中文摘要：

研究了Tb掺杂对双层锰氧化物La_（4/3）Sr_（5/3）Mn_2O_7磁熵变和电输运性质的影响.样品采用传统固相反应法制备,两样品的名义组分可以表示为（La_（1-x）Tb_x）_（4/3）Sr_（5/3）Mn_2O_7（x=0,0.025）,磁场为7 T时的最大磁熵变？S_M分别为-4.60 J/（kg·K）和-4.18 J/（kg·K）.比较后发现,Tb元素的掺杂使得最大磁熵变值减小,但同时增大了相对制冷温区.电性测量结果表明,x=0.025的样品在高温区的导电机制可以用小极化子模型解释,与母体三维变程跳跃模型不同;当温度降低至三维长程铁磁有序温度（T_c~（3D））附近时,掺杂样品发生金属绝缘相变;掺杂后样品在T_c~（3D）附近,磁电阻取得极大值（约为56%）,表明是本征磁电阻效应.

英文摘要：

The magnetic transition process in double-layer perovskite manganites is rather different from that in the coun- terpart compound with standard perovskite structure. In this paper, the magnetic phases below room temperature as well as the order of magnetic phase transition in terbium （Tb） doped La4/3Sr5/3Mn207 are studied by analyzing the magnetization curves, including thermal hysteresis, magnetic entropy change and its universal curve. The electrical conductivities with and without applied magnetic field are also discussed. Both the undoped and the doped samples （Lal-xTb）4/3Srs/3Mn207 （x = 0, 0.025） are prepared through the conventional solid-state reaction of mixed La203, Tb203, MnCO3 and SrCO3 whose purities are all higher than 99.9%. The mixture is calcined twice at 1000 ℃ for 12 h. Subsequently, the compactly compressed tablet of the calcined mixture is sintered in air at 1350 ℃ for 24 h. The data of X-ray diffraction show that the crystallographic structures of both samples are in the Sr3Ti2OT-type tetragonal phase with the space group I4/mmm. The refinement result indicates that the smaller radius of doped Tb3＋ reduces all three lattice parameters as well as the c/a ratio, which is attributed to the preferential occupation of Tb3＋on the R site in rocksalt layer instead of the P site in perovskite layer. The temperature and field dependence of magnetization M（T, H）, are recorded using the vibrating sample mag- netometer of physical property measurement system （Quantum Design）. Upon reducing the temperature, both samples exhibit two magnetic phase transitions from the paramagnetic phase at high temperature to the two-dimensional short- range-ordered ferromagnetic state at the intermediate temperature, and finally the three-dimensional long-range-ordered antiferromagnetic state at low temperature. The zero-field-cooling and field-cooling curves display the characteristics of spin-glass behavior which may be due to the competition between B-site ferromagnetic and antiferromagnet