dc.contributor.author |
Kostogloudis, G |
en |
dc.contributor.author |
Ftikos, C |
en |
dc.date.accessioned |
2014-03-01T01:46:56Z |
|
dc.date.available |
2014-03-01T01:46:56Z |
|
dc.date.issued |
1998 |
en |
dc.identifier.uri |
https://dspace.lib.ntua.gr/xmlui/handle/123456789/25107 |
|
dc.subject |
Crystal Structure |
en |
dc.subject |
Electric Conductivity |
en |
dc.subject |
Electrical Properties |
en |
dc.subject |
High Temperature |
en |
dc.subject |
Lattice Parameter |
en |
dc.subject |
Room Temperature |
en |
dc.subject |
Thermal Expansion |
en |
dc.subject |
Thermal Expansion Coefficient |
en |
dc.subject |
X Ray Powder Diffraction |
en |
dc.subject |
Metal Insulator |
en |
dc.subject |
Phase Transition |
en |
dc.title |
Structural, thermal and electrical properties of Pr 0.5Sr 0.5Co 1− y Ni y O 3− δ perovskite-type oxides |
en |
heal.type |
journalArticle |
en |
heal.identifier.primary |
10.1016/S0167-2738(98)00007-1 |
en |
heal.identifier.secondary |
http://dx.doi.org/10.1016/S0167-2738(98)00007-1 |
en |
heal.publicationDate |
1998 |
en |
heal.abstract |
Perovskite oxides in the system Pr0.5Sr0.5Co1−yNiyO3−δ (0<y<1) were prepared and characterized by X-ray powder diffraction, dilatometry and electrical conductivity measurements. The Pr0.5Sr0.5CoO3−δ end member has an orthorhombic GdFeO3 structure, while when Ni is substituted for Co, a tetragonal phase is formed, the concentration of which increases linearly in the range 0<y<0.6. Above y=0.6 the tetragonal is the only phase present. |
en |
heal.journalName |
Solid State Ionics |
en |
dc.identifier.doi |
10.1016/S0167-2738(98)00007-1 |
en |