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CeFe_(2-x)In_x合金磁性研究与CeFe_(1.95)In_(0.05)合金磁相变临界参数分析
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作者 陈湘 赵明骅 《物理学报》 SCIE EI CAS CSCD 北大核心 2018年第19期275-285,共11页
通过等温磁化曲线和等磁场变温曲线测量与标度理论,系统研究了CeFe_(2-x)In_x合金的磁性和CeFe_(1.95)In_(0.05)合金的磁相变临界参数.结果表明:用2.5 at.%的铟替代CeFe_2合金中的铁并不能使合金中的反铁磁态在低温下完全稳定,低场下在2... 通过等温磁化曲线和等磁场变温曲线测量与标度理论,系统研究了CeFe_(2-x)In_x合金的磁性和CeFe_(1.95)In_(0.05)合金的磁相变临界参数.结果表明:用2.5 at.%的铟替代CeFe_2合金中的铁并不能使合金中的反铁磁态在低温下完全稳定,低场下在2—80 K均能观察到反铁磁相振荡; CeFe_2与CeFe_(1.95)In_(0.05)合金的顺磁-铁磁二级相变居里温度均在230 K附近;在0—5 T磁场范围内, CeFe_(1.95)In_(0.05)合金居里温度处的最大磁熵变为3.13 J/(kg·K),相对制冷量为151.3 J/kg.通过不同方法得到的具有高度自洽性的磁相变标度临界参数均表明CeFe_(1.95)In_(0.05)合金的磁相互作用可以用基于短程相互作用的3D-Ising模型来描述. 展开更多
关键词 CeFe1.95In0.05合金 磁热性能 标度理论 临界参数
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Er-Fe-In三元系773 K等温截面相图与Er_(12)Fe_(2)In_(3)化合物磁性
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作者 陈湘 倪超 段宇静 《中国有色金属学报》 EI CAS CSCD 北大核心 2021年第6期1559-1567,共9页
本文以X射线粉末衍射谱、等温磁化曲线和等磁场变温曲线为基础,研究了Er-Fe-In三元系773 K等温截面相图与Er_(12)Fe_(2)In_(3)化合物的磁性。结果表明:该三元系中只有一个三元化合物Er_(12)Fe_(2)In_(3)存在,且二元化合物与三元化合物... 本文以X射线粉末衍射谱、等温磁化曲线和等磁场变温曲线为基础,研究了Er-Fe-In三元系773 K等温截面相图与Er_(12)Fe_(2)In_(3)化合物的磁性。结果表明:该三元系中只有一个三元化合物Er_(12)Fe_(2)In_(3)存在,且二元化合物与三元化合物均未观察到固溶现象。化合物的磁性研究表明,低场下Er_(12)Fe_(2)In_(3)合金分别在10 K出现了一个正常反铁磁-顺磁相变以及在36 K出现一个类似反铁磁-顺磁的磁相变。磁化过程中存在磁场诱导反铁磁-铁磁相变,在2 T以上磁场中该合金只在居里温度约12 K时存在铁磁-顺磁相变。在0~5 T磁场范围内,合金的最大等温磁熵变(-ΔSMax)为9.9 J/(kg·K),在等温磁熵变最大值半高宽ΔTcycl=38.0 K(5.7~43.7 K)范围内,其相对制冷能力为278.1 J/kg。 展开更多
关键词 Er-Fe-In相图 RE_(3×4)(T_(2))_(4-x)X_(x)相 变磁相变 磁热效应
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Investigation on the 773K isothermal section of Ho-Ni-Si ternary phase diagram by X-ray powder diffraction and magnetic property of Ho3NiSi2 alloy 被引量:1
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作者 Xiang Chen Jixin Gong +2 位作者 Jiaojiao Luo Wenxuan Yang Xian Qing 《Journal of Rare Earths》 SCIE EI CAS CSCD 2020年第9期969-975,I0002,共8页
The isothermal section of the Ho-Ni-Si system at 773 K was constructed by X-ray powder diffraction(XRD)in this work.The system contains sixteen known type structure compounds TiNiSi-type HoNiSi,BaAl4-type HoNi2Si2,CeN... The isothermal section of the Ho-Ni-Si system at 773 K was constructed by X-ray powder diffraction(XRD)in this work.The system contains sixteen known type structure compounds TiNiSi-type HoNiSi,BaAl4-type HoNi2Si2,CeNiSi2-type HoNiSi2,U1Co3Si5-type Ho2Ni3Si5,SmNiGe3-type HoNiSi3,Ce3 Ni6Si2-type Ho3Ni6Si2,ThMn12-type HoNi10Si2,YPd2Si-type HoNi2Si,YNi5Si3-type HoNi5Si3,YNi4Si-type HoNi4Si,Gd3NiSi2-type Ho3NiSi2,YNi6Si6-type HoNi6Si6.AlB2-type Ho2NiSi3,AlB2-type Ho3Ni2Si4,AlB2-type Ho4NiSi7,Gd3Ru4Al12-type Ho8Ni31Si11,and one unknown type structure compound Ho5Ni2Si3.At the same time,one unknown structure new phase Ho37Ni3Si60 was observed.In ternary compounds,Ho2NiSi3 and Ho4NiSi7 have the solid solution phenomena;the solid solution ranges are about Ho33.3Ni18.7-9.7Si-48.0-57.0 and Ho33.Ni-8.3-2.6Si-58.3-64.1,respectively.At the same time,quasi-binary solid solutions were detected at 773 K for Ho2Ni17,HoNi5,Ho2Ni7,HoNi3,HoNi2,HoNi,HoSi.Other binary compounds of the Ho-Ni-Si system do not show any visible solubility.The magnetic property studies show that Ho3NiSi2 compound has two successive magnetic phase transitions in a low field:a spinreorientation transition at TSR=10 K and a second order ferromagnetic(FM)-paramagnetic(PM)transition at Tc=37 K. 展开更多
关键词 Ternary alloys Ho-Ni-Si phase diagram Solid solution X-ray diffraction Rare earths
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Experimental isothermal section phase diagram of Ho-Fe-In at 773 K and magnetic properties of Ho_(12)Fe_(2.08)In_(2.92) alloy 被引量:1
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作者 Xiang Chen Chao Ni 《Rare Metals》 SCIE EI CAS CSCD 2021年第4期987-994,共8页
The isothermal section of the Ho-Fe-In system at 773 K has been constructed by X-ray powder diffraction.One known structure ternary compound Er_(12)Fe_(2) In_(3)-type Ho_(12)Fe_(2) In_(3) has been confirmed.At the sam... The isothermal section of the Ho-Fe-In system at 773 K has been constructed by X-ray powder diffraction.One known structure ternary compound Er_(12)Fe_(2) In_(3)-type Ho_(12)Fe_(2) In_(3) has been confirmed.At the same time,solid solutions are not detected in Ho-Fe-In system at 773 K.The magnetic transition and magnetocaloric effect of Ho_(12)Fe_(2.08)In_(2.92) alloy with Er_(12)Fe_(2) In_(3)-type structure were investigated by magnetic susceptibility and isothermal magnetization measurements.One normal antiferromagnetic-paramagnetic transition and another abnormal one are discovered at 18 and 76 K in ground state,respectively.Owing to a first-order field-induced metamagnetic transition(antiferromagnetic-ferromagnetic) at/below the Neel temperature of 18 K),the negative entropy changes are observed at corresponding temperature.There is only a second-order ferromagnetic-paramagnetic transition near Curie temperature(TC),the maximum entropy change(Δ_(Smax)) values are-6.14 J·kg^(-1)·K^(-1) at 3 K and 7.88 J·kg^(-1)·K^(-1) at 28 K in a field range of 0-7 T.The reversible relative cooling power corresponding to negative entropy change can reach about 600 J·kg^(-1) in an wide operating temperature region Δ_(Tcycl)=74 K from 16 to90 K,which suggests that Ho_(12)Fe_(2.08)In_(2.92) could be a potential material for magnetic refrigeration in the corresponding temperature range. 展开更多
关键词 Re_(3(x+y))(T2)_(x)X_(y)phase Metamagnetic transition Magnetothermal properties Ho-Fe-In alloy
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Dy_(13.60)Ni_(3.34)In_(3.06)合金磁相变与磁热性能研究
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作者 陈湘 王小蝶 +1 位作者 袁野 曾玲凤 《中国稀土学报》 EI CAS CSCD 北大核心 2023年第5期888-893,I0002,共7页
基于室温XRD和磁化强度随温度和磁场变化的实验数据,研究了Dy_(13.60)Ni_(3.34)In_(3.06)合金的相结构和磁相变与磁热效应。结果表明,室温下该合金为Lu_(14)Co_(2)In_(3)型结构近单相,由于合金中Dy原子有7个非等效Wyckoff占位而导致Dy^(... 基于室温XRD和磁化强度随温度和磁场变化的实验数据,研究了Dy_(13.60)Ni_(3.34)In_(3.06)合金的相结构和磁相变与磁热效应。结果表明,室温下该合金为Lu_(14)Co_(2)In_(3)型结构近单相,由于合金中Dy原子有7个非等效Wyckoff占位而导致Dy^(3+)的磁矩呈非共线,合金表现出较为复杂的磁结构和磁相变,除T_(C)=22 K的FM-PM转变和其他温度下未知磁相变外,基于磁化率实部和虚部峰值对应温度对频率的敏感性,证实在T_(g)=16 K附近存在磁自旋玻璃态与铁磁态之间的转变。高温范围(130~300 K)磁化率及其倒数的居里外斯公式拟合结果显示居里外斯温度为-28.66 K,合金中Dy^(3+)粒子的顺磁有效磁矩为μ_(eff)=10.86μB,同期望值μ_(eff)=g( J (J+1))1/2=10.64μB基本一致,Ni原子为非磁性或极弱磁性。Dy14Ni3In3合金磁场响应性较差,铁磁态分子的有效磁矩远低于顺磁分子有效磁矩,在50 kOe磁场下合金的低温(2 K)饱和磁矩仅为26.31μB/f.u或1.93μB/Dy^(3+)。在磁热性能方面,合金在0~50 kOe磁场下,居里温度附近最大磁熵变-ΔS_(max)仅为-1.40 J·(kg·K)^(-1)。 展开更多
关键词 Dy_(14)Ni_(3)In_(3)合金 自旋玻璃 非线性磁矩 磁热效应
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