2008
DOI: 10.1016/j.ijplas.2007.01.015
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Spatiotemporally inhomogeneous plastic flow of a bulk-metallic glass

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Cited by 100 publications
(71 citation statements)
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“…Based on systematical examination of the deformation and fracture in metallic glasses, Spaepen [8] first constructed a deformation map that distinguishes the plastic deformation into two basic modes: homogeneous and inhomogeneous. For the former, each volume element of the sample contributes to the macroscopic plastic strain [8]; for the latter, the strain is highly localized into a few nanoscale shear bands [9][10][11][12][13]. The deformation map has been subsequently extended by a number of other researchers [4,[14][15][16][17].…”
Section: Introductionmentioning
confidence: 99%
“…Based on systematical examination of the deformation and fracture in metallic glasses, Spaepen [8] first constructed a deformation map that distinguishes the plastic deformation into two basic modes: homogeneous and inhomogeneous. For the former, each volume element of the sample contributes to the macroscopic plastic strain [8]; for the latter, the strain is highly localized into a few nanoscale shear bands [9][10][11][12][13]. The deformation map has been subsequently extended by a number of other researchers [4,[14][15][16][17].…”
Section: Introductionmentioning
confidence: 99%
“…6,7,9 As a spatiotemporal behavior, the plastic dynamics is actually seriously affected by a loading rate. 10 So far, although some reports have found that high strain rate could reduce the amplitude of serration events of BMGs under nanoindentation and compression tests, [11][12][13][14] how the strain rates affecting the plastic dyanmics of BMGs remains unclearly. Since the serrated flow resulted from a competition between the loading process associated with loading rate and the internal relaxation process, 15 strain rate increasing must modify the time scale of the loading process and then causes the dynamic behavior shifting.…”
Section: Introductionmentioning
confidence: 99%
“…The underlying deformation and fracture physics, being one of the most fundamental problems of MGs, has attracted substantial research effort for the last decades (Spaepen, 1975;Argon and Salama, 1976;Ravichandran and Molinari, 2005;Schuh et al, 2007;Jiang et al, 2008a;Raghavan et al, 2009;Tandaiya et al, 2009;Xu et al, 2010;Chen et al, 2011;Jang et al, 2011;Greer et al, 2013;Tandaiya et al, 2013;Narayan et al, 2014;Narasimhan et al, 2015). Due to their special atomic structures, MGs may go through ductile failure via shear banding (Dai et al, 2005;Jiang et al, 2008b;Chen and Lin, 2010;Chen et al, 2013;Greer et al, 2013) or brittle fracture by cavitation (Jiang et al, 2008a;Murali et al, 2011a;Singh et al, 2013Singh et al, , 2014. At nanoscale, these inelastic deformation and fracture is accommodated by atomic clusters called as shear transformation zones (STZs) (Argon, 1979;Falk and Langer, 1998) or tension transformation zones (TTZs) (Jiang et al, 2008a;Huang et al, 2014a).…”
Section: Introductionmentioning
confidence: 99%