Abstract
The forced volume magnetostriction ∂ω⁄∂h and the electronic contribution to the bulk modulus Be in FeNi alloy are calculated with use of the Libemian-Pettifor virial theorem and the full single site approximation in the 2-field functional integral method in order to clarify the origin of the Invar effect. It is shown that the large ∂ω⁄∂h in the Invar region is caused by the large temperature variation of the derivative of 〈mFe2〉 (the amplitude of the Fe local moment) with respect to the field h, the softening of the bulk modulus by the increase of the volume change of 〈mFe2〉. It is found that the minimum in Be occurs below Tc because of the suppression of the temperature variation of 〈mFe2〉. The high-field susceptibility, the paramagnetic spin susceptibility and ∂Tc⁄∂P are also calculated.