Penrose process, superradiance, and ergoregion instabilities

Research output: Contribution to journalJournal articleResearchpeer-review

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Penrose process, superradiance, and ergoregion instabilities. / Vicente, Rodrigo; Cardoso, Vitor; Lopes, Jorge C.

In: Physical Review D, Vol. 97, No. 8, 084032, 16.04.2018.

Research output: Contribution to journalJournal articleResearchpeer-review

Harvard

Vicente, R, Cardoso, V & Lopes, JC 2018, 'Penrose process, superradiance, and ergoregion instabilities', Physical Review D, vol. 97, no. 8, 084032. https://doi.org/10.1103/PhysRevD.97.084032

APA

Vicente, R., Cardoso, V., & Lopes, J. C. (2018). Penrose process, superradiance, and ergoregion instabilities. Physical Review D, 97(8), [084032]. https://doi.org/10.1103/PhysRevD.97.084032

Vancouver

Vicente R, Cardoso V, Lopes JC. Penrose process, superradiance, and ergoregion instabilities. Physical Review D. 2018 Apr 16;97(8). 084032. https://doi.org/10.1103/PhysRevD.97.084032

Author

Vicente, Rodrigo ; Cardoso, Vitor ; Lopes, Jorge C. / Penrose process, superradiance, and ergoregion instabilities. In: Physical Review D. 2018 ; Vol. 97, No. 8.

Bibtex

@article{458047caa1f047e39614a33ae3215d3b,
title = "Penrose process, superradiance, and ergoregion instabilities",
abstract = "Superradiant scattering is a radiation enhancement process that takes place in many contexts, and which has recently found exciting applications in astrophysics and particle physics. In the framework of curved spacetime physics, it has been associated with the classical Penrose process for particles. Superradiance is usually also associated with bosonic fields around geometries with ergoregions and horizons. These notions are in clear tension however: the Penrose process occurs for horizonless geometries, and particles are composed of fermions. Here, we resolve the tension in its different aspects, by showing that (i) superradiance occurs for self-interacting fermions on flat spacetime. (ii) Superradiance occurs also for horizonless geometries, where it leads to an ergoregion instability. Ultracompact, horizonless geometries will usually respond with echoes of growing amplitude, until rotational (or electrostatic) energy is extracted from the object. (iii) The Fourier-domain analysis leads to absence of superradiance when horizons are not present. We elucidate why this analysis fails to give meaningful results. (iv) Finally, we show that superradiant, ergoregion instabilities have a particle analog of similar growth timescales and which can power the formation of a structure outside a compact, rotating star.",
keywords = "BLACK-HOLE, DIRAC-EQUATION, KLEIN PARADOX, WAVE, FIELD, EXTRACTION, ENERGETICS, RADIATION, ENERGY",
author = "Rodrigo Vicente and Vitor Cardoso and Lopes, {Jorge C.}",
year = "2018",
month = apr,
day = "16",
doi = "10.1103/PhysRevD.97.084032",
language = "English",
volume = "97",
journal = "Physical Review D",
issn = "2470-0010",
publisher = "American Physical Society",
number = "8",

}

RIS

TY - JOUR

T1 - Penrose process, superradiance, and ergoregion instabilities

AU - Vicente, Rodrigo

AU - Cardoso, Vitor

AU - Lopes, Jorge C.

PY - 2018/4/16

Y1 - 2018/4/16

N2 - Superradiant scattering is a radiation enhancement process that takes place in many contexts, and which has recently found exciting applications in astrophysics and particle physics. In the framework of curved spacetime physics, it has been associated with the classical Penrose process for particles. Superradiance is usually also associated with bosonic fields around geometries with ergoregions and horizons. These notions are in clear tension however: the Penrose process occurs for horizonless geometries, and particles are composed of fermions. Here, we resolve the tension in its different aspects, by showing that (i) superradiance occurs for self-interacting fermions on flat spacetime. (ii) Superradiance occurs also for horizonless geometries, where it leads to an ergoregion instability. Ultracompact, horizonless geometries will usually respond with echoes of growing amplitude, until rotational (or electrostatic) energy is extracted from the object. (iii) The Fourier-domain analysis leads to absence of superradiance when horizons are not present. We elucidate why this analysis fails to give meaningful results. (iv) Finally, we show that superradiant, ergoregion instabilities have a particle analog of similar growth timescales and which can power the formation of a structure outside a compact, rotating star.

AB - Superradiant scattering is a radiation enhancement process that takes place in many contexts, and which has recently found exciting applications in astrophysics and particle physics. In the framework of curved spacetime physics, it has been associated with the classical Penrose process for particles. Superradiance is usually also associated with bosonic fields around geometries with ergoregions and horizons. These notions are in clear tension however: the Penrose process occurs for horizonless geometries, and particles are composed of fermions. Here, we resolve the tension in its different aspects, by showing that (i) superradiance occurs for self-interacting fermions on flat spacetime. (ii) Superradiance occurs also for horizonless geometries, where it leads to an ergoregion instability. Ultracompact, horizonless geometries will usually respond with echoes of growing amplitude, until rotational (or electrostatic) energy is extracted from the object. (iii) The Fourier-domain analysis leads to absence of superradiance when horizons are not present. We elucidate why this analysis fails to give meaningful results. (iv) Finally, we show that superradiant, ergoregion instabilities have a particle analog of similar growth timescales and which can power the formation of a structure outside a compact, rotating star.

KW - BLACK-HOLE

KW - DIRAC-EQUATION

KW - KLEIN PARADOX

KW - WAVE

KW - FIELD

KW - EXTRACTION

KW - ENERGETICS

KW - RADIATION

KW - ENERGY

U2 - 10.1103/PhysRevD.97.084032

DO - 10.1103/PhysRevD.97.084032

M3 - Journal article

VL - 97

JO - Physical Review D

JF - Physical Review D

SN - 2470-0010

IS - 8

M1 - 084032

ER -

ID: 299202272