Polycrystalline samples RSr2Cu2.7Mo0.307 \_ 8 with R = Y, Pr, Gd, and Tb were synthesized and studied by means of powder X-ray diffraction, electrical resistivity, magnetic susceptibility, and specific-heat measurements. All four samples form a perovskite-layer structure with a tetragonal symmetry.
Superconductivity and valence states of Ce, Pr and Tb in bulk Lu1−xMxBa2Cu3O7−δ (M = Ce, Pr and Tb) systems
✍ Scribed by K.I. Gnanasekar; A.S. Tamhane; R. Pinto; R. Nagarajan; M. Sharon; L.C. Gupta; R. Vijayaraghavan
- Publisher
- Elsevier Science
- Year
- 1994
- Tongue
- English
- Weight
- 614 KB
- Volume
- 219
- Category
- Article
- ISSN
- 0921-4534
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✦ Synopsis
Bulk samples of composition Lut_xMxBa2Cu3OT_s (M=Ce, Pr and Tb) are examined with respect to the formation of 1-2-3 phase and the superconducting properties. Samples with M=Pr and Tb form a superconducting 1-2-3 phase for values of x<0.6. We observe that in case of M-: Tb, the zero-resistance transition temperature, Tc¢0), is 85-86 K and independent ofx for 0.1 < x < 0.3. For M=Pr, a maximum Tcco) of 86 K is observed for x=0.1. Tc¢o) decreases with increasing x for x>0.1 and the sample with x=0.6 is observed to be semiconducting down to 12 IC With M=Ce, samples of the composition Lu~_x_yCexCa~Ba2Cu3OT_8 form the superconducting 1-2-3 phase for x, y=0.1 and 0.15. Samples of the compositions Lul_x_~Pr~?,avBa2Cu3OT_8 with x=0.1, 0.2, 0.3 and y--0.1, have lower Tc¢o)'S than samples of a corresponding Pr content without Ca. We infer from our studies that the Pr ions are in the 3+ valence state for 0.1 <x<0.3, the Tb ions are mainly in the 3+ valence state for 0.1 <x<0.3, and the Ce ions are in the 4 + state.
📜 SIMILAR VOLUMES
Pb2Sr2Ceo.sCao.sCu30 s and Pb2Sr2Lnl\_xCaxCu308 with Ln =Pr, Tb and x= 0.0 and 0.5 have been studied by rare-earth L ILm edge XANES spectroscopy. The spectra of Pb 2 Sr2Ceo.sCao.sCu 308 show that Ca doping of Pb 2 Sr2CeCu 308 causes a partial oxidation of Ce. Analysis within the framework of the And