Advances in the physics of high-temperature superconductivity
By J. Orenstein, A. Millis. Science, 2000
706 citations recorded by the source corpus.
Subfields: Condensed Matter Physics, Electronic, Optical and Magnetic Materials
View Paper: https://www.semanticscholar.org/paper/12247b8416650b8b5e197d92778305f52c972a28
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In Condensed Matter Physics
In Electronic, Optical and Magnetic Materials
Citations in the corpus
- Doping a Mott insulator: Physics of high-temperature superconductivity (2004, background): “Orenstein and Millis, 2000 and Norman and Pepin, 2003 have provided highly readable accounts of experiments and general theoretical approaches.”
- Quantum Simulation (2013, background): “The CuO2 plane in a high-Tc superconductor (Orenstein and Millis, 2000) could be simulated in an analog manner by an array of electrostatically defined quantum dots, as suggested in (Manousakis, 2002) in one of the early proposals for AQS.”
- Progress and perspectives on electron-doped cuprates (2009, neutral): “29 31 v2 [ co nd -m at .s up rco n] 1 1 M ar 2 01 0 2 celli et al., 2003; Fischer et al., 2007; Kastner et al., 1998; Lee et al., 2006b; Orenstein and Millis, 2000; Scalapino, 1995; Timusk and Statt, 1999).”
- Angle-resolved photoemission studies of the cuprate superconductors (2002, background): “This point is centrally important to high-Tc superconductivity and the high-temperature superconductors, which are poor conductors in the normal state with a behavior fundamentally different from the Fermi-liquid paradigm and are often regarded as doped antiferromagnets (Orenstein and Millis, 2000).”
- SO(5) theory of antiferromagnetism and superconductivity (2004, background): “Instead, we refer the readers to a number of excellent review articles on the subject sImada et al., 1998; Kastner et al., 1998; Maple, 1998; Timusk and Statt, 1999; Orenstein and Millis, 2000; Campuzano et al., 2002; Yeh, 2002; Damascelli et al., 2003d.”
- Charge-order-maximized momentum-dependent superconductivity (2007, background): “In contrast to purely electron–phonon coupled systems, the high- T c copper oxide superconductors show superconductivity in close proximity to spin-density-wave order/antiferromagnetis”
- Imaging the two gaps of the high-temperature superconductor Bi 2 Sr 2 CuO 6+ x (2007, background): “In HTSC, however, the two energy scales are on the same order, especially in the underdoped region, where ps could be weaker, and therefore it would be Ps rather than A that determines the onset of superconductivity [16, 3, 13].”