Frequency and temperature dependence of ultrasonic attenuation in indium in a transverse magnetic field and in zero field
Identifieur interne : 000860 ( Main/Exploration ); précédent : 000859; suivant : 000861Frequency and temperature dependence of ultrasonic attenuation in indium in a transverse magnetic field and in zero field
Auteurs : RBID : ISTEX:10909_1980_Article_BF00115498.pdfAbstract
The frequency and temperature dependence of the electronic attenuation of longitudinal ultrasound in indium along [110] has been measured between 1.5 and 4.2 K in the frequency range 10–90 MHz. The zero-field results are well described by a modified free-electron Pippard expression. As expected from general theory the high-field attenuation was proportional to q2 and showed an anisotropy reflecting the symmetry of the electron distribution. The temperature dependence was found to depend on the direction of the magnetic field in the plane normal to q.
DOI: 10.1007/BF00115498
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<author><name>B. Berre</name>
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<author><name>E. Børsum</name>
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<front><div type="abstract" xml:lang="eng">The frequency and temperature dependence of the electronic attenuation of longitudinal ultrasound in indium along [110] has been measured between 1.5 and 4.2 K in the frequency range 10–90 MHz. The zero-field results are well described by a modified free-electron Pippard expression. As expected from general theory the high-field attenuation was proportional to q2 and showed an anisotropy reflecting the symmetry of the electron distribution. The temperature dependence was found to depend on the direction of the magnetic field in the plane normal to q.</div>
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<originInfo><publisher>Kluwer Academic Publishers, Dordrecht</publisher>
<dateCreated encoding="w3cdtf">1979-08-27</dateCreated>
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<abstract lang="eng">The frequency and temperature dependence of the electronic attenuation of longitudinal ultrasound in indium along [110] has been measured between 1.5 and 4.2 K in the frequency range 10–90 MHz. The zero-field results are well described by a modified free-electron Pippard expression. As expected from general theory the high-field attenuation was proportional to q2 and showed an anisotropy reflecting the symmetry of the electron distribution. The temperature dependence was found to depend on the direction of the magnetic field in the plane normal to q.</abstract>
<relatedItem type="series"><titleInfo type="abbreviated"><title>J Low Temp Phys</title>
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<titleInfo><title>Journal of Low Temperature Physics</title>
<partNumber>Year: 1980</partNumber>
<partNumber>Volume: 38</partNumber>
<partNumber>Number: 5-6</partNumber>
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<genre>Archive Journal</genre>
<originInfo><dateIssued encoding="w3cdtf">1980-03-01</dateIssued>
<copyrightDate encoding="w3cdtf">1980</copyrightDate>
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<subject usage="primary"><topic>Physics</topic>
<topic>Characterization and Evaluation Materials</topic>
<topic>Condensed Matter</topic>
<topic>Magnetism, Magnetic Materials</topic>
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<identifier type="issn">0022-2291</identifier>
<identifier type="issn">Electronic: 1573-7357</identifier>
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