首页> 外文期刊>Journal of Physics. Condensed Matter >Mossbauer spectroscopy under a magnetic field to explore the low-temperature spin structure of the layered ferrimagnetic material - {N(n-C4H9)(4)[(FeFeIII)-Fe-II(C2O4)(3)]}(infinity)
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Mossbauer spectroscopy under a magnetic field to explore the low-temperature spin structure of the layered ferrimagnetic material - {N(n-C4H9)(4)[(FeFeIII)-Fe-II(C2O4)(3)]}(infinity)

机译:磁场下的莫斯鲍尔光谱研究层状亚铁磁性材料的低温自旋结构-{N(n-C4H9)(4)[(FeFeIII)-Fe-II(C2O4)(3)]}(无穷大)

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Fe-57 Mossbauer spectroscopy of the metal-assembled layered ferrimagnetic material {N(n-C4H9)(4)[(FeFeIII)-Fe-II(C2O4)(3)]}(infinity) was performed under a high external magnetic field at 4.2 K. This study successfully detected different types of Fe-II and Fe-III high spin sites in the lattices. The hyperfine field values estimated for all the Fe-III high spin sites are close to the expected values, whereas those for Fe-II high spin sites are substantially different to those expected usually. A large fraction of magnetically disordered Fe-III high spin sites were found. It is understood that the layered structure of the compound may have two kinds of sub-lattices-(Fe-A(II)-ox-Fe-A(III)-(...)) and (Fe-B(II)-ox-Fe-B(III)-(...))-along with randomly placed magnetically disordered Fe-C(III) sites, where the, Fe-A(III) and Fe-B(III) are antiferromagnetically aligned. The existence of the magnetically and/or structurally non-equivalent spin sites in the same lattice has been held responsible for the coexistence of different ferrimagnetic interactions leading to the spin glass state, as observed through earlier magnetic and calorimetric measurements. [References: 26]
机译:金属组装层状亚铁磁性材料{N(n-C4H9)(4)[(FeFeIII)-Fe-II(C2O4)(3)]}(无限大)的Fe-57 Mossbauer光谱是在高外部磁场下进行的在4.2 K时。这项研究成功地检测出晶格中不同类型的Fe-II和Fe-III高自旋位点。对所有Fe-III高自旋位点估计的超精细场值都接近预期值,而对Fe-II高自旋位点的估计值与通常预期的值基本上不同。发现大部分磁性无序的Fe-III高自旋位点。可以理解,该化合物的层状结构可以具有两种亚晶格-(Fe-A(II)-ox-Fe-A(III)-(...))和(Fe-B(II) -ox-Fe-B(III)-(...))-以及随机放置的磁性无序Fe-C(III)位点,其中Fe-A(III)和Fe-B(III)反铁磁排列。通过较早的磁性和量热测量可以观察到,相同晶格中磁性和/或结构上不等价的自旋位点的存在是导致亚铁磁性相互作用并导致自旋玻璃态的共存的原因。 [参考:26]

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