The energy-frequency diagram of the (1+1)-dimensional Φ4 oscillon

A bstract Two different methods are used to study the existence and stability of the (1+1)-dimensional Φ 4 oscillon. The variational technique approximates it by a periodic function with a set of adiabatically changing parameters. An alternative approach treats oscillons as standing waves in a finite-size box; these are sought as solutions of a boundary-value problem on a two-dimensional domain. The numerical analysis reveals that the standing wave’s energy-frequency diagram is fragmented into disjoint segments with ω n +1 < ω < ω n , where ω n = ω 0 /( n + 1), n = 0, 1, 2, . . ., and ω 0 is the endpoint of the continuous spectrum (mass threshold of the model). The variational approximation involving the first, zeroth and second harmonic components provides an accurate description of the oscillon with the frequency in ( ω 1 , ω 0 ), but breaks down as ω falls out of that interval.

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Publication Details

Journal
Journal of High Energy Physics
Published
2024-10-18
DOI
https://doi.org/10.1007/jhep10(2024)136
Citations
5
Primary Topic
Mechanical and Optical Resonators
Type
article
Field-Weighted Citation Impact
1.69
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article

The energy-frequency diagram of the (1+1)-dimensional Φ4 oscillon

I. V. Barashenkov, N. V. Alexeeva, Alain Dika, Raphael De Sousa
5 citations
Journal of High Energy Physics
Mechanical and Optical Resonators
1.69
article

The energy-frequency diagram of the (1+1)-dimensional Φ4 oscillon

I. V. Barashenkov, N. V. Alexeeva, Alain Dika, Raphael De Sousa
article en
5 citations

Abstract

A bstract Two different methods are used to study the existence and stability of the (1+1)-dimensional Φ 4 oscillon. The variational technique approximates it by a periodic function with a set of adiabatically changing parameters. An alternative approach treats oscillons as standing waves in a finite-size box; these are sought as solutions of a boundary-value problem on a two-dimensional domain. The numerical analysis reveals that the standing wave’s energy-frequency diagram is fragmented into disjoint segments with ω n +1 < ω < ω n , where ω n = ω 0 /( n + 1), n = 0, 1, 2, . . ., and ω 0 is the endpoint of the continuous spectrum (mass threshold of the model). The variational approximation involving the first, zeroth and second harmonic components provides an accurate description of the oscillon with the frequency in ( ω 1 , ω 0 ), but breaks down as ω falls out of that interval.

Journal of High Energy PhysicsVol. 2024(10)
University of Cape Town (ZA), Joint Institute for Nuclear Research (RU)
Affordable and clean energy
Openalex Percentile: Top 16%
Mechanical and Optical Resonators
1.69
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