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非晶Fe73.5Cu1Nb3Si13.5B9合金激光纳米化的超精细结构研究
引用本文:陈岁元,刘常升,李慧莉,崔 彤. 非晶Fe73.5Cu1Nb3Si13.5B9合金激光纳米化的超精细结构研究[J]. 物理学报, 2005, 54(9): 4157-4163
作者姓名:陈岁元  刘常升  李慧莉  崔 彤
作者单位:东北大学材料与冶金学院,沈阳 110004
基金项目:国家自然科学基金(批准号:50274028)和沈阳市科技计划项目(1032040-1-01)资助的课题.
摘    要:在CO2激光功率为50—300W、扫描速度为20mm/s、激光散光斑为20mm照射条件下 ,诱导非 晶Fe735Cu1Nb3Si135B9带中发生结构重组,产生定量纳米α-F e(Si)晶相形成双相组织结构材料. 利用穆斯堡尔谱研究了非晶Fe735C u1Nb3Si135B9合金激光纳米化的 超精细结构. 实验结果表明,激光诱导非晶 Fe735Cu1Nb3Si135B 9纳米化后,其超精细磁场的分布随 着激光功率变 化由单峰向双峰变化,在高功率辐照时, 出现了双峰分布,并且峰位向高场移动. 高激光 功率辐照非晶Fe735Cu1Nb3Si135B9合金纳米晶化相有四种超精细结 构,即2个超精细磁场较小的初晶相和2个超精细磁场较大的纳米晶化相. 其中超精细磁场较 大(17—25MA/m)的α-Fe(Si)相为DO3结构.关键词:激光纳米晶α-Fe(Si)735Cu1Nb< sub>3Si135B9')" href="#">非晶Fe735Cu1Nb< sub>3Si135B9超精细结构超精细磁场

关 键 词:激光  纳米晶α-Fe(Si)  非晶Fe735Cu1Nb< sub>3Si135B9  超精细结构  超精细磁场
文章编号:1000-3290/2005/54(09)/4157-07
收稿时间:2005-11-30
修稿时间:2005-11-302004-12-21

Hyperfine stucture during nanocrystallization of amorphous Fe73.5Cu1Nb3Si13.5B9 alloy irradiated by laser
Chen Sui-Yuan,Liu Chang-Sheng,Li Hui-Li and Cui Tong. Hyperfine stucture during nanocrystallization of amorphous Fe73.5Cu1Nb3Si13.5B9 alloy irradiated by laser[J]. Acta Physica Sinica, 2005, 54(9): 4157-4163
Authors:Chen Sui-Yuan  Liu Chang-Sheng  Li Hui-Li  Cui Tong
Abstract:The material composed of a definite amount of nanocrystalline phase α-Fe(Si) with a double-phase structure was produced by laser irradiation on the amorphous Fe735Cu1Nb3Si135B9< /sub> alloy with a laser power ranging from 50 to 300W, scanning speed 20mm/s, laser beam spot 20mm. Hyperfine structures of the nanocrystallized samples were analyzed by Mssbauer spectra. Experimental result shows that after the CO2 laser irradiated on the amorphous allo y Fe735Cu1Nb3Si135B 9, its hyperfine magnetic field dist ribution transformed from a single peak to double peaks with the change of laser power. When irradiated at a high laser power, it formed a double-peak structure and the peaks moved to a high field position. Nanocrystallization of amorphous Fe7 35Cu1Nb3Si135B9 ir radiated by a higher laser power produces fou r hyperfine structures, i.e. two primary crystal phases with relatively small hy perfine magnetic field and two nanocrystalline phases with a relatively large hy perfine magnetic field. The major crystal phase is the α-Fe(Si) phase of DO3 whose hyperfine magnetic field is comparatively larger (17—25MA/m).
Keywords:laser  nanocrystal α-Fe(Si)  amorphous Fe735Cu1Nb3Si135B9 alloy  hyperfine structures  hyperfine magnetic field
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