边缘改性海森堡自旋纳米带中长程磁序的存在

Da-cheng Ma, Ling-yi Cui, Chu-xiao Sun, Xiao-dan Chi, Z. Xianyu, An Du
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摘要

虽然根据梅明-瓦格纳定理,一维或二维各向同性海森堡模型在任何非零温度下都不存在自发磁化,但在非零温度下,侧面装饰的海森堡自旋纳米带出现了长程磁序。利用自旋格林函数法,我们计算了单离子各向异性的边自旋装饰的海森堡纳米带的磁化率,发现无论系统中被装饰的边自旋连接在一起还是相互分离,系统都表现出非零的转变温度。当纳米带的宽度达到无穷大极限时,无论纳米带中的单边还是双边被边自旋装饰,系统的过渡温度最终都趋于同一个有限常数。研究结果表明,低维自旋系统的磁性与三维自旋系统的磁性不同。当海森堡自旋纳米带中边缘自旋的单离子各向异性可以被电场调制时,就可以得到该体系的各种有用的长程磁序。这些研究成果可为设计和制造下一代低维磁性随机存取存储器提供详尽的理论依据。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Existence of Long-Range Magnetic Order in Heisenberg Spin Nanoribbon with Edge Modification
A long-range magnetic order appears on side decorated Heisenberg spin nanoribbon at nonzero temperature, although no spontaneous magnetization exists in a one- or two-dimensional isotropic Heisenberg model at any nonzero temperature according to Mermin-Wagner theorem. By use of the spin Green’s function method, we calculated the magnetizations of Heisenberg nanoribbon decorated by side spins with single-ion anisotropy and found that the system exhibits a nonzero transition temperature, whether the decorated edge spins of the system link together or separate from each other. When the width of the nanoribbon achieves infinity limit, the transition temperatures of the system tend to a same finite constant eventually whether one edge or double edges are decorated by side spins in the nanoribbon. The results reveal that the magnetism of a low-dimensional spin system is different from that of a three-dimensional spin system. When the single-ion anisotropy of edge spins in Heisenberg spin nanoribbon can be modulated by an electric field experimentally, various useful long-range magnetic orders of the system can be obtained. The works can provide a detailed theoretical basis for designing and fabricating the next-generation low-dimensional magnetic random-access memory.
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