宽带脉冲DC SQUID核磁共振谱仪的研制

DC SQUID NMR在研究凝聚态体系 ,尤其在研究低温下量子有序态等方面是一项非常有价值的技术。文中描述了在带有宽带电子设备的商业 DC SQUID基础上建立起宽带脉冲谱仪 ,以及马鞍形激发线圈、采集线圈和低温装置的设计 ,并测量了铂样品在 4.2 Kz温度下的 NMR信号。     

Mn12-Ac磁性分子团簇单晶的热重-差热分析与结构转变

通过热重-差热分析(TG-DTA)，考察了Mn12-Ac磁性分子晶体从室温到270℃的热失重过程.结合x射线粉末衍射分析，认为在第一个失重阶段，即25—110℃，Mn12-Ac失去了处于团簇分子间隙的结晶乙酸和结晶水，同时失去了团簇分子中与4个Mn3+配位的4个H2O，Mn12-Ac单晶结构被破坏，但是团簇分子的基本结构依然存在；在第二个失重阶段，即180—230℃，Mn12-Ac转变为γ-Mn2O3，其中混有少量Mn3O4. 关键词： Mn12 分子团簇 热重-差热分析 x射线衍射     

Ti-50.8at%Ni马氏体相变中的电磁特性

研究Ti-50.8at%Ni合金在马氏体-奥氏体相变温度附近的电磁性质.由M-H曲线分析了传导电子的顺磁性以及少量局域电子引起的铁磁性.在M-T曲线中，降温曲线在180K附近有突降，升温曲线在230K附近有突升.在电阻率测量中，降温和升温的ρ-T曲线也有类似的突变.升温过程的质量热容c_p曲线在230K附近出现了由奥氏体相变引起的跳跃.这些实验结果表明，样品的马氏体相变温度约 关键词： TiNi合金 电磁性质 马氏体-奥氏体相变 质量热容     

重电子金属CeCu(6-x)Nix低温电阻与比热的研究

测量了重电子金属CeCu6-xNix(x=0,005,01,015,02)01K—250K的低温电阻和5K—70K低温比热,发现样品电阻的极大值温度随着掺Ni含量的增大而急剧下降,这一现象反映少数与Ni邻近的Ce离子在极低温下磁矩的加强和整个Ce离子点阵对导电电子相干散射的减弱.与此相反,低温电子比热系数γ在较低温度下近于常数,而在8K附近因有效质量变大而明显上升,但γ明显上升的温度,对Ni的含量却不敏感,表明绝大部分Ce离子的状况并未受到影响 关键词： 重费米子系统 低温比热 低温电阻     

重费密子系统CeCu6-xNix的极低温电阻研究

CeCu₆是一种重费密子系统,采用Ni替代Cu研究磁性原子掺杂的多晶样品CeCu_6-xNi_x(x=0.00,0.05,0.10,0.15,0.20)在极低温下的电阻随温度的变化规律.实验结果表明,随着Ni原子掺杂量的增加,电阻的规律发生变化.在500mK以下,x≈0.1的样品电阻与温度呈线性关系,表现出非费密液体行为,而其他样品皆为典型的费密液体,x≈0.1是其临界掺杂成分.对比用Au替代的情况,临界掺杂成分也是0.1,但Au掺杂是靠体积膨胀来改变合金的基态性质,而Ni掺杂则是因其磁性造成对合金基态性质的影响 关键词： 重费密子 临界掺杂 非费密液体     

Shape Dependence of Low-Temperature Magnetic Relaxation of Mn12Ac

We report the discovery that the low-temperature magnetic relaxation in Mn12Ac single crystals strongly depends on the shape of the samples. The relaxation time exhibits a minimum at the phase transition point between ferromagnetic and antiferromagnetie phases. The shape dependence is attributed to the dipolar interaction between molecular magnets.     

Anisotropic Applied Field Dependency of Two Successive Magnetic Transitions in LiCu2O2

The anisotropy of two successive transitions of the spin-ladder compound LiCu2O2 is studied by the specific heat （ C） under magnetic fields with H / / c and H / / ab （written as H^c and H^ab in the following） up to 14 T. The peak of specific heat at 24.5 K in zero field shifts to lower temperature when the field is increased and the magnitude of the peak is suppressed by the field. On the contrary, the peak of 22.5 K shifts to higher temperature, especially at 14 T. Its magnitude increases in the field of H^c, whereas it decreases in the field of H^ab. We calculate the entropy change between 21 K and 63 K. The different influence of the spin ordering by fields of different direction is obtained. Our experimental results suggest a mixed state between the long range incommensurate helimagnetic ground state and the higher-T short-range dimer liquid state. The temperature range of mixed state is shrunk with the increasing field. Possible mechanism is discussed.     

Magnetic Relaxation Study on Single Crystals of Nia Single-Molecule Magnets

The ac susceptibility of single crystals of Ni4 single-molecule magnets is measured by a compensation measurement setup. The magnetic relaxation time calculated from the peak of the out-phase component of the susceptibility fits the Arrhenius law well and gives an effective spin-flipping energy barrier of Uefr = 7.2 K. This value is fax below the classical activation energy barrier of U = 14 K, whereas it is close to the energy gap between the Sz= ±4 and S, = ±3 doublets, which indicates that quantum tunneling between the Sz = 3 and Sz = -3 states plays a key role in the magnetic relaxation. Therefore the relaxation process combines thermal activation and quantum tunneling. Also we deduce that the blocking temperature of Ni4 single-molecule magnets is lower than 0.3 K by extrapolating the relaxation time plot, which ensures that this single-molecule magnet material enters a long-range magnetic ordered state instead of a spin glass state at 0.91 K.     

Mn_(12)-Ac磁性分子团簇单晶的热重-差热分析与结构转变

通过热重 差热分析 (TG DTA) ,考察了Mn1 2 Ac磁性分子晶体从室温到 2 70℃的热失重过程 .结合x射线粉末衍射分析 ,认为在第一个失重阶段 ,即 2 5— 110℃ ,Mn1 2 Ac失去了处于团簇分子间隙的结晶乙酸和结晶水 ,同时失去了团簇分子中与 4个Mn3 配位的 4个H2 O ,Mn1 2 Ac单晶结构被破坏 ,但是团簇分子的基本结构依然存在 ;在第二个失重阶段 ,即 180— 2 30℃ ,Mn1 2 Ac转变为γ Mn2 O3,其中混有少量Mn3O4 .