Mechanism of temperature-induced transitions between stripe and undulation domain structures
Identifieur interne : 001886 ( Pascal/Curation ); précédent : 001885; suivant : 001887Mechanism of temperature-induced transitions between stripe and undulation domain structures
Auteurs : V. A. Zablotskii [Ukraine] ; Yu. A. Mamalui ; K. V. LamonovaSource :
- Physica status solidi. B. Basic research [ 0370-1972 ] ; 1992.
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- Pascal (Inist)
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- topic : Composé minéral.
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Abstract
The temperature-induced instability of thin magnetic film stripe domain structures (SDS) is studied. Dislocations present in the SDS are shown to be nuclei for the formation of an undulation structure, the domain wall bend period being determined by the dislocation strength. The range of thermal stability of the stripe domain structure is calculated
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<author><name sortKey="Mamalui, Yu A" sort="Mamalui, Yu A" uniqKey="Mamalui Y" first="Yu. A." last="Mamalui">Yu. A. Mamalui</name>
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<front><div type="abstract" xml:lang="en">The temperature-induced instability of thin magnetic film stripe domain structures (SDS) is studied. Dislocations present in the SDS are shown to be nuclei for the formation of an undulation structure, the domain wall bend period being determined by the dislocation strength. The range of thermal stability of the stripe domain structure is calculated</div>
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<fA14 i1="01"><s1>Donetsk univ., dep. physics</s1>
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<fA66 i1="01"><s0>DEU</s0>
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<fC01 i1="01" l="ENG"><s0>The temperature-induced instability of thin magnetic film stripe domain structures (SDS) is studied. Dislocations present in the SDS are shown to be nuclei for the formation of an undulation structure, the domain wall bend period being determined by the dislocation strength. The range of thermal stability of the stripe domain structure is calculated</s0>
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<s5>02</s5>
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<s5>03</s5>
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<s5>03</s5>
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<s5>03</s5>
</fC03>
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<s5>03</s5>
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<s5>04</s5>
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<fC03 i1="04" i2="X" l="ENG"><s0>Domain wall</s0>
<s5>04</s5>
</fC03>
<fC03 i1="04" i2="X" l="GER"><s0>Domaenenwand</s0>
<s5>04</s5>
</fC03>
<fC03 i1="04" i2="X" l="SPA"><s0>Pared dominio</s0>
<s5>04</s5>
</fC03>
<fC03 i1="05" i2="X" l="FRE"><s0>Dislocation</s0>
<s5>05</s5>
</fC03>
<fC03 i1="05" i2="X" l="ENG"><s0>Dislocation</s0>
<s5>05</s5>
</fC03>
<fC03 i1="05" i2="X" l="GER"><s0>Versetzung</s0>
<s5>05</s5>
</fC03>
<fC03 i1="05" i2="X" l="SPA"><s0>Dislocación</s0>
<s5>05</s5>
</fC03>
<fC03 i1="06" i2="X" l="FRE"><s0>Traitement thermique</s0>
<s5>06</s5>
</fC03>
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<s5>06</s5>
</fC03>
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<s5>06</s5>
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<s5>06</s5>
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<fC03 i1="07" i2="X" l="FRE"><s0>Ferrites grenats</s0>
<s5>10</s5>
</fC03>
<fC03 i1="07" i2="X" l="ENG"><s0>Ferrites garnets</s0>
<s5>10</s5>
</fC03>
<fC03 i1="07" i2="X" l="SPA"><s0>Ferritas granates</s0>
<s5>10</s5>
</fC03>
<fC03 i1="08" i2="X" l="FRE"><s0>Composé minéral</s0>
<s5>11</s5>
</fC03>
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<s5>11</s5>
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<fC03 i1="08" i2="X" l="SPA"><s0>Compuesto inorgánico</s0>
<s5>11</s5>
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<s5>12</s5>
</fC03>
<fC03 i1="09" i2="X" l="ENG"><s0>Thick film</s0>
<s5>12</s5>
</fC03>
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<s5>12</s5>
</fC03>
<fC03 i1="10" i2="X" l="FRE"><s0>Bismuth Fer Gallium Thulium Oxyde Mixte</s0>
<s2>NC</s2>
<s2>FX</s2>
<s2>NA</s2>
<s5>18</s5>
</fC03>
<fC03 i1="10" i2="X" l="ENG"><s0>Bismuth Iron Gallium Thulium Oxides Mixed</s0>
<s2>NC</s2>
<s2>FX</s2>
<s2>NA</s2>
<s5>18</s5>
</fC03>
<fC03 i1="10" i2="X" l="SPA"><s0>Bismuto Hierro Galio Tulio Óxido Mixto</s0>
<s2>NC</s2>
<s2>FX</s2>
<s2>NA</s2>
<s5>18</s5>
</fC03>
<fC07 i1="01" i2="X" l="FRE"><s0>Métal transition Composé</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>16</s5>
</fC07>
<fC07 i1="01" i2="X" l="ENG"><s0>Transition metal Compounds</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>16</s5>
</fC07>
<fC07 i1="01" i2="X" l="SPA"><s0>Metal transición Compuesto</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>16</s5>
</fC07>
<fC07 i1="02" i2="X" l="FRE"><s0>Lanthanide Composé</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>17</s5>
</fC07>
<fC07 i1="02" i2="X" l="ENG"><s0>Lanthanide Compounds</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>17</s5>
</fC07>
<fC07 i1="02" i2="X" l="SPA"><s0>Lantánido Compuesto</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>17</s5>
</fC07>
<fN21><s1>306</s1>
</fN21>
<fN82><s0>NBS</s0>
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