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Volumn 31, Issue 6, 1995, Pages 3805-3807

Effect of Magnetocrystalline Anisotropy in Single-Domain Polycrystalline Cobalt Islands

Author keywords

[No Author keywords available]

Indexed keywords

COBALT; COMPUTATIONAL METHODS; CRYSTAL ORIENTATION; MAGNETIC ANISOTROPY; MAGNETIC DOMAINS; MAGNETIC FIELD EFFECTS; MAGNETIC PROPERTIES; MAGNETIC RELAXATION; MAGNETIZATION; POLYCRYSTALLINE MATERIALS; REMANENCE;

EID: 0029404138     PISSN: 00189464     EISSN: 19410069     Source Type: Journal    
DOI: 10.1109/20.489778     Document Type: Article
Times cited : (33)

References (8)
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    • R. M. H. New, R. F. W. Pease, and R. L. White, “Submicron patterning of thin cobalt films for magnetic storage”, J. Vac. Sci. Technol. B, Vol. 12, No. 6, pp. 3196–3201, Nov/Dec 1994.
    • (1994) J. Vac. Sci. Technol. B , vol.12 , Issue.6 , pp. 3196-3201
    • New, R.M.H.1    Pease, R.F.W.2    White, R.L.3
  • 2
    • 36449002242 scopus 로고
    • Single-domain magnetic pillar array of 35 nm diameter and 65 Gbits/in2 density for ultrahigh density quantum magnetic storage
    • Nov.
    • S. Y. Chou, M. Wei, P. R. Krauss, and P. B. Fisher, “Single-domain magnetic pillar array of 35 nm diameter and 65 Gbits/in2 density for ultrahigh density quantum magnetic storage”, J.Appl.Phys., vol. 76, no. 10, pp. 6673–6675, Nov. 1994.
    • (1994) J.Appl.Phys. , vol.76 , Issue.10 , pp. 6673-6675
    • Chou, S.Y.1    Wei, M.2    Krauss, P.R.3    Fisher, P.B.4
  • 3
    • 0026258535 scopus 로고
    • Observation of the switching fields of individual permalloy particles in nanolithographic arrays via magnetic force microscopy
    • Nov.
    • G. A. Gibson, J. F. Smyth, and S. Schultz, “Observation of the switching fields of individual permalloy particles in nanolithographic arrays via magnetic force microscopy”, IEEE Trans. Mag. vol. 27, pp. 5187–5189, Nov. 1991.
    • (1991) IEEE Trans. Mag. , vol.27 , pp. 5187-5189
    • Gibson, G.A.1    Smyth, J.F.2    Schultz, S.3
  • 4
    • 20444390075 scopus 로고
    • Properties and measurement of scanning tunneling microscope fabricated ferromagnetic particle arrays
    • Nov.
    • A. D. Kent, S. von Molnár, S. Gider, and D. D. Awschalom, “Properties and measurement of scanning tunneling microscope fabricated ferromagnetic particle arrays”, J.Appl.Phys., vol. 76, no. 10, pp. 6656–6660, Nov. 1994.
    • (1994) J.Appl.Phys. , vol.76 , Issue.10 , pp. 6656-6660
    • Kent, A.D.1    von Molnár, S.2    Gider, S.3    Awschalom, D.D.4
  • 5
    • 0000557773 scopus 로고
    • Size effects on switching field of isolated and interactive arrays of nanoscale single-domain Ni bars fabricated using electron-beam nanolithography
    • Nov.
    • M. S. Wei and S. Y. Chou, “Size effects on switching field of isolated and interactive arrays of nanoscale single-domain Ni bars fabricated using electron-beam nanolithography”, J.Appl.Phys., vol. 76, no. 10, pp. 6679–6681, Nov. 1994.
    • (1994) J.Appl.Phys. , vol.76 , Issue.10 , pp. 6679-6681
    • Wei, M.S.1    Chou, S.Y.2
  • 6
    • 84939734622 scopus 로고    scopus 로고
    • Physical and magnetic properties of submicron lithographically patterned magnetic islands
    • press
    • R. M. H. New, R. F. W. Pease and R. L. White, “Physical and magnetic properties of submicron lithographically patterned magnetic islands”, J. Vac. Sci. Technol. A., in press.
    • J. Vac. Sci. Technol. A.
    • New, R.M.H.1    Pease, R.F.W.2    White, R.L.3
  • 7
    • 0004224256 scopus 로고
    • New York: Wiley, The reader should note that there is a difference of nomenclature here. The reference treats a summation of N phasors of length αk/√N while this paper treats a summation of N phasors of length rc. Also, the phase angle of the resultant phasor E is 2β rather than θ. This accounts for the differences in the probability density functions used
    • J. W. Goodman, Statistical Optics, New York: Wiley, 1985, pp. 45–55. The reader should note that there is a difference of nomenclature here. The reference treats a summation of N phasors of length αk/√N while this paper treats a summation of N phasors of length rc. Also, the phase angle of the resultant phasor E is 2β rather than θ. This accounts for the differences in the probability density functions used.
    • (1985) Statistical Optics , pp. 45-55
    • Goodman, J.W.1
  • 8
    • 84939711958 scopus 로고
    • Oxford, July
    • MRM Conference, Oxford, July 1995.
    • (1995) MRM Conference


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.