Dynamics of strong and radiative decays of Ds-mesons in the hadrogenesis conjecture
O4; The positive parity scalar D*s0(2317) and axial-vector D*s1(2460) charmed strange mesons are generated by coupled-channel dynamics through the s-wave scattering of Goldstone bosons off the pseudoscalar and vector D(Ds)-meson ground states. The specific masses of these states are obtained as a co...
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Published in | Chinese physics C Vol. 34; no. 9; pp. 1320 - 1323 |
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Main Authors | , |
Format | Journal Article |
Language | English |
Published |
IOP Publishing
01.09.2010
Irfu/SPhN,CEA/Saclay,F-91191 Gif-sur-Yvette Cedex,France%GSI,Planckstrasse 1,D-64291 Darmstadt,Germany |
Subjects | |
Online Access | Get full text |
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Summary: | O4; The positive parity scalar D*s0(2317) and axial-vector D*s1(2460) charmed strange mesons are generated by coupled-channel dynamics through the s-wave scattering of Goldstone bosons off the pseudoscalar and vector D(Ds)-meson ground states. The specific masses of these states are obtained as a consequence of the attraction arising from the Weinberg-Tomozawa interaction in the chiral Lagrangian. Chiral corrections to order Q2χ are calculated and found to be small. The D*s0(2317) and D*s1(2460) mesons decay either strongly into the isospin-violating π0Ds and π0D*s channels or electromagnetically. We show that the π0-η and (K0D+-K+D0) mixings act constructively to generate strong widths of the order of 140 keV and emphasize the sensitivity of this value to the KD component of the states. The one-loop contribution to the radiative decay amplitudes of scalar and axial-vector states is calculated using the electromagnetic Lagrangian to chiral order Q2χ. We show the importance of taking into account processes involving light vector mesons explicitly in the dynamics of electromagnetic decays. The radiative width are sensitive to both η Ds and KD components, hence providing information complementary to the strong widths on the positive parity Ds-meson structure. |
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ISSN: | 1674-1137 2058-6132 |
DOI: | 10.1088/1674-1137/34/9/032 |