Abstract

We present two-flavor lattice QCD estimates of the hadronic couplings gB0∗Bπg_{B^*_0 B π} and gB1∗B0∗πg_{B_1^* B_0^* π} that parametrise the non leptonic decays B0∗→BπB^*_0 \to B π and B1∗→B0∗πB^*_1 \to B_0^* π. We use CLS two-flavour gauge ensembles. Our framework is the Heavy Quark Effective Theory (HQET) in the static limit and solving a Generalized Eigenvalue Problem (GEVP) reveals crucial to disentangle the B0∗B^*_0(B1∗B^*_1) state from the BπB π(B∗πB^*π) state. This work brings us some experience on how to treat the possible contribution from multihadronic states to correlation functions calculated on the lattice, especially when SS-wave states are involved.

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