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Underdoped, optimally doped, and overdoped superconductors TlSr2(R1−xCax)Cu2O7−δ (R=Lu or Tl)

Y. Shimakawa, J. D. Jorgensen, H. Shaked, R. L. Hitterman, T. Kondo, T. Manako, Y. Kubo

DOI 10.1103/PhysRevB.51.568 · Physical Review B

T1

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Abstract

The crystal structures of underdoped, optimally doped, and overdoped TlSr2(R1−xCax)Cu2O7−δ (R=Lu or Tl) are refined from neutron powder-diffraction data. Carrier concentrations in this system are estimated from simple ionic consideration using the refined occupation numbers. The plot of Tc vs carrier concentration shows the characteristic bell-shaped dependence. The in-plane bond length Cu-O(1) is affected by only the change of carrier concentration and provides a measurement of the doping level, while the apical bond length Cu-O(2) is affected by both the change of carrier concentration and the amount of cation substitution. If we take the effect of cation substitution into account, these bond lengths change ‘‘linearly’’ with carrier concentration over the entire range from the underdoped, through the optimally doped, to the overdoped region.

Source-reported materials — not catalogue approval

FormulaReported Tc (K)Pressure (GPa)Type
TlSr2(Lu0.8Ca0.2)Cu2O7-δ

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—Pressure unresolvedonset
TlSr2(Lu0.6Ca0.4)Cu2O7-δ

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90Pressure unresolvedonset
TlSr2(Tl0.15Ca0.85)Cu2O7-δ

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Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

—Pressure unresolvedonset
YBa2Cu3O7-δ

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Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

90Pressure not reportedunknown
Tl2Ba2CuO6+δ

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Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

85Pressure not reportedunknown
La2-xSrxCuO4

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40Pressure not reportedunknown

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