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Electron Spin Resonance of Ni-doped CuGeO$_3$ in the paramagnetic, spin-Peierls and antiferromagnetic states: Comparison with non-magnetic impurities

机译:顺磁性的Ni掺杂CuGeO的电子自旋共振$ _3 $   spin-peierls和反铁磁态:与非磁性的比较   杂质

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摘要

We have performed Electron Spin Resonance measurements on single crystals ofthe doped spin-Peierls compounds CuGe$_{1-y}$Si$_y$O$_3$ andCu$_{1-x}$M$_x$GeO$_3$ with M = Zn, Mg, Ni ($x, y\leq 0.1$). The first part ofour experiments was performed in the paramagnetic and spin-Peierls phases at9.5, 95 and 190 GHz. All non-magnetic impurities (Si, Zn and Mg) were found tohardly affect the position and linewidth of the single line resonance, in spiteof the moment formation due to the broken chains. In contrast to Si, Zn andMg-doping, the presence of Ni (S = 1) at low concentration induces aspectacular shift towards high fields of the ESR line (up to 40% for x=0.002),together with a large broadening. This shift is strictly proportional to theratio of Ni to Cu susceptibilities: Hence it is strongly enhanced below thespin-Peierls transition. We interpret this shift and the broadening as due tothe exchange field induced by the Ni ions onto the strongly exchange coupled Cuspins. Second, the antiferromagnetic resonance was investigated in Ni-dopedsamples. The frequency vs magnetic field relation of the resonance is wellexplained by the classical theory with orthorhombic anisotropy, with $g$ valuesremarkably reduced, in accordance with the study of the spin-Peierls andparamagnetic phases. The easy, second-easy, and hard axes are found to be $a$,$c$, and $b$ axes, respectively. These results, which are dominated by thesingle ion anisotropy of Ni$^{2+}$, are discussed in comparison with those inthe Zn- and Si-doped CuGeO$_3$.
机译:我们已经对掺杂的自旋Peierls化合物CuGe $ _ {1-y} $ Si $ _y $ O $ _3 $和Cu $ _ {1-x} $ M $ _x $ GeO $ _3 $的单晶进行了电子自旋共振测量。其中M = Zn,Mg,Ni($ x,y \ leq 0.1 $)。实验的第一部分是在9.5 GHz,95 GHz和190 GHz的顺磁和自旋Peierls相中进行的。尽管由于断链而形成力矩,但发现所有非磁性杂质(Si,Zn和Mg)几乎不会影响单线谐振的位置和线宽。与Si,Zn和Mg掺杂相反,低浓度的Ni(S = 1)的存在会引起ESR谱线向高场的侧向偏移(对于x = 0.002高达40%),并伴随较大的展宽。该位移与Ni对Cu的磁化率的严格比例成正比:因此,在自旋-Peierls转变以下会大大增强。我们将这种转变和扩展解释为由于Ni离子在强交换耦合Cuspins上诱导的交换场。其次,在掺镍样品中研究了反铁磁共振。根据对自旋Peierls和顺磁相的研究,具有正交各向异性的经典理论很好地解释了共振的频率与磁场的关系,其中$ g $的值显着降低。容易轴,次要轴和硬轴分别是$ a $,$ c $和$ b $轴。与以Zn和Si掺杂的CuGeO $ _3 $进行比较,讨论了以Ni $ ^ {2 +} $的单离子各向异性为主导的这些结果。

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