2002
DOI: 10.1016/s0921-4534(02)00978-4
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Magnetic and transport measurements on melt-textured DyBCO single domains

Abstract: In this communication we report critical current measurements of melt processed DyBa 2 Cu 3 O 7-x samples determined by several measuring techniques. First the material was characterized by AC susceptibility and DC magnetization. The results are characteristic of good quality melt-processed (RE)BCO material with T c ≈ 89 K and J c (77 K, 1 T) ≈ 10 4 A/cm 2 . Next, pulsed currents were used in order to determine both I-V curves and transport critical currents. The origin of the discrepancy between transport and… Show more

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Cited by 14 publications
(9 citation statements)
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“…It is ∼1 × 10 6 A/cm 2 at zero fields and goes down to ∼3 × 10 5 A/cm 2 at 40,000 Oe. With the increase of temperature to 77 K, the intragrain J cm decreases sharply and takes values about 20–50 times in magnitude less than that of at 10 K. For instance, the intragrain J cm was calculated as ∼4 × 10 4 A/cm 2 at zero fields and 77 K. These values are, respectively, high for a polycrystalline superconductor having similar structure and even at the level of the J c ‐values of melt‐textured High T c cuprates 33–36. Such a high temperature dependence of the intragrain J cm shows that point defects, which act as pinning center at 10 K, are intensively present in the microstructure and they become ineffective at 77 K. Furthermore, the intragrain J cm also seems to be very sensitive to the applied field at 77 K. It is ∼7000 A/cm 2 under magnetic field of 1000 Oe.…”
Section: Resultsmentioning
confidence: 97%
“…It is ∼1 × 10 6 A/cm 2 at zero fields and goes down to ∼3 × 10 5 A/cm 2 at 40,000 Oe. With the increase of temperature to 77 K, the intragrain J cm decreases sharply and takes values about 20–50 times in magnitude less than that of at 10 K. For instance, the intragrain J cm was calculated as ∼4 × 10 4 A/cm 2 at zero fields and 77 K. These values are, respectively, high for a polycrystalline superconductor having similar structure and even at the level of the J c ‐values of melt‐textured High T c cuprates 33–36. Such a high temperature dependence of the intragrain J cm shows that point defects, which act as pinning center at 10 K, are intensively present in the microstructure and they become ineffective at 77 K. Furthermore, the intragrain J cm also seems to be very sensitive to the applied field at 77 K. It is ∼7000 A/cm 2 under magnetic field of 1000 Oe.…”
Section: Resultsmentioning
confidence: 97%
“…Due to these difficulties, a comprehensive dataset of transport J c and n-values for REBCO bulks is yet to be published, with previous works being predominantly focused on the LN2 temperature, self-field case for YBCO [28]- [32]. Other bulks such as DyBCO, (NdEuGd)BCO and GdBCO-Ag have also been investigated, but to a lesser degree [14], [33], [34]. Some critical current angle-dependence has been measured, such as in [28], [29], however the I c data is mostly sparse, unpublished for n-values and over 20 years old, when bulk manufacturing technology was less refined.…”
Section: Introductionmentioning
confidence: 99%
“…This means the determination of the critical current density J C . Different classical methods have been used for small samples [ 1 , 2 , 3 , 4 , 5 , 6 , 7 , 8 , 9 , 10 , 11 , 12 , 13 , 14 , 15 , 16 , 17 , 18 , 19 , 20 , 21 ]. The goal of these classical methods is mainly to obtain the dependence of J C on the magnetic field B and temperature of the HTS material.…”
Section: Introductionmentioning
confidence: 99%