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Volumn 97, Issue 1, 1997, Pages 21-47

Spin wave and stability of the double exchange ferromagnet

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EID: 0009867954     PISSN: 0033068X     EISSN: None     Source Type: Journal    
DOI: 10.1143/PTP.97.21     Document Type: Article
Times cited : (19)

References (25)
  • 13
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    • L. M. Roth, J. Phys. Chem. Solids 28 (1967), 1549; J. Appl. Phys. 39 (1968), 474.
    • (1968) J. Appl. Phys. , vol.39 , pp. 474
  • 15
    • 0030557620 scopus 로고    scopus 로고
    • g-orbitals of Mn. Especially, the latter structure will be indispensable to reproduce the spin-wave dispersion quantitatively.
    • (1996) J. Phys. Soc. Jpn. , vol.65 , pp. 1174
    • Furukawa, N.1
  • 16
    • 8644267289 scopus 로고
    • There are several works on the double exchange ferromagnet, where the similarity with the Nagaoka ferromagnetic state is pointed out. K. Kubo, J. Phys. Soc. Jpn. 33 (1972), 929. N. Ohata, J. Phys. Soc. Jpn. 34 (1973), 343. K. Kubo, J. Phys. Soc. Jpn. 51 (1982), 782.
    • (1972) J. Phys. Soc. Jpn. , vol.33 , pp. 929
    • Kubo, K.1
  • 17
    • 0009244541 scopus 로고
    • There are several works on the double exchange ferromagnet, where the similarity with the Nagaoka ferromagnetic state is pointed out. K. Kubo, J. Phys. Soc. Jpn. 33 (1972), 929. N. Ohata, J. Phys. Soc. Jpn. 34 (1973), 343. K. Kubo, J. Phys. Soc. Jpn. 51 (1982), 782.
    • (1973) J. Phys. Soc. Jpn. , vol.34 , pp. 343
    • Ohata, N.1
  • 18
    • 0000512093 scopus 로고
    • There are several works on the double exchange ferromagnet, where the similarity with the Nagaoka ferromagnetic state is pointed out. K. Kubo, J. Phys. Soc. Jpn. 33 (1972), 929. N. Ohata, J. Phys. Soc. Jpn. 34 (1973), 343. K. Kubo, J. Phys. Soc. Jpn. 51 (1982), 782.
    • (1982) J. Phys. Soc. Jpn. , vol.51 , pp. 782
    • Kubo, K.1
  • 20
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    • T. Okabe, J. Phys. Soc. Jpn. 64 (1995), 3442; 65 (1996), 333A.
    • (1996) J. Phys. Soc. Jpn. , vol.65
  • 22
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    • 13 have assigned the first term of (5·2) to the energy loss of the up-spin electron. Our assignment, as a constant shift in the down-spin electron, is corroborated by the investigation in §7.1 on the single quasi-particle
    • 13) have assigned the first term of (5·2) to the energy loss of the up-spin electron. Our assignment, as a constant shift in the down-spin electron, is corroborated by the investigation in §7.1 on the single quasi-particle.


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