메뉴 건너뛰기




Volumn 80, Issue 5, 2009, Pages

Magnetic model for the ordered double perovskites

Author keywords

[No Author keywords available]

Indexed keywords


EID: 70249084125     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.80.054411     Document Type: Article
Times cited : (36)

References (27)
  • 8
    • 41449108708 scopus 로고    scopus 로고
    • 10.1103/PhysRevB.77.115101
    • K. W. Lee and W. E. Pickett, Phys. Rev. B 77, 115101 (2008). 10.1103/PhysRevB.77.115101
    • (2008) Phys. Rev. B , vol.77 , pp. 115101
    • Lee, K.W.1    Pickett, W.E.2
  • 13
    • 70249108901 scopus 로고    scopus 로고
    • In this paper we will refer to this state as a ferromagnetic state, considering the order of the core spins.
    • In this paper we will refer to this state as a ferromagnetic state, considering the order of the core spins.
  • 19
    • 33646757213 scopus 로고    scopus 로고
    • 10.1140/epjb/e2006-00173-2
    • S. Kumar and P. Majumdar, Eur. Phys. J. B 50, 571 (2006). 10.1140/epjb/e2006-00173-2
    • (2006) Eur. Phys. J. B , vol.50 , pp. 571
    • Kumar, S.1    Majumdar, P.2
  • 20
    • 24044516571 scopus 로고    scopus 로고
    • 10.1140/epjb/e2005-00261-9
    • S. Kumar and P. Majumdar, Eur. Phys. J. B 46, 315 (2005). 10.1140/epjb/e2005-00261-9
    • (2005) Eur. Phys. J. B , vol.46 , pp. 315
    • Kumar, S.1    Majumdar, P.2
  • 21
    • 25044446672 scopus 로고
    • 10.1103/PhysRevB.36.3791
    • M. Takahashi, Phys. Rev. B 36, 3791 (1987). 10.1103/PhysRevB.36.3791
    • (1987) Phys. Rev. B , vol.36 , pp. 3791
    • Takahashi, M.1
  • 23
    • 70249110874 scopus 로고    scopus 로고
    • The x axis in this figure actually represents (3-n) rather than n. This is done to avoid numerical problems associated with the calculation of the exchange on the low filling side due to the singularity at μ=Δ. For small Δ, of course, there is an explicit symmetry between the two sides but for larger Δ, the ferromagnetic phase seems to have a larger extent on the high filling side compared to the low filling one.
    • The x axis in this figure actually represents (3-n) rather than n. This is done to avoid numerical problems associated with the calculation of the exchange on the low filling side due to the singularity at μ=Δ. For small Δ, of course, there is an explicit symmetry between the two sides but for larger Δ, the ferromagnetic phase seems to have a larger extent on the high filling side compared to the low filling one.
  • 24
    • 13944252493 scopus 로고    scopus 로고
    • 10.1103/PhysRevB.70.224438
    • A. Taraphder and F. Guinea, Phys. Rev. B 70, 224438 (2004). 10.1103/PhysRevB.70.224438
    • (2004) Phys. Rev. B , vol.70 , pp. 224438
    • Taraphder, A.1    Guinea, F.2


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.