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Title: Electric, magnetic, and transport critical current density behavior of the 2201, 2212, and 2223 phases of BSCCO (Bi sub 2 O sub 3 -SrO-CaO-CuO)

Journal Article · · Journal of Superconductivity; (USA)
DOI:https://doi.org/10.1007/BF00618525· OSTI ID:5999609
 [1];  [2];  [3]; ;  [4];  [5]
  1. Universita di Salerno (Italy) Istituto di Elettronica dello Stato Solido del C.N.R., Rome (Italy)
  2. INFN, Rome (Italy)
  3. ENEA, Rome (Italy) Istituto di Elettronica dello Stato Solido del C.N.R., Rome (Italy)
  4. Universita di Roma (Italy) Istituto di Elettronica dello Stato Solido del C.N.R., Rome (Italy)
  5. ENEA, Rome (Italy)

The authors have studied the electrical properties of polycrystalline pellets of the high-T{sub c} superconducting phases occurring in the Bi{sub 2}O{sub 3}-SrO-CaO-CuO (BSCCO) system, having nominal compositions Bi{sub 2}Sr{sub 2}Cu{sub 1}O{sub 6+y} (2201 phase, with T{sub c} = 10 K), Bi{sub 2}Sr{sub 2}CaCu{sub 2}O{sub 8+y} (2212 phase, with T{sub c} = 85 K), and Bi{sub 2}Sr{sub 2}Ca{sub 2}Cu{sub 3}O{sub 10+y} (2223 phase, with {Tc} = 110 K). Pellets containing the 2223 phase having zero resistance below 105 K were obtained. For the 2212 and 2223 phases, the transport critical current density was measured as a function of temperature and of the externally applied magnetic field. As previously found for YBa{sub 2}Cu{sub 3}O{sub 7{minus}x} (YBCO), results are consistent with the occurrence of a weak superconducting coupling among the grains. Such coupling was, however, noticeably stronger for the 2223 phase than for the 2212 phase.

OSTI ID:
5999609
Journal Information:
Journal of Superconductivity; (USA), Vol. 2:3; ISSN 0896-1107
Country of Publication:
United States
Language:
English

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