Abstract

In order to calculate the critical concentration for the metal–insulator transition in doped semiconductors, we study a model of randomly positioned interacting hydrogenic atoms within the one-electron approximation. We calculate approximate eigenfunctions for the system with the standard linear combination of atomic orbital variation method, considering explicitly the nonorthogonality of hydrogenic 1s orbitals. We then compute the correlation length using the concept of quantum connectivity, which we developed to study the localization transition in other disordered quantum-mechanical models. Finally, we employ a finite-size scaling analysis to determine the critical impurity concentration nc. If the isolated impurities have a Bohr radius a, then we find that Rc≡n1/3ca=0.250±0.011, which is in good agreement with experiment (Rc=0.26±0.05).

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