Models of one dimensional systems with short range correlated disorder have predicted the existence of an energy region where the states are delocalized. This is contrary to the earlier belief that all the eigenstates are localized in 1D disordered systems. We study the statistical properties of the spectra of finite superlattices made up of short chains of random binary alloy which present correlated disorder.In mesoscopic physics the effect of disorder on the electron propagation leads to the Anderson metal-insulator transition at T ¼ 0 [1]. It is generally argued that, in the case of full randomness of parameters of the model, all states are localized in 1D systems [2]. This implies that there is no diffusive (metallic) behavior. However, in recent years, a number of models [3][4][5] predict that, as a consequence of the introduction of short range correlations, there are sets of extended states in a determined energy region. One of these models is called the repulsive binary alloy (RBA), in which the inhibition of bonding between two elements of one of the two atomic species results in the above mentioned correlations [6]. In a previous work we have presented [7] a model of a disordered quantum well consisting of a short portion of RBA within ordered barriers. Within the energy range where the well material presents these extended states, the system shows quantum effects due to spatial confinement. This is a consequence of the multiple constructive interference of those states whose localization lengths are at least three times longer than the well width. An interesting question arises about the coupling of disordered quantum wells in finite superlattices (SLs). The aim of this paper is to present statistical properties of energy spectra in disordered one dimensional finite SLs and relate them to the transport properties.We show that the coupling of disordered quantum wells can be described by appropriate nearest level spacing statistics for an ensemble of SLs [8]. Furthermore, the level spacing statistics evolve to Poisson or Wigner surmise distributions in finite SLs as a function of the miniband position within the delocalization window as well as of the level position within their respective minibands.The Hamiltonian corresponds to a one-dimensional tight-binding chain of s-like orbitals, H ¼ P n ðE n jni hnj þ V n;nþ1 jni hn þ 1j þ V nþ1;n jn þ 1i hnjÞ :The well material has a length of 40 atomic sites which are framed by ordered barriers consisting of l b ð¼ 2; 3Þ sites for each ensemble. The whole chain itself is framed on both