scholarly journals Valence Bond Glass Theory of Electronic Disorder and the Pseudogap State of High-Temperature Cuprate Superconductors

2009 ◽  
Vol 102 (10) ◽  
Author(s):  
Liang Ren Niestemski ◽  
Ziqiang Wang
2021 ◽  
pp. 316-342
Author(s):  
Andrew Zangwill

Anderson is the only theorist who answers questions at a news conference at the 1987 March Meeting of the American Physical Society (the “Woodstock of Physics”) where most physicists learned details about the newly discovered high-temperature cuprate superconductors, which lose all resistance at temperatures not very far below room temperature. He had just proposed a radical non-BCS theory which attributed superconductivity in these materials to a “resonating valence bond” description of a doped Mott insulator using a model first proposed by John Hubbard. He spent the next twenty years trying to convince his colleagues of the correctness of this theory, with only limited success.


2011 ◽  
Vol 12 (5-6) ◽  
pp. 446-460 ◽  
Author(s):  
Baptiste Vignolle ◽  
David Vignolles ◽  
David LeBoeuf ◽  
Stéphane Lepault ◽  
Brad Ramshaw ◽  
...  

1996 ◽  
Vol 10 (07) ◽  
pp. 805-845 ◽  
Author(s):  
LAN YIN ◽  
SUDIP CHAKRAVARTY

Spectral anomaly for interacting fermions is characterized by the spectral function A ([k − k F ], ω) satisfying the scaling relation A (Λy1 [k − k F ], Λy2 ω) =ΛyA A ([k − k F ], ω), where y1, y2, and yA are the exponents defining the universality class. For a Fermi liquid y1 = 1, y2 = 1, yA = −1; all other values of the exponents are termed anomalous. In this paper, an example for which y1 = 1, y2 = 1, but yA = α − 1 is considered in detail. Attractive interaction added to such a critical system leads to a novel superconducting state, which is explored and its relevance to high temperature cuprate superconductors is discussed.


1999 ◽  
Vol 13 (29n31) ◽  
pp. 3688-3692 ◽  
Author(s):  
Howard A. Blackstead ◽  
John D. Dow ◽  
Martin Lehmann

Based (i) on data for the Pb 2 Sr 2 YCu 3 O 8 (PSYCO) homologues with Y replaced by R = Ce or R = Am, and (ii) on experimental facts for Nd 2-z Ce z CuO 4, we conclude that all the main high-temperature cuprate superconductors are p-type, and that very likely none are n-type.


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