← Back to search

Transport and magnetic properties of the (Eu,Ce)2(Ba,Eu)2Cu3O9−δ-type and T*-type superconductors: Dependence of Tc on the size of the rare-earth ion

S. Ikegawa, T. Wada, T. Yamashita, H. Yamauchi, S. Tanaka

DOI 10.1103/PhysRevB.45.5659 · Physical Review B

T1

Active bibliographic source — not scientific approval

Bibliographic access preserves source history; it does not approve extracted materials or validate reported claims. Review warnings on each occurrence separately.

Abstract

The electrical transport properties and magnetic susceptibility of (L2/3Ce1/3)2(La1/3Ba1/3Sr1/3)2 Cu3O9−δ (2:2:3 phase) where L is a rare-earth element are measured and compared with those of the T* phase (Nd1.4Ce0.2Sr0.4Cu1−xZnxO4−δ and La1.8−xLxSr0.2CuO4−δ) in order to investigate why the superconducting transition temperature (Tc) depends on the ionic radius of the atom L. For 2:2:3 samples with L=Eu, Dy, Y, or Ho, the smaller the size of the L3+ ion, the lower is the value of Tc, while the Hall coefficient (RH) remains at the same level at temperatures above 130 K. This is in contrast to the case of La1.8−xLxSr0.2CuO4−δ with L=Sm, Eu, or Gd, in which the decrease in Tc with decreasing ionic radius of the L atom may be attributed to the reduction in the carrier concentration. The resistivity, RH, and Seebeck coefficient for a nonsuperconducting 2:2:3 sample containing small L3+ ions are all parallel to those of a nonsuperconducting T*-phase sample with Zn doping. Judging from these experimental results, we suggest that a ‘‘disordered potential’’ similar to the case of the Zn-doped T*-phase compound exists in the nonsuperconducting 2:2:3 compound.

Source-reported materials — not catalogue approval

FormulaReported Tc (K)Pressure (GPa)Type
(Eu2/3Ce1/3)2(La1/3Ba1/3Sr1/3)2Cu3O9-δ

Archive — visibility unverified

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

28.5Pressure not reportedonset
(Dy2/3Ce1/3)2(La1/3Ba1/3Sr1/3)2Cu3O9-δ

Archive — visibility unverified

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

7Pressure not reportedonset
Nd1.4Ce0.2Sr0.4CuO4-δ

Archive — visibility unverified

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

23.1Pressure not reportedonset
La0.8SmSr0.2CuO4-δ

Archive — visibility unverified

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

21Pressure not reportedonset
La0.9Eu0.9Sr0.2CuO4-δ

Archive — visibility unverified

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

12Pressure not reportedonset

Similar papers