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Continuum bound states K L, D 1(2420), D s1(2536), and their partners K S, D 1(2400), D * sJ(2463)
Authors:E van Beveren and G Rupp
Institution:(1) Centro de Física Teórica, Departamento de Física, Universidade de Coimbra, 3000 Coimbra, Portugal;(2) Instituto Superior Técnico, Centro de Física das Interacções Fundamentais, Edifício Ciência, 1049-001 Lisboa Codex, Portugal
Abstract:The very recently observed D*sJ(2463) meson is described as a $J^{P}\! = \!1^{ + }$ $c\bar{s}$ bound state in a unitarised meson model, owing its existence to the strong OZI-allowed $^{3}\!P_{0}$ coupling to the nearby S-wave $D^{*}\!K$ threshold. By the same non-perturbative mechanism, the narrow axial-vector Ds1(2536) resonance shows up as a quasi-bound-state partner embedded in the $D^{*}\!K$ continuum. With the same model and parameters, it is also shown that the preliminary broad 1 + D1(2400) resonance and the established narrow 1 + D1(2420) may be similar $c\bar{n}$ partners, as a result of the strong OZI-allowed $^{3}\!P_{0}$ coupling to the nearby S-wave $D^{*}\!\pi$ threshold. The continuum bound states D1(2420) and Ds1(2536) are found to be mixtures of 33% $^{3\!}P_{1}$ and 67% $^{1\!}P_{1}$ , whereas their partners D1(2400) and D*sJ(2463) have more or less the opposite $^{2S + 1}\!P_1$ -state content, but additionally with some $D^{*}\!\pi$ or $D^{*}\!K$ admixture, respectively. The employed mechanism also reproduces the ratio of the KL-KS mass difference and the KS width, by describing KL as a bound state embedded in the $\pi\pi$ continuum. The modelrsquos results for $J^{P}\! = \!1^{ + }$ states containing one b quark are also discussed.Received: 7 June 2003, Revised: 20 October 2003, Published online: 18 December 2003PACS: 12.40.Yx, 14.40.Aq, 14.40.Lb, 13.25.Es, 13.25.Ft, 13.75.Lb
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