메뉴 건너뛰기




Volumn 311, Issue 17, 2009, Pages 4265-4269

Monte Carlo simulation of a cluster model for the chirality conversion of crystals with grinding

Author keywords

A1. Computer simulation; A1. Growth models; A1. Stirring; A2. Growth from solutions

Indexed keywords

A1. COMPUTER SIMULATION; A1. GROWTH MODELS; A1. STIRRING; A2. GROWTH FROM SOLUTIONS; CLUSTER MODELS; ENANTIOMERIC EXCESS; HOMOCHIRALITY; MONTE CARLO SIMULATION; SATURATED SOLUTIONS; STATISTICAL FLUCTUATIONS;

EID: 68549106037     PISSN: 00220248     EISSN: None     Source Type: Journal    
DOI: 10.1016/j.jcrysgro.2009.07.005     Document Type: Article
Times cited : (31)

References (29)
  • 13
    • 68549094972 scopus 로고    scopus 로고
    • W.L. Noorduin, P. van der Asdonk, H. Meekes, W.J.P. van Enckevort, B. Kaptein, M. Leeman, R.M. Kellogg, E. Vlieg, Angew. Chem., Published online: 25 March 2009.
    • W.L. Noorduin, P. van der Asdonk, H. Meekes, W.J.P. van Enckevort, B. Kaptein, M. Leeman, R.M. Kellogg, E. Vlieg, Angew. Chem., Published online: 25 March 2009.
  • 21
    • 68549121514 scopus 로고    scopus 로고
    • We performed the simulation for various values of lmin and lmax and checked that our conclusions do not change
    • max and checked that our conclusions do not change.
  • 24
    • 68549131263 scopus 로고    scopus 로고
    • 3 stand for achiral molecules that show the chirality conversion of crystals by grinding.
    • 3 stand for achiral molecules that show the chirality conversion of crystals by grinding.
  • 26
    • 68549113505 scopus 로고    scopus 로고
    • J.M. McBride, Lecture at NORDITA Workshop Origins of homochirality, February 2008 〈http://agenda.albanova.se/conferenceDisplay.py?confId=322〉.
    • J.M. McBride, Lecture at NORDITA Workshop "Origins of homochirality", February 2008 〈http://agenda.albanova.se/conferenceDisplay.py?confId=322〉.
  • 27
    • 68549085845 scopus 로고    scopus 로고
    • If the initial EE is very small, the probability of ending up in the opposite chirality becomes large, especially in small systems, For the initial EE φ = 0.01, a small size as N = 3000 makes the odds even.
    • If the initial EE is very small, the probability of ending up in the opposite chirality becomes large, especially in small systems, For the initial EE φ = 0.01, a small size as N = 3000 makes the odds even.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.