<?xml version="1.0" encoding="UTF-8"?>
<records>
<record>
<language>eng</language>
<publisher>Science and Education Publishing</publisher>
<journalTitle>Journal of Materials Physics and Chemistry</journalTitle>
<eissn>2333-4444</eissn>
<publicationDate>2018-10-23</publicationDate>
<volume>6</volume>
<issue>2</issue>
<startPage>36</startPage>
<endPage>38</endPage>
<doi>10.12691/jmpc-6-2-1</doi>
<publisherRecordId>JMPC2018621</publisherRecordId>
<documentType>article</documentType>
<title language="eng">Activation Energy Depending on the Thickness of the Ferromagnetic Layer</title>
<authors>
<author>
<name>A. Adanlété Adjanoh</name>
<email>adanlete.assiongbon@gmail.com</email>
<affiliationId>1</affiliationId>
</author>
<author>
<name>R. Belhi</name>
<affiliationId>2</affiliationId>
</author>

</authors>
<affiliationsList>
<affiliationName affiliationId="1">Département de Physique, Faculté des Sciences et Techniques, Université de Kara, B.P : 404, Kara, Togo</affiliationName>
<affiliationName affiliationId="2">Département de Physique, Faculté des Sciences de Tunis, Université de Tunis El Manar, Tunis 1060, Tunisia</affiliationName>
</affiliationsList>
<abstract language="eng">We present the detailed study of activation energy Ea according to the thickness of the magnetic layer (tCo=0.7,0.8 and 1nm). The study was carried out at room temperature by means of polar magneto-optical Kerr effect magnetometry (PMOKE) using a He-Ne laser (=633nm). We found that the activation field 0Ha, the coercive field 0HC and the average activation energy Ea are weak for the sample with thickness tCo = 1 nm.</abstract>
<fullTextUrl format="pdf">http://pubs.sciepub.com/jmpc/6/2/1/jmpc-6-2-1.pdf</fullTextUrl>
<keywords language="eng"><keyword>time of demagnetization</keyword>
<keyword>activation field</keyword>
<keyword>activation energy</keyword>
<keyword>activation volume</keyword>
</keywords>
</record>
</records>
