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Effect of Yttrium Doping on Magnetic Properties and Magnetic Entropy Change of Bilayered Perovskite La 1.3 Sr 1.7 Mn 2 O 7
Journal of Low Temperature Physics ( IF 2 ) Pub Date : 2020-05-07 , DOI: 10.1007/s10909-020-02457-8
Fengze Cao , Yi Lu , Hongye Wu , Bao Xu , Xiang Jin , Jianjun Zhao , Xiaodong Sun

La1.3−xYxSr1.7Mn2O7 (x = 0, 0.025) samples are prepared by the conventional solid-state reaction. X-ray diffraction spectrum reveals that the samples are in the Sr3Ti2O7-type tetragonal phase with the space group I4/mmm. By decreasing the temperature, two samples exhibit the paramagnetic phase at high temperatures to two-dimensional short-range-ordered ferromagnetic states at the intermediate temperatures and finally three-dimensional long-range-ordered ferromagnetic states. Furthermore, the doped sample also demonstrates antiferromagnetic ordering in the low-temperature region. The Arrott curve and calibration curve indicate that the sample behaves as a first-order phase transition. When the applied magnetic field is 6 T, the maximum magnetic entropy change (\(\Delta S_{M}\)) occurs in the two samples in the vicinity of the three-dimensional ordered temperature (T3Dc), and the value of \(\Delta S_{M}\) for the two samples reaches—4.81 J/kg K and—3.82 J/kg K, respectively. In addition, the relative cooling power is 108 J/kg and 112.2 J/kg at \(\mu_{0} H = 3\;T\), respectively. Although the doping of Y reduces T3Dc, \(\Delta S_{M}\) and the first-order phase transition character, the relative cooling power is enhanced, thus indicating its potential to realize magnetic refrigeration in high-temperature regions (T > 77 K).

中文翻译:

钇掺杂对双层钙钛矿La 1.3 Sr 1.7 Mn 2 O 7的磁性和磁熵变的影响

通过传统的固态反应制备La 1.3− x Y x Sr 1.7 Mn 2 O 7x  = 0,0.025)样品。X射线衍射光谱表明样品位于Sr 3 Ti 2 O 7中型四方相,空间群为I4 / mm。通过降低温度,两个样品在高温下表现出顺磁性相,在中间温度下呈现二维短程铁磁态,最后呈现三维长程铁磁态。此外,掺杂样品在低温区域也表现出反铁磁有序性。Arrott曲线和校准曲线表明样品表现为一阶相变。当施加的磁场为6 T时,在三维有序温度(T 3D c)附近的两个样本中发生最大磁熵变(\(\ Delta S_ {M} \)),并且的\(\德尔塔S_ {M} \)对于这两个样品,分别达到-4.81 J / kg K和-3.82 J / kgK。另外,在\(\ mu_ {0} H = 3 \; T \)时,相对冷却功率分别为108 J / kg和112.2 J / kg 。尽管Y的掺杂降低了T 3D c\(\ Delta S_ {M} \)和一阶相变特性,但相对冷却功率得到了增强,从而表明了其在高温区域实现磁制冷的潜力(T  > 77 K)。
更新日期:2020-05-07
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