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Volumn 70, Issue 4, 2001, Pages 1105-1116

Study on the magnetic and transport properties of low density carrier ferromagnetic semiconductors

Author keywords

Magnetic polaron; Magnetic semiconductor; Magnetization

Indexed keywords


EID: 0035645763     PISSN: 00319015     EISSN: None     Source Type: Journal    
DOI: 10.1143/JPSJ.70.1105     Document Type: Article
Times cited : (15)

References (69)
  • 1
    • 0033204760 scopus 로고    scopus 로고
    • For recent comprehensive review see for example, T. Ohno: J. Magn. Magn. Mater. 200 (1999) 110.
    • (1999) J. Magn. Magn. Mater. , vol.200 , pp. 110
    • Ohno, T.1
  • 49
    • 0039842768 scopus 로고    scopus 로고
    • Master Thesis Tohoku University, (unpublished)
    • K. Nishizawa: Master Thesis (Tohoku University, 1999) (unpublished)
    • (1999)
    • Nishizawa, K.1
  • 51
    • 24244473764 scopus 로고    scopus 로고
    • Proc. PASPS200, September 13-15, Sendai, (in press)
    • O. Sakai and S. Suzuki: Physica E (Proc. PASPS200, September 13-15, Sendai, 2000) (in press).
    • (2000) Physica E
    • Sakai, O.1    Suzuki, S.2
  • 59
    • 0040435773 scopus 로고    scopus 로고
    • note
    • Mn ions do not exit on all sites in the diluted semiconductor systems, while magnetic ions locate on all sites in Euchalcogenides. The result of the present calculation is not directly applicable to actual diluted semiconductor systems. The diagonalization of electronic states uses almost all of the computation time. Even when we use a alloy model by reducing magnetic ion sites, the electronic diagonalization part is not reduced. As the first step of study, we use the present model.
  • 62
    • 0041029693 scopus 로고    scopus 로고
    • note
    • Usually it is not easy to obtain q(ψ → ψ′). In the present calculation, it has a simple form given by eq. (2.8) because we choose a simple method for the generation of the first step.
  • 65
    • 0041029695 scopus 로고    scopus 로고
    • note
    • As seen from the inset of Fig. 8, the level splitting ∼ 0.4 due to the finite size calculation is larger than A = 0.1. In the strict sense we should use much larger value for A. However, the current matrix is non-zero only in the same group when the effect of the potential fluctuation is weak. So we can get smooth curves even when we put A = 0.1.
  • 66
    • 0040435771 scopus 로고    scopus 로고
    • note
    • When the electron is bounded not tightly in the square, η will be reduced to near 1/2.
  • 67
    • 0041029644 scopus 로고    scopus 로고
    • note
    • 15)
  • 68
    • 0040435723 scopus 로고    scopus 로고
    • note
    • It has been shown in ref. 35 by the density functional approach that the inhomogeneous electron density state is not so highly suppressed even when one considers the long range Coulomb interaction.
  • 69
    • 0039251124 scopus 로고    scopus 로고
    • note
    • The mode corresponding to the rotation of total spins of magnetic polaron will of course have very low energy. But other modes which cause the short range spatial change of electron spin direction, with the comparable to the magnetic polaron state, will have not so low energy.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.