Cubic-tetragonal-orthorhombic-rhombohedral ferroelectric transitions in perovskite potassium niobate
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Cubic-tetragonal-orthorhombic-rhombohedral ferroelectric transitions in perovskite potassium niobate
Cubic-tetragonal-orthorhombic-rhombohedral ferroelectric transitions in perovskite potassium niobate :
neutron powder profile refinement of the structures
Abstract. The orthorhombic and rhombohedral structures of ferroelectric potassium niobate have been determined by neutron diffraction measurements on powdered crystals, using the profile refinement technique to analyse the data. In the orthorhombic phase at 22 "C the atomic
displacements along [Oll] from the cubic perovskite positions are 6(K) = -0.006 + SA, 6(Nb) = 0,070A, S(0,) = -0.138 + 6A and 6(0,,) 6(0,,,) = -0,125 + 4A. In the rhombohedral phase at 230K, the displacements are along [lll]; 6(K) = -0,013 i 32A, 6(Nb) = 0.078A and 6(0,) = 6(0,,) = S(O,,,) = -0,140 + 4A. As a check on the profile technique, the tetragonal structure was redetermined, and good agreement obtained with the previous single-crystal work, with displacements along [OOl] of S(K) = -0,014 + 26A, 6(Nb) = 0.063A, S(0,) = -0.117 + 4A and 6(0,,) = 6(0,,,) = 0099 + 3A. All of these transitions result from the condensation at q = 0 of soft modes in which almost rigid oxygen octahedra vibrate against the potassium and niobium atoms. Our results account for the observed changes in the spontaneous polarization of potassium niobate, and demonstrate the power of the profile refinement technique for the investigation of structural phase transitions.
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neutron powder profile refinement of the structures
Abstract. The orthorhombic and rhombohedral structures of ferroelectric potassium niobate have been determined by neutron diffraction measurements on powdered crystals, using the profile refinement technique to analyse the data. In the orthorhombic phase at 22 "C the atomic
displacements along [Oll] from the cubic perovskite positions are 6(K) = -0.006 + SA, 6(Nb) = 0,070A, S(0,) = -0.138 + 6A and 6(0,,) 6(0,,,) = -0,125 + 4A. In the rhombohedral phase at 230K, the displacements are along [lll]; 6(K) = -0,013 i 32A, 6(Nb) = 0.078A and 6(0,) = 6(0,,) = S(O,,,) = -0,140 + 4A. As a check on the profile technique, the tetragonal structure was redetermined, and good agreement obtained with the previous single-crystal work, with displacements along [OOl] of S(K) = -0,014 + 26A, 6(Nb) = 0.063A, S(0,) = -0.117 + 4A and 6(0,,) = 6(0,,,) = 0099 + 3A. All of these transitions result from the condensation at q = 0 of soft modes in which almost rigid oxygen octahedra vibrate against the potassium and niobium atoms. Our results account for the observed changes in the spontaneous polarization of potassium niobate, and demonstrate the power of the profile refinement technique for the investigation of structural phase transitions.
To download the article clik on the link below ;
[You must be registered and logged in to see this link.]
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