2013
DOI: 10.1103/physrevb.88.064404
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57Fe NMR study of the magnetoelectric hexaferrite Ba0.5Sr1.5Zn

Abstract: Magnetoelectric hexaferrite Ba 0.5 Sr 1.5 Zn 2 Fe 12 O 22 (BSZFO) and Ba 0.5 Sr 1.5 Zn 2 (Fe 0.92 Al 0.08 ) 12 O 22 (BSZFAO) were investigated by 57 Fe nuclear magnetic resonance (NMR). The spin-canting angles of all NMR peaks were measured to assign each peak to corresponding Fe 3+ sites. It was revealed that the spin-canting angle of Fe 3+ ions at off-centered octahedra is fixed and Al 3+ ions substitute for Fe 3+ ions at those sites. The temperature dependence of the NMR frequency indicates that the low-tem… Show more

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Cited by 7 publications
(4 citation statements)
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“…Then the data were taken during warming. The frequency of H 1 was 69 MHz, the frequency of the peak from tetrahedral and octahedral sites [14]. The shape and the frequency of the spectra are almost identical before and after annealing (figure 2(a)).…”
Section: Methodsmentioning
confidence: 86%
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“…Then the data were taken during warming. The frequency of H 1 was 69 MHz, the frequency of the peak from tetrahedral and octahedral sites [14]. The shape and the frequency of the spectra are almost identical before and after annealing (figure 2(a)).…”
Section: Methodsmentioning
confidence: 86%
“…This conclusion, along with the fact that the slope of 1/T 2 changes around the CTC-ALC transition temperature, implies that the magnetic moments of the L and S blocks start to fluctuate as the temperature increases from zero, and that this increase becomes faster over 60 K. That is, the transition from CTC to ALC is gradual, not abrupt. Since the temperature dependence of the NMR frequency does not show any anomaly around 60 K [14], the fluctuation rate cannot be larger than the frequency at the point where the NMR spectrum was observed, at about 70 MHz.…”
Section: Thermal Spin Fluctuationmentioning
confidence: 94%
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