Bradley C. Sheath, Stanislav Savvin and Simon J. Clarke*,
{"title":"季系硫化物Ba2FeMS5 (M = Sb, Bi)的磁性结构对比","authors":"Bradley C. Sheath, Stanislav Savvin and Simon J. Clarke*, ","doi":"10.1021/acs.inorgchem.4c0377010.1021/acs.inorgchem.4c03770","DOIUrl":null,"url":null,"abstract":"<p >Ba<sub>2</sub>FeSbS<sub>5</sub> and Ba<sub>2</sub>FeBiS<sub>5</sub> are two isostructural quaternary sulfides that crystallize in the <i>Pnma</i> space group with four formula units per unit cell. Ba<sub>2</sub>FeSbS<sub>5</sub> has lattice parameters <i>a</i> = 12.08609(3) Å, <i>b</i> = 8.83426(2) Å, and <i>c</i> = 8.89114(2) Å, and Ba<sub>2</sub>FeBiS<sub>5</sub> has <i>a</i> = 12.09610(3) Å, <i>b</i> = 8.89281(2) Å, and <i>c</i> = 8.82437(2) Å at room temperature. They comprise infinite [FeMS<sub>5</sub>]<sup>4–</sup> (M = Sb, Bi) chains, where Fe<sup>3+</sup> is present in FeS<sub>4</sub> tetrahedra and M<sup>3+</sup> ions reside in edge-sharing MS<sub>6</sub> distorted octahedra, each of which shares an edge with an FeS<sub>4</sub> tetrahedron. Powder neutron diffraction measurements confirm the presence of long-range antiferromagnetic order of the Fe<sup>3+</sup> moments in both materials, where Fe–S···S–Fe super-superexchange interactions which act along the direction of the [FeMS<sub>5</sub>]<sup>4–</sup> (M = Sb, Bi) chains are the driving force for this antiferromagnetic order. The magnetic Bragg reflections reside on a <i>k</i>-vector with <i>k</i> = (1/2 0 1/2), and the relative orientations of the moments are similar in the two cases One significant difference is that the moments are aligned along the crystallographic <i>b</i>-axis in Ba<sub>2</sub>FeSbS<sub>5</sub>, whereas in Ba<sub>2</sub>FeBiS<sub>5</sub> they lie along the longer crystallographic <i>a</i>-axis, reflecting the weak directional preference of the Fe<sup>3+</sup> moments. Furthermore, an additional incommensurately modulated ordering of the Fe<sup>3+</sup> moments is suggested for Ba<sub>2</sub>FeSbS<sub>5</sub> (but not Ba<sub>2</sub>FeBiS<sub>5</sub>) by the appearance of small additional magnetic Bragg peaks in the neutron diffraction data, which may be a consequence of greater magnetic frustration in Ba<sub>2</sub>FeSbS<sub>5</sub>.</p><p >Ba<sub>2</sub>FeSbS<sub>5</sub> and Ba<sub>2</sub>FeBiS<sub>5</sub> differ in their magnetic structures likely reflecting the different levels of magnetic frustration determined computationally.</p>","PeriodicalId":40,"journal":{"name":"Inorganic Chemistry","volume":"63 49","pages":"23267–23275 23267–23275"},"PeriodicalIF":4.7000,"publicationDate":"2024-11-25","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://pubs.acs.org/doi/epdf/10.1021/acs.inorgchem.4c03770","citationCount":"0","resultStr":"{\"title\":\"Contrasting Magnetic Structures in the Quaternary Sulfides Ba2FeMS5 (M = Sb, Bi)\",\"authors\":\"Bradley C. Sheath, Stanislav Savvin and Simon J. Clarke*, \",\"doi\":\"10.1021/acs.inorgchem.4c0377010.1021/acs.inorgchem.4c03770\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p >Ba<sub>2</sub>FeSbS<sub>5</sub> and Ba<sub>2</sub>FeBiS<sub>5</sub> are two isostructural quaternary sulfides that crystallize in the <i>Pnma</i> space group with four formula units per unit cell. Ba<sub>2</sub>FeSbS<sub>5</sub> has lattice parameters <i>a</i> = 12.08609(3) Å, <i>b</i> = 8.83426(2) Å, and <i>c</i> = 8.89114(2) Å, and Ba<sub>2</sub>FeBiS<sub>5</sub> has <i>a</i> = 12.09610(3) Å, <i>b</i> = 8.89281(2) Å, and <i>c</i> = 8.82437(2) Å at room temperature. They comprise infinite [FeMS<sub>5</sub>]<sup>4–</sup> (M = Sb, Bi) chains, where Fe<sup>3+</sup> is present in FeS<sub>4</sub> tetrahedra and M<sup>3+</sup> ions reside in edge-sharing MS<sub>6</sub> distorted octahedra, each of which shares an edge with an FeS<sub>4</sub> tetrahedron. Powder neutron diffraction measurements confirm the presence of long-range antiferromagnetic order of the Fe<sup>3+</sup> moments in both materials, where Fe–S···S–Fe super-superexchange interactions which act along the direction of the [FeMS<sub>5</sub>]<sup>4–</sup> (M = Sb, Bi) chains are the driving force for this antiferromagnetic order. The magnetic Bragg reflections reside on a <i>k</i>-vector with <i>k</i> = (1/2 0 1/2), and the relative orientations of the moments are similar in the two cases One significant difference is that the moments are aligned along the crystallographic <i>b</i>-axis in Ba<sub>2</sub>FeSbS<sub>5</sub>, whereas in Ba<sub>2</sub>FeBiS<sub>5</sub> they lie along the longer crystallographic <i>a</i>-axis, reflecting the weak directional preference of the Fe<sup>3+</sup> moments. Furthermore, an additional incommensurately modulated ordering of the Fe<sup>3+</sup> moments is suggested for Ba<sub>2</sub>FeSbS<sub>5</sub> (but not Ba<sub>2</sub>FeBiS<sub>5</sub>) by the appearance of small additional magnetic Bragg peaks in the neutron diffraction data, which may be a consequence of greater magnetic frustration in Ba<sub>2</sub>FeSbS<sub>5</sub>.</p><p >Ba<sub>2</sub>FeSbS<sub>5</sub> and Ba<sub>2</sub>FeBiS<sub>5</sub> differ in their magnetic structures likely reflecting the different levels of magnetic frustration determined computationally.</p>\",\"PeriodicalId\":40,\"journal\":{\"name\":\"Inorganic Chemistry\",\"volume\":\"63 49\",\"pages\":\"23267–23275 23267–23275\"},\"PeriodicalIF\":4.7000,\"publicationDate\":\"2024-11-25\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://pubs.acs.org/doi/epdf/10.1021/acs.inorgchem.4c03770\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Inorganic Chemistry\",\"FirstCategoryId\":\"92\",\"ListUrlMain\":\"https://pubs.acs.org/doi/10.1021/acs.inorgchem.4c03770\",\"RegionNum\":2,\"RegionCategory\":\"化学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q1\",\"JCRName\":\"CHEMISTRY, INORGANIC & NUCLEAR\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Inorganic Chemistry","FirstCategoryId":"92","ListUrlMain":"https://pubs.acs.org/doi/10.1021/acs.inorgchem.4c03770","RegionNum":2,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"CHEMISTRY, INORGANIC & NUCLEAR","Score":null,"Total":0}
引用次数: 0
摘要
Ba2FeSbS5和Ba2FeBiS5是在Pnma空间群中结晶的两种同结构季化物,每晶胞有四个分子式单元。Ba2FeSbS5的晶格参数为a = 12.08609(3) Å, b = 8.83426(2) Å, c = 8.89114(2) Å, Ba2FeBiS5的晶格参数为a = 12.09610(3) Å, b = 8.89281(2) Å, c = 8.82437(2) Å。它们由无限的[FeMS5]4 - (M = Sb, Bi)链组成,其中Fe3+存在于FeS4四面体中,M3+离子存在于共享边的MS6扭曲八面体中,每一个都与FeS4四面体共享一条边。粉末中子衍射测量证实了两种材料中Fe3+矩的远程反铁磁阶序的存在,其中沿[FeMS5]4 - (M = Sb, Bi)链方向的Fe-S···S-Fe超超交换相互作用是这种反铁磁阶序的驱动力。磁Bragg反射位于k =(1/2 0 /2)的k向量上,两种情况下的磁Bragg反射的相对取向相似,其中显著的区别是,Ba2FeSbS5中的磁Bragg反射沿晶体学b轴排列,而Ba2FeBiS5中的磁Bragg反射沿较长的晶体学a轴排列,反映了Fe3+磁Bragg反射弱的方向偏好。此外,在Ba2FeSbS5(而不是Ba2FeBiS5)中,中子衍射数据中出现了小的附加磁Bragg峰,这可能是Ba2FeSbS5中更大的磁挫折的结果,从而表明了Fe3+矩的额外不相关调制顺序。Ba2FeSbS5和Ba2FeBiS5的磁性结构不同,这可能反映了计算确定的磁挫败程度的不同。
Contrasting Magnetic Structures in the Quaternary Sulfides Ba2FeMS5 (M = Sb, Bi)
Ba2FeSbS5 and Ba2FeBiS5 are two isostructural quaternary sulfides that crystallize in the Pnma space group with four formula units per unit cell. Ba2FeSbS5 has lattice parameters a = 12.08609(3) Å, b = 8.83426(2) Å, and c = 8.89114(2) Å, and Ba2FeBiS5 has a = 12.09610(3) Å, b = 8.89281(2) Å, and c = 8.82437(2) Å at room temperature. They comprise infinite [FeMS5]4– (M = Sb, Bi) chains, where Fe3+ is present in FeS4 tetrahedra and M3+ ions reside in edge-sharing MS6 distorted octahedra, each of which shares an edge with an FeS4 tetrahedron. Powder neutron diffraction measurements confirm the presence of long-range antiferromagnetic order of the Fe3+ moments in both materials, where Fe–S···S–Fe super-superexchange interactions which act along the direction of the [FeMS5]4– (M = Sb, Bi) chains are the driving force for this antiferromagnetic order. The magnetic Bragg reflections reside on a k-vector with k = (1/2 0 1/2), and the relative orientations of the moments are similar in the two cases One significant difference is that the moments are aligned along the crystallographic b-axis in Ba2FeSbS5, whereas in Ba2FeBiS5 they lie along the longer crystallographic a-axis, reflecting the weak directional preference of the Fe3+ moments. Furthermore, an additional incommensurately modulated ordering of the Fe3+ moments is suggested for Ba2FeSbS5 (but not Ba2FeBiS5) by the appearance of small additional magnetic Bragg peaks in the neutron diffraction data, which may be a consequence of greater magnetic frustration in Ba2FeSbS5.
Ba2FeSbS5 and Ba2FeBiS5 differ in their magnetic structures likely reflecting the different levels of magnetic frustration determined computationally.
期刊介绍:
Inorganic Chemistry publishes fundamental studies in all phases of inorganic chemistry. Coverage includes experimental and theoretical reports on quantitative studies of structure and thermodynamics, kinetics, mechanisms of inorganic reactions, bioinorganic chemistry, and relevant aspects of organometallic chemistry, solid-state phenomena, and chemical bonding theory. Emphasis is placed on the synthesis, structure, thermodynamics, reactivity, spectroscopy, and bonding properties of significant new and known compounds.