1997
DOI: 10.1063/1.364501
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Domain wall displacements in amorphous films and multilayers studied with a magnetic force microscope

Abstract: The magnetic force microscope (MFM) was used to study the displacement of domain walls (DW) in amorphous TbFe alloy films and Co/Pd multilayer films with high spatial resolution. The reversible bending of domain wall segments pinned to defects and irreversible, jumplike displacement of domain wall segments were imaged with the MFM in an applied magnetic field. The maximum reversible displacement of domain walls was 50–100 nm and the length of the segments which reversibly curved in the field was about 150 nm. … Show more

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Cited by 11 publications
(3 citation statements)
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“…It should be noted that care has to be taken in obtaining and interpreting MFM images, as the imaging process is intrinsically invasive. Due to the tip being magnetic, and therefore possessing a stray field, the imaging of a sample may itself alter the domain configuration within the sample [35]. The tip stray field could be at least 620 Oe [36] and may therefore cause domain walls to move, or in the worst case, saturate the area being imaged and hence erase any domains.…”
Section: Mfm Observation Of Domain Configurationsmentioning
confidence: 99%
“…It should be noted that care has to be taken in obtaining and interpreting MFM images, as the imaging process is intrinsically invasive. Due to the tip being magnetic, and therefore possessing a stray field, the imaging of a sample may itself alter the domain configuration within the sample [35]. The tip stray field could be at least 620 Oe [36] and may therefore cause domain walls to move, or in the worst case, saturate the area being imaged and hence erase any domains.…”
Section: Mfm Observation Of Domain Configurationsmentioning
confidence: 99%
“…At larger length scales (microns), the magnons propagate into the bulk of the sample carrying away significant energy. Such multiscale phenomena are encountered in the depinning of DW [1,2,3,4], the influence of surfaces and interfaces on the spins in the bulk [5,6,7,8], etc. These phenomena determine basic magnetic properties such as the coercive field and the dynamics of magnetization reversal.…”
mentioning
confidence: 99%
“…where Q is the statistical integral, and the torques F j and G j are determined from the conditions of local equilibrium: µ f µ,j α 1µ = α 1j , and µ f µ,j α 2µ = α 2j , where the angular brackets mean the statistical averaging with the distribution function (2).…”
mentioning
confidence: 99%