Abstract
It is observed that the ratio, A/γ 2, has a common value of 1.0 × 10 −5 μωcm (mole K/mJ) 2 for all of the heavy Fermion compounds, where A is the coefficient of the quadratic term in the temperature dependence of the resistivity and γ is the coefficient of the linear term in the temperature dependence of the specific heat. This universal value, which is at least an order of magnitude above that of common d- band metals, is not accounted for by current microscopic theories and strongly indicates that a more unified understanding of the electron scattering mechanism is required for heavy Fermion materials.
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Schedule a callDisclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.
