Abstract
The relationship between domain wall motion and magnetization rotation is investigated. A wall motion mechanism previously proposed by the author is examined. The model gives the novel concept that the energy difference between transition state (magnetization curling) and final state (after wall motion) accelerates the wall motion. The magnetic moments in the region coupled with 90° walls rotate more slowly than those moments in the non-coupled region, hence the magnetic flux change is confined to a narrower portion of central domains at higher frequencies.
| Original language | English |
|---|---|
| Pages (from-to) | 262-267 |
| Number of pages | 6 |
| Journal | Journal of Magnetism and Magnetic Materials |
| Volume | 134 |
| Issue number | 2-3 |
| DOIs | |
| Publication status | Published - 1994 |
| Externally published | Yes |
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ASJC Scopus subject areas
- Condensed Matter Physics
Cite this
Magnetization dynamics in thin film heads. / Ohashi, Keishi.
In: Journal of Magnetism and Magnetic Materials, Vol. 134, No. 2-3, 1994, p. 262-267.Research output: Contribution to journal › Article
}
TY - JOUR
T1 - Magnetization dynamics in thin film heads
AU - Ohashi, Keishi
PY - 1994
Y1 - 1994
N2 - The relationship between domain wall motion and magnetization rotation is investigated. A wall motion mechanism previously proposed by the author is examined. The model gives the novel concept that the energy difference between transition state (magnetization curling) and final state (after wall motion) accelerates the wall motion. The magnetic moments in the region coupled with 90° walls rotate more slowly than those moments in the non-coupled region, hence the magnetic flux change is confined to a narrower portion of central domains at higher frequencies.
AB - The relationship between domain wall motion and magnetization rotation is investigated. A wall motion mechanism previously proposed by the author is examined. The model gives the novel concept that the energy difference between transition state (magnetization curling) and final state (after wall motion) accelerates the wall motion. The magnetic moments in the region coupled with 90° walls rotate more slowly than those moments in the non-coupled region, hence the magnetic flux change is confined to a narrower portion of central domains at higher frequencies.
UR - http://www.scopus.com/inward/record.url?scp=0028445051&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=0028445051&partnerID=8YFLogxK
U2 - 10.1016/0304-8853(94)00150-2
DO - 10.1016/0304-8853(94)00150-2
M3 - Article
AN - SCOPUS:0028445051
VL - 134
SP - 262
EP - 267
JO - Journal of Magnetism and Magnetic Materials
JF - Journal of Magnetism and Magnetic Materials
SN - 0304-8853
IS - 2-3
ER -