References(45)
[1]
Muralidhar M, Jirsa M, Sakai N, et al. Current progress in ternary LREBa2Cu3Oy materials and their application. Mat Sci Eng B 2008, 151: 90–94.
[2]
Sakai N, Lee S, Chikumoto N, et al. Delamination behavior of Gd123 coated conductor fabricated by PLD. Physica C 2011, 471: 1075–1079.
[3]
Xu C, Hu A, Ichihara M, et al. Enhanced flux pinning of air-processed Gd123 by doping ZrO2 nanoparticles. Physica C 2007, 460–462: 1341–1342.
[4]
Xu C, Hu A, Sakai N, et al. Flux pinning properties and superconductivity of Gd-123 superconductor with addition of nanosized SnO2/ZrO2 particles. Physica C 2006, 445–448: 357–360.
[5]
Xu Y, Hu A, Xu C, et al. Effect of ZrO2 and ZnO nanoparticles inclusions on superconductive properties of the melt-processed GdBa2Cu3O7−δ bulk superconductor. Physica C 2008, 468: 1363–1365.
[6]
Zhang YF, Izumi M, Li YJ, et al. Enhanced JC in air-processed GdBa2Cu3O7−δ superconductor bulk grown by the additions of nano-particles. Physica C 2011, 471: 840–842.
[7]
Abou Aly AI, Mohammed NH, Awad R, et al. Determination of superconducting parameters of GdBa2Cu3O7−δ added with nanosized ferrite CoFe2O4 from excess conductivity analysis. J Supercond Nov Magn 2012, 25: 2281–2290.
[8]
Xu Y, Izumi M, Zhang YF, et al. Enhancement of critical current density in Gd123 bulk superconductor doped with magnetic powder. Physica C 2009, 469: 1215–1217.
[9]
Zhang YF, Izumi M, Xu Y, et al. Enhanced performance in bulk superconductor GdBa2Cu3O7-δ with additions of α-Fe2O3 particles. J Phys: Conf Ser 2010, 234: 012052.
[10]
Awad R, Abou-Aly AI, Ibrahim IH, et al. Superconducting properties of zinc substitution in Tl-2223 phase. J Alloys Compd 2008, 460: 500–506.
[11]
Çelebi S. Comparative AC susceptibility analysis on Bi–(Pb)–Sr–Ca–Cu–O high-Tc superconductors. Physica C 1999, 316: 251–256.
[12]
Lee CY, Kao YH. Low-field magnetic susceptibility studies of high-Tc superconductors. Physica C 1995, 241: 167–180.
[13]
Yamada N, Akune T, Sakamoto N, et al. Temperature dependence of irreversibility fields in Re doped Hg-1223 superconductors. Physica C 2004, 412–414: 425–429.
[14]
Wimbush SC, Yu R, Bali R, et al. Addition of ferromagnetic CoFe2O4 to YBCO thin films for enhanced flux pinning. Physica C 2010, 470: S223–S224.
[15]
Mumtaz M, Naeem S, Nadeem K, et al. Study of nano-sized (ZnFe2O4)y particles/CuTl-1223 superconductor composites. Solid State Sci 2013, 22: 21–26.
[16]
Awad R, Abou Aly AI, Mohammed NH. Physical and mechanical properties of GdBa2Cu3O7−δ added with nanosized CoFe2O4. J Supercond Nov Magn 2014, 27: 1757–1767.
[17]
Abou Aly AI, Mohammed NH, Awad R, et al. Magneto-conductivity analysis for GdBa2Cu3O7−δ added with nanosized ferrite CoFe2O4. J Supercond Nov Magn 2013, 26: 2419–2428.
[18]
Roumié M, Nsouli B, Zahraman K, et al. First accelerator based ion beam analysis facility in Lebanon: Development and applications. Nucl Instr Meth B 2004, 219–220: 389–393.
[19]
Harrison JF, Eldred RA. Adv X-ray Anal 1973, 17: 560–569.
[20]
Nejedly Z, Campbell JL, Gama S. An Excel utility for the rapid characterization of “funny filters” in PIXE analysis. Nucl Instr Meth B 2004, 219–220: 136–139.
[21]
Maxwell JA, Teesdale WJ, Campbell JL. The Guelph PIXE software package II. Nucl Instr Meth B 1995, 95: 407–421.
[22]
Namuco SB, Lao ML, Sarmago RV. Granular responses of GdBa2Cu3O7-δ using ac magnetic susceptibility measurement under ac and dc magnetic fields. Physics Procedia 2013, 45: 169–172.
[23]
Awad R, Abou-Aly AI, Mahmoud SA, et al. Normal-state conduction mechanisms in GdBa2Cu3−xRuxO7−δ superconducting phase. J Supercond Nov Magn 2011, 24: 2227.
[24]
Mohanta A, Behera D. Effect of granularity and inhomogeneity in excess conductivity of YBa2Cu3O7−δ+ xBaTiO3 superconductor. Physica B 2011, 406: 877–884.
[25]
Amira A, Bouaicha F, Boussouf N, et al. Substitution of Sr2+ by Eu3+ in Bi-2201 ceramics, effects on structure and physical properties. Solid State Sci 2010, 12: 699–705.
[26]
Sedky A, Youssif MI. Correlation between superconducting volume fraction and critical current density in copper oxide superconducting systems. Physica C 2004, 403: 297–303.
[27]
Wang XL, Horvat J, Gu GD, et al. Enhanced flux pinning by Fe point defects in Bi2Sr2Ca(Cu1−xFex)2O8+δ single crystals. Physica C 2000, 337: 221–224.
[28]
Xu Y, Izumi M, Tsuzuki K, et al. Flux pinning properties in a GdBa2Cu3O7−δ bulk superconductor with the addition of magnetic alloy particles. Supercond Sci Technol 2009, 22: 095009
[29]
Bahgat AA, Shaisha EE, Saber MM. Study of microstructure and magnetic properties in copper oxide superconducting systems through AC magnetic susceptibility. Physica B 2007, 399: 70–76.
[30]
Ilonca G, Pop AV, Yang T-R, et al. Transport properties and ac susceptibility of (Bi1.6Pb0.4)Sr2Ca2Cu1−xCox)3Oy superconductors. Int J Inorg Mater 2001, 3: 763–767.
[31]
Huth M, Schmitt M, Adrain H. Influence of composition and long term annealing on the weak link behaviour of the high-Tc superconductor (Bi,Pb)2+xSr2−yCa2+yCu3+zO10+δ. Physica C1991, 178: 203–212.
[32]
Müller K-H, MacFarlane JC, Driver R. Josephson vortices and flux penetration in high temperature superconductors. Physica C 1989, 158: 69–75.
[33]
Gömöry F. Characterization of high-temperature superconductors by AC susceptibility measurements. Supercond Sci Technol 1997, 10: 523
[34]
Sedky A, Youssif MI, Khalil SM, et al. On the correlation between order parameter, superconducting volume fraction and critical current density in R:123 superconductors. Solid State Commun 2006, 139: 126–131.
[35]
Salamati H, Kameli P. Effect of deoxygenation on the weak-link behavior of YBa2Cu3O7−δ superconductors. Solid State Commun 2003, 125: 407–411.
[36]
Bean CP. Magnetization of high-field superconductors. Rev Mod Phys 1964, 36: 31
[37]
Sedky A, Youssif MI. Low-field AC susceptibility study of critical current density in Eu:123 and Bi:2223 superconductors. J Magn Magn Mater 2001, 237: 22–26.
[38]
Murphy SD, Renouard K, Crittenden R, et al. AC susceptibility of sintered high Tc superconductors—Bean’s model and shielding current. Solid State Commun 1989, 69: 367–371.
[39]
Lee MW, Tai MF, Luo SC, et al. Critical current densities in K3C60/Rb3C60 powders determined from AC/DC susceptibility measurements. Physica C 1995, 245: 6–11
[40]
De Gennes PG. Boundary effects in superconductors. Rev Mod Phys 1964, 36: 225.
[41]
Ambegaokar V, Baratoff A. Tunneling between superconductors. Phys Rev Lett 1963, 10: 486
[42]
Farbod M, Batvandi MR. Doping effect of Ag nanoparticles on critical current of YBa2Cu3O7−δ bulk superconductor. Physica C 2011, 471: 112–117.
[43]
Clem JR. Granular and superconducting-glass properties of the high-temperature superconductors. Physica C 1988, 153: 50–55.
[44]
Müller K-H. AC susceptibility of high temperature superconductors in a critical state model. Physica C 1989, 159: 717–726.
[45]
Cho JH. Linear and nonlinear susceptibilities of a Bi2Sr2CaCu2O8 single crystal with isotropic columnar defects. Physica C 2001, 361: 99–106.