摘要
本文详细地叙述了α-Fe中^(57)Fe核处的超精细磁场(H_n)的来源,并用穆斯堡尔法测量了不同温度下^(57)Fe核处的超精细磁场H_n(T),同时从理论上并借助于计算机求解出不同温度(T),不同角量子数(J)下α-Fe的饱和磁化强度M_1(T),最后用计算机最小二乘法拟合得到,H_n(T)与M_J(T)之间符合修正的马歇尔方程,即: H_n(T)=A_0(1-αT^2)·M_J(T) 其中J=1/2,A_o,α为常数,且A_0=0.193016,α=2.472×10^(-7)
The origin of hyperfine field(H_n)within the ^(57)Fe nucleus in α-Fe has been fully discussed and the H_n (T)under different temperature(T)have been measured by Mossbauer spectroscopy as well. Meanwhile the saturation magnetization [M_I (T)]of different angular quantum numbers (J)and different tomperatttre(T) are calculated with a computer. It is found from the least-square fitting with a computer that the correlation between H_n (T) and M_J (J) obeys the corrected Marshall's equation, that is: H_n (T)=A_0(1-αT^2)M_J (T) Where J=1/2, A_0 and α are constants with A_0=0.193016 and α=2.472×10^(-7)
出处
《物理测试》
CAS
1993年第3期113-119,共7页
Physics Examination and Testing
关键词
自发磁化强度
穆斯堡尔学
Α-FE
spontaneous magnetization
Mossbauer spectroscopy
α-Fe