A quasi two-body QCD factorization is used to study the
D^0 \rightarrow K^0_S \pi^+ \pi^- decay channel. Starting from the weak effective Hamiltonian, 28 tree and annihilation (W-exchange) amplitudes build up the full
D^0 \rightarrow K^0_S \pi^+ \pi^- amplitude [1]. The meson-meson final state interactions are described by the kaon-pion and pion scalar and vector form factors for the S and P w
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