The electronic structures of soluble Prussian blue, insoluble Prussian blue, and Turnbull's blue were investigated by the Mössbauer effect of 57Fe. The results below their Curie temperatures of 5.5° ± 0.5°K show that all of them are ferric ferrocyanide: one kind of irons is Fe3 + with high spin and the other is Fe(II) with low spin. It is concluded that Prussian blue and Turnbull's blue have the same electronic structure. The results of a paramagnetic resonance absorption observed at room temperature also support the conclusions obtained by the Mössbauer study.
A systematic investigation of the structure and properties of ͓001͔ twist boundaries was made in Bi 2 Sr 2 CaCu 2 O 8ϩ␦ bicrystals. Contrary to conventional wisdom, all these boundaries, regardless of their misorientation angle, carried almost the same critical current as their constituent single crystals at magnetic fields up to 9 t. The origin of this misorientation-independent superconducting behavior at twist boundaries was sought by detailed structural characterization using high-resolution and nanoprobe transmission-electron microscopy. The robust electromagnetic properties of these grain boundaries were mainly attributed to the high anisotropy of the crystals, and to the softness of the double BiO layers at the boundaries which allow the CuO 2 layers adjacent to the boundary plane to remain undisturbed. The structural characteristics of these boundaries are identical to those found in Bi 2 Sr 2 CaCu 2 O 8ϩ␦ and Bi 2 Sr 2 Ca 2 Cu 3 O 10ϩ␦ tapes, suggesting that the large-angle ͓001͔ twist boundaries are not a current-limiting obstacle in this important conductor.
A two-step process is proposed for the formation of c-axis aligned (Bi,Pb)2Sr2Ca2Cu3O10+δ [Bi(2:2:2:3)] platelets in a silver sheath. The process involves: (1) the formation of c-axis aligned (Bi,Pb)2Sr2CaCu2O8+δ at early stage of heat treatment and (2) the subsequent intercalation of Ca–Cu–O layers to form Bi(2:2:2:3). This is based on the measurements of (1) the rocking curves for c-axis alignment and the two theta scans for the Bi(2:2:2:3) conversion ratio, both by a transmission x-ray technique, and (2) a quantitative study of the phase conversion due to intercalation of Ca–Cu–O layers into existing Bi(2:2:1:2) by transmission electron microscopy.
The angular distributions of large-angle grain boundaries were studied by electron microscopy for Bi(2:2:1:2) and Bi(2:2:2:3) composite tapes. For Bi(2:2:2:3) the distributions are random, while for Bi(2:2:1:2), there was a high incidence of special boundary misorientations. The preferred orientations in Bi(2:2:1:2), which were analyzed for [001] and [100] rotations, agreed well with the calculated lattice coincidences based on the constraint Coincidence Site Lattice model, and were attributed to the reorientation of the neighboring grains during its partial melt process.
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