Abstract
Abstract Fermi–liquid theory in two dimensions, for electron or hole liquids flowing through antiferromagnetic assemblies, yields RT 1 α T, where R is the electrical resistivity and T 1 −1 the nuclear relaxation rate. This relation holds over an appropriate temperature range for Cu spins in underdoped high Tc cuprates. Here a non–Fermi–liquid phase of a strongly disordered metallic spin glass is pointed out to exhibit a relation RT 1 ∝ Tn , again over a restricted temperature range, where the exponent n has the meanfield value of 5/4.
Sign-in/Register to access full text options 
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.
