The S=1/2 Heisenberg spin chain compound SrCuO2 doped with different amounts of nickel (Ni), palladium (Pd), zinc (Zn) and cobalt (Co) has been studied by means of Cu nuclear magnetic resonance (NMR). Replacing only a few of the S=1/2 Cu ions with Ni, Pd, Zn or Co has a major impact on the magnetic properties of the spin chain system. In the case of Ni, Pd and Zn an unusual line broadening in the low temperature NMR spectra reveals the existence of an impurity-induced local alternating magnetization (LAM), while exponentially decaying spin-lattice relaxation rates $T_1^{-1}$ towards low temperatures indicate the opening of spin gaps. A distribution of gap magnitudes is proven by a stretched spin-lattice relaxation and a variation of $T_1^{-1}$ within the broad resonance lines. These observations depend strongly on the impurity concentration and therefore can be understood using the model of finite segments of the spin 1/2 antiferromagnetic Heisenberg chain, i.e. pure chain segmentation due to S = 0 impurities. This is surprising for Ni as it was previously assumed to be a magnetic impurity with S = 1 which is screened by the neighboring copper spins. In order to confirm the S = 0 state of the Ni, we performed x-ray absorption spectroscopy (XAS) and compared the measurements to simulated XAS spectra based on multiplet ligand-field theory. Furthermore, Zn doping leads to much smaller effects on both the NMR spectra and the spin-lattice relaxation rates, indicating that Zn avoids occupying Cu sites. For magnetic Co impurities, $T_1^{-1}$ does not obey the gap like decrease, and the low-temperature spectra get very broad. This could be related to the increase of the Neel temperature which was observed by recent muSR and susceptibility measurements, and is most likely an effect of the impurity spin $S\neq0$.
翻译:S=1/2 Heisenberg 螺旋链化合物 SrCuO2 使用镍(Ni)、 ⁇ (Pd)、锌(Zn)和钴(Co)的不同量的硬度(镍)、 ⁇ ( ⁇ )、锌(Zn)和钴(Co)进行了研究。S=1/2 Cuion仅用镍、Pd、Zn或Co来代替少数S=1/2 Cuion,对旋转链系统的磁性影响很大。对于Ni、Pd和Zn,低温NMR光谱中不同程度的测量显示存在杂质导致的本地交替磁化(LAM),而快速腐蚀的旋拉伸缩率($_Z_1 ⁇ -1})则表示开阔差距。通过松散的旋转拉伸缩和1美元($T_1 ⁇ -1美元)在宽度线中的变异度中可以证明。这些观测结果主要取决于低度浓度,因此可以理解,而通过微量的磁度(O/2 递解) 递解(O-I) 的分解) 和直径(Sy) 递解) 的分解(Smax) 的分解(Smaxxx) 的分解结果) 的分解(Sil=)的分解(Sil=)的分解)的分解(Smax) ) 直成的分解) 的分解(S)。