2005
DOI: 10.1088/0953-8984/17/33/003
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Modulated phases in NaNbO3: Raman scattering, synchrotron x-ray diffraction, and dielectric investigations

Abstract: Raman spectra of sodium niobate (NaNbO 3 ) were obtained in all phases and revealed a significant disorder in the high-temperature U, T2 and T1 phases and a complicated folding of the Brillouin zone at the transitions into modulated S, R, P and N phases associated with the competitive zone-boundary soft modes (in-phase and out-of phase octahedral tilts) along the M-T-R line. An extensive Raman study combined with x-ray diffraction (XRD) and dielectric measurements confirmed the presence of the incommensurate (… Show more

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Cited by 108 publications
(77 citation statements)
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“…Extensive Raman studies combined with X-ray diffraction (XRD) and dielectric measurements confirmed the presence of an incommensurate phase in NaNbO 3 in the temperature interval 410-460 K. [2] Low wavenumber Raman studies on NaNbO 3 single crystal revealed the occurrence of a quasi-elastic peak, and the phase transition was attributed to the order-disorder process due to the relaxation response of Nb ion in the temperature interval 513-713 K. [7] Shen et al, [8] on the basis of the temperature variation of phonon modes during cooling and heating cycles of measurement, suggested that both FE and AFE phases coexist in the temperature range 40-180 K during cooling cycle. However, it is not clear from these studies [2,8] how the temperature range of coexistence of both phases was arrived, as no detailed intensity analysis had been done. Temperaturedependent Raman scattering studies in NaNbO 3 by Lima et al [10] suggested that the orientation of NbO 6 group plays an important role in stabilising the low-temperature FE phase.…”
Section: Introductionmentioning
confidence: 93%
“…Extensive Raman studies combined with X-ray diffraction (XRD) and dielectric measurements confirmed the presence of an incommensurate phase in NaNbO 3 in the temperature interval 410-460 K. [2] Low wavenumber Raman studies on NaNbO 3 single crystal revealed the occurrence of a quasi-elastic peak, and the phase transition was attributed to the order-disorder process due to the relaxation response of Nb ion in the temperature interval 513-713 K. [7] Shen et al, [8] on the basis of the temperature variation of phonon modes during cooling and heating cycles of measurement, suggested that both FE and AFE phases coexist in the temperature range 40-180 K during cooling cycle. However, it is not clear from these studies [2,8] how the temperature range of coexistence of both phases was arrived, as no detailed intensity analysis had been done. Temperaturedependent Raman scattering studies in NaNbO 3 by Lima et al [10] suggested that the orientation of NbO 6 group plays an important role in stabilising the low-temperature FE phase.…”
Section: Introductionmentioning
confidence: 93%
“…ere are also reports about a room-temperature phase transition into a FE phase (P2 1 ma) induced by an applied electric field [6,7], by nanoparticle growth [8] or by growth as a strained thin film [9], respectively. A full list of recent experimental data can be found in [2,[10][11][12].…”
Section: Introductionmentioning
confidence: 99%
“…Results demonstrated an increment in the dielectric permittivity of the ISRN Nanomaterials nanocomposites as the volume fraction increased, due to the high dielectric constants of both PTO and NNO, which are about two orders of magnitude higher than that of PVDF matrix [28,29]. Note that 0% volume fraction indicates pure PVDF samples here.…”
Section: Resultsmentioning
confidence: 84%