Colloidal particles with a dielectric constant mismatch with the surrounding solvent in an external biaxial magnetic or electric field experience an “inverted” dipolar interaction. We determine the phase behavior of such a system using Helmholtz free energy calculations in Monte Carlo simulations for colloidal hard spheres as well as for charged hard spheres interacting with a repulsive Yukawa potential. The phase diagram of colloidal hard spheres with inverted dipolar interactions shows a gas-liquid transition, a hexagonal ABC stacked crystal phase, and a stretched hexagonal-close-packed crystal. The phase diagram for charged spheres is very similar, but displays an additional layered-fluid phase. We compare our results with recent experimental observations.
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28 May 2010
Research Article|
May 28 2010
Phase diagram of colloidal spheres in a biaxial electric or magnetic field Available to Purchase
Frank Smallenburg;
Frank Smallenburg
a)
Soft Condensed Matter, Debye Institute for Nanomaterials Science,
Utrecht University
, Princetonplein 5, Utrecht 3584 CC, The Netherlands
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Marjolein Dijkstra
Marjolein Dijkstra
Soft Condensed Matter, Debye Institute for Nanomaterials Science,
Utrecht University
, Princetonplein 5, Utrecht 3584 CC, The Netherlands
Search for other works by this author on:
Frank Smallenburg
a)
Soft Condensed Matter, Debye Institute for Nanomaterials Science,
Utrecht University
, Princetonplein 5, Utrecht 3584 CC, The Netherlands
Marjolein Dijkstra
Soft Condensed Matter, Debye Institute for Nanomaterials Science,
Utrecht University
, Princetonplein 5, Utrecht 3584 CC, The Netherlands
a)
Electronic mail: [email protected].
J. Chem. Phys. 132, 204508 (2010)
Article history
Received:
October 19 2009
Accepted:
April 14 2010
Citation
Frank Smallenburg, Marjolein Dijkstra; Phase diagram of colloidal spheres in a biaxial electric or magnetic field. J. Chem. Phys. 28 May 2010; 132 (20): 204508. https://doi.org/10.1063/1.3425734
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