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Volumn 84, Issue 5, 1998, Pages 2805-2814

Giant magnetoimpedance in a cylindrical magnetic conductor

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EID: 0042080777     PISSN: 00218979     EISSN: None     Source Type: Journal    
DOI: 10.1063/1.368421     Document Type: Article
Times cited : (168)

References (41)
  • 8
    • 85034282283 scopus 로고    scopus 로고
    • private communication
    • F. B. Humphrey (private communication).
    • Humphrey, F.B.1
  • 19
    • 0042750036 scopus 로고
    • See, for example, D. S. Rodbell, Physics 1, 279 (1965); C. Vittoria, R. C. Barker, and A. Yelon, J. Appl. Phys. 40, 1561 (1969); A. Yelon, G. Spronken, T. Buithieu, R. C. Barker, Y.-J. Liu, and T. Kobayashi, Phys. Rev. B 10, 1070 (1974).
    • (1965) Physics , vol.1 , pp. 279
    • Rodbell, D.S.1
  • 20
    • 0014480095 scopus 로고
    • See, for example, D. S. Rodbell, Physics 1, 279 (1965); C. Vittoria, R. C. Barker, and A. Yelon, J. Appl. Phys. 40, 1561 (1969); A. Yelon, G. Spronken, T. Buithieu, R. C. Barker, Y.-J. Liu, and T. Kobayashi, Phys. Rev. B 10, 1070 (1974).
    • (1969) J. Appl. Phys. , vol.40 , pp. 1561
    • Vittoria, C.1    Barker, R.C.2    Yelon, A.3
  • 23
    • 85034292687 scopus 로고    scopus 로고
    • note
    • In many reports and textbooks, e.g., Refs. 1, 2, and 20, (1+i) is used in the numerator of Eq. (5) in the text. Consistency then requires using Z = R-iX as the definition for the impedance and the use of modified Bessel functions for solutions for the fields.
  • 26
    • 11644272692 scopus 로고
    • A. Kurn, J. F. Cochran, and B. Heinrich, Can. J. Phys. 54, 1083 (1976); A. Yelon, Phys. Rev. B 19, 533 (1979).
    • (1979) Phys. Rev. B , vol.19 , pp. 533
    • Yelon, A.1
  • 27
    • 85034303221 scopus 로고    scopus 로고
    • note
    • In Ref. 16, Ament and Rado used a somewhat different convention for the wave number. What they define as k corresponds to ik in the present work (see Note 21).
  • 31
    • 85034296842 scopus 로고    scopus 로고
    • note
    • See, Appendix 1 of AR (Ref. 16).
  • 35
    • 85034298415 scopus 로고    scopus 로고
    • note
    • 0/4π), unusual in the cgs system, is necessary here in order to obtain appropriate units of Ω s (Henry) for the external inductance.


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