It can be derived as a function of doping using a generalized Berezinskii-Kosterlitz-Thouless renormalization group theory.
It can be derived as a function of doping using a generalized Berezinskii-Kosterlitz-Thouless renormalization group theory. It can also be defined as the minimum or maximum of the second-order partial derivative of resistivity with respect to temperature, (*) depending on whether the material's resistivity has a peak. It is significantly lower for nanocrystalline chromiumthan it is for strain-free single-crystal chromium, as the former does not need to be as warm for its atomic magnetic dipoles to align with an external magnetic field. FTP, name this analog of the Curie temperature, the point above which an antiferromagnetic material becomes paramagnetic.
It can be derived as a function of doping using a generalized Berezinskii-Kosterlitz-Thouless renormalization group theory.
{Neel} temperature