Park Pyeongjae, Ghioldi E A, May Andrew F, Kolopus James A, Podlesnyak Andrey A, Calder Stuart, Paddison Joseph A M, Trumper A E, Manuel L O, Batista Cristian D, Stone Matthew B, Halász Gábor B, Christianson Andrew D
Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, TN, USA.
Department of Physics and Astronomy, University of Tennessee, Knoxville, TN, USA.
Nat Commun. 2024 Aug 23;15(1):7264. doi: 10.1038/s41467-024-51618-w.
The S = 1/2 triangular lattice antiferromagnet (TLAF) is a paradigmatic example of frustrated quantum magnetism. An ongoing challenge involves understanding the influence of exchange anisotropy on the collective behavior within such systems. Using inelastic neutron scattering (INS) and advanced calculation techniques, we have studied the low and high-temperature spin dynamics of BaLaCoTeO (BLCTO): a Co-based J = 1/2 TLAF that exhibits 120° order below T = 3.26 K. We determined the spin Hamiltonian by fitting the energy-resolved paramagnetic excitations measured at T > T, revealing exceptionally strong easy-plane XXZ anisotropy. Below T, the excitation spectrum exhibits a high energy continuum having a larger spectral weight than the single-magnon modes, suggesting a scenario characterized by a spinon confinement length that markedly exceeds the lattice spacing. We conjecture that this phenomenon arises from the proximity to a quantum melting point, even under strong easy-plane XXZ anisotropy. Finally, we highlight characteristic flat features in the excitation spectrum, which are connected to higher-order van Hove singularities in the magnon dispersion directly induced by easy-plane XXZ anisotropy. Our results provide a rare experimental insight into the nature of highly anisotropic S = 1/2 TLAFs between the Heisenberg and XY limits.
S = 1/2三角晶格反铁磁体(TLAF)是受挫量子磁体的一个典型例子。一个持续存在的挑战是理解交换各向异性对这类系统中集体行为的影响。利用非弹性中子散射(INS)和先进的计算技术,我们研究了BaLaCoTeO(BLCTO)的低温和高温自旋动力学:一种基于Co的J = 1/2 TLAF,在T = 3.26 K以下表现出120°有序。我们通过拟合在T > T时测量的能量分辨顺磁激发来确定自旋哈密顿量,揭示出异常强的易平面XXZ各向异性。在T以下,激发谱呈现出一个高能连续体,其谱权重比单磁振子模式更大,这表明一种由自旋子禁闭长度明显超过晶格间距所表征的情形。我们推测这种现象源于即使在强易平面XXZ各向异性下也接近量子熔点。最后,我们突出了激发谱中的特征性平坦特征,它们与易平面XXZ各向异性直接诱导的磁振子色散中的高阶范霍夫奇点相关。我们的结果为在海森堡极限和XY极限之间高度各向异性的S = 1/2 TLAF的性质提供了难得的实验见解。