Dominik Stamen, Jan Luca Dammann, Yannis Korte, Bastian Kubis
{"title":"Polarizabilities from kaon Compton scattering","authors":"Dominik Stamen, Jan Luca Dammann, Yannis Korte, Bastian Kubis","doi":"arxiv-2409.05955","DOIUrl":null,"url":null,"abstract":"The polarizabilities of light pseudoscalar mesons can be extracted from\ndifferential cross sections for Compton scattering near threshold. While this\nhas been accomplished for charged pions employing Primakoff reactions, a\ncorresponding measurement for kaons will be affected by the presence of the\n$K^*(892)$ resonance not too far from threshold. We propose a method to extend\nthe energy range serviceable for this purpose by reconstructing the $K^*(892)$\ncontribution model-independently from its $K\\pi$ intermediate state, using\ndispersion theory. We point out that, in contrast to the charged-pion analog,\nthere is likely no strong hierarchy between sum and difference of electric and\nmagnetic dipole polarizabilities; we discuss the sensitivity to disentangling\nboth by improved experimental angular coverage.","PeriodicalId":501573,"journal":{"name":"arXiv - PHYS - Nuclear Theory","volume":"4 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-09-09","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - Nuclear Theory","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.05955","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
The polarizabilities of light pseudoscalar mesons can be extracted from
differential cross sections for Compton scattering near threshold. While this
has been accomplished for charged pions employing Primakoff reactions, a
corresponding measurement for kaons will be affected by the presence of the
$K^*(892)$ resonance not too far from threshold. We propose a method to extend
the energy range serviceable for this purpose by reconstructing the $K^*(892)$
contribution model-independently from its $K\pi$ intermediate state, using
dispersion theory. We point out that, in contrast to the charged-pion analog,
there is likely no strong hierarchy between sum and difference of electric and
magnetic dipole polarizabilities; we discuss the sensitivity to disentangling
both by improved experimental angular coverage.