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Volumn 59, Issue 2, 1999, Pages 1523-1539

Planar lattice model with gas, liquid, and solid phases

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EID: 0001135278     PISSN: 1063651X     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevE.59.1523     Document Type: Article
Times cited : (14)

References (21)
  • 17
    • 85035239511 scopus 로고    scopus 로고
    • Order-Disorder Phenomena (Interscience, 1964); Chapter 5. Using magnetic language, the critical value of K (Formula presented) for isotropic interactions is given by the condition that (Formula presented) for the triangular lattice, (Formula presented) for the square planar lattice and (Formula presented) for the honeycomb lattice (called the hexagonal lattice by Green and Hurst). In all cases the conversion to lattice gas language is given by (Formula presented) where (Formula presented) where ɛ is the nearest-neighbor interaction energy.
    • See: H. S. Green and C. A. Hurst, Order-Disorder Phenomena (Interscience, 1964); Chapter 5. Using magnetic language, the critical value of K (Formula presented) for isotropic interactions is given by the condition that (Formula presented) for the triangular lattice, (Formula presented) for the square planar lattice and (Formula presented) for the honeycomb lattice (called the hexagonal lattice by Green and Hurst). In all cases the conversion to lattice gas language is given by (Formula presented) where (Formula presented) where ɛ is the nearest-neighbor interaction energy.
    • Green, H.S.1    Hurst, C.A.2


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.