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Volumn 80, Issue 10, 2009, Pages

Nucleation of a vortex-antivortex pair in the presence of an immobile magnetic vortex

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EID: 70349898775     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.80.100405     Document Type: Article
Times cited : (32)

References (17)
  • 1
    • 0036530889 scopus 로고    scopus 로고
    • 10.1016/S0304-8853(01)01086-1
    • R. P. Cowburn, J. Magn. Magn. Mater. 242-245, 505 (2002). 10.1016/S0304-8853(01)01086-1
    • (2002) J. Magn. Magn. Mater. , vol.242-245 , pp. 505
    • Cowburn, R.P.1
  • 4
    • 67649199961 scopus 로고    scopus 로고
    • 10.1038/nphys1231
    • A. Vansteenkiste, Nat. Phys. 5, 332 (2009). 10.1038/nphys1231
    • (2009) Nat. Phys. , vol.5 , pp. 332
    • Vansteenkiste, A.1
  • 6
    • 18244408290 scopus 로고    scopus 로고
    • 10.1103/PhysRevLett.94.027205
    • B. A. Ivanov and C. E. Zaspel, Phys. Rev. Lett. 94, 027205 (2005). 10.1103/PhysRevLett.94.027205
    • (2005) Phys. Rev. Lett. , vol.94 , pp. 027205
    • Ivanov, B.A.1    Zaspel, C.E.2
  • 8
    • 50449096890 scopus 로고    scopus 로고
    • 10.1103/PhysRevB.78.064418
    • R. Zivieri and F. Nizzoli, Phys. Rev. B 78, 064418 (2008). 10.1103/PhysRevB.78.064418
    • (2008) Phys. Rev. B , vol.78 , pp. 064418
    • Zivieri, R.1    Nizzoli, F.2
  • 9
    • 70349921557 scopus 로고    scopus 로고
    • We used for all OOMMF simulations material parameters adopted for the Py particle: the exchange constant A=2.6× 10-6 erg/cm, the saturation magnetization MS =8.6× 102 G, the damping coefficient η=0.006, and the anisotropy was neglected. This corresponds to the exchange length a= A/4π MS2 5.3nm. The mesh cells have sizes 3×3×hnm, where h is the thickness of the sample. The applied field was used in form b (t) =b (1- e- t2 /Δ t2) (cosωt,sinωt,0), with Δt=50ps.
    • We used for all OOMMF simulations material parameters adopted for the Py particle: the exchange constant A=2.6× 10-6 erg/cm, the saturation magnetization MS =8.6× 102 G, the damping coefficient η=0.006, and the anisotropy was neglected. This corresponds to the exchange length a= A/4π MS2 5.3nm. The mesh cells have sizes 3×3×hnm, where h is the thickness of the sample. The applied field was used in form b (t) =b (1- e- t2 /Δ t2) (cosωt,sinωt,0), with Δt=50ps.
  • 10
    • 33750344755 scopus 로고    scopus 로고
    • 10.1103/PhysRevLett.97.177202
    • R. Hertel and C. M. Schneider, Phys. Rev. Lett. 97, 177202 (2006). 10.1103/PhysRevLett.97.177202
    • (2006) Phys. Rev. Lett. , vol.97 , pp. 177202
    • Hertel, R.1    Schneider, C.M.2
  • 13
    • 70349923695 scopus 로고    scopus 로고
    • The cells with fixed magnetization contribute to the effective field but they are omitted from the procedure of numerical time integration of the LL equation.
    • The cells with fixed magnetization contribute to the effective field but they are omitted from the procedure of numerical time integration of the LL equation.
  • 14
    • 70349901012 scopus 로고    scopus 로고
    • For the planar vortex the magnon modes with opposite m are degenerated; for the general case see, e.g., Ref..
    • For the planar vortex the magnon modes with opposite m are degenerated; for the general case see, e.g., Ref..
  • 15
    • 0000986128 scopus 로고    scopus 로고
    • 10.1103/PhysRevA.60.3313
    • T. Isoshima and K. Machida, Phys. Rev. A 60, 3313 (1999). 10.1103/PhysRevA.60.3313
    • (1999) Phys. Rev. A , vol.60 , pp. 3313
    • Isoshima, T.1    MacHida, K.2


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.