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SPIN DYNAMICS IN MESOSCOPIC SIZE MAGNETIC SYSTEMS - A H-1 NMR STUDY IN RINGS OF IRON (III) IONS

机译:介观尺寸磁系统中的自旋动力学-铁(III)离子环中的H-1 NMR研究

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Two magnetic molecular clusters containing almost coplanar rings of iron(III) ions with spin S = 5/2 have been investigated by H-1 NMR and relaxation measurements. The first system, which will be referred to as Fe6, is a molecule of general formula [NaFe6(OCH3)(12)(C17O4H15)(6)]+ClO4- or [NaFe6(OCH3)(12)(C15H11O2)(6)]+ClO4- or [LiFe6(OCH3)(12)(C15H11O2)(6)]+ClO4- while the second type of ring, denoted Fe10, corresponds to the molecule [Fe-10(OCH3)(20)(C2H2O2Cl)(10)]. The H-1 NMR linewidth is broadened by the nuclear dipolar interaction and by the dipolar coupling of the protons with the iron (III) paramagnetic moment. It is found that the nuclear spin-lattice relaxation rate, T-1(-1), of the proton is a sensitive probe of the Fe spin dynamics. In both clusters, T-1(-1) decreases with decreasing temperatures from room temperature, goes through a peak just below about 30 K in Fe6 and 10 K in Fe10, and it drops exponentially to very small values at helium temperature. The temperature dependence of the relaxation rate is discussed in terms of the fluctuations of the local spins within the allowed total spin configurations in the framework of the weak collision theory to describe the nuclear relaxation. We use the calculated energy levels for the Fe6 ring based on a Heisenberg Hamiltonian and the value of J obtained from the fit of the magnetic susceptibility to describe semiquantitatively the behavior T-1(-1) vs T. The exponential drop of T-1(-1) at low temperature is consistent with a nonmagnetic singlet ground state separated by an energy gap from the first excited triplet state. The values obtained for the gap energies are E-T/k = 12 K for Fe10 and E-T/k = 38 K for Fe6 which are almost twice as big as the values deduced from susceptibility measurements. At all temperatures the relaxation rate decreases with increasing magnetic field, i.e., NMR resonance frequency. This effect could be related to the long time persistence of the spin correlation functions typical of diffusive modes in low dimensional magnetic systems. It is argued that the data presented are a direct experimental study of spin dynamics in mesoscopic spin rings and should afford a test for exact analytical and/or numerical solutions. [References: 30]
机译:通过H-1 NMR和弛豫测量研究了两个磁性分子簇,它们的自旋S = 5/2几乎包含共平面的铁(III)离子环。第一个系统称为Fe6,是通式为[NaFe6(OCH3)(12)(C17O4H15)(6)] + ClO4-或[NaFe6(OCH3)(12)(C15H11O2)(6 )] + ClO4-或[LiFe6(OCH3)(12)(C15H11O2)(6)] + ClO4-,而第二种类型的环表示为Fe10,对应于分子[Fe-10(OCH3)(20)(C2H2O2Cl )(10)]。 H-1 NMR线宽通过核偶极相互作用和质子与铁(III)顺磁矩的偶极耦合而变宽。发现质子的核自旋晶格弛豫速率T-1(-1)是铁自旋动力学的灵敏探针。在这两个簇中,T-1(-1)随温度从室温降低而降低,在Fe6中经历的峰值略低于30 K,在Fe10中经历的峰值低于10 K,并且在氦气温度下呈指数下降至非常小的值。在描述核弛豫的弱碰撞理论的框架内,根据局部自旋在允许的总自旋构型内的波动讨论了弛豫率的温度依赖性。我们使用基于Heisenberg哈密顿量的Fe6环计算的能级和从磁化率拟合获得的J值来半定量地描述行为T-1(-1)与T。T-1的指数下降(-1)在低温下与非磁性单重态基态相符,该基态由能隙与第一激发三重态隔开。对于Fe10,获得的缝隙能量的值是E-T / k = 12 K,对于Fe6,获得的缝隙能量的值是E-T / k = 38 K,几乎是磁化率测量值的两倍。在所有温度下,弛豫率都随着磁场即NMR共振频率的增加而降低。这种影响可能与低维磁系统中扩散模式典型的自旋相关函数的长时间持续存在有关。据认为,所提供的数据是介观自旋环中自旋动力学的直接实验研究,应为精确的解析和/或数值解提供测试。 [参考:30]

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