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Stability of Pb doped Bi{sub 2}Sr{sub 2}Ca{sub 1}Cu{sub 2}O{sub 8+{delta}} and the growth of Bi{sub 2}Sr{sub 2}Ca{sub 2}Cu{sub 3}O{sub 10+{delta}}

Journal Article · · Applied Physics Letters
DOI:https://doi.org/10.1063/1.113757· OSTI ID:64851
;  [1];  [2];  [3]
  1. Ames Laboratory, USDOE and Department of Physics, Iowa State University, Ames, Iowa 50011 (United States)
  2. Energy Technology Division, Argonne National Laboratory, Argonne Illinois 60439 (United States)
  3. Intermagnetics General Corporation, Latham, New York 12110 (United States)
{ital In} {ital situ} high-temperature x-ray measurements have been used to follow the crystallographic changes that occur as Pb-doped Bi{sub 2}Sr{sub 2}Ca{sub 1}Cu{sub 2}O{sub 8+{delta}} plus other phases transform to Bi{sub 2}Sr{sub 2}Ca{sub 2}Cu{sub 3}O{sub 10+{delta}} in a powder-in-tube process for forming tape conductors. On the initial ramp to the reaction temperature, the Bi{sub 2}Sr{sub 2}Ca{sub 1}Cu{sub 2}O{sub 8+{delta}} x-ray lines first diminish in amplitude, by about a factor of 2 or more, and then begin to grow again above 700 {degree}C. In the 790--795 {degree}C range, a transient new phase is seen. Finally, at temperatures as low as 790 {degree}C, the Bi{sub 2}Sr{sub 2}Ca{sub 2}Cu{sub 3}O{sub 10+{delta}} phase begins to grow as the Pb-doped Bi{sub 2}Sr{sub 2}Ca{sub 1}Cu{sub 2}O{sub 8+{delta}} disappears. Separate studies of a Pb-doped Bi{sub 2}Sr{sub 2}Ca{sub 1}Cu{sub 2}O{sub 8+{delta}} pellet without the Ca{sub 2}Cu{sub 1}O{sub 3} and CuO present show essentially the same peak intensity changes during the temperature ramp to 700 {degree}C. {copyright} {ital 1995} {ital American} {ital Institute} {ital of} {ital Physics}.
Research Organization:
Ames National Laboratory
DOE Contract Number:
W-7405-ENG-82; W-31109-ENG-38
OSTI ID:
64851
Journal Information:
Applied Physics Letters, Journal Name: Applied Physics Letters Journal Issue: 24 Vol. 66; ISSN APPLAB; ISSN 0003-6951
Country of Publication:
United States
Language:
English

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