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Volumn 96, Issue 21, 2010, Pages

Nonuniformity of a planar polarizer for spin-transfer-induced vortex oscillations at zero field

Author keywords

[No Author keywords available]

Indexed keywords

EXCITATION EFFICIENCY; FREE LAYERS; LARGE AMPLITUDE; MAGNETIZATION DISTRIBUTION; NONUNIFORM; NONUNIFORMITY; SPIN TRANSFER; SPIN-VALVES; VORTEX CHIRALITY; VORTEX MOTION; ZERO FIELDS;

EID: 77956234145     PISSN: 00036951     EISSN: None     Source Type: Journal    
DOI: 10.1063/1.3441405     Document Type: Article
Times cited : (55)

References (23)
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    • Choi, Y.-S.1    Lee, K.-S.2    Kim, S.-K.3
  • 18
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    • We note however that variation in time of even uniform planar polarization can have a similar effect on the vortex core as the variation in in space discussed in this work. Thus, a moving uniform planar polarizer can in principle excite the vortex motion.
    • We note however that variation in time of even uniform planar polarization p can have a similar effect on the vortex core as the variation in p in space discussed in this work. Thus, a moving uniform planar polarizer can in principle excite the vortex motion.
  • 19
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    • To check different signs of the current without changing the chirality of the Oersted field, we consider that the free layer can be above as well as below the polarizer layer in the stack.
    • To check different signs of the current without changing the chirality of the Oersted field, we consider that the free layer can be above as well as below the polarizer layer in the stack.
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  • 23
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    • We obtain the core radius b by fitting the simulated static vortex profile with the Ansatz (2), which gives b=16 nm and the parameter =1.46 is found using the numerical procedure described in Ref. The first critical current can be captured by the analytical model by taking into account the higher order terms in W (a) and W (a) for a≈b, an issue that is going beyond the scope of the present work.
    • We obtain the core radius b by fitting the simulated static vortex profile with the Ansatz (2), which gives b=16 nm and the parameter =1.46 is found using the numerical procedure described in Ref. The first critical current can be captured by the analytical model by taking into account the higher order terms in W (a) and W (a) for a≈b, an issue that is going beyond the scope of the present work.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.