(ricevuto il 25 Febbraio 1994; approvato il 12 Marzo 1994) Summary. --It is stressed that the stability of the superconducting ground state in the two-band model is guaranteed for both signs of the leading interband interaction W. Thereby the requirement for the energy minimum fixes the phase differences of two order parameters as I~1 -~21 = 0, 2= .... if W < 0 and t~1 -~21 = =, 3= .... if W > 0, and this difference is reflected in the ground-state wave function.PACS 63.90 -Other topics in lattice dynamics and crystal statistics.In the multiband models of superconductivity [1][2][3] it, is well known that the pairing may be achieved for both signs of the intei, band interactions [3,4]. For high-Te superconductors there is a number of new multiband approaches, see, e.g., review [5]. In the scheme developed in papers [6-8] the total leading interband interaction W, consisting of the Coulomb and the electron-phonon part, is assumed to be positive. In the multigap approach adopted in papers [9,10] the negative value of W leading to stable superconductive state has been emphasized [10] as a consequence of the assumption of a model exclusively relying upon electron-phonon interactions near the Fermi surface.The aim of the present note is to show that, regardless of the signature of W, the stability of the superconducting state can be guaranteed if the phase differences of the order parameters are properly fixed. For simplicity a two-band model is used.The starting Hamiltonian is of the same form as in [6] (1) a~-k~ a:,_k,~ a:,,k,~ 9 ~,k,s ~,~' k,k' Here the electron band energies ~(k) are measured with respect to the chemical potential, the arrows indicate the spin (s) orientation, and the second term--the (*) Permanent address: