2004/07/16 by M. Ortolani, Michele Ortolani, P. Calvani +1 · 4 citations
Materials Science · Physics and Astronomy · #Advanced Condensed Matter Physics #Magnetic and transport properties of perovskites and related materials #Physics of Superconductivity and Magnetism #cond-mat.str-el #cond-mat.supr-con
paper · pdf · doi:10.1103/physrevlett.94.067002
published as Phys. Rev. Lett. 94, 067002 (2005) · 4 pages with 3 figs
arxiv created 2004/07/16 · openalex publication_date 2005/02/14 · arxiv updated 2009/12/01 · openalex created_date 2016/06/24 · openalex updated_date 2026/07/28
In La_2\ensuremath-xSrxCuO4 (LSCO) the spectral weight W=\ensuremath∫0^\ensuremathΩ\ensuremathσ1ab(\ensuremathω,T)d\ensuremathω [where \ensuremathσ1ab(\ensuremathω,T) is the ab-plane conductivity] obeys the same law W=W0\ensuremath-B(\ensuremathΩ)T2 as in a conventional metal such as gold, for any \ensuremathΩ up to the plasma edge. However, in LSCO B(\ensuremathΩ) points toward correlation effects and, unlike in gold, is related to an energy scale tT\ensuremath≪t0\ensuremath∼W0. The Ferrell-Glover-Tinkham sum rule is fulfilled in LSCO superconductors for \ensuremathΩ\ensuremath\gtrsim2000 cm^\ensuremath-1.