6 research outputs found

    Evolution of the fishtail-effect in pure and Ag-doped MG-YBCO

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    We report on magnetic measurements carried out in a textured YBa2_2Cu3_3O7δ_{7-\delta} and YBa2_2(Cu1x_{1-x}Agx_x)3_3O7δ_{7-\delta} (at xx \approx 0.02) crystals. The so-called fishtail-effect (FE) or second magnetization peak has been observed in a wide temperature range 0.4~<T/Tc<<T/T_c<~0.8 for Hc\textbf{H}\parallel c. The origin of the FE arises for the competition between surface barrier and bulk pinning. This is confirmed in a non-monotonically behavior of the relaxation rate RR. The value HmaxH_{max} for Ag-doped crystals is larger than for the pure one due to the presence of additional pinning centers, above all on silver atoms.Comment: 6 pages, 6 figure

    Growth Rate of YBa2Cu3O7YBa_2Cu_3O_7 Bulk Crystals in Y1.5Ba2Cu3Y_{1.5}Ba_2Cu_3 System with CeO2CeO_2 Addition

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    The growth rate of Y1Ba2Cu3OxY_1Ba_2Cu_3O_{x} bulk single grain (in fact single crystal) superconductors in the system with composition Y1.5Ba2Cu3OxY_{1.5}Ba_2Cu_3O_{x} and CeO2CeO_2 addition was studied in the temperature range 991-1001°C. It is shown that the growth rate of bulk crystal is different for a- and c-growth direction. Slower measured growth rate in studied system than in pure Y1Ba2Cu3OxY_1Ba_2Cu_3O_{x} is related to the composition shift to the three-phase field containing CuO

    Critical Current Density and Microstructure of NdBa2Cu3O7NdBa_2Cu_3O_7 Single Crystal

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    The top-seeded solution growth method was used to grow NdBCOss single crystals in air. The microstructure of the samples has shown that the oxygenation crack structure developed in the single crystals. The intrinsic critical current density was estimated to be at least twice higher than the value of volume critical current density determined from the magnetization measurements

    Time Dependent Changes in Ag Doped YBCO Superconductors

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    Magnetization measurements at 77 K were conducted on the single-crystalline samples of YBCO superconductor doped with Ag prepared by the top-seeded melt-growth process. The single-grain samples had a nominal composition Y1.5Ba2(Cu,Ag)3OyY_{1.5}Ba_2(Cu,Ag)_3O_{y}. Magnetization measurements on the samples, oxygenated by two different processes: by standard oxygenation and by high pressure oxygenation, repeated after 24 months, revealed time dependent changes in magnetization behaviour and critical transition temperatures, T_{c}, which could be associated with redistribution of oxygen vacancies and their interaction with Ag dopant atoms
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