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Quasi-four-body semileptonic decay $\bar B^0\to a_0(1450)^+ (\toπ^+ η)\ell^-\barν_\ell$ within $a_0(1450)$-resonance leading-twist LCDA under QCDSR
The finite width of broad scalar resonances should be taken into account when relating semileptonic $B$-meson transitions to experimentally reconstructable multihadron final states. The quasi-four-body semileptonic decays $\bar B^0\to a_0(1450)^+ (\toπη)\ell^-\barν_\ell$ with $\ell=(e,μ,τ)$ provide
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