Dominik Stamen, Jan Luca Dammann, Yannis Korte, Bastian Kubis
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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.