1990
DOI: 10.1109/20.104526
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Large Barkhausen and Matteucci effects in FeCoSiB, FeCrSiB, and FeNiSiB amorphous wires

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Cited by 239 publications
(137 citation statements)
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“…It is remarkable to note that the study of the magnetic properties of amorphous wires is a topic of great interest because of their outstanding properties, such as single and large Barkhausen jump or giant magneto-impedance effect [4,5]. It is known that the domain structure of the amorphous wire consists of an axially magnetized inner core and the outer shell, in which "maze" or "bamboo" structure can be observed [6]. Taking into account that the giant magneto-impedance effect is mainly a "surface" effect, the investigation of magnetic structure in the outer shell becomes a special meaning.…”
mentioning
confidence: 99%
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“…It is remarkable to note that the study of the magnetic properties of amorphous wires is a topic of great interest because of their outstanding properties, such as single and large Barkhausen jump or giant magneto-impedance effect [4,5]. It is known that the domain structure of the amorphous wire consists of an axially magnetized inner core and the outer shell, in which "maze" or "bamboo" structure can be observed [6]. Taking into account that the giant magneto-impedance effect is mainly a "surface" effect, the investigation of magnetic structure in the outer shell becomes a special meaning.…”
mentioning
confidence: 99%
“…These peaks can be associated with a quick rotation of the magnetization from the circular to the axial direction (increase of absolute value of the axial magnetization) and a quick nucleation of new circular domains (the reverse jump of the signal). Therefore, it is reasonable to conclude (see [6]) that the surface domain structure of as-cast wire consists of circular domain and the remagnetization process is related with the formation of reversal circular domains. The longitudinal Kerr effect loop under applied axial field consists of two jumps (Fig.…”
mentioning
confidence: 99%
“…All dependences are characterized by the similar forms of both components (real as well as imaginary one). The susceptibility is zero up to the switching field H sw , where it abruptly increases as a result of the depining of the closure domain wall, according to the expected behavior in wires with positive magnetostriction [6]. Above the H sw , the imaginary parts immediately decrease in the hyperbolic dependence, whereas in the real part small concave decrease shows the reversible moment rotation in the external domain structure with the radial magnetization [5].…”
Section: Resultsmentioning
confidence: 87%
“…The existence of the axially oriented core domain along the wire explains the magnetic bistability, consisting of the sudden reorientation of this inner domain [30]. Wires exhibiting vanishing magnetostriction coefficient do not show spontaneous magnetic bistability.…”
Section: Resultsmentioning
confidence: 98%