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  1. NTU Theses and Dissertations Repository
  2. 理學院
  3. 物理學系
請用此 Handle URI 來引用此文件: http://tdr.lib.ntu.edu.tw/jspui/handle/123456789/31820
完整後設資料紀錄
DC 欄位值語言
dc.contributor.advisor張慶瑞
dc.contributor.authorYi-Chen Yangen
dc.contributor.author楊毅楨zh_TW
dc.date.accessioned2021-06-13T03:21:11Z-
dc.date.available2006-07-31
dc.date.copyright2006-07-31
dc.date.issued2006
dc.date.submitted2006-07-28
dc.identifier.citation[1] J. Slonczewski, J. Magn. Magn. Mater. 159, L1 (1996).
[2] L. Berger, Phys. Rev. B 54, 9359 (1996).
[3] Z. Li and S. Zhang, Phys. Rev. B 68, 024404 (2003)
[4] Z. Li and S. Zhang, Phys. Rev. B 70, 024417 (2004)
[5] S. Zhang and Z. Li, Phys. Rev. Lett. 93, 127204 (2004)
[6] Z. Li, J. He and S. Zhang, J. Appl. Phys. 99, 08Q702 (2006)
[7] F. Bloch 1932 ZS. f. Phys. 74 295.
[8] L. Landau and E. Lifshitz, Phys. Z. Sowjetunion 8, 153 (1935).
[9] S.Chikazumi, Physics of ferromagnetism,.Oxford University Press
(1997).
[10] T. L. Gilbert 1955 Proceeding of the Conference on Magnetism and
Magnetic Materials, Pittsburg.
[11] W. Doring 1948 Z. Maturforsch (German) 3a 373-379.
[12] S.I. Kiselev, J.C. Sankey, I.N. Krivorotov, N.C. Emley, R.J. Schoelkopf,
R.A. Buhrman, D. C. Ralph, Letters to Nature 425, p. 380 (2003).
[13] S. Urazhdin, N. O. Birge, W. P.Pratt, J. Bass, Phys. Rev. Lett. 91,
146803 (2003)
[14] A. Yamaguchi, T. Ono, S. Nasu, Phys. Rev. Lett. 92, 077205 (2004)
[15] M. Klaui et al., Phys. Rev. Lett. 95, 026601 (2005)
[16] N. L. Schryer and L. R. Walker, J. Appl. Phys. 45, 5406 (1974).
[17] Gerald, Applied numerical analysis, Wheatley sixth edition.
dc.identifier.urihttp://tdr.lib.ntu.edu.tw/jspui/handle/123456789/31820-
dc.description.abstractAbstract
When a spin-polarized current ‡ows through a ferromagnet, the local
magnetization receives a spin transfer torque. In one-dimention approxi-
mations, we solve the Landau-Lifshitz-Gilbert equation along with two spin
torque terms, both analytically and numerically, to realize the behavior of a
domain wall under the in‡uence of the spin-polarized current. As a …rst step,
we focus on the system of domain wall within a perfect magnetic nanowire.
Secondly, we consider the pinning case which may be caused by doping a
high-Ku material into the system. By numerically solving the LLG equation,
we …nd some characteristics of domain-wall motion under the spin-polarized
current. In the presence of domain-wall pinning centers, we also de…ned the
depinning …eld and construct a phase diagram for the domain-wall.
en
dc.description.provenanceMade available in DSpace on 2021-06-13T03:21:11Z (GMT). No. of bitstreams: 1
ntu-95-R92222046-1.pdf: 524616 bytes, checksum: d6e9de970fe459e36df65c56c39ef431 (MD5)
Previous issue date: 2006
en
dc.description.tableofcontentsContents
1 Introduction 11
2 Theoretical background of micromagnetics 15
2.1 Domain wall . . . . . . . . . . . . . . . . . . . . . . . . . . . . 15
2.2 Micromagnetics . . . . . . . . . . . . . . . . . . . . . . . . . . 17
2.3 Landau-Lifshitz-Gilbert Equation . . . . . . . . . . . . . . . . 18
2.3.1 Gyrotropic Equation of Motion . . . . . . . . . . . . . 19
2.3.2 Damping term . . . . . . . . . . . . . . . . . . . . . . . 20
2.3.3 Main energy terms . . . . . . . . . . . . . . . . . . . . 20
2.3.4 One-dimensional Bloch wall theory . . . . . . . . . . . 25
3 Theoretical background of spin-transfer model 29
3.1 Spin transfer e¤ect . . . . . . . . . . . . . . . . . . . . . . . . 29
3.2 Landau-Lifshitz-Gilbert equation with spin torque terms . . . 31
4 Analytic solution of current-driven domain wall motion 35
4.1 Model of the system . . . . . . . . . . . . . . . . . . . . . . . 35
4.2 Model calculations . . . . . . . . . . . . . . . . . . . . . . . . 37
4.3 Results and discussions . . . . . . . . . . . . . . . . . . . . . . 40
4.4 The special case: simple pendulum . . . . . . . . . . . . . . . 41
5 Numerical study of current-driven domain wall motion 45
5.1 Computational method of micromagnetics . . . . . . . . . . . 45
5.2 Discussion about units and typical values of parameters . . . . 47
5.3 Numerical results of domain wall motion in a perfect nanowire 48
5.3.1 Under the in‡uence of external magnetic …eld . . . . . 48
5.3.2 Under the in‡uence of adiabatic spin torque . . . . . . 50
5.3.3 Under the in‡uence of non-adiabatic spin torque . . . . 53
5.4 Numerical results of domain wall motion in a nanowire with a
pinning center . . . . . . . . . . . . . . . . . . . . . . . . . . . 55
5.4.1 Under the in‡uence of external magnetic …eld . . . . . 55
5.4.2 Under the in‡uence of spin current . . . . . . . . . . . 59
6 Summary 61
Bibliography 62
dc.language.isoen
dc.subject磁壁zh_TW
dc.subjectSpin-Polarized Currenten
dc.subjectDomain Wall Motionen
dc.title磁壁在磁場及極化自旋電流下之運動行為zh_TW
dc.titleOne-Dimentional Wall Motion Driven by Magnetic Field and Spin-Polarized Currenten
dc.typeThesis
dc.date.schoolyear94-2
dc.description.degree碩士
dc.contributor.oralexamcommittee楊志信,賴梅鳳
dc.subject.keyword磁壁,zh_TW
dc.subject.keywordDomain Wall Motion,Spin-Polarized Current,en
dc.relation.page64
dc.rights.note有償授權
dc.date.accepted2006-07-30
dc.contributor.author-college理學院zh_TW
dc.contributor.author-dept物理研究所zh_TW
顯示於系所單位:物理學系

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