Abstract:This study reports the effect of Cr addition on the structural and superconducting properties of Bi 1.8 Sr 2.0 Crx Ca 1.1 Cu 2.1 O y superconductor with x = 0, 0.1, 0.3, 0.5 0.7, and 1 by means of X-ray analysis (XRD), scanning electron microscopy (SEM), energy dispersive spectroscopy (EDS), and resistivity measurements. The samples studied in this work were prepared using the standard solid-state reaction method. Zero resistivity transition temperatures (T c ) are qualitatively estimated from the dc resistivi… Show more
“…Besides, this behavior (firstly increase then decrease in c value) can be explained by the fact that the ionic radius of Nd 2+ (143 pm) is slightly smaller compared to Ba 2+ (149 pm), leading to regular expansion of the cell parameter c with the rise of the Nd concentration in the Y-123 up to the certain content value of x=0.100 and y=0.100 beyond which the c axis length begins to shrink quickly. This is consistent with the fact that the Ho 3+ and Nd 2+ ions can be substituted for the Cu 2+ individuals in the crystal structure after the critical value of x=0.100 and y=0.100, supported by the findings of the EDS measurement [27]. In other words, hole filling plays a dominant role in determining the superconductivity of Ho and Nd substituted Y-123s.…”
This inclusive study reports the effect of the Nd atoms on the mechanical, microstructural, electrical and superconducting characteristics of Y0.9Ho0.1Ba2-yNdyCu3O7-δ superconductors with the aid of standard characterization methods, including X-ray diffraction, scanning electron microscopy, the bulk density, dc resistivity, and transport critical current density. The experimental results such as the degree of granularity, hole localization effect, room temperature resistivity, critical transition temperature, degree of the broadening, thermodynamic fluctuations, crystallinity, crystal plane alignments, crystal structure, grain size, phase purity and lattice parameters, the appearance of flux pinning centers, grain boundary weak-links, surface morphologies elemental compositions and distributions belonging to Y-site Ho and Ba-site Nd substituted Y-123 superconducting samples are discussed in detail for the first time. All the experimental findings show that the microstructural, electrical, mechanical and superconducting properties regularly improve with the increment in the HcN (Ho constant+Nd changeble) until a certain value of y=0.100, beyond which the characteristics tend to retrograde rapidly. This is attributed to the fact that excess penetration of the Nd damages the crucial properties given above.
“…Besides, this behavior (firstly increase then decrease in c value) can be explained by the fact that the ionic radius of Nd 2+ (143 pm) is slightly smaller compared to Ba 2+ (149 pm), leading to regular expansion of the cell parameter c with the rise of the Nd concentration in the Y-123 up to the certain content value of x=0.100 and y=0.100 beyond which the c axis length begins to shrink quickly. This is consistent with the fact that the Ho 3+ and Nd 2+ ions can be substituted for the Cu 2+ individuals in the crystal structure after the critical value of x=0.100 and y=0.100, supported by the findings of the EDS measurement [27]. In other words, hole filling plays a dominant role in determining the superconductivity of Ho and Nd substituted Y-123s.…”
This inclusive study reports the effect of the Nd atoms on the mechanical, microstructural, electrical and superconducting characteristics of Y0.9Ho0.1Ba2-yNdyCu3O7-δ superconductors with the aid of standard characterization methods, including X-ray diffraction, scanning electron microscopy, the bulk density, dc resistivity, and transport critical current density. The experimental results such as the degree of granularity, hole localization effect, room temperature resistivity, critical transition temperature, degree of the broadening, thermodynamic fluctuations, crystallinity, crystal plane alignments, crystal structure, grain size, phase purity and lattice parameters, the appearance of flux pinning centers, grain boundary weak-links, surface morphologies elemental compositions and distributions belonging to Y-site Ho and Ba-site Nd substituted Y-123 superconducting samples are discussed in detail for the first time. All the experimental findings show that the microstructural, electrical, mechanical and superconducting properties regularly improve with the increment in the HcN (Ho constant+Nd changeble) until a certain value of y=0.100, beyond which the characteristics tend to retrograde rapidly. This is attributed to the fact that excess penetration of the Nd damages the crucial properties given above.
“…T c (onset) transition temperatures of the A, B, C, and D samples are found to be about 86.3 K, 81.6 K, 78.7 K, and 75.2 K, respectively (see Table 1). This phenomenon may be dependent on weak links of the superconducting grains, impurity levels and lattice defects of the doped samples [10][11][12][13]. Moreover, roomtemperature resistivity of samples increases with Ni content.…”
In this study the samples were synthesized from a 2234 stoichiometric composition in order to obtain a large amount of pure 2212-BSCCO. The effects of Ni substitution on the properties of Bi-based Bi 2−x Ni x Sr 2 Ca 1 Cu 2 O y superconductor with x = 0, 0.05, 0.1 and 0.2 were investigated by means of X-ray analysis (XRD), DC electrical resistivity and magnetic-hysteresis loop measurements. It has been found that the T c (onset) transition temperature does not change independently of Ni content. In addition, J c values of the samples were calculated from the hysteresis loop measurement by using Bean's model, showing that J c decreases with increasing Ni substitution.
“…Among the high-temperature superconducting materials, the Bi-2212 phase is considered as the most attractive because it has high chemical stability and is relatively easy to synthesize for many technological and industrial applications [1][2][3][4][5][6][7].…”
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