Olga Yakubovich, Galina Kiriukhina, Elizaveta Manokhina, Anatoly Volkov, Olga Dimitrova, Larisa Shvanskaya and Alexander Vasiliev
{"title":"Na4.3Ni1.3Al1.7(PO4)4结构由填充α-CrPO4型转变为Na:磁性和离子迁移†驱动","authors":"Olga Yakubovich, Galina Kiriukhina, Elizaveta Manokhina, Anatoly Volkov, Olga Dimitrova, Larisa Shvanskaya and Alexander Vasiliev","doi":"10.1039/D5CE00268K","DOIUrl":null,"url":null,"abstract":"<p >A new phase Na<small><sub>4.3</sub></small>Ni<small><sub>1.3</sub></small>Al<small><sub>1.7</sub></small>(PO<small><sub>4</sub></small>)<small><sub>4</sub></small> was prepared by hydrothermal synthesis. Its crystal structure was determined using single-crystal X-ray diffraction data and refined against <em>F</em><small><sup>2</sup></small> to <em>R</em> = 0.055. The compound crystallizes in the orthorhombic space group <em>Cccm</em>, with unit cell parameters <em>a</em> = 6.3892(4), <em>b</em> = 19.6003(15) and <em>c</em> = 10.3570(6) Å, <em>V</em> = 1297.01(15) Å<small><sup>3</sup></small>, and <em>Z</em> = 4. Two symmetrically independent octahedra in the structure are jointly occupied by Ni and Al atoms. By sharing oxygen vertices, these octahedra form intercrossed chains stretched in the [101] and [<img>01] directions to build two-layered slabs perpendicular to the <em>b</em> axis. Phosphate tetrahedra strengthen the slabs by sharing most vertices and edges with the octahedra. One unshared vertex of each P1O<small><sub>4</sub></small> polyhedron is directed in the area between the slabs, which includes strongly disordered Na atoms. The title crystal structure is discussed as being derived from the α-CrPO<small><sub>4</sub></small> archetype, with a framework conversion from triperiodic to biperiodic slabs. The theoretical specific capacity of Na<small><sub>4.3</sub></small>Ni<small><sub>1.3</sub></small>Al<small><sub>1.7</sub></small>(PO<small><sub>4</sub></small>)<small><sub>4</sub></small> for the deintercalation of all sodium ions, equal to 140 mA h g<small><sup>−1</sup></small>, and the value of the migration barrier of about 0.5 eV in all three directions allow considering the compound as a potential material for the positive electrode of sodium-ion batteries. Magnetically, Na<small><sub>4.3</sub></small>Ni<small><sub>1.3</sub></small>Al<small><sub>1.7</sub></small>(PO<small><sub>4</sub></small>)<small><sub>4</sub></small> consists of isolated Ni<small><sup>2+</sup></small> ions and pairs of these ions coupled into ferromagnetic dimers. The exchange interactions between these entities are weak, which prevents the long-range magnetic order down to 2 K. The Schottky-type anomaly in the specific heat at low temperatures points to the energy gap between ferromagnetic ground state and antiferromagnetic excited state within the dimers.</p>","PeriodicalId":70,"journal":{"name":"CrystEngComm","volume":" 21","pages":" 3576-3583"},"PeriodicalIF":2.6000,"publicationDate":"2025-04-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Na4.3Ni1.3Al1.7(PO4)4 structure transformation from stuffed α-CrPO4 type driven by the incorporation of Na: magnetism and ionic migration†\",\"authors\":\"Olga Yakubovich, Galina Kiriukhina, Elizaveta Manokhina, Anatoly Volkov, Olga Dimitrova, Larisa Shvanskaya and Alexander Vasiliev\",\"doi\":\"10.1039/D5CE00268K\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p >A new phase Na<small><sub>4.3</sub></small>Ni<small><sub>1.3</sub></small>Al<small><sub>1.7</sub></small>(PO<small><sub>4</sub></small>)<small><sub>4</sub></small> was prepared by hydrothermal synthesis. Its crystal structure was determined using single-crystal X-ray diffraction data and refined against <em>F</em><small><sup>2</sup></small> to <em>R</em> = 0.055. The compound crystallizes in the orthorhombic space group <em>Cccm</em>, with unit cell parameters <em>a</em> = 6.3892(4), <em>b</em> = 19.6003(15) and <em>c</em> = 10.3570(6) Å, <em>V</em> = 1297.01(15) Å<small><sup>3</sup></small>, and <em>Z</em> = 4. Two symmetrically independent octahedra in the structure are jointly occupied by Ni and Al atoms. By sharing oxygen vertices, these octahedra form intercrossed chains stretched in the [101] and [<img>01] directions to build two-layered slabs perpendicular to the <em>b</em> axis. Phosphate tetrahedra strengthen the slabs by sharing most vertices and edges with the octahedra. One unshared vertex of each P1O<small><sub>4</sub></small> polyhedron is directed in the area between the slabs, which includes strongly disordered Na atoms. The title crystal structure is discussed as being derived from the α-CrPO<small><sub>4</sub></small> archetype, with a framework conversion from triperiodic to biperiodic slabs. The theoretical specific capacity of Na<small><sub>4.3</sub></small>Ni<small><sub>1.3</sub></small>Al<small><sub>1.7</sub></small>(PO<small><sub>4</sub></small>)<small><sub>4</sub></small> for the deintercalation of all sodium ions, equal to 140 mA h g<small><sup>−1</sup></small>, and the value of the migration barrier of about 0.5 eV in all three directions allow considering the compound as a potential material for the positive electrode of sodium-ion batteries. Magnetically, Na<small><sub>4.3</sub></small>Ni<small><sub>1.3</sub></small>Al<small><sub>1.7</sub></small>(PO<small><sub>4</sub></small>)<small><sub>4</sub></small> consists of isolated Ni<small><sup>2+</sup></small> ions and pairs of these ions coupled into ferromagnetic dimers. The exchange interactions between these entities are weak, which prevents the long-range magnetic order down to 2 K. The Schottky-type anomaly in the specific heat at low temperatures points to the energy gap between ferromagnetic ground state and antiferromagnetic excited state within the dimers.</p>\",\"PeriodicalId\":70,\"journal\":{\"name\":\"CrystEngComm\",\"volume\":\" 21\",\"pages\":\" 3576-3583\"},\"PeriodicalIF\":2.6000,\"publicationDate\":\"2025-04-23\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"CrystEngComm\",\"FirstCategoryId\":\"92\",\"ListUrlMain\":\"https://pubs.rsc.org/en/content/articlelanding/2025/ce/d5ce00268k\",\"RegionNum\":3,\"RegionCategory\":\"化学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"CHEMISTRY, MULTIDISCIPLINARY\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"CrystEngComm","FirstCategoryId":"92","ListUrlMain":"https://pubs.rsc.org/en/content/articlelanding/2025/ce/d5ce00268k","RegionNum":3,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"CHEMISTRY, MULTIDISCIPLINARY","Score":null,"Total":0}
引用次数: 0
摘要
采用水热合成法制备了新相Na4.3Ni1.3Al1.7(PO4)4。利用单晶x射线衍射数据确定了其晶体结构,并根据F2至R = 0.055进行了细化。化合物在正交空间群Cccm中结晶,晶胞参数a = 6.3892(4), b = 19.6003(15), c = 10.3570(6) Å, V = 1297.01(15) Å3, Z = 4。该结构中的两个对称独立的八面体被Ni和Al原子共同占据。通过共享氧顶点,这些八面体形成在[101]和[01]方向拉伸的交叉链,形成垂直于b轴的两层板。磷酸盐四面体通过与八面体共享大部分顶点和边缘来加强平板。每个p104多面体的一个未共享顶点指向板之间的区域,其中包括强烈无序的Na原子。讨论了标题晶体结构来源于α-CrPO4原型,其框架由三周期板转变为双周期板。Na4.3Ni1.3Al1.7(PO4)4对所有钠离子脱嵌的理论比容量等于140 mA h g−1,三个方向的迁移势垒值约为0.5 eV,可以考虑该化合物作为钠离子电池正极的潜在材料。在磁性上,Na4.3Ni1.3Al1.7(PO4)4由孤立的Ni2+离子和这些离子对偶联成铁磁性二聚体组成。这些实体之间的交换相互作用很弱,这阻止了远端磁序降低到2 K。低温比热中的肖特基型异常指出了二聚体中铁磁基态和反铁磁激发态之间的能量缺口。
Na4.3Ni1.3Al1.7(PO4)4 structure transformation from stuffed α-CrPO4 type driven by the incorporation of Na: magnetism and ionic migration†
A new phase Na4.3Ni1.3Al1.7(PO4)4 was prepared by hydrothermal synthesis. Its crystal structure was determined using single-crystal X-ray diffraction data and refined against F2 to R = 0.055. The compound crystallizes in the orthorhombic space group Cccm, with unit cell parameters a = 6.3892(4), b = 19.6003(15) and c = 10.3570(6) Å, V = 1297.01(15) Å3, and Z = 4. Two symmetrically independent octahedra in the structure are jointly occupied by Ni and Al atoms. By sharing oxygen vertices, these octahedra form intercrossed chains stretched in the [101] and [01] directions to build two-layered slabs perpendicular to the b axis. Phosphate tetrahedra strengthen the slabs by sharing most vertices and edges with the octahedra. One unshared vertex of each P1O4 polyhedron is directed in the area between the slabs, which includes strongly disordered Na atoms. The title crystal structure is discussed as being derived from the α-CrPO4 archetype, with a framework conversion from triperiodic to biperiodic slabs. The theoretical specific capacity of Na4.3Ni1.3Al1.7(PO4)4 for the deintercalation of all sodium ions, equal to 140 mA h g−1, and the value of the migration barrier of about 0.5 eV in all three directions allow considering the compound as a potential material for the positive electrode of sodium-ion batteries. Magnetically, Na4.3Ni1.3Al1.7(PO4)4 consists of isolated Ni2+ ions and pairs of these ions coupled into ferromagnetic dimers. The exchange interactions between these entities are weak, which prevents the long-range magnetic order down to 2 K. The Schottky-type anomaly in the specific heat at low temperatures points to the energy gap between ferromagnetic ground state and antiferromagnetic excited state within the dimers.