M otion of scalar (i.e. spinless) particles in quantum mechanics is investigated by solving Klein-Gordon equation (relativistic case) or Schrödinger equation (non-relativistic case) for the interaction in system [1, 2]. This interaction is represented by a potential function which is crucial for solving the eigenvalue equation, since it acts a part to determine the solving technique. The hyperbolic type molecular potential (or symmetrical well potential) [3] is one of the attractive potentials, and it represents some interactions in atomic and molecular levels. After Buyukkilic and friends introduced the potential and obtained one dimensional non-relativistic solutions in Ref.[3], many papers in which various solving methods are used, have been come out in the last decade. For instance, in Ref.[4], Yang has generalized the symmetrical well potential to the deformed one by way of the deformed hyperbolic functions [5]. In Ref.[6], exact solutions of relativistic cases have been obtained for l=0 states. Furthermore, Refs. [7, 8] can be adduced for using different solving methods to investigate the symmetrical well potential. Recently, Candemir[9] has tackled Klein-Gordon equation in spherical-coordinates, for equal vector and scalar symmetrical well potential. She has obtained the solutions for states by using Nikiforov-Uvarov (NU) method[10]. She has also used Green-Aldrich