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A hypernova (sometimes called a collapsar) is a very energetic supernova thought to result from an extreme core-collapse scenario. In this case, a massive star (>30 solar masses) collapses to form a rotating black hole emitting twin energetic jets and surrounded by an accretion disk. It is a type of stellar explosion that ejects material with an unusually high kinetic energy, an order of magnitude higher than most supernovae, with a luminosity at least 10 times greater. They usually appear similar to a type Ic supernova, but with unusually broad spectral lines indicating an extremely high expansion velocity. Hypernovae are one of the mechanisms for producing long gamma ray bursts (GRBs), which range from 2 seconds to over a minute in duration. They have also been referred to as superluminous supernovae, though that classification also includes other types of extremely luminous stellar explosions that have different origins.

History

In the 1980s, the term hypernova was used to describe a theoretical type of supernova now known as a pair-instability supernova. It referred to the extremely high energy of the explosion compared to typical core collapse supernovae.[1][2][3] The term had previously been used to describe hypothetical explosions from diverse events such as hyperstars, extremely massive population III stars in the early universe,[4] or from events such as black hole mergers.[5]

GRBs were initially detected on July 2, 1967 by US military satellites in high Earth orbit, which were meant to detect gamma radiation. The US had suspected the USSR of conducting secret nuclear tests despite signing the Nuclear Test Ban Treaty of 1963, and the Vela satellites were capable of detecting explosions behind the moon. The satellites detected a signal, but it was unlike that of a nuclear weapon signature, nor could it be correlated to solar flares.[6] Over the next few decades, the GRBs posed a compelling mystery. Gamma rays require highly energetic events to be produced, yet GRBs could not be correlated to supernovae, solar flares, or any other activity in the sky. Their brevity made them difficult to trace. Once their direction could be determined, it was found that they were evenly spread across the sky. Thus they were not originating in the Milky Way or nearby galaxies, but from deep space.

In February 1997, Dutch-Italian satellite BeppoSAX was able to trace GRB 970508 to a faint galaxy roughly 6 billion light years away.[7] From analyzing the spectroscopic data for both the GRB 970508 and its host galaxy, Bloom et al. concluded in 1998 that a hypernova was the likely cause.[7] That same year, hypernovae were hypothesized in greater detail by Polish astronomer Bohdan Paczyński as supernovae from rapidly spinning stars.[8]

The usage of the term hypernova from the late 20th century has since been refined to refer to those supernovae with unusually large kinetic energy.[9] The first hypernova observed was SN 1998bw, with a luminosity 100 times higher than a standard Type Ib.[10] This supernova was the first to be associated with a gamma-ray burst (GRB) and it produced a shockwave containing an order of magnitude more energy than a normal supernova. Other scientists prefer to call these objects simply broad-lined type Ic supernovae.[11] Since then the term has been applied to a variety of objects, not all of which meet the standard definition; for example ASASSN-15lh.[12]

Properties

Hypernovae are now widely accepted to be supernovae with ejecta having a kinetic energy larger than about 10⁴⁵ joule, an order of magnitude higher than a typical core collapse supernova. The ejected nickel masses are large and the ejection velocity up to 99% of the speed of light. These are typically of type Ic, and some are associated with long-duration gamma-ray bursts. The electromagnetic energy released by these events varies from comparable to other type Ic supernova, to some of the most luminous supernovae known such as SN 1999as.[13][14]

The archetypal hypernova, SN 1998bw, was associated with GRB 980425. Its spectrum showed no hydrogen and no clear helium features, but strong silicon lines identified it as a type Ic supernova. The main absorption lines were extremely broadened and the light curve showed a very rapid brightening phase, reaching the brightness of a type Ia supernova at day 16. The total ejected mass was about 10 M_☉ and the mass of nickel ejected about 0.4 M_☉.[13] All supernovae associated with GRBs have shown the high-energy ejecta that characterises them as hypernovae.[15]

Unusually bright radio supernovae have been observed as counterparts to hypernovae, and have been termed "radio hypernovae".[16]

Astrophysical models

Models for hypernova focus on the efficient transfer of energy into the ejecta. In normal core collapse supernovae, 99% of neutrinos generated in the collapsing core escape without driving the ejection of material. It is thought that rotation of the supernova progenitor drives a jet that accelerates material away from the explosion at close to the speed of light. Binary systems are increasingly being studied as the best method for both stripping stellar envelopes to leave a bare carbon-oxygen core, and for inducing the necessary spin conditions to drive a hypernova.

Collapsar model

The collapsar model describes a type of supernova that produces a gravitationally collapsed object, or black hole. The word "collapsar", short for "collapsed star", was formerly used to refer to the end product of stellar gravitational collapse, a stellar-mass black hole. The word is now sometimes used to refer to a specific model for the collapse of a fast-rotating star. When core collapse occurs in a star with a core at least around fifteen times the sun's mass (M_☉) — though chemical composition and rotational rate are also significant — the explosion energy is insufficient to expel the outer layers of the star, and it will collapse into a black hole without producing a visible supernova outburst.

A star with a core mass slightly below this level — in the range of 5–15 M_☉ — will undergo a supernova explosion, but so much of the ejected mass falls back onto the core remnant that it still collapses into a black hole. If such a star is rotating slowly, then it will produce a faint supernova, but if the star is rotating quickly enough, then the fallback to the black hole will produce relativistic jets. The energy that these jets transfer into the ejected shell renders the visible outburst substantially more luminous than a standard supernova. The jets also beam high energy particles and gamma rays directly outward and thereby produce x-ray or gamma-ray bursts; the jets can last for several seconds or longer and correspond to long-duration gamma-ray bursts, but they do not appear to explain short-duration gamma-ray bursts.[17][18]

Binary models

The mechanism for producing the stripped progenitor, a carbon-oxygen star lacking any significant hydrogen or helium, of type Ic supernovae was once thought to be an extremely evolved massive star, for example a type WO Wolf-Rayet star whose dense stellar wind expelled all its outer layers. Observations have failed to detect any such progenitors. It is still not conclusively shown that the progenitors are actually a different type of object, but several cases suggest that lower-mass "helium giants" are the progenitors. These stars are not sufficiently massive to expel their envelopes simply by stellar winds, and they would be stripped by mass transfer to a binary companion. Helium giants are increasingly favoured as the progenitors of type Ib supernovae, but the progenitors of type Ic supernovae is still uncertain.[19]

One proposed mechanism for producing gamma-ray bursts is induced gravitational collapse, where a neutron star is triggered to collapse into a black hole by the core collapse of a close companion consisting of a stripped carbon-oxygen core. The induced neutron star collapse allows for the formation of jets and high-energy ejecta that have been difficult to model from a single star.[20]

See also

• Gamma-ray burst progenitors – Types of celestial objects that can emit gamma-ray bursts
• Quark star – Compact exotic star which forms matter consisting mostly of quarks
• Quark-nova – Hypothetical violent explosion resulting from conversion of a neutron star to a quark star

References

Further reading

На других языках

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[de] Hypernova

Eine Hypernova ist eine Supernova mit einer elektromagnetisch abgestrahlten Energie von mehr als 1045 Joule unter Annahme einer räumlich isotropen Abstrahlung. Eine Hypernova stellt das obere Ende der superleuchtkräftigen oder superhellen Supernovae dar.[1]

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- [en] Hypernova

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[es] Hipernova

Una hipernova es un tipo de supernova producida cuando estrellas muy masivas (masas superiores a las 25 masas solares) se colapsan al final de sus vidas. Después de explotar como supernova, el núcleo de la hipernova se colapsaría directamente en un agujero negro, emitiendo dos chorros de plasma extremadamente energéticos desde sus polos a velocidades cercanas a la de la luz. Estos chorros podrían generar potentes rayos gamma y serían una posible explicación de las erupciones de rayos gamma. Estrellas tan masivas son muy raras, y por lo tanto también serían raras las hipernovas: se estima que un evento de esta naturaleza puede ocurrir en nuestra Galaxia cada 200 millones de años. La estrella Eta Carinae, en nuestra Galaxia, puede ser una candidata a hipernova. Otra buena candidata a estallar en hipernova puede ser R136a1, descubierta en julio de 2010 y con una asombrosa masa de 265 soles; también la estrella Pistola o LBV 1806-20 pueden ser candidatas a producir agujeros negros de aquí a decenas o centenas de miles de años.

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[ru] Гиперновая звезда

Гиперновая — взрыв сверхмассивной звезды (с массой более 20 масс Солнца) после коллапса её ядра; коллапс ядра происходит после того, как в нём истощается топливо для поддержания термоядерных реакций. То есть это очень большая (сверхмощная) сверхновая.

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