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Volumn 59, Issue 5, 1999, Pages 5790-5803

Off-lattice model for the phase behavior of lipid-cholesterol bilayers

Author keywords

[No Author keywords available]

Indexed keywords

ARTICLE;

EID: 0001407248     PISSN: 1063651X     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevE.59.5790     Document Type: Article
Times cited : (73)

References (33)
  • 1
    • 85037240789 scopus 로고    scopus 로고
    • Handbook of Biological Physics, edited by R. Lipowsky and E. Sackmann (North-Holland, Amsterdam, 1995), Vol. 1A-B
    • Handbook of Biological Physics, edited by R. Lipowsky and E. Sackmann (North-Holland, Amsterdam, 1995), Vol. 1A-B.
  • 19
    • 0004224163 scopus 로고
    • G. Cevc, Dekker, New York
    • Phospholipids Handbook, edited by G. Cevc (Dekker, New York, 1993).
    • (1993) Phospholipids Handbook
  • 25
    • 0004062244 scopus 로고
    • Leonard Finegold, CRL Press, Boca Raton, FL
    • Cholesterol in Membrane Models, edited by Leonard Finegold (CRL Press, Boca Raton, FL, 1993).
    • (1993) Cholesterol in Membrane Models
  • 26
    • 85037240503 scopus 로고    scopus 로고
    • the case where the lo phase consists of only cholesterol and gel chains in the ordered state, the microscopic Hamiltonian Eq. (2) can be rewritten as an Ising model in an external field. If we associate the Ising spin (Formula presented) state with a chain in the ordered state and the Ising spin (Formula presented) state with a cholesterol molecule, the occupation variables (Formula presented) and (Formula presented) can be expressed as (Formula presented) (Formula presented). Rewriting Eq. (2) in terms of the Ising spin variable we get (Formula presented) Noting that the interaction potentials (Formula presented) and (Formula presented) have very similar strength and that the strength of the interaction potential (Formula presented) is relatively small, we see that the model becomes an antiferromagnetic Ising model in an external temperature and pressure dependent field. (Formula presented) (Formula presented) and (Formula presented) are all attractive interaction potentials.)
    • In the case where the lo phase consists of only cholesterol and gel chains in the ordered state, the microscopic Hamiltonian Eq. (2) can be rewritten as an Ising model in an external field. If we associate the Ising spin (Formula presented) state with a chain in the ordered state and the Ising spin (Formula presented) state with a cholesterol molecule, the occupation variables (Formula presented) and (Formula presented) can be expressed as (Formula presented) (Formula presented). Rewriting Eq. (2) in terms of the Ising spin variable we get (Formula presented) Noting that the interaction potentials (Formula presented) and (Formula presented) have very similar strength and that the strength of the interaction potential (Formula presented) is relatively small, we see that the model becomes an antiferromagnetic Ising model in an external temperature and pressure dependent field. (Formula presented) (Formula presented) and (Formula presented) are all attractive interaction potentials.)
  • 30
    • 0001009808 scopus 로고
    • R. C. Aloia, J. M. Boggs, Academic Press, New York
    • F. T. Presti, in Membrane Fluidity in Biology, edited by R. C. Aloia and J. M. Boggs (Academic Press, New York, 1985), Vol. 4, pp. 97–146.
    • (1985) Membrane Fluidity in Biology , vol.4 , pp. 97-146
    • Presti, F.T.1
  • 32
    • 85037217324 scopus 로고    scopus 로고
    • Note that bilayers in our model are considered to be flat. An interpretation of ripple structures has recently been given in terms of a mesoscopic phenomenological model for lipid bilayers 32
    • Note that bilayers in our model are considered to be flat. An interpretation of ripple structures has recently been given in terms of a mesoscopic phenomenological model for lipid bilayers 32.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.