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The resulting field dependences of the magnetoconductivity and magnetoresistivity tensor components are presented and discussed.
The components of the electrical magnetoconductivity and magnetoresistivity tensors of indium were calculated by the path integral method with a formulation used previously for aluminum.
The induced torque calculated from the computed magnetoresistivity components is in excellent agreement with measured anisotropy and field dependence of the induced torque.
His focus has been on structure-property relationships in pigments, thermoelectrics, high-temperature superconductivity, magnetoresistivity, solid fast ion conductors and high-K dielectrics.
The components of the electrical magnetoconductivity and magnetoresistivity tensors of aluminum were calculated by the path-integral method using a nearly-free-electron Fermi surface and a uniform relaxation time.
The longitudinal–transverse components of magnetoresistivity can saturate at values as high as 0.16 of the zero-field resistivity, but the effects of the longitudinal–transverse magnetoconductivity on the magnetoresistance and Hall coefficients are small.
The magnetoconductivity and magnetoresistivity tensors of cadmium have been calculated by the path integral method for magnetic fields in the and directions. A uniform relaxation time and a modified nearly free electron Fermi surface were used.