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Volumn 34, Issue 3, 1986, Pages 1784-1791

Ferromagnetic phases of bcc and fcc Fe, Co, and Ni

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EID: 0001671590     PISSN: 01631829     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevB.34.1784     Document Type: Article
Times cited : (670)

References (26)
  • 6
    • 33144457506 scopus 로고
    • In this work we only consider ferromagnetic order. The fixed spin-moment method has not yet been extended to the more complicated problem of antiferromagnetic order.
    • (1984) J. Phys. F , vol.14 , pp. L129
    • Schwarz, K.1    Mohn, P.2
  • 18
    • 84926544986 scopus 로고    scopus 로고
    • The model of magnetic behavior used here only includes spin magnetization, which requires the moment to be parallel or antiparallel to the applied magnetic field. Negative fields, i.e., fields opposite to the direction of the moment, can be tolerated in the ferromagnetic state because the model provides an energy barrier to reversing the magnetization direction. When a threshold negative field is exceeded, the system will abruptly assume the opposite magnetization. Mechanisms outside the model, e.g., rotation of the spin direction, may permit spin reversal at smaller threshold fields.
  • 19
    • 84926576788 scopus 로고    scopus 로고
    • At the crossing point of the fcc and bcc curves in Fig. 9, which is where a transition to the fcc state would take place if the transition occurred at constant volume, the pressure in the bcc state is 140 kbar. The (extrapolated) experimental phase diagram for Fe indicates a transition at T=0 from bcc to hcp (alpha to epsilon) at about 140 kbar;
  • 22
    • 84926531406 scopus 로고    scopus 로고
    • J. Kübler, in the Proceedings of the Institute von Laue-Langevin Workshop on 3d Metallic Magnetism, Grenoble, France, 1983, edited by D. Givord and K. Ziebeck (unpublished).


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.