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Following the re-establishment of the \sigma(600) and the \kappa(900), thelight scalar mesons a_0(980) and f_0(980) together with the \sigma(600) and the\kappa(900) are considered as the chiral scalar partner of pseudoscalar nonetin SU(3) chiral symmetry, and the high mass scalar mesons a_0(1450),K^*_0(1430), f_0(1370) and f_0(1710) turned out to be considered as the L=1q\bar{q} scalar mesons. We assume that the high mass of the L=1 q\bar{q} scalarmesons is caused by the mixing with the light scalar mesons. For the structureof the light scalar mesons, we adopted the qq\bar{q}\bar{q} model in order toexplain the "scalar meson puzzle". The inter-mixing between the light scalarnonet and the high mass L=1 q\bar{q} nonet and the intra-mixing among eachnonet are analyzed by including the glueball into the high mass scalar nonet.Comment: 16 pages, 5 figure

Mixing among light scalar mesons and L $equal$ 1 q$\bar q$ scalar mesons