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Temperature dependence of electrical resistivity of Zr–Cu–Al–Ni–Nb bulk metallic glasses below 300K
The temperature dependence of electrical resistivitiy of Zr55Cu30-XAl10Ni5NbX (numbers indicate at.% X=0, 1, 3 and 5) bulk metallic glasses was investigated below 300K. For the Zr55Cu(30-X)Al10Ni5NbX alloys with X=1, 3 and 5 consisting of nanocrystals dispersed in the amorphous matrix, the electrica...
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Published in: | Materials science & engineering. A, Structural materials : properties, microstructure and processing Structural materials : properties, microstructure and processing, 2007-03, Vol.449-451, p.548-551 |
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container_end_page | 551 |
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container_start_page | 548 |
container_title | Materials science & engineering. A, Structural materials : properties, microstructure and processing |
container_volume | 449-451 |
creator | Okai, D. Nanbu, A. Fukami, T. Yamasaki, T. Zhang, T. Yokoyama, Y. Motoyama, G. Oda, Y. Kimura, H.M. Inoue, A. |
description | The temperature dependence of electrical resistivitiy of Zr55Cu30-XAl10Ni5NbX (numbers indicate at.% X=0, 1, 3 and 5) bulk metallic glasses was investigated below 300K. For the Zr55Cu(30-X)Al10Ni5NbX alloys with X=1, 3 and 5 consisting of nanocrystals dispersed in the amorphous matrix, the electrical resistivities decreased abruptly below approximately 2.3-2.9K. For the amorphous Zr55Cu30Al10Ni5 alloy, the electrical resistivitiy increased with decreasing temperature from 300K up to approximately 2.0K. The significant decrease of electrical resistivities of nanocrystal-dispersed amorphous alloys was attributable to the zero-resistivity effect of superconducting phases contained in the alloys. The Nb addition to Zr55Cu30Al10Ni5 metallic glass was found to precipitate superconducting phases within the amorphous matrix. |
doi_str_mv | 10.1016/j.msea.2006.02.446 |
format | article |
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A, Structural materials : properties, microstructure and processing</title><description>The temperature dependence of electrical resistivitiy of Zr55Cu30-XAl10Ni5NbX (numbers indicate at.% X=0, 1, 3 and 5) bulk metallic glasses was investigated below 300K. For the Zr55Cu(30-X)Al10Ni5NbX alloys with X=1, 3 and 5 consisting of nanocrystals dispersed in the amorphous matrix, the electrical resistivities decreased abruptly below approximately 2.3-2.9K. For the amorphous Zr55Cu30Al10Ni5 alloy, the electrical resistivitiy increased with decreasing temperature from 300K up to approximately 2.0K. The significant decrease of electrical resistivities of nanocrystal-dispersed amorphous alloys was attributable to the zero-resistivity effect of superconducting phases contained in the alloys. 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A, Structural materials : properties, microstructure and processing</jtitle><date>2007-03</date><risdate>2007</risdate><volume>449-451</volume><spage>548</spage><epage>551</epage><pages>548-551</pages><issn>0921-5093</issn><abstract>The temperature dependence of electrical resistivitiy of Zr55Cu30-XAl10Ni5NbX (numbers indicate at.% X=0, 1, 3 and 5) bulk metallic glasses was investigated below 300K. For the Zr55Cu(30-X)Al10Ni5NbX alloys with X=1, 3 and 5 consisting of nanocrystals dispersed in the amorphous matrix, the electrical resistivities decreased abruptly below approximately 2.3-2.9K. For the amorphous Zr55Cu30Al10Ni5 alloy, the electrical resistivitiy increased with decreasing temperature from 300K up to approximately 2.0K. The significant decrease of electrical resistivities of nanocrystal-dispersed amorphous alloys was attributable to the zero-resistivity effect of superconducting phases contained in the alloys. The Nb addition to Zr55Cu30Al10Ni5 metallic glass was found to precipitate superconducting phases within the amorphous matrix.</abstract><doi>10.1016/j.msea.2006.02.446</doi><tpages>4</tpages></addata></record> |
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title | Temperature dependence of electrical resistivity of Zr–Cu–Al–Ni–Nb bulk metallic glasses below 300K |
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