메뉴 건너뛰기




Volumn 78, Issue 18, 2008, Pages

Modeling the plastic relaxation onset in realistic SiGe islands on Si(001)

Author keywords

[No Author keywords available]

Indexed keywords


EID: 56349107056     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.78.184104     Document Type: Article
Times cited : (61)

References (45)
  • 22
    • 36149012981 scopus 로고
    • 10.1103/PhysRev.80.436
    • M. Peach and J. S. Koehler, Phys. Rev. 80, 436 (1950). 10.1103/PhysRev.80.436
    • (1950) Phys. Rev. , vol.80 , pp. 436
    • Peach, M.1    Koehler, J.S.2
  • 23
    • 0034899101 scopus 로고    scopus 로고
    • 10.1103/PhysRevB.63.205424
    • B. J. Spencer and J. Tersoff, Phys. Rev. B 63, 205424 (2001). 10.1103/PhysRevB.63.205424
    • (2001) Phys. Rev. B , vol.63 , pp. 205424
    • Spencer, B.J.1    Tersoff, J.2
  • 30
    • 34547678037 scopus 로고    scopus 로고
    • 10.1016/j.ijplas.2007.03.003
    • T. Belytschko and R. Gracie, Int. J. Plast. 23, 1721 (2007). 10.1016/j.ijplas.2007.03.003
    • (2007) Int. J. Plast. , vol.23 , pp. 1721
    • Belytschko, T.1    Gracie, R.2
  • 32
    • 56349160086 scopus 로고    scopus 로고
    • edited by Erich Kasper and Klara Lyutovich (University of Stuttgart, Germany
    • R. Hull in Properties of Silicon Germanium and SiGe: Carbon, edited by, Erich Kasper, and, Klara Lyutovich, (University of Stuttgart, Germany, 2000), pp. 21-39.
    • (2000) Properties of Silicon Germanium and SiGe: Carbon , pp. 21-39
    • Hull, R.1
  • 37
    • 16444366630 scopus 로고
    • 10.1103/PhysRevB.37.6991
    • J. Tersoff, Phys. Rev. B 37, 6991 (1988). 10.1103/PhysRevB.37.6991
    • (1988) Phys. Rev. B , vol.37 , pp. 6991
    • Tersoff, J.1
  • 38
    • 27744577658 scopus 로고
    • 10.1103/PhysRevB.39.5566
    • J. Tersoff, Phys. Rev. B 39, 5566 (1989). 10.1103/PhysRevB.39.5566
    • (1989) Phys. Rev. B , vol.39 , pp. 5566
    • Tersoff, J.1
  • 41
    • 56349159583 scopus 로고    scopus 로고
    • While introducing a 3 ML WL does not require any additional cost in the atomistic simulations, so that we considered its presence, inserting a three-layer Ge subdomain in the FEM calculation forces the creation of a dense mesh within this thin region. Since the WL has a negligible effect on the island stress field (Ref.) (as also demonstrated by the comparison between atomistic and FEM results), we avoided this additional computational cost in the FEM calculations by placing the island directly on the Si substrate. We also checked that neglecting the WL does not produce any significant variation in the critical volume for dislocation insertion.
    • While introducing a 3 ML WL does not require any additional cost in the atomistic simulations, so that we considered its presence, inserting a three-layer Ge subdomain in the FEM calculation forces the creation of a dense mesh within this thin region. Since the WL has a negligible effect on the island stress field (Ref.) (as also demonstrated by the comparison between atomistic and FEM results), we avoided this additional computational cost in the FEM calculations by placing the island directly on the Si substrate. We also checked that neglecting the WL does not produce any significant variation in the critical volume for dislocation insertion.
  • 43
    • 33748417557 scopus 로고    scopus 로고
    • 10.1103/PhysRevB.74.121302
    • F. Glas, Phys. Rev. B 74, 121302 (R) (2006). 10.1103/PhysRevB.74.121302
    • (2006) Phys. Rev. B , vol.74 , pp. 121302
    • Glas, F.1
  • 44
    • 56349085538 scopus 로고    scopus 로고
    • As discussed when describing the PK and the MF approaches, the presence of free surfaces causes a faster decay of the dislocation field. This allowed us to find converged values of Etot considering relatively thin substrates. For the results reported in Sec. 4, a Si substrate thickness of 2000 nm turned out to be more than sufficient.
    • As discussed when describing the PK and the MF approaches, the presence of free surfaces causes a faster decay of the dislocation field. This allowed us to find converged values of Etot considering relatively thin substrates. For the results reported in Sec. 4, a Si substrate thickness of 2000 nm turned out to be more than sufficient.
  • 45
    • 0343973898 scopus 로고
    • 10.1063/1.349451
    • D. C. Houghton, J. Appl. Phys. 70, 2136 (1991). 10.1063/1.349451
    • (1991) J. Appl. Phys. , vol.70 , pp. 2136
    • Houghton, D.C.1


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.