fed, rapidly rotating compact source) that produces X-rays for weeks after the explosion. This suggests that the production of relativistic ejecta is the key physical distinction between GRBs or XRFs and ordinary supernovae, while the nature of the central engine (black hole or magnetar) may distinguish typical bursts from low-luminosity, spherical events like XRF 060218.


Nature | 2011

Hydrogen-poor superluminous stellar explosions

Robert Michael Quimby; S. R. Kulkarni; Mansi M. Kasliwal; Avishay Gal-Yam; I. Arcavi; P. Nugent; R. C. Thomas; D. A. Howell; Ehud Nakar; Lars Bildsten; Christopher A. Theissen; Nicholas M. Law; Richard G. Dekany; Gustavo Rahmer; David Hale; Roger Smith; Eran O. Ofek; J. Zolkower; Viswa Velur; Robert J. Walters; John R. Henning; K. Bui; Daniel L. McKenna; Dovi Poznanski; S. B. Cenko; David Levitan

Supernovae are stellar explosions driven by gravitational or thermonuclear energy that is observed as electromagnetic radiation emitted over weeks or more. In all known supernovae, this radiation comes from internal energy deposited in the outflowing ejecta by one or more of the following processes: radioactive decay of freshly synthesized elements (typically 56Ni), the explosion shock in the envelope of a supergiant star, and interaction between the debris and slowly moving, hydrogen-rich circumstellar material. Here we report observations of a class of luminous supernovae whose properties cannot be explained by any of these processes. The class includes four new supernovae that we have discovered and two previously unexplained events (SN 2005ap and SCP 06F6) that we can now identify as members of the same class. These supernovae are all about ten times brighter than most type Ia supernova, do not show any trace of hydrogen, emit significant ultraviolet flux for extended periods of time and have late-time decay rates that are inconsistent with radioactivity. Our data require that the observed radiation be emitted by hydrogen-free material distributed over a large radius (∼1015 centimetres) and expanding at high speeds (>104 kilometres per second). These long-lived, ultraviolet-luminous events can be observed out to redshifts z > 4.


The Astrophysical Journal | 2010

THE AFTERGLOWS OF SWIFT-ERA GAMMA-RAY BURSTS. I. COMPARING PRE-SWIFT AND SWIFT-ERA LONG/SOFT (TYPE II) GRB OPTICAL AFTERGLOWS

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.


Nature | 2011

Birth of a relativistic outflow in the unusual γ-ray transient Swift J164449.3+573451

B. A. Zauderer; Edo Berger; Alicia M. Soderberg; Abraham Loeb; Ramesh Narayan; D. A. Frail; G. Petitpas; A. Brunthaler; Ryan Chornock; John M. Carpenter; G. G. Pooley; K. Mooley; S. R. Kulkarni; Raffaella Margutti; D. B. Fox; Ehud Nakar; Nimesh A. Patel; N. H. Volgenau; T. L. Culverhouse; M. F. Bietenholz; M. P. Rupen; W. Max-Moerbeck; Anthony C. S. Readhead; J. Richards; M. Shepherd; S. Storm; Charles L. H. Hull

Active galactic nuclei, which are powered by long-term accretion onto central supermassive black holes, produce relativistic jets with lifetimes of at least one million years, and the observation of the birth of such a jet is therefore unlikely. Transient accretion onto a supermassive black hole, for example through the tidal disruption of a stray star, thus offers a rare opportunity to study the birth of a relativistic jet. On 25 March 2011, an unusual transient source (Swift J164449.3+573451) was found, potentially representing such an accretion event. Here we report observations spanning centimetre to millimetre wavelengths and covering the first month of evolution of a luminous radio transient associated with Swift J164449.3+573451. The radio transient coincides with the nucleus of an inactive galaxy. We conclude that we are seeing a newly formed relativistic outflow, launched by transient accretion onto a million-solar-mass black hole. A relativistic outflow is not predicted in this situation, but we show that the tidal disruption of a star naturally explains the observed high-energy properties and radio luminosity and the inferred rate of such events. The weaker beaming in the radio-frequency spectrum relative to γ-rays or X-rays suggests that radio searches may uncover similar events out to redshifts of z ≈ 6.


The Astrophysical Journal | 2006

The Afterglow, Energetics, and Host Galaxy of the Short-Hard Gamma-Ray Burst 051221a

Alicia M. Soderberg; Edo Berger; Mansi M. Kasliwal; Dale A. Frail; Paul A. Price; Brian Paul Schmidt; S. R. Kulkarni; Derek B. Fox; S. B. Cenko; Avishay Gal-Yam; Ehud Nakar; Kathy Roth

We present detailed optical, X-ray, and radio observations of the bright afterglow of the short gamma-ray burst 051221a obtained with Gemini, Swift XRT, and the Very Large Array, as well as optical spectra from which we measure the redshift of the burst, z = 0.5464. At this redshift the isotropic-equivalent prompt energy release was about 1.5 × 10^(51) ergs, and using a standard afterglow synchrotron model, we find that the blast wave kinetic energy is similar, E_(K,iso) ≈ 8.4 × 10^(51) ergs. An observed jet break at t approx 5 days indicates that the opening angle is θ_j ≈ 7° and the total beaming-corrected energy is therefore ≈ 2.5 × 10^(49) ergs, comparable to the values inferred for previous short GRBs. We further show that the burst experienced an episode of energy injection by a factor of 3.4 between t = 1.4 and 3.4 hr, which was accompanied by reverse shock emission in the radio band. This result provides continued evidence that the central engines of short GRBs may be active significantly longer than the duration of the burst and/or produce a wide range of Lorentz factors. Finally, we show that the host galaxy is actively forming stars at a rate of about 1.6 M_☉ yr^(-1), yet exhibits evidence for an appreciable population of old stars (~1 Gyr) and near-solar metallicity. These properties are intermediate between those of long GRB hosts and previous short burst hosts. The lack of bright supernova emission and the low circumburst density (n ~ 10^(-3) cm^(-3)), however, continue to support the idea that short bursts are not related to massive stellar death. Given that the total energy release is larger than the predicted yield for a neutrino annihilation mechanism, this suggests that magnetohydrodynamic processes may be required to power the burst.


Nature | 2011

Detectable radio flares following gravitational waves from mergers of binary neutron stars

Ehud Nakar; Tsvi Piran

The question “what is the observable electromagnetic (EM) signature of a compact binary merger?” is an intriguing one with crucial consequences to the quest for gravitational waves (GW). Compact binary mergers are prime sources of GW, targeted by current and next generation detectors. Numerical simulations have demonstrated that these mergers eject energetic sub-relativistic (or even relativistic) outflows. This is certainly the case if the mergers produce short GRBs, but even if not, significant outflows are expected. The interaction of such outflows with the surround matter inevitably leads to a long lasting radio signal. We calculate the expected signal from these outflows (our calculations are also applicable to short GRB orphan afterglows) and we discuss their detectability. We show that the optimal search for such signal should, conveniently, take place around 1.4 GHz. Realistic estimates of the outflow parameters yield signals of a few hundred μJy, lasting a few weeks, from sources at the detection horizon of advanced GW detectors. Followup radio observations, triggered by GW detection, could reveal the radio remnant even under unfavorable conditions. Upcoming all sky surveys can detect a few dozen, and possibly even thousands, merger remnants at any give time, thereby providing robust merger rate estimates even before the advanced GW detectors become operational. In fact, the radio transient RT 19870422 fits well the overall properties predicted by our model and we suggest that its most probable origin is a compact binary merger radio remnant.Mergers of neutron-star/neutron-star binaries are strong sources of gravitational waves. They can also launch subrelativistic and mildly relativistic outflows and are often assumed to be the sources of short γ-ray bursts. An electromagnetic signature that persisted for weeks to months after the event would strengthen any future claim of a detection of gravitational waves. Here we present results of calculations showing that the interaction of mildly relativistic outflows with the surrounding medium produces radio flares with peak emission at 1.4 gigahertz that persist at detectable (submillijansky) levels for weeks, out to a redshift of 0.1. Slower subrelativistic outflows produce flares detectable for years at 150 megahertz, as well as at 1.4 gigahertz, from slightly shorter distances. The radio transient RT 19870422 (ref. 11) has the properties predicted by our model, and its most probable origin is the merger of a compact neutron-star/neutron-star binary. The lack of radio detections usually associated with short γ-ray bursts does not constrain the radio transients that we discuss here (from mildly relativistic and subrelativistic outflows) because short γ-ray burst redshifts are typically >0.1 and the appropriate timescales (longer than weeks) have not been sampled.


The Astrophysical Journal | 2010

EARLY SUPERNOVAE LIGHT CURVES FOLLOWING THE SHOCK BREAKOUT

Ehud Nakar; Re'em Sari

The first light from a supernova (SN) emerges once the SN shock breaks out of the stellar surface. The first light, typically a UV or X-ray flash, is followed by a broken power-law decay of the luminosity generated by radiation that leaks out of the expanding gas sphere. Motivated by recent detection of emission from very early stages of several SNe, we revisit the theory of shock breakout and the following emission, paying special attention to the photon-gas coupling and deviations from thermal equilibrium. We derive simple analytic light curves of SNe from various progenitors at early times. We find that for more compact progenitors, white dwarfs, Wolf-Rayet stars (WRs), and possibly more energetic blue-supergiant explosions, the observed radiation is out of thermal equilibrium at the breakout, during the planar phase (i.e., before the expanding gas doubles its radius), and during the early spherical phase. Therefore, during these phases we predict significantly higher temperatures than previous analysis that assumed equilibrium. When thermal equilibrium prevails, we find the location of the thermalization depth and its temporal evolution. Our results are useful for interpretation of early SN light curves. Some examples are (1) red supergiant SNe have an early bright peak in optical and UV flux, less than an hour after breakout. It is followed by a minimum at the end of the planar phase (about 10 hr), before it peaks again once the temperature drops to the observed frequency range. In contrast, WRs show only the latter peak in optical and UV. (2) Bright X-ray flares are expected from all core-collapse SNe types. (3) The light curve and spectrum of the initial breakout pulse hold information on the explosion geometry and progenitor wind opacity. Its spectrum in more compact progenitors shows a (nonthermal) power law and its light curve may reveal both the breakout diffusion time and the progenitor radius.


The Astrophysical Journal | 2011

THE AFTERGLOWS OF SWIFT-ERA GAMMA-RAY BURSTS. II. TYPE I GRB VERSUS TYPE II GRB OPTICAL AFTERGLOWS*

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

We use a large sample of GRB afterglow and prompt-emission data (adding further GRB afterglow observations in this work) to compare the optical afterglows (or the lack thereof) of Type I GRBs with those of Type II GRBs. In comparison to the afterglows of Type II GRBs, we find that those of Type I GRBs have a lower average luminosity and show an intrinsic spread of luminosities at least as wide. From late and deep upper limits on the optical transients, we establish limits on the maximum optical luminosity of any associated supernova, confirming older works and adding new results. We use deep upper limits on Type I GRB optical afterglows to constrain the parameter space of possible mini-SN emission associated with a compact-object merger. Using the prompt emission data, we search for correlations between the parameters of the prompt emission and the late optical afterglow luminosities. We find tentative correlations between the bolometric isotropic energy release and the optical afterglow luminosity at a fixed time after trigger (positive), and between the host offset and the luminosity (negative), but no significant correlation between the isotropic energy release and the duration of the GRBs. We also discuss three anomalous GRBs, GRB 060505, GRB 060614, and GRB 060121, in the light of their optical afterglow luminosities. (Abridged)

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Tsvi Piran

Hebrew University of Jerusalem

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S. R. Kulkarni

California Institute of Technology

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Avishay Gal-Yam

Weizmann Institute of Science

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Eran O. Ofek

Weizmann Institute of Science

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Re'em Sari

Hebrew University of Jerusalem

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Dale A. Frail

National Radio Astronomy Observatory

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Derek B. Fox

Pennsylvania State University

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S. B. Cenko

California Institute of Technology

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