Publication: Structural changes and superconducting properties of Gd <inf>1-2x</inf>Pr<inf>x</inf>Ca<inf>x</inf>Ba<inf>2</inf>Cu<inf>3</inf>O <inf>7-δ</inf> HTSCs
Issued Date
2005-10-01
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09532048
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2-s2.0-25144448573
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Mahidol University
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SCOPUS
Bibliographic Citation
Superconductor Science and Technology. Vol.18, No.10 (2005), 1294-1299
Suggested Citation
N. Udomkan, P. Winotai, R. Suryanarayanan, N. Charoenthai Structural changes and superconducting properties of Gd <inf>1-2x</inf>Pr<inf>x</inf>Ca<inf>x</inf>Ba<inf>2</inf>Cu<inf>3</inf>O <inf>7-δ</inf> HTSCs. Superconductor Science and Technology. Vol.18, No.10 (2005), 1294-1299. doi:10.1088/0953-2048/18/10/008 Retrieved from: https://repository.li.mahidol.ac.th/handle/20.500.14594/16507
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Title
Structural changes and superconducting properties of Gd <inf>1-2x</inf>Pr<inf>x</inf>Ca<inf>x</inf>Ba<inf>2</inf>Cu<inf>3</inf>O <inf>7-δ</inf> HTSCs
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Abstract
We report on structural changes and the properties of Gd 1-2xPrxCaxBa2Cu3O 7-δ (0≤x≤0.3) high temperature superconductors which were prepared and characterized. The transition temperature (Tc) was found to decrease roughly linearly with respect to the Pr and Ca concentration x. 65Cu2+(3d9) and 63Cu 2+(3d9) ions from impurity phase BaCuO2 give rise to X-band electron spin resonant (ESR) two-quartet absorption peaks centred at ∼310 mT (g∼2.020) which are superposed by the broad ESR peak of Gd3+(4f7) at g∼2.000 in the undoped Gd123. Both sets of ESR peaks shift towards low fields as the temperature is lowered, which is due to the change in crystal field experienced by the ions. It should be noted here that even at 77 K there still is no magnetic ordering from Gd3+ ions. However, at x ≤ 0.025 doping, a new six-peak hyperfine multiplet ESR signal arising from 141Pr4+ (4f1,S ≤ 1/2,I ≤ 5/2) appears at ∼323 mT (g∼2.029). Typical simulated ESR parameters of Gd3+ in Gd1-2xPrxCaxBa 2Cu3O7-δ at x ≤ 0.025, are g x ≤ 2.4879, gy ≤ 2.3921 and gz ≤ 2.2590, Axx ≤ 12.50, Ayy ≤ 23.50, Azz ≤ 32.00 G and the zero-field splitting parameter (D) of 66.0 G, respectively. This signal arises from some Pr ions entering the Gd site with a valence of four, thus lending support to the hole-filling and pair-breaking models. © 2005 IOP Publishing Ltd.