Phys. Rev. B 70, 134113 (2004) [13 pages]

Elastic constants of defected and amorphous silicon with the environment-dependent interatomic potential

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Clark L. Allred1,2,3, Xianglong Yuan1, Martin Z. Bazant4, and Linn W. Hobbs1 *
1Department of Materials Science and Engineering, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
2The Charles Stark Draper Laboratory, Inc., 555 Technology Square, Cambridge, Massachusetts 02139, USA
3Air Force Institute of Technology, Wright-Patterson AFB, Ohio 45433, USA
4Department of Mathematics, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA

Received 9 February 2004; revised 20 May 2004; published 29 October 2004

The elastic constants of a wide range of models of defected crystalline and amorphous silicon are calculated, using the environment-dependent interatomic potential (EDIP). The defected crystalline simulation cells contain randomly generated defect distributions. An extensive characterization of point defects is performed, including structure, energy and influence on elastic constants. Three important conclusions are drawn. (1) Defects have independent effects on the elastic constants of silicon up to (at least) a defect concentration of 0.3%. (2) The linear effect of Frenkel pairs on the ⟨110⟩ Young’s modulus of silicon is −1653  GPa per defect fraction. (3) 17 different point defect types cause a very similar decrease in the ⟨110⟩ Young’s modulus: −(0.28±0.05)% when calculated in isolation using a 1728-atom cell. These principles will be very useful for predicting the effect of radiation damage on the elastic modulus of silicon in the typical case in which point-defect concentrations can be estimated, but the exact distribution and species of defects is unknown. We also study amorphous samples generated in quenching the liquid with EDIP, including an ideal structure of perfect fourfold coordination, samples with threefold and fivefold coordinated defects, one with a nanovoid, and one with an amorphous inclusion in a crystalline matrix. In the last case, a useful finding is that the change in the Young’s modulus is simply related to the volume fraction of amorphous material, as has also been observed by experiment.


©2004 The American Physical Society

URL: http://link.aps.org/doi/10.1103/PhysRevB.70.134113
DOI: 10.1103/PhysRevB.70.134113
PACS: 62.20.Dc, 61.82.−d

* Electronic address: hobbs@mit.edu

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