Abstract

The spin-polarized band calculations for the iron nitrides, Fe 3N, Fe 4N and Fe 16N 2, have been performed with use of the LMTO-ASA method in the frame of local spin density functional formalism. The results show that the most distant Fe atoms from N have the largest magnetic moment. This can be ascribed mainly to the transfer of the down spin electrons, which is caused by the electronic interference due to the interstitial N atoms. The central role of the N atom is to bring about the large magnetic moments through the lattice expansion. Concurrently, the N atoms promote an itineracy of electrons and then in turn prevent the exchange-splitting. This leads to the behavior that the lower N concentration gives the larger magnetic moments. Quantitatively, the results are in fair agreement with the experimental results except for Fe 16N 2 whose measured value is considerably larger than the calculated result.

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