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Volumn 105, Issue 42, 2001, Pages 10147-10158

Maximizing entropy by minimizing area: Towards a new principle of self-organization

Author keywords

[No Author keywords available]

Indexed keywords

NON-CLOSED PACKED CRYSTAL STRUCTURES; SOFT CORONAS;

EID: 0035950787     PISSN: 10895647     EISSN: None     Source Type: Journal    
DOI: 10.1021/jp010944q     Document Type: Article
Times cited : (239)

References (67)
  • 16
    • 0011328720 scopus 로고    scopus 로고
    • note
    • Chemical formula: methyl-3,4,5-tris-3′,4′,5′-[tris(n-dodecyloxy)-benzyloxy]bezoi c acid, n = 2, 3, or 4 denotes the generation of the dendrimer.
  • 19
    • 0011377552 scopus 로고    scopus 로고
    • note
    • Actually, the hexagonal close-packed (HCP) lattice and random stacking of hexagonal close-packed planes (RHCP) lattice have the same maximal packing fraction as the FCC lattice. As far as the free energy of hard spheres is concerned, the differences between these lattices are very subtle and do not show up within our framework.
  • 27
    • 0011299378 scopus 로고    scopus 로고
    • note
    • "Flattening" the curved space refers to substituting some of the dodecahedral cells by bubbles with 14 (= 12 pentagonal + 2 hexagonal), 15 (= 12 pentagonal + 3 hexagonal), or 16 (= 12 pentagonal + 4 hexagonal) faces. Cells with 13 faces are forbidden for topological reasons, and those with more than 16 faces are dynamically unstable.
  • 32
    • 0003986744 scopus 로고
    • Pergamon: Oxford
    • Barker, J.A. Lattice Theory of the Liquid State; Pergamon: Oxford, 1963. For a rigorous result, see: Salzburg, Z.W.; Wood, W.W. J. Chem. Phys. 1962, 37, 798.
    • (1963) Lattice Theory of the Liquid State
    • Barker, J.A.1
  • 33
    • 84950545763 scopus 로고
    • Barker, J.A. Lattice Theory of the Liquid State; Pergamon: Oxford, 1963. For a rigorous result, see: Salzburg, Z.W.; Wood, W.W. J. Chem. Phys. 1962, 37, 798.
    • (1962) J. Chem. Phys. , vol.37 , pp. 798
    • Salzburg, Z.W.1    Wood, W.W.2
  • 59
    • 0011299103 scopus 로고    scopus 로고
    • note
    • Technically, this was done by storing the accepted moves of the central particle and then assigning randomly selected accepted moves to its neighbors. The array of accepted moves was big enough so that the free energy did not depend on its size and was updated continuously. After equilibration, this led to identical probability distributions at all equivalent positions.
  • 63


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.