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首页> 外文期刊>Journal of Experimental and Theoretical Physics >Special properties of overdoped 123 compounds; Cu(2) NQR and Tm NMR of TmBa2Cu30x at low temperatures
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Special properties of overdoped 123 compounds; Cu(2) NQR and Tm NMR of TmBa2Cu30x at low temperatures

机译:过量掺杂的123种化合物的特殊性能; TmBa2Cu30x在低温下的Cu(2)NQR和Tm NMR

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The 169Tm NMR and 63Cu(2) NQR spectra, as well as the spin-spin and spin-lattice relaxation of thulium nuclei, are studied in a series of oriented TmBa2Cu30( powders with an oxygen content x from 6.9 to 7.0 (in Ax=0.02 intervals). All the experiments are performed by the spin-echo technique at liquid helium temperatures. Additional measurements of the diamagnetic susceptibility at 1 kHz in a field H_1-1 Oe perpendicular to the c crystallographic axis show that the maximum critical temperature 7"c(onset)=92.2 K is achieved in the samples with j:=6.90-6.92. The results of the experiments with the overdoped compounds (j:^6.94) are consistent with the "ribbon model" of the quasi-one-dimensional spin and charge correlations in CuO2 planes [O. N. Bakharev, M. V. Eremin, and M. A. Teplov, JETP Lett. 61,515 (1995)]. A "disappearance" of 1/3 of the intensity of the Cu(2) NQR signal is discovered when the oxygen content is decreased from 7.00 to 6.98. Phase separation is discussed as a possible cause of this effect. It is theorized that in layers with a reduced concentration of holes in the CuO2 planes, the mobility of the holes decreases, the fluctuations of the strong internal fields from the spins of the Cu2+ ions slow, and the spin echo of the Cu(2) nuclei is not observed due to acceleration of the transverse nuclear relaxation.
机译:在一系列定向的TmBa2Cu30(粉末中的氧含量x从6.9到7.0(Ax ==)中研究了169Tm NMR和63Cu(2)NQR光谱以及th核的自旋-自旋和自旋晶格弛豫0.02个间隔)。所有实验均在液氦温度下通过自旋回波技术进行。在垂直于c晶轴的H_1-1 Oe场中,在1 kHz处的抗磁化率的其他测量结果表明,最大临界温度为7“ j:= 6.90-6.92的样品中c(起始)= 92.2 K.掺杂化合物(j:^ 6.94)的实验结果与准一维的“色带模型”一致CuO2平面中的自旋和电荷相关性[ON Bakharev,MV Eremin,and MA Teplov,JETP Lett。61,515(1995)]。氧含量从7.00降低至6.98。造成这种影响的原因。从理论上讲,在CuO2平面中空穴浓度降低的层中,空穴的迁移率降低,来自Cu2 +离子自旋的强内部场的波动变慢,并且Cu(2)的自旋回波由于横向核弛豫的加速,未观察到核。

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