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R. B. Martin, Chem. Rev. (Washington, D.C.) CHREAY 0009-2665 10.1021/cr960037v 96, 3043 (1996) (one argument is that the self-assembly of a dimer involves twice the loss of orientational entropy than when a monomer joins a cluster).
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Martin, R.B.1
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A. Aggeli, M. Bell, N. Boden, J. N. Keen, T. C. B. McLeish, I. Nyrkova, S. E. Radford, and A. Semenov, J. Mater. Chem. JMACEP 0959-9428 10.1039/a701088e 7, 1135 (1997).
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Semenov, A.8
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4
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0042640726
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JCPSA6 0021-9606 10.1063/1.1734110, () [in the current context (monomer insertion) this sum rule is best derived from enforcing detailed balance between the system of interest and an ideal-gas reservoir of monomers at the same temperature and chemical potential].
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B. Widom, J. Chem. Phys. JCPSA6 0021-9606 10.1063/1.1734110 39, 2808 (1963) [in the current context (monomer insertion) this sum rule is best derived from enforcing detailed balance between the system of interest and an ideal-gas reservoir of monomers at the same temperature and chemical potential].
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Widom, B.1
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Since 1+ fa =1/ (1- ρ a), N- t evaluates to [(1+ fa) 2 -1] / fa
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Since 1+ fa =1/ (1- ρ a), N- t evaluates to [(1+ fa) 2 -1] / fa.
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7
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20144388657
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ACIEF5 1433-7851 10.1002/anie.200462160, () (see Fig.).
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C. Whitehouse, J. Fang, A. Aggeli, M. Bell, R. Brydson, C. W. G. Fishwick, J. R. Henderson, C. M. Knobler, R. W. Owens, N. H. Thomson, D. A. Smith, and N. Boden, Angew. Chem., Int. Ed. ACIEF5 1433-7851 10.1002/anie.200462160 44, 1965 (2005) (see Fig.).
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Whitehouse, C.1
Fang, J.2
Aggeli, A.3
Bell, M.4
Brydson, R.5
Fishwick, C.W.G.6
Henderson, J.R.7
Knobler, C.M.8
Owens, R.W.9
Thomson, N.H.10
Smith, D.A.11
Boden, N.12
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8
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0035131972
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JPCBFK 1089-5647 10.1021/jp003021o, () and references therein.
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S. May and A. Ben-Shaul, J. Phys. Chem. B JPCBFK 1089-5647 10.1021/jp003021o 105, 630 (2001) and references therein.
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May, S.1
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