首页> 外文期刊>Physical Review, B. Condensed Matter >MAGNETIZATION STUDY OF GAMMA-FE80-XNIXCR20 (14-LESS-THAN-OR-EQUAL-TO-X-LESS-THAN-OR-EQUAL-TO-30) ALLOYS TO 20 T
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MAGNETIZATION STUDY OF GAMMA-FE80-XNIXCR20 (14-LESS-THAN-OR-EQUAL-TO-X-LESS-THAN-OR-EQUAL-TO-30) ALLOYS TO 20 T

机译:GAMMA-FE80-XNIXCR20(14少或等于到X少或相等到30)合金的磁化强度至20 T

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Very-high-field (0-20 T) dc-magnetization measurements M(H) and M(T) between 4.2-60 K and 19-700 K, respectively, have been carried out on substitutionally disordered gamma-Fe80-xNixCr20 (14 less than or equal to x less than or equal to 30), austenitic stainless steel alloys having a wide variety of exotic magnetic phases. Distinct functional relationships M(H) have been found in different magnetic phases below their respective transition temperatures. In a ferromagnetic (FM) alloy with x=30, contributions from long-wavelength spin-wave and Stoner single-particle excitations have been found in the temperature-dependent demagnetization process. In the light of the Rhodes-Wohlfarth criterion, this alloy is found to be a weak-itinerant FM. For the alloys with x=26 and 23 (mixed or reentrant phase) the coexistence of long-range FM ordering along with spin-glass (SG) freezing has been established supporting the Gabay-Toulouse model. For x=21 and 19 (SG), the field-dependent magne tization (after scaling) falls on a single universal curve, which implies the same kind of response dynamics of the frozen spins. For an antiferromagnetic (AFM) alloy with x=14, a spin-flop transition has been observed at 1 T due to the canting of the AFM spins in the strong external magnetic field. The long-range AFM structure of this alloy is found to be of type 1. [References: 92]
机译:在取代无序的γ-Fe80-xNixCr20上进行了分别在4.2-60 K和19-700 K之间的高磁场(0-20 T)直流磁化测量M(H)和M(T)( 14小于或等于x小于或等于30),奥氏体不锈钢合金具有多种奇特的磁相。已经在低于其各自的转变温度的不同磁相中发现了不同的功能关系M(H)。在x = 30的铁磁(FM)合金中,在与温度相关的退磁过程中发现了长波自旋波和Stoner单粒子激发的贡献。根据Rhodes-Wohlfarth准则,发现该合金为弱巡回调频。对于x = 26和23(混合相或折返相)的合金,已经建立了长程FM有序和自旋玻璃(SG)冻结的共存,从而支持了Gabay-Toulouse模型。对于x = 21和19(SG),取决于场的氧化(按比例缩放后)落在一条通用曲线上,这意味着冻结自旋的响应动力学类型相同。对于x = 14的反铁磁(AFM)合金,由于AFM自旋在强外部磁场中的倾斜,在1 T处观察到了自旋转变。该合金的远距离AFM结构为1型。[参考文献:92]

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