According to the results of the temperature dependencies of the intensity, linewidth and resonance field, we conclude that the peak at T(subscript M2) is a transition of antiferromagnetism.
通过对铁磁共振线
、线宽和共振场与温依赖关系讨论，我们得出T(下
M2)附近峰对应着体系反铁磁转变。
According to the results of the temperature dependencies of the intensity, linewidth and resonance field, we conclude that the peak at T(subscript M2) is a transition of antiferromagnetism.
通过对铁磁共振线、线宽和共振场与温依赖关系讨论，我们得出T(下M2)附近峰对应着体系反铁磁转变。
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