Molecular aspects of charm physics
We study the influence of possible molecular structures in the charmonium spectrum. We focus on the 0{sup ++}, 1{sup ++} and 1{sup --} sectors. In the first one we coupled the 2{sup 3}P{sub 0}cc pair with DD, J/{psi}{omega}, D{sub s}D{sub s} and J/{psi}{phi} channels and we obtain two states compatibles with the X(3945) and the Y(3940). In the second one we couple the 2{sup 3}P{sub 1}cc state with the DD{sup *} channel and we obtain a dressed state compatible with the X(3940) and a new state that we assign to the X(3872). In the third one we include the 3{sup 3}S{sub 1} and 2{sup 3}D{sub 1} charmonium states coupled to DD, DD{sup *}, D{sup *}D{sup *}, D{sub s}D{sub s}, D{sub s}D{sup *}s and D{sup *}{sub s}D{sup *}{sub s}. In this calculation we obtain a new molecular state that could be the G(3900) or the controversial Y(4008) and two cc states dressed by the molecular components assigned to the {psi}(4040) and the {psi}(4160). Finally we perform a calculation in the five quark sector where we can describe the {Lambda}{sub c}(2940){sup +} as a ND{sup *} molecular state and predict a {Lambda}{sub b}(6248){sup +} state.