1987
DOI: 10.1103/physrevlett.58.1891
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Superconductivity above 90 K in the square-planar compound systemABa2Cu3

Abstract: We have found superconductivity in the 90-K range in ^Ba2Cu306+x with A = La, Nd, Sm, Eu, Gd, Ho, Er, and Lu in addition to Y. The results suggest that the unique square-planar Cu atoms, each surrounded by four or six oxygen atoms, are crucial to the superconductivity of oxides in general. In particular, the high T c of /!Ba2Cu3C>6+x is attributed mainly to the quasi two-dimensional assembly of the Cu02-Ba-CuC>2+x-Ba-Cu02 layers sandwiched between two A layers, with particular emphasis in the Cu02+* layers. Hi… Show more

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Cited by 907 publications
(91 citation statements)
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“…The origin of this striking difference to the large pressure coefficient of LBCO was attributed to the presence of the large chemical pressure associated with the smaller Y 3+ ions. The superconducting phase in the YBCO system was later identified as the tetragonal YBa 2 Cu 3 O 6+δ and it was shown that a homologous series of isostructural compounds can be derived by replacing Y with different rare earth ions, such as La, Nd, Sm, Eu, Gd, Ho, Er, and Lu, with superconducting T c 's all above 90 K [49]. These results are particularly interesting because they prove that not the size of the A-ion in the structure of A-Ba 2 Cu 3 O 6+δ determines the high T c but it is the layered structure with CuO 2 -Ba-CuO 2+δ -Ba-CuO 2 slabs separated by the A-ions and stacked along the c-axis that gives rise to the large T c values.…”
Section: The Increase Of T C To New Records Under Imposed Pressurementioning
confidence: 99%
“…The origin of this striking difference to the large pressure coefficient of LBCO was attributed to the presence of the large chemical pressure associated with the smaller Y 3+ ions. The superconducting phase in the YBCO system was later identified as the tetragonal YBa 2 Cu 3 O 6+δ and it was shown that a homologous series of isostructural compounds can be derived by replacing Y with different rare earth ions, such as La, Nd, Sm, Eu, Gd, Ho, Er, and Lu, with superconducting T c 's all above 90 K [49]. These results are particularly interesting because they prove that not the size of the A-ion in the structure of A-Ba 2 Cu 3 O 6+δ determines the high T c but it is the layered structure with CuO 2 -Ba-CuO 2+δ -Ba-CuO 2 slabs separated by the A-ions and stacked along the c-axis that gives rise to the large T c values.…”
Section: The Increase Of T C To New Records Under Imposed Pressurementioning
confidence: 99%
“…͑In the case of TbBa 2 Cu 3 O 7Ϫy and CeBa 2 Cu 3 O 7Ϫy the orthorhombic 1-2-3 structure could not be synthesized.͒ For YBa 2 Cu 3 O 7Ϫy it has been suggested that the block layers act as a charge reservoir and that due to their interaction with adjacent CuO 2 planes they are able to supply holes for the planes when the CuO 3 chains are formed. Since almost all isostructural members of the rare-earth-based 1-2-3 family result in a high-temperature superconductor with transition temperature near 93 K, [3][4][5] it was assumed that the rare-earth atoms serve merely as counterions stabilizing the structure without significantly affecting the superconducting properties. Among those rare-earth-based cuprates that are isostructural to YBa 2 Cu 3 O 7Ϫy , the PrBa 2 Cu 3 O 7Ϫy compound is a puzzling exception since it shows neither metallic nor superconducting behavior.…”
Section: Introductionmentioning
confidence: 99%
“…According to Aliabadi et al [6], to have improvement in T c , one should pump more holes from the chains to the oxygen sites of the planes. Fisk et al [7] and Horet et al [8] have shown that in YBCO system superconductors, substitution at the rare earth site or alkaline-earth site would not change T c considerably. But substitution at the oxygen site is very crucial in the formation of superconductors.…”
Section: Introductionmentioning
confidence: 99%