Wan W, Christensen N B, Sandvik A W, Tregenna-Piggott P, Nilsen G J, Mourigal M, Perring T G, Frost C D, McMorrow D F, Rønnow H M
Department of Physics, Technical University of Denmark, DK-2800 Kongens Lyngby, Denmark.
Department of Physics, Boston University, 590 Commonwealth Avenue, Boston, MA 02215, United States of America.
J Phys Condens Matter. 2020 Jun 18;32(37). doi: 10.1088/1361-648X/ab757a.
It is well established that in the low-temperature limit, the two-dimensional quantum Heisenberg antiferromagnet on a square lattice (2DQHAFSL) exhibits an anomaly in its spectrum at short-wavelengths on the zone-boundary. In the vicinity of thepoint the pole in the one-magnon response exhibits a downward dispersion, is heavily damped and attenuated, giving way to an isotropic continuum of excitations extending to high energies. The origin of the anomaly and the presence of the continuum are of current theoretical interest, with suggestions focused around the idea that the latter evidences the existence of spinons in a two-dimensional system. Here we present the results of neutron inelastic scattering experiments and Quantum Monte Carlo calculations on the metallo-organic compound Cu(DCOO)DO (CFTD), an excellent physical realisation of the 2DQHAFSL, designed to investigate how the anomaly atevolves up to finite temperatures. Our data reveal that on warming the anomaly survives the loss of long-range, three-dimensional order, and that it is thus a robust feature of the two-dimensional system. With further increase of temperature the zone-boundary response gradually softens and broadens, washing out theanomaly. This is confirmed by a comparison of our data with the results of finite-temperature Quantum Monte Carlo simulations where the two are found to be in good accord. In the vicinity of the antiferromagnetic zone centre, there was no significant softening of the magnetic excitations over the range of temperatures investigated.
众所周知,在低温极限下,方形晶格上的二维量子海森堡反铁磁体(2DQHAFSL)在区域边界的短波长处其光谱会出现异常。在该点附近,单磁振子响应中的极点呈现向下色散,受到强烈阻尼和衰减,让位于延伸到高能的各向同性激发连续体。这种异常的起源以及连续体的存在是当前理论研究的热点,相关观点主要围绕后者证明了二维系统中自旋子的存在这一想法。在此,我们展示了对金属有机化合物Cu(DCOO)DO (CFTD)进行中子非弹性散射实验和量子蒙特卡罗计算的结果,该化合物是2DQHAFSL的一个出色物理实例,旨在研究这种异常如何演变至有限温度。我们的数据表明,在升温过程中,这种异常在长程三维有序消失后依然存在,因此它是二维系统的一个稳健特征。随着温度进一步升高,区域边界响应逐渐变软并展宽,异常消失。将我们的数据与有限温度量子蒙特卡罗模拟结果进行比较证实了这一点,两者结果吻合良好。在反铁磁区域中心附近,在所研究的温度范围内,磁激发没有明显变软。