Please use this identifier to cite or link to this item: http://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/11402
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dc.contributor.authorSINGH, JASVEERen_US
dc.contributor.authorVARDARAJAN, SUNEETAen_US
dc.date.accessioned2026-08-04T11:31:22Z
dc.date.available2026-08-04T11:31:22Z
dc.date.issued2026-07en_US
dc.identifier.citationPhysical Review D, 114, 024057.en_US
dc.identifier.issn2470-0029en_US
dc.identifier.issn2470-0010en_US
dc.identifier.urihttps://doi.org/10.1103/h2yj-x6qgen_US
dc.identifier.urihttp://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/11402
dc.description.abstractWe revisit an analytical approximation scheme for computing nonlinearity ratios involving quadratic quasinormal modes (QQNMs). We compute these ratios for the general case when the QQNM is not one of the linear QNMs, for the (𝑙,𝑚) channel (2,2) ×(2,2) →(4,4). We find an excellent match with numerical simulations. We also discuss where and why the method can fail, for example, for the channel (2,0) ×(2,0) →(2,0), where we can only get crude estimates for the nonlinearity ratio. Motivated by recent studies on nonlinear ringdown at the horizon, we also compute the nonlinearity ratios at the horizon. We find that the ratio both at the horizon and infinity is insensitive to different choices of regularization of the source term in the second-order perturbations. We also discuss amplitudes of QQNMs sourced by linear overtones. Finally, we discuss the issues that must be resolved within this method to do precision analysis of nonlinear ringdown.en_US
dc.language.isoenen_US
dc.publisherAmerican Physical Societyen_US
dc.subjectGeneral relativityen_US
dc.subject2026-JUL-WEEK4en_US
dc.subjectTOC-JUL-2026en_US
dc.subject2026en_US
dc.titleComputing nonlinearity ratios using second-order black hole perturbation theoryen_US
dc.typeArticleen_US
dc.contributor.departmentDept. of Physicsen_US
dc.identifier.sourcetitlePhysical Review Den_US
dc.publication.originofpublisherForeignen_US
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