Study of the nonlinear instability of confined geometries

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Study of the nonlinear instability of confined geometries. / Okawa, Hirotada; Cardoso, Vitor; Pani, Paolo.

In: Physical Review D, Vol. 90, No. 10, 104032, 21.11.2014.

Research output: Contribution to journalJournal articleResearchpeer-review

Harvard

Okawa, H, Cardoso, V & Pani, P 2014, 'Study of the nonlinear instability of confined geometries', Physical Review D, vol. 90, no. 10, 104032. https://doi.org/10.1103/PhysRevD.90.104032

APA

Okawa, H., Cardoso, V., & Pani, P. (2014). Study of the nonlinear instability of confined geometries. Physical Review D, 90(10), [104032]. https://doi.org/10.1103/PhysRevD.90.104032

Vancouver

Okawa H, Cardoso V, Pani P. Study of the nonlinear instability of confined geometries. Physical Review D. 2014 Nov 21;90(10). 104032. https://doi.org/10.1103/PhysRevD.90.104032

Author

Okawa, Hirotada ; Cardoso, Vitor ; Pani, Paolo. / Study of the nonlinear instability of confined geometries. In: Physical Review D. 2014 ; Vol. 90, No. 10.

Bibtex

@article{13f3a244a9514e89ac0ce7279f8c43e2,
title = "Study of the nonlinear instability of confined geometries",
abstract = "The discovery of a {"}weakly turbulent{"} instability of anti-de Sitter spacetime supports the idea that confined fluctuations eventually collapse to black holes and suggests that similar phenomena might be possible in asymptotically flat spacetime, for example in the context of spherically symmetric oscillations of stars or nonradial pulsations of ultracompact objects. Here we present a detailed study of the evolution of the Einstein-Klein-Gordon system in a cavity, with different types of deformations of the spectrum, including a mass term for the scalar and Neumann conditions at the boundary. We provide numerical evidence that gravitational collapse always occurs, at least for amplitudes that are three orders of magnitude smaller than Choptuik's critical value and corresponding to more than 10(5) reflections before collapse. The collapse time scales as the inverse square of the initial amplitude in the small-amplitude limit. In addition, we find that fields with nonresonant spectrum collapse earlier than in the fully resonant case, a result that is at odds with the current understanding of the process. Energy is transferred through a direct cascade to high frequencies when the spectrum is resonant, but we observe both direct-and inverse-cascade effects for nonresonant spectra. Our results indicate that a fully resonant spectrum might not be a crucial ingredient of the conjectured turbulent instability and that other mechanisms might be relevant. We discuss how a definitive answer to this problem is essentially impossible within the present framework.",
keywords = "RELATIVITY",
author = "Hirotada Okawa and Vitor Cardoso and Paolo Pani",
year = "2014",
month = nov,
day = "21",
doi = "10.1103/PhysRevD.90.104032",
language = "English",
volume = "90",
journal = "Physical Review D",
issn = "2470-0010",
publisher = "American Physical Society",
number = "10",

}

RIS

TY - JOUR

T1 - Study of the nonlinear instability of confined geometries

AU - Okawa, Hirotada

AU - Cardoso, Vitor

AU - Pani, Paolo

PY - 2014/11/21

Y1 - 2014/11/21

N2 - The discovery of a "weakly turbulent" instability of anti-de Sitter spacetime supports the idea that confined fluctuations eventually collapse to black holes and suggests that similar phenomena might be possible in asymptotically flat spacetime, for example in the context of spherically symmetric oscillations of stars or nonradial pulsations of ultracompact objects. Here we present a detailed study of the evolution of the Einstein-Klein-Gordon system in a cavity, with different types of deformations of the spectrum, including a mass term for the scalar and Neumann conditions at the boundary. We provide numerical evidence that gravitational collapse always occurs, at least for amplitudes that are three orders of magnitude smaller than Choptuik's critical value and corresponding to more than 10(5) reflections before collapse. The collapse time scales as the inverse square of the initial amplitude in the small-amplitude limit. In addition, we find that fields with nonresonant spectrum collapse earlier than in the fully resonant case, a result that is at odds with the current understanding of the process. Energy is transferred through a direct cascade to high frequencies when the spectrum is resonant, but we observe both direct-and inverse-cascade effects for nonresonant spectra. Our results indicate that a fully resonant spectrum might not be a crucial ingredient of the conjectured turbulent instability and that other mechanisms might be relevant. We discuss how a definitive answer to this problem is essentially impossible within the present framework.

AB - The discovery of a "weakly turbulent" instability of anti-de Sitter spacetime supports the idea that confined fluctuations eventually collapse to black holes and suggests that similar phenomena might be possible in asymptotically flat spacetime, for example in the context of spherically symmetric oscillations of stars or nonradial pulsations of ultracompact objects. Here we present a detailed study of the evolution of the Einstein-Klein-Gordon system in a cavity, with different types of deformations of the spectrum, including a mass term for the scalar and Neumann conditions at the boundary. We provide numerical evidence that gravitational collapse always occurs, at least for amplitudes that are three orders of magnitude smaller than Choptuik's critical value and corresponding to more than 10(5) reflections before collapse. The collapse time scales as the inverse square of the initial amplitude in the small-amplitude limit. In addition, we find that fields with nonresonant spectrum collapse earlier than in the fully resonant case, a result that is at odds with the current understanding of the process. Energy is transferred through a direct cascade to high frequencies when the spectrum is resonant, but we observe both direct-and inverse-cascade effects for nonresonant spectra. Our results indicate that a fully resonant spectrum might not be a crucial ingredient of the conjectured turbulent instability and that other mechanisms might be relevant. We discuss how a definitive answer to this problem is essentially impossible within the present framework.

KW - RELATIVITY

U2 - 10.1103/PhysRevD.90.104032

DO - 10.1103/PhysRevD.90.104032

M3 - Journal article

VL - 90

JO - Physical Review D

JF - Physical Review D

SN - 2470-0010

IS - 10

M1 - 104032

ER -

ID: 300080988