Conclusion
We have measured the electrical conductivity of NTD 70Ge:Ga to study the metal-insulator transition, ruling out an ambiguity due to inhomogeneous distribution of impurities. The critical exponent μ≈0.5 in zero magnetic field for doped semiconductors without impurity compensation has been confirmed. On the insulating side of the MIT, while the relation 2V≈ζ predicted by scaling theories [15] holds for 0.9 <N/NC <1, the critical exponents for localization length and impurity dielectric susceptibility change at N/NC ≈0.99. The small amount of doping compensation that is unavoidably present in our samples may be responsible for such a change in the exponents. We have also measured the conductivity in magnetic fields up to B=8 T in order to study the doping-induced MIT (in magnetic fields) and the magnetic-field-induced MIT. For both of the MIT, the critical exponent of the conductivity is 1.1, which is different from the value 0.5 at B=0. The change of the critical exponent caused by the applied magnetic fields supports a picture in which μ varies depending on the universality class to which the system belongs. The phase diagram has been determined in magnetic fields for the 70Ge:Ga system.
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Watanabe, M. (2002). Metal-Insulator Transition in Homogeneously Doped Germanium. In: Thorpe, M.F., Phillips, J.C. (eds) Phase Transitions and Self-Organization in Electronic and Molecular Networks. Fundamental Materials Research. Springer, Boston, MA. https://doi.org/10.1007/0-306-47113-2_18
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