Transport critical current densities in bulk Tl sub 2 Ba sub 2 Ca sub 2 Cu sub 2 O sub x and polycrystalline-thin-film Tl sub 2 Ba sub 2 Ca sub 1 Cu sub 2 O sub x; Dependence on microstructure and neutron irradiation damage

This paper reports investigations of the dependence of transport critical current density, J{sub c}, upon magnetic field, B at 4, 64 and 75 K in a bulk ceramic sample of T1{sub 2}Ba{sub 2}Ca{sub 2}Cu{sub 3}O{sub x} and in a polycrystalline, textured thin film of T1{sub 2}Ba{sub 2}CaCu{sub 2}O{sub x}...

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Bibliographic Details
Published inIEEE Transactions on Magnetics (Institute of Electrical and Electronics Engineers); (United States) Vol. 27:2
Main Authors Maley, M.P., Vogt, G.J., Phillips, D.S., Coulter, J.Y., Arendt, P.N., Elliot, N.E.
Format Conference Proceeding
LanguageEnglish
Published United States 01.03.1991
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Summary:This paper reports investigations of the dependence of transport critical current density, J{sub c}, upon magnetic field, B at 4, 64 and 75 K in a bulk ceramic sample of T1{sub 2}Ba{sub 2}Ca{sub 2}Cu{sub 3}O{sub x} and in a polycrystalline, textured thin film of T1{sub 2}Ba{sub 2}CaCu{sub 2}O{sub x}. In ceramic samples of T1-2223 we generally observe the double-step J{sub c} versus B characteristics first pointed out by Ekin, in which J{sub c} drops from its zero field value to a plateau reached at B{approximately}100 Oe. The plateau region then extends to a higher field B* (T) beyond which J{sub c}(B) decreases monotonically. We have achieved plateau J{sub c} (75 K. 1.OT) values {gt}300 A/cm{sup 2} with B* (75 K) {approximately} 1.5 T. In these samples a pronounced peak effect is observed in which J{sub c} (B) increases monotonically with increasing B for 100 {lt} B(O{sub e}) {lt} B*. After neutron irradiation, we observe B* to be significantly enhanced suggesting that B* signals the onset of rapid flux creep.
Bibliography:CONF-900944--
None
ISSN:0018-9464
1941-0069