首页> 外文期刊>Physical Review, B. Condensed Matter >Electron spin resonance of Ni-doped CuGeO3 in the paramagnetic, spin-Peierls, and antiferromagnetic states: Comparison with nonmagnetic impurities - art. no. 094425
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Electron spin resonance of Ni-doped CuGeO3 in the paramagnetic, spin-Peierls, and antiferromagnetic states: Comparison with nonmagnetic impurities - art. no. 094425

机译:Ni掺杂的CuGeO3在顺磁性,自旋Peierls和反铁磁性状态下的电子自旋共振:与非磁性杂质的比较-艺术。没有。 094425

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We have performed electron-spin-resonance measurements on single crystals of the doped spin-Peierls compounds CuGe1-ySiyO3 and Cu1-xMxGeO3 with M=Zn, Mg, Ni (x,yless than or equal to0.1). The first part of our experiments was performed in the paramagnetic and spin-Peierls phases at 9.5, 95, and 190 GHz. All nonmagnetic impurities (Si, Zn and Mg) were found to hardly affect the position and linewidth of the single line resonance, in spite of the moment formation due to the broken chains. In contrast to Si, Zn, and Mg dopings, the presence of Ni (S = 1) at low concentration induces a spectacular shift toward high fields of the ESR line (up to 40% for x = 0.002), together with a large broadening. This shift is strictly proportional to the ratio of Ni to Cu susceptibilities: Hence it is strongly enhanced below the spin-Peierls transition. We interpret this shift and the broadening as due to the exchange field induced by the Ni ions onto strongly exchange coupled Cu spins. Second, the antiferromagnetic resonance was investigated in Ni-doped samples. The frequency vs magnetic-field relation of the resonance is well explained by the classical theory with orthorhombic anisotropy, with g values remarkably reduced, in accordance with the study of the spin-Peierls and paramagnetic phases. The easy, second-easy, and hard axes are found to be a, c, and b axes, respectively. These results, which are dominated by the single ion anisotropy of Ni2+ are discussed in comparison with those in the Zn- and Si-doped CuGeO3. [References: 39]
机译:我们已经对掺杂的自旋-Peierls化合物CuGe1-ySiyO3和Cu1-xMxGeO3的单晶进行了电子自旋共振测量,其中M = Zn,Mg,Ni(x,y小于或等于0.1)。我们的实验的第一部分是在9.5、95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谱线向高场的急剧变化(x = 0.002时高达40%),并且展宽范围大。 。该位移严格与Ni与Cu的磁化率之比成正比:因此,在自旋Peierls转变以下会大大增强。我们将这种位移和变宽解释为由于Ni离子在强交换耦合的Cu自旋上诱导的交换场。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CuGeO3相比,讨论了以Ni2 +的单离子各向异性为主导的这些结果。 [参考:39]

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