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首页> 外文期刊>Physical review. B, Condensed Matter And Materials Physics >Magnetism of Mn_2O_3 nanocrystals dispersed in a silica matrix: Size effects and phase transformations
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Magnetism of Mn_2O_3 nanocrystals dispersed in a silica matrix: Size effects and phase transformations

机译:分散在二氧化硅基质中的Mn_2O_3纳米晶体的磁性:尺寸效应和相变

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摘要

Mn_2O_3 nanocrystals have been grown in a silica matrix following the sol-gel route and subsequent calcination at various temperatures in the range 700℃-900℃. These nanocrystals have been studied by x ray and various magnetic methods including electron paramagnetic resonance (EPR). X-ray studies have revealed the presence of single-phase cubic α-Mn_2O_3 nanocrystals, the mean sizes lying in the range 9-18 nm. A large increment in the intensity and asymmetry of the EPR signal in lowering the temperature from room temperature to liquid-nitrogen temperature suggest that Mn_2O_3 nanocrystals become ferromagnetic (FM) at low temperatures. This is in sharp contrast with the observation of antiferromagnetic (AFM) ordering in bulk α-Mn_2O_3 crystals below 90 K. From zero-field-cooled (ZFC) and field-cooled (FC) magnetization and magnetic hysteresis measurements in the temperature range 5-300 K it has been established that α-Mn_2O_3 nanocrystals present in the calcined samples are superparamagnetic above the blocking temperature TB and weakly ferromagnetic below T_B. Small-sized nanocrystals are observed to have larger uncompensated magnetic moments. This is consistent with the postulate that uncompensated spins are present in a greater number on the surface of the antiferromagnetic inner cores of the smaller-sized nanomagnets. ac susceptibility experiments at various audio frequencies in the low-temperature region down to 5 K, have confirmed the presence of magnetic-phase transitions in Mn_2O_3 doped silica samples (calcined at various temperatures) at low temperatures and have also provided evidence that α-Mn_2O_3 nanocrystals grown in the silica matrix are best described as an assembly of randomly frozen nearly noninteracting magnetic particles.
机译:Mn_2O_3纳米晶体已经遵循溶胶-凝胶法并随后在700℃-900℃的不同温度下煅烧在二氧化硅基质中生长。这些纳米晶体已通过X射线和各种磁性方法(包括电子顺磁共振(EPR))进行了研究。 X射线研究表明存在单相立方α-Mn_2O_3纳米晶体,平均粒径在9-18 nm之间。在将温度从室温降低到液氮温度时,EPR信号的强度和不对称性的大幅增加表明Mn_2O_3纳米晶体在低温下变成铁磁(FM)。这与在90 K以下的块状α-Mn_2O_3晶体中反铁磁(AFM)有序观察形成鲜明对比。在温度范围5内,从零场冷(ZFC)和场冷(FC)磁化和磁滞测量-300 K已确定煅烧样品中存在的α-Mn_2O_3纳米晶体在阻断温度TB以上为超顺磁性,在T_B以下为弱铁磁性。观察到小尺寸的纳米晶体具有较大的未补偿磁矩。这与在较小尺寸的纳米磁体的反铁磁内芯的表面上存在大量未补偿自旋的假设相一致。在低至5 K的低温区域中的各种音频频率下进行的磁化率实验已证实,在低温下Mn_2O_3掺杂的二氧化硅样品(在不同温度下煅烧)中存在磁相变,并且还提供了α-Mn_2O_3的证据在二氧化硅基质中生长的纳米晶体最好描述为随机冻结的几乎不相互作用的磁性粒子的集合。

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