Resonant tunneling through superlattice and multiquantum-well heterostructures has attracted considerable attention recently because of its possible application in ultrahighspeed electronic devices. The technique for atomic layer doping, &doping, is currently the subject of experimental and theoretical studies, as it can provide very high electronic sheet densities with enhanced low-field mobility in compound semiconductors [l]. For a GaAs/Al,Ga,-,As heterostructure as an example, Si or Be sources can be used for such doping layers [2]. The charcteristics of resonant tunneling diodes and the mechanism of the electron tunneling are strongly affected by the doping profile of the structures, so it is interesting to investigate these modified structures.Recently, Beltram and Capasso [3] and Ihm et al. [4] have shown that enormous changes in the electronic states of a superlattice can be made by introducing spatially localized defects with a periodic array in the well layers as well as in the barrier layers of a superlattice.They also found that the creation of a band or the annihilation of a given band and the control of the miniband gap, band positions, and their widths are possible by adjusting the weight and the inserted defects. More recent calculations done by Arsenault and Meunier [5] have shown that the resonant energy of a &doped carrier has a larger width than an identical double-barrier structure. Very recently, Pandey et al.[6] and Gu et al. [7] have shown that with a scattering center in the well, the transmission probability and the resonance energies may change and interesting effects are exposed. However, they all assumed an equal effective mass for the barrier and the well regions and have not obtained analytical expressions for the transmission probability and the resonance condition, although this is necessary for the analysis and prediction of experimental results for the doped double-barrier structures.In this note, we present calculations on the resonant tunneling through a double-barrier structure with an impurity sheet in the middle of the well, we use a &function to describe the scattering perturbation potential of the impurity sheet. Along with the analytical expressions for the transmission probability and the resonance condition, which properly account for the mass profile of this structure, the effect of the scattering on transmission probability and the resonance energy have been numerically calculated as well. It is found that the effects of scattering reduce the transmission probability and broaden the transmission peaks, and all these effects depend strongly on the scattering strength of the impurity sheet. Our calculations also show that the impurity sheet may be an additional growthcontrolling parameter and can be used to modify the energy structure of the quantum well.I ) Lanzhou 730000, People's Republic of China.