Hostname: page-component-84b7d79bbc-c654p Total loading time: 0 Render date: 2024-07-25T13:46:31.875Z Has data issue: false hasContentIssue false

Photon Correlation Spectroscopy of Liquid Crystals Confined in Porous Matrices with Different Structure and Pore Size

Published online by Cambridge University Press:  10 February 2011

F.M. Aliev
Affiliation:
Department of Physics and Materials Research Center, PO BOX 23343, University of Puerto Rico, San Juan, PR 00931–3343, USA
I.V. Plechakov
Affiliation:
Department of Physics and Materials Research Center, PO BOX 23343, University of Puerto Rico, San Juan, PR 00931–3343, USA
Get access

Abstract

We present the results of photon correlation spectroscopy investigations of the influence of confinement, interface, porous matrix structure, pore size and shape on the dynamic behavior of nematic liquid crystals (LC) dispersed in porous matrices with randomly oriented, interconnected pores (porous glasses) and parallel cylindrical pores (Anopore membranes). Investigations of LC in cylindrical pores together with studies in random porous matrices, makes it possible to separate the role of random structure and domain formation from the contributions due to existence of LC - solid pore wall interface and pure finite size effect in relaxation of order parameter or director fluctuations. In the temperature range below nematic - isotropie phase transition temperature we observed two overlapping relaxational processes which are satisfactorily described by the decay function f(q,t) = a·exp(–t1) + (1–aexp(–xz), where x = ln(t0)/ln20) and τ0 = 10−8s. For LC in 100 Å random pores the second term describing the slow process dominates, whereas for 200 Å and 2000 Å cylindrical pores as well as 1000 Å random pores the contribution from the first term (fast process) is more visible. Since the slow relaxational process which does not exist in the bulk LC and broad spectrum of relaxation times (10−6 - 10)s appear not only for LC in random pores but in cylindrical as well, we conclude that differences in dynamical behavior of confined LC from that in the bulk are mainly due to the existence of the interface.

Type
Research Article
Copyright
Copyright © Materials Research Society 1997

Access options

Get access to the full version of this content by using one of the access options below. (Log in options will check for institutional or personal access. Content may require purchase if you do not have access.)

References

REFERENCES

1. Wu, X-I., Goldburg, W.I., Liu, M.X., and Xue, J.Z, Phys. Rev. Lett. 69, 470, (1992).Google Scholar
2. Goldburg, W.I., Aliev, F.M., Wu, X-I., Physica A 213, 61, (1995).Google Scholar
3. Bellini, T., Clark, N.A., Schaefer, D.W., Phys. Rev. Lett. 74, 2740, (1995).Google Scholar
4. Zhang, Z. and Chakrabarti, A., Phys. Rev. E52, 4991, (1995).Google Scholar
5. Aliev, F.M. and Nadtotchi, V.V. in: Disordered Materials and Interfaces, edited by Cummins, H.Z., Durian, D.J., Johnson, D.L., and Stanley, H.E., (Mater. Res. Soc. Proc. 407, Pittsburgh, PA, 1996), pp. 125130.Google Scholar
6. Finotello, D. and Iannacchione, J., Int. Journ. Mod. Phys. B9, 109, 1995.Google Scholar
7. Crawford, G.P. and Zumer, S., Int. Journ. Mod. Phys. B9, 331, 1995.Google Scholar
8. Aliev, F.M., in Access in Nanoporous Materials, edited by Pinnavaia, T.J. and Thorpe, M.F., (Plenum Press, New York, 1995), pp. 335354.Google Scholar
9. Crawford, G.P. and Zumer, S., Liquid crystals in complex geometries, (Taylor & Francis, London, 1996).Google Scholar
10. de Gennes, P.G. and Prost, J., The Physics of Liquid Crystals, 2nd ed. (Clarendon Press, Oxford, 1993).Google Scholar