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Physical Review B - Condensed Matter and Materials Physics

Volumn 81, Issue 2, 2010, Pages

Direct imaging of domain-wall interactions in Ni80Fe 20 planar nanowires

(8) Hayward, T J a Bryan, M T a Fry, P W a Fundi, P M a Gibbs, M R J a Allwood, D A a Im, M Y b Fischer, P b

a UNIVERSITY OF SHEFFIELD (United Kingdom)

b LAWRENCE BERKELEY NATIONAL LABORATORY (United States)

Author keywords

[No Author keywords available]

Indexed keywords

EID: 77954773217 PISSN: 10980121 EISSN: 1550235X Source Type: Journal
DOI: 10.1103/PhysRevB.81.020410 Document Type: Article

Times cited : (47)

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- The reader can reconcile this dipolar coupling with the Coulomb-like interaction picture used earlier by realizing that this orientation of transverse walls brings together large edge charges of opposite polarity
- The reader can reconcile this dipolar coupling with the Coulomb-like interaction picture used earlier by realizing that this orientation of transverse walls brings together large edge charges of opposite polarity.

20
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- E= qi qj /4π μ0 r where q=±2 μ0 Mwt is an analytically derived value of DW's net magnetic "charge" ( +H2H, -T2T) and r is the distance between the DWs. M represents the saturation magnetization of Ni80 Fe20, while w and t are the nanowires' thickness and width respectively
- E = q i q j / 4 π μ 0 r where q = ± 2 μ 0 M w t is an analytically derived value of DW's net magnetic "charge" (+ H 2 H, -T2T) and r is the distance between the DWs. M represents the saturation magnetization of Ni 80 Fe 20, while w and t are the nanowires' thickness and width respectively.

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