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关于非磁性杂质对准一维磁体中类自旋-派尔斯转变的掺杂效应的结构和磁性研究:1-(4'-硝基苄基)吡啶双(马来腈二硫醇)镍酸盐。

Structural and magnetic investigations for the doping effect of nonmagnetic impurity on the spin-Peierls-like transition in a quasi-one-dimensional magnet: 1-(4'-nitrobenzyl)pyridinium bis(maleonitriledithiolato)nickelate.

作者信息

Ren X M, Akutagawa T, Noro S, Nishihara S, Nakamura T, Yoshida Y, Inoue K

机构信息

Research Institute for Electronic Science, Hokkaido University, Sapporo 060-0812, Japan.

出版信息

J Phys Chem B. 2006 Apr 20;110(15):7671-7. doi: 10.1021/jp0556106.

Abstract

A nonmagnetic compound, [NO(2)BzPy][Au(mnt)(2)] (NO(2)BzPy(+) = 1-(4'-nitrobenzyl)pyridinium; mnt(2-) = maleonitriledithiolate), was synthesized and characterized structurally, which is isostructural with [NO(2)BzPy][Ni(mnt)(2)] that is a quasi-one-dimensional magnet and possesses a spin-Peierls-like transition with J = 192 K in the gapless state and spin energy gap = 738 K in the dimerization state, respectively. Further, ten nonmagnetic impurity doped compounds with a formula [NO(2)BzPy][Au(x)Ni(1-x)(mnt)(2)] (x = 0.01-0.73) were prepared and investigated by crystal structural determinations and magnetic susceptibility measurements. The nonmagnetic doping causes the suppression of the spin transition with an average rate of 221(12) K/percentage of dopant concentration. From the plots of chi(m)-T, the transition collapse (the characteristic of the transition is the sudden drop of chi(m) upon cooling, and the disappearance of this characteristic is considered as the criterion for the transition collapse) is estimated at around x > 0.27. In heavier doped system x = 0.49, the spin gap vanishes and a gapless phase is achieved again.

摘要

合成并通过结构表征了一种非磁性化合物[NO(2)BzPy][Au(mnt)(2)](NO(2)BzPy(+) = 1-(4'-硝基苄基)吡啶鎓;mnt(2-) = 马来二腈二硫醇盐),它与[NO(2)BzPy][Ni(mnt)(2)]同构,[NO(2)BzPy][Ni(mnt)(2)]是一种准一维磁体,在无隙态下具有J = 192 K的类自旋-派尔斯转变,在二聚化态下自旋能隙 = 738 K。此外,制备了十种化学式为[NO(2)BzPy][Au(x)Ni(1-x)(mnt)(2)](x = 0.01 - 0.73)的非磁性杂质掺杂化合物,并通过晶体结构测定和磁化率测量进行了研究。非磁性掺杂导致自旋转变受到抑制,平均速率为221(12) K/掺杂剂浓度百分比。从χm-T图来看,转变崩溃(转变的特征是χm在冷却时突然下降,这种特征的消失被视为转变崩溃的标准)估计在x > 0.27左右出现。在重掺杂体系x = 0.49中,自旋能隙消失,再次实现了无隙相。

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