Abstract
We show our results for the bottomonium spectrum with self energy corrections, due to the coupling to the meson-meson continuum. We also discuss our results for the open bottom strong decays of higher bottomonia in the 3 P 0 pair-creation model.
Highlights
Continuum coupling effects, due to the creation of qqpairs, determine a shift of the physical mass of a hadron with respect to its bare mass, as already shown by several authors in the baryon [1] and meson [2,3,4,5,6] sectors
We show our results for the bottomonium spectrum with self energy corrections, due to the coupling to the meson-meson continuum
We show an application of the unquenched quark model (UQM) [4,5,6, 17,18,19] to the calculation of the bottomonium spectrum with self energy corrections [6]
Summary
Due to the creation of qqpairs, determine a shift of the physical mass of a hadron with respect to its bare mass, as already shown by several authors in the baryon [1] and meson [2,3,4,5,6] sectors. The resonance (1405) is strongly influenced by the nearby K N channel [7] and the f0(980) behaves remarkably as a KKmolecule [8] These continuum coupling (or pair-creation) effects, neglected in the naive quark model (QM) [9,10,11,12,13,14] Since the qqpair corresponds to a 3P0 quark-antiquark state, this is generally known as the 3P0 pair-creation model [20]. In this contribution, we show an application of the unquenched quark model (UQM) [4,5,6, 17,18,19] to the calculation of the bottomonium spectrum with self energy corrections [6].
Sign-in/Register to view highlights & summary Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Schedule a callDisclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.
