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Structural, transport and spectroscopic properties of Ti~(4+) substituted magnetite: Fe_(3-x)Ti_xO_4

机译:Ti〜(4+)取代磁铁矿Fe_(3-x)Ti_xO_4的结构,输运和光谱性质

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The effect of Ti~(4+) ion on the formation of magnetite, which were prepared by solid-state route reaction method, were studied by resistivity, Raman and ~(57)Fe Moessbauer spectrometry. Resistivity measured in the range of 10<T<300K for Ti~(4+) magnetite Fe_(3-x)Ti_xO_4 exhibit first order phase transformations at the Verwey transition T_v for Fe_3O_4, Fe_(2.98)Ti_(0.02)O_4 and Fe_(2.97)Ti_(0.03)O_4 at 123 K, 121 K and 118K, respectively. No first order phase transition was observed for Fe_(2.9)Ti_(0.1)O_4 and small polaron model retraces the semiconducting resistivity behavior with activation energy of about 72 meV. The changes in Raman spectra as a function of doping show that the changes are gradual for samples with higher Ti doping. The Raman active mode for Fe_(2.9)Ti_(0.1)O_4 at ≌ 634.4 cm~(-1) is shifted as compared to parent Fe_3O_4 at =670 cm~(-1), inferring that Mn~(2+) ions are located mostly on the octahedral sites. ~(57)Fe Mossbauer spectroscopy probes the site preference of the substitutions and their effect on the hyperfine magnetic fields confirms that Ti~(4+) ions are located mostly on the octahedral sites of the Fe_(3-x)Ti_xO_4 spinel structure.
机译:通过电阻率,拉曼光谱和〜(57)Fe Moessbauer光谱研究了通过固态途径反应方法制备的Ti〜(4+)离子对磁铁矿形成的影响。 Ti〜(4+)磁铁矿Fe_(3-x)Ti_xO_4的电阻率在10 <T <300K范围内,在Fe_3O_4,Fe_(2.98)Ti_(0.02)O_4和Fe_的Verwey转变T_v处表现出一阶相变。 (2.97)Ti_(0.03)O_4分别为123 K,121 K和118K。 Fe_(2.9)Ti_(0.1)O_4未观察到一阶相变,小极化子模型以约72 meV的活化能回溯了半导体的电阻率行为。拉曼光谱作为掺杂的函数的变化表明,对于具有较高Ti掺杂的样品,该变化是逐渐的。 Fe_(2.9)Ti_(0.1)O_4在4.4 634.4 cm〜(-1)处的拉曼活性模式与母Fe_3O_4在= 670 cm〜(-1)处发生位移,从而推断Mn〜(2+)离子为主要位于八面体位置。 〜(57)Fe Mossbauer光谱仪探测了取代的位点偏爱,并且它们对超精细磁场的影响证实Ti〜(4+)离子主要位于Fe_(3-x)Ti_xO_4尖晶石结构的八面体位点上。

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