Mizuno Asato, Shuku Yoshiaki, Matsushita Michio M, Tsuchiizu Masahisa, Hara Yuuki, Wada Nobuo, Shimizu Yasuhiro, Awaga Kunio
Department of Chemistry & Integrated Research Consortium on Chemical Sciences (IRCCS), Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602, Japan.
Venture business laboratory (VBL), Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602, Japan.
Phys Rev Lett. 2017 Aug 4;119(5):057201. doi: 10.1103/PhysRevLett.119.057201. Epub 2017 Jul 31.
We report the first 3D spin liquid state of isotropic organic spins. Structural analysis, and magnetic and heat-capacity measurements were carried out for a chiral organic radical salt, (TBA){1.5}[(-)-NDI-Δ] (TBA denotes tetrabutylammonium and NDI denotes naphthalene diimide), in which (-)-NDI-Δ forms a K{4} structure due to its triangular molecular structure and an intermolecular π-π overlap between the NDI moieties. This lattice was identical to the hyperkagome lattice of S=1/2 Mott dimers, and should exhibit 3D spin frustration. In fact, even though the high-temperature magnetic susceptibility followed the Curie-Weiss law with a negative Weiss constant of θ=-15 K, the low-temperature magnetic measurements revealed no long-range magnetic ordering down to 70 mK, and suggested the presence of a spin liquid state with a large residual paramagnetism χ_{0} of 8.5×10^{-6} emu g^{-1} at the absolute zero temperature. This was supported by the ^{14}N NMR measurements down to 0.38 K. Further, the low-temperature heat capacities c_{p} down to 68 mK clearly indicated the presence of c_{p} for the spin liquid state, which can be fitted to the power law of T^{0.62} in the wide temperature range 0.07-4.5 K.
我们报道了各向同性有机自旋的首个三维自旋液体态。对一种手性有机自由基盐(TBA)₁.₅[(-)-NDI-Δ](TBA表示四丁基铵,NDI表示萘二酰亚胺)进行了结构分析、磁性和热容量测量,其中(-)-NDI-Δ因其三角形分子结构以及NDI部分之间的分子间π-π重叠而形成K₄结构。该晶格与S = 1/2莫特二聚体的超 Kagome晶格相同,应表现出三维自旋阻挫。实际上,尽管高温磁化率遵循居里 - 外斯定律,外斯常数θ = -15 K为负,但低温磁性测量显示直至70 mK都没有长程磁有序,这表明存在自旋液体态,在绝对零度时具有8.5×10⁻⁶ emu g⁻¹的大剩余顺磁性χ₀。这得到了直至0.38 K的¹⁴N NMR测量的支持。此外,直至68 mK的低温热容量cₚ清楚地表明存在自旋液体态的cₚ,在0.07 - 4.5 K的宽温度范围内可拟合为T⁰.⁶²的幂律。