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Volumn 31, Issue 5, 1985, Pages 3199-3213

Finite-size effect for the critical point of an anisotropic dimer model of domain walls

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Indexed keywords


EID: 26144456293     PISSN: 10502947     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevA.31.3199     Document Type: Article
Times cited : (48)

References (30)
  • 3
    • 84927246816 scopus 로고    scopus 로고
    • We are using the conventional notations, namely, β =(kBT)-1, where T is the temperature and kB is the Boltzmann constant. The specific-heat exponent alpha is given by c(t) app t-α as t -> 0, where c is the specific heat and t is the reduced temperature (T-Tc)/Tc. For the length scale ξi the exponent νi is given by ξiapp t-νi for i=x,y as t -> 0. For an isotropic system the subscript i may be omitted.
  • 6
    • 84927246815 scopus 로고    scopus 로고
    • B. M. McCoy and T. T. Wu, The Two Dimensional Ising Model, (Harvard University, Cambridge, Mass., 1973).
  • 26
    • 84927246813 scopus 로고    scopus 로고
    • S. M. Bhattacharjee, Ph.D thesis, Carnegie Mellon University, 1984.
  • 27
    • 84927246811 scopus 로고    scopus 로고
    • In Ref. 7 the partition function is written as Z=(-Z1+Z2+Z3+Z4)/2. However we have incorporated the minus sign associated with Z1 in the definition in Eq. (2.2).
  • 30
    • 84927246809 scopus 로고    scopus 로고
    • International Mathematical and Statistical Libraries subroutines, available from IMSL, Inc., Houston, Texas 77036-5085.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.