2007
DOI: 10.1103/physrevlett.99.165502
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Threshold Crack Speed Controls Dynamical Fracture of Silicon Single Crystals

Abstract: Fracture experiments of single silicon crystals reveal that after the critical fracture load is reached, the crack speed jumps from zero to 2 km= sec, indicating that crack motion at lower speeds is forbidden. This contradicts classical continuum fracture theories predicting a continuously increasing crack speed with increasing load. Here we show that this threshold crack speed may be due to a localized phase transformation of the silicon lattice from 6-membered rings to a 5-7 double ring at the crack tip.

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Cited by 138 publications
(136 citation statements)
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“…Since all intended applications were at temperatures well above the water boiling point, this was not a major development concern. In 2009, efforts were initiated to redevelop ReaxFF for aqueous chemistry, and it became clear that the 2008-C/H/O combustion force field, which at that time was already extended to a significant range of metal oxide (Me = V/Bi/Mo/Nb/Si) materials and catalysts, [27][28][29][30][31] could not be parameterised to treat liquid water without changing general-ReaxFF and atom-specific parameters. As such, the decision was made to initiate a new branch-the aqueousbranch-that employs the same functional form as the 2008-C/H/O description, but with different O/H atom and bond parameters.…”
Section: Current Reaxff Methodologymentioning
confidence: 99%
“…Since all intended applications were at temperatures well above the water boiling point, this was not a major development concern. In 2009, efforts were initiated to redevelop ReaxFF for aqueous chemistry, and it became clear that the 2008-C/H/O combustion force field, which at that time was already extended to a significant range of metal oxide (Me = V/Bi/Mo/Nb/Si) materials and catalysts, [27][28][29][30][31] could not be parameterised to treat liquid water without changing general-ReaxFF and atom-specific parameters. As such, the decision was made to initiate a new branch-the aqueousbranch-that employs the same functional form as the 2008-C/H/O description, but with different O/H atom and bond parameters.…”
Section: Current Reaxff Methodologymentioning
confidence: 99%
“…In this work, we use a parameterization of ReaxFF extended to the simulation of silica (Duin et al 2003;Chenoweth et al 2005) which is suitable for the two materials we consider in this work. Previous studies on the fracture of silicon have used ReaxFF successfully (Buehler et al , 2007, and the potential formulation does not seem to exhibit spurious features that would strongly affect the fracture behavior such as the force peak in the REBO reactive potential (Belytschko et al 2002). In our simulations, the fracture behavior simulated with reaxFF is consistent with the expected materials behaviors: brittle fracture but without cleavage for the silica (Swiler 1994;Swiler et al 1995), and chain elongation and scission of the nanoporous carbon (Rottler 2009).…”
Section: Simulation Detailsmentioning
confidence: 99%
“…For eight different iron potentials, they concluded that there was too much variation of unstable stacking fault energies and the resulting K IC variation for emitting dislocations of 40% was far too large. However, use of other material simulation techniques, [194][195][196][197] mostly theoretical and applied mechanics, have produced some success, but are not often compared to the atomistic fundamentals. To achieve a more complete understanding of DBTs over multiple modeling scales, detailed in situ experiments measuring plastic and fracture properties of multiple materials are needed.…”
Section: Future Nanomechanical Approaches To Brittleness Transitionsmentioning
confidence: 99%