Articles citing this article

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Cited article:

Phase behaviour and long-time self-diffusion in a binary hard sphere dispersion

A. Imhof and J.K.G. Dhont
Colloids and Surfaces A: Physicochemical and Engineering Aspects 122 (1-3) 53 (1997)
https://doi.org/10.1016/S0927-7757(96)03843-5

Self-Diffusion of Charged Polybutadiene Latex Particles in Water Measured by Pulsed Field Gradient NMR

M. H. Blees, J. M. Geurts and J. C. Leyte
Langmuir 12 (8) 1947 (1996)
https://doi.org/10.1021/la9502960

The influence of structure on diffusion in screened Coulombic suspensions

Stephen J. Nilsen and Alice P. Gast
The Journal of Chemical Physics 101 (6) 4975 (1994)
https://doi.org/10.1063/1.467420

Hydrodynamic effects in polydisperse charged colloidal suspensions at short times

G. Nägele, O. Kellerbauer, R. Krause and R. Klein
Physical Review E 47 (4) 2562 (1993)
https://doi.org/10.1103/PhysRevE.47.2562

Trends in Colloid and Interface Science V

J. L. Arauz-Lara, H. Ruiz-Estrada, M. Medina-Noyola, G. Nägele and R. Klein
Progress in Colloid & Polymer Science, Trends in Colloid and Interface Science V 84 377 (1991)
https://doi.org/10.1007/BFb0116008

Trends in Colloid and Interface Science V

T. Palberg, R. Simon and P. Leiderer
Progress in Colloid & Polymer Science, Trends in Colloid and Interface Science V 84 397 (1991)
https://doi.org/10.1007/BFb0116011

Collective diffusion in colloidal crystals

Paul A. Rundquist, R. Kesavamoorthy, S. Jagannathan and Sanford A. Asher
The Journal of Chemical Physics 95 (11) 8546 (1991)
https://doi.org/10.1063/1.461283

Statics and tracer-diffusion in binary suspensions of polystyrene spheres: experiment vs. theory

R. Krause, J.L. Arauz-Lara, G. Nägele, et al.
Physica A: Statistical Mechanics and its Applications 178 (2) 241 (1991)
https://doi.org/10.1016/0378-4371(91)90020-D

Rescaled mean spherical approximation for colloidal mixtures

H. Ruiz-Estrada, M. Medina-Noyola and G. Nägele
Physica A: Statistical Mechanics and its Applications 168 (3) 919 (1990)
https://doi.org/10.1016/0378-4371(90)90263-R