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The angle-dependent interlayer magnetoresistance of the pressurized (to the normal metallic state) layered organic metal α-(BEDT-TTF)₂KHg(SCN)₄ is found to change from the conventional behavior at low magnetic fields to an anomalous one at high fields. The dependence of this field-induced crossover on the sample purity and temperature reveals parallel contribution of the classical Boltzmann and incoherent channels in the interlayer conductivity. The latter channel, having a metallic temperature dependence but being insensitive to an in-plane magnetic field, may be responsible for magnetoresistance anomalies observed in a number of layered metals. We propose a possible mechanism for the incoherent channel combining interlayer tunneling via local hopping centers and intralayer diffusion.
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Kartsovnı̆k et al. (2009) studied this question.
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