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Correction factor in nondiffusive Hall magnetometry
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10.1063/1.3597619
/content/aip/journal/apl/98/23/10.1063/1.3597619
http://aip.metastore.ingenta.com/content/aip/journal/apl/98/23/10.1063/1.3597619
View: Figures

Figures

Image of FIG. 1.
FIG. 1.

Hysteretic Hall resistance as a function of caused by a MB produced under the edge of a Dy film (lower right insets). The traces are for increasing density as indicated by the solid arrow. Upper left inset: , indicating that depends on .

Image of FIG. 2.
FIG. 2.

(a) Calculated in a homogeneous perpendicular magnetic field of 0.1 T for different W. (b) for the MB introduced in Fig. 1. for 3 MB heights.

Image of FIG. 3.
FIG. 3.

as a function of the cyclotron radius in for different Hall cross sizes in the ballistic case (symbols with lines), the peaks are at the position where the MB closes and the length of the Hall cross matches the average cyclotron diameter; also shown, with line, the simulation corresponding to the experimental trace indicated by the dashed arrow in Fig. 1.

Image of FIG. 4.
FIG. 4.

The dependence of on the height of the MB for three different magnetic field profiles, magnetic dot d, stripe s, and wire w.

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/content/aip/journal/apl/98/23/10.1063/1.3597619
2011-06-09
2014-04-16
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Correction factor in nondiffusive Hall magnetometry
http://aip.metastore.ingenta.com/content/aip/journal/apl/98/23/10.1063/1.3597619
10.1063/1.3597619
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