001     41956
005     20240610120439.0
017 _ _ |a This version is available at the following Publisher URL: http://jap.aip.org
024 7 _ |a 10.1063/1.1827344
|2 DOI
024 7 _ |a WOS:000226778300012
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024 7 _ |a 2128/1083
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037 _ _ |a PreJuSER-41956
041 _ _ |a eng
082 _ _ |a 530
084 _ _ |2 WoS
|a Physics, Applied
100 1 _ |a Heggen, M.
|b 0
|u FZJ
|0 P:(DE-Juel1)VDB5029
245 _ _ |a Creation and annihilation of free volume during homogeneous flow of a metallic glass
260 _ _ |a Melville, NY
|b American Institute of Physics
|c 2005
300 _ _ |a 033506
336 7 _ |a Journal Article
|0 PUB:(DE-HGF)16
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336 7 _ |a Journal Article
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336 7 _ |a article
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440 _ 0 |a Journal of Applied Physics
|x 0021-8979
|0 3051
|v 97
500 _ _ |a Record converted from VDB: 12.11.2012
520 _ _ |a Bulk samples of Pd41Ni10Cu29P20 glass were tested at constant true stress (20-636 MPa) in compression at 550, 555, and 565 K to study the transition from steady-state creep at low stress to deformation-induced softening at high stress. In the high-stress regime strongly accelerating creep was observed. All deformation was homogeneous. The activation volume was 106 Angstrom(3). The isoconfigurational activation energy was 9.03+/-0.64 eV. The disordering rate is proportional to the applied power density (stressxstrain rate). The disordering process is inefficient in energy and in the production of free volume. (C) 2005 American Institute of Physics.
536 _ _ |a Kondensierte Materie
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588 _ _ |a Dataset connected to Web of Science
650 _ 7 |a J
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700 1 _ |a Spaepen, F.
|b 1
|0 P:(DE-HGF)0
700 1 _ |a Feuerbacher, M.
|b 2
|u FZJ
|0 P:(DE-Juel1)130637
773 _ _ |a 10.1063/1.1827344
|g Vol. 97, p. 033506
|p 033506
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|t Journal of applied physics
|v 97
|y 2005
|x 0021-8979
856 7 _ |u http://dx.doi.org/10.1063/1.1827344
|u http://hdl.handle.net/2128/1083
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|v Kondensierte Materie
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914 1 _ |y 2005
915 _ _ |0 StatID:(DE-HGF)0010
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920 1 _ |k IFF-IMF
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