The application of a small magnetic field (B≈0.1T) either parallel or perpendicular to a low-density (≈10¹¹cm^-2) magnetic two-dimensional electron gas (2DEG) creates a striking positive magnetoresistance of up to 700%. This is a spin effect, caused by the suppression of spin-dependent hopping paths between localized states with on-site correlation. At higher fields, a spin-related delocalization is observed. In the perpendicular field geometry, orbital effects combine with this delocalization and lead to quantum phase transitions between the spin-polarized insulating state and the ν=1 quantum Hall liquid.
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Smorchkova et al. (1998) studied this question.
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