On Some Common Features in High- and Low-TC Superconducting Perovskites
I. Vobornik, D. Ariosa, Helmuth Berger, L. Forró, Rafael Gatt, M. Grioni, G. Margaritondo, M. Onellion, Torsten Schmauder, Davor Pavuna
Abstract
I. Vobornik, D. Ariosa, Helmuth Berger, L. Forró, Rafael Gatt, M. Grioni, G. Margaritondo, M. Onellion, Torsten Schmauder, Davor Pavuna
Abstract
Recent photoemission evidence for non-zero gap in highly overdoped Bi 2 Sr 2 -CaCu 2 O 8+x , along the directions in the Brillouin zone where the d -wave gap exhibits nodes, is in accordance with more conventional behavior in strongly overdoped high- T c cuprates. This differs from underdoped regime, where departures from Fermi-liquid (FL) behavior are found. Observed non-FL linear resistivity up to ~ 1050 K in low- T c perovskite Sr 2 RuO 4−δ is reminiscent of cuprates and implies some similarities between high- and low- T c perovskites.
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Recent photoemission evidence for non-zero gap in highly overdoped Bi 2 Sr 2 -CaCu 2 O 8+x , along the directions in the Brillouin zone where the d -wave gap exhibits nodes, is in accordance with more conventional behavior in strongly overdoped high- T c cuprates. This differs from underdoped regime, where departures from Fermi-liquid (FL) behavior are found. Observed non-FL linear resistivity up to ~ 1050 K in low- T c perovskite Sr 2 RuO 4−δ is reminiscent of cuprates and implies some similarities between high- and low- T c perovskites.
Key concepts: Condensed matter physics, Brillouin zone, Cuprate, Superconductivity, Perovskite (structure), Electrical resistivity and conductivity, Fermi Gamma-ray Space Telescope, Physics