1997
DOI: 10.1002/1521-396x(199712)164:2<805::aid-pssa805>3.0.co;2-n
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Analysis of Magnetic After-Effect Spectra in Titanium-Doped Magnetite

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Cited by 24 publications
(55 citation statements)
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“…Second, there is also considerable variation in the disaccommodation spectra peak temperatures for magnetites from different origins [11,30].…”
Section: Discussionmentioning
confidence: 79%
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“…Second, there is also considerable variation in the disaccommodation spectra peak temperatures for magnetites from different origins [11,30].…”
Section: Discussionmentioning
confidence: 79%
“…First, the different timescales of the measurements are likely to be important as the positions of the peaks in the disaccommodation spectra are known to be time dependent; the peaks shift to lower temperatures as the measurement time increases due to the thermally activated nature of the processes contributing to disaccommodation. For example, for a polycrystalline magnetite sample a disaccommodation peak located at 320 K measured at 2 s, shifted to 290 K on measuring after 180 s [30]. As the viscosity measurements were made over longer timescales, i.e., > 2000 s, it would be expected that the positions of the viscosity peaks would be shifted to even lower temperatures.…”
Section: Discussionmentioning
confidence: 81%
“…At room temperature, electron hopping between Fe 2+ and Fe 3+ ions in the B sites (and possibly also in the A sites) occurs on timescales shorter than the Mössbauer measurement time, and consequently the Fe 2+ and Fe 3+ are blurred together in the Mössbauer spectra, yielding a broadened composite sextet with an average oxidation state of Fe 2.5+ . Measurements at 4.2 K, where electron hopping is suppressed (e.g., Walz et al, ), allow sharper distinction of iron valence states, and the application of a strong field allows clearer resolution of sites by shifting the A‐site and B‐site subspectra in opposite directions. Because of the dominance of the B sublattice moment and negative A‐B exchange interactions, the moments of the B‐site cations align with the applied field and those of the A site in the antiparallel direction, effectively decreasing and increasing the B‐ and A‐site hyperfine fields, respectively (e.g., Daniels & Rosencwaig, ; Hamdeh et al, ; Murad & Cashion, ).…”
Section: Methodsmentioning
confidence: 99%
“…1, 2) from lowest temperatures (T < 4 K), down to a plateau of minute strength, extending between 55 and 75 K, thereby surpassing a Debye-type maximum near 50 K of annealing-depending strength. This behaviour is at variance to that of e À -irradiated stoichiometric magnetite where, immediately after irradiation, the corresponding tunneling zone is found to be strongly suppressed [15]; it ressembles, however, that of magnetite compounds submitted to charge-order perturbations by quenching-in of octahedral vacancies [29 to 31] or doping with ionic impurities like Ti 4 [32,33], Ga 3 [34], Mn 2 [35,36], etc.…”
Section: The Mae Spectrum Of Electron-irradiated Yigmentioning
confidence: 99%