000075643 001__ 75643
000075643 005__ 20231221135828.0
000075643 0247_ $$2doi$$a10.1016/j.ceramint.2015.10.137
000075643 0248_ $$2sideral$$a106215
000075643 037__ $$aART-2016-106215
000075643 041__ $$aeng
000075643 100__ $$aOzcelik, B.
000075643 245__ $$aEffect of Yttrium substitution on superconductivity in Bi-2212 textured rods prepared by a LFZ technique
000075643 260__ $$c2016
000075643 5060_ $$aAccess copy available to the general public$$fUnrestricted
000075643 5203_ $$aIn this study, the physical and superconducting properties of the Bi2Sr2Ca1-xYxCu2O8+delta with x=0.0, 0.05, 0.075 0.1, and 0.20 textured superconducting rods prepared by a laser floating zone technique were presented. The effects of Y3+ substitution for Ca2+ have been investigated by X-ray diffraction (XRD), scanning electron microscopy (SEM), energy dispersive X-ray spectroscopy (EDX), dc-magnetization, magnetic hysteresis and critical current density calculation by using the Bean''s critical state model. The powder XRD patterns of the samples have shown the Bi-2212 phase is the major one. Along with the powder samples, the textured rod surfaces also were investigated by XRD. The grains found to be well-oriented along the longitudinal rod axis which is a typical result for superconductors prepared by laser floating zone (LFZ) method, has been observed. The best critical temperature, T-C, has been found as 92.9 K for the sample with 0.15Y substitution, under DC magnetic field of 50 Oe in ZFC mode. It has also been observed that the critical current density decreases with increasing Y-substitution. Using those values, the maximum J(C) value has been determined as 2.37 x 10(5) A/cm(2) for the undoped sample.
000075643 536__ $$9info:eu-repo/grantAgreement/ES/DGA/T12$$9info:eu-repo/grantAgreement/ES/MINECO/MAT2013-46505-C3-1-R
000075643 540__ $$9info:eu-repo/semantics/openAccess$$aby-nc-nd$$uhttp://creativecommons.org/licenses/by-nc-nd/3.0/es/
000075643 590__ $$a2.986$$b2016
000075643 591__ $$aMATERIALS SCIENCE, CHARACTERIZATION & TESTING$$b2 / 26 = 0.077$$c2016$$dQ1$$eT1
000075643 591__ $$aMATERIALS SCIENCE, CERAMICS$$b2 / 26 = 0.077$$c2016$$dQ1$$eT1
000075643 592__ $$a0.843$$b2016
000075643 593__ $$aElectronic, Optical and Magnetic Materials$$c2016$$dQ1
000075643 593__ $$aCeramics and Composites$$c2016$$dQ1
000075643 593__ $$aSurfaces, Coatings and Films$$c2016$$dQ1
000075643 593__ $$aProcess Chemistry and Technology$$c2016$$dQ1
000075643 593__ $$aMaterials Chemistry$$c2016$$dQ1
000075643 655_4 $$ainfo:eu-repo/semantics/article$$vinfo:eu-repo/semantics/acceptedVersion
000075643 700__ $$aNane, O.
000075643 700__ $$0(orcid)0000-0001-7056-0546$$aSotelo, A.$$uUniversidad de Zaragoza
000075643 700__ $$0(orcid)0000-0002-0794-3998$$aMadre, M.A.$$uUniversidad de Zaragoza
000075643 7102_ $$15001$$2065$$aUniversidad de Zaragoza$$bDpto. Ciencia Tecnol.Mater.Fl.$$cÁrea Cienc.Mater. Ingen.Metal.
000075643 773__ $$g42, 2-B (2016), 3418-3423$$pCeram. int.$$tCeramics International$$x0272-8842
000075643 8564_ $$s465435$$uhttps://zaguan.unizar.es/record/75643/files/texto_completo.pdf$$yPostprint
000075643 8564_ $$s68215$$uhttps://zaguan.unizar.es/record/75643/files/texto_completo.jpg?subformat=icon$$xicon$$yPostprint
000075643 909CO $$ooai:zaguan.unizar.es:75643$$particulos$$pdriver
000075643 951__ $$a2023-12-21-13:41:27
000075643 980__ $$aARTICLE