Abstract

There is increasing observational evidence that short and long Gamma-ray bursts (GRBs) originate in different subclasses, each one with specific energy release, spectra, duration, etc, and all of them with binary progenitors. The binary components involve carbon-oxygen cores (CO core ), neutron stars (NSs), black holes (BHs), and white dwarfs (WDs). We review here the salient features of the specific class of binary-driven hypernovae (BdHNe) within the induced gravitational collapse (IGC) scenario for the explanation of the long GRBs. The progenitor is a CO core -NS binary. The supernova (SN) explosion of the CO core , producing at its center a new NS ( ν NS), triggers onto the NS companion a hypercritical, i.e., highly super-Eddington accretion process, accompanied by a copious emission of neutrinos. By accretion the NS can become either a more massive NS or reach the critical mass for gravitational collapse with consequent formation of a BH. We summarize the results on this topic from the first analytic estimates in 2012 all the way up to the most recent three-dimensional (3D) smoothed-particle-hydrodynamics (SPH) numerical simulations in 2018. Thanks to these results it is by now clear that long GRBs are richer and more complex systems than thought before. The SN explosion and its hypercritical accretion onto the NS explain the X-ray precursor. The feedback of the NS accretion, the NS collapse and the BH formation produce asymmetries in the SN ejecta, implying the necessity of a 3D analysis for GRBs. The newborn BH, the surrounding matter and the magnetic field inherited from the NS, comprises the inner engine from which the GRB electron-positron ( e + e − ) plasma and the high-energy emission are initiated. The impact of the e + e − on the asymmetric ejecta transforms the SN into a hypernova (HN). The dynamics of the plasma in the asymmetric ejecta leads to signatures depending on the viewing angle. This explains the ultrarelativistic prompt emission in the MeV domain and the mildly-relativistic flares in the early afterglow in the X-ray domain. The feedback of the ν NS pulsar-like emission on the HN explains the X-ray late afterglow and its power-law regime. All of the above is in contrast with a simple GRB model attempting to explain the entire GRB with the kinetic energy of an ultrarelativistic jet extending through all of the above GRB phases, as traditionally proposed in the “collapsar-fireball” model. In addition, BdHNe in their different flavors lead to ν NS-NS or ν NS-BH binaries. The gravitational wave emission drives these binaries to merge producing short GRBs. It is thus established a previously unthought interconnection between long and short GRBs and their occurrence rates. This needs to be accounted for in the cosmological evolution of binaries within population synthesis models for the formation of compact-object binaries.

Highlights

  • It was there shown the interesting result that the temperature of this outflow and its evolution can explain the early X-ray emission that has been observed in some binary-driven hypernovae (BdHNe) and in X-ray flashes (XRFs), exemplified there analyzing the early X-ray emission observed in Gamma-ray bursts (GRBs) 090618, a Binary-driven hypernova (BdHN) I, and in GRB 060218, a BdHN II

  • We have recently presented in [90] new, 3D hydrodynamic simulations of the induced gravitational collapse (IGC) scenario by adapting the SPH code developed at Los Alamos, SNSPH [103], which has been tested and applied in a variety of astrophysical situations [104,105,106,107]

  • It is clear from the derived rates that the short GRB population is dominated by the low-luminosity class of short Gamma-ray flashes (S-GRFs), double neutron stars (NSs) mergers that do not lead to black holes (BHs) formation

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Summary

The Quest for the Binary Nature of GRB Progenitors

We first recall that GRBs have been traditionally classified by a phenomenological division based on the duration of the time-interval in which the 90% of the total isotropic energy in Gamma-rays is emitted, the T90. It is theoretically known that massive stars with such a relatively low mass do not lead to a direct collapse to a BH (see [38,39] for details) It was recently shown in [40] that the observed thermal emission in the X-ray flares present in the early (rest-frame time t ∼ 102 s) afterglow implies an emitter of size ∼1012 cm expanding at mildly-relativistic velocity, e.g., Γ . Much more about this binary scenario has been discovered since its initial proposal; its theoretical studies and the search for its observational verification have led to the formulation of a much rich phenomenology which will be the main subject of this article Both short and long GRBs appear to be produced by binary systems, well in line with the expectation that most massive stars belong to binary systems (see, e.g., [43,44], and references therein). This, in addition to the multiyear effort of reaching a comprehensive theoretical interpretation of such regimes, have lead to the conclusion that GRBs separate into subclasses, each with specific energy release, spectra, duration, among other properties and, all with binary progenitors [45,46,47,48,49]

GRB Subclasses
The Specific Case of BdHNe
First Analytic Estimates
First Numerical Simulations
First 3D Simulations
The Hypercritical Accretion Process
Accretion Rate and NS Evolution
Hydrodynamics in the Accretion Region
Neutrino Emission and Effective Accretion Rate
Ṁacc vacc c
Accretion Luminosity
New 3D SPH Simulations
Consequences on GRB Data Analysis and Interpretation
X-ray Precursor
GRB Prompt Emission
Early X-ray Afterglow
Late X-ray Afterglow
High-Energy GeV Emission
Additional Considerations
Post-Explosion Orbits and Formation of NS-BH Binaries
An Evolutionary Scenario
Occurrence Rate
Connection with Short GRBs
Findings
Conclusions
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