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Numéro
J. Phys. II France
Volume 5, Numéro 2, February 1995
Page(s) 243 - 248
DOI https://doi.org/10.1051/jp2:1995126
References of J. Phys. II France 5 243-248
  1. Odijk T, J Phys. France 48 (1987) 125 [CrossRef] [EDP Sciences].
  2. van der Schoot P. and Cates M. E., Langmuir 10 (1994) 670 [CrossRef].
  3. Attwood T. K., Lydon J. E. and Jones F., Liq Cryst. 1 (1986) 499 [CrossRef]
  4. van der Schoot P and Cates M. E., Europhys. Lett 25 (1994) 515 [CrossRef].
  5. The deflection length measures the average distance over which the contour of a chain is deflected towards the director of the nematic molecular field [6].
  6. Odijk T., Macromolecules 19 (1986) 2313 [CrossRef].
  7. Onsager L., Ann. N.Y. Acad. Sci. 51 (1949) 627 [CrossRef].
  8. Vroege G J. and Lekkerkerker H N. W., Rep. Prog. Phys 55 (1992) 1241 [CrossRef].
  9. a) Khokhlov A R. and Semenov A. N., Physica 108 (1981) 546 [CrossRef]; b) Khokhlov A. R and Semenov A. N., Physica A 112 (1982) 605 [CrossRef].
  10. To obtain Equation (4) from [9] one merely has to realize that $\rho(s$, u) can be written as the product of the orientationally averaged number density rods of size s and the normalized angular distribution of these rods (not to be confused with the orientational mass distribution $\Psi$ introduced in Eq. (5)).
  11. Vroege G. J., Private communication.
  12. Taylor M. P. and Herzfeld J., J. Phys Condens. Matter 5 (1993) 2651 [CrossRef].
  13. Khokhlov A. R. and Semenov A. N., J. Stat Phys. 38 (1985) 161 [CrossRef].