Phillips George S, Steele James M A, Sayed Farheen N, Karger Leonhard, Nagle-Cocco Liam A V, Genreith-Schriever Annalena R, Pérez Gabriel E, Keen David A, Janek Jürgen, Brezesinski Torsten, Bocarsly Joshua D, Dutton Siân E, Grey Clare P
Yusuf Hamied Department of Chemistry, University of Cambridge, Lensfield Road, Cambridge CB2 1EW, U.K.
The Faraday Institution, Didcot OX11 0RA, U.K.
J Am Chem Soc. 2025 Aug 13;147(32):29042-29051. doi: 10.1021/jacs.5c07435. Epub 2025 Jul 31.
Lithium nickel oxide, LiNiO (LNO), and its doped derivatives are promising battery cathode materials with high gravimetric capacity and operating voltages. They are also of interest to the field of quantum magnetism due to the presumed = 1/2 triangular lattice and associated geometric frustration. However, the tendency for Li/Ni substitutional defects and off-stoichiometry makes fundamental studies challenging. In particular, there is still a discrepancy between the rhombohedral (3̅) bulk structure and the Jahn-Teller (JT) distortions of the NiO octahedra inferred on the basis of local structural probes. Karger . ( , , 648-657) recently used Na/Li ion exchange to synthesize "defect-free" LNO by exploiting the absence of antisite disorder in NaNiO (NNO). Here we characterize the short- and long-range structure of this ion-exchanged material and observe splittings of key Bragg reflections at 100 K in X-ray and neutron diffraction (XRD and NPD), indicative of a monoclinic distortion induced by a cooperative collinear JT distortion, similar to that seen in NNO. Variable temperature XRD reveals a second-order phase transition from the monoclinic (2/) low-temperature structure to a rhombohedral (3̅) structure above ∼400 K. We propose that this collinear JT ordering is also present in solid-state synthesized LNO with the domain size and extent of monoclinic distortion controlled by defect concentration. This new structural description of LNO will help advance our understanding of its electronic and magnetic properties and the series of phase transformations that this material undergoes upon electrochemical cycling in Li-ion batteries.
锂镍氧化物LiNiO₂(LNO)及其掺杂衍生物是很有前景的电池正极材料,具有高比容量和工作电压。由于其假定的自旋S = 1/2三角晶格以及相关的几何阻挫,它们在量子磁学领域也备受关注。然而,Li/Ni替代缺陷和非化学计量比的倾向使得基础研究具有挑战性。特别是,基于局部结构探针推断出的菱面体(R3̅)体相结构与NiO₆八面体的 Jahn-Teller(JT)畸变之间仍存在差异。Karger等人(《物理评论B》,第95卷,第12期,125148,2017年;648 - 657页)最近利用Na/Li离子交换,通过利用NaNiO₂(NNO)中不存在反位无序的特点来合成“无缺陷”的LNO。在此,我们对这种离子交换材料的短程和长程结构进行了表征,并在100 K下的X射线和中子衍射(XRD和NPD)中观察到关键布拉格反射的分裂,这表明由协同共线JT畸变引起的单斜畸变,类似于在NNO中看到的情况。变温XRD揭示了从单斜(C2/m)低温结构到约400 K以上的菱面体(R3̅)结构的二级相变。我们提出,这种共线JT有序也存在于固态合成的LNO中,其畴尺寸和单斜畸变程度由缺陷浓度控制。LNO的这种新结构描述将有助于推进我们对其电子和磁性特性以及该材料在锂离子电池中电化学循环时所经历的一系列相变的理解。