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Superconductivity and magnetic order in RSr2Cu2.7Mo0.3O7−δ (R = Y, Pr, Gd, and Tb)

✍ Scribed by H.L. Tsay; C.R. Shih; Y.C. Chen; W.H. Lee; T.H. Meen; H.D. Yang


Publisher
Elsevier Science
Year
1995
Tongue
English
Weight
581 KB
Volume
252
Category
Article
ISSN
0921-4534

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✦ Synopsis


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. The calculated lattice constants using space group P4/mmm indicate that these rare-earth ions are basically in the 3 + valence state. Samples R = Y, Gd, and Tb are superconducting with transitions at around 30 K, while PrSr2Cu2,7Moo.307_~ remains semiconducting down to 2 K. Effective magnetic moments /xon. derived from a Curie-Weiss-behavior susceptibility for R = Gd and Tb are 7.92 /x B and 9.75 /x B, respectively, which are close to those of trivalent free ions. While the /zef f = 3.05 /z B for R = Pr is smaller than that expected for a Pr 3+ free ion. A magnetic ordering transition is observed by a A-type anomaly in specific-heat measurements at 2.27 K and 5.43 K for R = Gd and Tb, respectively. In contrast, no significant feature was observed in specific heat for PrSr2Cu2.vMo0.307-8 in the temperature range 0.6-40 K. The similarities and differences in superconducting and magnetic properties between RSr2Cuz.7Moo.30 7_ ~ and RBa2Cu307_ 8 are discussed.


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The crystal structure of the Mo-stabilized Sr-based superconductor with nominal composition \(\mathrm{YSr}_{2} \mathrm{Cu}_{2.7} \mathrm{Mo}_{0.3} \mathrm{O}_{7-\delta}\) has been analyzed by X-ray powder diffraction (XRD), electron diffraction, and high-resolution electron microscope techniques. Th