“APPLICATIONS OF THE SPIN POLARON THEORY AS A MICROSCOPIC MECHANISM OF HIGH TEMPERATURE SUPERCONDUCTIVITY”

APPC 2000 ◽  
2001 ◽  
Author(s):  
DANILO M. YANGA ◽  
AUGUSTO A. MORALES
2008 ◽  
Vol 77 (Suppl.C) ◽  
pp. 109-112
Author(s):  
Koichi Kusakabe ◽  
Hiroshi Katayama-Yoshida ◽  
Hidetoshi Kizaki ◽  
Akitaka Nakanishi

1988 ◽  
Vol 02 (05) ◽  
pp. 699-709 ◽  
Author(s):  
Hiroshi Kamimura

In this paper a review is given on the mechanism of high temperature superconductivity recently developed by Kamimura, Matsuno, and Saito. In this mechanism spin-polarons associated with itinerant holes in the e v band (Cu dz 2- Op π band) are created in CuO 2 layers by strong intra-atomic exchange interaction (Hund's coupling) with localized dx 2− y 2 holes. Then the interplay of Hund's coupling and superexchange between Cu 2+( dx 2− y 2) spins gives rise to an attractive exchange interaction between spin-polarons, which leads to the formation of spin-singlet spin-polarons pairs. This contributes to high temperature superconductivity. Further the s-wave pairing reproduces the observed x dependence of T c as well as the right magnitudes of T c in ( La 1−x Sr x )2 CuO 4 satisfactorily.


1988 ◽  
Vol 67 (4) ◽  
pp. 363-367 ◽  
Author(s):  
Hiroshi Kamimura ◽  
Shunichi Matsuno ◽  
Riichiro Saito

1999 ◽  
Vol 10 (01) ◽  
pp. 309-320 ◽  
Author(s):  
INGO MORGENSTERN ◽  
WERNER FETTES ◽  
THOMAS HUSSLEIN ◽  
DENNIS M. NEWNS ◽  
PRATAP C. PATTNAIK

In this paper we revisit the glass model describing the macroscopic behavior of the High-Temperature superconductors. We link the glass model at the microscopic level to the striped phase phenomenon, recently discussed widely. The size of the striped phase domains is consistent with earlier predictions of the glass model when it was introduced for High-Temperature Superconductivity in 1987. In an additional step we use the Hubbard model to describe the microscopic mechanism for d-wave pairing within these finite size stripes. We discuss the implications for superconducting correlations of the Hubbard model, which are much higher for stripes than for squares, for finite size scaling, and for the new view of the glass model picture.


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