Thennakoon Asiri, Yokokura Ryouga, Yang Yang, Kajimoto Ryoichi, Nakamura Mitsutaka, Hayashi Masahiro, Michioka Chishiro, Chern Gia-Wei, Broholm Collin, Ueda Hiroaki, Lee Seung-Hun
Department of Physics, University of Virginia, Charlottesville, VA, 22904, USA.
Solid State Physics and Chemistry Lab, Division of Chemistry, Graduate School of Science, Kyoto University, Kyoto City, 606-8502, Japan.
Nat Commun. 2025 Apr 26;16(1):3939. doi: 10.1038/s41467-025-58971-4.
The pursuit of quantum spin liquid (QSL) states in condensed matter physics has drawn attention to kagome antiferromagnets (AFM) where a two-dimensional corner-sharing network of triangles frustrates conventional magnetic orders. While quantum kagome AFMs based on Cu (3d, s = ½) ions have been extensively studied, there is so far little work beyond copper-based systems. Here we present our bulk magnetization, specific heat and neutron scattering studies on single crystals of a new titanium fluorides CsRbKTiF where Ti (3d, s = ½) ions form a modulated quantum kagome antiferromagnet that does not order magnetically down to 1.5 K. Our comprehensive map of the dynamic response function acquired at 1.5 K where the heat capacity is T-linear reveals a dispersive continuum emanating from soft lines that extend along (100). The data indicate fractionalized spinon-like excitations with quasi-one-dimensional dispersion within a quasi-two-dimensional spin system.
凝聚态物理中对量子自旋液体(QSL)态的追求,使人们将注意力投向了 Kagome 反铁磁体(AFM),其中由三角形构成的二维角共享网络阻碍了传统磁序。虽然基于 Cu(3d,s = ½)离子的量子 Kagome AFM 已得到广泛研究,但迄今为止,除铜基体系外几乎没有其他研究。在此,我们展示了对新型钛氟化物 CsRbKTiF 单晶进行的体磁化、比热和中子散射研究,其中 Ti(3d,s = ½)离子形成了一种调制量子 Kagome 反铁磁体,其在低至 1.5 K 时仍未发生磁有序。我们在 1.5 K 下获取的动态响应函数的全面图谱显示,在热容量呈 T 线性的情况下,存在从沿(100)方向延伸的软线发出的色散连续体。数据表明在准二维自旋系统中存在具有准一维色散的类自旋子分数化激发。