Stanisław Baran, Aleksandra Deptuch, Andreas Hoser, Bogusław Penc, Janusz Przewoźnik, Andrzej Szytuła
{"title":"R2Ni2In化合物(R=Tb和Ho)的晶体和磁性结构。","authors":"Stanisław Baran, Aleksandra Deptuch, Andreas Hoser, Bogusław Penc, Janusz Przewoźnik, Andrzej Szytuła","doi":"10.1107/S2052520623006315","DOIUrl":null,"url":null,"abstract":"<p><p>Crystal and magnetic structures of R<sub>2</sub>Ni<sub>2</sub>In (R = Tb and Ho) have been studied using powder neutron diffraction at low temperatures. The compounds crystallize as orthorhombic crystal structures of the Mn<sub>2</sub>AlB<sub>2</sub> type. At low temperatures, the magnetic moments localized solely on the rare earth atoms form antiferromagnetic structures. The Tb magnetic moments, equal to 8.8 (4) μ<sub>B</sub> and parallel to the c axis, form a collinear magnetic structure described by the propagation vector k = [½ , ½ , ½]. This magnetic structure is stable up to the Néel temperature T<sub>N</sub> = 40 K. For Ho<sub>2</sub>Ni<sub>2</sub>In a complex, temperature-dependent magnetic structure is detected. In the temperature range 6.1-8.6 K, an incommensurate sinusoidal magnetic structure, described by the propagation vector k<sub>1</sub> = [0.24, 1, 0.52] is observed, while in the temperature interval 2.2-2.5 K a square-modulated magnetic structure, related to k<sub>2</sub> = [0.17,{{5} \\over {6}},{{1} \\over {2}}] (the component along the a axis slightly differs from the commensurate value) and its third harmonics 3k<sub>2</sub> = [0.50,{{5} \\over {2}},{{3} \\over {2}}] is found. At 3.1-3.7 K as well as below 2 K, a coexistence of both detected magnetic structures is observed. The Ho magnetic moments remain parallel to the c axis in both the sine- and square-modulated magnetic structures. The low-temperature heat capacity data confirm a first-order transition near 3 K.</p>","PeriodicalId":7320,"journal":{"name":"Acta crystallographica Section B, Structural science, crystal engineering and materials","volume":null,"pages":null},"PeriodicalIF":1.3000,"publicationDate":"2023-10-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Crystal and magnetic structures of R<sub>2</sub>Ni<sub>2</sub>In compounds (R = Tb and Ho).\",\"authors\":\"Stanisław Baran, Aleksandra Deptuch, Andreas Hoser, Bogusław Penc, Janusz Przewoźnik, Andrzej Szytuła\",\"doi\":\"10.1107/S2052520623006315\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p><p>Crystal and magnetic structures of R<sub>2</sub>Ni<sub>2</sub>In (R = Tb and Ho) have been studied using powder neutron diffraction at low temperatures. The compounds crystallize as orthorhombic crystal structures of the Mn<sub>2</sub>AlB<sub>2</sub> type. At low temperatures, the magnetic moments localized solely on the rare earth atoms form antiferromagnetic structures. The Tb magnetic moments, equal to 8.8 (4) μ<sub>B</sub> and parallel to the c axis, form a collinear magnetic structure described by the propagation vector k = [½ , ½ , ½]. This magnetic structure is stable up to the Néel temperature T<sub>N</sub> = 40 K. For Ho<sub>2</sub>Ni<sub>2</sub>In a complex, temperature-dependent magnetic structure is detected. In the temperature range 6.1-8.6 K, an incommensurate sinusoidal magnetic structure, described by the propagation vector k<sub>1</sub> = [0.24, 1, 0.52] is observed, while in the temperature interval 2.2-2.5 K a square-modulated magnetic structure, related to k<sub>2</sub> = [0.17,{{5} \\\\over {6}},{{1} \\\\over {2}}] (the component along the a axis slightly differs from the commensurate value) and its third harmonics 3k<sub>2</sub> = [0.50,{{5} \\\\over {2}},{{3} \\\\over {2}}] is found. At 3.1-3.7 K as well as below 2 K, a coexistence of both detected magnetic structures is observed. The Ho magnetic moments remain parallel to the c axis in both the sine- and square-modulated magnetic structures. The low-temperature heat capacity data confirm a first-order transition near 3 K.</p>\",\"PeriodicalId\":7320,\"journal\":{\"name\":\"Acta crystallographica Section B, Structural science, crystal engineering and materials\",\"volume\":null,\"pages\":null},\"PeriodicalIF\":1.3000,\"publicationDate\":\"2023-10-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Acta crystallographica Section B, Structural science, crystal engineering and materials\",\"FirstCategoryId\":\"92\",\"ListUrlMain\":\"https://doi.org/10.1107/S2052520623006315\",\"RegionNum\":3,\"RegionCategory\":\"化学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"2023/8/11 0:00:00\",\"PubModel\":\"Epub\",\"JCR\":\"Q3\",\"JCRName\":\"CHEMISTRY, MULTIDISCIPLINARY\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Acta crystallographica Section B, Structural science, crystal engineering and materials","FirstCategoryId":"92","ListUrlMain":"https://doi.org/10.1107/S2052520623006315","RegionNum":3,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"2023/8/11 0:00:00","PubModel":"Epub","JCR":"Q3","JCRName":"CHEMISTRY, MULTIDISCIPLINARY","Score":null,"Total":0}
引用次数: 0
摘要
用粉末中子衍射方法研究了R2Ni2In(R=Tb和Ho)在低温下的晶体和磁性结构。这些化合物结晶为Mn2AlB2型的正交晶体结构。在低温下,仅局限于稀土原子上的磁矩形成反铁磁结构。Tb磁矩,等于8.8 (4) μB并平行于c轴,形成由传播矢量k=[½描述的共线磁结构 , ½ , ½]。这种磁性结构在Néel温度TN=40之前是稳定的 K.对于Ho2Ni2,在复合物中检测到温度相关的磁性结构。在温度范围6.1-8.6 K、 由传播矢量k1=[0.24, 1. 0.52],而在温度区间2.2-2.5 K是一个正方形调制的磁结构,与k2=[0.17,{{5}\over{6}},{1}\over{2}}](沿a轴的分量与相应值略有不同)及其三次谐波3k2=[0.50,{5}\over{2}},{3}\over{2}}]有关。在3.1-3.7 K以及低于2 K、 观察到两个检测到的磁性结构的共存。在正弦和方形调制磁结构中,Ho磁矩保持平行于c轴。低温热容数据证实了3附近的一阶跃迁 K
Crystal and magnetic structures of R2Ni2In compounds (R = Tb and Ho).
Crystal and magnetic structures of R2Ni2In (R = Tb and Ho) have been studied using powder neutron diffraction at low temperatures. The compounds crystallize as orthorhombic crystal structures of the Mn2AlB2 type. At low temperatures, the magnetic moments localized solely on the rare earth atoms form antiferromagnetic structures. The Tb magnetic moments, equal to 8.8 (4) μB and parallel to the c axis, form a collinear magnetic structure described by the propagation vector k = [½ , ½ , ½]. This magnetic structure is stable up to the Néel temperature TN = 40 K. For Ho2Ni2In a complex, temperature-dependent magnetic structure is detected. In the temperature range 6.1-8.6 K, an incommensurate sinusoidal magnetic structure, described by the propagation vector k1 = [0.24, 1, 0.52] is observed, while in the temperature interval 2.2-2.5 K a square-modulated magnetic structure, related to k2 = [0.17,{{5} \over {6}},{{1} \over {2}}] (the component along the a axis slightly differs from the commensurate value) and its third harmonics 3k2 = [0.50,{{5} \over {2}},{{3} \over {2}}] is found. At 3.1-3.7 K as well as below 2 K, a coexistence of both detected magnetic structures is observed. The Ho magnetic moments remain parallel to the c axis in both the sine- and square-modulated magnetic structures. The low-temperature heat capacity data confirm a first-order transition near 3 K.
期刊介绍:
Acta Crystallographica Section B: Structural Science, Crystal Engineering and Materials publishes scientific articles related to the structural science of compounds and materials in the widest sense. Knowledge of the arrangements of atoms, including their temporal variations and dependencies on temperature and pressure, is often the key to understanding physical and chemical phenomena and is crucial for the design of new materials and supramolecular devices. Acta Crystallographica B is the forum for the publication of such contributions. Scientific developments based on experimental studies as well as those based on theoretical approaches, including crystal-structure prediction, structure-property relations and the use of databases of crystal structures, are published.